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Dynamic ProgrammingOperations ResearchStochastic Systems·Captain: mikedeng1

Dynamic Pricing of Relocating Resources in Large Networks: the Lagrangian policy is within O(√(ln n/n)) of optimal in hub-and-spoke networksResearch Paper

Motivation

Ride-hailing, car-sharing and bike-sharing platforms price trips whose execution moves the resource itself: a car that takes a passenger from the suburbs to the airport is no longer available in the suburbs. Each price therefore sets both the revenue of the current request and the future spatial distribution of the fleet. Choosing prices to maximise long-run revenue is a Markov decision problem whose state, the number of resources at each location, has a number of configurations exponential in the number of locations. Exact dynamic programming is impossible at the scale of a city.

Balseiro, Brown and Chen (SSRN 3313737, version of May 23, 2020; published in Management Science, doi:10.1287/mnsc.2020.3735) study hub-and-spoke networks and propose a Lagrangian policy. The capacity constraint coupling the locations is relaxed with a dual variable, the relaxation separates into one small problem per spoke, and the per-spoke solutions are implemented in the real system. Earlier work on this model (Waserhole and Jost, 2016; Banerjee, Freund and Lykouris, 2016) uses fluid relaxations that lead to static prices, depending on the origin and destination but not on the resource levels. These are within a factor m/(m+n−1)m/(m+n-1)m/(m+n−1) of the fluid bound, hence asymptotically optimal when the number of resources mmm grows faster than the number of locations nnn. When mmm and nnn grow at the same rate, which is the regime of a large city with few vehicles per area, no static policy is asymptotically optimal (the paper's Example 5.1). The Lagrangian policy is a dynamic, state-dependent policy that is computable and asymptotically optimal in that regime.

Setting

A hub (location 000) and nnn spokes i∈[n]i\in[n]i∈[n] share mmm resources. In each period one request arrives: it asks to relocate a resource from spoke iii to the hub, type (i,0)(i,0)(i,0), with probability qi0>0q_{i0}>0qi0​>0, or from the hub to spoke iii, type (0,i)(0,i)(0,i), with probability q0i>0q_{0i}>0q0i​>0; these probabilities sum to one and are independent across periods. The provider picks a demand level d∈[0,1]d\in[0,1]d∈[0,1], equivalently a price. The request is fulfilled with probability ddd if its origin holds a resource and is lost otherwise; the expected revenue is rij(d)r_{ij}(d)rij​(d). Assumption 2.1: each rijr_{ij}rij​ is strictly concave on [0,1][0,1][0,1], rij(0)=0r_{ij}(0)=0rij​(0)=0, max⁡rij≤rˉ\max r_{ij}\le\bar rmaxrij​≤rˉ, max⁡∣rij′∣≤ωˉ\max|r_{ij}'|\le\bar\omegamax∣rij′​∣≤ωˉ, and the maximiser is interior.

The state is the vector of spoke levels x∈X={x∈Nn:∑ixi≤m}x\in\mathcal X=\{x\in\mathbb N^n:\sum_ix_i\le m\}x∈X={x∈Nn:∑i​xi​≤m}, the hub holding x0=m−∑ixix_0=m-\sum_ix_ix0​=m−∑i​xi​. The optimal average revenue VOPTV^{\mathrm{OPT}}VOPT (problem (1)) is the supremum, over non-anticipative feasible policies, of the long-run average expected revenue.

Penalising the spoke resources with a dual variable λ≥0\lambda\ge0λ≥0 yields, for each spoke, the spoke problem (6): maximise ∑xpi(x)[qi0ri0(di(x,i,0))+q0ir0i(di(x,0,i))]−λ∑xx pi(x)\sum_xp_i(x)[q_{i0}r_{i0}(d_i(x,i,0))+q_{0i}r_{0i}(d_i(x,0,i))]-\lambda\sum_xx\,p_i(x)∑x​pi​(x)[qi0​ri0​(di​(x,i,0))+q0i​r0i​(di​(x,0,i))]−λ∑x​xpi​(x) over a distribution pip_ipi​ on [0:m][0:m][0:m] and controls satisfying the birth–death balance equations pi(x)q0idi(x,0,i)=pi(x+1)qi0di(x+1,i,0)p_i(x)q_{0i}d_i(x,0,i)=p_i(x+1)q_{i0}d_i(x+1,i,0)pi​(x)q0i​di​(x,0,i)=pi​(x+1)qi0​di​(x+1,i,0). Its value is hiλh_i^\lambdahiλ​. The relaxation value is Vˉλ=mλ+∑ihiλ\bar V^\lambda=m\lambda+\sum_ih_i^\lambdaVˉλ=mλ+∑i​hiλ​ (4), the Lagrangian bound is VR=min⁡λ≥0VˉλV^{\mathrm R}=\min_{\lambda\ge0}\bar V^\lambdaVR=minλ≥0​Vˉλ (9), and the perturbed dual is VR(δ)=min⁡λ≥0Vˉλ−δλV^{\mathrm R}(\delta)=\min_{\lambda\ge0}\bar V^\lambda-\delta\lambdaVR(δ)=minλ≥0​Vˉλ−δλ (11), with optimal solution λ∗(δ)\lambda^*(\delta)λ∗(δ). The Lagrangian policy π(δ)\pi(\delta)π(δ) (Definition 3.1) applies the controls of optimal solutions of (6) at λ∗(δ)\lambda^*(\delta)λ∗(δ), spoke by spoke, and drops a hub request when the hub is empty. Vπ(δ)V^{\pi(\delta)}Vπ(δ) is its average revenue and P[X0(δ)=0]\mathbb P[X_0(\delta)=0]P[X0​(δ)=0] the stationary probability that the hub is empty. In the relaxed system the hub may go negative; there the spokes are independent with laws pip_ipi​.

Formalization targets

Goal: Corollary 4.7

Under Assumption 4.1 (E[X~i(δ)]≤c\mathbb E[\tilde X_i(\delta)]\le cE[X~i​(δ)]≤c for every spoke, c>0c>0c>0 independent of nnn) and with b=1/(1+c)b=1/(1+c)b=1/(1+c), for 0≤δ<m0\le\delta<m0≤δ<m,

Vπ(δ)≤VOPT≤VR≤Vπ(δ)+rˉ δm−δ+(rˉ+ωˉ)exp⁡(−b2⋅δ2m+n),V^{\pi(\delta)}\le V^{\mathrm{OPT}}\le V^{\mathrm R}\le V^{\pi(\delta)}+\bar r\,\frac{\delta}{m-\delta}+(\bar r+\bar\omega)\exp\Big(-\frac b2\cdot\frac{\delta^2}{m+n}\Big),Vπ(δ)≤VOPT≤VR≤Vπ(δ)+rˉm−δδ​+(rˉ+ωˉ)exp(−2b​⋅m+nδ2​),

and with δ=(1/b)(m+n)ln⁡n\delta=\sqrt{(1/b)(m+n)\ln n}δ=(1/b)(m+n)lnn​,

VOPT−Vπ(δ)=O(ln⁡n/n)when m and n grow at the same rate.V^{\mathrm{OPT}}-V^{\pi(\delta)}=O\Big(\sqrt{\ln n/n}\Big)\quad\text{when }m\text{ and }n\text{ grow at the same rate.}VOPT−Vπ(δ)=O(lnn/n​)when m and n grow at the same rate.

Milestones

The milestones follow the paper's proof. The spoke problem solves the spoke Bellman equation (Proposition 3.2), the relaxation's value is independent of the initial state, equals mλ+∑ihiλm\lambda+\sum_ih_i^\lambdamλ+∑i​hiλ​ and bounds VOPTV^{\mathrm{OPT}}VOPT (Proposition 3.1), and the controls are monotone (Proposition 3.3). The relaxed and original chains have stationary laws ∏ipi\prod_ip_i∏i​pi​ and a unique μ\muμ (Corollaries B.10, B.11). The perturbation costs at most rˉδ/(m−δ)\bar r\delta/(m-\delta)rˉδ/(m−δ) (Lemma 4.2), continuation-value differences are at most ωˉ\bar\omegaωˉ (Lemma A.10), and the relaxed–original gap is controlled by hub depletion (Lemma 4.3), giving Theorem 4.1,

Vπ(δ)≤VOPT≤VR≤Vπ(δ)+rˉ δm−δ+(rˉ+ωˉ) P[X0(δ)=0].V^{\pi(\delta)}\le V^{\mathrm{OPT}}\le V^{\mathrm R}\le V^{\pi(\delta)}+\bar r\,\frac{\delta}{m-\delta}+(\bar r+\bar\omega)\,\mathbb P[X_0(\delta)=0].Vπ(δ)≤VOPT≤VR≤Vπ(δ)+rˉm−δδ​+(rˉ+ωˉ)P[X0​(δ)=0].

Stochastic dominance between the two systems (Lemma 4.4) gives P[X0(δ)=0]≤P[X~0(δ)≤0]\mathbb P[X_0(\delta)=0]\le\mathbb P[\tilde X_0(\delta)\le0]P[X0​(δ)=0]≤P[X~0​(δ)≤0] (Corollary 4.5). The spoke laws are log-concave (Proposition B.9), log-concave generating functions are dominated by geometric ones (Lemma A.14), a concentration bound for sums of log-concave variables follows (Lemma A.12), and the relaxed depletion probability is at most exp⁡(−b2δ2/(m+n))\exp(-\tfrac b2\delta^2/(m+n))exp(−2b​δ2/(m+n)) (Proposition 4.6).

Significance

The result. A policy computed from nnn independent problems of size m+1m+1m+1 loses only O(ln⁡n/n)O(\sqrt{\ln n/n})O(lnn/n​) per period against the optimal policy of a problem with exponentially many states. No static policy achieves a vanishing gap. Theorem 4.1 also yields a practical certificate: VRV^{\mathrm R}VR is a computable upper bound, and the gap is governed by one observable quantity, the hub-depletion probability. The same structure extends to several hubs (the paper's Theorem 6.1).

Formalizing it. The result is proved in the paper; nothing here is open, and no part of it has been machine-checked. A formal proof would check a chain that combines average-reward dynamic programming, convex duality and sensitivity analysis, a coupling argument between two Markov chains, and a concentration inequality for log-concave variables. Several of these steps are stated in the paper with brief or cited arguments (the Bellman equation of the spoke problem, the class structure of the chains, Keilson's factorial-moment inequality behind Lemma A.14).

Difficulty

The natural first idea is to use the Lagrangian policy at the optimal dual λ∗\lambda^*λ∗ of (9). At λ∗>0\lambda^*>0λ∗>0 the relaxation keeps zero resources in the hub in expectation, so the real hub is empty a constant fraction of the time and every hub request lost there costs a constant. The perturbation δ\deltaδ is what makes the argument work. The key step is then to compare the relaxed system, where spokes are independent and the hub may go negative, with the original system, where the hub constraint couples all spokes. This needs both a loss bound per depletion event (Lemma A.10, which rests on the monotonicity of Proposition 3.3) and a pathwise coupling (Lemma 4.4). A Chebyshev bound on the hub level gives only a polynomial rate. The exponential rate requires the log-concavity of every spoke law and a geometric domination of its generating function.

Formalization scope

  • No measure theory. Policies are deterministic functions of the observed history (past request types and fulfilment outcomes) and the current request type. The finite-horizon expected revenue is a finite recursion, and VOPTV^{\mathrm{OPT}}VOPT is the supremum over feasible policies of the limsup of its time average. Stationary distributions are finite probability vectors, via the published definition MarkovChain.IsStationary. Sums of independent ℕ-valued variables are iterated convolutions.
  • Primitives. The revenue functions rijr_{ij}rij​ are primitives satisfying Assumption 2.1. Request types are Fin n ⊕ Fin n, spoke levels Fin (m+1), the hub level is m−∑ixim-\sum_ix_im−∑i​xi​, and the original chain lives on X\mathcal XX.
  • Definitions. hiλh_i^\lambdahiλ​ is defined as the value of (6); Proposition 3.2 is stated as "(6)'s value solves (5)". The Lagrangian policy is built from any optimal solutions of (6) at any optimal λ∗(δ)\lambda^*(\delta)λ∗(δ), with the paper's controls (111 and 000) above the support.
  • Disclosed choices. Assumption 4.1 is assumed only at the δ\deltaδ in use. "Grow at the same rate" is κ1n≤m≤κ2n\kappa_1n\le m\le\kappa_2nκ1​n≤m≤κ2​n, with the constant CCC and the threshold N0N_0N0​ chosen before the network.
  • Non-vacuity. The goal includes an attainment clause: λ∗(δ)\lambda^*(\delta)λ∗(δ), optimal solutions of (6) and a stationary distribution exist. A proof cannot pass through empty hypotheses, and suprema and infima are taken over nonempty, bounded index sets.
  • Not formalized. Proposition 2.1 (continuous-time utilisation), Proposition 2.2 (Bellman equation (2)), Lemma 4.8 (primitive sufficient conditions for Assumption 4.1), §5–§6 and the appendices on algorithms are not formalized.
  • Reusable pieces. The log-concavity and convolution vocabulary and Lemmas A.12/A.14 are independent of the model and reusable. Contributions to the class structure of finite birth–death product chains, and to Keilson's moment inequality (Lemma A.13), are welcome.

Selected references

  • S. R. Balseiro, D. B. Brown, C. Chen, Dynamic Pricing of Relocating Resources in Large Networks, SSRN working paper 3313737, version of May 23, 2020. https://ssrn.com/abstract=3313737 ; Management Science, https://doi.org/10.1287/mnsc.2020.3735
  • J. Keilson, A threshold for log-concavity for probability generating functions and associated moment inequalities, Annals of Mathematical Statistics 43(5), 1702–1708, 1972.
  • S. Janson, Tail bounds for sums of geometric and exponential variables, Statistics & Probability Letters 135, 2018. https://arxiv.org/abs/1709.08157
  • S. Banerjee, D. Freund, T. Lykouris, Pricing and optimization in shared vehicle systems: an approximation framework, 2016. https://arxiv.org/abs/1608.06819
  • A. Waserhole, V. Jost, Pricing in vehicle sharing systems: optimization in queuing networks with product forms, EURO Journal on Transportation and Logistics 5(3), 293–320, 2016.
19 thms2 active usersReviewed
Operations ResearchOptimizationTheoretical Computer Science·Captain: mikedeng1

Display Optimization for Vertically Differentiated Locations Under Multinomial Logit Preferences: Revenue Lower Bound for the Assignment Rounded from Dynamic-Programming ActionsResearch Paper

Motivation

Retailers, online travel agencies and search engines display products in an ordered list or on a physical layout, and customers inspect only a prefix of it. Display optimization asks how to assign products to positions so as to maximize expected revenue when each customer considers only the products shown in the first kkk positions, with kkk random. Aouad and Segev (SSRN 2709652; Management Science 67(6), 2021) study this problem with vertically differentiated locations (every customer who sees position k+1k+1k+1 also sees positions 1,…,k1,\dots,k1,…,k) and multinomial logit (MNL) choice within the consideration set. The model covers assortment planning over time and product framing on web pages, and it was calibrated on Expedia hotel-search data in the paper's case study.

The paper's headline claim (Theorem 1.1) is a polynomial-time approximation scheme, obtained by a dynamic program over approximate assortments followed by a rounding of its actions into an assignment. The rounding analysis, Section 5.2, contains a self-contained chain of combinatorial inequalities about the rounded assignment. That chain is the subject of this mission.

Setting

There are nnn items. Item i∈[n]i\in[n]i∈[n] has a price ri>0r_i>0ri​>0 and an MNL preference weight wi>0w_i>0wi​>0; write ρi=riwi\rho_i=r_iw_iρi​=ri​wi​ and, for an assortment S⊆[n]S\subseteq[n]S⊆[n],

ρ(S)=∑i∈Sρi,w(S)=∑i∈Swi,R(S)=ρ(S)1+w(S),\rho(S)=\sum_{i\in S}\rho_i,\qquad w(S)=\sum_{i\in S}w_i,\qquad R(S)=\frac{\rho(S)}{1+w(S)} ,ρ(S)=i∈S∑​ρi​,w(S)=i∈S∑​wi​,R(S)=1+w(S)ρ(S)​,

the expected revenue of offering SSS to an MNL customer with a no-purchase option of weight 111. An assignment A\mathcal AA is a bijection from positions [n][n][n] to items; A[k]\mathcal A[k]A[k] is the set of items in positions 1,…,k1,\dots,k1,…,k, Rk(A)=R(A[k])R_k(\mathcal A)=R(\mathcal A[k])Rk​(A)=R(A[k]), and with position weights λk>0\lambda_k>0λk​>0 the objective is

R(A)=∑k=1nλkRk(A).\mathcal R(\mathcal A)=\sum_{k=1}^n\lambda_kR_k(\mathcal A).R(A)=k=1∑n​λk​Rk​(A).

The algorithm fixes an accuracy ϵ∈(0,1/5)\epsilon\in(0,1/5)ϵ∈(0,1/5) and a guessed position kmidk_{\mathrm{mid}}kmid​. A sequence of dynamic-programming actions consists of events e1,…,eT∈[n]e_1,\dots,e_T\in[n]e1​,…,eT​∈[n] and pairs (Sj−,Sj+)(S^-_j,S^+_j)(Sj−​,Sj+​) of item sets (a sub-assortment and a super-assortment), starting from e1=1e_1=1e1​=1, S1−=S1+={i1}S^-_1=S^+_1=\{i_1\}S1−​=S1+​={i1​} and ending at eT=ne_T=neT​=n, ST−=ST+=[n]S^-_T=S^+_T=[n]ST−​=ST+​=[n]. Consecutive actions must satisfy seven constraints, (8)–(14) of the paper: nestedness Sj−1−⊆Sj−1+⊆Sj+S^-_{j-1}\subseteq S^+_{j-1}\subseteq S^+_jSj−1−​⊆Sj−1+​⊆Sj+​, the accuracy bounds ρ(Sj−1+∖Sj−1−)≤4ϵ2ρ(Sj−1−)\rho(S^+_{j-1}\setminus S^-_{j-1})\le4\epsilon^2\rho(S^-_{j-1})ρ(Sj−1+​∖Sj−1−​)≤4ϵ2ρ(Sj−1−​) and the same for www, a cardinality constraint linking sets to events, and three growth conditions on the proxies

αj=ρ(Sj−)1+w(Sj+)\alpha_j=\frac{\rho(S^-_j)}{1+w(S^+_j)}αj​=1+w(Sj+​)ρ(Sj−​)​

depending on the position of ej−1,eje_{j-1},e_jej−1​,ej​ relative to kmidk_{\mathrm{mid}}kmid​. With jmidj_{\mathrm{mid}}jmid​ the last index whose event is at most kmidk_{\mathrm{mid}}kmid​, the actions are rounded into blocks Δ1,…,ΔT\Delta_1,\dots,\Delta_TΔ1​,…,ΔT​ of new items (from Sj−S^-_jSj−​ before jmidj_{\mathrm{mid}}jmid​, from Sj+S^+_jSj+​ after), and the rounded assignment A~\tilde{\mathcal A}A~ lists the blocks in order, each by non-increasing price. The block boundaries are e~j=∣Δ1∪⋯∪Δj∣\tilde e_j=|\Delta_1\cup\dots\cup\Delta_j|e~j​=∣Δ1​∪⋯∪Δj​∣, and I~j\tilde I_jI~j​ are the position intervals between consecutive boundaries, split at kmidk_{\mathrm{mid}}kmid​.

Formalization targets

Goal: the rounded assignment dominates the DP proxies

For every 1≤kmid≤n−11\le k_{\mathrm{mid}}\le n-11≤kmid​≤n−1, every feasible action sequence and every rounded assignment A~\tilde{\mathcal A}A~,

R(A~) ≥ (1−8ϵ)(∑j=1jmidλ(I~j)min⁡{αj,αj+1}+∑j=jmid+1Tλ(I~j)min⁡{αj−1,αj}),\mathcal R(\tilde{\mathcal A})\ \ge\ (1-8\epsilon)\left(\sum_{j=1}^{j_{\mathrm{mid}}}\lambda(\tilde I_j)\min\{\alpha_j,\alpha_{j+1}\}+\sum_{j=j_{\mathrm{mid}}+1}^{T}\lambda(\tilde I_j)\min\{\alpha_{j-1},\alpha_j\}\right),R(A~) ≥ (1−8ϵ)(j=1∑jmid​​λ(I~j​)min{αj​,αj+1​}+j=jmid​+1∑T​λ(I~j​)min{αj−1​,αj​}),

with λ(J)=∑k∈Jλk\lambda(J)=\sum_{k\in J}\lambda_kλ(J)=∑k∈J​λk​. This is inequality (15) of the paper combined with (16), in the proof of Lemma 5.4.

Milestones

  1. The MNL identity R(S∪{i})=R(S)1+w(S)1+w(S)+wi+riwi1+w(S)+wiR(S\cup\{i\})=R(S)\frac{1+w(S)}{1+w(S)+w_i}+r_i\frac{w_i}{1+w(S)+w_i}R(S∪{i})=R(S)1+w(S)+wi​1+w(S)​+ri​1+w(S)+wi​wi​​ for i∉Si\notin Si∈/S (§3.1).
  2. A~[e~j]⊆Sj+\tilde{\mathcal A}[\tilde e_j]\subseteq S^+_jA~[e~j​]⊆Sj+​ (proof of Lemma 5.3), and Lemma 5.3: w(A~[e~j])≤w(Sj+)w(\tilde{\mathcal A}[\tilde e_j])\le w(S^+_j)w(A~[e~j​])≤w(Sj+​).
  3. Lemma 5.2: ρ(A~[e~j])≥(1−8ϵ)ρ(Sj−)\rho(\tilde{\mathcal A}[\tilde e_j])\ge(1-8\epsilon)\rho(S^-_j)ρ(A~[e~j​])≥(1−8ϵ)ρ(Sj−​).
  4. Inequality (16): min⁡{Re~j(A~),Re~j+1(A~)}≥(1−8ϵ)min⁡{αj,αj+1}\min\{R_{\tilde e_j}(\tilde{\mathcal A}),R_{\tilde e_{j+1}}(\tilde{\mathcal A})\}\ge(1-8\epsilon)\min\{\alpha_j,\alpha_{j+1}\}min{Re~j​​(A~),Re~j+1​​(A~)}≥(1−8ϵ)min{αj​,αj+1​}.
  5. Claim 5.5: k↦Rk(A~)k\mapsto R_k(\tilde{\mathcal A})k↦Rk​(A~) is unimodal on each [e~j,e~j+1][\tilde e_j,\tilde e_{j+1}][e~j​,e~j+1​].

Significance

The goal is the step that converts the dynamic program's value into a revenue guarantee for an actual assignment: whatever action sequence the dynamic program returns, the assignment built from it earns at least (1−8ϵ)(1-8\epsilon)(1−8ϵ) times the interval-weighted minima of the program's proxies. Any repaired analysis of the scheme has to pass through a statement of this form, since the rounding of §4.4 is the only link between the program's actions and a display.

The remaining half of the paper's argument is not true as printed. Lemma 5.4, R(A~)≥(1−15ϵ)R(A∗)\mathcal R(\tilde{\mathcal A})\ge(1-15\epsilon)\mathcal R(\mathcal A^*)R(A~)≥(1−15ϵ)R(A∗), and with it the approximation clause of Theorem 1.1, fail for the paper's own algorithm: with n=4n=4n=4, w=(32,1,32,4)w=(32,1,32,4)w=(32,1,32,4), ρ=(4,16,64,8)\rho=(4,16,64,8)ρ=(4,16,64,8), λ=(0.85,0.45,0.40,0.34)\lambda=(0.85,0.45,0.40,0.34)λ=(0.85,0.45,0.40,0.34) and ϵ=1/80\epsilon=1/80ϵ=1/80, no feasible action sequence can place item 2 first, and every rounded assignment earns at most 75364/16625≈4.5375364/16625\approx4.5375364/16625≈4.53 against an optimum of 165804/16625≈9.97165804/16625\approx9.97165804/16625≈9.97. A formal proof of the true half isolates precisely where the published argument stops working. No part of this chain has a machine-checked proof.

Difficulty

The rounding discards items. Before jmidj_{\mathrm{mid}}jmid​, block Δj\Delta_jΔj​ keeps only the part of the sub-assortment Sj−S^-_jSj−​ that is new with respect to Sj−1+S^+_{j-1}Sj−1+​, so the prefix of A~\tilde{\mathcal A}A~ can carry less ρ\rhoρ-mass than Sj−S^-_jSj−​. A loss bounded by the per-step accuracy 4ϵ24\epsilon^24ϵ2 would accumulate over up to nnn steps; Lemma 5.2's constant 1−8ϵ1-8\epsilon1−8ϵ is independent of TTT, and holds only because the growth constraint forces ρ(Sj−)\rho(S^-_j)ρ(Sj−​) to grow geometrically, which the obvious step-by-step bound does not use. The second obstacle is that the revenue between two block boundaries is not monotone; bounding it by the boundary values requires the unimodality of Claim 5.5, which depends on the price order inside each block and on the MNL convex-combination structure, not on the dynamic program.

Formalization scope

Items are Fin n; positions and DP indices are 1-based natural numbers as on the page, and an assignment is an equivalence Fin n ≃ Fin n from the 0-based position k−1k-1k−1 to the item at position kkk. A DP sequence stores events and set pairs as functions on ℕ, read through accessors implementing the root convention eT+1=eTe_{T+1}=e_TeT+1​=eT​, S⃗T+1=S⃗T\vec S_{T+1}=\vec S_TST+1​=ST​ and S0+=∅S^+_0=\emptysetS0+​=∅. Feasibility is exactly the boundary and root conditions plus (8)–(14), with (11) written without natural-number truncation and (14) in the lower-bound form printed on p. 19. The rounded assignment is a predicate: block contents fixed by Δj\Delta_jΔj​, non-increasing prices within a block, ties in any order.

Conventions and additions relative to the page:

  • 1≤kmid≤n−11\le k_{\mathrm{mid}}\le n-11≤kmid​≤n−1 is assumed. For kmid=nk_{\mathrm{mid}}=nkmid​=n the construction of §4.4 can leave an item unplaced, so no rounded assignment exists and the statement would be vacuous.
  • The approximate assortments range over all subsets of [n][n][n] rather than the families of Lemma 2.5, events may repeat, and Assumptions 2.1–2.2 enter only as positivity of prices and weights. Each of these makes the statements stronger.
  • Every statement quantifies over all feasible action sequences, not only the optimal one.
  • Theorem 1.1, Lemma 5.4, Lemma 5.1 and inequalities (17)–(19) are not formalized, because they fail for the paper's algorithm (counterexample above).

Feasibility and rounding are the page's constructions; neither predicate builds in Lemma 5.2, Lemma 5.3 or any revenue property, so the goal cannot be obtained by unfolding a hypothesis. A sorry-free sanity check exhibits an instance (n=3n=3n=3, kmid=2k_{\mathrm{mid}}=2kmid​=2) satisfying all hypotheses at once.

The development needs only finite sums over Finset, real arithmetic and induction over the block index. Contributions of all milestones are welcome; the identity and Claim 5.5 are reusable for any MNL ranking or display model.

Selected references

  • A. Aouad and D. Segev, Display Optimization for Vertically Differentiated Locations Under Multinomial Logit Preferences, Management Science 67(6):3519–3550, 2021; authors' version of 31/07/2019, SSRN 2709652. https://ssrn.com/abstract=2709652 — DOI https://doi.org/10.1287/mnsc.2020.3664
8 thms2 active usersReviewed
AnalysisFunctional AnalysisMathematical Physics·Captain: mikedeng1

Self-adjoint differential operators assosiated with self-adjoint differential expressions: Self-Adjoint Extensions Are Restrictions of the Adjoint Cut Out by m Asymmetry-Form ConditionsResearch Paper

Why self-adjoint extensions

In quantum mechanics an observable is a self-adjoint operator, not just a symmetric one. A differential expression such as −d2/dx2-d^2/dx^2−d2/dx2 on an interval or a half-line first defines a symmetric operator on smooth functions with compact support, and this operator usually has many self-adjoint extensions or none. Each extension is a different physical theory, with its own spectrum and dynamics, and choosing one amounts to choosing boundary conditions. Voronov, Gitman and Tyutin (arXiv:quant-ph/0603187) give a self-contained account of this problem written for physicists. Its abstract result is a description of all self-adjoint extensions that does not require computing the deficient subspaces.

Timeline. von Neumann (1929–30) classified the self-adjoint extensions of a closed symmetric operator through isometries between its deficient subspaces. The classical treatments are Akhiezer–Glazman and Naimark (Linear Differential Operators), and the Cayley-transform form is in Teschl's Mathematical Methods in Quantum Mechanics (2009), Theorem 2.26. Voronov, Gitman and Tyutin (2006) restate the finite-index case as a restriction of the adjoint by asymmetry-form conditions (their Theorem 3, (35)). They then remove the deficient subspaces from the description altogether (Theorem 15). For differential operators this gives self-adjoint boundary conditions in terms of boundary forms (Theorem 16).

Setting

Let H\mathcal HH be a complex Hilbert space whose inner product (⋅,⋅)(\cdot,\cdot)(⋅,⋅) is linear in the second argument. Let f^\hat ff^​ be a linear operator with domain Df⊆HD_f\subseteq\mathcal HDf​⊆H. It is symmetric if DfD_fDf​ is dense and (η,f^ξ)=(f^η,ξ)(\eta,\hat f\xi)=(\hat f\eta,\xi)(η,f^​ξ)=(f^​η,ξ) for all ξ,η∈Df\xi,\eta\in D_fξ,η∈Df​. It then has an adjoint f^+\hat f^{+}f^​+ extending it and a closure fˉ\bar ffˉ​ with domain DfˉD_{\bar f}Dfˉ​​, and f^⊆fˉ⊆f^+\hat f\subseteq\bar f\subseteq\hat f^+f^​⊆fˉ​⊆f^​+. An operator g^\hat gg^​ is self-adjoint if g^+=g^\hat g^{+}=\hat gg^​+=g^​, domains included.

The deficient subspaces are D+=ker⁡(f^+−i)D_+=\ker(\hat f^{+}-i)D+​=ker(f^​+−i) and D−=ker⁡(f^++i)D_-=\ker(\hat f^{+}+i)D−​=ker(f^​++i). The deficiency indices are m±=dim⁡D±m_\pm=\dim D_\pmm±​=dimD±​.

The asymmetry form of the adjoint is the sesquilinear form on Df+D_{f^+}Df+​

ω∗(η∗,ξ∗)=(η∗,f^+ξ∗)−(f^+η∗,ξ∗).\omega_*(\eta_*,\xi_*)=(\eta_*,\hat f^{+}\xi_*)-(\hat f^{+}\eta_*,\xi_*).ω∗​(η∗​,ξ∗​)=(η∗​,f^​+ξ∗​)−(f^​+η∗​,ξ∗​).

It vanishes identically exactly when f^+\hat f^{+}f^​+ is symmetric.

Vectors w1,…,wm∈Df+w_1,\dots,w_m\in D_{f^+}w1​,…,wm​∈Df+​ are linearly independent modulo DfˉD_{\bar f}Dfˉ​​ if ∑kckwk∈Dfˉ\sum_kc_kw_k\in D_{\bar f}∑k​ck​wk​∈Dfˉ​​ forces c1=⋯=cm=0c_1=\dots=c_m=0c1​=⋯=cm​=0. Given such vectors, f^U\hat f_Uf^​U​ denotes the restriction of f^+\hat f^{+}f^​+ to their joint ω∗\omega_*ω∗​-annihilator:

f^U:DfU={ψ∈Df+: ω∗(wk,ψ)=0, k=1,…,m},f^Uψ=f^+ψ.\hat f_U:\quad D_{f_U}=\{\psi\in D_{f^+}:\ \omega_*(w_k,\psi)=0,\ k=1,\dots,m\},\qquad \hat f_U\psi=\hat f^{+}\psi .f^​U​:DfU​​={ψ∈Df+​: ω∗​(wk​,ψ)=0, k=1,…,m},f^​U​ψ=f^​+ψ.

Formalization targets

Goal: Theorem 15 (p. 68)

Assume m+=m−=mm_+=m_-=mm+​=m−​=m with 0<m<∞0<m<\infty0<m<∞. Then

{g^: f^⊆g^=g^+}={f^U : w1,…,wm∈Df+ linearly independent mod Dfˉ,  ω∗(wk,wl)=0 ∀k,l}.\{\hat g:\ \hat f\subseteq\hat g=\hat g^{+}\}=\Big\{\hat f_U\ :\ w_1,\dots,w_m\in D_{f^+}\ \text{linearly independent mod } D_{\bar f},\ \ \omega_*(w_k,w_l)=0\ \forall k,l\Big\}.{g^​: f^​⊆g^​=g^​+}={f^​U​ : w1​,…,wm​∈Df+​ linearly independent mod Dfˉ​​,  ω∗​(wk​,wl​)=0 ∀k,l}.

Both inclusions are part of the goal: every self-adjoint extension arises from such a family, and every such family gives a self-adjoint extension.

Milestones, in attack order

  • Sec. 2.2 (p. 8): ℵz=(Rf−zI)⊥=(Rfˉ−zI)⊥=ker⁡(f^+−zˉ)\aleph_z=(R_{f-zI})^\perp=(R_{\bar f-zI})^\perp=\ker(\hat f^+-\bar z)ℵz​=(Rf−zI​)⊥=(Rfˉ​−zI​)⊥=ker(f^​+−zˉ).
  • Theorem 1 (p. 8), the first von Neumann theorem: Df+=Dfˉ∔ker⁡(f^+−z)∔ker⁡(f^+−zˉ)D_{f^+}=D_{\bar f}\dotplus\ker(\hat f^+-z)\dotplus\ker(\hat f^+-\bar z)Df+​=Dfˉ​​∔ker(f^​+−z)∔ker(f^​+−zˉ) for Im⁡z≠0\operatorname{Im}z\ne0Imz=0, with the action of f^+\hat f^+f^​+ on the components.
  • (13) (p. 11): Dfˉ={ψ∈Df+:ω∗(ξ∗,ψ)=0 ∀ξ∗∈Df+}D_{\bar f}=\{\psi\in D_{f^+}:\omega_*(\xi_*,\psi)=0\ \forall\xi_*\in D_{f^+}\}Dfˉ​​={ψ∈Df+​:ω∗​(ξ∗​,ψ)=0 ∀ξ∗​∈Df+​}.
  • (18)–(19) (p. 12): ω∗(η∗,ξ∗)=(z−zˉ)[(ηz,ξz)−(ηzˉ,ξzˉ)]\omega_*(\eta_*,\xi_*)=(z-\bar z)[(\eta_z,\xi_z)-(\eta_{\bar z},\xi_{\bar z})]ω∗​(η∗​,ξ∗​)=(z−zˉ)[(ηz​,ξz​)−(ηzˉ​,ξzˉ​)].
  • Theorem 3, existence (p. 19): self-adjoint extensions exist iff m+=m−m_+=m_-m+​=m−​. This one is already proved on the platform and is referenced.
  • Theorem 3, (33)–(35) (p. 20): for U∈U(m)U\in U(m)U∈U(m) and eU,k=e+,k+∑lUlke−,le_{U,k}=e_{+,k}+\sum_lU_{lk}e_{-,l}eU,k​=e+,k​+∑l​Ulk​e−,l​, the self-adjoint extensions are exactly the operators cut out by the eU,ke_{U,k}eU,k​, and distinct UUU give distinct extensions.
  • (141) (p. 65) and (142)–(143) (p. 66): the eU,ke_{U,k}eU,k​ are admissible, and admissibility and the cut-out operator are invariant under wk↦∑aXakwa+ξ‾kw_k\mapsto\sum_aX_{ak}w_a+\underline\xi_kwk​↦∑a​Xak​wa​+ξ​k​ with det⁡X≠0\det X\ne0detX=0 and ξ‾k∈Dfˉ\underline\xi_k\in D_{\bar f}ξ​k​∈Dfˉ​​.
  • Proof of Theorem 15, pp. 67–68: for admissible wk=∑aXake+,a+∑aYake−,a+ξ‾kw_k=\sum_aX_{ak}e_{+,a}+\sum_aY_{ak}e_{-,a}+\underline\xi_kwk​=∑a​Xak​e+,a​+∑a​Yak​e−,a​+ξ​k​, both XXX and YYY are nonsingular and YX−1YX^{-1}YX−1 is unitary.

Significance

The result. Theorem 15 lists all self-adjoint extensions of f^\hat ff^​ as solutions of mmm linear conditions on Df+D_{f^+}Df+​. The vectors wkw_kwk​ can be any vectors of the adjoint's domain satisfying two checkable conditions. For a differential operator, ω∗\omega_*ω∗​ reduces to a boundary form [wk,ψ]∣ab[w_k,\psi]\big|_a^b[wk​,ψ]​ab​, and Theorem 16 of the paper turns Theorem 15 into a recipe for self-adjoint boundary conditions that never solves f^+ψ=±iψ\hat f^{+}\psi=\pm i\psif^​+ψ=±iψ. In von Neumann's parametrization that equation must be solved, and doing so is often the hardest part of a concrete calculation. The price is redundancy: families related by a nonsingular matrix give the same extension.

Formalizing it. The mathematics is known: von Neumann's theory is classical and Theorem 15 is proved on pp. 65–68. The Prove2Me platform has Teschl's Cayley-transform version of the existence criterion as a machine-checked proof. To our knowledge, the first von Neumann formula for LinearPMap, the asymmetry-form description of the closure, and the unitary-matrix parametrization are not formalized in Mathlib or on the platform. This mission produces those statements, together with Theorem 15 itself.

Difficulty

The forward direction rests on the unitary parametrization of Theorem 3, which in turn rests on the direct-sum decomposition of Df+D_{f^+}Df+​. Each of these steps requires working with DfˉD_{\bar f}Dfˉ​​ rather than DfD_fDf​, because f^\hat ff^​ need not be closed. The converse is the substantial part. Linear independence modulo DfˉD_{\bar f}Dfˉ​​ and isotropy ω∗(wk,wl)=0\omega_*(w_k,w_l)=0ω∗​(wk​,wl​)=0 are conditions on the wkw_kwk​ as whole vectors. They say nothing directly about the deficient components, and relating an arbitrary admissible family to the deficient-subspace description of Theorem 3 is where the work lies. A count of dimensions alone does not give self-adjointness. Showing that a restriction of f^+\hat f^+f^​+ is symmetric is easy; showing that its adjoint is no larger than itself is not.

Formalization scope

  • H\mathcal HH is a complex Hilbert space (InnerProductSpace ℂ H, CompleteSpace H), and operators are LinearPMaps H →ₗ.[ℂ] H. The adjoint, closure, extension order and self-adjointness are Mathlib's f.adjoint, f.closure, f ≤ g and IsSelfAdjoint g (g† = g). Mathlib's inner product is conjugate-linear in the first slot, as in the paper.
  • Symmetry is the published TeschlQM.Shared.IsSymmetric, which includes density. The initial operator is not assumed closed.
  • Deficient subspaces are kernels of the adjoint at z=iz=iz=i: kerAdd f.adjoint (-I) =ker⁡(f+−i)=\ker(f^+-i)=ker(f+−i) and kerAdd f.adjoint I =ker⁡(f++i)=\ker(f^++i)=ker(f++i), from the published TeschlQM.SelfAdjoint.addScalar. The index hypotheses are Module.finrank … = m with 0 < m, which forces both indices to be finite. Theorem 1 and (18)–(19) keep a general zzz with Im⁡z≠0\operatorname{Im}z\ne0Imz=0, as the paper does.
  • ω∗\omega_*ω∗​ (asymForm) is defined only on f.adjoint.domain. Families are indexed by Fin m. Linear independence is modulo f.closure.domain. The operator (144) is cutOut f w, which is f.adjoint restricted to the annihilator.
  • The goal is not trivialized by its encoding. The extension in (144) is f^+\hat f^+f^​+ restricted to an explicitly defined subspace, not an operator chosen to fit. The conclusion is genuine self-adjointness, g†=gg^\dagger=gg†=g, not symmetry on the cut-out domain. Without the hypothesis m>0m>0m>0, an index with infinite-dimensional deficient subspaces would satisfy finrank = 0, so that hypothesis is kept.
  • A complete development needs the following: the first von Neumann formula for unbounded LinearPMaps; closures of symmetric operators; the identity Ran⁡(f−z)⊥=ker⁡(f+−zˉ)\operatorname{Ran}(f-z)^\perp=\ker(f^+-\bar z)Ran(f−z)⊥=ker(f+−zˉ); and the unitary-matrix parametrization. These are reusable beyond this mission, for example for Sturm–Liouville realizations and Theorem 16 of the paper. Contributions of any of them are welcome, as are proofs routed through the published Cayley-transform results.

