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Linear OptimizationOperations ResearchProbability+1·Captain: mikedeng1

Near-Optimal Bayesian Online Assortment of Reusable Resources: the hybrid simulation-based algorithm is (1 − min{1/2, ε*(c_min)})-competitive against the Bayesian expected LPResearch Paper

Motivation

Rental platforms, cloud computing, hotel and car-rental systems, and on-demand services all sell access to reusable resources: a unit that is rented comes back after a random rental duration and can be rented again. When such a platform displays a menu of products (an assortment) to each arriving customer, it faces an online decision problem: offering a product now earns a fee, but ties up a unit that a later, more valuable customer might have wanted. Feng, Niazadeh and Saberi study this problem in a Bayesian setting, where customer types are drawn from known distributions, and give an algorithm whose expected revenue is within a factor 1−min⁡{1/2,ε∗(cmin⁡)}1 - \min\{1/2, \varepsilon^*(c_{\min})\}1−min{1/2,ε∗(cmin​)} of an LP upper bound on any online policy (arXiv:2512.06997; Operations Research, 2024). The factor tends to 111 as the smallest inventory grows and never drops below 1/21/21/2.

Earlier work on online assortment of reusable resources (Gong, Goyal, Iyengar, Simchi-Levi, Udwani and Wang, Management Science 2021; Goyal, Iyengar and Udwani, arXiv:2002.02430) studied the prior-free, adversarial setting, in which fees and rental-duration distributions are type-independent and identical across time. The Bayesian model here lets both depend on the customer type.

Setting

There are nnn products; product iii has ci≥1c_i \ge 1ci​≥1 identical units, and cmin⁡=min⁡icic_{\min} = \min_i c_icmin​=mini​ci​. Customers arrive at times t=1,…,Tt = 1, \dots, Tt=1,…,T. Customer ttt has a type ztz_tzt​, drawn independently from a known distribution FtF_tFt​ on a finite set. A type zzz fixes

  • a choice model ϕz(S,i)\phi^z(S, i)ϕz(S,i): the probability that a customer of type zzz rents product iii when offered the assortment SSS (with probability 1−∑i∈Sϕz(S,i)1 - \sum_{i \in S}\phi^z(S,i)1−∑i∈S​ϕz(S,i) she rents nothing);
  • fees riz≥0r^z_i \ge 0riz​≥0;
  • rental-duration distributions gizg^z_igiz​ on {1,…,T}\{1, \dots, T\}{1,…,T}; write Gˉiz(k)=Pr⁡[d>k]\bar G^z_i(k) = \Pr[d > k]Gˉiz​(k)=Pr[d>k].

Assortments come from a family S\mathcal SS that is downward closed (Assumption 2), and choice models are weakly substitutable (Assumption 1): ϕz(∅,i)=0\phi^z(\emptyset, i) = 0ϕz(∅,i)=0, and adding a product to an assortment never increases the choice probability of another. A rented unit with duration ddd is unavailable at times t,…,t+d−1t, \dots, t+d-1t,…,t+d−1; a product with no unit on hand cannot be offered.

The benchmark is the Bayesian expected LP Expected-LP[{Ft}][\{F_t\}][{Ft​}]: with yS,t,zy_{S,t,z}yS,t,z​ the probability of offering SSS to type zzz at time ttt, maximize ∑t,z,S,iFt(z) riz ϕz(S,i) yS,t,z\sum_{t,z,S,i} F_t(z)\, r^z_i\, \phi^z(S,i)\, y_{S,t,z}∑t,z,S,i​Ft​(z)riz​ϕz(S,i)yS,t,z​ subject to each product's inventory holding in expectation at every time, ∑τ≤t∑z,SFτ(z) Gˉiz(t−τ) ϕz(S,i) yS,τ,z≤ci\sum_{\tau \le t}\sum_{z,S} F_\tau(z)\, \bar G^z_i(t-\tau)\, \phi^z(S,i)\, y_{S,\tau,z} \le c_i∑τ≤t​∑z,S​Fτ​(z)Gˉiz​(t−τ)ϕz(S,i)yS,τ,z​≤ci​, and ∑SyS,t,z≤1\sum_S y_{S,t,z} \le 1∑S​yS,t,z​≤1. Let y∗y^*y∗ be an optimal solution with ∑SyS,t,z∗=1\sum_S y^*_{S,t,z} = 1∑S​yS,t,z∗​=1, and

ε∗(x)=min⁡γ∈[0,1] 1−(1−γ)(1−e−γ2x/(2−γ)).\varepsilon^*(x) = \min_{\gamma \in [0,1]}\ 1 - (1-\gamma)\Big(1 - e^{-\gamma^2 x/(2-\gamma)}\Big).ε∗(x)=γ∈[0,1]min​ 1−(1−γ)(1−e−γ2x/(2−γ)).

All algorithms of the paper follow one template: at time ttt, sample S^∼y⋅,t,zt∗\hat S \sim y^*_{\cdot,t,z_t}S^∼y⋅,t,zt​∗​; for each i∈S^i \in \hat Si∈S^, discard iii if it has no unit on hand and otherwise according to a per-product discarding rule; then offer a random subset of the survivors drawn by sub-assortment sampling (Procedure 1). Algorithm 2 discards at random with probability γ\gammaγ. Algorithm 3 keeps iii only if its fee exceeds a threshold computed from an optimistic per-unit dynamic program Vi,t\mathcal V_{i,t}Vi,t​ (equation (3)). Sim+Hybrid(i) chooses, product by product, between the two rules by comparing Ri=ciVi,1/(LP contribution of i)\mathcal R_i = c_i\mathcal V_{i,1}/(\text{LP contribution of } i)Ri​=ci​Vi,1​/(LP contribution of i) with 1−ε∗(ci)1 - \varepsilon^*(c_i)1−ε∗(ci​).

Formalization targets

Goal: Theorem 3

For every instance and every optimal normalized y∗y^*y∗,

E[Rev(Sim+Hybrid(i))] ≥ (1−min⁡{12,ε∗(cmin⁡)}) LP(y∗).\mathbb E\big[\mathrm{Rev}(\texttt{Sim+Hybrid(i)})\big] \ \ge\ \Big(1 - \min\Big\{\tfrac12, \varepsilon^*(c_{\min})\Big\}\Big)\, \mathrm{LP}(y^*).E[Rev(Sim+Hybrid(i))] ≥ (1−min{21​,ε∗(cmin​)})LP(y∗).

Milestones

  1. Proposition 3: sub-assortment sampling returns S~⊆S\tilde S \subseteq SS~⊆S with E[ϕ(S~,i)]=pi\mathbb E[\phi(\tilde S, i)] = p_iE[ϕ(S~,i)]=pi​ for every i∈Si \in Si∈S.
  2. Lemma EC.2: the multiplicative Chernoff bound (already posed on the platform; referenced).
  3. (EC.2): a randomly discarded product has no unit on hand with probability at most exp⁡(−γ2ci/(2−γ))\exp(-\gamma^2 c_i/(2-\gamma))exp(−γ2ci​/(2−γ)).
  4. Per-product bound in the proof of Theorem 1: E[riztIi,t]≥(1−γ)(1−e−γ2ci/(2−γ))∑z,SFt(z) riz ϕz(S,i) yS,t,z\mathbb E[r^{z_t}_i I_{i,t}] \ge (1-\gamma)(1 - e^{-\gamma^2 c_i/(2-\gamma)})\sum_{z,S} F_t(z)\, r^z_i\, \phi^z(S,i)\, y_{S,t,z}E[rizt​​Ii,t​]≥(1−γ)(1−e−γ2ci​/(2−γ))∑z,S​Ft​(z)riz​ϕz(S,i)yS,t,z​.
  5. Theorem 1: Algorithm 2 with γ=γ∗(cmin⁡)\gamma = \gamma^*(c_{\min})γ=γ∗(cmin​) is (1−ε∗(cmin⁡))(1 - \varepsilon^*(c_{\min}))(1−ε∗(cmin​))-competitive.
  6. ε∗(x)\varepsilon^*(x)ε∗(x) and its minimizers are O(log⁡x/x)O(\sqrt{\log x / x})O(logx/x​).
  7. Lemma EC.3: the per-unit revenue-to-go of Algorithm 3 from any inventory state is at least Vi,t\mathcal V_{i,t}Vi,t​.
  8. Part (ii) of the proof of Theorem 2: ciVi,1≥12c_i \mathcal V_{i,1} \ge \frac12ci​Vi,1​≥21​ (LP contribution of iii).
  9. Theorem 2: Algorithm 3 is 12\frac1221​-competitive.
  10. ε∗\varepsilon^*ε∗ is continuous and nonincreasing, ε∗(0)=1\varepsilon^*(0) = 1ε∗(0)=1, ε∗(∞)=0\varepsilon^*(\infty) = 0ε∗(∞)=0.

Significance

The result gives a single polynomial-time policy that is simultaneously 12\frac1221​-competitive, which is optimal for small inventories (a two-period example on p. 17 shows no online policy does better against this LP), and asymptotically optimal as inventories grow. Its analysis is modular: each product is treated separately, which is what allows mixing two discarding rules in one algorithm. Sub-assortment sampling is of independent use whenever an assortment must be thinned without distorting the choice probabilities of the remaining products.

The paper's proofs are on paper only; the per-product decoupling, which the paper invokes in a few lines for Theorem 3, is exactly the kind of step a formal proof makes explicit. A complete development produces a reusable finite model of a Bayesian online rental process (types, simulated assortments, discarding, choices and durations), a verified sub-assortment sampler, and an LP-duality certificate for the optimistic DP. None of these results is formalized elsewhere.

Difficulty

The obvious argument fails at the first step: whether product iii is available at time ttt depends on all earlier rentals, and the offer probabilities of different products are correlated through the shared assortment and through substitution, so rental indicators are neither independent nor product-separable. Two ingredients are needed. Sub-assortment sampling must make each product's selection probability exactly its LP target, whatever happened to the other products; only then can the rentals of product iii be coupled with an independent sequence for a concentration bound (EC.2). For small inventories, a concentration bound is too weak, and the analysis instead compares the true process with the optimistic DP by backward induction over inventory states (Lemma EC.3), then bounds the DP against the LP with an explicit dual solution (Part (ii)).

Formalization scope

Everything is finite: products are Fin n (the paper's product iii is index i−1i-1i−1), times are 1,…,T1, \dots, T1,…,T, types range over one finite type space (the paper's Zt\mathcal Z_tZt​ as subsets), and durations lie in {1,…,T}\{1, \dots, T\}{1,…,T}. The online process is a product of explicit per-step kernels over finite sample paths; probabilities and expectations are finite sums, with no measure theory. Conventions committed to:

  • ϕz(S,⋅)\phi^z(S,\cdot)ϕz(S,⋅) is a sub-probability supported on SSS for S∈SS \in \mathcal SS∈S; weak substitutability is required when S∪{j}∈SS \cup \{j\} \in \mathcal SS∪{j}∈S; S\mathcal SS is nonempty and downward closed;
  • r≥0r \ge 0r≥0, ci≥1c_i \ge 1ci​≥1, n≥1n \ge 1n≥1;
  • a unit rented at τ\tauτ is out at ttt iff its duration exceeds t−τt - \taut−τ, matching Gˉ(k)=Pr⁡[d>k]\bar G(k) = \Pr[d > k]Gˉ(k)=Pr[d>k] in the LP; Vi,s=0\mathcal V_{i,s} = 0Vi,s​=0 for s>Ts > Ts>T;
  • the competitive ratio is α⋅LP(y∗)≤E[Rev]\alpha \cdot \mathrm{LP}(y^*) \le \mathbb E[\mathrm{Rev}]α⋅LP(y∗)≤E[Rev] for every optimal y∗y^*y∗ with ∑SyS,t,z∗=1\sum_S y^*_{S,t,z} = 1∑S​yS,t,z∗​=1;
  • Procedure 1 breaks ties among equal ratios by product index, and its recursive step uses the j∗j^*j∗ products of largest ratio;
  • the page does not say which discarding probability a "large inventory" product uses; it is a minimizer γ∗(ci)\gamma^*(c_i)γ∗(ci​) of (1) at x=cix = c_ix=ci​;
  • the page calls ε∗\varepsilon^*ε∗ "monotone increasing"; the formalized statement is nonincreasing, which is what the proof uses;
  • running-time claims are not formalized.