Selected references

  • B. L. Voronov, D. M. Gitman, I. V. Tyutin, Self-adjoint differential operators assosiated with self-adjoint differential expressions, preprint, 2006. https://arxiv.org/abs/quant-ph/0603187 (v2 is the cited version)
  • J. von Neumann, Allgemeine Eigenwerttheorie Hermitescher Funktionaloperatoren, Math. Ann. 102 (1930), 49–131. https://doi.org/10.1007/BF01782338
  • N. I. Akhiezer, I. M. Glazman, Theory of Linear Operators in Hilbert Space, Dover, 1993 (reprint of the 1961/1963 translation).
  • M. A. Naimark, Linear Differential Operators, Part II, Ungar, 1968.
  • G. Teschl, Mathematical Methods in Quantum Mechanics, Graduate Studies in Mathematics 99, AMS, 2009, Theorem 2.26. https://doi.org/10.1090/gsm/099
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Algorithmic Game TheoryEconomicsOperations Research·Captain: mikedeng1

The Folk Theorem for Repeated Games with Time-Dependent Discounting: Subgame Perfect Equilibrium Payoffs Converge to the Feasible and Individually Rational Set as Players Become PatientResearch Paper

Motivation

Repeated games model long-run relationships: the same players meet stage after stage, observe what was played, and can condition today's behavior on the past. The folk theorem describes what such relationships can sustain. When players are patient, every payoff vector that is feasible and gives each player at least what the others can force on them is the payoff of an equilibrium, and the equilibrium can be chosen subgame perfect, so that every threatened punishment is itself credible. Economics, operations research and computer science use the result to explain cooperation and collusion and to reason about long-term contracts and repeated auctions.

The classical statement assumes stationary discounting: a payoff at stage ttt is worth δt−1\delta^{t-1}δt−1 of a payoff today, and "patient" means δ→1\delta\to1δ→1. Experimental and behavioral evidence points instead to discount rates that change over time (hyperbolic and quasi-hyperbolic discounting), and planning problems with a finite or decaying horizon have weights that are not geometric at all. X. Li (later with D. Kim) asks whether the perfect folk theorem survives when the weight of stage ttt is an arbitrary decreasing sequence, and gives a patience condition under which it does.

Timeline.

  • 1986. Fudenberg and Maskin prove the perfect folk theorem for discounted repeated games with at least three players under a full-dimensionality condition on the feasible and individually rational set (Econometrica 54).
  • 1986. Sorin shows that any feasible payoff can be written as a discounted sum of pure-action payoffs once δ\deltaδ is large, which removes the need for public randomization on the equilibrium path (Math. Oper. Res. 11).
  • 1991. Fudenberg and Maskin use such decompositions to dispense with public randomization in the perfect folk theorem.
  • 2019–2021. Li (SSRN 3407197) and Kim and Li (Math. Oper. Res., 2021) extend the asymptotic perfect folk theorem to time-dependent discounting.

The repeated game with time-dependent discounting

A finite set III of players plays a stage game repeatedly. Player iii has a finite action set AiA^iAi, A=∏iAiA=\prod_iA^iA=∏i​Ai, and g=(gi)i∈I:A→RIg=(g^i)_{i\in I}:A\to\mathbb R^Ig=(gi)i∈I​:A→RI gives the stage payoffs. At each stage t≥1t\ge1t≥1 every player observes the past actions (a1,…,at−1)(a_1,\dots,a_{t-1})(a1​,…,at−1​) and chooses an action, possibly at random. A behavior strategy σi\sigma^iσi assigns a mixed action to every finite history, and a profile σ\sigmaσ determines a distribution over infinite plays.

An evaluation is a sequence θ=(θt)t≥1\theta=(\theta_t)_{t\ge1}θ=(θt​)t≥1​ in [0,1][0,1][0,1] that is decreasing and sums to one; the payoff of σ\sigmaσ is

γθ(σ)=Eσ[∑t≥1θt g(at)].\gamma_\theta(\sigma)=\mathbb E_\sigma\Big[\sum_{t\ge1}\theta_t\,g(a_t)\Big].γθ​(σ)=Eσ​[t≥1∑​θt​g(at​)].

Stationary discounting is θt=(1−δ)δt−1\theta_t=(1-\delta)\delta^{t-1}θt​=(1−δ)δt−1. After a history of T−1T-1T−1 stages the remaining game is evaluated by the continuation evaluation θt[T]=θT−1+t/∑s≥Tθs\theta_t[T]=\theta_{T-1+t}/\sum_{s\ge T}\theta_sθt​[T]=θT−1+t​/∑s≥T​θs​; unlike the stationary case, θ[T]\theta[T]θ[T] depends on TTT. A profile is a subgame perfect equilibrium of Γθ\Gamma_\thetaΓθ​ if, after every history hTh_ThT​, the induced profile is a Nash equilibrium of the subgame Γθ[T](hT)\Gamma_{\theta[T]}(h_T)Γθ[T]​(hT​). Eθ⊆RIE_\theta\subseteq\mathbb R^IEθ​⊆RI is the set of subgame perfect equilibrium payoffs.

The minmax level of player iii is

vi=min⁡s∈∏j≠iΔ(Aj) max⁡ai∈Ai ∑a−is(a−i) gi(ai,a−i),v^i=\min_{s\in\prod_{j\ne i}\Delta(A^j)}\ \max_{a^i\in A^i}\ \sum_{a^{-i}}s(a^{-i})\,g^i(a^i,a^{-i}),vi=s∈∏j=i​Δ(Aj)min​ ai∈Aimax​ a−i∑​s(a−i)gi(ai,a−i),

the lowest payoff the others can hold iii to by mixing independently. S=co⁡{g(a):a∈A}S=\operatorname{co}\{g(a):a\in A\}S=co{g(a):a∈A} is the set of feasible payoffs and F={x∈S:xi≥vi ∀i}\mathcal F=\{x\in S:x^i\ge v^i\ \forall i\}F={x∈S:xi≥vi ∀i} the set of feasible and individually rational payoffs.

A sequence of evaluations (θk)k≥1(\theta^k)_{k\ge1}(θk)k≥1​ is patient if θtk/θt+1k→1\theta^k_t/\theta^k_{t+1}\to1θtk​/θt+1k​→1 as k→∞k\to\inftyk→∞, uniformly in ttt.

Formalization targets

Goal: Theorem 3.1 (Asymptotic Perfect Folk Theorem)

If int⁡F≠∅\operatorname{int}\mathcal F\ne\emptysetintF=∅ and (θk)(\theta^k)(θk) is patient, then

Eθk→k→∞Fin the Hausdorff distance.E_{\theta^k}\xrightarrow[k\to\infty]{}\mathcal F\quad\text{in the Hausdorff distance.}Eθk​k→∞​Fin the Hausdorff distance.

The goal fixes no rate and no constants; it asserts only the limit.

Milestones

  • Lemma 4.1: patience is equivalent to ∑t=TT+T1θtk/∑t=TT+T2θtk→(T1+1)/(T2+1)\sum_{t=T}^{T+T_1}\theta^k_t\big/\sum_{t=T}^{T+T_2}\theta^k_t\to(T_1+1)/(T_2+1)∑t=TT+T1​​θtk​/∑t=TT+T2​​θtk​→(T1​+1)/(T2​+1) uniformly in TTT.
  • Lemma 4.2: for patient (θk)(\theta^k)(θk), θ1k[T]→0\theta^k_1[T]\to0θ1k​[T]→0 and θtk[T]/θt+1k[T]→1\theta^k_t[T]/\theta^k_{t+1}[T]\to1θtk​[T]/θt+1k​[T]→1, uniformly in TTT and ttt.
  • Claim 7.1 and Lemma 4.4: a perturbed decomposition x=∑mθmkxφ(m)′x=\sum_m\theta^k_m x'_{\varphi(m)}x=∑m​θmk​xφ(m)′​ with each xφ(m)′x'_{\varphi(m)}xφ(m)′​ near a vertex.
  • Proposition 4.3, and its form for the continuation evaluations θk[T]\theta^k[T]θk[T]: every x∈Fx\in\mathcal Fx∈F is the θk\theta^kθk-payoff of a pure path along which all continuation payoffs stay within η\etaη of xxx.
  • (5.1), Lemma 5.1, Lemma 5.2: the punishment length and the bounds that make punishments and rewards consistent.
  • The one-shot deviation principle under general discounting (§5.1 Part C, footnote 12).
  • Interior payoffs are equilibrium payoffs: every x∈int⁡Fx\in\operatorname{int}\mathcal Fx∈intF lies in EθkE_{\theta^k}Eθk​ for all large kkk.

Significance

The result. The theorem says that the set of credible long-run outcomes is the same under any patient time-dependent discounting as under stationary discounting with δ→1\delta\to1δ→1. Quasi-hyperbolic (β,δ)(\beta,\delta)(β,δ) preferences with β,δ→1\beta,\delta\to1β,δ→1 and discount factors that vary by stage are special cases. Patience is stated through ratios of consecutive weights. The paper notes that this condition does not cover TTT-stage averages with T→∞T\to\inftyT→∞, where the folk theorem is known to need extra assumptions. The equilibria use pure paths, with no public randomization.

Formalizing it. The result is proved in the paper; no part of it has a machine-checked proof. The mission builds a reusable Lean model of discounted repeated games with perfect monitoring: behavior strategies, the induced distribution over finite histories, continuation games, subgame perfection, minmax levels and the feasible and individually rational set. It then states the theorem and the lemmas of its proof. The one-shot deviation principle under general discounting and the pure-path decomposition (Proposition 4.3) are standard tools that the literature usually cites without proof, and both are useful well beyond this paper.

Difficulty

The stationary proof relies on the fact that every subgame looks like the original game: θ[T]=θ\theta[T]=\thetaθ[T]=θ. Under time-dependent discounting the continuation evaluation changes with the starting stage. A punishment phase of fixed length therefore carries a different weight depending on when it starts, and the number of stages needed to deter a deviation depends on the stage. Two consequences make the obvious adaptation fail. First, a deviation during a punishment starts a new punishment whose length differs from the remaining length of the old one, so the incentive check splits into cases (Lemma 5.2). Second, the pure paths that deliver the reward payoffs have to work for every continuation evaluation at once, which needs the uniformity statements of Lemma 4.2 and the perturbed decomposition of Lemma 4.4. Replacing each continuation evaluation by a geometric one does not work, because nothing forces the weights of a patient sequence to be close to geometric.

Formalization scope

All declarations live in the namespace TimeDepFolk.Asymptotic. Stages are 0-based: Lean stage sss is the paper's t=s+1t=s+1t=s+1, a history of nnn played stages is Fin n → (∀ i, A i), and cont θ n is the paper's θ[n+1]\theta[n+1]θ[n+1], which is 000 when the tail sum vanishes. Mixed actions are lotteries (AGT.IsLottery) and the minmax level uses AGT.expectedPayoff from the published definition agt_games, with independent mixing by the others. Action sets are finite, so expectations are finite sums over histories and the payoff is the series ∑sθs Eσ[g(as)]\sum_s\theta_s\,\mathbb E_\sigma[g(a_s)]∑s​θs​Eσ​[g(as​)]; no measure theory is needed. Payoff vectors live in I → ℝ with the sup norm. Subgame perfection quantifies over all histories, the empty history included, and over all behavior-strategy deviations; the one-shot reduction is a milestone to prove, not part of the definition. The player set and every action set are finite and nonempty. "int⁡F\operatorname{int}\mathcal FintF nonempty and fully dimensional" is (interior (F g)).Nonempty.

The goal uses the extended-valued Hausdorff distance Metric.hausdorffEDist. The real-valued Metric.hausdorffDist is 000 when one set is empty, so a goal stated with it would hold vacuously for every kkk at which no equilibrium is known; the extended version makes nonemptiness of EθkE_{\theta^k}Eθk​ part of the claim. Stating the goal for a single payoff, with Nash instead of subgame perfect equilibrium, or with Theorem 3.2's discount factors in place of evaluations would each prove a different and weaker theorem.

A complete development needs the probability of finite histories under behavior strategies, the decomposition of the payoff into the first stage and the continuation, the one-shot deviation principle, Carathéodory's theorem (in Mathlib), and the barycentric sensitivity of Claim 7.1. The repeated-game layer and the one-shot deviation principle can be reused for any discounted repeated game with perfect monitoring. Contributions to any milestone, and alternative proofs of the decomposition results, are welcome.

Selected references

  • X. Li, The folk theorem for repeated games with time-dependent discounting, SSRN Working Paper 3407197, version of August 16, 2019. https://ssrn.com/abstract=3407197
  • D. Kim and X. Li, The folk theorem for repeated games with time-dependent discounting, Mathematics of Operations Research, 2021. https://doi.org/10.1287/moor.2021.1183
  • D. Fudenberg and E. Maskin, The folk theorem in repeated games with discounting or with incomplete information, Econometrica 54(3), 1986. https://doi.org/10.2307/1911307
  • S. Sorin, On repeated games with complete information, Mathematics of Operations Research 11(1), 1986. https://doi.org/10.1287/moor.11.1.147
  • G. J. Mailath and L. Samuelson, Repeated Games and Reputations: Long-Run Relationships, Oxford University Press, 2006. https://doi.org/10.1093/acprof:oso/9780195300796.001.0001
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Algorithmic Game TheoryLinear algebraOperations Research·Captain: mikedeng1

Technical Note—Global Robust Stability in a General Price and Assortment Competition Model: Robust Best-Response Price Dynamics Contract Geometrically to the Special Equilibrium from Any StartResearch Paper

Motivation

Retailers that sell many products set prices against one another, and the demand for each product depends on the prices of all of them. Affine demand models, q(p)=a−Rpq(p)=a-Rpq(p)=a−Rp, are the standard starting point for this kind of multi-product price competition in operations management and industrial organization. Two questions follow once an equilibrium is known to exist. Can the firms reach it, and does it matter where they start? A Nash equilibrium that the firms cannot find by adjusting their prices tells little about what prices will actually be observed.

Federgruen and Hu (Operations Research 69(1), 2021; submitted manuscript at SSRN 3010503) answer this for a general multi-firm, multi-product model with an arbitrary number of firms and arbitrary product assortments. The game has features that defeat the usual tools. Once the affine demands are extended so that no demand turns negative, the game is in general not supermodular. Example 1 of the paper, after McGuire and Staelin (1983/2008), is a duopoly that is not supermodular and has a continuum of equilibria. Earlier work (Federgruen and Hu, Operations Research 63(3), 2015) characterized the equilibria. One of them, the special equilibrium (p∗∣w)(p^*|w)(p∗∣w), has a closed form. The 2021 paper shows that this equilibrium is reached from any starting price vector when every firm repeatedly plays a robust best response.

Setting

A finite set N\mathcal NN of products is partitioned among firms. Firm iii sells the products N(i)\mathcal N(i)N(i). The foundational demands are

q(p)=a−Rp,a≥0,q(p)=a-Rp,\qquad a\ge 0,q(p)=a−Rp,a≥0,

where RRR is an N×N\mathcal N\times\mathcal NN×N price-sensitivity matrix subject to three assumptions:

  1. (P) RRR is positive definite in the quadratic-form sense: x⊤Rx>0x^\top Rx>0x⊤Rx>0 for all x≠0x\ne 0x=0. RRR need not be symmetric.
  2. (Z) RRR is a Z-matrix: Rlm≤0R_{lm}\le 0Rlm​≤0 for l≠ml\ne ml=m, so the products are substitutes.
  3. (IS) RRR is symmetric within each firm: Rlm=RmlR_{lm}=R_{ml}Rlm​=Rml​ when l,m∈N(i)l,m\in\mathcal N(i)l,m∈N(i).

Each firm has a cost vector, w∈R++Nw\in\mathbb R^{\mathcal N}_{++}w∈R++N​. Let T(R)T(R)T(R) be the block-diagonal matrix of the transposed firm blocks RN(i),N(i)⊤R^\top_{\mathcal N(i),\mathcal N(i)}RN(i),N(i)⊤​, and let Ψ(R)=T(R)[R+T(R)]−1\Psi(R)=T(R)[R+T(R)]^{-1}Ψ(R)=T(R)[R+T(R)]−1 and Q(w′)=Ψ(R)a−Ψ(R)Rw′Q(w')=\Psi(R)a-\Psi(R)Rw'Q(w′)=Ψ(R)a−Ψ(R)Rw′. The cost projection w′=Θ(w)w'=\Theta(w)w′=Θ(w) solves the linear complementarity problem

w′≤w,Q(w′)⊤(w−w′)=0,Q(w′)≥0,w'\le w,\qquad Q(w')^\top(w-w')=0,\qquad Q(w')\ge 0,w′≤w,Q(w′)⊤(w−w′)=0,Q(w′)≥0,

and the special equilibrium is

(p∗∣w)=w′+[R+T(R)]−1(a−Rw′).(p^*|w)=w'+[R+T(R)]^{-1}(a-Rw').(p∗∣w)=w′+[R+T(R)]−1(a−Rw′).

Given the other firms' prices p−N(i)p_{-\mathcal N(i)}p−N(i)​, firm iii sees the residual intercept α=aN(i)−RN(i),−N(i)p−N(i)\alpha=a_{\mathcal N(i)}-R_{\mathcal N(i),-\mathcal N(i)}p_{-\mathcal N(i)}α=aN(i)​−RN(i),−N(i)​p−N(i)​. Its robust best response maximizes

(x−wN(i))⊤(α−RN(i),N(i)x)over x≥0, α−RN(i),N(i)x≥0.(x-w_{\mathcal N(i)})^\top(\alpha-R_{\mathcal N(i),\mathcal N(i)}x)\quad\text{over } x\ge 0,\ \alpha-R_{\mathcal N(i),\mathcal N(i)}x\ge 0.(x−wN(i)​)⊤(α−RN(i),N(i)​x)over x≥0, α−RN(i),N(i)​x≥0.

Prices are restricted to keep the firm's own affine demands nonnegative, so the firm needs only its own demand and cost data. Collecting all firms gives the map RBRBRB, and RB(n)RB^{(n)}RB(n) is its nnn-fold iterate. Finally, Λ(R)=I−[T(R)]−1R\Lambda(R)=I-[T(R)]^{-1}RΛ(R)=I−[T(R)]−1R.

Formalization targets

Goal: Theorem 3 (global robust stability)

There exist a norm ∥⋅∥\|\cdot\|∥⋅∥ on RN\mathbb R^{\mathcal N}RN and a constant 0<γ<10<\gamma<10<γ<1 such that

∥RB(p^)−RB(p~)∥≤γ∥p^−p~∥(p^,p~≥0),\|RB(\hat p)-RB(\tilde p)\|\le\gamma\|\hat p-\tilde p\|\quad(\hat p,\tilde p\ge 0),∥RB(p^​)−RB(p~​)∥≤γ∥p^​−p~​∥(p^​,p~​≥0), ∥RB(n)(p)−(p∗∣w)∥≤γn∥p−(p∗∣w)∥,lim⁡n→∞RB(n)(p)=(p∗∣w)(p≥0).\|RB^{(n)}(p)-(p^*|w)\|\le\gamma^n\|p-(p^*|w)\|,\qquad \lim_{n\to\infty}RB^{(n)}(p)=(p^*|w)\quad(p\ge 0).∥RB(n)(p)−(p∗∣w)∥≤γn∥p−(p∗∣w)∥,n→∞lim​RB(n)(p)=(p∗∣w)(p≥0).

Neither the norm nor γ\gammaγ is fixed, because the paper asserts only that they exist.

Milestones

The milestones follow the paper's own proof:

  • Lemma 1: RBRBRB is well defined.
  • The proof of Theorem 2: the projection LCP has a unique, nonnegative solution.
  • Theorem 2: (p∗∣w)(p^*|w)(p∗∣w) is a fixed point of RBRBRB.
  • Lemma B.1(a), (c), (e), (f), (g): the M-matrix lemmas.
  • Lemma 2: the per-firm comparison of robust best responses.
  • Three claims from the proof of Theorem 3(a):
    • the componentwise bound ∣RB(p^)−RB(p~)∣≤Λ(R)∣p^−p~∣|RB(\hat p)-RB(\tilde p)|\le\Lambda(R)|\hat p-\tilde p|∣RB(p^​)−RB(p~​)∣≤Λ(R)∣p^​−p~​∣;
    • Λ(R)≥0\Lambda(R)\ge 0Λ(R)≥0 with spectral radius ρ(Λ(R))<1\rho(\Lambda(R))<1ρ(Λ(R))<1;
    • for every ε>0\varepsilon>0ε>0, an absolute norm whose induced norm satisfies ∥Λ(R)∥≤ρ(Λ(R))+ε\|\Lambda(R)\|\le\rho(\Lambda(R))+\varepsilon∥Λ(R)∥≤ρ(Λ(R))+ε.

Significance

Theorem 3 makes the special equilibrium an operational prediction. Firms that adjust prices myopically, each using only its own demand and cost information, converge to (p∗∣w)(p^*|w)(p∗∣w) from any start. The convergence is geometric, so the number of rounds needed to come within ϵ\epsilonϵ grows only logarithmically in the initial distance. This holds although the game is not supermodular and can have infinitely many equilibria, so the lattice-theoretic stability results that cover supermodular games do not apply. Theorem 2 also identifies which of the possibly many equilibria the dynamics select.

The result is proved in the paper, but it has not been formalized. A machine-checked version has two parts: a model layer (affine multi-product demand, the cost projection, robust best responses), and an M-matrix layer (Lemma B.1: inverse-positivity, Schur complements of inverse M-matrices, spectral radius bounds). Mathlib has neither. The proof also rests on results that the paper cites without proof: Propositions 2 and 3 of Federgruen and Hu (2015), and Theorem 4(b) and Lemma B.2(d) of Federgruen and Hu (2016). A formalization has to supply them. In one place the proof cites Horn and Johnson (1985, Lemma 5.6.10) for an absolute norm close to the spectral radius. As stated there, that lemma does not give absoluteness for general matrices: (11−1−1)\begin{pmatrix}1&1\\-1&-1\end{pmatrix}(1−1​1−1​) has spectral radius 000, but every absolute norm gives it induced norm at least 111. The claim holds for the nonnegative matrix Λ(R)\Lambda(R)Λ(R), and the corresponding milestone is stated for that matrix only.

Difficulty

The obvious route is to show that RBRBRB is a contraction in the sup norm and invoke Banach's fixed-point theorem. This fails: ∥Λ(R)∥∞\|\Lambda(R)\|_\infty∥Λ(R)∥∞​ can exceed 111 even though ρ(Λ(R))<1\rho(\Lambda(R))<1ρ(Λ(R))<1, and the bound ∣RB(p^)−RB(p~)∣≤Λ(R)∣p^−p~∣|RB(\hat p)-RB(\tilde p)|\le\Lambda(R)|\hat p-\tilde p|∣RB(p^​)−RB(p~​)∣≤Λ(R)∣p^​−p~​∣ is all the structure gives. The norm must be adapted to Λ(R)\Lambda(R)Λ(R) and must also be absolute, so that the componentwise bound transfers. The per-firm estimate behind that bound (Lemma 2) is itself not a Lipschitz estimate for an explicit formula. The robust best response is the solution of a constrained quadratic program whose active set changes with the competitors' prices, and the comparison goes through a componentwise minimum pˇ=min⁡{p^,p~}\check p=\min\{\hat p,\tilde p\}pˇ​=min{p^​,p~​} and monotonicity in the intercept. Separately, the fixed-point property needs the cost projection Θ(w)\Theta(w)Θ(w), an LCP whose unique solvability and nonnegativity depend on (IS).

Formalization scope

Products form a finite type ι and firms a type F, with firm : ι → F assigning each product to its firm. Vectors are ι → ℝ with the pointwise order. Matrices are Matrix ι ι ℝ, and every matrix inequality is entrywise. The commitments are:

  • (P) is ∀ x ≠ 0, 0 < x ⬝ᵥ R *ᵥ x, not Mathlib's Matrix.PosDef, which would add global symmetry.
  • The special equilibrium (p∗∣w)(p^*|w)(p∗∣w) is written through any solution w′w'w′ of the LCP (12)–(14). The paper says this form is valid for all w>0w>0w>0. A milestone proves that the solution exists, is unique, and is nonnegative.
  • The robust best response is a relation, "qqq is a robust best response to ppp", with the feasibility constraint of (8) built in. Lemma 1 makes it single-valued. Part (b) of the goal is stated for every robust best-response sequence started at p0≥0p^0\ge 0p0≥0.
  • "A norm on RN\mathbb R^{\mathcal N}RN" is a seminorm that vanishes only at 000.
  • The spectral radius is that of the matrix viewed over C\mathbb CC, so complex eigenvalues count.
  • Matrix inverses use Mathlib's ⁻¹. Every inverted matrix is invertible under the hypotheses.

No trivializing reading is available. The norm must be definite, the robust best response keeps its feasibility constraint and is never defined by a closed form, and the convergence statement holds for every iterate. A sorry-free sanity check confirms that the standing assumptions, the cost projection and the fixed-point relation are all satisfiable on a two-firm example.

The following results are not formalized here:

  • Theorem 1 and Proposition 1, which characterize the set of Nash equilibria and the existence of (p∗∣w)(p^*|w)(p∗∣w) under the full LCP-extended demand. They are independent of the goal.
  • Example 1, Lemma B.2, Lemma C.1 and Proposition 2 of Appendix D.

Contributions that would be reusable beyond this mission include:

  • a general M-matrix library (inverse-positivity, Schur complements, Perron–Frobenius bounds);
  • uniqueness for P-matrix LCPs;
  • the existence of absolute norms close to the spectral radius for nonnegative matrices.

Selected references

  • A. Federgruen, M. Hu, Technical Note—Global Robust Stability in a General Price and Assortment Competition Model, Operations Research 69(1) 164–174, 2021. https://doi.org/10.1287/opre.2020.2001 (submitted manuscript: https://ssrn.com/abstract=3010503)
  • A. Federgruen, M. Hu, Multi-Product Price and Assortment Competition, Operations Research 63(3) 572–584, 2015.
  • A. Federgruen, M. Hu, Sequential Multiproduct Price Competition in Supply Chain Networks, Operations Research 64(1) 135–149, 2016.
  • R. A. Horn, C. R. Johnson, Matrix Analysis, Cambridge University Press, 1985; Topics in Matrix Analysis, Cambridge University Press, 1991.
  • I. N. Imam, The Schur complement and the inverse M-matrix problem, Linear Algebra and its Applications 62 235–240, 1984.
  • T. W. McGuire, R. Staelin, An industry equilibrium analysis of downstream vertical integration, Marketing Science 27(1) 115–130, 2008 (reprint of Marketing Science 2(2), 1983).
15 thms2 active usersReviewed
Algorithmic Game TheoryOperations ResearchOptimization·Captain: mikedeng1

Network Pricing: How to Induce Optimal Flows Under Strategic Link Operators: Optimal Tolls Bounded by the Marginal Tolls Are (Strong) Cap EquilibriaResearch Paper

Motivation

Congestion pricing charges road users for the delay they impose on others. The classical theory, going back to Beckmann, McGuire and Winsten (1956), assumes a single benevolent authority that sets every toll: charging each link its marginal toll makes the selfish (Wardrop) traffic pattern socially optimal. Many real networks are different. Roads, bridges and tunnels built under build-operate-transfer schemes are run by private operators who set their own prices to maximize their own revenue. When operators compete, an equilibrium of the pricing game need not exist, need not be unique, and can be far from optimal (Acemoglu and Ozdaglar 2007; Hayrapetyan, Tardos and Wexler 2007).

Correa, Guzmán, Lianeas, Nikolova and Schröder (2021) ask whether a regulator who can only impose price caps — an upper bound tˉe\bar t_etˉe​ on the toll of each link — can steer competing operators to the optimal flow. Their main result, Theorem 1, answers yes: optimal tolls bounded by the marginal tolls, used as caps, are the unique equilibrium of the capped game, even against coalitions of operators. This mission formalizes that theorem and the two monotonicity lemmas it rests on.

Setting

A network has links e∈Ee \in Ee∈E and commodities k∈Kk \in Kk∈K; each commodity has a finite set Pk\mathcal P^kPk of routes, each route being a set of links. Commodity kkk has a maximum demand rk≥0r_k \ge 0rk​≥0 and a nonincreasing, continuous, nonnegative utility function uku_kuk​ on [0,rk][0, r_k][0,rk​]; its aggregate utility is Uk(y)=∫0yuk(s) dsU_k(y) = \int_0^y u_k(s)\,dsUk​(y)=∫0y​uk​(s)ds. Each link has a latency function ℓe\ell_eℓe​ on [0,∞)[0,\infty)[0,∞), nonnegative, nondecreasing, convex and smooth.

A flow assigns xP≥0x_P \ge 0xP​≥0 to each route so that rxk=∑P∈PkxP≤rkr^k_x = \sum_{P \in \mathcal P^k} x_P \le r_krxk​=∑P∈Pk​xP​≤rk​; XXX is the set of flows and xe=∑P∋exPx_e = \sum_{P \ni e} x_Pxe​=∑P∋e​xP​ is the flow on link eee. Under a toll vector t≥0t \ge 0t≥0, users settle in a Wardrop equilibrium, which is a maximizer over XXX of the potential

Φt(x)=∑k∈KUk(rxk)−∑e∈E∫0xe(ℓe(y)+te) dy.(1)\Phi_t(x) = \sum_{k \in K} U_k(r^k_x) - \sum_{e \in E} \int_0^{x_e} \big(\ell_e(y) + t_e\big)\,dy. \qquad (1)Φt​(x)=k∈K∑​Uk​(rxk​)−e∈E∑​∫0xe​​(ℓe​(y)+te​)dy.(1)

The paper restricts to instances where this maximizer is unique (linkwise) for every t≥0t \ge 0t≥0, and writes x(t)x(t)x(t) for it.

The social welfare of a flow is SW(x)=∑kUk(rxk)−∑eℓe(xe) xeSW(x) = \sum_k U_k(r^k_x) - \sum_e \ell_e(x_e)\,x_eSW(x)=∑k​Uk​(rxk​)−∑e​ℓe​(xe​)xe​; an optimal flow x∗x^*x∗ maximizes it over XXX. The marginal tolls are t^e=xe∗ ℓe′(xe∗)\hat t_e = x^*_e\,\ell'_e(x^*_e)t^e​=xe∗​ℓe′​(xe∗​), and a toll vector tˉ\bar ttˉ is optimal if x(tˉ)x(\bar t)x(tˉ) is the optimal flow.

Each link is run by a separate operator, whose profit is πe(t)=te xe(t)\pi_e(t) = t_e\,x_e(t)πe​(t)=te​xe​(t). Given caps tˉ≥0\bar t \ge 0tˉ≥0, operator eee chooses se∈[0,tˉe]s_e \in [0, \bar t_e]se​∈[0,tˉe​]. A profile ttt is a Nash equilibrium of the capped game if no operator gains by a unilateral change within its cap, and a strong Nash equilibrium if no nonempty coalition EΔE^\DeltaEΔ has a joint change, within the caps and confined to EΔE^\DeltaEΔ, that strictly raises the profit of every member. By Definition 1, tˉ\bar ttˉ is a (strong) cap equilibrium if tˉ\bar ttˉ itself is the unique (strong) Nash equilibrium of the game with caps tˉ\bar ttˉ.

Formalization targets

Goal: Theorem 1

If tˉ\bar ttˉ is an optimal toll vector with

tˉe≤t^e=xe∗ ℓe′(xe∗)for all e∈E,\bar t_e \le \hat t_e = x^*_e\,\ell'_e(x^*_e) \quad \text{for all } e \in E,tˉe​≤t^e​=xe∗​ℓe′​(xe∗​)for all e∈E,

then tˉ\bar ttˉ is both a cap equilibrium and a strong cap equilibrium.

Milestones

  1. Continuity (§2.1.2, p. 5). Each link flow t↦xe(t)t \mapsto x_e(t)t↦xe​(t) is continuous on {t≥0}\{t \ge 0\}{t≥0}.
  2. Lemma 1 (p. 6). If 0≤t≤t′0 \le t \le t'0≤t≤t′ and E<={e:te<te′}≠∅E^< = \{e : t_e < t'_e\} \neq \emptysetE<={e:te​<te′​}=∅, there are e1,e2∈E<e_1, e_2 \in E^<e1​,e2​∈E< with xe1(t′)≤xe1(t)x_{e_1}(t') \le x_{e_1}(t)xe1​​(t′)≤xe1​​(t) and [xe2(t′)−xe2(t)][ℓe2(xe2(t′))+te2′−ℓe2(xe2(t))−te2]≤0[x_{e_2}(t') - x_{e_2}(t)][\ell_{e_2}(x_{e_2}(t')) + t'_{e_2} - \ell_{e_2}(x_{e_2}(t)) - t_{e_2}] \le 0[xe2​​(t′)−xe2​​(t)][ℓe2​​(xe2​​(t′))+te2​′​−ℓe2​​(xe2​​(t))−te2​​]≤0.
  3. Lemma 2 (p. 7). If tet_ete​ locally maximizes πe(⋅,t−e)\pi_e(\cdot, t_{-e})πe​(⋅,t−e​), then xe(t) ℓe′(xe(t))≤tex_e(t)\,\ell'_e(x_e(t)) \le t_exe​(t)ℓe′​(xe​(t))≤te​.
  4. Remark 1 / first half of the proof (p. 7). Under the hypotheses of Theorem 1, no coalition has a capped deviation from tˉ\bar ttˉ with πe(t′)≥πe(tˉ)\pi_e(t') \ge \pi_e(\bar t)πe​(t′)≥πe​(tˉ) on the coalition and at least one strict inequality.
  5. Second half of the proof (p. 8). Under the same hypotheses, every Nash equilibrium of the game with caps tˉ\bar ttˉ equals tˉ\bar ttˉ.

Significance

Theorem 1 resolves, for capped games, the problems of existence, uniqueness and inefficiency that the literature on competing link operators identified: the regulator needs only to know the optimal flow and its marginal tolls, and then no operator, and no coalition of operators, has a reason to move away from the optimal tolls. The paper's consumer-surplus comparison (Theorem 2) is a comparison among such great tolls, and its extensions with operating costs, multi-link operators and complementary links (Theorems 3–6) follow the same pattern. The two lemmas are general facts about Wardrop flows under elastic demand — monotonicity in the tolls and a first-order bound at a profit maximum — that are reusable for any toll-setting or pricing question in nonatomic routing.

The result is proved in the paper; none of it is formalized. The mission produces a machine-checked version of the full argument, including the steps the paper states without proof.

Difficulty

The equilibrium flow x(t)x(t)x(t) is defined only implicitly, as the maximizer of a concave potential that depends on the tolls, so every statement about operators' profits is a statement about a parametric optimization problem. Lemma 1 needs first-order optimality conditions of (1) on a polytope of route flows with elastic demand, and continuity needs a maximum-theorem argument in which only the link flows, not the route flows, are unique. Lemma 2 cannot simply differentiate πe\pi_eπe​: xe(t)x_e(t)xe​(t) need not be differentiable in tet_ete​, so the argument must work with one-sided difference quotients. The coalition part of Theorem 1 cannot be reduced to unilateral deviations; a deviation by many operators at once moves the flow on every link of the network simultaneously.

Formalization scope

All declarations live in the namespace NetworkPricing.Caps. Links, routes and commodities are Fin J, Fin R, Fin Sd; link flows are KellyStochasticNetworks.linkFlow of the published definition KellyStochasticNetworks_Wardrop. The model commits to the following conventions:

  • Routes form an abstract finite route system with 0/1 incidence and a commodity per route; the oko_kok​–dkd_kdk​ paths of a graph are an instance, and the proofs never use the graph.
  • uku_kuk​ and ℓe\ell_eℓe​ are functions R→R\mathbb R \to \mathbb RR→R constrained only on [0,rk][0, r_k][0,rk​] and [0,∞)[0, \infty)[0,∞). "Smooth" is read as differentiable on R\mathbb RR, and ℓe′\ell'_eℓe′​ is the derivative.
  • The Wardrop flow is a hypothesis, not a definition: every theorem takes a selection flow with flow t a maximizer of (1) for each t≥0t \ge 0t≥0, together with the paper's uniqueness assumption on link flows.
  • An optimal toll is tˉ≥0\bar t \ge 0tˉ≥0 whose Wardrop flow has the link flows of an optimal flow x∗x^*x∗; t^\hat tt^ is computed from x∗x^*x∗.
  • In the capped game, unilateral and coalition deviations stay in [0,tˉ][0, \bar t][0,tˉ], and coalitions are nonempty (with the empty coalition the page's formula would rule out every profile). Local optimality in Lemma 2 is relative to tolls se≥0s_e \ge 0se​≥0.
  • "(strong) cap equilibrium" in Theorem 1 is the conjunction of both notions.

Formalizations that make the goal trivial are ruled out: x(t)x(t)x(t) must maximize the potential (1), not be an arbitrary function of ttt; uniqueness of the equilibrium is part of the conclusion, not just that tˉ\bar ttˉ is an equilibrium; and the strong notion quantifies over all coalition deviations, not single-player ones.

A complete development needs first-order optimality conditions for concave maximization over polytopes, a version of Berge's maximum theorem, and convexity facts about differentiable functions. All of these are reusable well beyond this mission. Contributions are welcome on each milestone independently, and on general lemmas about parametric Wardrop flows.

Selected references

  • J. Correa, C. Guzmán, T. Lianeas, E. Nikolova, M. Schröder, Network Pricing: How to Induce Optimal Flows Under Strategic Link Operators, Operations Research, Articles in Advance, 2021. https://doi.org/10.1287/opre.2020.2067
  • M. Beckmann, C. B. McGuire, C. B. Winsten, Studies in the Economics of Transportation, Yale University Press, New Haven, 1956 (book; no DOI).
  • D. Acemoglu, A. Ozdaglar, Competition and Efficiency in Congested Markets, Mathematics of Operations Research 32(1), 2007. https://doi.org/10.1287/moor.1060.0231
  • A. Hayrapetyan, É. Tardos, T. Wexler, A Network Pricing Game for Selfish Traffic, Distributed Computing 19(4), 2007. https://doi.org/10.1007/s00446-006-0012-4
  • C. Berge, Topological Spaces: Including a Treatment of Multi-valued Functions, Vector Spaces, and Convexity, Oliver and Boyd, 1963; Dover reprint (book; no DOI).
8 thms2 active usersReviewed
Algorithmic Game TheoryBandit AlgorithmsOperations Research+1·Captain: mikedeng1

Game of Thrones: Fully Distributed Learning for Multiplayer Bandits: Without Communication, the Game of Thrones Algorithm Has Expected Total Regret O(log^{1+δ} T)Research Paper

Motivation

In a multiplayer multi-armed bandit, several agents repeatedly choose among the same finite set of arms, and two agents that choose the same arm collide and receive nothing. The model comes from cognitive radio and wireless networks: users share channels, a channel used by two users at once carries neither transmission, and the quality of a channel differs from user to user. Each user must learn the channel qualities from her own rewards while avoiding the others, and in a large network the users can neither exchange messages nor observe each other's choices.

When all players share the same arm means, the problem reduces to finding the NNN best arms and spreading the players over them; algorithms such as Musical Chairs (Rosenski, Shamir and Szlak, 2016) do this. When each player has her own means μn,i\mu_{n,i}μn,i​, the target is an optimal solution of an assignment problem, which couples the players. Bistritz and Leshem (arXiv:1810.11162, NeurIPS 2018; a journal version appeared in Mathematics of Operations Research) gave the first algorithm for this heterogeneous case that uses no communication at all and has near-logarithmic expected regret. This mission formalizes the main theorem of the preprint arXiv:1810.11162v7.

Setting

There are NNN players and M≥NM\ge NM≥N arms. At every turn t=1,…,Tt=1,\dots,Tt=1,…,T each player nnn picks an arm an(t)a_n(t)an​(t). The non-collision indicator ηi(a)\eta_i(a)ηi​(a) is 000 if more than one player chose arm iii in the profile aaa and 111 otherwise. Player nnn receives rn,an(t)(t) ηan(t)(a(t))r_{n,a_n(t)}(t)\,\eta_{a_n(t)}(a(t))rn,an​(t)​(t)ηan​(t)​(a(t)): the reward of her arm, or 000 after a collision.

The rewards satisfy Definition II.1: for each (n,i)(n,i)(n,i) the sequence rn,i(t)r_{n,i}(t)rn,i​(t) is i.i.d. with a continuous law, mean μn,i>0\mu_{n,i}>0μn,i​>0, variance σn,i2\sigma^2_{n,i}σn,i2​ and Bernstein's moment condition with parameter bn,ib_{n,i}bn,i​, and the sequences are independent. Because the law is continuous, a zero reward reveals a collision almost surely; this is the only feedback a player gets. The horizon TTT is unknown to the players.

Write gn(a)=μn,anηan(a)g_n(a)=\mu_{n,a_n}\eta_{a_n}(a)gn​(a)=μn,an​​ηan​​(a). The benchmark is an optimal assignment a∗∈arg⁡max⁡a∑ngn(a)a^*\in\arg\max_a\sum_ng_n(a)a∗∈argmaxa​∑n​gn​(a), assumed unique, and the total regret is

R=∑t=1T∑n=1Nrn,an∗(t) ηan∗(a∗)−∑t=1T∑n=1Nrn,an(t)(t) ηan(t)(a(t)),Rˉ=E{R}.R=\sum_{t=1}^T\sum_{n=1}^Nr_{n,a^*_n}(t)\,\eta_{a^*_n}(a^*)-\sum_{t=1}^T\sum_{n=1}^Nr_{n,a_n(t)}(t)\,\eta_{a_n(t)}(a(t)),\qquad \bar R=\mathbb E\{R\}.R=t=1∑T​n=1∑N​rn,an∗​​(t)ηan∗​​(a∗)−t=1∑T​n=1∑N​rn,an​(t)​(t)ηan​(t)​(a(t)),Rˉ=E{R}.

The Game of Thrones (GoT) algorithm (Algorithm 1) runs in epochs k=1,2,…k=1,2,\dotsk=1,2,…, each with three phases: an exploration phase of ⌈c1kδ⌉\lceil c_1k^\delta\rceil⌈c1​kδ⌉ turns, where players sample arms uniformly and average their collision-free rewards into estimates μn,ik\mu^k_{n,i}μn,ik​; a GoT phase of ⌈c2kδ⌉\lceil c_2k^\delta\rceil⌈c2​kδ⌉ turns, where players run a perturbed content/discontent dynamic with perturbation ε\varepsilonε and exponent ccc on the game un(a)=μn,ankηan(a)u_n(a)=\mu^k_{n,a_n}\eta_{a_n}(a)un​(a)=μn,an​k​ηan​​(a); and an exploitation phase of c32kc_32^kc3​2k turns, where each player plays the arm with which she was most often content during the last ⌊k/2⌋+1\lfloor k/2\rfloor+1⌊k/2⌋+1 GoT phases. The GoT dynamics form a Markov chain PεP^\varepsilonPε on the states Z=∏n(An×{C,D})Z=\prod_n(\mathcal A_n\times\{C,D\})Z=∏n​(An​×{C,D}) (baseline arm and mood of every player), with optimal state z∗=[a∗,CN]z^*=[a^*,C^N]z∗=[a∗,CN].

Formalization targets

Goal: Theorem III.1

With J1=max⁡a∑ngn(a)J_1=\max_a\sum_ng_n(a)J1​=maxa​∑n​gn​(a), J0=∑nmax⁡agn(a)J_0=\sum_n\max_ag_n(a)J0​=∑n​maxa​gn​(a), integers c1,c2,c3>0c_1,c_2,c_3>0c1​,c2​,c3​>0, δ>0\delta>0δ>0 and c>J0−J1c>J_0-J_1c>J0​−J1​, there is ε∈(0,1)\varepsilon\in(0,1)ε∈(0,1) such that for all large enough TTT

Rˉ≤4(max⁡n,iμn,i)(c1+c2) Nlog⁡21+δ(Tc3+2).\bar R\le4\Big(\max_{n,i}\mu_{n,i}\Big)(c_1+c_2)\,N\log_2^{1+\delta}\Big(\frac T{c_3}+2\Big).Rˉ≤4(n,imax​μn,i​)(c1​+c2​)Nlog21+δ​(c3​T​+2).

Milestones

  1. Lemma IV.2. If ∣μ^n,i−μn,i∣<Δ≤(J1−J2)/(2N)|\hat\mu_{n,i}-\mu_{n,i}|<\Delta\le(J_1-J_2)/(2N)∣μ^​n,i​−μn,i​∣<Δ≤(J1​−J2​)/(2N), every optimal assignment for μ^\hat\muμ^​ is optimal for μ\muμ (J2J_2J2​ the second best objective).
  2. Lemma IV.3, Eq. (20). P(max⁡n,i∣μn,ik−μn,i∣>Δmin⁡/4)≤2NMe−wc1(k/2)δk+NMe−c1(k/2)δk/(36M2)\mathbb P(\max_{n,i}|\mu^k_{n,i}-\mu_{n,i}|>\Delta_{\min}/4)\le2NMe^{-wc_1(k/2)^\delta k}+NMe^{-c_1(k/2)^\delta k/(36M^2)}P(maxn,i​∣μn,ik​−μn,i​∣>Δmin​/4)≤2NMe−wc1​(k/2)δk+NMe−c1​(k/2)δk/(36M2).
  3. Lemma IV.3, Eq. (21). The same for the union over the last ⌊k/2⌋+1\lfloor k/2\rfloor+1⌊k/2⌋+1 epochs.
  4. Lemma V.3. The estimated assignment problem has a unique optimum almost surely.
  5. Theorem V.6. If c>∑nun,max⁡−J1c>\sum_nu_{n,\max}-J_1c>∑n​un,max​−J1​, then πz∗>12(1−η)\pi_{z^*}>\frac1{2(1-\eta)}πz∗​>2(1−η)1​ for every small enough ε\varepsilonε.
  6. Lemma V.7, Eq. (31). Markov-chain concentration of the visits to z∗z^*z∗ in one GoT phase.
  7. Lemma V.8, Eq. (33). The GoT phases of the last ⌊k/2⌋+1\lfloor k/2\rfloor+1⌊k/2⌋+1 epochs fail with probability at most (C0e−Θ((k/2)δ))k(C_0e^{-\Theta((k/2)^\delta)})^k(C0​e−Θ((k/2)δ))k.

Significance

The theorem shows that full decentralization costs at most a factor log⁡δT\log^\delta TlogδT in regret: the Ω(log⁡T)\Omega(\log T)Ω(logT) lower bound of Proposition II.3 holds already with full information, and GoT reaches O(log⁡1+δT)O(\log^{1+\delta}T)O(log1+δT) with no messages, no knowledge of TTT, and no observation of the other players. It is a learning-in-games result as much as a bandit result: the players reach the welfare-maximizing assignment of a game that is not interdependent, which the content/discontent dynamics of Marden, Young and Pao (2014) require, and the requirement on the exponent is c>∑nun,max⁡−J1c>\sum_nu_{n,\max}-J_1c>∑n​un,max​−J1​ instead of c>Nc>Nc>N.

The result is proved on paper and has no machine-checked proof; nothing in this mission is formalized yet. A formal proof would also settle points the paper leaves implicit, recorded in the formalization notes: one ε\varepsilonε must serve every epoch although the stationary threshold of Theorem V.6 depends on the epoch's estimated utilities, and the GoT chain has transient states, so the tree formula of Lemma V.5 and the norm ∥ϕk∥π\|\phi_k\|_\pi∥ϕk​∥π​ must be applied to its closed class.

Difficulty

Each phase is analysed separately, and the work lies in the parts that are not standard. The exploration bound needs a concentration inequality for averages over a random number of collision-free samples. The GoT phase needs a lower bound on a stationary probability of a perturbed chain on (2M)N(2M)^N(2M)N states, obtained by comparing the resistances of trees in the sense of Freidlin and Wentzell (Appendix A, pp. 15–18). It then needs a Chernoff bound for Markov chains (Chung, Lam, Liu and Mitzenmacher, 2012) in terms of the mixing time. Finally, the epochs interact: the estimates of epoch kkk determine the chain of epoch kkk, the GoT phase starts from the end of an earlier GoT phase, and the exploitation phase votes over ⌊k/2⌋+1\lfloor k/2\rfloor+1⌊k/2⌋+1 dependent phases.

The natural first idea, to treat each epoch's GoT run as a fixed ergodic chain and apply a stationary-mass bound, fails twice. The chain is random through the estimates, so the threshold on ε\varepsilonε must hold uniformly over a neighbourhood of the true means. The chain is also not irreducible: a state where a colliding player is content can never be entered.

Formalization scope

Players, arms and turns are 0-based (Fin N, Fin M, t : ℕ), and epochs are 1-based. The collision indicator is noColl, because η\etaη also names the slack in Theorem V.6 and Lemmas V.7–V.8. The rewards live on a probability space as r n i t. The players' randomization is a family of private uniform seeds, jointly independent of the rewards, and every random choice of Algorithm 1 is realized from a seed with exactly the prescribed law. Each player's action and update read only her own memory, her own seeds and her own received reward; the means, a∗a^*a∗, TTT and the other players' actions never enter a rule. Collisions are read off a zero reward, as in Algorithm 1. The regret is Eq. (3) with the realized comparison rewards. The GoT chain is an explicit matrix on Fin N → Fin M × Mood. Stationarity and the mixing time Tm(1/8)T_m(1/8)Tm​(1/8) (worst start, total variation) come from the published MarkovMixing definitions.

Conventions and disclosed additions:

  • c>J0−J1c>J_0-J_1c>J0​−J1​ in the goal, because Theorem III.1 omits ccc;
  • ε<1\varepsilon<1ε<1 for the goal's witness;
  • Δmin⁡>0\Delta_{\min}>0Δmin​>0 in Lemma IV.3, Eq. (21);
  • visited arms and positive estimates in Lemma V.3;
  • positive utilities and M≥2M\ge2M≥2 in Theorem V.6 and Lemmas V.7–V.8;
  • initial laws vanishing where π\piπ vanishes in Lemmas V.7–V.8;
  • Algorithm 1's GoT starting rule, rather than Lemma V.7's;
  • ties in Eq. (15) broken toward the smallest index;
  • the junk value μk=0\mu^k=0μk=0 for an unvisited arm.

A formalization in which a player's rule sees the instance would make the goal trivial (play a∗a^*a∗ from the start), and a policy class in place of Algorithm 1 would change the theorem. Neither is used. Irreducibility of the GoT chain is false, and no statement assumes it.

Needed infrastructure that Mathlib lacks: Bernstein's inequality for sums over random index sets, the Markov-chain tree theorem (already posed on the platform as YoungConventions.Perturbed.markov_chain_tree_formula), and a Chernoff bound for finite Markov chains. The last two are reusable well beyond this mission, and contributions of them as separate theorems are welcome.

Selected references

  • I. Bistritz and A. Leshem, Game of Thrones: Fully Distributed Learning for Multiplayer Bandits, arXiv:1810.11162v7, 2021. https://arxiv.org/abs/1810.11162
  • J. R. Marden, H. P. Young and L. Y. Pao, Achieving Pareto optimality through distributed learning, SIAM J. Control Optim. 52(5), 2014. https://doi.org/10.1137/12089705X
  • K.-M. Chung, H. Lam, Z. Liu and M. Mitzenmacher, Chernoff–Hoeffding bounds for Markov chains: generalized and simplified, STACS 2012. https://arxiv.org/abs/1201.0559
  • J. Rosenski, O. Shamir and L. Szlak, Multi-player bandits — a musical chairs approach, ICML 2016. https://arxiv.org/abs/1512.02866
  • M. I. Freidlin and A. D. Wentzell, Random Perturbations of Dynamical Systems, Springer, 1984. https://doi.org/10.1007/978-1-4684-0176-9
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Modeling, Measuring and Managing Risk X: Dual Representation of Polyhedral Acceptability FunctionalsTextbook

Motivation

Risk measures enter optimization models as objectives or constraints, and the models that use them most, multi-stage stochastic programs, are solved as large linear programs. A risk functional is only usable there if it can itself be written as the value of a linear program. Eichhorn and Römisch introduced polyhedral risk measures for this purpose (doi:10.1137/040605217). They are risk functionals defined as the optimal value of a linear stochastic program whose right-hand side is the random income being evaluated. The average value-at-risk of Rockafellar and Uryasev (doi:10.21314/JOR.2000.038) is the basic example. Sums and nestings of average values-at-risk over several periods are further examples.

Sections 2.4.4 and 3.3.5 of Pflug and Römisch, Modeling, Measuring and Managing Risk (World Scientific, 2007, doi:10.1142/6478) develop this class in the book's profit convention (larger is better). They prove that, under two finite-dimensional conditions on the program's data, the functional is finite, concave and continuous, and that it has a dual representation over an explicitly polyhedral set of densities. The book then reads off from that dual set which axioms of multi-period acceptability functionals the functional satisfies. This mission formalizes those results.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space, T≥1T\ge1T≥1, and F=(F0,…,FT)\boldsymbol{\mathcal F}=(\mathcal F_0,\dots,\mathcal F_T)F=(F0​,…,FT​) a filtration in F\mathcal FF with trivial F0={∅,Ω}\mathcal F_0=\{\emptyset,\Omega\}F0​={∅,Ω}. Fix p∈[1,∞)p\in[1,\infty)p∈[1,∞) and q∈(1,∞]q\in(1,\infty]q∈(1,∞] with 1/p+1/q=11/p+1/q=11/p+1/q=1. Income processes Y=(Y1,…,YT)Y=(Y_1,\dots,Y_T)Y=(Y1​,…,YT​) live in Y=×t=1TLp(Ft)\mathcal Y=\times_{t=1}^TL_p(\mathcal F_t)Y=×t=1T​Lp​(Ft​), densities ZZZ in Z=×t=1TLq(Ft)\mathcal Z=\times_{t=1}^TL_q(\mathcal F_t)Z=×t=1T​Lq​(Ft​). Random variables equal almost surely are identified.

A set V⊆RkV\subseteq\mathbb R^kV⊆Rk is polyhedral if it is a finite intersection of closed half-spaces, and a polyhedral cone if all of those half-spaces pass through the origin. Its polar cone is V∗={v∗:⟨v∗,v⟩≤0 ∀v∈V}V^*=\{v^*:\langle v^*,v\rangle\le0\ \forall v\in V\}V∗={v∗:⟨v∗,v⟩≤0 ∀v∈V}, which is the negative of the usual dual cone.

The data of a polyhedral functional are dimensions ktk_tkt​, vectors ct∈Rktc_t\in\mathbb R^{k_t}ct​∈Rkt​ and non-empty polyhedral sets Vt⊆RktV_t\subseteq\mathbb R^{k_t}Vt​⊆Rkt​ for t=0,…,Tt=0,\dots,Tt=0,…,T, together with coefficients wt,τ∈Rkt−τw_{t,\tau}\in\mathbb R^{k_{t-\tau}}wt,τ​∈Rkt−τ​. The functional is

R(Y)=sup⁡{∑t=0TE⟨ct,vt⟩ : vt∈Lp(Ft;Rkt), vt∈Vt a.s., ∑τ=0t⟨wt,τ,vt−τ⟩=Yt a.s. (t≥1)}.\mathcal R(Y)=\sup\Bigl\{\sum_{t=0}^T\mathbb E\langle c_t,v_t\rangle\ :\ v_t\in L_p(\mathcal F_t;\mathbb R^{k_t}),\ v_t\in V_t\ \text{a.s.},\ \sum_{\tau=0}^t\langle w_{t,\tau},v_{t-\tau}\rangle=Y_t\ \text{a.s.}\ (t\ge1)\Bigr\}.R(Y)=sup{t=0∑T​E⟨ct​,vt​⟩ : vt​∈Lp​(Ft​;Rkt​), vt​∈Vt​ a.s., τ=0∑t​⟨wt,τ​,vt−τ​⟩=Yt​ a.s. (t≥1)}.

The first decision v0v_0v0​ is deterministic. The functional depends on the filtration only through the measurability of the decisions. The two standing conditions are:

  • (i): every VtV_tVt​ is a polyhedral cone, and ⟨wt,0,Vt⟩=R\langle w_{t,0},V_t\rangle=\mathbb R⟨wt,0​,Vt​⟩=R (complete recourse);
  • (ii): some uˉ∈RT\bar u\in\mathbb R^Tuˉ∈RT satisfies c0−∑τwτ,τuˉτ∈V0∗c_0-\sum_\tau w_{\tau,\tau}\bar u_\tau\in V_0^*c0​−∑τ​wτ,τ​uˉτ​∈V0∗​ and ct−∑τ≥twτ,τ−tuˉτ∈Vt∗c_t-\sum_{\tau\ge t}w_{\tau,\tau-t}\bar u_\tau\in V_t^*ct​−∑τ≥t​wτ,τ−t​uˉτ​∈Vt∗​ (dual feasibility).

The dual set is

Z∗={Z∈Z: c0−∑τ=1Twτ,τE(Zτ)∈V0∗,  ct−∑τ=tTwτ,τ−tE(Zτ∣Ft)∈Vt∗ a.s., t=1,…,T}.\mathcal Z_*=\Bigl\{Z\in\mathcal Z:\ c_0-\sum_{\tau=1}^Tw_{\tau,\tau}\mathbb E(Z_\tau)\in V_0^*,\ \ c_t-\sum_{\tau=t}^Tw_{\tau,\tau-t}\mathbb E(Z_\tau\mid\mathcal F_t)\in V_t^*\ \text{a.s.},\ t=1,\dots,T\Bigr\}.Z∗​={Z∈Z: c0​−τ=1∑T​wτ,τ​E(Zτ​)∈V0∗​,  ct​−τ=t∑T​wτ,τ−t​E(Zτ​∣Ft​)∈Vt∗​ a.s., t=1,…,T}.

The single-period case T=1T=1T=1 with F1=F\mathcal F_1=\mathcal FF1​=F is the book's Definition 2.66.

Formalization targets

Goal: Theorem 3.38

Under (i) and (ii), R\mathcal RR is finite, positively homogeneous, concave and continuous on Y\mathcal YY. It is information monotone (MA0): enlarging the filtration does not decrease it. For every Y∈YY\in\mathcal YY∈Y,

R(Y)=inf⁡{∑t=1TE(YtZt):Z∈Z∗}.\mathcal R(Y)=\inf\Bigl\{\sum_{t=1}^T\mathbb E(Y_tZ_t):Z\in\mathcal Z_*\Bigr\}.R(Y)=inf{t=1∑T​E(Yt​Zt​):Z∈Z∗​}.

Milestones

  • Example 2.70. For α∈(0,1]\alpha\in(0,1]α∈(0,1] the parameters k0=1k_0=1k0​=1, k1=2k_1=2k1​=2, c0=w0=1c_0=w_0=1c0​=w0​=1, c1=(−1/α,0)c_1=(-1/\alpha,0)c1​=(−1/α,0), w1=(−1,1)w_1=(-1,1)w1​=(−1,1), V0=RV_0=\mathbb RV0​=R, V1=R+2V_1=\mathbb R^2_+V1​=R+2​ give max⁡x{x−1αE[(x−Y)+]}\max_x\{x-\frac1\alpha\mathbb E[(x-Y)^+]\}maxx​{x−α1​E[(x−Y)+]}, the average value-at-risk. It is an acceptability functional with Z∗={EZ=1, 0≤Z≤1/α}\mathcal Z_*=\{\mathbb E Z=1,\ 0\le Z\le1/\alpha\}Z∗​={EZ=1, 0≤Z≤1/α}.
  • Proposition 2.68. The single-period version of the goal. If moreover Z∗⊆{Z≥0, EZ=1}\mathcal Z_*\subseteq\{Z\ge0,\ \mathbb EZ=1\}Z∗​⊆{Z≥0, EZ=1}, then R\mathcal RR is an acceptability functional.
  • Eqs. (3.57)–(3.58). R\mathcal RR is the infimum of ∑tE(YtZt)−R+(Z)\sum_t\mathbb E(Y_tZ_t)-\mathcal R^+(Z)∑t​E(Yt​Zt​)−R+(Z) over Z∈ZZ\in\mathcal ZZ∈Z, where R+(Z)=inf⁡Y∈Y{∑tE(YtZt)−R(Y)}\mathcal R^+(Z)=\inf_{Y\in\mathcal Y}\{\sum_t\mathbb E(Y_tZ_t)-\mathcal R(Y)\}R+(Z)=infY∈Y​{∑t​E(Yt​Zt​)−R(Y)} is its conjugate.
  • Eq. (3.59). R+(Z)=0\mathcal R^+(Z)=0R+(Z)=0 for Z∈Z∗Z\in\mathcal Z_*Z∈Z∗​, and −∞-\infty−∞ otherwise.
  • Theorem 3.39. Under complete recourse, inclusions of Z∗\mathcal Z_*Z∗​ in three density sets yield three versions of the multi-period acceptability axioms (MA0)–(MA5), together with finiteness and continuity.

Significance

Theorem 3.38 turns a linear multi-stage program into a risk functional with known structure. The functional is concave and continuous, and it is the lower envelope of linear functionals over a dual set cut out by finitely many linear conditions on conditional expectations. Theorem 3.39 makes that dual set into a design tool. Which translation equivariance a polyhedral functional has can be read off from finitely many vector conditions, without evaluating the functional. The multi-period average value-at-risk and sums of single-period average values-at-risk are obtained this way. These are the risk functionals that can be embedded in large-scale stochastic programming models without leaving linear programming.

The results are proved in the book and in Eichhorn–Römisch (2005). As far as is known, no part of them has a machine-checked proof. The platform has no polyhedral risk functional. It has finite-dimensional linear programming duality and a loss-side, upper-tail average value-at-risk on L∞L_\inftyL∞​, which uses a different convention and so is not a substitute.

Difficulty

The theorem is linear programming duality, but in an infinite-dimensional space of adapted processes. Finite-dimensional LP duality does not apply directly, for three reasons:

  • the decisions are random vectors in LpL_pLp​, constrained by measurability with respect to a filtration;
  • the constraint vt∈Vtv_t\in V_tvt​∈Vt​ holds pointwise almost surely;
  • the dual objects are conditional expectations, not vectors.

Finiteness needs feasible decisions with a uniform LpL_pLp​ bound, which is a measurable-selection question for a polyhedral set-valued map. The duality step needs conjugacy on a product of LpL_pLp​ spaces. It also needs to exchange an infimum over random decisions with an expectation, and that exchange is a theorem about normal integrands, not a formality. Little of this exists in Mathlib.

The two inclusions of Theorem 3.39 that use complete recourse alone cannot simply be combined with the goal: a non-empty dual set is an extra hypothesis there (see below).

Formalization scope

Lean namespace RiskFunctionals.Polyhedral.

  • Representation. Vectors are Fin k → ℝ with the dot product ⬝ᵥ. Polyhedral sets and cones are explicit finite systems of inequalities, never general closed convex cones. The polar cone uses the book's sign.
  • Random variables. They are functions with MemLp hypotheses and an Ft\mathcal F_tFt​-measurable representative. Constraints hold almost surely, and conditional expectations are Mathlib's.
  • Coefficients. Time indices are natural numbers. The coefficient wt,τw_{t,\tau}wt,τ​ is stored as W t (t-τ), indexed by the period of the decision it multiplies, so that its type matches.
  • Values. The functional, its conjugate and the dual infimum are computed in EReal, so empty or unbounded programs give ∓∞\mp\infty∓∞ instead of a junk value. Finiteness is always a conclusion and never a hypothesis. The other properties are stated for the real value only alongside finiteness. The dual set is the printed polyhedral set, not an existential family.
  • Trivializing formalizations. A bare real sSup over the feasible set, or a dual set given only by its existence, would make the goal trivially true. Both are ruled out by the EReal values and by the explicit dual set.

Beyond the paper. There are two corrected variants, each stated next to the faithful item.

  • Theorem 3.39(a)–(b) as printed fails when Z∗\mathcal Z_*Z∗​ is empty. With complete recourse, T=1T=1T=1, V0=V1=RV_0=V_1=\mathbb RV0​=V1​=R, c0=1c_0=1c0​=1, c1=0c_1=0c1​=0, w1,0=1w_{1,0}=1w1,0​=1, w1,1=0w_{1,1}=0w1,1​=0, the inclusions hold vacuously but R≡+∞\mathcal R\equiv+\inftyR≡+∞. The corrected variant adds Z∗≠∅\mathcal Z_*\neq\emptysetZ∗​=∅.
  • Example 2.70's maximum is not attained at α=1\alpha=1α=1 for YYY unbounded above. The corrected variant states the supremum.

Two sign slips in Example 2.70 (a printed (x−z)−(x-z)^-(x−z)− and z−v0z-v_0z−v0​) are corrected in the faithful item itself.

The development needs measurable selections of polyhedral multifunctions, Fenchel–Moreau conjugacy on LpL_pLp​ products, and interchange of infimum and integral. All three are reusable well beyond risk measures. Contributions of any of them, of the single-period case, or of the multi-period average value-at-risk as an instance are welcome.

Selected references

  • G. Ch. Pflug, W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007. doi:10.1142/6478
  • A. Eichhorn, W. Römisch, Polyhedral risk measures in stochastic programming, SIAM Journal on Optimization 16 (2005), 69–95. doi:10.1137/040605217
  • R. T. Rockafellar, S. Uryasev, Optimization of conditional value-at-risk, Journal of Risk 2 (2000), 21–41. doi:10.21314/JOR.2000.038
  • R. T. Rockafellar, R. J.-B. Wets, Variational Analysis, Springer, 1998. doi:10.1007/978-3-642-02431-3
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Modeling, Measuring and Managing Risk IX: Dual Representation of the Nested Average Value-at-RiskTextbook

Motivation

Risk that unfolds over several periods is measured in two common ways. One adds up one-period measurements of each payment, each made with the information available one step earlier. The other composes one-period conditional measurements backwards in time, the way dynamic programming evaluates a policy. The second way is the one used in multistage stochastic programming with risk-averse objectives, because it is time-consistent by construction: a plan that is optimal today stays optimal when re-evaluated tomorrow. Ruszczyński and Shapiro (Conditional risk mappings, Math. Oper. Res. 2006) built the general theory of such compositions. Artzner, Delbaen, Eber, Heath and Ku (Ann. Oper. Res. 2007) studied the matching dynamic-programming (Bellman) principle for coherent multiperiod risk-adjusted values.

The most widely used one-period building block is the average value-at-risk. When it is applied conditionally at every stage, the composition is the nested average value-at-risk. Section 3.3 of Pflug and Römisch, Modeling, Measuring and Managing Risk (World Scientific 2007), treats both constructions. It builds the nested functional, shows that it depends only on the total payoff, gives its dual representation as an infimum over bounded-growth martingale densities, and compares it with the additive (multi-period) average value-at-risk. This mission formalizes that section's statements.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space with a filtration F0={∅,Ω}⊆F1⊆⋯⊆FT=F\mathcal F_0=\{\emptyset,\Omega\}\subseteq\mathcal F_1\subseteq\dots\subseteq\mathcal F_T=\mathcal FF0​={∅,Ω}⊆F1​⊆⋯⊆FT​=F. Random variables that agree almost surely are identified, and all (in)equalities between them hold almost surely. The book uses profit variables, where larger is better. Fix p∈[1,∞)p\in[1,\infty)p∈[1,∞) and put Yt=Lp(Ω,Ft,P)\mathcal Y_t=L_p(\Omega,\mathcal F_t,\mathbb P)Yt​=Lp​(Ω,Ft​,P). An income process is Y=(Y1,…,YT)Y=(Y_1,\dots,Y_T)Y=(Y1​,…,YT​) with Yt∈YtY_t\in\mathcal Y_tYt​∈Yt​.

A conditional acceptability mapping At−1:YT→Yt−1\mathcal A_{t-1}:\mathcal Y_T\to\mathcal Y_{t-1}At−1​:YT​→Yt−1​ has three properties:

  • (CA1) At−1(YT+Yt−1)=At−1(YT)+Yt−1\mathcal A_{t-1}(Y_T+Y_{t-1})=\mathcal A_{t-1}(Y_T)+Y_{t-1}At−1​(YT​+Yt−1​)=At−1​(YT​)+Yt−1​ for Yt−1∈Yt−1Y_{t-1}\in\mathcal Y_{t-1}Yt−1​∈Yt−1​;
  • (CA2) it is concave;
  • (CA3) it is monotone.

A family A0,…,AT−1\mathcal A_0,\dots,\mathcal A_{T-1}A0​,…,AT−1​ defines the nested functional and the compositions

A(Y;F)=A0[Y1+⋯+AT−2[YT−1+AT−1(YT)]⋯],A(t)=A0∘⋯∘At−1.\mathcal A(Y;\boldsymbol{\mathcal F})=\mathcal A_0\big[Y_1+\dots+\mathcal A_{T-2}[Y_{T-1}+\mathcal A_{T-1}(Y_T)]\cdots\big],\qquad \mathcal A^{(t)}=\mathcal A_0\circ\dots\circ\mathcal A_{t-1}.A(Y;F)=A0​[Y1​+⋯+AT−2​[YT−1​+AT−1​(YT​)]⋯],A(t)=A0​∘⋯∘At−1​.

Since F0\mathcal F_0F0​ is trivial, both are constants.

For α∈(0,1]\alpha\in(0,1]α∈(0,1] and a sub-σ\sigmaσ-field G\mathcal GG, the conditional average value-at-risk AV@Rα(Y∣G)∈L1(G)\mathbb{AV@R}_\alpha(Y\mid\mathcal G)\in L_1(\mathcal G)AV@Rα​(Y∣G)∈L1​(G) of Y∈L1(F)Y\in L_1(\mathcal F)Y∈L1​(F) is defined implicitly by

E(AV@Rα(Y∣G) 1B)=inf⁡{E(YZ):0≤Z≤1α1B, E(Z∣G)=1B}(B∈G).\mathbb E\big(\mathbb{AV@R}_\alpha(Y\mid\mathcal G)\,\mathbb 1_B\big)=\inf\Big\{\mathbb E(YZ):0\le Z\le\tfrac1\alpha\mathbb 1_B,\ \mathbb E(Z\mid\mathcal G)=\mathbb 1_B\Big\}\qquad(B\in\mathcal G).E(AV@Rα​(Y∣G)1B​)=inf{E(YZ):0≤Z≤α1​1B​, E(Z∣G)=1B​}(B∈G).

With trivial G\mathcal GG this is the lower-tail average 1α∫0αG−1(u) du\frac1\alpha\int_0^\alpha G^{-1}(u)\,duα1​∫0α​G−1(u)du of the quantile function. The nested average value-at-risk is

nAV@Rα(Y;F)=AV@Rα(⋅∣F0)∘⋯∘AV@Rα(⋅∣FT−1)(∑t=1TYt).\mathrm{n}\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F})=\mathbb{AV@R}_\alpha(\cdot\mid\mathcal F_0)\circ\dots\circ\mathbb{AV@R}_\alpha(\cdot\mid\mathcal F_{T-1})\Big(\sum_{t=1}^TY_t\Big).nAV@Rα​(Y;F)=AV@Rα​(⋅∣F0​)∘⋯∘AV@Rα​(⋅∣FT−1​)(t=1∑T​Yt​).

The multi-period average value-at-risk is AV@Rα,c(Y;F)=∑t=1Tct E[AV@Rαt(Yt∣Ft−1)]\mathbb{AV@R}_{\alpha,c}(Y;\boldsymbol{\mathcal F})=\sum_{t=1}^Tc_t\,\mathbb E[\mathbb{AV@R}_{\alpha_t}(Y_t\mid\mathcal F_{t-1})]AV@Rα,c​(Y;F)=∑t=1T​ct​E[AV@Rαt​​(Yt​∣Ft−1​)]. Below it is used with all αt=α\alpha_t=\alphaαt​=α and ct=1c_t=1ct​=1.

Formalization targets

Goal: dual representation of the nested average value-at-risk (Proposition 3.35, (3.49))

For Yt∈L1(Ft)Y_t\in L_1(\mathcal F_t)Yt​∈L1​(Ft​) and α∈(0,1]\alpha\in(0,1]α∈(0,1], the nested average value-at-risk is well defined, and

nAV@Rα(Y;F)=inf⁡{E[(Y1+⋯+YT)ZT]:0≤Zt≤1αZt−1, E(Zt∣Ft−1)=Zt−1, Z0=1, t=1,…,T}.\mathrm{n}\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F})=\inf\Big\{\mathbb E\big[(Y_1+\dots+Y_T)Z_T\big]:0\le Z_t\le\tfrac1\alpha Z_{t-1},\ \mathbb E(Z_t\mid\mathcal F_{t-1})=Z_{t-1},\ Z_0=1,\ t=1,\dots,T\Big\}.nAV@Rα​(Y;F)=inf{E[(Y1​+⋯+YT​)ZT​]:0≤Zt​≤α1​Zt−1​, E(Zt​∣Ft−1​)=Zt−1​, Z0​=1, t=1,…,T}.

Here ZtZ_tZt​ is Ft\mathcal F_tFt​-measurable. The feasible (Zt)(Z_t)(Zt​) are nonnegative martingales whose one-step growth is at most 1/α1/\alpha1/α.

Milestones

  1. Proposition 3.33. The nested functional of any family of conditional acceptability mappings has these properties:
    • it is weakly translation-equivariant, concave and monotone;
    • every A(t)\mathcal A^{(t)}A(t) is an acceptability functional;
    • A(Y;F)=A(T)(Y1+⋯+YT)\mathcal A(Y;\boldsymbol{\mathcal F})=\mathcal A^{(T)}(Y_1+\dots+Y_T)A(Y;F)=A(T)(Y1​+⋯+YT​) (3.47);
    • positive homogeneity is inherited from the mappings.
  2. The step in the proof of Proposition 3.35 (via (2.59)). For bounded Z1≥0Z_1\ge0Z1​≥0 that is F1\mathcal F_1F1​-measurable, E(AV@Rα(Y∣F1)Z1)=inf⁡{E(YZ2):0≤Z2≤1αZ1, E(Z2∣F1)=Z1}\mathbb E(\mathbb{AV@R}_\alpha(Y\mid\mathcal F_1)Z_1)=\inf\{\mathbb E(YZ_2):0\le Z_2\le\frac1\alpha Z_1,\ \mathbb E(Z_2\mid\mathcal F_1)=Z_1\}E(AV@Rα​(Y∣F1​)Z1​)=inf{E(YZ2​):0≤Z2​≤α1​Z1​, E(Z2​∣F1​)=Z1​}.
  3. Proposition 3.36(ii). For a final process (Y1=⋯=YT−1=0Y_1=\dots=Y_{T-1}=0Y1​=⋯=YT−1​=0), nAV@Rα(Y;F)≤AV@Rα(Y;F)\mathrm{n}\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F})\le\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F})nAV@Rα​(Y;F)≤AV@Rα​(Y;F).

Further items

  • Proposition 3.36(i), nAV@Rα≤α−(T−1)AV@Rα\mathrm{n}\mathbb{AV@R}_\alpha\le\alpha^{-(T-1)}\mathbb{AV@R}_\alphanAV@Rα​≤α−(T−1)AV@Rα​, stated as printed.
  • The information-monotonicity clause of Proposition 3.35: if Ft⊆Ft′\mathcal F_t\subseteq\mathcal F'_tFt​⊆Ft′​ for all ttt, then nAV@Rα(Y;F)≤nAV@Rα(Y;F′)\mathrm{n}\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F})\le\mathrm{n}\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F}')nAV@Rα​(Y;F)≤nAV@Rα​(Y;F′). It is stated as its own item, as printed.

Significance

The representation (3.49) shows that the nested average value-at-risk is a coherent functional of the total payoff. Its dual set consists of martingale densities with a multiplicative growth bound. Proposition 3.36 builds on this description to compare the nested and additive constructions. The same description underlies cutting-plane methods for risk-averse multistage programs: there the nested value is evaluated stage by stage, and each stage contributes one factor Zt/Zt−1∈[0,1/α]Z_t/Z_{t-1}\in[0,1/\alpha]Zt​/Zt−1​∈[0,1/α]. Proposition 3.33 is the general mechanism behind this: predictable translation-equivariance collapses a nested definition into a cumulative one.

All of these results are proved in the book, some only in outline. None is machine-checked. The platform has loss-side, upper-tail conditional value-at-risk results in other conventions and a nested risk-adjusted cost in an SDDP setting. It has no statement of the nested average value-at-risk or of (3.49). Formalizing this section yields a reusable treatment of conditional average values-at-risk defined by duality, together with their compositions along a filtration.

Difficulty

The conditional average value-at-risk is not given by a formula. It is defined through a family of infima indexed by the sets B∈GB\in\mathcal GB∈G, so composing two of them requires knowing what the first one does when paired with a general bounded weight rather than an indicator. Merging the infima of successive stages into one infimum over processes needs measurable selection of near-optimal densities, conditional on the earlier stages, and the martingale constraint must be preserved. The printed proof treats T=2T=2T=2 in a few lines and asserts that the general case "follows by induction". Its last display also carries a misprint, E(Z1)=0\mathbb E(Z_1)=0E(Z1​)=0 for E(Z1)=1\mathbb E(Z_1)=1E(Z1​)=1 (FINDINGS F5).

Formalization scope

Random variables are functions Ω → ℝ. The filtration is Mathlib's Filtration ℕ, and only indices 0,…,T0,\dots,T0,…,T matter. IsStandardFiltration records that F0\mathcal F_0F0​ is trivial and FT=F\mathcal F_T=\mathcal FFT​=F. The conditional average value-at-risk is the predicate IsConditionalAVaR, a literal transcription of the defining relation, with the infimum computed in EReal. The nested and multi-period values are predicates that are existential over versions of the conditional average values-at-risk. The goal therefore asserts existence and the identity separately. A version of the goal that only assumed some value exists, or that took a bare real infimum, would be vacuous or junk-valued, and the formal statement rules out both. The expectation of the F0\mathcal F_0F0​-measurable output is the functional's real value. The dual set requires ZtZ_tZt​ to be Ft\mathcal F_tFt​-measurable, which the page leaves implicit.

Beyond the paper. Two corrected variants are posed beside the faithful statements:

  • Information monotonicity (F1). Refining F1\mathcal F_1F1​ in a two-period example lowers the nested value from −5-5−5 to −10-10−10. The variant asserts that a counterexample exists.
  • Proposition 3.36(i) for Yt≥0Y_t\ge0Yt​≥0 (F2). The printed inequality fails for Y2≡−1Y_2\equiv-1Y2​≡−1 with α=1/2\alpha=1/2α=1/2. The variant adds the nonnegativity that the proof uses.