The process is not allowed to rent a unit that is not on hand, the post-processing targets are ϕz(S^,i)\phi^{z}(\hat S, i)ϕz(S^,i) (not ϕz(Sˉ,i)\phi^z(\bar S, i)ϕz(Sˉ,i), which would make sub-assortment sampling the identity), and the path law uses the same y∗y^*y∗ as the benchmark; any formalization that drops one of these makes the goal a statement about a different process. Milestones 3, 4, 7 and 8 are stated for any feasible normalized yyy and arbitrary rules for the other products, which is the generality Theorem 3's proof needs.

Contributions welcome: lemmas on the process (normalization of the path law, the marginal law of one product's rentals), the Chernoff bound, and analytic facts about ε∗\varepsilon^*ε∗.

Selected references

  • Y. Feng, R. Niazadeh, A. Saberi, Near-Optimal Bayesian Online Assortment of Reusable Resources, Operations Research (Technical Note), 2024; arXiv:2512.06997v1. https://arxiv.org/abs/2512.06997
  • V. Goyal, G. Iyengar, R. Udwani, Online Allocation of Reusable Resources: Achieving Optimal Competitive Ratio, arXiv preprint, 2020. https://arxiv.org/abs/2002.02430
  • V. Goyal, G. Iyengar, R. Udwani, Online Allocation of Reusable Resources via Algorithms Guided by Fluid Approximations, arXiv preprint, 2020 (an idea similar to sub-assortment sampling, found concurrently). https://arxiv.org/abs/2010.03983
  • H. Chernoff, A Measure of Asymptotic Efficiency for Tests of a Hypothesis Based on the Sum of Observations, Annals of Mathematical Statistics, 1952. https://doi.org/10.1214/aoms/1177729330
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AnalysisQuantum InformationRepresentation Theory·Captain: mikedeng1

The Rate of Optimal Purification procedures: At Output Rate M/N → μ the Optimal All-Qubit Fidelity Tends to 2λ²/(2λ²+μ(1−λ)) for μ ≤ λ and 2λ²/(μ(1+λ)) for μ ≥ λResearch Paper

Motivation

A qubit stored or transmitted in the presence of noise loses purity. If many copies of the same unknown pure state σ=∣φ⟩⟨φ∣\sigma = |\varphi\rangle\langle\varphi|σ=∣φ⟩⟨φ∣ have each passed through the same noisy channel, one may try to undo the noise collectively: feed the NNN noisy copies into a quantum device and ask for MMM output qubits that are as close as possible to MMM perfect copies σ⊗M\sigma^{\otimes M}σ⊗M. The noise map itself is invertible as a linear map, but its inverse is not completely positive, so this purification problem is a genuine optimization over physical devices, closely related to optimal quantum cloning (Werner 1998, Keyl–Werner 1999).

Cirac, Ekert and Macchiavello (1999) found the optimal device for a single output qubit. Keyl and Werner (arXiv:quant-ph/9910124, 1999) solved the problem for an arbitrary number MMM of outputs and two figures of merit, and computed the trade-off between output number and quality. For the figure of merit that tests all outputs jointly, the best fidelity is a function of the output rate M/NM/NM/N alone in the limit, and that function is explicit. This mission formalizes that rate formula.

Setting

A qubit is C2\mathbb C^2C2 with basis ∣0⟩,∣1⟩|0\rangle, |1\rangle∣0⟩,∣1⟩; nnn qubits are (C2)⊗n(\mathbb C^2)^{\otimes n}(C2)⊗n, with basis indexed by words x:{0,…,n−1}→{0,1}x : \{0,\dots,n-1\} \to \{0,1\}x:{0,…,n−1}→{0,1}. Fix a noise parameter λ\lambdaλ with 0<λ<10 < \lambda < 10<λ<1. The depolarizing channel acts on a one-qubit density matrix σ\sigmaσ by

R∗σ=λ σ+(1−λ) 121.R_*\sigma = \lambda\,\sigma + (1-\lambda)\,\tfrac{1}{2}\mathbb 1 .R∗​σ=λσ+(1−λ)21​1.

A device from NNN to MMM qubits is a quantum channel T∗T_*T∗​, i.e. a trace-preserving completely positive linear map from 2N×2N2^N\times 2^N2N×2N to 2M×2M2^M\times 2^M2M×2M complex matrices. Its all-qubit fidelity is the worst case over pure inputs:

Fall(T)=inf⁡∥φ∥=1 tr⁡(σ⊗M T∗((R∗σ)⊗N)),σ=∣φ⟩⟨φ∣.F_{\mathrm{all}}(T) = \inf_{\|\varphi\|=1}\ \operatorname{tr}\Big(\sigma^{\otimes M}\, T_*\big((R_*\sigma)^{\otimes N}\big)\Big), \qquad \sigma = |\varphi\rangle\langle\varphi| .Fall​(T)=∥φ∥=1inf​ tr(σ⊗MT∗​((R∗​σ)⊗N)),σ=∣φ⟩⟨φ∣.

The optimal all-qubit fidelity is Fallmax⁡(N,M)=sup⁡TFall(T)F^{\max}_{\mathrm{all}}(N,M) = \sup_T F_{\mathrm{all}}(T)Fallmax​(N,M)=supT​Fall​(T), the supremum over all channels from NNN to MMM qubits. Finally, the rate function is

Φ(μ)={2λ22λ2+μ(1−λ)μ≤λ,2λ2μ(1+λ)μ≥λ.\Phi(\mu) = \begin{cases} \dfrac{2\lambda^2}{2\lambda^2 + \mu(1-\lambda)} & \mu \le \lambda,\\[2mm] \dfrac{2\lambda^2}{\mu(1+\lambda)} & \mu \ge \lambda. \end{cases}Φ(μ)=⎩⎨⎧​2λ2+μ(1−λ)2λ2​μ(1+λ)2λ2​​μ≤λ,μ≥λ.​

The proof works with the parametrization λ=tanh⁡β\lambda = \tanh\betaλ=tanhβ, β>0\beta > 0β>0, and with the decomposition of (C2)⊗N(\mathbb C^2)^{\otimes N}(C2)⊗N into spin-sss blocks, s∈I[N]={N/2,N/2−1,… }∩[0,∞)s \in I[N] = \{N/2, N/2-1, \dots\}\cap[0,\infty)s∈I[N]={N/2,N/2−1,…}∩[0,∞). Each block carries a weight wN(s)w_N(s)wN​(s) (eq. (14)), an explicit probability vector built from sinh⁡\sinhsinh, cosh⁡\coshcosh and binomial coefficients, and a state ρs(β)\rho_s(\beta)ρs​(β) on the symmetric subspace of 2s2s2s qubits.

Formalization targets

Goal: eq. (10)

For every sequence Nk→∞N_k \to \inftyNk​→∞ and every sequence MkM_kMk​ with Mk/Nk→μ>0M_k/N_k \to \mu > 0Mk​/Nk​→μ>0,

lim⁡k→∞Fallmax⁡(Nk,Mk)=Φ(μ).\lim_{k\to\infty} F^{\max}_{\mathrm{all}}(N_k, M_k) = \Phi(\mu).k→∞lim​Fallmax​(Nk​,Mk​)=Φ(μ).

Milestones

  1. Multiplicities (p. 9). sinh⁡β (2cosh⁡β)N=∑s∈I[N]sinh⁡((2s+1)β)dim⁡KN,s\sinh\beta\,(2\cosh\beta)^N = \sum_{s\in I[N]}\sinh((2s+1)\beta)\dim\mathcal K_{N,s}sinhβ(2coshβ)N=∑s∈I[N]​sinh((2s+1)β)dimKN,s​ with dim⁡KN,s=2s+1N/2+s+1(NN/2−s)\dim\mathcal K_{N,s} = \frac{2s+1}{N/2+s+1}\binom{N}{N/2-s}dimKN,s​=N/2+s+12s+1​(N/2−sN​), and wNw_NwN​ is a probability vector.
  2. Natural purifier block (p. 14). tr⁡ρs(β)=1\operatorname{tr}\rho_s(\beta) = 1trρs​(β)=1 and tr⁡(σ⊗2sρs(β))=1−e−2β1−e−(4s+2)β\operatorname{tr}(\sigma^{\otimes 2s}\rho_s(\beta)) = \frac{1-e^{-2\beta}}{1-e^{-(4s+2)\beta}}tr(σ⊗2sρs​(β))=1−e−(4s+2)β1−e−2β​.
  3. Proposition 4.2, corrected (p. 15). The fidelity of one block of the optimal purifier is the closed form fall(M,β,s)f_{\mathrm{all}}(M,\beta,s)fall​(M,β,s).
  4. Theorem 5.1, all-qubit half (p. 15). Fallmax⁡(N,M)=∑swN(s) fall(M,β,s)F^{\max}_{\mathrm{all}}(N,M) = \sum_{s} w_N(s)\,f_{\mathrm{all}}(M,\beta,s)Fallmax​(N,M)=∑s​wN​(s)fall​(M,β,s), and the supremum is attained.
  5. Lemma 6.1, corrected (pp. 18–19). ∑swN(s)fN(2s/N)→f∞(λ)\sum_s w_N(s) f_N(2s/N) \to f_\infty(\lambda)∑s​wN​(s)fN​(2s/N)→f∞​(λ) for uniformly bounded fNf_NfN​ converging uniformly near λ\lambdaλ.
  6. Lemma 6.2, corrected (pp. 21–22). (KM)−1∑R=MK(RM)zK−R→11−(1−c)z\binom{K}{M}^{-1}\sum_{R=M}^{K}\binom{R}{M}z^{K-R} \to \frac{1}{1-(1-c)z}(MK​)−1∑R=MK​(MR​)zK−R→1−(1−c)z1​ for ∣z∣<1|z|<1∣z∣<1, M/K→c∈[0,1]M/K \to c \in [0,1]M/K→c∈[0,1].

Significance

The result. Formula (10) says that Φ(μ)<1\Phi(\mu) < 1Φ(μ)<1 for every μ>0\mu > 0μ>0: in the all-qubit sense no purification procedure with a positive output rate approaches perfect fidelity, so optimal purification "works with zero rate". At the same time every fidelity level below one is achieved at a positive rate, and Φ\PhiΦ gives the exact trade-off. This contrasts with the one-qubit figure of merit treated in the same paper, where the fidelity of each output tends to one at any rate. Theorem 5.1 reduces an optimization over all channels between exponentially large spaces to a sum of ⌊N/2⌋+1\lfloor N/2\rfloor + 1⌊N/2⌋+1 explicit terms.

Formalizing it. The results are proved in the paper; none of them, to our knowledge, has a machine-checked proof. The paper's statement of Proposition 4.2 contains printing errors (swapped cases, a missing normalization factor, fonef_{\mathrm{one}}fone​ for fallf_{\mathrm{all}}fall​), and Lemmas 6.1 and 6.2 are stated with an incorrect domain and range; the milestones state the corrected versions, which were checked numerically against a semidefinite program for small N,MN, MN,M. A formal proof would certify the corrected formulas. Related platform items, not posed again here: uniqueness of the optimal cloner (Support21.P16.unique_optimal_cloner, open) and covariance averaging for cloners (Renew46.P45.symmetrization, open), both used in the optimality argument of Theorem 5.1.

Difficulty

The obvious route to the goal is to evaluate the fidelity of one good device. That gives only a lower bound: the goal is about the supremum over all channels, and the upper bound requires the optimality theorem (Theorem 5.1), whose proof needs a reduction to covariant, permutation-symmetric channels, the decomposition of tensor-power representations of SU(2)SU(2)SU(2), and the optimality and uniqueness of the cloning maps on each spin block. The asymptotic part is also not a direct substitution: the weights wN(s)w_N(s)wN​(s) must be shown to concentrate at 2s/N=λ2s/N = \lambda2s/N=λ, and on the side μ<λ\mu < \lambdaμ<λ the dominant blocks need the binomial-sum branch of fallf_{\mathrm{all}}fall​, whose limit is Lemma 6.2. Near μ=λ\mu = \lambdaμ=λ the two branches meet, and the limit must be controlled uniformly in the block index.