The faithful statements stay as printed and are expected to be disproved.

Contributions that would be reused beyond this mission:

  • existence and uniqueness of the conditional average value-at-risk on L1L_1L1​;
  • its extension to bounded nonnegative weights;
  • a general composition lemma for dual representations of conditional acceptability mappings.

Selected references

  • G. Ch. Pflug and W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007, §3.3. https://doi.org/10.1142/6478
  • A. Ruszczyński and A. Shapiro, Conditional risk mappings, Mathematics of Operations Research 31(3), 2006. https://doi.org/10.1287/moor.1060.0204
  • P. Artzner, F. Delbaen, J.-M. Eber, D. Heath and H. Ku, Coherent multiperiod risk adjusted values and Bellman's principle, Annals of Operations Research 152, 2007. https://doi.org/10.1007/s10479-006-0132-6
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Convex OptimizationOperations ResearchOptimization+2·Captain: Shuze Chen

Modeling, Measuring and Managing Risk VII: Dual Representation of Minimal Loss Deviation FunctionalsTextbook

Motivation

A deviation functional measures how far a random profit YYY spreads around its mean: the variance, the standard deviation, the mean absolute deviation from the median, and the average value-at-risk deviation are the standard examples in portfolio selection and in risk-averse stochastic programming. Pflug and Römisch, Modeling, Measuring and Managing Risk (World Scientific 2007, doi:10.1142/6478), §2.5, organize many of them under one construction, the minimal loss functional: the smallest expected loss incurred when YYY is predicted by a constant under a convex loss hhh. Optimization over portfolios with such a functional as the risk term relies on writing it as a supremum of linear functionals of YYY — a dual representation — because a supremum of linear functions can be handled by linear and conic programming and by subgradient methods.

The best known instance is the representation of the average value-at-risk as a minimum over a scalar aaa, due to Rockafellar and Uryasev (J. Risk 2000; J. Banking Finance 2002), stated in the loss convention. The general convex-analytic tool behind such representations is Rockafellar's conjugacy theorem for integral functionals (Pacific J. Math. 1968). This mission formalizes the book's Theorem 2.75, which combines the two for every minimal loss functional, together with the results its special cases rest on.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space, 1≤p<∞1\le p<\infty1≤p<∞, and qqq the conjugate exponent, 1/p+1/q=11/p+1/q=11/p+1/q=1. Random variables YYY are profits (larger is better) in LpL_pLp​; dual variables ZZZ are in LqL_qLq​, so that E(YZ)\mathbb E(YZ)E(YZ) is finite.

Let h:R→Rh:\mathbb R\to\mathbb Rh:R→R be non-negative, convex, with h(0)=0h(0)=0h(0)=0. The minimal loss functional of hhh is

D(Y)=min⁡{E[h(Y−a)]:a∈R},(2.109)\mathcal D(Y)=\min\{\mathbb E[h(Y-a)] : a\in\mathbb R\}, \tag{2.109}D(Y)=min{E[h(Y−a)]:a∈R},(2.109)

defined for YYY such that E[h(Y)]\mathbb E[h(Y)]E[h(Y)] exists. The Fenchel conjugate of hhh is

h∗(v)=sup⁡{uv−h(u):u∈R}∈(−∞,+∞].h^*(v)=\sup\{uv-h(u) : u\in\mathbb R\}\in(-\infty,+\infty].h∗(v)=sup{uv−h(u):u∈R}∈(−∞,+∞].

For example h(v)=v2h(v)=v^2h(v)=v2 gives D=Var\mathcal D=\mathbb{V}\mathrm{ar}D=Var and h∗(v)=v2/4h^*(v)=v^2/4h∗(v)=v2/4; h(v)=∣v∣h(v)=|v|h(v)=∣v∣ gives the mean absolute deviation from the median and h∗h^*h∗ equal to 000 on [−1,1][-1,1][−1,1] and +∞+\infty+∞ outside.

The distribution function of YYY is G(u)=P{Y≤u}G(u)=\mathbb P\{Y\le u\}G(u)=P{Y≤u}, its quantile function the left-continuous inverse G−1(p)=inf⁡{u:G(u)≥p}G^{-1}(p)=\inf\{u : G(u)\ge p\}G−1(p)=inf{u:G(u)≥p}, 0<p≤10<p\le10<p≤1. For 0<α≤10<\alpha\le 10<α≤1 the average value-at-risk is the lower-tail average

AV@Rα(Y)=1α∫0αG−1(u) du,\mathbb{AV@R}_\alpha(Y)=\frac1\alpha\int_0^\alpha G^{-1}(u)\,du,AV@Rα​(Y)=α1​∫0α​G−1(u)du,

and the average value-at-risk deviation is AV@RDα(Y)=E(Y)−AV@Rα(Y)\mathbb{AV@R}\mathbb D_\alpha(Y)=\mathbb E(Y)-\mathbb{AV@R}_\alpha(Y)AV@RDα​(Y)=E(Y)−AV@Rα​(Y). Write [y]+=max⁡(y,0)[y]^+=\max(y,0)[y]+=max(y,0) and [y]−=−min⁡(y,0)[y]^-=-\min(y,0)[y]−=−min(y,0).

Formalization targets

Goal: Theorem 2.75 (pp. 109–110)

For every hhh as above and every Y∈LpY\in L_pY∈Lp​ with E[h(Y)]\mathbb E[h(Y)]E[h(Y)] finite,

D(Y)=sup⁡{E(YZ)−Eh∗(Z):EZ=0},(2.113)\mathcal D(Y)=\sup\{\mathbb E(YZ)-\mathbb Eh^*(Z) : \mathbb EZ=0\}, \tag{2.113}D(Y)=sup{E(YZ)−Eh∗(Z):EZ=0},(2.113) EY−D(Y)=inf⁡{E(YZ)+E[h∗(1−Z)]:E(Z)=1},\mathbb EY-\mathcal D(Y)=\inf\{\mathbb E(YZ)+\mathbb E[h^*(1-Z)] : \mathbb E(Z)=1\},EY−D(Y)=inf{E(YZ)+E[h∗(1−Z)]:E(Z)=1},

and, for every Y∈LpY\in L_pY∈Lp​ and 0<α≤10<\alpha\le 10<α≤1,

AV@RDα(Y)=sup⁡{E(YZ):−1−αα≤Z≤1, EZ=0},(2.114)\mathbb{AV@R}\mathbb D_\alpha(Y)=\sup\Big\{\mathbb E(YZ) : -\frac{1-\alpha}{\alpha}\le Z\le1,\ \mathbb EZ=0\Big\}, \tag{2.114}AV@RDα​(Y)=sup{E(YZ):−α1−α​≤Z≤1, EZ=0},(2.114) AV@Rα(Y)=min⁡{E(YZ):EZ=1, 0≤Z≤1α}.\mathbb{AV@R}_\alpha(Y)=\min\Big\{\mathbb E(YZ) : \mathbb EZ=1,\ 0\le Z\le\frac1\alpha\Big\}.AV@Rα​(Y)=min{E(YZ):EZ=1, 0≤Z≤α1​}.

The constants −(1−α)/α-(1-\alpha)/\alpha−(1−α)/α, 111 and 1/α1/\alpha1/α are exactly the book's; the last minimum is attained.

Milestones

  1. Proposition B.3 (p. 272): for real valued convex l.s.c. hhh with h∗≥0h^*\ge0h∗≥0 and V∈LpV\in L_pV∈Lp​,
E[h(V)]=sup⁡{E(VZ)−E(h∗(Z)):E(h∗(Z))<∞}.\mathbb E[h(V)]=\sup\{\mathbb E(VZ)-\mathbb E(h^*(Z)) : \mathbb E(h^*(Z))<\infty\}.E[h(V)]=sup{E(VZ)−E(h∗(Z)):E(h∗(Z))<∞}.
  1. Proposition 2.74 (p. 109): min⁡{E([Y−a]+)+1−ααE([Y−a]−):a∈R}=AV@RDα(Y)\min\{\mathbb E([Y-a]^+)+\frac{1-\alpha}{\alpha}\mathbb E([Y-a]^-) : a\in\mathbb R\}=\mathbb{AV@R}\mathbb D_\alpha(Y)min{E([Y−a]+)+α1−α​E([Y−a]−):a∈R}=AV@RDα​(Y) (2.112), the minimum being attained.
  2. Eq. (2.100) (p. 101): Std(Y)=∥Y−EY∥2=sup⁡{E(YZ):E(Z)=0, E(Z2)≤1}\mathbb{S}\mathrm{td}(Y)=\|Y-\mathbb EY\|_2=\sup\{\mathbb E(YZ) : \mathbb E(Z)=0,\ \mathbb E(Z^2)\le1\}Std(Y)=∥Y−EY∥2​=sup{E(YZ):E(Z)=0, E(Z2)≤1}.

Two further items state Eq. (2.89) (p. 97), Var(Y)=∥Y−EY∥22=sup⁡{E(YZ)−14Var(Z):EZ=0}\mathbb{V}\mathrm{ar}(Y)=\|Y-\mathbb EY\|_2^2=\sup\{\mathbb E(YZ)-\frac14\mathbb{V}\mathrm{ar}(Z) : \mathbb EZ=0\}Var(Y)=∥Y−EY∥22​=sup{E(YZ)−41​Var(Z):EZ=0}, and Eq. (2.101) (p. 102) as printed, E(Y)−Std(Y)=inf⁡{E(YZ):E(Z)=0, E[(1−Z)2]≤1}=inf⁡{E(YZ):E(Z)=0, E[Z2]≤2}\mathbb E(Y)-\mathbb{S}\mathrm{td}(Y)=\inf\{\mathbb E(YZ) : \mathbb E(Z)=0,\ \mathbb E[(1-Z)^2]\le1\}=\inf\{\mathbb E(YZ) : \mathbb E(Z)=0,\ \mathbb E[Z^2]\le2\}E(Y)−Std(Y)=inf{E(YZ):E(Z)=0, E[(1−Z)2]≤1}=inf{E(YZ):E(Z)=0, E[Z2]≤2}.

Significance

The result. Theorem 2.75 gives every minimal loss functional an explicit dual set: the centered ZZZ, penalized by Eh∗(Z)\mathbb E h^*(Z)Eh∗(Z). For piecewise linear hhh the penalty is the indicator of a box, so D\mathcal DD is a supremum of linear functionals over a polyhedral set, and the acceptability functional E−D\mathbb E-\mathcal DE−D is an infimum over mean-one dual variables; (2.114) and the last display recover the dual representation (2.20) of the average value-at-risk from this general principle. For quadratic hhh the theorem returns the variance representation (2.89). The same dual sets feed the book's later results on the monotonicity of E−D\mathbb E-\mathcal DE−D with respect to stochastic orders and on conditional versions (2.116)–(2.117).

Formalizing it. No platform item states Theorem 2.75, the integral conjugacy of Proposition B.3, or the dual representations of the variance and standard deviation. Related platform results use other conventions — the loss-side, upper-tail CVaR minimization formula (RUCVaR.MinFormula), a minimal weighted mean absolute deviation in Ogryczak–Ruszczyński normalization (DualSSD.MeanRisk.hDiam_eq_min), finite-dimensional Fenchel–Young and biconjugation (ConvexOptimization.fenchel_young, ConvexOptimization.fenchel_biconjugate_eq_self). The mission produces the profit-side, LpL_pLp​ statements of the book.

Difficulty

The weak inequality in (2.113) is the Fenchel–Young inequality integrated; equality is the content. The printed proof treats piecewise linear hhh by choosing, from YYY alone, a partition on which one affine piece of hhh is maximal, and claims E[h(Y−a)]=E(YZ)−a E(Z)−E[h∗(Z)]\mathbb E[h(Y-a)]=\mathbb E(YZ)-a\,\mathbb E(Z)-\mathbb E[h^*(Z)]E[h(Y−a)]=E(YZ)−aE(Z)−E[h∗(Z)] for every aaa; that identity holds only at a=0a=0a=0, and the conclusion EZ=0\mathbb E Z=0EZ=0 does not follow (for h=∣⋅∣h=|\cdot|h=∣⋅∣ and YYY uniform on {1,2,3}\{1,2,3\}{1,2,3} the chosen ZZZ is ≡1\equiv1≡1). The statement itself is correct in that example, but a complete argument has to choose the dual variable at a minimizing aaa, which need not exist, and has to pass from piecewise linear to general hhh by a limiting argument the book does not give. On the LpL_pLp​ side, an optimal ZZZ such as h′(Y−a∗)h'(Y-a^*)h′(Y−a∗) need not lie in LqL_qLq​ when hhh grows faster than ∣v∣p|v|^p∣v∣p, so the supremum is in general not attained and must be approached. Proposition B.3 requires a measurable selection of subgradients and handles the case E[h(V)]=+∞\mathbb E[h(V)]=+\inftyE[h(V)]=+∞.

Formalization scope

Lean represents random variables as measurable functions Ω→R\Omega\to\mathbb RΩ→R with MemLp hypotheses (Y∈LpY\in L_pY∈Lp​, Z∈LqZ\in L_qZ∈Lq​, p.HolderConjugate q, 1≤p<∞1\le p<\infty1≤p<∞) on a probability space; constraints on ZZZ hold almost surely. h∗h^*h∗ is an extended-real supremum (EReal), so it is +∞+\infty+∞ where the book's supremum is unbounded. The suprema and infima of the dual representations are taken in EReal over the ZZZ for which Eh∗(Z)\mathbb Eh^*(Z)Eh∗(Z) (resp. E[h∗(1−Z)]\mathbb E[h^*(1-Z)]E[h∗(1−Z)]) is finite — h∗(Z)h^*(Z)h∗(Z) almost surely finite and integrable — which does not change the book's value. D(Y)\mathcal D(Y)D(Y) is defined as the infimum in [0,+∞][0,+\infty][0,+∞] of ∫h(Y−a) dP\int h(Y-a)\,d\mathbb P∫h(Y−a)dP: the book's "min" presupposes attainment, which fails for h(v)=[v]+h(v)=[v]^+h(v)=[v]+ and YYY unbounded above, and attainment is not claimed. The standing assumption of §2.5.5 that E[h(Y)]\mathbb E[h(Y)]E[h(Y)] exists is a hypothesis of the parts on general hhh. AV@Rα\mathbb{AV@R}_\alphaAV@Rα​ is the book's lower-tail average of the left-continuous quantile function, not the loss-side upper-tail CVaR; variance is Mathlib's ProbabilityTheory.variance and Std=Var\mathbb{S}\mathrm{td}=\sqrt{\mathbb{V}\mathrm{ar}}Std=Var​.

A trivializing formalization is ruled out: no supremum or infimum is a bare real sSup/sInf whose junk value 000 on an empty or unbounded set could make an identity hold, the dual sets are nonempty (Z=0Z=0Z=0 resp. Z=1Z=1Z=1 is admissible), D\mathcal DD is an infimum in [0,∞][0,\infty][0,∞] rather than a real sInf, and the minimum for AV@Rα\mathbb{AV@R}_\alphaAV@Rα​ is stated with attainment (IsLeast).

Beyond the paper. Two variants are posed beside the faithful items. A corrected Proposition 2.74 adds the hypothesis that G−1(α)G^{-1}(\alpha)G−1(α) is finite: at α=1\alpha=1α=1 and YYY exponentially distributed, E([Y−a]+)>0\mathbb E([Y-a]^+)>0E([Y−a]+)>0 for every aaa while AV@RD1(Y)=0\mathbb{AV@R}\mathbb D_1(Y)=0AV@RD1​(Y)=0, so the printed minimum does not exist. A corrected (2.101) replaces the constraint E(Z)=0\mathbb E(Z)=0E(Z)=0 by E(Z)=1\mathbb E(Z)=1E(Z)=1: for Y≡1Y\equiv1Y≡1 the left side is 111 but every ZZZ with E(Z)=0\mathbb E(Z)=0E(Z)=0 gives E(YZ)=0\mathbb E(YZ)=0E(YZ)=0; the book's own rule (2.79) gives mean-one dual variables.

Definitions needed: the quantile function and AV@Rα\mathbb{AV@R}_\alphaAV@Rα​, the Fenchel conjugate, the expectation of h∗(Z)h^*(Z)h∗(Z) and the minimal loss functional; all are reusable by any formalization of law-invariant deviation measures. Welcome contributions include a measurable-selection lemma for subgradients of a convex function of one variable, Rockafellar's integral conjugacy on LpL_pLp​ (of which Proposition B.3 is a case), and the variant statements.

Selected references

  • G. Ch. Pflug, W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007. https://doi.org/10.1142/6478
  • R. T. Rockafellar, Integrals which are convex functionals, Pacific Journal of Mathematics 24 (1968), 525–539. https://doi.org/10.2140/pjm.1968.24.525
  • R. T. Rockafellar, S. Uryasev, Optimization of conditional value-at-risk, Journal of Risk 2 (2000), 21–41. https://doi.org/10.21314/JOR.2000.038
  • R. T. Rockafellar, S. Uryasev, Conditional value-at-risk for general loss distributions, Journal of Banking & Finance 26 (2002), 1443–1471. https://doi.org/10.1016/S0378-4266(02)00271-6
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Modeling, Measuring and Managing Risk V: Dual Representation of Conditional Acceptability MappingsTextbook

Motivation

A risk measure that returns a single number answers the question "how acceptable is this random profit, seen from today?". Multi-period decision problems — portfolio rebalancing, insurance reserves, stochastic programs on scenario trees — need the same question asked at every later date, given the information available then. The answer is no longer a number but a random variable measurable with respect to the information available at that date. Section 2.3 of Pflug and Römisch, Modeling, Measuring and Managing Risk (World Scientific, 2007, doi:10.1142/6478), sets up these conditional acceptability mappings axiomatically and gives them a dual representation modelled on the defining relation of the conditional expectation. The conditional average value-at-risk defined there is the building block of the nested risk measures used in multi-stage stochastic optimization (Chapter 3 of the same book), and of the time-consistent risk measures of Ruszczyński and Shapiro (doi:10.1287/moor.1060.0204) and Detlefsen and Scandolo (doi:10.1007/s00780-005-0159-6).

Setting

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space and F1⊆F\mathcal F_1\subseteq\mathcal FF1​⊆F a sub-σ\sigmaσ-field, the observable information. Fix p∈[1,∞)p\in[1,\infty)p∈[1,∞) and let qqq be its conjugate exponent, 1/p+1/q=11/p+1/q=11/p+1/q=1. Put Y=Lp(Ω,F,P)\mathcal Y=L_p(\Omega,\mathcal F,\mathbb P)Y=Lp​(Ω,F,P) and Y1=Lp(Ω,F1,P)\mathcal Y_1=L_p(\Omega,\mathcal F_1,\mathbb P)Y1​=Lp​(Ω,F1​,P), the subspace of classes with an F1\mathcal F_1F1​-measurable version. Random variables equal almost surely are identified, and every (in)equality between them holds almost surely. Variables are profits: larger is better.

A map A:Y→Y1\mathcal A:\mathcal Y\to\mathcal Y_1A:Y→Y1​ is a conditional acceptability mapping if for all Y,Y~∈YY,\tilde Y\in\mathcal YY,Y~∈Y

  • (CA1) A(Y+Y(1))=A(Y)+Y(1)\mathcal A(Y+Y^{(1)})=\mathcal A(Y)+Y^{(1)}A(Y+Y(1))=A(Y)+Y(1) for every Y(1)∈Y1Y^{(1)}\in\mathcal Y_1Y(1)∈Y1​;
  • (CA2) A(λY+(1−λ)Y~)≥λA(Y)+(1−λ)A(Y~)\mathcal A(\lambda Y+(1-\lambda)\tilde Y)\ge\lambda\mathcal A(Y)+(1-\lambda)\mathcal A(\tilde Y)A(λY+(1−λ)Y~)≥λA(Y)+(1−λ)A(Y~) for λ∈[0,1]\lambda\in[0,1]λ∈[0,1];
  • (CA3) Y≤Y~Y\le\tilde YY≤Y~ implies A(Y)≤A(Y~)\mathcal A(Y)\le\mathcal A(\tilde Y)A(Y)≤A(Y~).

It is positively homogeneous if A(λY)=λA(Y)\mathcal A(\lambda Y)=\lambda\mathcal A(Y)A(λY)=λA(Y) for λ>0\lambda>0λ>0, and upper semicontinuous if, for every B∈F1B\in\mathcal F_1B∈F1​, the real functional Y↦E(A(Y)1B)Y\mapsto\mathbb E(\mathcal A(Y)\mathbb 1_B)Y↦E(A(Y)1B​) is upper semicontinuous on Y\mathcal YY. For B∈F1B\in\mathcal F_1B∈F1​ and Z∈Lq(F)Z\in L_q(\mathcal F)Z∈Lq​(F) the dual function is

AB(Z)=inf⁡{E(YZ)−E(A(Y)1B):Y∈Y}∈[−∞,∞).A_B(Z)=\inf\{\mathbb E(YZ)-\mathbb E(\mathcal A(Y)\mathbb 1_B):Y\in\mathcal Y\}\in[-\infty,\infty).AB​(Z)=inf{E(YZ)−E(A(Y)1B​):Y∈Y}∈[−∞,∞).

For 0<α≤10<\alpha\le10<α≤1 and Y∈L1(F)Y\in L_1(\mathcal F)Y∈L1​(F), the conditional average value-at-risk AV@Rα(Y∣F1)\mathbb{AV@R}_\alpha(Y\mid\mathcal F_1)AV@Rα​(Y∣F1​) is a class in L1(F1)L_1(\mathcal F_1)L1​(F1​) such that, for every B∈F1B\in\mathcal F_1B∈F1​,

E(AV@Rα(Y∣F1)1B)=inf⁡{E(YZ):0≤Z≤1α1B, E(Z∣F1)=1B}.\mathbb E(\mathbb{AV@R}_\alpha(Y\mid\mathcal F_1)\mathbb 1_B)=\inf\Big\{\mathbb E(YZ):0\le Z\le\tfrac1\alpha\mathbb 1_B,\ \mathbb E(Z\mid\mathcal F_1)=\mathbb 1_B\Big\}.E(AV@Rα​(Y∣F1​)1B​)=inf{E(YZ):0≤Z≤α1​1B​, E(Z∣F1​)=1B​}.

When F1\mathcal F_1F1​ is trivial it reduces to the lower-tail average AV@Rα(Y)=1α∫0αG−1(u) du\mathbb{AV@R}_\alpha(Y)=\frac1\alpha\int_0^\alpha G^{-1}(u)\,duAV@Rα​(Y)=α1​∫0α​G−1(u)du of the left-continuous quantile function G−1(u)=inf⁡{v:G(v)≥u}G^{-1}(u)=\inf\{v:G(v)\ge u\}G−1(u)=inf{v:G(v)≥u} of YYY.

Formalization targets

Goal: Theorem 2.51

For an upper semicontinuous conditional acceptability mapping A\mathcal AA, every Y∈YY\in\mathcal YY∈Y and every B∈F1B\in\mathcal F_1B∈F1​,

E(A(Y)1B)=inf⁡Z∈Lq(F){E(YZ)−AB(Z):Z≥0, E(Z∣F1)=1B},\mathbb E(\mathcal A(Y)\mathbb 1_B)=\inf_{Z\in L_q(\mathcal F)}\{\mathbb E(YZ)-A_B(Z):Z\ge0,\ \mathbb E(Z\mid\mathcal F_1)=\mathbb 1_B\},E(A(Y)1B​)=Z∈Lq​(F)inf​{E(YZ)−AB​(Z):Z≥0, E(Z∣F1​)=1B​},

and if A\mathcal AA is positively homogeneous then ABA_BAB​ takes only the values 000 (on SB={Z:AB(Z)≥0}S_B=\{Z:A_B(Z)\ge0\}SB​={Z:AB​(Z)≥0}) and −∞-\infty−∞ (off SBS_BSB​), and

E(A(Y)1B)=inf⁡Z∈SB{E(YZ):Z≥0, E(Z∣F1)=1B}.\mathbb E(\mathcal A(Y)\mathbb 1_B)=\inf_{Z\in S_B}\{\mathbb E(YZ):Z\ge0,\ \mathbb E(Z\mid\mathcal F_1)=\mathbb 1_B\}.E(A(Y)1B​)=Z∈SB​inf​{E(YZ):Z≥0, E(Z∣F1​)=1B​}.

Milestones

  1. Eqs. (2.48)–(2.49): the unconstrained form, E(A(Y)1B)=inf⁡Z∈Lq{E(YZ)−AB(Z)}\mathbb E(\mathcal A(Y)\mathbb 1_B)=\inf_{Z\in L_q}\{\mathbb E(YZ)-A_B(Z)\}E(A(Y)1B​)=infZ∈Lq​​{E(YZ)−AB​(Z)}.
  2. Theorem 2.54: a conditional acceptability mapping that is bounded below, in the order of the cone K\mathcal KK of a.s. non-negative elements of Lp(F1)L_p(\mathcal F_1)Lp​(F1​), by a bounded set on a neighbourhood of one point is continuous.
  3. Proposition 2.57 (i)–(ix): version-independence and unique existence in L1(F1)L_1(\mathcal F_1)L1​(F1​), concavity with F1\mathcal F_1F1​-measurable weights, homogeneity under bounded non-negative F1\mathcal F_1F1​-measurable factors, monotonicity, AV@Rα(Y∣F1)=Y\mathbb{AV@R}_\alpha(Y\mid\mathcal F_1)=YAV@Rα​(Y∣F1​)=Y for F1\mathcal F_1F1​-measurable YYY, reduction to AV@Rα(Y)\mathbb{AV@R}_\alpha(Y)AV@Rα​(Y) for trivial F1\mathcal F_1F1​, monotonicity in α\alphaα, AV@R1(Y∣F1)=E(Y∣F1)\mathbb{AV@R}_1(Y\mid\mathcal F_1)=\mathbb E(Y\mid\mathcal F_1)AV@R1​(Y∣F1​)=E(Y∣F1​), and the tower inequalities (2.58).

Further items of the section, stated faithfully but not milestones:

  • Example 2.53(a): E(E(Y∣F1)1B)=inf⁡{E(YZ):0≤Z≤1, E(Z∣F1)=1B}=E(Y1B)\mathbb E(\mathbb E(Y\mid\mathcal F_1)\mathbb 1_B)=\inf\{\mathbb E(YZ):0\le Z\le1,\ \mathbb E(Z\mid\mathcal F_1)=\mathbb 1_B\}=\mathbb E(Y\mathbb 1_B)E(E(Y∣F1​)1B​)=inf{E(YZ):0≤Z≤1, E(Z∣F1​)=1B​}=E(Y1B​), and E(⋅∣F1)\mathbb E(\cdot\mid\mathcal F_1)E(⋅∣F1​) maps Lp(F)L_p(\mathcal F)Lp​(F) onto Lp(F1)L_p(\mathcal F_1)Lp​(F1​).
  • Theorem 2.52: a closed convex S⊆L∞(F)S\subseteq L_\infty(\mathcal F)S⊆L∞​(F) with 1∈S\mathbb 1\in S1∈S and Z1B∈SZ\mathbb 1_B\in SZ1B​∈S defines, through E(Y1∗1B)=inf⁡Z∈S{E(YZ):Z≥0, E(Z∣F1)=1B}\mathbb E(Y_1^*\mathbb 1_B)=\inf_{Z\in S}\{\mathbb E(YZ):Z\ge0,\ \mathbb E(Z\mid\mathcal F_1)=\mathbb 1_B\}E(Y1∗​1B​)=infZ∈S​{E(YZ):Z≥0, E(Z∣F1​)=1B​}, a positively homogeneous u.s.c. conditional acceptability mapping on L1L_1L1​.
  • Example 2.53(b): AV@Rα(⋅∣F1)\mathbb{AV@R}_\alpha(\cdot\mid\mathcal F_1)AV@Rα​(⋅∣F1​) is well defined on L1(F)L_1(\mathcal F)L1​(F) and is a positively homogeneous u.s.c. conditional acceptability mapping.

Significance

Theorem 2.51 says that a conditional acceptability mapping is determined by the family of real concave functionals Y↦E(A(Y)1B)Y\mapsto\mathbb E(\mathcal A(Y)\mathbb 1_B)Y↦E(A(Y)1B​), and that each of these is an infimum of expectations under densities whose conditional expectation is 1B\mathbb 1_B1B​. It turns the axioms (CA1)–(CA3) into a computable object: a dual set, one per observable event, which is what stochastic programs with conditional risk constraints actually optimize over. The converse direction (Theorem 2.52 and Example 2.53) is how the book manufactures conditional versions of the average value-at-risk and of other dual-representable functionals, and Proposition 2.57 lists the properties used later when these mappings are nested over a tree.

None of these results is formalized. Mathlib has conditional expectation, LpL_pLp​ spaces, Hölder duality and the Hahn–Banach separation theorem, but no Fenchel–Moreau theorem on LpL_pLp​ and no conditional risk mappings. Prove2Me poses, as an open problem, Ruszczyński and Shapiro's representation of lower semicontinuous conditional risk mappings (CondRiskMap.Repr.theorem_1); it is stated pointwise in ω\omegaω on abstract paired spaces with loss variables, not in the integrated form over events B∈F1B\in\mathcal F_1B∈F1​ used here. Two of the printed statements are false as stated, and the mission records this: see Beyond the paper below.

Difficulty

The obvious route to (2.45) applies the Fenchel–Moreau theorem to hBh_BhB​ and then shows that the dual function is −∞-\infty−∞ off the constraint set. The first step needs the biconjugation theorem for concave upper semicontinuous real functionals on LpL_pLp​, with the dual identified as LqL_qLq​, for every p∈[1,∞)p\in[1,\infty)p∈[1,∞) including p=1p=1p=1 where the dual is L∞L_\inftyL∞​; none of this is in Mathlib. The second step must handle the constraint E(Z∣F1)=1B\mathbb E(Z\mid\mathcal F_1)=\mathbb 1_BE(Z∣F1​)=1B​ as an equality of conditional expectations, not of expectations. For Theorem 2.52 the natural argument builds a measure on F1\mathcal F_1F1​ from the infimum and takes its Radon–Nikodym derivative; the additivity of that set function is exactly what fails for general SSS.

Formalization scope

Y\mathcal YY is Lp ℝ p P with 1 ≤ p, p ≠ ∞, and Y1\mathcal Y_1Y1​ is Mathlib's subspace lpMeas ℝ ℝ m p P of classes a.e. equal to an m-measurable function, where m ≤ mΩ is F1\mathcal F_1F1​; the dual exponent is given by p.HolderConjugate q. Pointwise axioms are almost sure. E(Z∣F1)\mathbb E(Z\mid\mathcal F_1)E(Z∣F1​) is Mathlib's P[Z|m]. Every infimum, and the dual function ABA_BAB​, is computed in EReal, so an empty constraint set gives +∞+\infty+∞, an unbounded one −∞-\infty−∞, and no infimum has a junk value; the difference E(YZ)−AB(Z)\mathbb E(YZ)-A_B(Z)E(YZ)−AB​(Z) always has a real first term. Upper semicontinuity is that of the real functionals indexed by B∈F1B\in\mathcal F_1B∈F1​, as the book defines it — reading it as upper semicontinuity of the map into Lp(F1)L_p(\mathcal F_1)Lp​(F1​), or replacing the infimum by an unconstrained one over all of LqL_qLq​, would change the theorem. The conditional AV@R\mathbb{AV@R}AV@R is a predicate on classes in L1(F1)L_1(\mathcal F_1)L1​(F1​), never a construction: its existence is a stated result, not an assumption. Profits, not losses: the lower tail is averaged. Version-independence (Definition 2.55, used in Proposition 2.57(i)) is stated pointwise: the conditional AV@Rα\mathbb{AV@R}_\alphaAV@Rα​ is almost surely one fixed function of the conditional distribution function G(⋅∣F1)(ω)G(\cdot\mid\mathcal F_1)(\omega)G(⋅∣F1​)(ω) of (2.56), for every YYY.

Needed infrastructure: the Fenchel–Moreau theorem on LpL_pLp​, the LpL_pLp​–LqL_qLq​ duality pairing, and Radon–Nikodym on a sub-σ\sigmaσ-field. All three are reusable well beyond this mission.

Beyond the paper. Two corrected variants are posed beside the faithful statements. Theorem 2.52, corrected (findings F1, F2) adds that SSS is bounded in L∞L_\inftyL∞​ and closed under pasting along F1\mathcal F_1F1​; without pasting, S={E(Z2)≤1, ∥Z∥∞≤2}S=\{\mathbb E(Z^2)\le1,\ \|Z\|_\infty\le2\}S={E(Z2)≤1, ∥Z∥∞​≤2} on [0,1][0,1][0,1] makes the right side of (2.50) non-additive in BBB, and without boundedness S=L∞S=L_\inftyS=L∞​ with Y(ω)=−ω−1/2Y(\omega)=-\omega^{-1/2}Y(ω)=−ω−1/2 makes it −∞-\infty−∞. Proposition 2.57, corrected (finding F3) replaces the second inequality of (2.58), E[AV@Rα(Y∣F2)∣F1]≤AV@Rα(E(Y∣F2)∣F1)\mathbb E[\mathbb{AV@R}_\alpha(Y\mid\mathcal F_2)\mid\mathcal F_1]\le\mathbb{AV@R}_\alpha(\mathbb E(Y\mid\mathcal F_2)\mid\mathcal F_1)E[AV@Rα​(Y∣F2​)∣F1​]≤AV@Rα​(E(Y∣F2​)∣F1​), which fails on two equally likely points with Y=(0,1)Y=(0,1)Y=(0,1), F1\mathcal F_1F1​ trivial, F2\mathcal F_2F2​ full and α=12\alpha=\frac12α=21​, by AV@Rα(Y∣F1)≤AV@Rα(E(Y∣F2)∣F1)\mathbb{AV@R}_\alpha(Y\mid\mathcal F_1)\le\mathbb{AV@R}_\alpha(\mathbb E(Y\mid\mathcal F_2)\mid\mathcal F_1)AV@Rα​(Y∣F1​)≤AV@Rα​(E(Y∣F2​)∣F1​). Disproofs of the faithful Theorem 2.52 and of the faithful Proposition 2.57 are welcome contributions, as are proofs of the variants.

Selected references

  • G. Ch. Pflug, W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007. doi:10.1142/6478
  • A. Ruszczyński, A. Shapiro, Conditional risk mappings, Mathematics of Operations Research 31(3), 2006. doi:10.1287/moor.1060.0204
  • K. Detlefsen, G. Scandolo, Conditional and dynamic convex risk measures, Finance and Stochastics 9(4), 2005. doi:10.1007/s00780-005-0159-6
  • K. Nikodem, Continuity properties of convex-type set-valued maps, Journal of Inequalities in Pure and Applied Mathematics 4(3), Article 52, 2003. http://jipam.vu.edu.au
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Modeling, Measuring and Managing Risk II: Dual Representation of Acceptability FunctionalsTextbook

Motivation

Risk functionals assign a number to an uncertain profit and are used as objectives and constraints in portfolio selection, insurance and energy planning. Since the axiomatization of coherent risk measures by Artzner, Delbaen, Eber and Heath (Math. Finance 1999), the standard way to understand such a functional is through a dual representation: the functional is written as a worst case of expectations under a family of probability densities, penalized by a convex or concave function of the density. Föllmer and Schied (Finance Stoch. 2002) and Ruszczyński and Shapiro (Math. Oper. Res. 2006) established this representation for convex risk measures on L∞L_\inftyL∞​ and on paired spaces. Pflug and Römisch, Modeling, Measuring and Managing Risk (World Scientific 2007), develop the same theory on the profit side, for acceptability functionals (larger is better) and deviation risk functionals, on LpL_pLp​ spaces. Section 2.2 of their book recognizes these functionals by their dual representations. This mission formalizes that section and the conjugate duality of Appendix B it rests on.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a non-atomic probability space: no measurable AAA with P(A)>0P(A)>0P(A)>0 has every measurable subset of probability 000 or P(A)P(A)P(A) (the book assumes this throughout). Fix 1≤p<∞1\le p<\infty1≤p<∞ and q∈(1,∞]q\in(1,\infty]q∈(1,∞] with 1p+1q=1\frac1p+\frac1q=1p1​+q1​=1. Write Y=Lp(Ω,F,P)\mathcal Y=L_p(\Omega,\mathcal F,P)Y=Lp​(Ω,F,P) and Z=Lq(Ω,F,P)\mathcal Z=L_q(\Omega,\mathcal F,P)Z=Lq​(Ω,F,P), paired by

⟨Y,Z⟩=E(YZ)=∫ΩYZ dP.\langle Y,Z\rangle=\mathbb E(YZ)=\int_\Omega Y Z\,dP .⟨Y,Z⟩=E(YZ)=∫Ω​YZdP.

A functional is a map A:Y→[−∞,+∞]\mathcal A:\mathcal Y\to[-\infty,+\infty]A:Y→[−∞,+∞]; constants ccc are constant random variables. An acceptability functional satisfies

  • (A1) A(Y+c)=A(Y)+c\mathcal A(Y+c)=\mathcal A(Y)+cA(Y+c)=A(Y)+c,
  • (A2) A(λY(1)+(1−λ)Y(2))≥λA(Y(1))+(1−λ)A(Y(2))\mathcal A(\lambda Y^{(1)}+(1-\lambda)Y^{(2)})\ge\lambda\mathcal A(Y^{(1)})+(1-\lambda)\mathcal A(Y^{(2)})A(λY(1)+(1−λ)Y(2))≥λA(Y(1))+(1−λ)A(Y(2)) for 0≤λ≤10\le\lambda\le10≤λ≤1, and
  • (A3) Y(1)≤Y(2)Y^{(1)}\le Y^{(2)}Y(1)≤Y(2) a.s. ⇒A(Y(1))≤A(Y(2))\Rightarrow\mathcal A(Y^{(1)})\le\mathcal A(Y^{(2)})⇒A(Y(1))≤A(Y(2)).

Positive homogeneity (A4) is A(λY)=λA(Y)\mathcal A(\lambda Y)=\lambda\mathcal A(Y)A(λY)=λA(Y) for λ≥0\lambda\ge0λ≥0, and strictness (A5) is A(Y)≤E(Y)\mathcal A(Y)\le\mathbb E(Y)A(Y)≤E(Y). A deviation risk functional D\mathcal DD satisfies (D1) D(Y+c)=D(Y)\mathcal D(Y+c)=\mathcal D(Y)D(Y+c)=D(Y), (D2) convexity, and (D3) X≤Y⇒E(X)−D(X)≤E(Y)−D(Y)X\le Y\Rightarrow\mathbb E(X)-\mathcal D(X)\le\mathbb E(Y)-\mathcal D(Y)X≤Y⇒E(X)−D(X)≤E(Y)−D(Y). The acceptance set of A\mathcal AA is SA={Y:A(Y)≥0}\mathcal S_{\mathcal A}=\{Y:\mathcal A(Y)\ge0\}SA​={Y:A(Y)≥0}, and a set S\mathcal SS defines AS(Y)=sup⁡{a:Y−a∈S}\mathcal A_{\mathcal S}(Y)=\sup\{a: Y-a\in\mathcal S\}AS​(Y)=sup{a:Y−a∈S}.

The concave conjugate and the convex conjugate are

A+(Z)=inf⁡Y∈Y{E(YZ)−A(Y)},D∗(Z)=sup⁡Y∈Y{E(YZ)−D(Y)},\mathcal A^+(Z)=\inf_{Y\in\mathcal Y}\{\mathbb E(YZ)-\mathcal A(Y)\},\qquad \mathcal D^*(Z)=\sup_{Y\in\mathcal Y}\{\mathbb E(YZ)-\mathcal D(Y)\},A+(Z)=Y∈Yinf​{E(YZ)−A(Y)},D∗(Z)=Y∈Ysup​{E(YZ)−D(Y)},

and h∗∗(Y)=sup⁡Z{E(YZ)−h∗(Z)}h^{**}(Y)=\sup_{Z}\{\mathbb E(YZ)-h^*(Z)\}h∗∗(Y)=supZ​{E(YZ)−h∗(Z)}. A convex-type hhh is proper if h>−∞h>-\inftyh>−∞ everywhere and h<+∞h<+\inftyh<+∞ somewhere; a concave-type ggg is proper if −g-g−g is.