Formalization scope

  • Representation. nnn-qubit operators are complex matrices indexed by words Fin n → Fin 2; tensor powers are QAlgorithms.piKron; a pure state is QAlgorithms.pureDensity φ with ‖φ‖ = 1; a channel is a superoperator with a finite normalized Kraus family (QAlgorithms.IsChannel), which in finite dimension is exactly a CPTP map. The infimum and supremum are sInf/sSup on ℝ over sets that are nonempty and contained in [0,1][0,1][0,1].
  • Committed conventions. The noise is applied to each input copy before the tensor power, and the target is σ⊗M\sigma^{\otimes M}σ⊗M for the same σ\sigmaσ. The worst case is over all unit vectors in C2\mathbb C^2C2. The supremum is over all channels, not over covariant channels or the paper's purifiers. The goal assumes 0<λ<10 < \lambda < 10<λ<1 and μ>0\mu > 0μ>0, and the limit is taken along every pair of sequences with Nk→∞N_k \to \inftyNk​→∞, Mk/Nk→μM_k/N_k \to \muMk​/Nk​→μ. Milestones are stated in β>0\beta > 0β>0 with λ=tanh⁡β\lambda = \tanh\betaλ=tanhβ. Spins are encoded by k=N/2−s∈{0,…,⌊N/2⌋}k = N/2 - s \in \{0,\dots,\lfloor N/2\rfloor\}k=N/2−s∈{0,…,⌊N/2⌋}, so 2s=N−2k∈N2s = N - 2k \in \mathbb N2s=N−2k∈N; ψ=(1,0)\psi = (1,0)ψ=(1,0) is basis vector 000.
  • Ruled out. Fixing the input state to ∣0⟩|0\rangle∣0⟩ trivializes the problem (the channel that outputs ∣0⋯0⟩|0\cdots0\rangle∣0⋯0⟩ has fidelity one); the infimum over all φ\varphiφ is essential. Restricting the supremum to symmetric channels would make Theorem 5.1 a different statement.
  • Infrastructure. A full development needs: Kraus-form channels and their compactness, the symmetric-subspace projector (boseProjector) and the optimal cloner (canonicalCloner), the SU(2)SU(2)SU(2) decomposition of (C2)⊗N(\mathbb C^2)^{\otimes N}(C2)⊗N with multiplicities, and concentration of the weights wNw_NwN​. The binomial-sum limit (Lemma 6.2) and the weight concentration (Lemma 6.1) are reusable outside this mission. Contributions of any milestone, or of lemmas toward the SU(2)SU(2)SU(2) decomposition, are welcome.

Selected references

  • M. Keyl, R. F. Werner, The rate of optimal purification procedures, arXiv:quant-ph/9910124v1, 1999; Ann. Henri Poincaré 2 (2001) 1–26. https://arxiv.org/abs/quant-ph/9910124
  • J. I. Cirac, A. K. Ekert, C. Macchiavello, Optimal purification of single qubits, Phys. Rev. Lett. 82 (1999) 4344. https://arxiv.org/abs/quant-ph/9812075
  • R. F. Werner, Optimal cloning of pure states, Phys. Rev. A 58 (1998) 1827. https://arxiv.org/abs/quant-ph/9804001
  • M. Keyl, R. F. Werner, Optimal cloning of pure states, testing single clones, J. Math. Phys. 40 (1999) 3283. https://arxiv.org/abs/quant-ph/9807010
14 thms2 active usersReviewed
Machine LearningOperations ResearchStatistics·Captain: mikedeng1

Fixing Inventory Inaccuracies at Scale: The Entrywise Algorithm's Expected Anomaly-Detection Cost Is Within O(log^1.5(m)/√m) of the Optimal CostResearch Paper

Motivation

Retail inventory records are often wrong. A store's system may report units on the shelf that are not there (phantom inventory), so the replenishment system never reorders and the product silently stops selling. Audits fix such errors but are expensive, so a retailer wants to decide which store–SKU pairs to audit from sales data alone. The classical way, studying each pair's sales history over a long period, needs time-homogeneous data that rarely exists.

Farias, Li and Peng (arXiv:2006.13126v3, Manufacturing & Service Operations Management, 2024) instead use a single cross-sectional snapshot of sales across nnn stores and mmm SKUs. Expected demand is modelled as a low-rank matrix, anomalies corrupt a random subset of entries, and only some entries are observed. The paper proposes the entrywise (EW) algorithm and proves that its expected decision cost approaches that of an oracle knowing the model, at rate log⁡1.5(m)/m\log^{1.5}(m)/\sqrt mlog1.5(m)/m​. A matching Ω(1/m)\Omega(1/\sqrt m)Ω(1/m​) lower bound (Proposition 1) is also proved. The paper evaluates the method on synthetic data and on real data from a consumer goods retailer.

Setting

An instance has an expected-demand matrix M∗∈R+n×mM^*\in\mathbb R_+^{n\times m}M∗∈R+n×m​ with 2≤m≤n2\le m\le n2≤m≤n, rank rrr and SVD M∗=UΣV⊤M^*=U\Sigma V^\topM∗=UΣV⊤ with singular values σ1∗≥⋯≥σr∗>0\sigma_1^*\ge\dots\ge\sigma_r^*>0σ1∗​≥⋯≥σr∗​>0 and κ=σ1∗/σr∗\kappa=\sigma_1^*/\sigma_r^*κ=σ1∗​/σr∗​. It also has an anomaly model Anom(α,M)\mathrm{Anom}(\alpha,M)Anom(α,M), which is a family of laws on N\mathbb NN indexed by a parameter α∈Γ⊂Rd\alpha\in\Gamma\subset\mathbb R^dα∈Γ⊂Rd and a mean level M≥0M\ge0M≥0. The remaining data are a true parameter α∗\alpha^*α∗, an anomaly probability pA∗p_A^*pA∗​, an observation probability pOp_OpO​, and costs cij(0)c^{(0)}_{ij}cij(0)​ (flagging a normal entry) and cij(1)c^{(1)}_{ij}cij(1)​ (missing an anomaly). Independently for every entry:

  1. the entry is observed with probability pOp_OpO​; the observed set is Ω\OmegaΩ;
  2. Bij∼Bernoulli(pA∗)B_{ij}\sim\mathrm{Bernoulli}(p_A^*)Bij​∼Bernoulli(pA∗​) marks an anomaly;
  3. sales are Xij∼Poisson(Mij∗)X_{ij}\sim\mathrm{Poisson}(M^*_{ij})Xij​∼Poisson(Mij∗​) if Bij=0B_{ij}=0Bij​=0 and Xij∼Anom(α∗,Mij∗)X_{ij}\sim\mathrm{Anom}(\alpha^*,M^*_{ij})Xij​∼Anom(α∗,Mij∗​) if Bij=1B_{ij}=1Bij​=1.

Assumptions (§2):

  • ∥M∗∥max⁡\|M^*\|_{\max}∥M∗∥max​ lies between a constant cM>0c_M>0cM​>0 and LLL.
  • Incoherence: ∥U∥2,∞≤μr/n\|U\|_{2,\infty}\le\sqrt{\mu r/n}∥U∥2,∞​≤μr/n​ and ∥V∥2,∞≤μr/m\|V\|_{2,\infty}\le\sqrt{\mu r/m}∥V∥2,∞​≤μr/m​.
  • Sparsity: pO≥Clog⁡1.5(m)μrκ2/m\sqrt{p_O}\ge C\log^{1.5}(m)\mu r\kappa^2/\sqrt mpO​​≥Clog1.5(m)μrκ2/m​.
  • pA∗≤1−cAp_A^*\le1-c_ApA∗​≤1−cA​.
  • Anom(α∗,Mij∗)\mathrm{Anom}(\alpha^*,M^*_{ij})Anom(α∗,Mij∗​) has sub-exponential norm ≤L\le L≤L.
  • P(Anom(α,M)=k)\mathbb P(\mathrm{Anom}(\alpha,M)=k)P(Anom(α,M)=k) is KKK-Lipschitz in (α,M)(\alpha,M)(α,M).
  • Mean decomposition: E Anom(α,M)=g(α)M\mathbb E\,\mathrm{Anom}(\alpha,M)=g(\alpha)MEAnom(α,M)=g(α)M with ggg valued in [0,1][0,1][0,1] and KKK-Lipschitz.

The oracle π∗\pi^*π∗ knows θ∗=(α∗,pA∗)\theta^*=(\alpha^*,p_A^*)θ∗=(α∗,pA∗​) and M∗M^*M∗. It computes the posterior fij∗=P(Bij=0∣XΩ)=yij∗/(xij∗+yij∗)f^*_{ij}=\mathbb P(B_{ij}=0\mid X_\Omega)=y^*_{ij}/(x^*_{ij}+y^*_{ij})fij∗​=P(Bij​=0∣XΩ​)=yij∗​/(xij∗​+yij∗​), where xij∗=pA∗PAnom(α∗,Mij∗)(Xij)x^*_{ij}=p_A^*\mathbb P_{\mathrm{Anom}(\alpha^*,M^*_{ij})}(X_{ij})xij∗​=pA∗​PAnom(α∗,Mij∗​)​(Xij​) and yij∗=(1−pA∗)PPoisson(Mij∗)(Xij)y^*_{ij}=(1-p_A^*)\mathbb P_{\mathrm{Poisson}(M^*_{ij})}(X_{ij})yij∗​=(1−pA∗​)PPoisson(Mij∗​)​(Xij​). It flags (i,j)(i,j)(i,j) iff cij(1)/(cij(0)+cij(1))≥fij∗c^{(1)}_{ij}/(c^{(0)}_{ij}+c^{(1)}_{ij})\ge f^*_{ij}cij(1)​/(cij(0)​+cij(1)​)≥fij∗​. The EW algorithm πEW\pi^{EW}πEW runs four steps:

  1. It computes M^=nm∣Ω∣SVD(XΩ)r\hat M=\frac{nm}{|\Omega|}\mathrm{SVD}(X_\Omega)_rM^=∣Ω∣nm​SVD(XΩ​)r​, a rescaled best rank-rrr approximation of the zero-filled observations.
  2. It estimates θ^\hat\thetaθ^ by matching TTT empirical CDF values ∣{Xij≤t,(i,j)∈Ω}∣/∣Ω∣|\{X_{ij}\le t,(i,j)\in\Omega\}|/|\Omega|∣{Xij​≤t,(i,j)∈Ω}∣/∣Ω∣ to their model predictions gt(θ,M^/e(θ))g_t(\theta,\hat M/e(\theta))gt​(θ,M^/e(θ)), where e(θ)=pAg(α)+1−pAe(\theta)=p_Ag(\alpha)+1-p_Ae(θ)=pA​g(α)+1−pA​.
  3. It forms plug-in estimates f^ij\hat f_{ij}f^​ij​ of fij∗f^*_{ij}fij∗​.
  4. It applies the oracle's threshold rule to f^\hat ff^​.

The cost of decisions AAA is

costA(XΩ)=1∣Ω∣∑(i,j)∈Ω(cij(0)1{Aij=1}fij∗+cij(1)1{Aij=0}(1−fij∗)).\mathrm{cost}^A(X_\Omega)=\frac1{|\Omega|}\sum_{(i,j)\in\Omega}\Big(c^{(0)}_{ij}\mathbf 1\{A_{ij}=1\}f^*_{ij}+c^{(1)}_{ij}\mathbf 1\{A_{ij}=0\}(1-f^*_{ij})\Big).costA(XΩ​)=∣Ω∣1​(i,j)∈Ω∑​(cij(0)​1{Aij​=1}fij∗​+cij(1)​1{Aij​=0}(1−fij∗​)).

Formalization targets

Goal: Theorem 1 (p. 12)

EXΩ(costπEW(XΩ)−costπ∗(XΩ))≤cmax⁡ C0 (1+K+L+κ+μ+r+pO−1)k log⁡1.5(m)m.\mathbb E_{X_\Omega}\Big(\mathrm{cost}^{\pi^{EW}}(X_\Omega)-\mathrm{cost}^{\pi^*}(X_\Omega)\Big)\le c_{\max}\,C_0\,(1+K+L+\kappa+\mu+r+p_O^{-1})^k\,\frac{\log^{1.5}(m)}{\sqrt m}.EXΩ​​(costπEW(XΩ​)−costπ∗(XΩ​))≤cmax​C0​(1+K+L+κ+μ+r+pO−1​)km​log1.5(m)​.

The constants C0C_0C0​ and kkk and the sparsity constant depend only on ddd, cMc_McM​, cAc_AcA​ and the regularity constant CRCC_{RC}CRC​. The statement asserts the paper's rate with polynomial dependence on the model parameters. It does not fix the polynomial, so a sharper analysis still proves it.