Formalization targets

Goal: Corollary 2.32, representation (2.11)

A proper upper semicontinuous acceptability functional satisfies, for every Y∈YY\in\mathcal YY∈Y,

A(Y)=inf⁡{E(YZ)−A+(Z): Z∈Lq, EZ=1, Z≥0},\mathcal A(Y)=\inf\{\mathbb E(YZ)-\mathcal A^+(Z):\ Z\in L_q,\ \mathbb EZ=1,\ Z\ge0\},A(Y)=inf{E(YZ)−A+(Z): Z∈Lq​, EZ=1, Z≥0},

and conversely, a functional represented in this form by any proper functional in place of A+\mathcal A^+A+ is upper semicontinuous and satisfies (A1)–(A3). Up to semicontinuity, acceptability functionals are exactly the penalized infima of expectations under probability densities.

Milestones

  1. Proposition 2.26: (A1) together with u.s.c., (A2), (A3), (A4) or (A5) make SA\mathcal S_{\mathcal A}SA​ closed, convex, monotone, a cone, or disjoint from {E<0}\{\mathbb E<0\}{E<0}, respectively.
  2. Proposition 2.27: the converse passage from a set S\mathcal SS to AS\mathcal A_{\mathcal S}AS​, as printed.
  3. Theorem B.1 (Fenchel–Moreau–Rockafellar): h∗∗=hh^{**}=hh∗∗=h for proper, l.s.c., convex hhh on LpL_pLp​.
  4. Theorem 2.30, (A)(i)–(iv) and (B)(vi)–(ix): sufficient conditions on a dual representation for (A1), (A4), version independence, (A3) and first-order dominance, and for (D1), (D4), version independence and (D3).
  5. Theorem 2.31: necessary conditions on the conjugate. Under (A1), A+(Z)>−∞\mathcal A^+(Z)>-\inftyA+(Z)>−∞ implies EZ=1\mathbb E Z=1EZ=1. Under (A4), A+∈{0,−∞}\mathcal A^+\in\{0,-\infty\}A+∈{0,−∞}. Under (A3), P{Z<0}>0P\{Z<0\}>0P{Z<0}>0 implies A+(Z)=−∞\mathcal A^+(Z)=-\inftyA+(Z)=−∞. Antitonicity under conditional expectation passes to A+\mathcal A^+A+. Items (v)–(vii) are the deviation mirrors.

Further items, not milestones: the first sentence of Theorem B.1 (h∗∗h^{**}h∗∗ is the largest l.s.c. convex minorant of a proper hhh) and the deviation half of Corollary 2.32, representation (2.12), each stated as printed.

Significance

The corollary is the profit-side, LpL_pLp​ form of the dual representation of convex risk measures. It turns a property of a functional into a constraint on its dual domain. Translation equivariance becomes the requirement that the densities ZZZ have mean one, and monotonicity becomes the requirement that they be nonnegative. This is how later chapters of the book compute with the average value-at-risk, distortion functionals and multi-period functionals: each is specified by its supergradient set. A machine-checked version gives these computations a common, verified foundation.

The results are classical and proved on paper; none is formalized in this form. The platform holds a loss-side analogue on abstract paired spaces with signed-measure duals (ConvexRiskFn.Dual.theorem_2_2) and a Fenchel–Moreau theorem in the same setting (ConvexRiskFn.Dual.theorem_2_1). Neither states the LpL_pLp​/LqL_qLq​, profit-side, density-constrained representation (2.11). Formalizing the chapter also checks its statements: three printed statements are false as written, and the mission poses a corrected form beside each faithful one.

Difficulty

Representation (2.11) needs the Fenchel–Moreau theorem in infinite dimension, for an extended-real concave functional, on LpL_pLp​ with dual LqL_qLq​. That requires Hahn–Banach separation of a closed convex hypograph and the identification of the dual of LpL_pLp​, and Mathlib provides only parts of the latter. Upper semicontinuity in the norm topology must be converted to weak semicontinuity, and the value −∞-\infty−∞ must be handled throughout. Example 2.28 of the book shows that dropping upper semicontinuity breaks the representation, so the hypothesis cannot be avoided. The restriction of the infimum to densities with EZ=1\mathbb EZ=1EZ=1, Z≥0Z\ge0Z≥0 is a separate step: one must show that every other ZZZ has A+(Z)=−∞\mathcal A^+(Z)=-\inftyA+(Z)=−∞. The first sentence of Theorem B.1 fails as printed when hhh has no continuous affine minorant, so the natural "largest l.s.c. convex minorant" route to the biconjugate needs care.

Formalization scope

Functionals are EReal-valued maps on Mathlib's Lp ℝ p P, with p ≠ ⊤, [Fact (1 ≤ p)] and [p.HolderConjugate q]. The pairing is the Bochner integral of YZYZYZ, integrable by Hölder's inequality. Conjugates are EReal suprema and infima over the whole space, so they are never a junk default. (A2), (D2) and (A4) are written as the book's inequalities in EReal, where 0⋅(±∞)=00\cdot(\pm\infty)=00⋅(±∞)=0. Non-atomicity is the book's atom definition, which is stronger than Mathlib's NoAtoms. Semicontinuity is for the norm topology. "Proper" follows the concave or convex notion of Appendix B. The book's abstract dual pair is instantiated as (Lp,Lq)(L_p,L_q)(Lp​,Lq​) with 1≤p<∞1\le p<\infty1≤p<∞, the example it gives itself.

A trivializing formalization would take the infimum in (2.11) over all of LqL_qLq​ (Fenchel–Moreau alone), or replace A+\mathcal A^+A+ by a real-valued function and so discard the −∞-\infty−∞ values that encode the constraints. The goal does neither: the infimum ranges over the densities, and A+\mathcal A^+A+ is the EReal conjugate.

Beyond the paper. There are three variants, each a corrected statement beside its faithful one:

  • deviation_representation_corrected (F1): (2.12) prints inf⁡\infinf where sup⁡\supsup is meant. For D=E−AV@R1/2\mathcal D=\mathbb E-\mathbb{AV@R}_{1/2}D=E−AV@R1/2​ and Y=±1Y=\pm1Y=±1, D(Y)=1\mathcal D(Y)=1D(Y)=1, but Z=−YZ=-YZ=−Y gives −1-1−1.
  • fenchel_moreau_largest_corrected (F2): Theorem B.1's first sentence needs h∗≢+∞h^*\not\equiv+\inftyh∗≡+∞. For h=−(EY)2h=-(\mathbb EY)^2h=−(EY)2 on {EY≥0}\{\mathbb EY\ge0\}{EY≥0}, h∗∗≡−∞h^{**}\equiv-\inftyh∗∗≡−∞ is not the largest l.s.c. convex minorant.
  • acceptabilityOfSet_properties_corrected (F3): Proposition 2.27(i) needs a monotone S\mathcal SS (a closed set built from line segments gives AS(1n1B)=2n\mathcal A_{\mathcal S}(\tfrac1n1_B)=2nAS​(n1​1B​)=2n but AS(0)=0\mathcal A_{\mathcal S}(0)=0AS​(0)=0), and (v) holds only for λ>0\lambda>0λ>0 (S=∅\mathcal S=\emptysetS=∅).

A complete development needs Fenchel–Moreau for extended-real functionals on LpL_pLp​, the duality Lp∗≅LqL_p^*\cong L_qLp∗​≅Lq​ for 1≤p<∞1\le p<\infty1≤p<∞, and coupling constructions on non-atomic spaces for version independence. All of these are reusable well beyond risk theory. Contributions of any of these pieces, or proofs of the corrected variants, are welcome.

Selected references

  • G. Ch. Pflug, W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007. https://doi.org/10.1142/6478
  • P. Artzner, F. Delbaen, J.-M. Eber, D. Heath, Coherent measures of risk, Mathematical Finance 9 (1999) 203–228. https://doi.org/10.1111/1467-9965.00068
  • H. Föllmer, A. Schied, Convex measures of risk and trading constraints, Finance and Stochastics 6 (2002) 429–447. https://doi.org/10.1007/s007800200072
  • A. Ruszczyński, A. Shapiro, Optimization of convex risk functions, Mathematics of Operations Research 31 (2006) 433–452. https://doi.org/10.1287/moor.1050.0186
  • R. T. Rockafellar, Conjugate Duality and Optimization, SIAM, 1974. https://doi.org/10.1137/1.9781611970524
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Algorithmic Game TheoryEconomicsOperations Research+1·Captain: Shuze Chen

Food Delivery Service and Restaurant: Friend or Foe?: With Convenient Delivery, a Critical Mass of Tech-Savvy Customers Makes the Restaurant Delivery-Only and Cuts Platform Profit and WelfareResearch Paper

Motivation

Food delivery platforms such as Uber Eats, DoorDash and Meituan let a restaurant serve customers who never enter it, but they also charge those customers a delivery fee and share the restaurant's kitchen with its walk-in trade. Whether the platform helps or hurts the restaurant is a question restaurant owners, platforms and regulators all ask. Chen, Hu and Wang (Management Science, 2022) answer it in a stylized game: a restaurant whose kitchen is a queue, a platform that sets a fee, and two kinds of customers who decide where to eat by comparing expected waiting costs. Their first main result, Proposition 1, describes how the equilibrium changes as more customers become able to order through the platform: below a critical mass nothing changes for the restaurant, and at the critical mass the restaurant abruptly turns into a delivery-only kitchen. The analysis builds on the unobservable-queue joining games of Edelson and Hilderbrand (1975) and Hassin and Haviv (2003).

Setting

A kitchen serves meals at rate μ>0\mu>0μ>0. At total joining rate λ<μ\lambda<\muλ<μ the expected wait for food is 1/(μ−λ)1/(\mu-\lambda)1/(μ−λ). A meal is worth RRR to a customer. Walk-in customers pay the food price ppp and incur waiting cost rate c>0c>0c>0; food-delivery customers pay ppp plus the delivery fee θ\thetaθ and incur the smaller waiting cost rate ϕ∈[0,c)\phi\in[0,c)ϕ∈[0,c). Their expected utilities are

UW(λ)=R−p−cμ−λ,UD(λ)=R−p−θ−ϕμ−λ,U_W(\lambda)=R-p-\frac{c}{\mu-\lambda},\qquad U_D(\lambda)=R-p-\theta-\frac{\phi}{\mu-\lambda},UW​(λ)=R−p−μ−λc​,UD​(λ)=R−p−θ−μ−λϕ​,

and balking gives 000. Tech-savvy customers arrive at rate Λ1∈(0,μ)\Lambda_1\in(0,\mu)Λ1​∈(0,μ) and may walk in, use delivery or balk; traditional customers arrive at rate Λ0≥μ\Lambda_0\ge\muΛ0​≥μ and may walk in or balk. The delivery-worker pool is unlimited and costless.

A customers' equilibrium under (p,θ)(p,\theta)(p,θ) is a profile of joining rates (λD,λ1W,λ0W)(\lambda_D,\lambda_{1W},\lambda_{0W})(λD​,λ1W​,λ0W​) with λ=λD+λ1W+λ0W<μ\lambda=\lambda_D+\lambda_{1W}+\lambda_{0W}<\muλ=λD​+λ1W​+λ0W​<μ in which every option used by a positive rate is a best reply at λ\lambdaλ, and an arrival stream that does not fully join is no better off joining. Ties between delivery and walking in at UD=UW≥0U_D=U_W\ge0UD​=UW​≥0 go to delivery. The game has three stages. The restaurant sets p≥0p\ge0p≥0. The platform then sets θ≥0\theta\ge0θ≥0 to maximize π=θλD\pi=\theta\lambda_Dπ=θλD​. Finally customers play an equilibrium. The restaurant maximizes Π=p(λD+λW)\Pi=p(\lambda_D+\lambda_W)Π=p(λD​+λW​), where λW=λ0W+λ1W\lambda_W=\lambda_{0W}+\lambda_{1W}λW​=λ0W​+λ1W​. A subgame-perfect equilibrium (SPE) combines a customers' equilibrium after every (p,θ)(p,\theta)(p,θ), a best-response fee after every ppp, and an optimal price p∗p^*p∗. Its outcome is p∗p^*p∗, θ∗\theta^*θ∗, λD∗\lambda^*_DλD∗​, λW∗\lambda^*_WλW∗​, Π∗\Pi^*Π∗, π∗\pi^*π∗ and the social welfare S∗=Π∗+π∗+λD∗UD+λW∗UWS^*=\Pi^*+\pi^*+\lambda^*_DU_D+\lambda^*_WU_WS∗=Π∗+π∗+λD∗​UD​+λW∗​UW​, the total surplus of all stakeholders.

Formalization targets

Goal: Proposition 1 (p. 8)

Assume μ>0\mu>0μ>0, c>0c>0c>0, c<Rμc<R\muc<Rμ, Λ0≥μ\Lambda_0\ge\muΛ0​≥μ. There is ϕ1\phi_1ϕ1​ such that for every ϕ∈[0,c)\phi\in[0,c)ϕ∈[0,c) there are λ1∈(0,μ)\lambda_1\in(0,\mu)λ1​∈(0,μ) and an SPE for every Λ1∈(0,μ)\Lambda_1\in(0,\mu)Λ1​∈(0,μ) whose outcome, viewed as a function of Λ1\Lambda_1Λ1​, satisfies the following. With I=(0,μ)I=(0,\mu)I=(0,μ) if ϕ>ϕ1\phi>\phi_1ϕ>ϕ1​ and I=(0,λ1]I=(0,\lambda_1]I=(0,λ1​] otherwise:

  1. on III, p∗p^*p∗ and λD∗+λW∗\lambda^*_D+\lambda^*_WλD∗​+λW∗​ are constant, and π∗\pi^*π∗, S∗S^*S∗, λD∗\lambda^*_DλD∗​, −λW∗-\lambda^*_W−λW∗​ are weakly increasing;
  2. if ϕ≤ϕ1\phi\le\phi_1ϕ≤ϕ1​,
p∗(a)<p∗(b)  (a≤λ1<b),π∗(λ1)>lim⁡Λ1↘λ1π∗,S∗(λ1)>lim⁡Λ1↘λ1S∗;p^*(a)<p^*(b)\ \ (a\le\lambda_1<b),\qquad \pi^*(\lambda_1)>\lim_{\Lambda_1\searrow\lambda_1}\pi^*,\qquad S^*(\lambda_1)>\lim_{\Lambda_1\searrow\lambda_1}S^*;p∗(a)<p∗(b)  (a≤λ1​<b),π∗(λ1​)>Λ1​↘λ1​lim​π∗,S∗(λ1​)>Λ1​↘λ1​lim​S∗;
  1. if ϕ<c/(2Rμ/c−1)\phi<c/(2\sqrt{R\mu/c}-1)ϕ<c/(2Rμ/c​−1), then c/(2Rμ/c−1)≤ϕ1c/(2\sqrt{R\mu/c}-1)\le\phi_1c/(2Rμ/c​−1)≤ϕ1​ and λD∗+λW∗\lambda^*_D+\lambda^*_WλD∗​+λW∗​ on (0,λ1](0,\lambda_1](0,λ1​] is below its limit as Λ1↗μ\Lambda_1\nearrow\muΛ1​↗μ.

The thresholds are existential, as printed. The milestones pin them to the values the proof constructs: χ\chiχ is the root of −Rχ3−μϕχ+2μ2ϕ-R\chi^3-\mu\phi\chi+2\mu^2\phi−Rχ3−μϕχ+2μ2ϕ in [0,μ][0,\mu][0,μ], λ2=μ−χ\lambda_2=\mu-\chiλ2​=μ−χ, λ1\lambda_1λ1​ is the smallest root of λ(R−μϕ/(μ−λ)2)=(Rμ−c)2\lambda(R-\mu\phi/(\mu-\lambda)^2)=(\sqrt{R\mu}-\sqrt c)^2λ(R−μϕ/(μ−λ)2)=(Rμ​−c​)2, and ϕ1\phi_1ϕ1​ has a closed form (Online Appendix p. 23).

Milestones

The paper's own chain (Online Appendix C.1): Lemma C.2 (customers' equilibrium), Proposition C.3 (platform's best response), Corollary C.2 (restaurant's profit curve), Lemmas C.6–C.8 (the three profit curves, their maxima and intersections), Proposition C.4 (restaurant's optimal price), and Corollaries C.3–C.4 (platform profit and welfare in equilibrium). "We have Proposition 1 from Proposition C.4, Corollary C.3 and Corollary C.4."

Significance

The result separates two regimes. In the delivery-irrelevant regime, more tech-savvy customers only change who eats at the restaurant; the price and the throughput are fixed while the platform's profit and welfare grow. Past the critical mass λ1\lambda_1λ1​, the restaurant raises its price and serves only delivery customers, and the platform's profit and social welfare drop. This is the basis of the paper's answer to "friend or foe" and of its later analysis of revenue-sharing contracts that restore coordination (Proposition 2, not part of this mission).

The paper's proof is a long chain of case analyses over piecewise-defined profit functions, spread over 22 pages of appendix. A machine-checked version settles every boundary case. Reading the proof closely has already turned up several (findings F1–F9): ties in the restaurant's optimum at Λ1=λ1\Lambda_1=\lambda_1Λ1​=λ1​ and at ϕ=ϕ1\phi=\phi_1ϕ=ϕ1​; table rows that are wrong outside their derived price range; an implicit hypothesis c<Rμc<R\muc<Rμ; the degenerate case ϕ=0\phi=0ϕ=0; a tie rule that needs a precise reading; and a boundary error in Lemma C.7(3). The definitions of the queue-joining equilibrium and the three-stage Stackelberg game can be reused for other platform and queueing games. None of this has been formalized before.

Difficulty

The equilibrium is defined by optimality conditions, so each stage needs an existence-and-characterization argument, not a formula check. The customers' stage has mixed strategies with three utility comparisons and a tie rule. The platform's profit is piecewise in θ\thetaθ, with branches that switch depending on ppp and on whether Λ1≶c−ϕcμ\Lambda_1\lessgtr\frac{c-\phi}{c}\muΛ1​≶cc−ϕ​μ. The restaurant's profit is the upper envelope of three curves whose maxima must be compared through the cubic defining χ\chiχ and a quartic-type equation defining λ1\lambda_1λ1​. The obvious approach, substituting the tables, fails at the boundaries. At Λ1=λ1\Lambda_1=\lambda_1Λ1​=λ1​ and at ϕ=ϕ1\phi=\phi_1ϕ=ϕ1​ the restaurant has two optimal prices with different platform profits, so "the" equilibrium price is not unique. The jump statements are therefore about a particular equilibrium selection and about one-sided limits.

Formalization scope

All objects live in FoodDeliv.Decentral, with one definitions file, FoodDeliv_Decentral_Model. Conventions:

  • Parameters are real; the standing assumptions are μ>0\mu>0μ>0, c>0c>0c>0, 0≤ϕ<c0\le\phi<c0≤ϕ<c, Λ0≥μ\Lambda_0\ge\muΛ0​≥μ, 0<Λ1<μ0<\Lambda_1<\mu0<Λ1​<μ (the paper's focus, Online Appendix p. 7), and c<Rμc<R\muc<Rμ, which the paper uses ("Rμ/c>1R\mu/c>1Rμ/c>1") without stating it.
  • Prices and fees range over p≥0p\ge0p≥0, θ≥0\theta\ge0θ≥0.
  • The tie rule reads: at UD=UW≥0U_D=U_W\ge0UD​=UW​≥0 no tech-savvy customer walks in, and none balks while traditional customers walk in.
  • S∗S^*S∗ includes the customers' surplus. The equilibrium is defined by optimality conditions, never by the paper's tables. λ1∈(0,μ)\lambda_1\in(0,\mu)λ1​∈(0,μ), and an SPE is required at λ1\lambda_1λ1​ itself. The jumps compare the value at λ1\lambda_1λ1​ with the right limit, and every limit is asserted to exist.
  • "p∗p^*p∗" in the goal is read existentially, as an SPE selection, because of the ties; in Proposition C.4 it is read as "the table's price is optimal". Proposition 1 keeps ϕ=0\phi=0ϕ=0. The milestones about a fixed ϕ\phiϕ assume ϕ>0\phi>0ϕ>0, because at ϕ=0\phi=0ϕ=0 the delivery utility does not depend on congestion and the demand under some fees is not determined.
  • Lemma C.2's last row and Corollary C.2's last rows are stated on the price range the paper derives them for. Lemma C.7 omits item 3 and Lemma C.8 omits item 2.

Beyond the paper. No variant items are posed. The findings file records the evidence for each deviation above.

Contributions welcome: proofs of the milestones in any order; existence of customers' equilibria for every (p,θ)(p,\theta)(p,θ) under the tie rule; reusable lemmas on unimodal functions, cubic roots and one-sided limits of piecewise functions.

Selected references

  • M. Chen, M. Hu, J. Wang, Food Delivery Service and Restaurant: Friend or Foe?, Management Science, 2022. https://doi.org/10.1287/mnsc.2021.4245 (author version: SSRN 3469971, https://ssrn.com/abstract=3469971)
  • N. M. Edelson, D. K. Hilderbrand, Congestion Tolls for Poisson Queuing Processes, Econometrica 43(1), 1975. https://doi.org/10.2307/1911385
  • R. Hassin, M. Haviv, To Queue or Not to Queue: Equilibrium Behavior in Queueing Systems, Springer, 2003. https://doi.org/10.1007/978-1-4615-0359-0
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Functional AnalysisMathematical PhysicsRepresentation Theory·Captain: mikedeng1

C*-Algebras and Direct Integral Decomposition for Lie Supergroups: Unitary Representations of a Lie Supergroup and Nondegenerate -Representations of Its C-Algebra Form Isomorphic CategoriesResearch Paper

Motivation

Unitary representations turn symmetries into operators on Hilbert spaces. For ordinary locally compact groups, the associated group C∗C^*C∗-algebra lets one study these operators through a single algebraic object. A Lie supergroup adds odd infinitesimal symmetries to an ordinary Lie group. Its unitary representations must respect both the group action and those odd operators. Neeb and Salmasian construct a C∗C^*C∗-algebra A(G,g)\mathcal A(G,\mathfrak g)A(G,g) that captures this combined structure Neeb–Salmasian 2015. The representation correspondence is the point at which their construction becomes useful: a representation of A\mathcal AA retains precisely the data of a unitary supergroup representation.

The paper subsequently uses this bridge to discuss direct integral decompositions through the C∗C^*C∗-algebra. This mission concerns the bridge itself, Theorem 6.4. Its input is not a special connected or nilpotent group: the paper works with an arbitrary finite-dimensional Lie supergroup. The later CCR results in §7 add hypotheses and are outside this mission.

Setting

A finite-dimensional Lie supergroup is a pair (G,g)(G,\mathfrak g)(G,g). Here GGG is a real Lie group and g=g0ˉ⊕g1ˉ\mathfrak g=\mathfrak g_{\bar 0}\oplus\mathfrak g_{\bar 1}g=g0ˉ​⊕g1ˉ​ is a real Lie superalgebra. Its even part g0ˉ\mathfrak g_{\bar 0}g0ˉ​ is the Lie algebra of GGG. The group acts smoothly on the superalgebra by an adjoint action whose even restriction is the derivative of conjugation; differentiation of the action recovers the superbracket. These are the conditions of Definition 2.1, including the finite-dimensional convention stated just after it.

A unitary representation consists of a graded complex Hilbert space H=H0ˉ⊕H1ˉ\mathcal H=\mathcal H_{\bar 0}\oplus\mathcal H_{\bar 1}H=H0ˉ​⊕H1ˉ​, a strongly continuous unitary action π\piπ of GGG preserving that grading, and a real-linear superalgebra action ρπ\rho^\piρπ on the space H∞\mathcal H^\inftyH∞ of smooth orbit vectors. On even elements, ρπ\rho^\piρπ equals the derived group action. On odd elements, e−πi/4ρπ(x)e^{-\pi i/4}\rho^\pi(x)e−πi/4ρπ(x) is symmetric, and the odd action transforms under GGG through the adjoint action. This is Definition 2.3, including its parity and bracket requirements.

The paper adjoins a parity element ε\varepsilonε and writes Gε=G×{1,ε}G_\varepsilon=G\times\{1,\varepsilon\}Gε​=G×{1,ε}. A test function on this group is a pair of smooth, compactly supported complex functions on GGG. Using the complex universal enveloping algebra, the authors form an algebraic crossed product A∘\mathcal A^\circA∘. A word D=x1⋯xkD=x_1\cdots x_kD=x1​⋯xk​ and a test function fff act in each unitary representation by the bounded operator ρπ(D)π(f)\rho^\pi(D)\pi(f)ρπ(D)π(f). The norm of an algebraic element is the supremum of the norms of these represented operators; completion after quotienting its zero seminorm gives the non-unital C∗C^*C∗-algebra A=A(G,g)\mathcal A=\mathcal A(G,\mathfrak g)A=A(G,g) §§3–4.

A star representation of A\mathcal AA on H\mathcal HH is nondegenerate when the span of its image applied to H\mathcal HH is dense. A morphism between two unitary supergroup representations is a bounded, even, complex-linear operator intertwining both their GGG-actions and their g\mathfrak gg-actions on smooth vectors. A morphism between C∗C^*C∗-algebra representations intertwines every element of A\mathcal AA.

Formalization targets

Uniform control and smooth multiplier action

The first targets are the uniform bound of Proposition 3.2 and the smoothness statement of Proposition 5.1. For each word DDD and test pair fff, the same constant works for every unitary representation:

∃MD,f>0∀(π,ρπ,H),∥ρπ(D)π(f)∥≤MD,f.\exists M_{D,f}>0\quad\forall(\pi,\rho^\pi,\mathcal H),\qquad \|\rho^\pi(D)\pi(f)\|\le M_{D,f}.∃MD,f​>0∀(π,ρπ,H),∥ρπ(D)π(f)∥≤MD,f​.

The left multiplier orbit g↦ηG(g)ag\mapsto\eta_G(g)ag↦ηG​(g)a is smooth for every a∈A∘a\in\mathcal A^\circa∈A∘. The construction from a nondegenerate representation also identifies its smooth vectors with the represented algebraic core, as in Lemma 6.2. These are the analytic steps named in the milestone list.

Isomorphism of representation categories

The goal is Theorem 6.4. Propositions 6.1 and 6.3 give mutually inverse assignments on objects, and Theorem 6.4 retains the same intertwiners:

URep⁡(G,g)  ≅  Rep⁡nd(A(G,g)).\operatorname{URep}(G,\mathfrak g) \;\cong\; \operatorname{Rep}_{\mathrm{nd}}\bigl(\mathcal A(G,\mathfrak g)\bigr).URep(G,g)≅Repnd​(A(G,g)).

Thus each unitary representation yields exactly one nondegenerate representation agreeing on every generator, each nondegenerate representation comes from exactly one unitary supergroup representation, and a bounded operator intertwines one pair exactly when it intertwines the other. The goal includes all three clauses.

Significance

The result lets questions about unitary Lie supergroup representations be transferred to a C∗C^*C∗-algebra without losing the odd infinitesimal action or the morphisms. In the paper, this is the foundation for the later direct integral discussion and CCR criteria. Without the equivalence, properties of A\mathcal AA would have no stated connection to decomposition of unitary supergroup representations §7.

The mathematical result is proved in the cited paper; the local Lean declarations are open statements. A complete formal development would add machine-checked proofs for the uniform operator bounds, the algebra and multiplier facts, reconstruction of the odd action, and the categorical equivalence. The reusable parts include smooth-vector actions, integrated test-function operators, and a universal bounded family of representations.

Difficulty

The odd infinitesimal operators are defined on H∞\mathcal H^\inftyH∞, not automatically as bounded operators on all of H\mathcal HH. Integrating π\piπ against a test function supplies smooth vectors, but it does not by itself give a bound for an arbitrary word in the odd and even operators that is uniform over every representation. That uniformity is needed to construct one C∗C^*C∗-norm. In the reverse direction, a nondegenerate representation of A\mathcal AA first gives bounded operators; recovering the derived action on precisely the smooth core requires the multiplier and smoothness statements. An object-level bijection alone would still miss the paper's assertion about intertwiners.

Formalization scope

Lean models GGG as a finite-dimensional smooth real Lie group, with g0ˉ\mathfrak g_{\bar 0}g0ˉ​ its Mathlib group Lie algebra and g1ˉ\mathfrak g_{\bar 1}g1ˉ​ a finite-dimensional real normed space. The superbracket and odd adjoint action are fields of a Harish–Chandra pair. Smoothness uses C∞C^\inftyC∞, not analyticity. The group is neither assumed connected nor second countable. A left Haar measure is fixed. The Hilbert spaces quantified in the mission belong to Type; the index of all such unitary representations belongs to Type 1.

The test space D(Gε)\mathcal D(G_\varepsilon)D(Gε​) is encoded as pairs of functions, and the enveloping-algebra elements needed here as finite words. A\mathcal AA is the closed non-unital star subalgebra of the bounded product of operator algebras generated by their representation families. This uses all Type-small unitary representations; the paper takes unitary-equivalence classes of cyclic ones, which yield the same norm through its Remark 2.5. The algebra depends only on (G,g)(G,\mathfrak g)(G,g) and Haar measure, and ρπ\rho^\piρπ acts on H∞\mathcal H^\inftyH∞ itself. This rules out a choice of algebra or an off-domain operator value that would make the correspondence automatic.

The published smooth-orbit and vector-integral definitions from van Dijk–Neeb–Salmasian–Zellner are reused. Completing this mission calls for the Dixmier–Malliavin factorization, Gårding smoothing, bounded operator estimates, non-unital C∗C^*C∗-algebra representations and multiplier actions. Contributions proving those general tools or the source-labelled milestones are within scope. The generator family is represented through vectors rather than an operator-norm Bochner integral, whose measurability is unavailable for a merely strongly continuous representation.

Selected references

  • K.-H. Neeb and H. Salmasian, “C*-algebras and direct integral decomposition for Lie supergroups,” arXiv:1506.01558v1, 2015. Preprint.
  • G. van Dijk, K.-H. Neeb, H. Salmasian and C. Zellner, On the characterization of trace class representations and Schwartz operators, arXiv:1512.02451v1, 2015. Preprint.
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Functional AnalysisQuantum Information·Captain: mikedeng1

Approximation of Multipartite Quantum States and the Relative Entropy of Entanglement: Lower Semicontinuity of the Relative Entropy of Entanglement at States with n−1 FA-Property MarginalsResearch Paper

Motivation

The relative entropy of entanglement measures how distinguishable a multipartite quantum state is from all fully separable states. In finite dimensions it is a standard entanglement measure, but infinite-dimensional systems raise a basic analytical problem: the measure may take the value +∞+\infty+∞, and finite-rank approximations do not automatically control its behavior at a limit state. Shirokov's analysis identifies a broad class of states at which the direct relative entropy of entanglement is finite and lower semicontinuous. The result applies when all but possibly one marginal state satisfy the FA-property, a spectral condition that includes useful finite-entropy states without requiring finite-dimensional Hilbert spaces.

The paper relates the direct measure to a universal extension formed from local finite-rank compressions. This mission isolates the ERE_RER​ part of Theorem 2 A) and the source results needed to reach it. A later paper by Lami and Shirokov addresses more general global lower semicontinuity questions using a different operator model and hypotheses; its statements are related work, not imports into this mission. Shirokov, §4.3; Lami–Shirokov.

Setting

There are nnn parties A1,…,AnA_1,\ldots,A_nA1​,…,An​, with separable Hilbert spaces HAs\mathcal H_{A_s}HAs​​. A state ρ\rhoρ is a positive trace-class operator with trace one on their joint system. Its marginal ρAs\rho_{A_s}ρAs​​ is obtained by tracing out every party except AsA_sAs​. A product state is a tensor product of one state per party. The set Ss\mathfrak S_sSs​ of fully separable states is the trace-norm closed convex hull of product states. Closure matters in infinite dimension: restricting to finite convex combinations would change the infimum below. Shirokov, pp. 10–11, (26).

Write H(ρ∥σ)H(\rho\|\sigma)H(ρ∥σ) for Lindblad's quantum relative entropy, including the trace correction for unnormalized positive operators and the value +∞+\infty+∞ on support failure. The direct relative entropy of entanglement is

ER(ρ)=inf⁡σ∈SsH(ρ∥σ).E_R(\rho)=\inf_{\sigma\in\mathfrak S_s}H(\rho\|\sigma).ER​(ρ)=σ∈Ss​inf​H(ρ∥σ).

The von Neumann entropy H(ρ)H(\rho)H(ρ) and ER(ρ)E_R(\rho)ER​(ρ) are extended nonnegative real quantities in natural-logarithm units. A state has the FA-property when its eigenvalues λj\lambda_jλj​ admit nonnegative numbers gjg_jgj​ with ∑jλjgj<+∞\sum_j\lambda_jg_j<+\infty∑j​λj​gj​<+∞ and lim⁡β↓0(∑je−βgj)β=1\lim_{\beta\downarrow0}(\sum_je^{-\beta g_j})^\beta=1limβ↓0​(∑j​e−βgj​)β=1. In particular, the FA-property implies finite entropy. The set S∗\mathfrak S_*S∗​ consists of joint states with the FA-property on at least n−1n-1n−1 marginals. Shirokov, pp. 2, 4, 14, (1), (34).

For each party, a finite-rank orthogonal projector compresses the joint state. The universal extension E^R\widehat E_RER​ takes the supremum of the homogeneous ERE_RER​ values of all such local compressions. A compressed positive operator XXX with trace c>0c>0c>0 is valued as cER(X/c)cE_R(X/c)cER​(X/c); the zero operator has value zero. Local spectral projectors built from the marginals define the approximation ΛrL(ρ)\Lambda_r^L(\rho)ΛrL​(ρ) used in Theorem 1. Shirokov, pp. 7, 12–13, (17), (31).

Formalization targets

Goal: Theorem 2 A), the ERE_RER​ case

For ρ0∈S∗\rho_0\in\mathfrak S_*ρ0​∈S∗​, ER(ρ0)<+∞E_R(\rho_0)<+\inftyER​(ρ0​)<+∞. For every sequence of states ρk→ρ0\rho_k\to\rho_0ρk​→ρ0​ in trace norm,

ER(ρ0)≤lim inf⁡k→∞ER(ρk).E_R(\rho_0)\le\liminf_{k\to\infty}E_R(\rho_k).ER​(ρ0​)≤k→∞liminf​ER​(ρk​).

The sequence itself may lie anywhere in the full state space. This is the sequential lower semicontinuity assertion (35), together with finiteness, in Theorem 2 A).

Supporting targets

The milestones, in attack order, are: the FA entropy consequence (p. 4); the pure-state separable comparison of Lemma 3; the σ\sigmaσ-convexity of ERE_RER​ (first sentence of Theorem 2 E)); the upper bound (28) by any n−1n-1n−1 marginal entropies,

ER(ρ)≤∑s≠tH(ρAs);E_R(\rho)\le\sum_{s\ne t}H(\rho_{A_s});ER​(ρ)≤s=t∑​H(ρAs​​);

the concavity-defect bound (27), pER(ρ)+(1−p)ER(σ)≤ER(pρ+(1−p)σ)+h2(p)pE_R(\rho)+(1-p)E_R(\sigma)\le E_R(p\rho+(1-p)\sigma)+h_2(p)pER​(ρ)+(1−p)ER​(σ)≤ER​(pρ+(1−p)σ)+h2​(p); membership of ERE_RER​ in Lnn−1(1,1)L_n^{n-1}(1,1)Lnn−1​(1,1); the LLL-class assertion of Theorem 1; the relative-entropy inequality of Lemma 1 for positive maps with trace-preserving sum; the comparison E^R≤ER\widehat E_R\le E_RER​≤ER​; lower semicontinuity of E^R\widehat E_RER​; and the equality ER=E^RE_R=\widehat E_RER​=ER​ on S∗\mathfrak S_*S∗​ (Theorem 2 B)). These are claims made in the paper, with the portions outside the ERE_RER​ route explicitly scoped in the item descriptions. Shirokov, pp. 4, 8, 11, 13–15, 20, 25.

Significance

The theorem gives a stable finite value of ERE_RER​ at every state in S∗\mathfrak S_*S∗​: approximating sequences cannot converge there while hiding a smaller limiting value. This matters when infinite-dimensional states are approximated by finite-rank or energy-constrained states, because pointwise convergence of operators alone does not control an extended-valued entanglement measure. The equality with E^R\widehat E_RER​ also identifies the direct measure with a globally lower semicontinuous construction on the stated domain. Shirokov, Theorem 2 and discussion in §4.3.

The mathematical result is proved in the source paper. The formalization work is to express its spectral FA condition, multipartite partial traces, trace-norm separability, finite-rank compression, homogeneous extension, and extended-real inequalities in Lean, then prove the milestones and goal. The published P01 definition already supplies von Neumann entropy and Lindblad relative entropy; the propositions in this mission are open Lean statements, not machine-checked proofs. This shared infrastructure can support other infinite-dimensional quantum information results involving separability and marginal entropies.

Difficulty

A direct argument from the infimum defining ERE_RER​ cannot simply exchange that infimum with a state limit: the separable comparison state that nearly minimizes at one point need not remain useful along a convergent sequence. Infinite values also make real-valued continuity bounds insufficient. The paper's theorem therefore has to coordinate a finite-entropy estimate on n−1n-1n−1 marginals with control of local finite-rank approximations and a lower semicontinuous extension. The approximation estimate is uniform over a class of functions, with the rank threshold and error sequence chosen before the function. Shirokov, Theorem 1 and proof of Theorem 2 A).

Formalization scope

Each HAs\mathcal H_{A_s}HAs​​ is represented as ℓ2(Is)\ell^2(I_s)ℓ2(Is​) for a countable basis index type. Parties are indexed by Fin⁡(n)\operatorname{Fin}(n)Fin(n), and the joint basis uses their dependent Cartesian product. The state topology is the trace-norm topology of the published P33 state structure. Entropy, relative entropy, and ERE_RER​ take values in [0,+∞][0,+\infty][0,+∞]; no real-valued surrogate replaces an infinite value. The FA-property requires an actual orthonormal eigenbasis tied to the state's coefficients. Its partition sum is computed in [0,+∞][0,+\infty][0,+∞], so divergence cannot default to zero. The definition of S∗\mathfrak S_*S∗​ says at least n−1n-1n−1 FA marginals and does not impose FA on the sequence in the goal.

The Lnm(C,D)L_n^m(C,D)Lnm​(C,D) class is represented with a finite set of FA parties in place of the first mmm parties, reflecting the paper's relabeling symmetry. Within that class, ERE_RER​ is converted to a real number only on the finite-entropy domain. The universal extension uses all finite orthonormal local families and the homogeneous convention for compressed positive operators. The setting also defines countable separable decompositions, finite-rank projectors, the spectral approximation relation, binary entropy in nats, and positive linear maps on the trace class. The proviso of (27) that "all the involved quantities are finite" (p. 11) is stated as finiteness of ERE_RER​ at the two mixed states. These definitions and the cited P01/P33 libraries are the reusable work. A definition of FA that every state satisfies, a separable set without trace closure, or a real ERE_RER​ that discards +∞+\infty+∞ would trivialize or alter the target.

The paper also states a regularized ER∞E_R^\inftyER∞​ case. It is outside this mission: its proof in version 2 invokes propositions by broken “??” references that are absent from the source. The hatted-class and NNN-class portions of Theorem 1, the regularized equality in Theorem 2 B), and the entanglement-monotone part of the universal-extension bullet are likewise outside these ERE_RER​ milestones. Contributions proving the stated Lean milestones, improving the common operator definitions, and then proving the goal are welcome.

Selected references

  • M. E. Shirokov, Approximation of multipartite quantum states and the relative entropy of entanglement, arXiv preprint, version 2, 2024. arXiv:2103.12111v2.
  • L. Lami and M. E. Shirokov, Attainability and lower semi-continuity of the relative entropy of entanglement, and variations on the theme, arXiv preprint, 2021. arXiv:2105.08091.
14 thms2 active usersReviewed
Information TheoryQuantum Information·Captain: mikedeng1

Entropy and Optimal Decompositions of States Relative to a Maximal Commutative Subalgebra: Equivalent Characterizations of a Symmetric Optimal Pair for Transposition-Invariant Rank-Two StatesResearch Paper

Motivation

In finite dimensional quantum information, a state of a full matrix algebra can be restricted to a smaller algebra of observables. The resulting entropy depends on which observables are retained. For a maximal commutative subalgebra, the retained observables are equivalent to measurements in a fixed orthonormal basis. The restriction has an ordinary probability distribution, but the state before restriction can still contain coherence between basis vectors. Uhlmann studies how the entropy of this restricted state compares with the least average entropy obtainable from pure states whose mixture is the original state. This comparison is an instance of the entropy of a subalgebra introduced by Narnhofer and Thirring and developed in the setting of matrix algebras Uhlmann, pp. 2–4.

Symmetry can make that minimization more concrete. A unitary that swaps two basis projections acts on states and their decompositions. Uhlmann's Lemma 6 asks when a rank two state fixed by this swap has a distinguished two-state optimal decomposition, and relates that event to the geometry of a set on which the entropy roof is affine Uhlmann, pp. 8–11. The result is a specific connection between a physical symmetry, an optimization problem over pure states, and the extreme points of a convex set.

Setting

Let H=Cd\mathcal H=\mathbb C^dH=Cd with its standard basis ∣j⟩|j\rangle∣j⟩, and let C\mathcal CC be the diagonal algebra. Its minimal projections are Pj=∣j⟩⟨j∣P_j=|j\rangle\langle j|Pj​=∣j⟩⟨j∣. A state is represented by a positive semidefinite matrix DDD of trace one. A pure state has density matrix ∣ψ⟩⟨ψ∣|\psi\rangle\langle\psi|∣ψ⟩⟨ψ∣ for a unit vector ψ\psiψ. The state of C\mathcal CC obtained by restricting DDD records the diagonal probabilities DjjD_{jj}Djj​ Uhlmann, p. 4, equations (1)–(3).

Write s(x)=−xln⁡xs(x)=-x\ln xs(x)=−xlnx, with s(0)=0s(0)=0s(0)=0. The diagonal entropy is S~(D)=∑js(Djj)\widetilde S(D)=\sum_j s(D_{jj})S(D)=∑j​s(Djj​). The convex roof R(D)R(D)R(D) is the infimum of ∑kpkS~(ρk)\sum_k p_k\widetilde S(\rho_k)∑k​pk​S(ρk​) over finite decompositions D=∑kpkρkD=\sum_k p_k\rho_kD=∑k​pk​ρk​ into pure states with positive weights pkp_kpk​ summing to one. A decomposition attaining the infimum is optimal. Uhlmann's entropy of C\mathcal CC at DDD is HD=S~(D)−R(D)H_D=\widetilde S(D)-R(D)HD​=S(D)−R(D) Uhlmann, pp. 4–5, equations (4)–(7).

An affine functional lll supports RRR if l≤Rl\le Rl≤R on all states and equality holds at some state. Its contact set is Ω(l)={ν:R(ν)=l(ν)}\Omega(l)=\{\nu:R(\nu)=l(\nu)\}Ω(l)={ν:R(ν)=l(ν)}. Given DDD, define ΩD\Omega_DΩD​ as the intersection of all contact sets whose support functional touches RRR at DDD. This intersection is compact and convex, contains every pure state used by an optimal decomposition of DDD, and is a region on which RRR is affine Uhlmann, pp. 6–7, Lemma 3 and equation (10). A transposition UUU swaps two PjP_jPj​ and fixes the remaining minimal projections. It transforms a density matrix as D↦U∗DUD\mapsto U^*DUD↦U∗DU Uhlmann, p. 8.

Formalization targets

Goal: equivalent rank two conditions

For a rank two state DDD fixed by a transposition UUU, Uhlmann's Lemma 6 asserts equivalence of three statements:

(a)  D is the only U-invariant state in ΩD;(b)  D has an optimal decomposition into two different pure states, and some member of ΩD does not commute with U;(c)  Ext⁡(ΩD)={ρ,U∗ρU} for two distinct states.\begin{aligned} \text{(a)}\;&D\text{ is the only }U\text{-invariant state in }\Omega_D;\\ \text{(b)}\;&D\text{ has an optimal decomposition into two different pure states,}\ &\text{and some member of }\Omega_D\text{ does not commute with }U;\\ \text{(c)}\;&\operatorname{Ext}(\Omega_D)=\{\rho,U^*\rho U\}\text{ for two distinct states.} \end{aligned}(a)(b)(c)​D is the only U-invariant state in ΩD​;D has an optimal decomposition into two different pure states, Ext(ΩD​)={ρ,U∗ρU} for two distinct states.​and some member of ΩD​ does not commute with U;​

The milestone list follows the paper's supporting results: finite optimal decompositions with rank bounds (Lemma 1), comparison on an RRR-set (Lemma 2), compact supporting contact sets and their covering (Lemma 3), the intersection properties of ΩD\Omega_DΩD​ (the Corollary at equation (10)), zero entropy implying purity (Lemma 4), and the rank two support projection formula (equation (13)) Uhlmann, pp. 5–9. The goal preserves all three clauses of the printed equivalence.

Significance

When the equivalent conditions hold, the rank two state has an optimal decomposition using just two pure states, while the entire supporting contact set has only the two swapped extreme points. Thus the statement identifies circumstances under which the symmetry of a matrix state controls both the optimizer and the geometry of the convex roof. Uhlmann subsequently gives an explicit expression for R(D)R(D)R(D) under these conditions in equation (27), which is outside the present goal Uhlmann, pp. 10–12.

The result is proved in the cited paper; the remaining task here is a machine checked development of the definitions, supporting results, and equivalence. The local Lean files state the targets and compile with proof placeholders; they do not constitute machine checked proofs of the milestones or goal. A completed development would also supply reusable finite dimensional infrastructure for pure state roofs, supporting contact sets, and optimal decompositions of density matrices.

Difficulty

An optimal pair alone does not immediately determine every extreme point of ΩD\Omega_DΩD​. That set is an intersection of all contact sets, and may be larger than the convex hull of the pure states seen in one decomposition. The paper itself says equality with that smaller convex hull remains a conjecture in general Uhlmann, p. 7, Remark and footnote 3. Its printed discussion of the implication from the optimal pair to the two extreme points does not resolve this general distinction. The equivalence is therefore retained exactly as printed and the gap is recorded for review.

Formalization scope

Matrices are indexed by Fin d, so the paper's indices 1,…,d1,\ldots,d1,…,d become 0,…,d−10,\ldots,d-10,…,d−1. The state predicate reuses the published QAlgorithms.IsDensityMatrix. Pure states are unit-vector outer products. Finite decompositions use strictly positive real weights and complex matrix mixtures. Real.negMulLog supplies natural logarithms and s(0)=0s(0)=0s(0)=0. The real infimum defining RRR is applied only to states; there the decomposition set is nonempty and its costs are bounded below. Off the state space, Lean's real infimum can return a default value that has no meaning in the paper.

Supporting affine functionals are represented by Hermitian matrices via lA(ν)=Re⁡Tr⁡(νA)l_A(\nu)=\operatorname{Re}\operatorname{Tr}(\nu A)lA​(ν)=ReTr(νA), as in the paper's equation (9). The set ΩD\Omega_DΩD​ is the full intersection in equation (10), and its extreme points are taken in the ambient real matrix space. The transposition in the goal is explicitly self-adjoint, U∗=UU^*=UU∗=U, matching the identity used in the printed proof. The rank is matrix rank. “Length two” means two distinct pure states with positive weights whose cost attains R(D)R(D)R(D). No optimal pair is assumed as a hypothesis.

The needed contributions are proofs of the six stated milestones, the finite dimensional properties of the model definitions they use, and the three implications of Lemma 6. The model's pure state decomposition and supporting set definitions are reusable for other convex roof problems on finite density matrices.

Selected references

  • Armin Uhlmann, Entropy and optimal decompositions of states relative to a maximal commutative subalgebra, preprint arXiv:quant-ph/9704017v2, 1998. arXiv
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Information TheoryQuantum Information·Captain: mikedeng1

General Benchmarks for Quantum Repeaters: For the Qudit Dephasing Channel the Entanglement-Flux Upper Bound Meets the Coherent Information, log₂ d − H(P)Research Paper

Motivation

A quantum repeater is judged by how much it beats direct transmission over a point-to-point link. The natural yardsticks are the two-way assisted capacities of the link's channel E\mathcal EE: the quantum capacity Q2(E)Q_2(\mathcal E)Q2​(E) and the secret-key capacity K(E)K(\mathcal E)K(E), the best rates of entanglement and key that two parties can obtain over many uses of E\mathcal EE when unlimited two-way classical communication and local operations are free. Computing them exactly for a given channel is rare, because it requires a lower and an upper bound that meet.

Pirandola and Laurenza (arXiv:1512.04945v2, 2016) obtain such matching bounds for a family of channels. The lower bound is the coherent information of the channel (with its reverse version), which is achievable by the hashing protocol. The upper bound is the entanglement flux Φ(E)\Phi(\mathcal E)Φ(E), the relative entropy of entanglement of the channel's Choi matrix, which bounds KKK for channels that can be simulated by teleportation. For the qudit dephasing channel the two bounds coincide, which gives Q2=K=log⁡2d−H(P)Q_2=K=\log_2 d-H(\mathbf P)Q2​=K=log2​d−H(P) (Eqs. (20) and (95)). This mission formalizes that coincidence.

Setting

Fix a dimension d≥2d\ge2d≥2 and the computational basis {∣j⟩}j=0d−1\{|j\rangle\}_{j=0}^{d-1}{∣j⟩}j=0d−1​ of a qudit. Let ω=e2πi/d\omega=e^{2\pi i/d}ω=e2πi/d and let ZZZ be the generalized phase operator, Z∣j⟩=ωj∣j⟩Z|j\rangle=\omega^j|j\rangleZ∣j⟩=ωj∣j⟩. For a dephasing probability p∈[0,1]p\in[0,1]p∈[0,1] define the binomial weights

Pm(p,d)=(d−1m)pm(1−p)d−1−m,m=0,…,d−1,P_m(p,d)=\binom{d-1}{m}p^m(1-p)^{d-1-m},\qquad m=0,\dots,d-1,Pm​(p,d)=(md−1​)pm(1−p)d−1−m,m=0,…,d−1,

and the qudit dephasing channel, given by its Kraus operators,

Pd(ρ)=∑m=0d−1EmρEm†,Em=Pm(p,d) Zm.\mathcal P_d(\rho)=\sum_{m=0}^{d-1}E_m\rho E_m^\dagger,\qquad E_m=\sqrt{P_m(p,d)}\,Z^m .Pd​(ρ)=m=0∑d−1​Em​ρEm†​,Em​=Pm​(p,d)​Zm.

Write P={Pm(p,d)}m\mathbf P=\{P_m(p,d)\}_mP={Pm​(p,d)}m​ and H(P)=−∑mPmlog⁡2PmH(\mathbf P)=-\sum_mP_m\log_2P_mH(P)=−∑m​Pm​log2​Pm​ (with 0log⁡0=00\log0=00log0=0) for its Shannon entropy.

The Choi matrix of a map E\mathcal EE on d×dd\times dd×d matrices is ρE=(I⊗E)(Ψd)\rho_{\mathcal E}=(\mathcal I\otimes\mathcal E)(\Psi_d)ρE​=(I⊗E)(Ψd​), where ∣Ψd⟩=d−1/2∑i∣ii⟩|\Psi_d\rangle=d^{-1/2}\sum_i|ii\rangle∣Ψd​⟩=d−1/2∑i​∣ii⟩. The first tensor factor is the reference RRR, the second the channel output BBB. With the von Neumann entropy S(ρ)=−Tr ρlog⁡2ρS(\rho)=-\mathrm{Tr}\,\rho\log_2\rhoS(ρ)=−Trρlog2​ρ:

  • the coherent information of the channel is IC(E)=S(TrRρE)−S(ρE)I_C(\mathcal E)=S(\mathrm{Tr}_R\rho_{\mathcal E})-S(\rho_{\mathcal E})IC​(E)=S(TrR​ρE​)−S(ρE​);
  • the reverse coherent information is IRC(E)=S(TrBρE)−S(ρE)I_{RC}(\mathcal E)=S(\mathrm{Tr}_B\rho_{\mathcal E})-S(\rho_{\mathcal E})IRC​(E)=S(TrB​ρE​)−S(ρE​);
  • the relative entropy is S(ρ∥σ)=Tr[ρ(log⁡2ρ−log⁡2σ)]S(\rho\|\sigma)=\mathrm{Tr}[\rho(\log_2\rho-\log_2\sigma)]S(ρ∥σ)=Tr[ρ(log2​ρ−log2​σ)], and +∞+\infty+∞ when the support of ρ\rhoρ is not inside that of σ\sigmaσ;
  • the relative entropy of entanglement of a bipartite state is ER(ρ)=inf⁡σ∈SEPS(ρ∥σ)E_R(\rho)=\inf_{\sigma\in\mathrm{SEP}}S(\rho\|\sigma)ER​(ρ)=infσ∈SEP​S(ρ∥σ), the infimum over all separable states for the cut R:BR:BR:B;
  • the entanglement flux of the channel is Φ(E)=ER(ρE)\Phi(\mathcal E)=E_R(\rho_{\mathcal E})Φ(E)=ER​(ρE​).

The paper's candidate separable state is σ~=∑i1d∣i⟩⟨i∣⊗Pd(∣i⟩⟨i∣)\tilde\sigma=\sum_i\frac1d|i\rangle\langle i|\otimes\mathcal P_d(|i\rangle\langle i|)σ~=∑i​d1​∣i⟩⟨i∣⊗Pd​(∣i⟩⟨i∣).

Formalization targets

Goal (Eqs. (94)–(95), p. 11)

For every d≥2d\ge2d≥2 and p∈[0,1]p\in[0,1]p∈[0,1]:

IC(Pd)=IRC(Pd)=log⁡2d−H(P),Φ(Pd)≤log⁡2d−H(P).I_C(\mathcal P_d)=I_{RC}(\mathcal P_d)=\log_2d-H(\mathbf P),\qquad \Phi(\mathcal P_d)\le\log_2d-H(\mathbf P).IC​(Pd​)=IRC​(Pd​)=log2​d−H(P),Φ(Pd​)≤log2​d−H(P).

The lower and the upper bound on the two-way capacities therefore meet. The statement keeps ddd and ppp free and asserts exact values, not numerical constants.

Milestones (in attack order)

  1. The Choi matrix of Pd\mathcal P_dPd​ in closed form (p. 11, display between Eqs. (90) and (91)).
  2. Eq. (91): S(ρPd)=H(P)S(\rho_{\mathcal P_d})=H(\mathbf P)S(ρPd​​)=H(P).
  3. Eq. (68): S(ρ∥σ)=−S(ρ)−∑i⟨i∣ρ∣i⟩log⁡siS(\rho\|\sigma)=-S(\rho)-\sum_i\langle i|\rho|i\rangle\log s_iS(ρ∥σ)=−S(ρ)−∑i​⟨i∣ρ∣i⟩logsi​ in the eigenbasis of σ\sigmaσ, under support inclusion.
  4. Eq. (92): σ~=∑i1d∣ii⟩⟨ii∣\tilde\sigma=\sum_i\frac1d|ii\rangle\langle ii|σ~=∑i​d1​∣ii⟩⟨ii∣ and σ~\tilde\sigmaσ~ is separable.
  5. Eq. (93): Tr(ρPdlog⁡2σ~)=−log⁡2d\mathrm{Tr}(\rho_{\mathcal P_d}\log_2\tilde\sigma)=-\log_2dTr(ρPd​​log2​σ~)=−log2​d, with the support of ρPd\rho_{\mathcal P_d}ρPd​​ inside that of σ~\tilde\sigmaσ~.
  6. Eq. (94): Φ(Pd)≤S(ρPd∥σ~)=log⁡2d−H(P)\Phi(\mathcal P_d)\le S(\rho_{\mathcal P_d}\|\tilde\sigma)=\log_2d-H(\mathbf P)Φ(Pd​)≤S(ρPd​​∥σ~)=log2​d−H(P).
  7. Eq. (45): for a unital, trace-preserving map E\mathcal EE, IC(E)=IRC(E)=log⁡2d−S(ρE)I_C(\mathcal E)=I_{RC}(\mathcal E)=\log_2d-S(\rho_{\mathcal E})IC​(E)=IRC​(E)=log2​d−S(ρE​).

Significance

The result. The coincidence of the two bounds pins down Q2Q_2Q2​ and KKK of the qudit dephasing channel for every ddd and ppp, which gives the repeaterless benchmark for any qudit link dominated by dephasing. At d=2d=2d=2 it recovers the qubit dephasing benchmark 1−H2(p)1-H_2(p)1−H2​(p) of the same paper (Eq. (75), with p↔1−pp\leftrightarrow1-pp↔1−p, which the binary entropy does not see). Combined with the operational facts the paper imports (the hashing inequality and the bound of KKK by the flux for teleportation-covariant channels), it yields the capacity formula (95).

Formalizing it. The paper's computation is complete but terse. The formalization makes three implicit points explicit: the support of the Choi matrix lies inside the support of the rank-ddd state σ~\tilde\sigmaσ~ (so log⁡σ~\log\tilde\sigmalogσ~ is taken on its support); the claim of "ddd non-zero eigenvalues" in (91) fails at p∈{0,1}p\in\{0,1\}p∈{0,1}, while the entropy identity does not; and (45) needs trace preservation as well as unitality. The results are proved in the paper and, as far as the platform's catalogue shows, formalized nowhere. Eq. (68) and Eq. (45) are reusable lemmas about arbitrary states and unital channels.

Difficulty

The calculation on the page is short; the difficulty lies in what it leaves to the reader. The entropy identity (91) asks for the spectrum of a d2×d2d^2\times d^2d2×d2 matrix that is not diagonal in the computational basis, while the von Neumann entropy is defined through the matrix functional calculus, so "diagonalizing" has to be made precise. The state σ~\tilde\sigmaσ~ has rank ddd in dimension d2d^2d2: the relative entropy against it is finite only because of a support inclusion the paper does not mention, and a computation that ignores the kernel of σ~\tilde\sigmaσ~ does not establish the value. The upper bound needs σ~\tilde\sigmaσ~ to be separable in the sense of the infimum, a finite convex combination of product density matrices, not merely diagonal. Finally, the coherent information is a difference of entropies of a partial trace and of the full Choi matrix; equating it to log⁡2d−H(P)\log_2 d-H(\mathbf P)log2​d−H(P) requires both that the output marginal is maximally mixed and the entropy identity (91).

Formalization scope

Qudit indices are Fin d, with d≥2d\ge2d≥2 (and [NeZero d] where an instance needs it); ppp is real with 0≤p≤10\le p\le10≤p≤1. ZmZ^mZm is a matrix power, ω=exp⁡(2πi/d)\omega=\exp(2\pi i/d)ω=exp(2πi/d), and the channel is the published QAlgorithms.krausApply of the Kraus family Pm Zm\sqrt{P_m}\,Z^mPm​​Zm. The Choi matrix is the published QAlgorithms.idTensorSuperop applied to maximallyEntangledProjector d (entries 1/d1/d1/d on ∣ii⟩⟨jj∣|ii\rangle\langle jj|∣ii⟩⟨jj∣), the reference being the first factor of Fin d × Fin d. Entropies are in bits with 0log⁡0=00\log0=00log0=0: QAlgorithms.vnEntropy for states and a local Shannon entropy for the weights. The partial traces are QAlgorithms.traceLeft (over the reference) and QAlgorithms.traceRight (over the output). The relative entropy and ERE_RER​ are the published relativeEntropyBits and relativeEntanglement (Umegaki entropy divided by ln⁡2\ln2ln2, +∞+\infty+∞ off support, infimum over IsSeparableDensity, values in [0,∞][0,\infty][0,∞]). The real bound is embedded with ENNReal.ofReal; since H(P)≤log⁡2dH(\mathbf P)\le\log_2dH(P)≤log2​d, nothing is lost.

None of the defined quantities is given by its closed form: the Choi matrix is computed from the channel, ERE_RER​ is the infimum over all separable states (not S(ρ∥σ~)S(\rho\|\tilde\sigma)S(ρ∥σ~) or an infimum over diagonal states), and ICI_CIC​ is defined from partial traces, not as log⁡2d−S(ρE)\log_2d-S(\rho_{\mathcal E})log2​d−S(ρE​). This rules out the trivializing formalization in which a milestone or the goal holds by definition. The bound log⁡2d\log_2dlog2​d alone holds for every state; the goal's bound is log⁡2d−H(P)\log_2d-H(\mathbf P)log2​d−H(P).

The operational capacities Q2Q_2Q2​ and KKK of Eq. (95) are not formalized. They are defined over adaptive LOCC protocols with private-state targets, which have no substrate on the platform. The paper also does not prove the two bridges from them to the bounds: it imports K≤ΦK\le\PhiK≤Φ (Eq. (2), from Pirandola et al.) and the hashing inequality (from Devetak and Winter). For the same reason, the reverse inequality Φ(Pd)≥log⁡2d−H(P)\Phi(\mathcal P_d)\ge\log_2d-H(\mathbf P)Φ(Pd​)≥log2​d−H(P) is not stated, since the paper obtains it only through the hashing bound. Teleportation stretching, convexity of the flux, the bosonic Gaussian channels and the erasure channel are outside this mission.

Contributions are welcome at every level: the spectrum of circulant blocks, the support calculus of the Umegaki entropy, and the separable decomposition of diagonal states are all reusable beyond this mission.

Selected references

  • S. Pirandola, R. Laurenza, General Benchmarks for Quantum Repeaters, arXiv preprint, v2, 2016. https://arxiv.org/abs/1512.04945v2
  • S. Pirandola, R. Laurenza, C. Ottaviani, L. Banchi, Fundamental limits of repeaterless quantum communications, Nature Communications 8, 15043, 2017. https://doi.org/10.1038/ncomms15043
  • I. Devetak, A. Winter, Distillation of secret key and entanglement from quantum states, Proc. R. Soc. A 461, 207–235, 2005. https://doi.org/10.1098/rspa.2004.1372
  • V. Vedral, M. B. Plenio, Entanglement measures and purification procedures, Phys. Rev. A 57, 1619, 1998. https://doi.org/10.1103/PhysRevA.57.1619
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Bandit AlgorithmsOperations ResearchProbability·Captain: mikedeng1

A Note on the Equivalence of Upper Confidence Bounds and Gittins Indices for Patient Agents: The Gaussian Gittins Index Equals the Posterior γ-Quantile μ + Φ⁻¹(γ)σ up to o(1) as γ → 1Research Paper

Motivation

A Gittins index assigns a number to an uncertain arm in a discounted bandit problem. The index converts a sequential choice, where an agent may keep gathering information or retire, into a tax threshold for playing the arm. Computing it generally requires an optimal stopping calculation. A Bayesian upper confidence bound, by comparison, is a quantile of the posterior distribution and is directly available for a Gaussian posterior. Russo's note asks how closely these two quantities agree when the agent is patient and the discount factor approaches one. The answer is an asymptotic identity for a Gaussian arm, not a finite-discount formula. Russo, 2019, pp. 1–3.

The note places its result alongside work on computational approximations of Gittins indices and finite-horizon index policies, but aims at the conceptual relationship with Bayesian confidence bounds. It appeared as an arXiv preprint in 2019; this mission follows that version's theorem numbering and formulas. A later journal publication appeared in Operations Research in 2021, but its numbering is not used here.

Setting

One arm has an unknown quality θ\thetaθ. The prior distribution is Gaussian, θ∼N(μ,σ2)\theta\sim N(\mu,\sigma^2)θ∼N(μ,σ2), where μ∈R\mu\in\mathbb Rμ∈R and σ2>0\sigma^2>0σ2>0. Playing the arm at time ttt yields Rt=θ+WtR_t=\theta+W_tRt​=θ+Wt​, where the observation noises WtW_tWt​ are independent Gaussian variables of mean zero and variance σW2>0\sigma_W^2>0σW2​>0. After observing R0,…,Rt−1R_0,\ldots,R_{t-1}R0​,…,Rt−1​, the posterior is N(μt,σt2)N(\mu_t,\sigma_t^2)N(μt​,σt2​). Its mean and variance follow the Gaussian update (1) of Russo, p. 2. In particular, σt2=(1/σ2+t/σW2)−1\sigma_t^2=(1/\sigma^2+t/\sigma_W^2)^{-1}σt2​=(1/σ2+t/σW2​)−1.

For each play, the agent pays a tax λ∈R\lambda\in\mathbb Rλ∈R. The agent may retire, receiving zero thereafter. At discount factor 0<γ<10<\gamma<10<γ<1, an admissible retirement time τ≥1\tau\ge1τ≥1 uses only the rewards observed through the current time. Its discounted payoff includes the play at τ\tauτ: ∑t=0τγt(θ−λ)\sum_{t=0}^{\tau}\gamma^t(\theta-\lambda)∑t=0τ​γt(θ−λ). The value Vγλ(μ,σ2;σW2)V^\lambda_\gamma(\mu,\sigma^2;\sigma_W^2)Vγλ​(μ,σ2;σW2​) is the supremum of the expected payoff over these retirement times. The Gittins index λγ(μ,σ2;σW2)\lambda_\gamma(\mu,\sigma^2;\sigma_W^2)λγ​(μ,σ2;σW2​) is the supremum of taxes for which the value is nonnegative. These are the stopping-time value and fair-tax definition in equations (2)–(3) of Russo, p. 2.

Write Φ\PhiΦ and ϕ\phiϕ for the distribution function and density of N(0,1)N(0,1)N(0,1), and Φ−1(γ)=inf⁡{z:Φ(z)≥γ}\Phi^{-1}(\gamma)=\inf\{z:\Phi(z)\ge\gamma\}Φ−1(γ)=inf{z:Φ(z)≥γ}. Thus μ+σΦ−1(γ)\mu+\sigma\Phi^{-1}(\gamma)μ+σΦ−1(γ) is the prior's upper γ\gammaγ-quantile, with σ=σ2\sigma=\sqrt{\sigma^2}σ=σ2​.

Formalization targets

Gaussian Gittins index asymptotic

The goal is Theorem 1, p. 3, for each fixed prior mean, positive prior variance, and positive observation-noise variance:

λγ(μ,σ2;σW2)=μ+σΦ−1(γ)+o(1)(γ↑1).\lambda_\gamma(\mu,\sigma^2;\sigma_W^2) =\mu+\sigma\Phi^{-1}(\gamma)+o(1) \qquad(\gamma\uparrow1).λγ​(μ,σ2;σW2​)=μ+σΦ−1(γ)+o(1)(γ↑1).

The remainder is an additive quantity tending to zero; the claim does not assert equality at any fixed discount factor. The paper reduces the general prior to a standardized one. Its intermediate targets are the normal-quantile asymptotic, explicit bounds on E[(X−λ)+]\mathbb E[(X-\lambda)^+]E[(X−λ)+], an upper bound obtained from noiseless information, and a matching lower bound from an admissible exploration policy. They appear as the mission's milestones, along with the posterior identities the lower bound uses. Russo, pp. 3–6.

Significance

The theorem identifies the limiting tax threshold with a familiar statistical quantile. It explains why a Bayesian upper confidence bound can approximate the Gittins priority of an arm when the effective horizon is large. It does not state that a quantile policy is exactly optimal at a fixed horizon or discount factor, and the paper's limitations section notes that significant observation noise relative to the horizon can make exploration costly. Russo, pp. 3, 7.

For a formal development, the reusable pieces are a Gaussian stopping-time model, the fair-tax index, the normal tail and positive-part estimates, and posterior update identities. The asymptotic theorem is proved in the source paper but has no machine-checked proof in this mission. Its local Lean statement is a target with sorry; the same applies to the milestone theorems. The definitions and a small sanity lemma compile in the pinned environment. Contributions that establish the source's stated bounds, their probabilistic prerequisites, or the final asymptotic reduction are relevant.

Difficulty

The direct idea of replacing the index by a posterior quantile at each fixed γ\gammaγ does not establish the theorem. The index optimizes over retirement times that adapt to noisy observations. A decision maker who sees θ\thetaθ without noise has a larger value, so the resulting expression supplies an upper bound, but it does not give a lower bound for the original information structure. The paper's matching lower estimate uses an actual reward-adapted policy and tracks both the cost of initial sampling and the benefit of later commitment. The two estimates must agree to an additive o(1)o(1)o(1), not merely at their leading order. Russo, §§3.3–3.4, pp. 4–7.

Formalization scope

Lean uses the canonical probability space Ω=R×(N→R)\Omega=\mathbb R\times(\mathbb N\to\mathbb R)Ω=R×(N→R): the first coordinate is θ\thetaθ, and the second is the independent noise sequence. The model measure is the Gaussian prior times an infinite product of Gaussian noise laws. The reward history at time ttt generates Ft=σ(R0,…,Rt)\mathcal F_t=\sigma(R_0,\ldots,R_t)Ft​=σ(R0​,…,Rt​). An admissible N∞\mathbb N_\inftyN∞​-valued stopping time has τ≥1\tau\ge1τ≥1; τ=∞\tau=\inftyτ=∞ means never retire. The stopped reward is a countable sum. The index is the supremum of the nonnegative-value tax set. Only the discount domain 0<γ<10<\gamma<10<γ<1 is used in fixed-discount statements; limits approach one from below. Variances are nonnegative reals at the Mathlib Gaussian interface, with strict positivity assumed in the theorem statements. The paper suppresses σW2\sigma_W^2σW2​ in the index notation; Lean keeps it explicit and arbitrary.

The value is defined from the stopping problem and the index from the fair-tax set. Retirement decisions depend on observed rewards only; giving them access to θ\thetaθ would change the target. The posterior variance uses t/σW2t/\sigma_W^2t/σW2​ in its closed form, correcting a printed error in (1). Lemma 3's limit is γ↑1\gamma\uparrow1γ↑1, and Lemma 7 uses log⁡(1/(1−γ))\log(1/(1-\gamma))log(1/(1−γ)) in its little-o scale; their printed versions are inconsistent with the surrounding derivations. The natural-language item notes identify these corrections. Russo, pp. 2, 4, 6, 9.

Selected references

  • Daniel Russo, A Note on the Equivalence of Upper Confidence Bounds and Gittins Indices for Patient Agents, arXiv:1904.04732v1, 2019. Preprint.
  • J. C. Gittins, K. D. Glazebrook, and R. Weber, Multi-Armed Bandit Allocation Indices, 2nd ed., Wiley, 2011. DOI.
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Mathematical PhysicsProbabilityQuantum Information·Captain: mikedeng1

Large Deviations in Quantum Spin Chain: Full Large Deviation Principle with a Good Rate Function for C*-Finitely Correlated StatesResearch Paper

Motivation

Measurements of long quantum spin chains can have outcomes far from their typical values. A large-deviation principle quantifies how quickly the probability of such outcomes decreases with the number of sites. In a classical lattice system this is a standard way to describe rare macroscopic fluctuations; in a quantum chain, observables on overlapping sets of sites generally fail to commute, which makes the corresponding probability laws harder to analyze. Ogata's 2008 paper establishes a full principle for the energy density of any translation-invariant finite-range interaction in a C∗C^*C∗-finitely correlated state. Its introduction explains that earlier spin-chain results covered upper bounds or more restricted observables and states, while the lower bound for general observables remained the substantial issue. Ogata, pp. 2–4

The finitely correlated class includes local states generated from finite auxiliary memory. It is large enough to include mixtures and periodic behavior, so a theorem restricted to a primitive transfer map would miss part of Ogata's statement. This mission targets the printed Theorem 1.2 in its full scope. Ogata, p. 4

Setting

At each site let Md(C)M_d(\mathbb C)Md​(C) be the algebra of complex d×dd\times dd×d matrices. On sites 1,…,n1,\ldots,n1,…,n, the local algebra is the nnn-fold tensor product, represented as matrices whose rows and columns are spin configurations. A finite-range translation-invariant interaction Φ\PhiΦ assigns a Hermitian operator Φ(X)\Phi(X)Φ(X) to each finite set of sites X⊂ZX\subset\mathbb ZX⊂Z, with the same term on translated sets and with Φ(X)=0\Phi(X)=0Φ(X)=0 when the diameter of XXX exceeds a fixed range. Its finite-volume Hamiltonian is

HΦ([1,n])=∑X⊆[1,n]Φ(X).H_\Phi([1,n])=\sum_{X\subseteq[1,n]}\Phi(X).HΦ​([1,n])=X⊆[1,n]∑​Φ(X).

The sum includes the scalar term associated with the empty set. The interaction need not be nearest-neighbor and may have a term on any finite pattern within its range. Ogata, pp. 2–3

A C∗C^*C∗-finitely correlated state is specified by a finite-dimensional auxiliary algebra B\mathcal BB, a unital completely positive map E:Md(C)⊗B→B\mathcal E:M_d(\mathbb C)\otimes\mathcal B\to\mathcal BE:Md​(C)⊗B→B, and a faithful stationary state ρ\rhoρ on B\mathcal BB. Iterating E\mathcal EE gives a compatible local state ωn\omega_nωn​ on nnn sites. The probability measure μn,Φ\mu_{n,\Phi}μn,Φ​ is the spectral distribution of HΦ([1,n])/nH_\Phi([1,n])/nHΦ​([1,n])/n in ωn\omega_nωn​: for a Borel set B⊆RB\subseteq\mathbb RB⊆R, it assigns the state weight of the spectral projection corresponding to BBB. These local restrictions determine the distributions used in the theorem. Ogata, pp. 3–4

Formalization targets

Full large-deviation principle

The goal is a good rate function I:R→[0,∞]I:\mathbb R\to[0,\infty]I:R→[0,∞]: III is lower semicontinuous and each set {x:I(x)≤a}\{x:I(x)\le a\}{x:I(x)≤a} is compact for finite a≥0a\ge0a≥0. For every closed CCC and open OOO in R\mathbb RR, Theorem 1.2 asserts

lim sup⁡n→∞1nlog⁡μn,Φ(C)≤−inf⁡x∈CI(x),\limsup_{n\to\infty}\frac1n\log\mu_{n,\Phi}(C)\le-\inf_{x\in C}I(x),n→∞limsup​n1​logμn,Φ​(C)≤−x∈Cinf​I(x), lim inf⁡n→∞1nlog⁡μn,Φ(O)≥−inf⁡x∈OI(x).\liminf_{n\to\infty}\frac1n\log\mu_{n,\Phi}(O)\ge-\inf_{x\in O}I(x).n→∞liminf​n1​logμn,Φ​(O)≥−x∈Oinf​I(x).

One rate function serves both inequalities and every eligible set. The statement asserts existence, without imposing a formula for III or a primitivity condition on the auxiliary map. Ogata, pp. 3–4

Supporting targets

The milestone list includes the paper's Gärtner–Ellis theorem, the spectral-law exponential-moment identity behind equation (1), the two-sided order estimate (15) for a gapped auxiliary map, the regrouping of lll consecutive sites into one site, under which the same state is generated by the lll-th iterate E(l)\mathcal E^{(l)}E(l) of the transfer map and E(l)^1=(E^1)l\widehat{\mathcal E^{(l)}}_1=(\widehat{\mathcal E}_1)^lE(l)1​=(E1​)l, and the differentiable limiting pressure under condition (14). In the last target, the pressure is the limit of n−1log⁡ωn(eαHΦ([1,n]))n^{-1}\log\omega_n(e^{\alpha H_\Phi([1,n])})n−1logωn​(eαHΦ​([1,n])) for every real α\alphaα. These are narrower claims with separate hypotheses; none replaces the full goal. Ogata, pp. 4–5, 12–15

Significance

The theorem gives an exponential-scale description of the energy-density distribution for all translation-invariant finite-range interactions in this state class. The upper bound controls probability on closed sets; the lower bound supplies the matching guarantee for open sets. Compact sublevel sets prevent low-rate mass from escaping to infinity. The result is already proved in Ogata's paper; the remaining work here is a machine-checked development of the statement and its supporting mathematics. Ogata, Theorem 1.2

Formalizing the finite-dimensional transfer construction, its spectral measures, and an extended-valued LDP vocabulary would also make these objects available for later spin-chain results. The goal itself is not currently accompanied by a machine-checked proof in this mission. The Gärtner–Ellis and auxiliary-map statements are likewise proof targets, not asserted as solved Lean facts.

Difficulty

The exponential of a sum of overlapping local interaction terms cannot generally be factored into independent one-site contributions. Even when an auxiliary transfer map has a spectral gap and yields a differentiable limiting pressure, that argument does not directly cover every finitely correlated state. A mixture can have a limiting log moment generating function with a corner; the resulting rate function can be nonconvex. Ogata's printed Lemma 4.1 reduces to special components but omits the separate mixture step needed to recover the unrestricted theorem. The goal retains the theorem's printed hypotheses, while the condition-(14) milestone records precisely the restricted pressure claim. Ogata, pp. 12–15

Formalization scope

The Lean model uses finite matrices for local algebras. A nonempty finite site basis represents Md(C)M_d(\mathbb C)Md​(C), with site 1 indexed by 0. An interaction stores one Hermitian term for each support anchored at its least site; all translates that fit in [1,n][1,n][1,n] appear in the Hamiltonian. The scalar empty-set term is retained. The auxiliary algebra is represented by a full matrix algebra Mk(C)M_k(\mathbb C)Mk​(C); finite-dimensional C∗C^*C∗-algebra data have an equivalent full-matrix representation for the generated local states. Stationarity is written in the primal trace form. The recursive local state places the first site's matrix in the outermost application of E\mathcal EE.

The spectral law is formed from the eigenvalues and spectral weights of the actual Hamiltonian. It is not supplied as an arbitrary sequence of measures. The theorem uses no ergodicity, spectral-gap, or condition-(14) binder, and both LDP bounds range over every closed or open subset of R\mathbb RR. Logarithms of probabilities take values in the extended reals, with log⁡0=−∞\log0=-\inftylog0=−∞; sequence limits are at n→∞n\to\inftyn→∞, so the placeholder value at n=0n=0n=0 is immaterial. Nonnegative lower integrals represent exponential moments. In the restricted pressure milestone, the real logarithm applies to a positive state expectation. These choices also rule out a vacuous proof based on a zero measure, a moment represented by a non-integrable Bochner integral, or a rate function unrelated to the spectral law.

Reusable contributions include finite-dimensional spectral-law lemmas, positivity and stationarity facts for completely positive maps, good-rate-function and LDP lemmas on R\mathbb RR, and the Gärtner–Ellis result. The full theorem additionally needs a treatment of non-ergodic finite mixtures and periodic components that preserves both large-deviation bounds.