Milestones, in the proof's order

  • Lemma 8: ∥Poisson(λ)∥ψ1≤4λ+1\|\mathrm{Poisson}(\lambda)\|_{\psi_1}\le4\lambda+1∥Poisson(λ)∥ψ1​​≤4λ+1.
  • Lemma 14: a Bernstein bound for ∑(i,j)∈ΩTij\sum_{(i,j)\in\Omega}T_{ij}∑(i,j)∈Ω​Tij​.
  • Theorem 2: the entrywise bound ∥M^−e(θ∗)M∗∥max⁡≤Cδ′\|\hat M-e(\theta^*)M^*\|_{\max}\le C\delta'∥M^−e(θ∗)M∗∥max​≤Cδ′ with δ′=κ4μrLlog⁡m/(pOm)\delta'=\kappa^4\mu rL\sqrt{\log m/(p_Om)}δ′=κ4μrLlogm/(pO​m)​.
  • Lemmas 15 and 16: the model moments and the objective h(θ∗)h(\theta^*)h(θ∗).
  • Lemma 2: ∥F(θ^)−F(θ∗)∥≲(K+L)δ′\|F(\hat\theta)-F(\theta^*)\|\lesssim(K+L)\delta'∥F(θ^)−F(θ∗)∥≲(K+L)δ′.
  • Lemma 17: a quantitative inverse-function bound.
  • Lemma 1: ∥θ^−θ∗∥≲(K+L)δ′\|\hat\theta-\theta^*\|\lesssim(K+L)\delta'∥θ^−θ∗∥≲(K+L)δ′.
  • Lemmas 18 and 19: plug-in likelihoods and the ratio perturbation bound.
  • Lemma 3: ∣fij∗−f^ij∣≤min⁡(Cδ/(xij∗+yij∗),1)|f^*_{ij}-\hat f_{ij}|\le\min(C\delta/(x^*_{ij}+y^*_{ij}),1)∣fij∗​−f^​ij​∣≤min(Cδ/(xij∗​+yij∗​),1).
  • Step 4 of the proof sketch: the excess cost is at most 1∣Ω∣∑Ω∣aij−bij∣\frac1{|\Omega|}\sum_\Omega|a_{ij}-b_{ij}|∣Ω∣1​∑Ω​∣aij​−bij​∣.

Significance

Theorem 1 says that the value of cross-sectional data grows with the number of stores and SKUs. A retailer that can only see one snapshot does nearly as well as one that knows the demand matrix and the anomaly law exactly. With Proposition 1, the rate is optimal up to the logarithmic factor. Theorem 2 is, per the authors, the first entrywise guarantee for matrix completion under Poisson (more generally sub-exponential) noise, and it is reusable outside inventory problems.

The results are proved on paper: Theorem 1 by a proof sketch in §5.1 plus Appendix B, and Theorem 2 in Appendix A, which builds on a cited entrywise eigenvector perturbation theorem of Abbe et al. None of this is formalized. A machine-checked proof would also settle the constants and conventions that the paper leaves implicit. These include the dimension restriction in Lemma 17, the unspecified constant in Lemma 3, the form of the sparsity assumption used in the proof of Theorem 2, and the closed range of pAp_ApA​ in Θ\ThetaΘ.

Difficulty

The obvious argument plugs consistent estimates of M∗M^*M∗ and θ∗\theta^*θ∗ into the Bayes rule. It breaks at the first step: a Frobenius-norm bound for M^\hat MM^, which is what standard matrix completion gives, does not control any single f^ij\hat f_{ij}f^​ij​. An entrywise bound is needed, under heavy-tailed (sub-exponential, not sub-Gaussian) noise, and with the anomalies corrupting the mean by the unknown factor e(θ∗)e(\theta^*)e(θ∗). The second step inverts the moment map FFF. Closeness of moments yields closeness of parameters only through a quantitative inverse-function argument, which needs the regularity conditions of Lemma 1. A third subtlety is that fij∗f^*_{ij}fij∗​ is a ratio whose denominator xij∗+yij∗x^*_{ij}+y^*_{ij}xij∗​+yij∗​ can be tiny. The error bound of Lemma 3 therefore degrades on rare sales values, and Theorem 1 averages this over the law of XXX.

Formalization scope

One definitions module, InventoryAnomaly.EW.Model, holds the instance, the product sampling law over {\{{observed}×{\}\times\{}×{anomalous}×N\}\times\mathbb N}×N per entry, the estimators, the costs and four predicates:

  • Model: §2's assumptions;
  • SparsityMax: the sparsity condition as read in the proof of Theorem 2, p. 41;
  • Regular: Lemma 1's conditions;
  • CostBound: costs in [0,cmax⁡][0,c_{\max}][0,cmax​].

The sub-exponential norm is the published HighDimProb.Concentration.subexponentialNorm.

Conventions:

  • Parameters. θ=(α,pA)∈Rd+1\theta=(\alpha,p_A)\in\mathbb R^{d+1}θ=(α,pA​)∈Rd+1, and T=d+1T=d+1T=d+1 moments are matched.
  • Parameter set. Θ=Γ×[0,1−cA]\Theta=\Gamma\times[0,1-c_A]Θ=Γ×[0,1−cA​].
  • Clamped means. Laws are evaluated at the mean max⁡(M,0)\max(M,0)max(M,0).
  • Cost. The cost is the closed form (5) with f∗f^*f∗ by Bayes' rule (8). c(0)c^{(0)}c(0) is the false-positive cost (the display on p. 12 swaps the labels).
  • Estimators. SVDr\mathrm{SVD}_rSVDr​ is any exact best rank-rrr approximation. θ^\hat\thetaθ^ is any point of Θ\ThetaΘ with h(θ^)≤h(θ∗)h(\hat\theta)\le h(\theta^*)h(θ^)≤h(θ∗), which every minimiser of (7) satisfies.
  • Constants. "O(⋅)O(\cdot)O(⋅)" and "with probability 1−O(1/nm)1-O(1/nm)1−O(1/nm)" are existential constants. They come after d,cM,cA,CRCd,c_M,c_A,C_{RC}d,cM​,cA​,CRC​ and before the instance.
  • Added conditions. 2≤m≤n2\le m\le n2≤m≤n, 1≤r≤m1\le r\le m1≤r≤m, finite anomaly means, and nonnegative costs. Lemma 17 is stated for square Jacobians. Lemma 3 has a constant CCC in place of 2. Lemma 19's δ/(x^+y^)\delta/(\hat x+\hat y)δ/(x^+y^​) clause is stated when x^+y^>0\hat x+\hat y>0x^+y^​>0. Each item's Formalization Note lists these.

The algorithm's selections are universally quantified together with their defining properties. Neither may be replaced by unconstrained functions. The cost of π∗\pi^*π∗ must use f∗f^*f∗, not f^\hat ff^​. The goal must keep the explicit rate log⁡1.5(m)/m\log^{1.5}(m)/\sqrt mlog1.5(m)/m​ and the full probability model, without assuming Theorem 2's event.

Not formalized: Proposition 1 (the lower bound), Appendix E (the TPR/FPR-constrained variant), the cited Lemmas 6–7, and the internal Lemmas 9–13 and Propositions 2–3 of Appendix A.

Useful infrastructure includes entrywise singular-subspace perturbation bounds, Bernstein's inequality for bounded independent sums, and Orlicz-norm bounds for Poisson variables. All three are reusable beyond this mission. Proofs of individual milestones are welcome, especially Lemmas 8, 14, 17 and 19 and Step 4, which are self-contained.

Selected references

  • V. F. Farias, A. A. Li, T. Peng, Fixing Inventory Inaccuracies at Scale, Manufacturing & Service Operations Management, 2024; arXiv:2006.13126v3 (2022). https://arxiv.org/abs/2006.13126
  • E. Abbe, J. Fan, K. Wang, Y. Zhong, Entrywise Eigenvector Analysis of Random Matrices with Low Expected Rank, Annals of Statistics 48(3), 2020. https://arxiv.org/abs/1709.09565
  • A. D. McRae, M. A. Davenport, Low-rank matrix completion and denoising under Poisson noise, Information and Inference 10(2), 2021. https://arxiv.org/abs/1907.05325
  • R. Vershynin, High-Dimensional Probability, Cambridge University Press, 2018. https://doi.org/10.1017/9781108231596
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CombinatoricsGroup TheoryRepresentation Theory·Captain: mikedeng1

Comparison of Gelfand-Tsetlin Bases for Alternating and Symmetric Groups: The Recursively Defined Vectors u_α Form a Gelfand–Tsetlin Basis of Each Irreducible Representation of A_nResearch Paper

Motivation

A Gelfand–Tsetlin basis of a representation of the last group in a tower G1⊂G2⊂⋯⊂GnG_1 \subset G_2 \subset \cdots \subset G_nG1​⊂G2​⊂⋯⊂Gn​ is a basis adapted to every restriction at once: each basis vector spans a line that is cut out by the isotypic decompositions at all levels k=1,…,nk = 1, \dots, nk=1,…,n. When every restriction Gk↓Gk−1G_k \downarrow G_{k-1}Gk​↓Gk−1​ is multiplicity-free, these lines are canonical, and the basis vectors are indexed by paths in the branching graph. For the symmetric groups, Young's orthogonal form gives such a basis with completely explicit matrices for the simple transpositions (Young, 1932; see Headley, 1996, Theorem 2.1), and the Vershik–Okounkov approach (arXiv:math/0503040) builds the representation theory of SnS_nSn​ around it.

The alternating groups AnA_nAn​ also form a multiplicity-free tower, so their irreducible representations have Gelfand–Tsetlin bases too. Geetha and Prasad (arXiv:1606.04424) write these bases down explicitly inside Young's orthogonal form, so that the Gelfand–Tsetlin bases of AnA_nAn​ and SnS_nSn​ can be compared vector by vector. The branching rules of AnA_nAn​ were known before (Ruff, Algebra Colloquium 2008, Theorem 6.1); the new ingredient is a sign normalisation of the associator that identifies the two halves Vλ±V_\lambda^{\pm}Vλ±​ of a self-conjugate VλV_\lambdaVλ​ consistently along the whole tower.

Setting

For a partition λ\lambdaλ of nnn, VλV_\lambdaVλ​ is the complex vector space with basis {vT}\{v_T\}{vT​} indexed by the standard Young tableaux TTT of shape λ\lambdaλ. Tableaux are written inline row by row, e.g. [1 2 4/3/5][1\,2\,4/3/5][124/3/5]. The simple transposition si=(i,i+1)s_i = (i, i+1)si​=(i,i+1) acts by Young's formulas (2): if iii lies in row jjj, column kkk of TTT and i+1i+1i+1 in row j′j'j′, column k′k'k′, and r=(k′−j′)−(k−j)r = (k'-j') - (k-j)r=(k′−j′)−(k−j), then ρλ(si)vT\rho_\lambda(s_i) v_Tρλ​(si​)vT​ is vTv_TvT​ (same row), −vT-v_T−vT​ (same column), and otherwise r−1vT+1−r−2 vsiTr^{-1} v_T + \sqrt{1-r^{-2}}\, v_{s_iT}r−1vT​+1−r−2​vsi​T​. For μ∈λ↓\mu \in \lambda^{\downarrow}μ∈λ↓ (one box fewer), VμV_\muVμ​ embeds in VλV_\lambdaVλ​ by vT↦vTλv_T \mapsto v_{T^\lambda}vT​↦vTλ​, with nnn written in the new box (4).

For self-conjugate λ=λ′\lambda = \lambda'λ=λ′, the associator φλ\varphi_\lambdaφλ​ is the operator

φλ(vT)=i(n−d(λ))/2 ϵ(wT) vT′(9),\varphi_\lambda(v_T) = i^{(n-d(\lambda))/2}\,\epsilon(w_T)\,v_{T'} \qquad (9),φλ​(vT​)=i(n−d(λ))/2ϵ(wT​)vT′​(9),

where T′T'T′ is the transposed tableau, d(λ)d(\lambda)d(λ) the number of diagonal boxes, and ϵ(wT)\epsilon(w_T)ϵ(wT​) the sign of the permutation carrying a fixed reference tableau TλT_\lambdaTλ​ to TTT. The reference tableau is chosen through self-conjugate covers (μ,λ)(\mu, \lambda)(μ,λ) (μ∈λ↓\mu \in \lambda^\downarrowμ∈λ↓, both self-conjugate): the smaller partition gets the row superstandard tableau, and the larger one the same tableau with nnn added on the diagonal. Vλ±V_\lambda^{\pm}Vλ±​ are the ±1\pm 1±1 eigenspaces of φλ\varphi_\lambdaφλ​.