Selected references

  • Yoshiko Ogata, Large Deviations in Quantum Spin Chain, arXiv preprint, 2008. arXiv:0803.0113v1.
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Mathematical PhysicsQuantum InformationQuantum Mechanics·Captain: mikedeng1

A No-Go Theorem for Gaussian Quantum Error Correction: Gaussian Encoding and Decoding Cannot Lower the Entanglement Degradation of a Single-Mode Gaussian ChannelResearch Paper

Motivation

Optical quantum communication commonly encodes information in continuous variables such as the position and momentum quadratures of a light mode. Gaussian states and Gaussian operations are attractive in this setting because phase shifters, squeezers, beam splitters, and homodyne measurements are standard optical tools. Transmission through a lossy or noisy line can also be modeled by a Gaussian channel. The practical question is whether adding vacuum modes and Gaussian encoding and decoding can protect a signal against such a channel. Niset, Fiurášek, and Cerf (2008) give a negative answer for the code class defined in their Fig. 1.

The result sits after the early impossibility results for distilling Gaussian entanglement with Gaussian operations, including Giedke and Cirac (2002). Those results concern shared states and allowed local operations. The 2008 paper asks the channel-coding question directly: whether a finite Gaussian code can make a fixed single-mode Gaussian channel less damaging to entanglement. It introduces a scalar, entanglement degradation, to state the answer for every single-mode Gaussian channel in one inequality.

Setting

A single optical mode has two real quadratures, xxx and ppp. For nnn modes, the order is (x1,p1,…,xn,pn)(x_1,p_1,\ldots,x_n,p_n)(x1​,p1​,…,xn​,pn​). A state has a real covariance matrix γ\gammaγ recording its second moments in this order. The vacuum covariance matrix is the identity III. A Gaussian channel TTT on one mode is described at the covariance level by two real 2×22\times22×2 matrices MMM and NNN:

γ⟼MγMT+N.\gamma\longmapsto M\gamma M^{\mathsf T}+N.γ⟼MγMT+N.

Here NNN is the added noise. Complete positivity imposes symmetry and a matrix positivity condition on NNN; in particular, it gives det⁡N≥(det⁡M−1)2\det N\ge(\det M-1)^2detN≥(detM−1)2. A Gaussian unitary changes covariances by a symplectic matrix SSS, satisfying SJST=JSJS^{\mathsf T}=JSJST=J for the canonical symplectic form JJJ. Displacements affect first moments only and therefore play no role in these covariance formulas.

The code G(n,E,D)G(n,E,D)G(n,E,D) uses a positive integer nnn. The input occupies mode zero in the formalization; the other n−1n-1n−1 modes are vacuum ancillas. A Gaussian encoding unitary EEE acts on all modes, then the same channel TTT acts independently once on each mode, and a Gaussian decoding unitary DDD acts on all modes. Only the first output mode is retained. This defines an effective single-mode channel TGCT_{GC}TGC​ with matrices MGC,NGCM_{GC},N_{GC}MGC​,NGC​. The ancillas contribute noise to NGCN_{GC}NGC​ even before the nnn channel uses are counted.

For a channel T=(M,N)T=(M,N)T=(M,N), the paper defines its degradation by

D[T]=min⁡{det⁡N(1+det⁡M)2,1}.D[T]=\min\left\{\frac{\det N}{(1+\det M)^2},1\right\}.D[T]=min{(1+detM)2detN​,1}.

The intended value is 111 when the denominator vanishes: the quotient is then interpreted as infinite and is saturated by the minimum. This quantity is related to the entanglement remaining when TTT acts on one half of a two-mode squeezed vacuum as the squeezing grows. The paper measures that entanglement through the smallest symplectic eigenvalue ν−\nu_-ν−​ after partial transpose and the logarithmic negativity EN=max⁡{0,−log⁡ν−}E_N=\max\{0,-\log\nu_-\}EN​=max{0,−logν−​}.

Formalization targets

Main no-go theorem

The mission goal is the theorem on page 3, equation (11): for every completely positive single-mode Gaussian channel and every finite code of the stated form,

D[T]≤D[TGC].D[T]\le D[T_{GC}].D[T]≤D[TGC​].

This is the assertion that the code cannot lower the channel's entanglement degradation. It includes n=1n=1n=1, singular channels, and channels with negative determinant MMM. No numerical performance constant or bound on the number of modes is fixed.

Supporting results

The milestones record the paper's channel-noise constraint (2), the fact that the code produces a Gaussian channel, the local matrix normal forms used in Lemma 2, the asymptotic calculations (8) and (10), the entanglement-breaking case, and Lemma 2 itself. Lemma 2 characterizes the degradation through the limiting squared eigenvalue and, when finite, gives EN=−12log⁡D[T]E_N=-\tfrac12\log D[T]EN​=−21​logD[T]. The milestones retain the paper's distinction between positive, negative, and zero determinant regimes.

Significance

The theorem rules out a specific and broad way of improving Gaussian transmission: adding any finite number of vacuum ancillas and using Gaussian unitaries before and after independent uses of a fixed channel cannot improve this intrinsic entanglement measure. The paper applies this conclusion to attenuation, amplification, and classical-noise channels, showing how an apparent reduction in one channel parameter can be offset by increased noise. It also relates degradation to an upper bound on quantum capacity, though that further bound is outside this mission. Niset, Fiurášek, and Cerf (2008)

The paper's theorem is proved in the mathematical literature; the goal here is a machine-checked statement and, eventually, a proof in the covariance-matrix representation. The published covariance layer already supplies symplectic forms, two-mode squeezed covariances, partial transpose, and an intrinsic ν−\nu_-ν−​; this mission adds the channel and code definitions required to state the no-go theorem. Those definitions can be reused for other single-mode Gaussian-channel questions. A complete proof still needs substantial results connecting codes, Gaussian operations, and entanglement behavior; a compiled sorry statement alone does not establish the theorem.

Difficulty

One might try to compare det⁡N\det NdetN before and after the code. That scalar does not track the code: encoding mixes signal and vacuum modes, each copy of the channel adds noise, decoding mixes the modes again, and discarding modes changes both MGCM_{GC}MGC​ and NGCN_{GC}NGC​. Neither determinant separately gives the desired inequality. The boundary det⁡M=−1\det M=-1detM=−1 also defeats a direct real-valued transcription of the printed quotient. The asymptotic entanglement formulas cross several determinant regimes, with different normal forms and a separate entanglement-breaking case. The central challenge is to retain the physical meaning of all these cases in one theorem over arbitrary finite codes.

Formalization scope

Lean uses real matrices indexed by interleaved mode and quadrature coordinates. The published QAlgorithms_Papers_Independent_Frontier30_P13 layer provides ModeQuadrature, phaseJ, squeezedCM, partial transpose, and the intrinsic smallest symplectic eigenvalue lambdaMin; QAlgorithms_Papers_Independent_Dependency50_P10 provides entrywise complexification. A channel is required to satisfy the Gaussian complete-positivity matrix inequality. Encoders and decoders satisfy SJST=JSJS^{\mathsf T}=JSJST=J. The code uses the same (M,N)(M,N)(M,N) on every one of its nnn modes, with n≥1n\ge1n≥1, and includes the vacuum covariance on every ancillary mode. Gaussian unitaries enter through their symplectic matrices; their displacement parts do not affect covariances.

The definition of DDD explicitly saturates at 111 when 1+det⁡M=01+\det M=01+detM=0, avoiding Lean's zero value for division by zero. The squeezed input uses cosh⁡(2r)\cosh(2r)cosh(2r) and sinh⁡(2r)\sinh(2r)sinh(2r). The eigenvalue ν−\nu_-ν−​ is the intrinsic lambdaMin, not an unguarded square-root expression. Logarithmic negativity uses the natural logarithm; its finite limit statement assumes det⁡N>0\det N>0detN>0, while the degradation statement still covers det⁡N=0\det N=0detN=0. The infinite-squeezing output is represented by limits of finite-rrr covariances and entanglement quantities.

The code's vacuum term, all nnn noise blocks, the symplectic equation, and the guarded degradation are essential to the target; dropping any of them would change the question. Lemma 1's teleportation equivalence and the external Gaussian no-distillation theorem are not formalized here. Their faithful treatment would require operational Gaussian states, measurements, and protocols beyond the covariance model. Contributions establishing those interfaces, proving the stated matrix milestones, or connecting the two layers are welcome.

Selected references

  • J. Niset, J. Fiurášek, and N. J. Cerf, A No-Go Theorem for Gaussian Quantum Error Correction, Physical Review Letters 102, 120501, 2009; arXiv:0811.3128v1 (2008). The preprint is the citation basis for page and equation numbers here.
  • G. Giedke and J. I. Cirac, Characterization of Gaussian operations and distillation of Gaussian states, Physical Review A 66, 032316, 2002; arXiv:quant-ph/0204085.
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Qudit circuits with SU(d) symmetry: Locality imposes additional conservation laws: Tr(Ω[ρ]^l) is conserved by every unitary generated by 2-local SU(d)-invariant gatesResearch Paper

Motivation

Quantum circuits whose gates respect a global symmetry are a standard model for quantum simulation, for symmetry-protected quantum computing, and for the study of conserved quantities in quantum dynamics. For SU(d) symmetry on nnn qudits, the unitaries that commute with every U⊗nU^{\otimes n}U⊗n are, by Schur–Weyl duality, exactly the unitaries in the linear span of the qudit permutations. A natural question is whether every such unitary can be built from local symmetric gates, as happens without symmetry, where 2-qudit gates are universal.

Marvian, Liu and Hulse (arXiv:2105.12877) show that for d≥3d \ge 3d≥3 the answer is no, and that the obstruction appears as conservation laws. Unitaries generated by 2-local SU(d)-invariant gates conserve quantities that general SU(d)-invariant unitaries change. The paper gives two families of such laws. The first, Theorem 1 (the fsgnf_{\mathrm{sgn}}fsgn​ law, from a Z2\mathbb Z_2Z2​ symmetry of the swap Hamiltonians), is a separate result of the paper and is not part of this mission. The second, Theorem 2, is the target here. It comes from a correspondence between a subspace of the qudits and a system of free fermions.

Timeline: Marvian (Nature Physics 18, 283, 2022) showed that symmetry together with locality restricts the realizable unitaries in general, with examples for U(1) and SU(2) symmetry. For qubits with SU(2) symmetry, the constraints restrict only relative phases between sectors of inequivalent irreducible representations (p. 3 of the present paper). The present paper (arXiv:2105.12877, v2 January 2022) treats SU(d) with d≥3d\ge 3d≥3, where constraints beyond relative phases appear. The connection to Marin's 2007 description of the Lie algebra generated by transpositions (J. Algebra 310, 742) is discussed on p. 9.

Setting

Consider nnn qudits with Hilbert space (Cd)⊗n(\mathbb C^d)^{\otimes n}(Cd)⊗n and computational basis ∣x1⟩⋯∣xn⟩|x_1\rangle\cdots|x_n\rangle∣x1​⟩⋯∣xn​⟩, xi∈{0,…,d−1}x_i\in\{0,\dots,d-1\}xi​∈{0,…,d−1}.

  • A unitary VVV is SU(d)-invariant if [V,U⊗n]=0[V,U^{\otimes n}]=0[V,U⊗n]=0 for every U∈SU(d)U\in\mathrm{SU}(d)U∈SU(d) (Eq. (1)).
  • VVV is 2-local on qudits a,ba,ba,b if V=Wab⊗IrestV=W_{ab}\otimes\mathbb I_{\text{rest}}V=Wab​⊗Irest​.
  • V2\mathcal V_2V2​ is the group generated by finite products of 2-local SU(d)-invariant unitaries.
  • P(σ)\mathbf P(\sigma)P(σ) is the permutation operator of σ∈Sn\sigma\in S_nσ∈Sn​, and Pab\mathbf P_{ab}Pab​ is the swap of qudits a,ba,ba,b.

For L≤min⁡{n,d−1}L\le\min\{n,d-1\}L≤min{n,d−1}, the vector (⋀m=1L∣m⟩)⊗∣0⟩⊗(n−L)\big(\bigwedge_{m=1}^L|m\rangle\big)\otimes|0\rangle^{\otimes(n-L)}(⋀m=1L​∣m⟩)⊗∣0⟩⊗(n−L) antisymmetrizes the levels 1,…,L1,\dots,L1,…,L over the first LLL qudits with weight 1/L!1/\sqrt{L!}1/L!​ (Eq. (40)). The subspace Hcomp\mathcal H_{\mathrm{comp}}Hcomp​ is the span of all permutations of these vectors (Eq. (42)), and Πcomp\Pi_{\mathrm{comp}}Πcomp​ is the orthogonal projector onto it.

For an operator AAA on one qudit, AiA_iAi​ is AAA acting on qudit iii. Let Qij=(Ii−∣0⟩⟨0∣i)∣0⟩⟨0∣jQ_{ij}=(\mathbb I_i-|0\rangle\langle0|_i)|0\rangle\langle0|_jQij​=(Ii​−∣0⟩⟨0∣i​)∣0⟩⟨0∣j​. The map Ω\OmegaΩ sends an operator ρ\rhoρ on the qudits to the n×nn\times nn×n matrix

Ω[ρ]=∑i,j=1nΩij[ρ] ∣i⟩⟨j∣,Ωij[ρ]={Tr(ΠcompρΠcomp PijQij)i≠j,Tr(ΠcompρΠcomp (Ii−∣0⟩⟨0∣i))i=j\Omega[\rho]=\sum_{i,j=1}^n\Omega_{ij}[\rho]\,|i\rangle\langle j|,\qquad \Omega_{ij}[\rho]=\begin{cases}\mathrm{Tr}\big(\Pi_{\mathrm{comp}}\rho\Pi_{\mathrm{comp}}\,\mathbf P_{ij}Q_{ij}\big)& i\neq j,\\ \mathrm{Tr}\big(\Pi_{\mathrm{comp}}\rho\Pi_{\mathrm{comp}}\,(\mathbb I_i-|0\rangle\langle0|_i)\big)& i=j\end{cases}Ω[ρ]=i,j=1∑n​Ωij​[ρ]∣i⟩⟨j∣,Ωij​[ρ]={Tr(Πcomp​ρΠcomp​Pij​Qij​)Tr(Πcomp​ρΠcomp​(Ii​−∣0⟩⟨0∣i​))​i=j,i=j​

(Eqs. (49), (51)). On the fermionic side there are nnn sites, creation operators cj†c_j^\daggercj†​, the vacuum ∣vac⟩|\mathrm{vac}\rangle∣vac⟩, and the fermionic swap Pabf=If−(ca†−cb†)(ca−cb)\mathbf P^f_{ab}=\mathbb I^f-(c_a^\dagger-c_b^\dagger)(c_a-c_b)Pabf​=If−(ca†​−cb†​)(ca​−cb​) (Eq. (28)). Its single-particle counterpart is Eab=I−(∣a⟩−∣b⟩)(⟨a∣−⟨b∣)E_{ab}=\mathbb I-(|a\rangle-|b\rangle)(\langle a|-\langle b|)Eab​=I−(∣a⟩−∣b⟩)(⟨a∣−⟨b∣) on Cn\mathbb C^nCn (Eq. (33)). The map UfU^fUf sends P(σ)[(⋀m∣m⟩)⊗∣0⟩⊗(n−L)]\mathbf P(\sigma)\big[\big(\bigwedge_{m}|m\rangle\big)\otimes|0\rangle^{\otimes(n-L)}\big]P(σ)[(⋀m​∣m⟩)⊗∣0⟩⊗(n−L)] to ∏i=1Lcσ(i)†∣vac⟩\prod_{i=1}^L c^\dagger_{\sigma(i)}|\mathrm{vac}\rangle∏i=1L​cσ(i)†​∣vac⟩ (Eq. (41)).

Formalization targets

Goal: Theorem 2 (p. 11)

For every V∈V2V\in\mathcal V_2V∈V2​, every density operator ρ\rhoρ on nnn qudits and every positive integer lll,

Tr(Ω[VρV†]l)=Tr(Ω[ρ]l).\mathrm{Tr}\big(\Omega[V\rho V^\dagger]^l\big)=\mathrm{Tr}\big(\Omega[\rho]^l\big).Tr(Ω[VρV†]l)=Tr(Ω[ρ]l).

The statement holds for all nnn and ddd. Its content is the case l≥2l\ge 2l≥2: the case l=1l=1l=1 holds for every SU(d)-invariant unitary (Eq. (55)).

Milestones (in attack order)

  1. Eq. (5): up to a global phase, a 2-local SU(d)-invariant unitary on qudits a,ba,ba,b equals eiθPab=cos⁡θ I+isin⁡θ Pabe^{i\theta\mathbf P_{ab}}=\cos\theta\,\mathbb I+i\sin\theta\,\mathbf P_{ab}eiθPab​=cosθI+isinθPab​.
  2. Eqs. (27)–(29): Pabfcj†Pabf†=cσab(j)†\mathbf P^f_{ab}c_j^\dagger\mathbf P^{f\dagger}_{ab}=c^\dagger_{\sigma_{ab}(j)}Pabf​cj†​Pabf†​=cσab​(j)†​, Pabf∣vac⟩=∣vac⟩\mathbf P^f_{ab}|\mathrm{vac}\rangle=|\mathrm{vac}\ranglePabf​∣vac⟩=∣vac⟩, and Pabf\mathbf P^f_{ab}Pabf​ is Hermitian and unitary.
  3. Eq. (31): eiθPabfcj†e−iθPabf=e−iθ(cos⁡θ cj†+isin⁡θ cσab(j)†)e^{i\theta\mathbf P^f_{ab}}c_j^\dagger e^{-i\theta\mathbf P^f_{ab}}=e^{-i\theta}(\cos\theta\,c_j^\dagger+i\sin\theta\,c^\dagger_{\sigma_{ab}(j)})eiθPabf​cj†​e−iθPabf​=e−iθ(cosθcj†​+isinθcσab​(j)†​).
  4. Eq. (34): the same dynamics written through the single-particle unitary eiθ(Eab−I)e^{i\theta(E_{ab}-\mathbb I)}eiθ(Eab​−I).
  5. p. 9: P(σ)Πcomp=ΠcompP(σ)\mathbf P(\sigma)\Pi_{\mathrm{comp}}=\Pi_{\mathrm{comp}}\mathbf P(\sigma)P(σ)Πcomp​=Πcomp​P(σ).
  6. Eq. (41) and App. C5: UfU^fUf satisfies (41) and is an isometry on Hcomp\mathcal H_{\mathrm{comp}}Hcomp​.
  7. Eq. (44): UfeiθPabΠcomp=eiθPabfUfΠcompU^fe^{i\theta\mathbf P_{ab}}\Pi_{\mathrm{comp}}=e^{i\theta\mathbf P^f_{ab}}U^f\Pi_{\mathrm{comp}}UfeiθPab​Πcomp​=eiθPabf​UfΠcomp​.
  8. App. C7, (C42)–(C43): the qudit form (51) and the fermionic form (50) of Ω\OmegaΩ agree.
  9. Lemma 3: Ω[eiθPabρe−iθPab]=eiθEabΩ[ρ]e−iθEab\Omega[e^{i\theta\mathbf P_{ab}}\rho e^{-i\theta\mathbf P_{ab}}]=e^{i\theta E_{ab}}\Omega[\rho]e^{-i\theta E_{ab}}Ω[eiθPab​ρe−iθPab​]=eiθEab​Ω[ρ]e−iθEab​, and Ω\OmegaΩ is completely positive.

Significance

Theorem 2 gives an infinite family of polynomial invariants of the state, Tr(Ω[ρ]l)\mathrm{Tr}(\Omega[\rho]^l)Tr(Ω[ρ]l) for l=1,2,…l=1,2,\dotsl=1,2,…. Together these fix the spectrum of Ω[ρ]\Omega[\rho]Ω[ρ], so every Rényi entropy of the single-particle density operator Ω[ρ]/Tr Ω[ρ]\Omega[\rho]/\mathrm{Tr}\,\Omega[\rho]Ω[ρ]/TrΩ[ρ] is conserved. Already for l=2l=2l=2 the law is violated by SU(d)-invariant Hamiltonians with 3-local terms (p. 11 and §IV D). This shows that, for d≥3d\ge3d≥3, 2-local SU(d)-invariant gates are not universal among SU(d)-invariant unitaries, even up to relative phases, and that 3-local interactions can be detected from the dynamics of Ω\OmegaΩ. For d=2d=2d=2 the laws hold for all SU(2)-invariant unitaries.

The result is proved in the paper. As far as a search of the platform shows, it has not been formalized. A formalization adds machine-checked versions of the qudit–fermion correspondence of §IV B, including the isometry UfU^fUf and the intertwining relation (44), and of the free-fermion form of the swap dynamics. These are statements about finite-dimensional matrices, so the whole development stays inside Mathlib's linear algebra.

Difficulty

The obvious route is to show that each generator acts on Ω[ρ]\Omega[\rho]Ω[ρ] by conjugation with an n×nn\times nn×n unitary, and then to induct over products. The difficulty is the generator step. The definition (51) of Ω\OmegaΩ involves the projector Πcomp\Pi_{\mathrm{comp}}Πcomp​ onto a span of antisymmetrized vectors, and nothing in (51) shows directly why conjugating ρ\rhoρ by eiθPabe^{i\theta\mathbf P_{ab}}eiθPab​ should conjugate Ω[ρ]\Omega[\rho]Ω[ρ] by eiθEabe^{i\theta E_{ab}}eiθEab​. The covariance becomes visible only after Hcomp\mathcal H_{\mathrm{comp}}Hcomp​ is identified with fermionic Fock sectors, where the swap becomes a quadratic, particle-number-preserving Hamiltonian. That identification needs care with the signs of the fermionic creation operators and with the ordering of products. A second obstacle is the characterization of the generators (Eq. (5)). It rests on the commutant of {U⊗U:U∈SU(d)}\{U\otimes U : U\in\mathrm{SU}(d)\}{U⊗U:U∈SU(d)} being spanned by I\mathbb II and the swap, a Schur–Weyl statement for two qudits that Mathlib does not provide.

Formalization scope

Operators on the qudits are matrices indexed by Fin n → Fin d, with sites and levels 0-based and [NeZero d] assumed so that ∣0⟩|0\rangle∣0⟩ exists. Fock-space operators are matrices indexed by Finset (Fin n), the set of occupied sites. The creation operator uses the Jordan–Wigner sign (−1)∣{k∈T:k<j}∣(-1)^{|\{k\in T:k<j\}|}(−1)∣{k∈T:k<j}∣, the encoding of the public definition QAlgorithms_Papers_Independent_Next46_P23, copied rather than imported.

The following conventions are fixed:

  • P(σ)∣y⟩=∣y∘σ−1⟩\mathbf P(\sigma)|y\rangle=|y\circ\sigma^{-1}\rangleP(σ)∣y⟩=∣y∘σ−1⟩, the representation convention the paper uses in Eq. (30) and App. C5. Eq. (9) as printed describes P(σ−1)\mathbf P(\sigma^{-1})P(σ−1), and under it the map of Eq. (41) is not well defined. All other objects coincide under the two conventions.
  • Exponentials of involutions are written in the closed form cos⁡θ I+isin⁡θX\cos\theta\,\mathbb I+i\sin\theta XcosθI+isinθX of Eq. (5), and θ\thetaθ ranges over [0,2π)[0,2\pi)[0,2π) as in the paper.
  • Πcomp\Pi_{\mathrm{comp}}Πcomp​ is the matrix of Mathlib's orthogonal projection onto Hcomp⊆\mathcal H_{\mathrm{comp}}\subseteqHcomp​⊆ EuclideanSpace ℂ (Fin n → Fin d).
  • UfU^fUf is an explicit linear map defined on the whole space. It sends the basis state with ∣m⟩|m\rangle∣m⟩ on site p(m)p(m)p(m), m=1,…,Lm=1,\dots,Lm=1,…,L, to 1L!cp(1)†⋯cp(L)†∣vac⟩\frac1{\sqrt{L!}}c^\dagger_{p(1)}\cdots c^\dagger_{p(L)}|\mathrm{vac}\rangleL!​1​cp(1)†​⋯cp(L)†​∣vac⟩, and all other basis states to 000.
  • Complete positivity is the published QAlgorithms.Entanglement.IsCompletelyPositive.

The following trivializing formalizations are ruled out:

  • Ω\OmegaΩ is not identically zero: the normalization 1/L!1/\sqrt{L!}1/L!​ and the range L≤min⁡{n,d−1}L\le\min\{n,d-1\}L≤min{n,d−1} are as printed, and Hcomp≠0\mathcal H_{\mathrm{comp}}\neq 0Hcomp​=0 is checked.
  • V2\mathcal V_2V2​ is the group generated by all 2-local SU(d)-invariant unitaries, defined literally on p. 3. It is neither the generating set of Eq. (6) nor the group of all SU(d)-invariant unitaries, for which the statement is false when d≥3d\ge3d≥3.
  • The goal uses the qudit form (51) of Ω\OmegaΩ, not the fermionic form (50).

A complete development needs:

  • the two-qudit commutant of U⊗UU\otimes UU⊗U;
  • the CAR algebra on Finset Fock space;
  • the orthonormality of the antisymmetrized vectors;
  • the trace identity Tr((WXW†)l)=Tr(Xl)\mathrm{Tr}((WXW^\dagger)^l)=\mathrm{Tr}(X^l)Tr((WXW†)l)=Tr(Xl).

The Fock-space and permutation-operator lemmas can be reused for other qudit–fermion and Schur–Weyl statements. Contributions welcome: proofs of any milestone, and lemma-level infrastructure on the Fock space.

Selected references

  • I. Marvian, H. Liu, A. Hulse, Qudit circuits with SU(d) symmetry: Locality imposes additional conservation laws, arXiv:2105.12877v2, 2022. https://arxiv.org/abs/2105.12877
  • I. Marvian, Restrictions on realizable unitary operations imposed by symmetry and locality, Nature Physics 18, 283–289, 2022. https://doi.org/10.1038/s41567-021-01464-0
  • I. Marin, L'algèbre de Lie des transpositions, Journal of Algebra 310, 742–774, 2007. https://doi.org/10.1016/j.jalgebra.2006.08.018
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CombinatoricsGraph TheoryOperations Research+1·Captain: mikedeng1

A (Slightly) Improved Approximation Algorithm for Metric TSP: Max-Entropy Spanning Tree Plus Odd-Vertex Matching Costs at Most (3/2 − ε)·OPT in Expectation, ε > 10⁻³⁶Research Paper

Motivation

The metric traveling salesperson problem asks for the cheapest tour through a finite set of cities whose pairwise costs are symmetric and satisfy the triangle inequality. The classical Christofides–Serdyukov algorithm combines a spanning tree with a matching on its odd-degree vertices and has a worst-case guarantee of 3/23/23/2 times the optimal tour cost. Karlin, Klein, and Oveis Gharan showed that a randomized choice of spanning tree can improve that factor by an absolute amount, however small. Their Theorem 1.1 gives an ε>10−36\varepsilon>10^{-36}ε>10−36 for which the expected cost is at most (3/2−ε)OPT⁡(3/2-\varepsilon)\operatorname{OPT}(3/2−ε)OPT Karlin–Klein–Oveis Gharan, §1.

The paper was circulated as a preprint before its 2024 Operations Research publication. This mission uses the pinned arXiv version 6, whose theorem numbers and page references appear throughout. The authors explicitly distinguish their algorithmic guarantee from an improvement to the Held–Karp integrality gap; the former does not itself establish the latter Karlin–Klein–Oveis Gharan, p. 1. Their separate work studies that integrality-gap question Karlin–Klein–Oveis Gharan, 2022.

Setting

Let VVV be a set of n≥3n\ge3n≥3 cities and let c(u,v)c(u,v)c(u,v) be a metric cost. A tour visits every city once and returns to its start; OPT⁡(c)\operatorname{OPT}(c)OPT(c) is the least tour cost. A Held–Karp vector x0x^0x0 assigns a nonnegative fractional value to every undirected edge, has degree two at every city, and crosses every nontrivial vertex cut with total value at least two. Its objective is c(x0)=12∑u,vc(u,v)xuv0c(x^0)=\tfrac12\sum_{u,v}c(u,v)x^0_{uv}c(x0)=21​∑u,v​c(u,v)xuv0​. We take x0x^0x0 to attain the minimum Held–Karp objective. These objects reuse the published MetricTSP model.

The paper chooses any city uuu and splits it into u0u_0u0​ and v0v_0v0​. Each edge incident to uuu gives half its LP value to each copy. A new edge e0={u0,v0}e_0=\{u_0,v_0\}e0​={u0​,v0​} has LP value one and cost zero. Let EEE be the positive support of the split LP vector after removing e0e_0e0​, and let xxx denote its values on EEE. A spanning-tree law μ\muμ gives probabilities to the spanning trees contained in EEE and has marginal Pr⁡T∼μ[e∈T]=xe\Pr_{T\sim\mu}[e\in T]=x_ePrT∼μ​[e∈T]=xe​ for each e∈Ee\in Ee∈E.

Among all such laws, a maximum-entropy law maximizes H(μ)=−∑Tμ(T)log⁡μ(T)H(\mu)=-\sum_T\mu(T)\log\mu(T)H(μ)=−∑T​μ(T)logμ(T), taking 0log⁡0=00\log0=00log0=0. A sampled tree TTT has an even number of odd-degree vertices. Let MTM_TMT​ be a minimum-cost perfect matching of those vertices in the complete metric graph. The cost studied here is algCost⁡(c,μ)=ET∼μ[c(T)+c(MT)]\operatorname{algCost}(c,\mu)=\mathbb E_{T\sim\mu}[c(T)+c(M_T)]algCost(c,μ)=ET∼μ​[c(T)+c(MT​)]. The tree and matching make a connected Eulerian multigraph; metric shortcutting gives a tour with no larger cost Karlin–Klein–Oveis Gharan, pp. 1–3.

Formalization targets

The goal is a single absolute constant, chosen before the size, costs, LP optimum, split city, or tree law:

∃ε>10−36∀(n,c,x0,u,μ),algCost⁡(c′,μ)≤(32−ε)OPT⁡(c).\exists\varepsilon>10^{-36}\quad\forall(n,c,x^0,u,\mu),\qquad \operatorname{algCost}(c',\mu) \le\left(\frac32-\varepsilon\right)\operatorname{OPT}(c).∃ε>10−36∀(n,c,x0,u,μ),algCost(c′,μ)≤(23​−ε)OPT(c).

Here c′c'c′ is the split cost, x0x^0x0 is any Held–Karp optimum, and μ\muμ is any maximum-entropy law with exact marginals of the split LP vector. The maximum-entropy existence milestone ensures this class of laws is nonempty. The attack path records the node split, membership in the spanning-tree polytope, existence of the exact law, the tree-cost identity, the OOO-join characterization, Theorem 3.1's payment bounds, and the final expected matching-cost bound Karlin–Klein–Oveis Gharan, pp. 2, 6, 18–19.

The proof of Theorem 1.1 uses εP=3.12⋅10−16\varepsilon_P=3.12\cdot10^{-16}εP​=3.12⋅10−16, η=εP/1308\eta=\varepsilon_P/1308η=εP​/1308, and β=η/4.1\beta=\eta/4.1β=η/4.1. Its matching analysis gives the sharper intermediate target E[c(MT)]≤(1/2−εPβ/6)OPT⁡\mathbb E[c(M_T)]\le(1/2-\varepsilon_P\beta/6)\operatorname{OPT}E[c(MT​)]≤(1/2−εP​β/6)OPT. With the expected tree cost at most OPT⁡\operatorname{OPT}OPT, this yields an improvement greater than 10−3610^{-36}10−36 Karlin–Klein–Oveis Gharan, proof of Theorem 1.1.

Significance

The result supplies a strict improvement over the 3/23/23/2 guarantee for general metric TSP using a specified random-tree and parity-correction algorithm. It also isolates a useful probabilistic statement: a maximum-entropy spanning-tree law with fixed LP marginals admits a cheaper expected odd-vertex matching than the standard half-of-OPT bound. The constant is tiny; the claim is a worst-case theoretical guarantee rather than a prediction of practical performance Karlin–Klein–Oveis Gharan, §1.

The paper theorem is proved, but the statements in this mission have no machine-checked proofs yet. A completed formalization would connect existing Lean definitions for tours, Held–Karp feasibility, graph cost, tour incidence vectors, and TTT-joins to reusable definitions for finite spanning-tree distributions, entropy, rooted near-minimum cuts, and the OOO-join cut relaxation. The mission also keeps the quantitative constants and the uniform order of quantifiers visible to later developments.

Difficulty

The marginal constraints make the expected tree cost straightforward, but they do not determine the parity of a tree cut. A matching on the odd-degree vertices must simultaneously satisfy every relevant parity cut, while its total expected cost must fall strictly below half of the optimal tour. Near-minimum cuts can overlap and cross, so a bound on any one cut does not automatically coexist with bounds on all the others. Theorem 3.1 captures the required simultaneous payment statement, including a negative expected payment on LP edges and a controlled positive payment on optimal-tour edges Karlin–Klein–Oveis Gharan, §3.

Formalization scope

Cities are Fin n with n≥3n\ge3n≥3; edges are unordered pairs, and LP vectors remain symmetric functions on ordered city pairs as in the published Held–Karp model. Cut sums count each crossing edge once. A tree is a finite edge set that spans the split vertex type Fin (n+1). Distributions and expectations are finite sums, with probabilities zero away from spanning trees of EEE. The distinguished edge has split cost zero and LP value one. Matchings use an involution on the vertices, fixed on even-degree vertices; the matching cost is half the sum over matched vertices. The real infimum defining that cost is over a finite, nonempty set.

The paper's printed spanning-tree inequality for S=∅S=\varnothingS=∅ has the impossible bound 0≤−10\le-10≤−1, so Fact 2.1 uses nonempty SSS. Theorem 3.1 explicitly assumes 0≤η≤10−120\le\eta\le10^{-12}0≤η≤10−12: without nonnegativity, its bound on a nonnegative random vector can be negative. Every near-minimum cut is nonempty and excludes both endpoints of e0e_0e0​, matching the paper's rooted-cut convention. The optimal tour in Theorem 3.1 is any optimal Hamiltonian cycle through e0e_0e0​. The O-join bound uses ye0=1y_{e_0}=1ye0​​=1 in place of the proof's infinite placeholder; the edge has zero cost.

The goal uses the exact maximum-entropy law. An arbitrary tree distribution would not state the paper's improvement, and an existential over unspecified tour-producing procedures would be satisfied by always returning an optimal tour. The polynomial-time construction of an approximately marginal-preserving λ\lambdaλ-uniform sampler, and therefore the runtime guarantee of the algorithm as implemented in the paper, are outside this formalization. The path version, Theorem 1.2, is also outside this mission Karlin–Klein–Oveis Gharan, §1.1 and proof of Theorem 1.1.

Selected references

  • A. R. Karlin, N. Klein, and S. Oveis Gharan, A (Slightly) Improved Approximation Algorithm for Metric TSP, Operations Research, 2024; arXiv:2007.01409v6.
  • A. R. Karlin, N. Klein, and S. Oveis Gharan, A (Slightly) Improved Bound on the Integrality Gap of the Subtour LP for TSP, FOCS, 2022; arXiv:2105.10043.
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Quantum InformationTheoretical Computer Science·Captain: mikedeng1

Asymptotically Optimal Approximation of Single Qubit Unitaries by Clifford and T Circuits Using a Constant Number of Ancillary Qubits: O(log(1/ε)) Gates Approximate Every Single-Qubit UnitaryResearch Paper

Motivation

A fault-tolerant quantum computer executes only a discrete set of gates. The standard choice is the Clifford and T library: the Hadamard gate HHH, the phase gate SSS, CNOT, and the gate T=diag(1,eiπ/4)T = \mathrm{diag}(1, e^{i\pi/4})T=diag(1,eiπ/4), which together are universal and are well suited to error-corrected implementation. Every other gate, in particular every single-qubit rotation that appears in quantum simulation or the quantum Fourier transform, has to be approximated by a circuit over this library, and the number of gates spent per rotation multiplies the cost of the whole computation. The question is therefore how many library gates are needed to approximate a single-qubit unitary to precision ε\varepsilonε.

A short history of the question:

  • Solovay–Kitaev (Kitaev 1997; Dawson–Nielsen 2005, arXiv:quant-ph/0505030): any universal library approximates any single-qubit unitary with O(log⁡3+δ(1/ε))O(\log^{3+\delta}(1/\varepsilon))O(log3+δ(1/ε)) gates, without ancillas.
  • Lower bound (Harrow–Recht–Chuang 2002, arXiv:quant-ph/0111031): a volume count shows that Ω(log⁡(1/ε))\Omega(\log(1/\varepsilon))Ω(log(1/ε)) gates are necessary in general.
  • Phase kickback: a special resource state on O(log⁡(1/ε))O(\log(1/\varepsilon))O(log(1/ε)) ancilla qubits gives O(log⁡(1/ε))O(\log(1/\varepsilon))O(log(1/ε)) gates, but the resource state itself costs O(log⁡2(1/ε)log⁡log⁡(1/ε))O(\log^2(1/\varepsilon)\log\log(1/\varepsilon))O(log2(1/ε)loglog(1/ε)) gates and O(log⁡2(1/ε))O(\log^2(1/\varepsilon))O(log2(1/ε)) ancillas.
  • Exact synthesis (Kliuchnikov–Maslov–Mosca 2012, arXiv:1206.5236; Giles–Selinger 2012, arXiv:1212.0506): a unitary is a Clifford and T circuit, on the same qubits plus at most one ancilla, exactly when its entries lie in the ring Z[i,1/2]\mathbb Z[i, 1/\sqrt2]Z[i,1/2​], with gate count linear in the denominator exponent.
  • This paper (Kliuchnikov–Maslov–Mosca, December 2012, arXiv:1212.0822): with two ancillas initialized to ∣0⟩|0\rangle∣0⟩, O(log⁡(1/ε))O(\log(1/\varepsilon))O(log(1/ε)) Clifford and T gates suffice, matching the lower bound up to a constant factor.
  • Ancilla-free optimal synthesis followed shortly after (Selinger 2012, arXiv:1212.6253; Ross–Selinger 2014, arXiv:1403.2975), using number-theoretic rounding in Z[i,1/2]\mathbb Z[i,1/\sqrt2]Z[i,1/2​] directly.

Setting

A register of nnn qubits has computational basis {∣z⟩:z∈{0,1}n}\{|z\rangle : z \in \{0,1\}^n\}{∣z⟩:z∈{0,1}n}. The circuits of this mission act on three wires: the data qubit (wire 0) and two ancillas (wires 1 and 2), which start in ∣0⟩|0\rangle∣0⟩. A circuit is a finite list of gates, each being HHH or TTT on one wire or CNOT on an ordered pair of distinct wires; it is applied in list order, and its size #C\#C#C is the number of gates.

The quality of a circuit CCC as an implementation of a one-qubit unitary UUU is measured on the input–output map with the ancillas initialized: compare the linear maps from one qubit to three qubits

C:ψ↦C(ψ⊗∣00⟩),U:ψ↦(Uψ)⊗∣00⟩,\mathcal C : \psi \mapsto C(\psi\otimes|00\rangle), \qquad \mathcal U : \psi \mapsto (U\psi)\otimes|00\rangle ,C:ψ↦C(ψ⊗∣00⟩),U:ψ↦(Uψ)⊗∣00⟩,

by the Frobenius norm ∥C−U∥F\|\mathcal C - \mathcal U\|_F∥C−U∥F​. This is sensitive to the global phase of UUU, and it charges any amplitude the circuit leaves on the ancillas.