Labels α∈Θ~(n)\alpha \in \tilde\Theta(n)α∈Θ~(n) are non-self-conjugate partitions λ\lambdaλ, with Vα=VλV_\alpha = V_\lambdaVα​=Vλ​, and symbols λ±\lambda^{\pm}λ± for self-conjugate λ\lambdaλ, with Vα=Vλ±V_\alpha = V_\lambda^{\pm}Vα​=Vλ±​. Conjugate non-self-conjugate labels are equivalent, λ∼λ′\lambda \sim \lambda'λ∼λ′. A path α‾=(α(2),…,α(n))∈S~(α)\underline\alpha = (\alpha^{(2)}, \dots, \alpha^{(n)}) \in \tilde{\mathcal S}(\alpha)α​=(α(2),…,α(n))∈S~(α) has each α(i)\alpha^{(i)}α(i) obtained from α(i+1)\alpha^{(i+1)}α(i+1) by removing one box, with equal signs whenever both are self-conjugate. Definition 2 builds a vector uα‾∈Vαu_{\underline\alpha} \in V_\alphauα​​∈Vα​ recursively from u(2)=v[1 2]u_{(2)} = v_{[1\,2]}u(2)​=v[12]​ and u(12)=v[1/2]u_{(1^2)} = v_{[1/2]}u(12)​=v[1/2]​. At each step the previous vector xxx is embedded by (4), and when the path passes from a non-self-conjugate shape to λ±\lambda^{\pm}λ± it is replaced by x±φλ(x)x \pm \varphi_\lambda(x)x±φλ​(x).

Formalization targets

Goal: Theorem 4 (Main Theorem), p. 14

For n≥2n \ge 2n≥2 and α∈Θ~(n)\alpha \in \tilde\Theta(n)α∈Θ~(n):

uα‾≠0,uα‾∈Vα∩⋂k=2n−1IsoAk(Vα(k))for every α‾∈S~(α),u_{\underline\alpha} \ne 0,\quad u_{\underline\alpha} \in V_\alpha \cap \bigcap_{k=2}^{n-1} \mathrm{Iso}_{A_k}\big(V_{\alpha^{(k)}}\big) \quad\text{for every } \underline\alpha \in \tilde{\mathcal S}(\alpha),uα​​=0,uα​​∈Vα​∩k=2⋂n−1​IsoAk​​(Vα(k)​)for every α​∈S~(α),

and for any set RRR of paths ending at α\alphaα containing one path from each equivalence class,

Vα=⨁α‾∈RC uα‾.V_\alpha = \bigoplus_{\underline\alpha \in R} \mathbb C\, u_{\underline\alpha}.Vα​=α​∈R⨁​Cuα​​.

Milestones

  1. Lemma 1 (p. 4): the recursive characterisation of Gelfand–Tsetlin subspaces.
  2. Lemma 2 (p. 6): every associator maps vTv_TvT​ to a multiple of vT′v_{T'}vT′​.
  3. §3, (7)–(9) (pp. 7–9): for every partition, reference tableau TλT_\lambdaTλ​ and scalar cTλc_{T_\lambda}cTλ​​, the map vT↦cTλϵ(wT)vT′v_T \mapsto c_{T_\lambda}\epsilon(w_T)v_{T'}vT​↦cTλ​​ϵ(wT​)vT′​ satisfies (5); the normalised self-conjugate φλ\varphi_\lambdaφλ​ of (9) also satisfies φλ2=id\varphi_\lambda^2 = \mathrm{id}φλ2​=id.
  4. Theorem 1 (1)–(2) (p. 9): Vλ≅Vλ′V_\lambda \cong V_{\lambda'}Vλ​≅Vλ′​ irreducible on AnA_nAn​ for λ≠λ′\lambda \ne \lambda'λ=λ′; Vλ±V_\lambda^\pmVλ±​ non-isomorphic irreducibles for λ=λ′\lambda = \lambda'λ=λ′.
  5. Lemma 3 (p. 9): for self-conjugate μ∈λ↓\mu \in \lambda^\downarrowμ∈λ↓, the embedding (4) is An−1A_{n-1}An−1​-equivariant and maps Vμ±V_\mu^{\pm}Vμ±​ into Vλ±V_\lambda^{\pm}Vλ±​.
  6. Theorem 2 (p. 10): the branching table of An−1⊂AnA_{n-1} \subset A_nAn−1​⊂An​.
  7. Theorem 3 (p. 12): each equivalence class of paths has 2r+12^{r+1}2r+1 elements.

Significance

The theorem gives closed-form Gelfand–Tsetlin bases for every irreducible representation of every alternating group. Each vector is a combination of Young's orthogonal basis vectors with Gaussian-integer coefficients; Example 2 of the paper shows one with four terms and coefficients 1,i,−1,i1, i, -1, i1,i,−1,i. The matrices of AnA_nAn​ in this basis then follow directly from Young's formulas. It also shows exactly how the two Gelfand–Tsetlin bases compare: on non-self-conjugate shapes they coincide, and on self-conjugate shapes the AnA_nAn​-vectors are the ±\pm±-symmetrisations x±φλ(x)x \pm \varphi_\lambda(x)x±φλ​(x) under the associator.

The result is proved in the paper; nothing about it is formalized. Lean's Mathlib has Young diagrams and the platform has standard tableaux, but there is no Young orthogonal form, no associator, no representation of AnA_nAn​ built from partitions, and no Gelfand–Tsetlin basis for any group. A complete development would give the first machine-checked Gelfand–Tsetlin basis for AnA_nAn​. Along the way it would give a machine-checked Young orthogonal form with its sign calculus, which is reusable for any later work on symmetric-group representations.

Difficulty

The Gelfand–Tsetlin property is a statement about isotypic components at every level. Checking it needs, at each level, the branching rule and an argument that the recursively built vector lands in the right isotypic component. For non-self-conjugate shapes this is inherited from SnS_nSn​. The difficulty is the self-conjugate case. A path through two consecutive self-conjugate shapes μ±→λ±\mu^{\pm} \to \lambda^{\pm}μ±→λ± keeps the sign only if φλ\varphi_\lambdaφλ​ restricts exactly to φμ\varphi_\muφμ​ on VμV_\muVμ​, so the bare existence of an associator for each λ\lambdaλ, unique up to scalar by Schur's lemma, is not enough. The sign of each φλ\varphi_\lambdaφλ​ has to be fixed coherently along self-conjugate covers, and this is what the choice of TλT_\lambdaTλ​ and the factor i(n−d(λ))/2i^{(n-d(\lambda))/2}i(n−d(λ))/2 do. The basis half needs, in addition, the count of how many paths share a geodesic (Theorem 3) and the fact that distinct classes give distinct lines.

Formalization scope

  • Tableaux. Standard tableaux are the published YoungTableau of QAlgorithms_Papers_Independent_Renew46_P26. Labels are 0,…,n−10, \dots, n-10,…,n−1 (the paper's entry iii is label i−1i-1i−1) and boxes are 0-based (row, column).
  • Spaces and operators. VλV_\lambdaVλ​ is the space of finitely supported functions on standard tableaux of shape λ\lambdaλ. Young's formulas (2), the embedding (4) and the associator (9) are explicit linear operators. That (2) defines a representation of SnS_nSn​ is the cited [5, Theorem 2.1], not a result of the paper.
  • Equivariance. "AkA_kAk​-equivariant" means commuting with every product ρ(si)ρ(sj)\rho(s_i)\rho(s_j)ρ(si​)ρ(sj​), 1≤i,j≤k−11 \le i, j \le k-11≤i,j≤k−1. These products generate AkA_kAk​, so this is equivalent to AkA_kAk​-equivariance once (2) defines a representation.
  • Isotypic subspaces. The AkA_kAk​-isotypic subspace of type WWW is the sum of the images of WWW under all AkA_kAk​-equivariant linear maps.
  • Gelfand–Tsetlin vectors. A Gelfand–Tsetlin vector for a path is a nonzero vector of VαV_\alphaVα​ lying in the isotypic subspace of type Vα(k)V_{\alpha^{(k)}}Vα(k)​ at every level kkk.
  • Standing hypothesis. The goal assumes n≥2n \ge 2n≥2, as the paper's paths start at Θ~(2)\tilde\Theta(2)Θ~(2).

Ruled out. The Gelfand–Tsetlin predicate is defined intrinsically through isotypic components. It is never defined as membership in a span of the vectors that Definition 2 produces, and uα‾u_{\underline\alpha}uα​​ is never replaced by a formula that makes Theorem 4 hold by definition.

Not formalized. Corollary 1, the completeness clause of Theorem 1, the bijection clause of Theorem 3, Examples 1–3 and Remarks 1–4.

Solvers will need several pieces of infrastructure:

  • that Young's formulas satisfy the Coxeter relations;
  • the sign calculus csiT=−cTc_{s_iT} = -c_Tcsi​T​=−cT​ for ϵ(wT)\epsilon(w_T)ϵ(wT​);
  • multiplicity-freeness of Sn↓Sn−1S_n \downarrow S_{n-1}Sn​↓Sn−1​ in this model;
  • the passage from generator-wise equivariance to isotypic decompositions.

The Coxeter relations and the sign calculus are reusable beyond this mission. Contributions proving any milestone, or proving that Young's operators define a representation, are welcome.

Selected references

  • T. Geetha, A. Prasad, Comparison of Gelfand-Tsetlin bases for alternating and symmetric groups, arXiv:1606.04424v2, 2017 (published in Algebras and Representation Theory). https://arxiv.org/abs/1606.04424
  • P. Headley, On Young's orthogonal form and the characters of the alternating group, Journal of Algebraic Combinatorics 5(2):127–134, 1996.
  • A. M. Vershik, A. Yu. Okounkov, A new approach to the representation theory of the symmetric groups. II, Journal of Mathematical Sciences 131(2):5471–5494, 2005. https://arxiv.org/abs/math/0503040
  • O. Ruff, Weight theory for alternating groups, Algebra Colloquium 15(3):391–404, 2008.
  • A. Young, On quantitative substitutional analysis, Proceedings of the London Mathematical Society 2(1):196–230, 1932.
  • A. Prasad, Representation Theory: A Combinatorial Viewpoint, Cambridge Studies in Advanced Mathematics 147, Cambridge University Press, 2015.
10 thms2 active usersReviewed
Algorithmic Game TheoryOperations ResearchProbability·Captain: mikedeng1

Approximation and Convergence of Large Atomic Congestion Games: Equilibria of Bernoulli Congestion Games Converge to Poisson Flows Whose Means Are Wardrop Equilibria of a Limit GameResearch Paper

Motivation

Traffic models in transportation and network design come in two kinds. Nonatomic congestion games, with Wardrop equilibria, treat traffic as a continuum of infinitesimal users. Atomic games have finitely many players, each with a non-negligible effect on congestion. The Wardrop model is the one used in practice, and the usual justification is that it is the limit of atomic games as the number of players grows. Cominetti, Scarsini, Schröder and Stier-Moses (arXiv:2001.02797v7, forthcoming in Mathematics of Operations Research) make this precise in two regimes. In the first, the players' weights vanish. In the second, each player is present only with a small probability.

This mission is about the second regime, Bernoulli congestion games. Each of many potential users takes part only with a small probability, for example a commuter who may or may not travel on a given day. The limit is a Wardrop model for the mean flows, but with modified costs, and the flows themselves stay random: they are Poisson. This links Wardrop equilibria with Myerson's Poisson games (Myerson 1998).

Setting

A congestion structure consists of a finite set E\mathcal EE of resources, each with a cost ce:N∗→R+c_e:\mathbb N^*\to\mathbb R_+ce​:N∗→R+​ that is nonnegative and weakly increasing on N∗={1,2,… }\mathbb N^*=\{1,2,\dots\}N∗={1,2,…}, and a finite set T\mathcal TT of types. Each type ttt has a nonempty family St⊆2E\mathcal S_t\subseteq 2^{\mathcal E}St​⊆2E of feasible strategies.

In the nonatomic game with demands d=(dt)td=(d_t)_td=(dt​)t​, a strategy flow y=(yt,s)y=(y_{t,s})y=(yt,s​) and a load vector x=(xe)x=(x_e)x=(xe​) are feasible, (y,x)∈F(d)(y,x)\in\mathcal F(d)(y,x)∈F(d), when dt=∑s∈Styt,sd_t=\sum_{s\in\mathcal S_t}y_{t,s}dt​=∑s∈St​​yt,s​, yt,s≥0y_{t,s}\ge0yt,s​≥0 and xe=∑t∑s∈Styt,s1{e∈s}x_e=\sum_t\sum_{s\in\mathcal S_t}y_{t,s}\mathbb 1_{\{e\in s\}}xe​=∑t​∑s∈St​​yt,s​1{e∈s}​. A feasible pair is a Wardrop equilibrium for costs CeC_eCe​ when every used strategy is cheapest: y^t,s>0\hat y_{t,s}>0y^​t,s​>0 implies ∑e∈sCe(x^e)≤∑e∈s′Ce(x^e)\sum_{e\in s}C_e(\hat x_e)\le\sum_{e\in s'}C_e(\hat x_e)∑e∈s​Ce​(x^e​)≤∑e∈s′​Ce​(x^e​) for all s,s′∈Sts,s'\in\mathcal S_ts,s′∈St​.

A Bernoulli congestion game ΓB\Gamma_BΓB​ has finitely many players iii, each with a type tit_iti​ and a participation probability ui∈(0,1]u_i\in(0,1]ui​∈(0,1]. Player iii plays a mixed strategy σi\sigma_iσi​ on Sti\mathcal S_{t_i}Sti​​ and is present (Ui=1U_i=1Ui​=1) with probability uiu_iui​, independently of the other players. The random flows and loads are

Yt,s=∑i:ti=tUi1{Si=s},Xe=∑iUi,e,Ui,e=Ui1{e∈Si},Y_{t,s}=\sum_{i:t_i=t}U_i\mathbb 1_{\{S_i=s\}},\qquad X_e=\sum_iU_{i,e},\qquad U_{i,e}=U_i\mathbb 1_{\{e\in S_i\}},Yt,s​=i:ti​=t∑​Ui​1{Si​=s}​,Xe​=i∑​Ui,e​,Ui,e​=Ui​1{e∈Si​}​,

with means yt,s=∑i:ti=tuiσi(s)y_{t,s}=\sum_{i:t_i=t}u_i\sigma_i(s)yt,s​=∑i:ti​=t​ui​σi​(s) and xe=∑iuiσi,ex_e=\sum_iu_i\sigma_{i,e}xe​=∑i​ui​σi,e​. A present player on resource eee pays ce(1+Zi,e)c_e(1+Z_{i,e})ce​(1+Zi,e​), where Zi,e=∑j≠iUj,eZ_{i,e}=\sum_{j\ne i}U_{j,e}Zi,e​=∑j=i​Uj,e​ is the load of the others. A profile σ^\hat\sigmaσ^ is a Bayesian Nash equilibrium when every strategy in its support minimizes ∑e∈sEσ^[ce(1+Zi,e)]\sum_{e\in s}\mathsf E_{\hat\sigma}[c_e(1+Z_{i,e})]∑e∈s​Eσ^​[ce​(1+Zi,e​)].

The limit game Γ˘∞\breve\Gamma^\inftyΓ˘∞ is the nonatomic game with the same demands and the auxiliary costs

c˘e(x)=E[ce(1+X)],X∼Poisson(x).\breve c_e(x)=\mathsf E[c_e(1+X)],\qquad X\sim\mathrm{Poisson}(x).c˘e​(x)=E[ce​(1+X)],X∼Poisson(x).

Formalization targets

Goal: Theorem 2

Consider a sequence ΓBn\Gamma^n_BΓBn​ with ∣Nn∣→∞|\mathcal N^n|\to\infty∣Nn∣→∞, un=max⁡iuin→0u^n=\max_iu^n_i\to0un=maxi​uin​→0 and dtn=∑i:tin=tuin→dtd^n_t=\sum_{i:t^n_i=t}u^n_i\to d_tdtn​=∑i:tin​=t​uin​→dt​ (14). Assume condition (18): there are ν\nuν and dmax⁡>∑tdtd_{\max}>\sum_td_tdmax​>∑t​dt​ with E∣Δ2ce(1+V)∣≤ν\mathsf E|\Delta^2c_e(1+V)|\le\nuE∣Δ2ce​(1+V)∣≤ν for all eee, where V∼Poisson(dmax⁡)V\sim\mathrm{Poisson}(d_{\max})V∼Poisson(dmax​) and Δ2ce(k)=ce(k+2)−2ce(k+1)+ce(k)\Delta^2c_e(k)=c_e(k+2)-2c_e(k+1)+c_e(k)Δ2ce​(k)=ce​(k+2)−2ce​(k+1)+ce​(k). For every sequence of Bayesian Nash equilibria σ^n\hat\sigma^nσ^n:

(y^n,x^n) bounded,(y^,x^)=lim⁡k(y^φ(k),x^φ(k)) ⇒ (y^,x^)∈WE(Γ˘∞),(\hat y^n,\hat x^n)\ \text{bounded},\qquad (\hat y,\hat x)=\lim_k(\hat y^{\varphi(k)},\hat x^{\varphi(k)})\ \Rightarrow\ (\hat y,\hat x)\in\mathsf{WE}(\breve\Gamma^\infty),(y^​n,x^n) bounded,(y^​,x^)=klim​(y^​φ(k),x^φ(k)) ⇒ (y^​,x^)∈WE(Γ˘∞),

and along that subsequence Yt,sn→Poisson(y^t,s)Y^n_{t,s}\to\mathrm{Poisson}(\hat y_{t,s})Yt,sn​→Poisson(y^​t,s​) jointly and independently, and Xen→Poisson(x^e)X^n_e\to\mathrm{Poisson}(\hat x_e)Xen​→Poisson(x^e​), in total variation.

Milestones

The milestones are the results the proof of Theorem 2 uses, in attack order:

  • the Poisson–Poisson total-variation bound (46);
  • the Barbour–Hall bound, Theorem 9(a);
  • the limit theorem for arbitrary profiles, Proposition 1;
  • the Poisson-moment facts, Propositions 5(a)–(b);
  • the smoothness of Poisson mixtures, Proposition 6(b), and the derivative bound, Corollary 5(a);
  • the Borisov–Ruzankin bound, Theorem 9(b);
  • Lemma 1 in two parts: the regularity of c˘e\breve c_ec˘e​, and the uniform approximation (21) of a player's expected cost by c˘e(xe)\breve c_e(x_e)c˘e​(xe​), with a corrected constant (see Formalization scope).

Significance

Theorem 2 justifies a Wardrop description for large games with rare participation, and it says which Wardrop model. The costs are not cec_ece​ but their Poisson averages c˘e\breve c_ec˘e​, which account for the player's own presence and for the randomness of the others. The theorem also describes the fluctuations: flows are asymptotically independent Poisson variables, while loads are Poisson but correlated. The paper builds its approximation rates (§6) and its price-of-anarchy convergence results (§7) on the same Poisson calculus.

The result is proved in the paper. As far as is known, none of it is formalized. Mathlib has the Poisson distribution but no Poisson approximation of Bernoulli sums. The platform has nonatomic routing models and one-variable Chen–Stein bounds, but no Bernoulli players and no convergence-of-equilibria theorem. Formalizing the mission therefore produces:

  • a checked Barbour–Hall bound and Poisson–Poisson total-variation bound;
  • a calculus of Poisson mixtures (integrability transfer, smoothness, derivative bounds);
  • the first machine-checked limit theorem from atomic equilibria to Wardrop equilibria.

Difficulty

The obvious approach is to say that Bayesian Nash equilibrium inequalities pass to the limit because the expected costs converge. That step fails without control on cec_ece​: the costs are unbounded and evaluated at random loads, so convergence of the laws in total variation does not give convergence of E[ce(1+Zi,e)]\mathsf E[c_e(1+Z_{i,e})]E[ce​(1+Zi,e​)]. Condition (18) supplies the integrability, and the error must be bounded uniformly in the player and the profile. The Borisov–Ruzankin bound gives this, but at the Poisson parameter zi,ez_{i,e}zi,e​ rather than at dmax⁡d_{\max}dmax​, so integrability has to be transferred between Poisson parameters. The other difficulties are independence of the limit flows, which is a joint statement on N{(t,s)}\mathbb N^{\{(t,s)\}}N{(t,s)}, and differentiating series in their Poisson parameter up to the end point dmax⁡d_{\max}dmax​.

Formalization scope

  • Model. Players are Fin N, strategies are Finset E, and types and resources are finite types. Costs are c : E → ℕ → ℝ, nonnegative and monotone on {k≥1}\{k\ge1\}{k≥1}; ce(0)c_e(0)ce​(0) is never read. The page prints ce:N+→N+c_e:\mathbb N_+\to\mathbb N_+ce​:N+​→N+​ and ν∈N\nu\in\mathbb Nν∈N, which are read as real-valued, the weaker hypothesis. Nonempty St\mathcal S_tSt​ is made explicit.
  • Probability space. Ω=({0,1}×2E)N\Omega=(\{0,1\}\times 2^{\mathcal E})^{\mathcal N}Ω=({0,1}×2E)N carries the product weights ∏iPi(ωi)σi(si)\prod_i\mathsf P_i(\omega_i)\sigma_i(s_i)∏i​Pi​(ωi​)σi​(si​). Expectations are finite sums, and the laws of flows, loads and the flow vector are image measures. Laws are therefore computed from uuu and σ\sigmaσ, never passed in as free measures.
  • Total variation. Total variation is the published MarkovChainCLT.tvDist, the supremum over events (15). Poisson laws are Mathlib's poissonMeasure.
  • Accumulation points are limits along a strictly increasing φ\varphiφ.
  • Independence. "The Yt,sY_{t,s}Yt,s​ are independent" is formalized as total-variation convergence of the joint law of (Yt,sn)(Y^n_{t,s})(Yt,sn​) to the product of Poisson laws. On a countable space this is equivalent to the joint convergence in distribution that the paper proves.
  • Junk values. Every expectation that is a series carries summability: in (18), Propositions 5–6, Corollary 5 and Theorem 9(b). Without it, a cost such as ce(k)=k!c_e(k)=k!ce​(k)=k! would satisfy (18) through Lean's value 000 for a divergent tsum, and Theorem 2 would become false. Derivatives are taken within [0,dmax⁡][0,d_{\max}][0,dmax​]. Lemma 1 and Theorem 9 assume u<1u<1u<1 and p<1p<1p<1, so that (1−u)−2(1-u)^{-2}(1−u)−2 is not Lean's 1/0=01/0=01/0=0.
  • Correction to Lemma 1 (21). As printed, (21) is false. Take one resource with ce(j)=403(j−2)+c_e(j)=403(j-2)^+ce​(j)=403(j−2)+, ν=1\nu=1ν=1, dmax⁡=6d_{\max}=6dmax​=6 and 300 players with ui=1/100u_i=1/100ui​=1/100. Then ∣E[ce(1+Zi,e)]−c˘e(3)∣=4.1311>Λ(1/100)=4.0552|\mathsf E[c_e(1+Z_{i,e})]-\breve c_e(3)|=4.1311>\Lambda(1/100)=4.0552∣E[ce​(1+Zi,e​)]−c˘e​(3)∣=4.1311>Λ(1/100)=4.0552. The mission states (21) with Λ~(u)=νdmax⁡edmax⁡2ueu(1−u)2+uζ\tilde\Lambda(u)=\frac{\nu d_{\max}e^{d_{\max}}}{2}\frac{ue^u}{(1-u)^2}+u\zetaΛ~(u)=2νdmax​edmax​​(1−u)2ueu​+uζ, which is what the paper's proof gives once Proposition 5(a) transfers (18) to the parameter zi,ez_{i,e}zi,e​. It adds the counterexample as a separate item. Theorem 2 needs only Λ~(u)→0\tilde\Lambda(u)\to0Λ~(u)→0 and is unaffected.
  • Not trivializable. The goal cannot hold vacuously: the hypotheses are met by one resource, one type, n+1n+1n+1 players with ui=1/(n+1)u_i=1/(n+1)ui​=1/(n+1) and linear costs, for which every profile is an equilibrium (checked in Lean).
  • Contributions. Contributions toward any milestone are welcome. The Poisson-approximation and Poisson-mixture results (Theorem 9, (46), Propositions 5–6, Corollary 5) do not depend on the game and can be reused elsewhere.
  • Out of scope. Weighted games (Theorem 1), Poisson games (Theorems 3–4), rates (§6) and price of anarchy (§7) are not part of this mission.