The paper's central gate is the phase gate Λ(eiφ)=diag(1,eiφ)\Lambda(e^{i\varphi}) = \mathrm{diag}(1, e^{i\varphi})Λ(eiφ)=diag(1,eiφ). For k∈Nk\in\mathbb Nk∈N it uses the roundings ⌊2kcos⁡φ⌋\lfloor 2^k\cos\varphi\rfloor⌊2kcosφ⌋, ⌊2ksin⁡φ⌋\lfloor 2^k\sin\varphi\rfloor⌊2ksinφ⌋, the Gaussian rational

γ=⌊2kcos⁡φ⌋+i⌊2ksin⁡φ⌋2k,\gamma = \frac{\lfloor 2^k\cos\varphi\rfloor + i\lfloor 2^k\sin\varphi\rfloor}{2^k},γ=2k⌊2kcosφ⌋+i⌊2ksinφ⌋​,

and the two-qubit vector ∣v⟩=12k(⌊2kcos⁡φ⌋+i⌊2ksin⁡φ⌋,0,a+ib,c+id)=γ∣00⟩+∣1⟩⊗∣g⟩|v\rangle = \frac{1}{2^k}(\lfloor 2^k\cos\varphi\rfloor + i\lfloor 2^k\sin\varphi\rfloor, 0, a+ib, c+id) = \gamma|00\rangle + |1\rangle\otimes|g\rangle∣v⟩=2k1​(⌊2kcosφ⌋+i⌊2ksinφ⌋,0,a+ib,c+id)=γ∣00⟩+∣1⟩⊗∣g⟩, where the integers a,b,c,da,b,c,da,b,c,d solve a2+b2+c2+d2=4k−⌊2kcos⁡φ⌋2−⌊2ksin⁡φ⌋2a^2+b^2+c^2+d^2 = 4^k - \lfloor 2^k\cos\varphi\rfloor^2 - \lfloor 2^k\sin\varphi\rfloor^2a2+b2+c2+d2=4k−⌊2kcosφ⌋2−⌊2ksinφ⌋2.

Formalization targets

Goal: every single-qubit unitary with O(log⁡(1/ε))O(\log(1/\varepsilon))O(log(1/ε)) gates and two ancillas

∃A>0  ∀U∈U(2)  ∀ε∈(0,1]  ∃C:∥C−U∥F≤ε  and  #C≤A(log⁡21ε+1).\exists A>0\ \ \forall U\in U(2)\ \ \forall \varepsilon\in(0,1]\ \ \exists C:\quad \|\mathcal C - \mathcal U\|_F \le \varepsilon \ \text{ and }\ \#C \le A\Big(\log_2\tfrac1\varepsilon + 1\Big).∃A>0  ∀U∈U(2)  ∀ε∈(0,1]  ∃C:∥C−U∥F​≤ε  and  #C≤A(log2​ε1​+1).

The constant AAA is absolute. The goal asserts only the shape of the bound, so a sharper constant does not invalidate it.

Milestones

  1. Every U∈U(2)U\in U(2)U∈U(2) is a fixed-length product of HHH and phase gates Λ(eiθ)\Lambda(e^{i\theta})Λ(eiθ) (§2, p. 2).
  2. Λ(eiφ)=TmΛ(eiφ′)\Lambda(e^{i\varphi}) = T^m\Lambda(e^{i\varphi'})Λ(eiφ)=TmΛ(eiφ′) with m<8m<8m<8 and 0≤φ′≤π/40\le\varphi'\le\pi/40≤φ′≤π/4 (§2.1, p. 3).
  3. For 0≤φ≤π/40\le\varphi\le\pi/40≤φ≤π/4 the four-square equation is solvable and every solution makes ∣v⟩|v\rangle∣v⟩ a unit vector (§2.1, p. 3).
  4. ∣γ−eiφ∣≤2/2k|\gamma - e^{i\varphi}| \le \sqrt2/2^k∣γ−eiφ∣≤2​/2k (§2.2, p. 3).
  5. ∥∣g⟩∥2=1−∣γ∣2≤22/2k\||g\rangle\|^2 = 1-|\gamma|^2 \le 2\sqrt2/2^k∥∣g⟩∥2=1−∣γ∣2≤22​/2k (§2.2, p. 3).
  6. Any controlled preparation of ∣v⟩|v\rangle∣v⟩ is within 2/4k+22/2k\sqrt{2/4^k + 2\sqrt2/2^k}2/4k+22​/2k​ of Λ(eiφ)⊗∣00⟩\Lambda(e^{i\varphi})\otimes|00\rangleΛ(eiφ)⊗∣00⟩ (§2.2, p. 3).
  7. ∣v⟩|v\rangle∣v⟩ is prepared, controlled on the data qubit, by O(k)O(k)O(k) gates with no further ancilla (§2.2, p. 3; §2.3, p. 4).
  8. Λ(eiφ)\Lambda(e^{i\varphi})Λ(eiφ) is approximated within 2/4k+22/2k\sqrt{2/4^k + 2\sqrt2/2^k}2/4k+22​/2k​ by O(k)O(k)O(k) gates (§2.2, p. 3).
  9. Errors add when approximating circuits are composed (§2, p. 2).

Significance

The result. The theorem shows that the logarithmic lower bound on the gate count can be attained constructively with the Clifford and T library, at the price of two clean ancillas and with a classical compilation cost dominated by solving one four-square equation. Before it, the best constructive count for this library was the polylogarithmic one of Solovay–Kitaev. The construction also separates the problem into a number-theoretic rounding step and an exact-synthesis step, which is the structure later ancilla-free algorithms refine.

Formalizing it. The result is proved on paper but, to our knowledge, no part of it is machine-checked. A complete development formalizes: the reduction of single-qubit unitaries to phase gates; the rounding and four-square estimates; the controlled exact synthesis of a two-qubit state over Z[i]/2k\mathbb Z[i]/2^kZ[i]/2k with linear gate count; and the error bookkeeping on initialized maps. The nnn-qubit generalization from Kliuchnikov's later paper (arXiv:1306.3200) is posed on the platform as an open goal (QAlgorithms.Papers.Independent.Renew46.P12.approximateSynthesis), using the same error measure; this mission is its single-qubit, exactly-two-ancilla case, with its own proof route.

Difficulty

The estimates of §2.1–§2.2 are elementary. The weight sits in milestone 7, which the paper cites rather than proves: a two-qubit unit vector with entries in Z[i]/2k\mathbb Z[i]/2^kZ[i]/2k must be prepared from ∣00⟩|00\rangle∣00⟩ by O(k)O(k)O(k) gates (the Giles–Selinger column lemma, a reduction by two-level unitaries of types iXiXiX, T−m(iH)TmT^{-m}(iH)T^mT−m(iH)Tm and WWW), and the resulting circuit must be made controlled on the data qubit without introducing a third ancilla. The naive route, controlling each gate of a generic exact-synthesis circuit, ordinarily consumes an extra ancilla (the paper itself notes that a straightforward count gives three), and ancilla-free exact synthesis is not available for arbitrary operators: circuits over {H,T,CNOT}\{H,T,\mathrm{CNOT}\}{H,T,CNOT} on three qubits realize only a restricted set of determinants. Keeping the gate count linear in kkk through both steps requires the count of two-level operators to be linear in the denominator exponent, which is the substance of the column lemma.

Formalization scope

  • Registers are Qubits n = Fin n → Bool; wire 0 is the data qubit and wires 1, 2 are the ancillas, appended after the data wire.
  • The gate set is the published {H,T,CNOT}\{H, T, \mathrm{CNOT}\}{H,T,CNOT} (htcxGateSet); S=T2S = T^2S=T2 and X=HT4HX = HT^4HX=HT4H, so gate counts against the full Clifford and T library differ by a constant factor. Circuits and their unitaries are the published Circuit, Circuit.unitary, Circuit.size.
  • The error is frobNorm (initializedMap c.unitary - idealMap U 2): the Frobenius norm of the rectangular map above. It dominates the per-state distance of §2.2 and the paper's "larger system" remark.
  • Every O(⋅)O(\cdot)O(⋅) of the page is pinned: 22/2k2\sqrt2/2^k22​/2k for 1−∣γ∣21-|\gamma|^21−∣γ∣2, 2/4k+22/2k\sqrt{2/4^k + 2\sqrt2/2^k}2/4k+22​/2k​ for the distance, A(k+1)A(k+1)A(k+1) and A(log⁡2(1/ε)+1)A(\log_2(1/\varepsilon)+1)A(log2​(1/ε)+1) for gate counts, with AAA quantified before every other variable. The printed bound 2/2k\sqrt2/2^k2​/2k is kept as is.
  • "Up to two ancillary qubits" is formalized as exactly two ancilla wires; an unused one stays idle. The ancillas need not be returned clean, since leakage is charged by the error.
  • The hypothesis 0≤φ≤π/40\le\varphi\le\pi/40≤φ≤π/4 of §2.1 is kept wherever the page uses it; milestone 2 removes it.
  • The page prints the transformed state as α∣000⟩+βγ∣100⟩+β∣01⟩⊗∣g⟩\alpha|000\rangle + \beta\gamma|100\rangle + \beta|01\rangle\otimes|g\rangleα∣000⟩+βγ∣100⟩+β∣01⟩⊗∣g⟩; by its own definition of ∣v⟩|v\rangle∣v⟩ the last term is β∣11⟩⊗∣g⟩\beta|11\rangle\otimes|g\rangleβ∣11⟩⊗∣g⟩, and the formalization uses the latter.

Trivializing readings are excluded: dropping the ancillas makes the goal false (with no ancillas and a phase-sensitive error, unitaries whose determinant is not a power of eiπ/4e^{i\pi/4}eiπ/4 cannot be approximated), quotienting by the global phase or allowing arbitrary one-qubit gates would make it a different and weaker statement, and a constant AAA depending on UUU or ε\varepsilonε would make it vacuous.

Not formalized here: Lemma 1 (the Ω(log⁡(1/ε))\Omega(\log(1/\varepsilon))Ω(log(1/ε)) lower bound with ancillas, p. 4), the average classical runtime O(log⁡2(1/ε)log⁡log⁡(1/ε))O(\log^2(1/\varepsilon)\log\log(1/\varepsilon))O(log2(1/ε)loglog(1/ε)) of the randomized four-square solver, and the auxiliary bound 4k−⌊2kcos⁡φ⌋2−⌊2ksin⁡φ⌋2≤4⋅2k+Const4^k - \lfloor 2^k\cos\varphi\rfloor^2 - \lfloor 2^k\sin\varphi\rfloor^2 \le 4\cdot2^k + \mathrm{Const}4k−⌊2kcosφ⌋2−⌊2ksinφ⌋2≤4⋅2k+Const that serves only that runtime.

Reusable beyond this mission: the controlled exact-preparation lemma (milestone 7) and the composition lemma for initialized maps (milestone 9) apply to any ancilla-based synthesis result. Proofs of individual milestones, Mathlib-style lemmas on embedOp and circuit unitarity, and a formal treatment of two-level unitaries over Z[i,1/2]\mathbb Z[i,1/\sqrt2]Z[i,1/2​] are all welcome.

Selected references

  • V. Kliuchnikov, D. Maslov, M. Mosca, Asymptotically optimal approximation of single qubit unitaries by Clifford and T circuits using a constant number of ancillary qubits, arXiv:1212.0822v2, 2012 (Phys. Rev. Lett. 110, 190502, 2013). http://arxiv.org/abs/1212.0822
  • B. Giles, P. Selinger, Exact synthesis of multiqubit Clifford+T circuits, Phys. Rev. A 87, 032332, 2013. http://arxiv.org/abs/1212.0506
  • V. Kliuchnikov, D. Maslov, M. Mosca, Fast and efficient exact synthesis of single qubit unitaries generated by Clifford and T gates, Quantum Inf. Comput. 13, 2013. http://arxiv.org/abs/1206.5236
  • M. Amy, D. Maslov, M. Mosca, M. Roetteler, A meet-in-the-middle algorithm for fast synthesis of depth-optimal quantum circuits, IEEE Trans. CAD 32, 2013. http://arxiv.org/abs/1206.0758
  • C. M. Dawson, M. A. Nielsen, The Solovay–Kitaev algorithm, Quantum Inf. Comput. 6, 2006. http://arxiv.org/abs/quant-ph/0505030
  • A. W. Harrow, B. Recht, I. L. Chuang, Efficient discrete approximations of quantum gates, J. Math. Phys. 43, 2002. http://arxiv.org/abs/quant-ph/0111031
  • A. Y. Kitaev, A. H. Shen, M. N. Vyalyi, Classical and Quantum Computation, Graduate Studies in Mathematics 47, AMS, 2002.
  • M. O. Rabin, J. O. Shallit, Randomized algorithms in number theory, Comm. Pure Appl. Math. 39, 1986.
  • V. Kliuchnikov, Synthesis of unitaries with Clifford+T circuits, 2013. http://arxiv.org/abs/1306.3200
  • P. Selinger, Efficient Clifford+T approximation of single-qubit operators, 2012. http://arxiv.org/abs/1212.6253
  • N. J. Ross, P. Selinger, Optimal ancilla-free Clifford+T approximation of z-rotations, 2014. http://arxiv.org/abs/1403.2975
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Control TheoryMathematical PhysicsQuantum Information·Captain: mikedeng1

Stabilizing qubit coherence via tracking-control: Under Pure Dephasing, Coherence Can Be Held Constant Exactly Until t_b = v_z(0)²/(2γc), Where the Control Fields DivergeResearch Paper

Motivation

A qubit coupled to an environment loses the phase relation between its basis states ∣0⟩|0\rangle∣0⟩ and ∣1⟩|1\rangle∣1⟩: the off-diagonal entries of its density matrix decay. This decoherence is the main obstacle to storing quantum information, and a large body of work tries to counter it with external control fields. Lidar and Schneider (arXiv:quant-ph/0410048, Quantum Information and Computation 2005) ask a sharp question in the simplest nontrivial setting: if the controller may observe the state and choose the Hamiltonian at every instant (tracking control), can it keep the coherence of a dephasing qubit exactly constant, and for how long?

Their answer, stated in the abstract, is that "it is possible to maintain coherence for finite time durations, until the control field diverges." It was known that Hamiltonian control cannot hold the purity Tr⁡ρ2\operatorname{Tr}\rho^2Trρ2 of a Markovian open system at its initial value (Ketterle and Pritchard, Phys. Rev. A 46, 4051 (1992), and Tannor and Bartana, J. Phys. Chem. A 103, 10359 (1999), refs. [25, 26] of the paper), and the paper's §II.A shows that under a unital Lindbladian the purity decreases whatever the Hamiltonian; the present result locates exactly how much of the coherence, as opposed to the purity, control can protect.

Setting

A qubit state is a complex 2×22\times22×2 matrix ρ\rhoρ with Tr⁡ρ=1\operatorname{Tr}\rho=1Trρ=1, ρ10=ρ01∗\rho_{10}=\rho_{01}^*ρ10​=ρ01∗​ and Tr⁡(ρ2)≤1\operatorname{Tr}(\rho^2)\le1Tr(ρ2)≤1. With the Pauli matrices σx,σy,σz\sigma_x,\sigma_y,\sigma_zσx​,σy​,σz​, its Bloch vector is v⃗=(vx,vy,vz)\vec v=(v_x,v_y,v_z)v=(vx​,vy​,vz​), vα=Tr⁡(ρσα)v_\alpha=\operatorname{Tr}(\rho\sigma_\alpha)vα​=Tr(ρσα​), so that ρ=12(I+v⃗⋅σ⃗)\rho=\tfrac12(I+\vec v\cdot\vec\sigma)ρ=21​(I+v⋅σ) (eq. (9)). The coherence is the squared radius of v⃗\vec vv in the xxx–yyy plane,

c=vx2+vy2=4∣ρ01∣2(eq. (11)).c=v_x^2+v_y^2=4|\rho_{01}|^2 \quad\text{(eq. (11))}.c=vx2​+vy2​=4∣ρ01​∣2(eq. (11)).

The controller applies the Hamiltonian H(t)=ℏ2(ω0(t)σz+ω1(t)σx−ω2(t)σy)H(t)=\tfrac{\hbar}{2}\bigl(\omega_0(t)\sigma_z+\omega_1(t)\sigma_x-\omega_2(t)\sigma_y\bigr)H(t)=2ℏ​(ω0​(t)σz​+ω1​(t)σx​−ω2​(t)σy​) (eq. (13)) with three real fields ω0,ω1,ω2\omega_0,\omega_1,\omega_2ω0​,ω1​,ω2​, and the qubit undergoes pure dephasing at rate γ>0\gamma>0γ>0:

∂ρ∂t=−iℏ[H,ρ]+γ2(σzρσz−ρ)(eq. (32)).\frac{\partial\rho}{\partial t}=-\frac{i}{\hbar}[H,\rho]+\frac{\gamma}{2}(\sigma_z\rho\sigma_z-\rho)\quad\text{(eq. (32))}.∂t∂ρ​=−ℏi​[H,ρ]+2γ​(σz​ρσz​−ρ)(eq. (32)).

Equivalently the Bloch vector obeys v⃗˙=M(t)v⃗\dot{\vec v}=M(t)\vec vv˙=M(t)v with

M(t)=(−γ−ω0−ω2ω0−γ−ω1ω2ω10)(eq. (30)).M(t)=\begin{pmatrix}-\gamma&-\omega_0&-\omega_2\\ \omega_0&-\gamma&-\omega_1\\ \omega_2&\omega_1&0\end{pmatrix}\quad\text{(eq. (30))}.M(t)=​−γω0​ω2​​−ω0​−γω1​​−ω2​−ω1​0​​(eq. (30)).

Without control the coherence decays as e−2γtce^{-2\gamma t}ce−2γtc. The breakdown time of an initial state with coherence c>0c>0c>0 is

tb=vz(0)22γc(eq. (38)).t_b=\frac{v_z(0)^2}{2\gamma c}\quad\text{(eq. (38))}.tb​=2γcvz​(0)2​(eq. (38)).

The tracking fields are, with s=sign⁡vz(0)s=\operatorname{sign}v_z(0)s=signvz​(0), an arbitrary ω0\omega_0ω0​, and R(t)=vz(0)2−2γctR(t)=v_z(0)^2-2\gamma ctR(t)=vz​(0)2−2γct,

ω2(t)=s −γvx(0)−ω0(t)vy(0)R(t),ω1(t)=s −γvy(0)+ω0(t)vx(0)R(t)(eqs. (41)–(42)),\omega_2(t)=s\,\frac{-\gamma v_x(0)-\omega_0(t)v_y(0)}{\sqrt{R(t)}},\qquad \omega_1(t)=s\,\frac{-\gamma v_y(0)+\omega_0(t)v_x(0)}{\sqrt{R(t)}}\quad\text{(eqs. (41)–(42))},ω2​(t)=sR(t)​−γvx​(0)−ω0​(t)vy​(0)​,ω1​(t)=sR(t)​−γvy​(0)+ω0​(t)vx​(0)​(eqs. (41)–(42)),

and the tracked state is 12(I+v⃗(t)⋅σ⃗)\tfrac12(I+\vec v(t)\cdot\vec\sigma)21​(I+v(t)⋅σ) with v⃗(t)=(vx(0),vy(0),sR(t))\vec v(t)=(v_x(0),v_y(0),s\sqrt{R(t)})v(t)=(vx​(0),vy​(0),sR(t)​).

Formalization targets

Goal: coherence can be held exactly on [0,tb)[0,t_b)[0,tb​), and no longer

For ℏ>0\hbar>0ℏ>0, γ>0\gamma>0γ>0 and a qubit state ρ0\rho_0ρ0​ with coherence c>0c>0c>0:

  1. No-go. For all controls and every solution ρ(t)\rho(t)ρ(t) of (32) on [0,T)[0,T)[0,T) with ρ(0)=ρ0\rho(0)=\rho_0ρ(0)=ρ0​ and constant coherence ccc,
vz(t)2=vz(0)2−2γc t(t∈[0,T)),T≤tb.v_z(t)^2=v_z(0)^2-2\gamma c\,t\quad(t\in[0,T)),\qquad T\le t_b .vz​(t)2=vz​(0)2−2γct(t∈[0,T)),T≤tb​.
  1. Achievability. If vz(0)≠0v_z(0)\ne0vz​(0)=0, then for every ω0\omega_0ω0​ the tracked state starts at ρ0\rho_0ρ0​, is a qubit state, keeps vx,vyv_x,v_yvx​,vy​ fixed, and solves (32) at every t∈[0,tb)t\in[0,t_b)t∈[0,tb​) with the tracking fields.
  2. Divergence. If vz(0)≠0v_z(0)\ne0vz​(0)=0, then ω1(t)2+ω2(t)2→+∞\omega_1(t)^2+\omega_2(t)^2\to+\inftyω1​(t)2+ω2​(t)2→+∞ as t→tb−t\to t_b^-t→tb−​, whatever ω0\omega_0ω0​ is.

Milestones

The milestones follow the paper's derivation: the Bloch parametrization (§II.B, p. 3); the equivalence of (32) and (30) (§III.B, p. 5); eq. (36), v˙z=−γc/vz\dot v_z=-\gamma c/v_zv˙z​=−γc/vz​ under constant coherence (p. 6); eqs. (37)–(38), vz(t)=(±)vz(0)2−2γctv_z(t)=(\pm)\sqrt{v_z(0)^2-2\gamma ct}vz​(t)=(±)vz​(0)2−2γct​ and T≤tbT\le t_bT≤tb​ (p. 6); eqs. (41)–(42), the tracking fields solve (30) and are forced once vx,vyv_x,v_yvx​,vy​ are frozen (p. 6); and the field-strength identity of §III.C (p. 8),

ω1(t)2+ω2(t)2=(γ2+ω0(t)2) cvz(0)2−2γct.\omega_1(t)^2+\omega_2(t)^2=\frac{(\gamma^2+\omega_0(t)^2)\,c}{v_z(0)^2-2\gamma ct}.ω1​(t)2+ω2​(t)2=vz​(0)2−2γct(γ2+ω0​(t)2)c​.

Significance

The result gives an exact, state-dependent budget for coherence protection under dephasing. The time tbt_btb​ is inversely proportional to the coherence to be maintained and proportional to vz(0)2=p(0)−cv_z(0)^2=p(0)-cvz​(0)2=p(0)−c, where p=∣v⃗∣2p=|\vec v|^2p=∣v∣2 is the purity: the more coherent the initial state, the shorter the protection, and a state of maximal coherence for its purity (vz(0)=0v_z(0)=0vz​(0)=0) cannot be protected at all. The no-go part holds for every control law, so it bounds any tracking strategy, not only the linearized one the paper constructs. The divergence of the fields is the physical cost: protection up to tbt_btb​ requires unbounded control amplitude, which any bounded actuator cuts short.

The paper proves these statements by direct calculation. As far as is known, none of them has a machine-checked proof. The mission turns a physics derivation, in which "the solution is" and "does not stay real" carry the logical weight, into precise statements about solutions of an ODE on a half-open interval, with the sign choice, the degenerate case vz(0)=0v_z(0)=0vz​(0)=0 and the domain of the square roots made explicit.

Difficulty

The calculations are elementary, but the no-go statement quantifies over arbitrary, possibly discontinuous control fields and arbitrary solutions of the matrix equation. Nothing is assumed about the controls beyond being real functions of time, nothing about the solution beyond continuity on [0,T)[0,T)[0,T) and the equation on (0,T)(0,T)(0,T), and the conclusion constrains only the zzz-component while the hypothesis constrains only the xxx–yyy components. The tempting shortcut, assuming that vxv_xvx​ and vyv_yvy​ are frozen as in the paper's explicit construction, proves a strictly weaker statement and is not the goal. On the achievability side, the square root is not differentiable where its argument vanishes, so differentiability has to be established on [0,tb)[0,t_b)[0,tb​), including the endpoint t=0t=0t=0, and the sign sign⁡vz(0)\operatorname{sign}v_z(0)signvz​(0) has to be carried through the derivative.

Formalization scope

Operators are Matrix (Fin 2) (Fin 2) ℂ in the basis ∣0⟩,∣1⟩|0\rangle,|1\rangle∣0⟩,∣1⟩; the Pauli matrices are the published MIPRE.LCS.Pauli.X/Y/Z. Bloch vectors and controls are Fin 3 → ℝ: Bloch components in the order x,y,zx,y,zx,y,z, control components in the order ω0,ω1,ω2\omega_0,\omega_1,\omega_2ω0​,ω1​,ω2​ (with ω0\omega_0ω0​ multiplying σz\sigma_zσz​, as in (13)). The Bloch vector is vα=Re⁡Tr⁡(ρσα)v_\alpha=\operatorname{Re}\operatorname{Tr}(\rho\sigma_\alpha)vα​=ReTr(ρσα​), following eq. (9); eq. (8) prints an extra factor 12\tfrac1221​, which contradicts (9) and is treated as a misprint. A trajectory solves (32) or (30) on [0,T)[0,T)[0,T) if it is continuous on [0,T)[0,T)[0,T) and has the prescribed derivative at every t∈(0,T)t\in(0,T)t∈(0,T). Controls are arbitrary functions R→R\mathbb R\to\mathbb RR→R. The hypotheses γ>0\gamma>0γ>0 and c>0c>0c>0 are added, because tbt_btb​ divides by 2γc2\gamma c2γc; ℏ>0\hbar>0ℏ>0 is a parameter. The sign (±)(\pm)(±) of (37), (41), (42) is sign⁡vz(0)\operatorname{sign}v_z(0)signvz​(0).

Statements about tbt_btb​, the tracked state and the fields are restricted to [0,tb)[0,t_b)[0,tb​), because Lean's square root and division are total (x=0\sqrt{x}=0x​=0 for x<0x<0x<0, x/0=0x/0=0x/0=0); a statement that only asserts that the closed-form curve solves the ODE would be the achievability half alone, and the goal requires the no-go half over all controls as well.

A complete development needs the Bloch dictionary for 2×22\times22×2 matrices, the passage from (32) to (30), and one-variable real analysis on half-open intervals. The Bloch dictionary and the reduction of a Lindblad equation to Bloch form are reusable for other qubit control problems. Proofs of any milestone, and sorry-free lemmas on the Pauli algebra, are welcome.

Selected references

  • D. A. Lidar and S. Schneider, Stabilizing qubit coherence via tracking-control, Quantum Information and Computation (2005); arXiv:quant-ph/0410048v1, 2004. https://arxiv.org/abs/quant-ph/0410048
  • W. Ketterle and D. E. Pritchard, Atom cooling by time-dependent potentials, Physical Review A 46, 4051 (1992). https://doi.org/10.1103/PhysRevA.46.4051
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AlgebraCombinatoricsRepresentation Theory·Captain: mikedeng1

Supersymmetric Polynomials and the Center of the Walled Brauer Algebra: When B_{r,s}(δ) Is Semisimple, Supersymmetric Polynomials in the Jucys–Murphy Elements Generate Its CenterResearch Paper

Motivation

The walled Brauer algebra Br,s(δ)B_{r,s}(\delta)Br,s​(δ) is the centralizer algebra of mixed Schur–Weyl duality: for δ=n\delta=nδ=n it acts on the mixed tensor space V⊗r⊗(V∗)⊗sV^{\otimes r}\otimes (V^*)^{\otimes s}V⊗r⊗(V∗)⊗s of V=CnV=\mathbb C^nV=Cn and commutes with gln\mathfrak{gl}_ngln​, and for δ=m−n\delta=m-nδ=m−n it plays the same role for the general linear supergroup GL(m∣n)GL(m|n)GL(m∣n). Its representation theory has been studied through cellular structures and blocks (Cox–De Visscher–Doty–Martin 2008), Khovanov arc algebras (Brundan–Stroppel 2012) and cyclotomic quotients (Sartori–Stroppel 2015).

For the group algebra CSn\mathbb C\mathfrak S_nCSn​ of the symmetric group there is a classical description of the center: it consists of the symmetric polynomials in the Jucys–Murphy elements Lk=∑j<k(j,k)L_k=\sum_{j<k}(j,k)Lk​=∑j<k​(j,k) (Jucys 1974, Murphy 1983). Jung and Kim (arXiv:1508.06469v2) prove the walled analogue: when Br,s(δ)B_{r,s}(\delta)Br,s​(δ) is semisimple, its center is generated by the supersymmetric polynomials in its Jucys–Murphy elements. This mission formalizes that theorem and the chain of results leading to it.

Timeline. Jucys (1974) and Murphy (1981, 1983) describe the center of CSn\mathbb C\mathfrak S_nCSn​ through Jucys–Murphy elements. Stembridge (1985) characterizes supersymmetric polynomials and shows that the power sums generate them. Cox, De Visscher, Doty and Martin (2008) give the cellular structure of Br,s(δ)B_{r,s}(\delta)Br,s​(δ), its blocks in characteristic zero and a semisimplicity criterion. Brundan and Stroppel (2012) prove that the central element zr,sz_{r,s}zr,s​ (essentially L1+⋯+Lr+sL_1+\dots+L_{r+s}L1​+⋯+Lr+s​) acts on cell modules by a content sum. Jung and Kim (2015, revised 2017) prove the generation theorem for all supersymmetric polynomials.

Setting

Fix integers r,s≥0r,s\ge0r,s≥0 and δ∈C\delta\in\mathbb Cδ∈C. An (r,s)(r,s)(r,s)-walled Brauer diagram is a pairing of 2(r+s)2(r+s)2(r+s) vertices, r+sr+sr+s on top and r+sr+sr+s on the bottom, with a wall between positions rrr and r+1r+1r+1, such that vertical edges do not cross the wall and horizontal edges do. Br,s(δ)B_{r,s}(\delta)Br,s​(δ) is the complex vector space with these diagrams as basis; two diagrams are multiplied by stacking them and replacing each closed loop by a factor δ\deltaδ.

For vertices a≠ba\ne ba=b on the same side of the wall, (a,b)(a,b)(a,b) is the diagram of the transposition of aaa and bbb. For 1≤j≤r<k≤r+s1\le j\le r<k\le r+s1≤j≤r<k≤r+s, ej,ke_{j,k}ej,k​ is the diagram with a top arc and a bottom arc joining jjj and kkk and all other vertices joined straight down. The Jucys–Murphy elements (Definition 2.1) are

Lk=∑j=1k−1(j,k)(1≤k≤r),Lk=−∑j=1rej,k+∑j=r+1k−1(j,k)+δ(r<k≤r+s).L_k=\sum_{j=1}^{k-1}(j,k)\quad(1\le k\le r),\qquad L_k=-\sum_{j=1}^{r}e_{j,k}+\sum_{j=r+1}^{k-1}(j,k)+\delta\quad(r<k\le r+s).Lk​=j=1∑k−1​(j,k)(1≤k≤r),Lk​=−j=1∑r​ej,k​+j=r+1∑k−1​(j,k)+δ(r<k≤r+s).

A polynomial p∈C[x1,…,xr,y1,…,ys]p\in\mathbb C[x_1,\dots,x_r,y_1,\dots,y_s]p∈C[x1​,…,xr​,y1​,…,ys​] is supersymmetric (Definition 2.8) if it is symmetric in the xix_ixi​ and in the yjy_jyj​ separately, and the substitution xr=−y1=tx_r=-y_1=txr​=−y1​=t produces a polynomial independent of ttt. Examples are the power sums pk=∑ixik+(−1)k+1∑jyjkp_k=\sum_i x_i^k+(-1)^{k+1}\sum_j y_j^kpk​=∑i​xik​+(−1)k+1∑j​yjk​. Write Sr,s[x;y]S_{r,s}[x;y]Sr,s​[x;y] for the supersymmetric polynomials and p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) for the substitution xi↦Lix_i\mapsto L_ixi​↦Li​, yj↦Lr+jy_j\mapsto L_{r+j}yj​↦Lr+j​.

The cell modules Cr,s(λ)C_{r,s}(\lambda)Cr,s​(λ) are indexed by bipartitions λ=(λL,λR)\lambda=(\lambda^L,\lambda^R)λ=(λL,λR) with ∣λL∣=r−t|\lambda^L|=r-t∣λL∣=r−t, ∣λR∣=s−t|\lambda^R|=s-t∣λR∣=s−t, 0≤t≤min⁡(r,s)0\le t\le\min(r,s)0≤t≤min(r,s); this set is Λr,s\Lambda_{r,s}Λr,s​. The set Λ˙r,s\dot\Lambda_{r,s}Λ˙r,s​ equals Λr,s\Lambda_{r,s}Λr,s​ except when δ=0\delta=0δ=0 and r=s≠0r=s\ne0r=s=0, where (∅,∅)(\varnothing,\varnothing)(∅,∅) is removed; it indexes the simple modules. The content vector c(λ,⋅)∈Cr+sc(\lambda,\cdot)\in\mathbb C^{r+s}c(λ,⋅)∈Cr+s lists the contents of λL\lambda^LλL, then 2t2t2t zeros, then the contents of λR\lambda^RλR shifted by δ\deltaδ.

Formalization targets

Goal: Theorem 3.5

Br,s(δ) semisimple ⟹ C[p(L1,…,Lr+s):p∈Sr,s[x;y]]=Z(Br,s(δ)).B_{r,s}(\delta)\ \text{semisimple}\ \Longrightarrow\ \mathbb C\bigl[p(L_1,\dots,L_{r+s}) : p\in S_{r,s}[x;y]\bigr]=Z\bigl(B_{r,s}(\delta)\bigr).Br,s​(δ) semisimple ⟹ C[p(L1​,…,Lr+s​):p∈Sr,s​[x;y]]=Z(Br,s​(δ)).

Both inclusions are asserted. The goal fixes no constants; the hypothesis holds for all but finitely many δ\deltaδ (Proposition 1.1).

Milestones

  1. Relations among generators: Lemma 2.3 and Proposition 2.4.
  2. The LkL_kLk​ commute (Proposition 2.6); the power sums pk(L1,…,Lr+s)p_k(L_1,\dots,L_{r+s})pk​(L1​,…,Lr+s​) are central (Proposition 2.7).
  3. Stembridge's theorem, Sr,s[x;y]=C[p0,p1,… ]S_{r,s}[x;y]=\mathbb C[p_0,p_1,\dots]Sr,s​[x;y]=C[p0​,p1​,…], and its consequence, Corollary 2.9: every p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) with ppp supersymmetric is central, for every δ\deltaδ.
  4. Separation: Lemma 2.11 (generating functions), the semisimplicity criterion Proposition 1.1, and Lemma 2.12 (supersymmetric polynomials separate the content vectors).
  5. Central characters: Lemma 3.2, Proposition 3.1 and Corollary 3.3, by which f(L1,…,Lr+s)f(L_1,\dots,L_{r+s})f(L1​,…,Lr+s​) acts on Cr,s(λ)C_{r,s}(\lambda)Cr,s​(λ) as f(c(λ,1),…,c(λ,r+s))f(c(\lambda,1),\dots,c(\lambda,r+s))f(c(λ,1),…,c(λ,r+s)).
  6. Counting: Lemma 3.4 (a nonsingular evaluation matrix) and dim⁡Z(Br,s(δ))=∣Λ˙r,s∣\dim Z(B_{r,s}(\delta))=|\dot\Lambda_{r,s}|dimZ(Br,s​(δ))=∣Λ˙r,s​∣ in the semisimple case.

Significance

The theorem gives an explicit generating set for the center of a semisimple walled Brauer algebra, parallel to the symmetric-group case. Its consequences in the paper include a description of the Gelfand–Zetlin subalgebra and formulas for primitive idempotents (§4), an alternative proof of the block classification of Cox et al. (§5), and, via the same method, the center of the quantized walled Brauer algebra (§6). Corollary 2.9 alone, valid for every δ\deltaδ, provides a supply of central elements whose action on each cell module is computed by Corollary 3.3.

The theorem is proved in the paper; no part of it is formalized. A formalization would supply machine-checked Jucys–Murphy relations for a diagram algebra built on a published, generic encoding of walled Brauer diagrams, a Lean development of supersymmetric polynomials (including Stembridge's theorem, absent from Mathlib), and a reusable dimension count for centers of semisimple algebras in terms of simple modules.

Difficulty

The inclusion of the supersymmetric polynomials in the center (Corollary 2.9) reduces to diagram relations plus Stembridge's theorem; the latter is a nontrivial statement about polynomial rings, with no counterpart in Mathlib. The reverse inclusion is the harder half. A central element is not visibly a polynomial in the LkL_kLk​: the argument must show that enough linearly independent central elements of the form p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) exist, which requires computing their scalars on every cell module (an explicit cellular computation involving the arc elements τt\tau_tτt​), separating all content vectors (where semisimplicity enters through the criterion of Cox et al.), and comparing with dim⁡Z\dim ZdimZ, which needs Wedderburn–Artin together with the classification of simple modules. Separation genuinely fails outside the semisimple range, so no argument independent of δ\deltaδ can work.

Formalization scope

The algebra, diagrams, cell modules Cr,s(λ)C_{r,s}(\lambda)Cr,s​(λ), the index sets Λr,s\Lambda_{r,s}Λr,s​ (CellIndex) and Λ˙r,s\dot\Lambda_{r,s}Λ˙r,s​ (Label) and contents are the published definitions WalledBrauer_Blocks_{Diagram, Algebra, ModuleTheory, Partitions, CellModules}, used as references. New definitions are in WalledBrauer.Center.Setting. Conventions:

  • The base field is C\mathbb CC; r,sr,sr,s are arbitrary natural numbers, including 000; δ∈C\delta\in\mathbb Cδ∈C is arbitrary.
  • Vertices are 0-based (Fin (r + s)); the paper's LkL_kLk​ is jm δ ⟨k-1, _⟩.
  • The published algebra multiplies diagrams with the left factor on top, the opposite of the paper's convention. One-sided relations are transcribed literally with the platform's product; each is the image of the paper's relation under the up–down flip, an anti-automorphism fixing every (a,b)(a,b)(a,b), ej,ke_{j,k}ej,k​, LkL_kLk​ and τt\tau_tτt​. The center, generated subalgebras, semisimplicity and central characters do not depend on the convention.
  • Polynomials are MvPolynomial (Fin r ⊕ Fin s) ℂ. The evaluation p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) is defined monomial by monomial in increasing vertex order, without assuming that the LkL_kLk​ commute; it is never routed through a commutative subalgebra.
  • The cancellation property is vacuous when r=0r=0r=0 or s=0s=0s=0. Semisimplicity is IsSemisimpleRing, the center is Subalgebra.center ℂ, "generate" is Algebra.adjoin ℂ. In Proposition 1.1, r+s−2r+s-2r+s−2 is real.
  • Lemma 2.11's equality of rational functions is stated cross-multiplied in C[z]\mathbb C[z]C[z].

Supersymmetry is defined intrinsically on polynomials, never through the algebra, so neither inclusion of the goal holds by definition; stating only ⊆\subseteq⊆ or only ⊇\supseteq⊇ as the goal is excluded.

Proofs of any milestone are welcome, as are reusable developments of supersymmetric polynomials (Stembridge's theorem, elementary supersymmetric polynomials) and of the center of a split semisimple algebra.

Selected references

  • J. H. Jung and M. Kim, Supersymmetric polynomials and the center of the walled Brauer algebra, arXiv:1508.06469v2, 2017. https://arxiv.org/abs/1508.06469
  • A. Cox, M. De Visscher, S. Doty and P. Martin, On the blocks of the walled Brauer algebra, J. Algebra 320 (2008), 169–212. https://arxiv.org/abs/0709.0851
  • J. Brundan and C. Stroppel, Gradings on walled Brauer algebras and Khovanov's arc algebra, Adv. Math. 231 (2012), 709–773. https://arxiv.org/abs/1107.0999
  • A. Sartori and C. Stroppel, Walled Brauer algebras as idempotent truncations of level 2 cyclotomic quotients, J. Algebra 440 (2015), 602–638. https://arxiv.org/abs/1411.2771
  • J. R. Stembridge, A characterization of supersymmetric polynomials, J. Algebra 95 (1985), 439–444. https://mathscinet.ams.org/mathscinet-getitem?mr=801279
  • Y. Li, Jucys–Murphy elements and centres of cellular algebras, Bull. Aust. Math. Soc. 85 (2012), 261–270. https://mathscinet.ams.org/mathscinet-getitem?mr=2891540
  • G. E. Murphy, The idempotents of the symmetric group and Nakayama's conjecture, J. Algebra 81 (1983), 258–265. https://mathscinet.ams.org/mathscinet-getitem?mr=696137
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