Selected references

  • R. Cominetti, M. Scarsini, M. Schröder, N. Stier-Moses, Approximation and Convergence of Large Atomic Congestion Games, Mathematics of Operations Research (forthcoming), arXiv:2001.02797v7, 2022. https://arxiv.org/abs/2001.02797
  • A. D. Barbour, P. Hall, On the rate of Poisson convergence, Math. Proc. Cambridge Philos. Soc. 95(3), 1984. https://doi.org/10.1017/S0305004100061806
  • I. S. Borisov, P. S. Ruzankin, Poisson approximation for expectations of unbounded functions of independent random variables, Annals of Probability 30(4), 2002. https://doi.org/10.1214/aop/1039548369
  • J. A. Adell, A. Lekuona, Sharp estimates in signed Poisson approximation of Poisson mixtures, Bernoulli 11(1), 2005. https://doi.org/10.3150/bj/1110228242
  • R. B. Myerson, Population uncertainty and Poisson games, International Journal of Game Theory 27, 1998. https://doi.org/10.1007/s001820050079
  • J. G. Wardrop, Some theoretical aspects of road traffic research, Proceedings of the Institution of Civil Engineers, Part II, 1, 325–378, 1952 (no DOI given in the paper).
14 thms2 active usersReviewed
Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

To Pool or Not to Pool: Queueing Design for Large-Scale Service Systems: In Moderate Overload, Dedicated Queues Under JSQ Match Pooled Abandonment While Their Delay Probability Stays Below OneResearch Paper

Motivation

Large service systems (call centers, hospital wards, emergency departments) must decide how customers wait. In a pooled queue (PQ) all customers wait in one line served by nnn agents; in dedicated queues (DQ) each server has its own line, which is what physical layouts, server-specific information and accountability often force. Classical queueing theory says pooling is more efficient: an idle server never coexists with a waiting customer. Cao, He, Huang and Liu (Operations Research, 2020) show that when customers may abandon and join the shortest queue, the efficiency loss of dedicated queues vanishes in large systems, and that in moderate overload the dedicated design has a strictly better delay probability than the pooled one. Service-level contracts are written in terms of this probability, so the comparison bears directly on staffing and design decisions.

Setting

There are nnn servers. Customers arrive in a Poisson process of rate λ\lambdaλ; service times are exponential with mean 1/μ1/\mu1/μ; each waiting customer has an exponential patience time with mean 1/θ1/\theta1/θ and leaves when its wait exceeds it. The traffic intensity is ρ=λ/(nμ)\rho = \lambda/(n\mu)ρ=λ/(nμ).

In the DQ–JSQ system each arriving customer joins a server with the fewest customers and stays in that server's FCFS queue. Let QiQ_iQi​ be the number of servers with at least iii customers. Q=(Qi)i≥1Q = (Q_i)_{i \ge 1}Q=(Qi​)i≥1​ is a continuous-time Markov chain (genAb): an arrival joins a server with exactly iii customers when Q1=⋯=Qi=n>Qi+1Q_1 = \dots = Q_i = n > Q_{i+1}Q1​=⋯=Qi​=n>Qi+1​, and each of the Qi−Qi+1Q_i - Q_{i+1}Qi​−Qi+1​ servers with exactly iii customers loses one at rate μ+θ(i−1)\mu + \theta(i-1)μ+θ(i−1). The PQ system is the M/M/n+M (Erlang-A) queue with the same λ,μ,θ\lambda, \mu, \thetaλ,μ,θ.

The potential waiting time (PWT) WWW is the time a customer would wait for service if it never abandoned; the actual waiting time (AWT) is V=W∧RV = W \wedge RV=W∧R, with RRR the customer's patience. A customer who joins a server with iii customers has PWT distributed as Ta(i)T_a(i)Ta​(i), a sum of independent exponentials with rates μ,μ+θ,…,μ+(i−1)θ\mu, \mu + \theta, \dots, \mu + (i-1)\thetaμ,μ+θ,…,μ+(i−1)θ.

Along a sequence of systems with arrival rates λn\lambda_nλn​ and λn/(nμ)→ρ\lambda_n/(n\mu) \to \rhoλn​/(nμ)→ρ (condition (21)), the fluid constants are

q=μ(ρ−1)+θ,qˉ=⌊q⌋+1,r=q−⌊q⌋,q = \frac{\mu(\rho - 1)^+}{\theta}, \qquad \bar q = \lfloor q \rfloor + 1, \qquad r = q - \lfloor q \rfloor,q=θμ(ρ−1)+​,qˉ​=⌊q⌋+1,r=q−⌊q⌋,

and the moderate overload condition (1) is 1<ρ<1+θ/μ1 < \rho < 1 + \theta/\mu1<ρ<1+θ/μ, equivalently 0<q<10 < q < 10<q<1.

Formalization targets

Goal: Theorem 5

Under (21) and (1), with w=ln⁡(ρ)/θw = \ln(\rho)/\thetaw=ln(ρ)/θ, nine pairs of steady-state limits hold as n→∞n \to \inftyn→∞ (subscripts D and P for the two designs), among them

lim⁡PDn(Ab)=ρ−1ρ=lim⁡PPn(Ab),lim⁡PDn(De)=r(μ+θ)ρμ<1=lim⁡PPn(De),\lim P^n_D(\mathrm{Ab}) = \frac{\rho - 1}{\rho} = \lim P^n_P(\mathrm{Ab}), \qquad \lim P^n_D(\mathrm{De}) = \frac{r(\mu + \theta)}{\rho\mu} < 1 = \lim P^n_P(\mathrm{De}),limPDn​(Ab)=ρρ−1​=limPPn​(Ab),limPDn​(De)=ρμr(μ+θ)​<1=limPPn​(De), lim⁡Var(WDn)=r(μ+θ)ρμ3(2−r(μ+θ)ρμ)>0=lim⁡Var(WPn),\lim \mathrm{Var}(W^n_D) = \frac{r(\mu + \theta)}{\rho\mu^3}\Bigl(2 - \frac{r(\mu + \theta)}{\rho\mu}\Bigr) > 0 = \lim \mathrm{Var}(W^n_P),limVar(WDn​)=ρμ3r(μ+θ)​(2−ρμr(μ+θ)​)>0=limVar(WPn​),

together with the limits of the mean occupancy, mean AWT, the conditional means of WWW and VVV, and mean PWT. The goal is the full nine-part statement as printed.

Milestones

The fluid model and its invariant state q∗q^*q∗ (Theorems 1 and 2), the steady-state limit Qn(∞)/n⇒q∗Q^n(\infty)/n \Rightarrow q^*Qn(∞)/n⇒q∗ (Theorem 3(ii)), the distribution of Ta(i)T_a(i)Ta​(i) ((22), (23)), the PWT limit

Wn⇒χ Ta(qˉ)+(1−χ) Ta(⌊q⌋),P(χ=1)=r(μ+θqˉ)ρμW^n \Rightarrow \chi\,T_a(\bar q) + (1 - \chi)\,T_a(\lfloor q \rfloor), \qquad P(\chi = 1) = \frac{r(\mu + \theta\bar q)}{\rho\mu}Wn⇒χTa​(qˉ​)+(1−χ)Ta​(⌊q⌋),P(χ=1)=ρμr(μ+θqˉ​)​

(Theorem 4), its moderate-overload specialisation (Remark 3), and the pooled abandonment limit, already proved on the platform as ErlangA.Abandonment.theorem_1 (Garnett, Mandelbaum and Reiman, 2002).

Significance

The result separates two performance measures that are usually treated together. In moderate overload the two designs agree to first order in occupancy, abandonment and mean actual wait, so the capacity loss of dedicated queues is negligible; but the dedicated design lets a positive fraction 1−p1 - p1−p of customers enter service immediately, while in the pooled design almost every customer waits. The cost is fairness: delayed customers in dedicated queues wait about one full service time, and the PWT variance stays positive, whereas the pooled PWT concentrates at www. These limits drive the staffing comparison of §6 of the paper.

All statements are proved in the paper's e-companion; none is formalized. The mission produces machine-checked versions of a fluid model with reflection-type constraints, an interchange-of-limits theorem for a countable-state chain with unbounded rates, hypoexponential distributions, and many-server limits of Erlang-A waiting times (Whitt, 2004), most of which are reusable across the many-server literature.

Difficulty

The pooled system is a birth–death chain with an explicit stationary law; the dedicated system is not. Its stationary law has no closed form, so the DQ limits cannot be computed directly. The natural approach, a process-level fluid limit followed by t→∞t \to \inftyt→∞, does not by itself give the steady-state statements: the two limits must be interchanged, which needs tightness of the stationary laws and global attraction to q∗q^*q∗ (Theorem 2). The fluid model itself is a reflection system in which Uˉi\bar U_iUˉi​ may grow only when Qˉi=1\bar Q_i = 1Qˉ​i​=1, so even its well-posedness (Theorem 1) is not a standard ODE result. Finally, weak convergence of WnW^nWn (Theorem 4) does not yield convergence of means and variances without uniform integrability.

Formalization scope

  • The DQ–JSQ state space and the stationary-law predicate are the published JSQHalfinWhitt.Tightness.State (0-based: Lean q.1 i is Qi+1Q_{i+1}Qi+1​) and IsStationaryDist (probability solutions of πG=0\pi\mathcal G = 0πG=0); the chain is non-explosive, so these are its stationary laws. The arrival rate in genAb is the total rate λ\lambdaλ.
  • The PQ stationary law is the published ErlangA.Abandonment.stationaryDist; PP(Ab)P_P(\mathrm{Ab})PP​(Ab) and PP(De)P_P(\mathrm{De})PP​(De) are the published probAbandon and probWait.
  • Waiting-time laws are measures on R\mathbb RR (additive convolutions of expMeasure). The DQ PWT law is a definition: the arrival-seen mixture ∑iπ{join a server with i} L(Ta(i))\sum_i \pi\{\text{join a server with } i\}\,\mathcal L(T_a(i))∑i​π{join a server with i}L(Ta​(i)) (PASTA). Patience is an independent expMeasure θ; conditional means are ratios.
  • Fluid model: paper indices; (11)–(13), (15) for all t≥0t \ge 0t≥0 with the integral required to exist; (16) in integrated form; (14) as "Uˉi′=0\bar U_i' = 0Uˉi′​=0 almost everywhere on {Qˉi<1}\{\bar Q_i < 1\}{Qˉ​i​<1}". Uniqueness is asserted on t≥0t \ge 0t≥0 only.
  • Theorem 3(ii)'s "Qˉn(t)⇒Qˉn(∞)\bar Q^n(t) \Rightarrow \bar Q^n(\infty)Qˉ​n(t)⇒Qˉ​n(∞)" is read as existence and uniqueness of the stationary law; convergence to q∗q^*q∗ is convergence in probability in the metric ddd.
  • Added hypotheses: μ,θ,λn>0\mu, \theta, \lambda_n > 0μ,θ,λn​>0, and ρ>0\rho > 0ρ>0 for the fluid model.
  • A statement that holds because a quantity takes Lean's default value is ruled out: the goal also asserts, for every nnn, that both PWT laws are probability laws with finite second moment and that both occupancy series converge, and the DQ laws are built from the stationary law of the chain, never from the limit mixture.

Contributions are welcome on the fluid model (Theorems 1–2), the hypoexponential facts ((22), (23)), the Erlang-A many-server limits, and the DQ–JSQ interchange of limits.

Selected references

  • P. Cao, S. He, J. Huang, Y. Liu, To Pool or Not to Pool: Queueing Design for Large-Scale Service Systems, Operations Research, Articles in Advance, 2020. https://doi.org/10.1287/opre.2019.1976
  • O. Garnett, A. Mandelbaum, M. Reiman, Designing a Call Center with Impatient Customers, Manufacturing & Service Operations Management 4(3), 2002. https://doi.org/10.1287/msom.4.3.208.7753
  • W. Whitt, Efficiency-Driven Heavy-Traffic Approximations for Many-Server Queues with Abandonments, Management Science 50(10), 2004. https://doi.org/10.1287/mnsc.1040.0279
  • A. Braverman, Steady-State Analysis of the Join-the-Shortest-Queue Model in the Halfin–Whitt Regime, Mathematics of Operations Research 45(3), 2020. https://doi.org/10.1287/moor.2019.1023
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Algorithmic Game TheoryEconomicsOperations Research·Captain: mikedeng1

Competitive Equilibrium and Trading Networks: A Network Flow Approach: Every Chain-Stable Outcome Is Supported by Competitive Equilibrium PricesResearch Paper

Motivation

Markets in which goods pass through intermediaries (supply chains, interbank lending, procurement networks) do not fit the two-sided buyer–seller models of matching theory: one firm can buy inputs on some trades and sell outputs on others. Trading networks model such markets as a directed graph of possible bilateral trades. Hatfield, Kominers, Nichifor, Ostrovsky and Westkamp (J. Polit. Econ. 2013) showed that when every agent's preferences are fully substitutable, competitive equilibria exist and several notions of stability coincide with competitive equilibrium. Stability notions describe outcomes that agents cannot undo by renegotiating, and competitive equilibrium describes outcomes supported by prices. Knowing that the two coincide matters for market design: a decentralised market that only has to rule out simple deviations already achieves a price-supported, efficient allocation.

Candogan, Epitropou and Vohra (Operations Research, 2021; working paper version IHS Economics Series 323, 2016) rederived these results from the theory of M-convex submodular flows (Murota, Discrete Convex Analysis, SIAM 2003). Full substitutability is equivalent to M♮-concavity of the valuations, and efficient outcomes correspond to optimal flows.

Timeline:

  • 1982, 1999: Kelso–Crawford and Gul–Stacchetti establish existence of competitive equilibrium with gross substitutes in two-sided markets.
  • 2003: Fujishige–Yang and Murota–Tamura identify gross substitutes with M♮-concavity (see Murota's book).
  • 2005, 2008: Hatfield–Milgrom and Ostrovsky extend matching with contracts and supply-chain stability.
  • 2013: Hatfield et al. prove existence, the welfare theorems and the stability equivalences in trading networks.
  • 2016/2021: Candogan, Epitropou and Vohra reprove them through network flows, introduce chain stability as the weakest notion, and show it already implies competitive equilibrium.

Setting

A trading network is a finite directed multigraph G=(N,E)G=(N,E)G=(N,E). Each vertex i∈Ni\in Ni∈N is an agent, each arc e∈Ee\in Ee∈E a possible trade, with seller e+e^+e+ and buyer e−e^-e−. Write δ+(i)\delta^+(i)δ+(i) for the trades iii sells, δ−(i)\delta^-(i)δ−(i) for the trades iii buys, and δ(i)=δ+(i)∪δ−(i)\delta(i)=\delta^+(i)\cup\delta^-(i)δ(i)=δ+(i)∪δ−(i). An outcome is a set of trades X⊆EX\subseteq EX⊆E, and a price vector is p∈REp\in\mathbb R^Ep∈RE. Agent iii has a valuation wi:2δ(i)→Rw_i:2^{\delta(i)}\to\mathbb Rwi​:2δ(i)→R and utility

ui(S,p)=wi(S)+∑e∈S∩δ+(i)pe−∑e∈S∩δ−(i)pe.u_i(S,p)=w_i(S)+\sum_{e\in S\cap\delta^+(i)}p_e-\sum_{e\in S\cap\delta^-(i)}p_e .ui​(S,p)=wi​(S)+e∈S∩δ+(i)∑​pe​−e∈S∩δ−(i)∑​pe​.

For T⊆ET\subseteq ET⊆E, the demand restricted to TTT is Di(pT)=arg⁡max⁡{ui(Y,p):Y⊆T∩δ(i)}D_i(p^T)=\arg\max\{u_i(Y,p):Y\subseteq T\cap\delta(i)\}Di​(pT)=argmax{ui​(Y,p):Y⊆T∩δ(i)}; with T=ET=ET=E it is the ordinary demand Di(p)D_i(p)Di​(p).

  • (X,p)(X,p)(X,p) is a competitive equilibrium if X∩δ(i)∈Di(p)X\cap\delta(i)\in D_i(p)X∩δ(i)∈Di​(p) for every iii (Definition 2.1).
  • XXX is efficient if it maximizes the welfare ∑iwi(X∩δ(i))\sum_i w_i(X\cap\delta(i))∑i​wi​(X∩δ(i)) (Definition 2.2).
  • Represent S⊆δ(i)S\subseteq\delta(i)S⊆δ(i) by the vector with entry +1+1+1 on sold trades and −1-1−1 on bought trades, and set wi=−∞w_i=-\inftywi​=−∞ elsewhere on Zδ(i)\mathbb Z^{\delta(i)}Zδ(i). The standing assumption is that every wiw_iwi​ is M♮-concave in this representation (§3.2).
  • (X,pX)(X,p^X)(X,pX) is individually rational if X∩δ(i)∈Di(pX)X\cap\delta(i)\in D_i(p^X)X∩δ(i)∈Di​(pX), the demand restricted to XXX, for every iii.
  • A chain is a nonempty set of distinct trades e1,…,eme_1,\dots,e_me1​,…,em​ with ek−=ek+1+e_k^-=e_{k+1}^+ek−​=ek+1+​. A chain ZZZ with prices pZp^ZpZ blocks (X,pX)(X,p^X)(X,pX) if Z∩X=∅Z\cap X=\emptysetZ∩X=∅ and, for every agent iii involved in ZZZ, every Yi∈Di(pZ∪X)Y^i\in D_i(p^{Z\cup X})Yi∈Di​(pZ∪X) contains Z∩δ(i)Z\cap\delta(i)Z∩δ(i). The prices pZ∪Xp^{Z\cup X}pZ∪X combine pXp^XpX and pZp^ZpZ.
  • (X,pX)(X,p^X)(X,pX) is chain stable if it is individually rational and has no blocking chain (Definition 5.3).
  • The contraction GXG^XGX with respect to (X,pX)(X,p^X)(X,pX) has trades E∖XE\setminus XE∖X and valuations w^i(S)=max⁡Y⊆X∩δ(i)[wi(S∪Y)+∑e∈Y∩δ+(i)peX−∑e∈Y∩δ−(i)peX]\hat w_i(S)=\max_{Y\subseteq X\cap\delta(i)}[w_i(S\cup Y)+\sum_{e\in Y\cap\delta^+(i)}p^X_e-\sum_{e\in Y\cap\delta^-(i)}p^X_e]w^i​(S)=maxY⊆X∩δ(i)​[wi​(S∪Y)+∑e∈Y∩δ+(i)​peX​−∑e∈Y∩δ−(i)​peX​] (eq. (6)).

Formalization targets

Goal: Theorem 5.8

If (X,pX)(X,p^X)(X,pX) is chain stable, then there is p∈REp\in\mathbb R^Ep∈RE with

(X,p) a competitive equilibrium andpe=peX  for all e∈X.(X,p)\ \text{a competitive equilibrium and}\quad p_e=p^X_e\ \ \text{for all }e\in X.(X,p) a competitive equilibrium andpe​=peX​  for all e∈X.

Milestones

  1. The contraction's valuations w^i\hat w_iw^i​ are M♮-concave (eq. (6), PDF p. 16).
  2. Theorem 4.1: a competitive equilibrium exists.
  3. Theorem 4.3: for any competitive equilibrium (X,p)(X,p)(X,p) and efficient X′X'X′, (X′,p)(X',p)(X′,p) is a competitive equilibrium.
  4. Lemma 5.5: if ∅\emptyset∅ is inefficient, some chain ZZZ has ∑iwi(∅)<∑iwi(Z∩δ(i))\sum_i w_i(\emptyset)<\sum_i w_i(Z\cap\delta(i))∑i​wi​(∅)<∑i​wi​(Z∩δ(i)).
  5. Corollary 5.6: a minimal welfare-improving set of trades is a chain, and with suitable prices it is a blocking chain of ∅\emptyset∅.
  6. Proof of Theorem 5.8: a blocking chain of ∅\emptyset∅ in GXG^XGX blocks (X,pX)(X,p^X)(X,pX) in GGG.
  7. Proof of Theorem 5.8: if (X,pX)(X,p^X)(X,pX) is individually rational and (∅,p^)(\emptyset,\hat p)(∅,p^​) is a competitive equilibrium of GXG^XGX, then (X,(pX,p^))(X,(p^X,\hat p))(X,(pX,p^​)) is a competitive equilibrium of GGG.

Significance

Theorem 5.8 closes the hierarchy of solution concepts in trading networks. Combined with Theorem 5.7 (competitive equilibria are strongly stable, hence chain stable), every notion between chain stability and competitive equilibrium describes the same outcomes. Since chain stability is the weakest of them, it is enough to check deviations along chains to certify an outcome as price supported and, by the first welfare theorem, efficient. The result is also the basis of the paper's algorithmic section, which finds blocking chains as negative cycles.

The theorem is proved, in Hatfield et al. (2013) and again in this paper. No part of it is formalized on the platform. The mission produces a machine-checked trading-network model with M♮-concave valuations, the existence and second welfare theorems for it, and the chain-stability equivalence. The M♮-concavity definition reused here comes from the platform's formalization of Murota's book.

Difficulty

The lifting steps (milestones 6 and 7) are bookkeeping. The substance is in two places. First, Theorems 4.1 and 4.3 and Lemma 5.5 are where substitutability is used: existence of equilibrium prices is a duality statement for a nonlinear integer program, and Lemma 5.5 asserts that an improvement over no trade can always be found with the special shape of a chain. Neither follows from finite enumeration. Without substitutability both fail: with complementary valuations an inefficient no-trade outcome can need a non-chain set of trades to improve on it, and equilibria need not exist. Second, milestone 1 requires closure of M♮-concavity under adding a linear function and maximizing out a group of coordinates (projection). This closure is standard in Murota's book but is not on the platform.

Formalization scope

  • Agents and trades are finite types with decidable equality. Valuations are real-valued functions on Finset E, evaluated only on subsets of δ(i)\delta(i)δ(i). Prices are functions E → ℝ.
  • M♮-concavity is the published definition DiscreteConvex.EconomicEquilibrium.MNaturalConcave (values in R∪{−∞}\mathbb R\cup\{-\infty\}R∪{−∞}, exchange axiom on the effective domain), applied to the signed representation +1+1+1 sold, −1-1−1 bought, −∞-\infty−∞ off the box {0,−1}δ−(i)×{0,1}δ+(i)\{0,-1\}^{\delta^-(i)}\times\{0,1\}^{\delta^+(i)}{0,−1}δ−(i)×{0,1}δ+(i). The paper's printed axiom on PDF p. 8 has f(x+χu−χv)f(x+\chi_u-\chi_v)f(x+χu​−χv​) in its last term, a typo for f(y+χu−χv)f(y+\chi_u-\chi_v)f(y+χu​−χv​), which is what the definition uses.
  • Added hypothesis: every trade has distinct seller and buyer. This is a reading of §2, and it is needed for the signed representation to be well defined.
  • The word "feasible" in Definition 5.3 is dropped, since real-valued valuations make every set of trades feasible. Chains are nonempty lists without repetition, with buyer of each trade equal to seller of the next, and may close into cycles. The contraction's trades are the subtype {e // e ∉ X}.
  • Ruled out: blocking with "some demanded set contains Z∩δ(i)Z\cap\delta(i)Z∩δ(i)" instead of "every", blocking by arbitrary sets instead of chains, or chain stability without individual rationality. Each of these changes the goal into a different statement. The goal keeps the page's quantifiers.
  • Infrastructure needed: closure of M♮-concavity under linear perturbation and projection, an M-convex submodular flow optimality criterion or a direct duality argument, and the exchange properties of M♮-concave set functions. These are reusable for any market with gross-substitutes valuations. Proofs of any milestone, and alternative proofs of Theorems 4.1 and 4.3 that avoid flows, are welcome.

Selected references

  • O. Candogan, M. Epitropou, R. V. Vohra, Competitive Equilibrium and Trading Networks: A Network Flow Approach, IHS Economics Series Working Paper 323, 2016 (journal version: Operations Research, 2021). https://irihs.ihs.ac.at/id/eprint/4027
  • J. W. Hatfield, S. D. Kominers, A. Nichifor, M. Ostrovsky, A. Westkamp, Stability and Competitive Equilibrium in Trading Networks, Journal of Political Economy 121(5), 2013. https://doi.org/10.1086/673402
  • K. Murota, Discrete Convex Analysis, SIAM, 2003. https://doi.org/10.1137/1.9780898718508
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Algorithmic Game TheoryGraph TheoryProbability·Captain: mikedeng1

Pure Nash Equilibria and Best-Response Dynamics in Random Games: Best-Response Dynamics Reaches a Pure Nash Equilibrium for All Large N When the Tie Probability Is SmallResearch Paper

Why random games, and why ties

A pure Nash equilibrium (PNE) of a game is a strategy profile from which no player gains by a unilateral deviation. Unlike mixed equilibria, pure equilibria need not exist, and even when they do they can be hard to find: computing an equilibrium is PPAD-complete in general (Daskalakis, Goldberg & Papadimitriou 2009). The simplest learning procedure that searches for a PNE is best-response dynamics (BRD): repeatedly let some player who can strictly improve switch strategy. BRD is guaranteed to stop at a PNE only for special classes such as potential games (Monderer & Shapley 1996); in general it can wander forever inside a trap, the "sink equilibrium" of Goemans, Mirrokni & Vetta 2005.

A way to measure how often these failures occur is to draw the payoffs at random. The classical line of work, from Goldman (1957) and Goldberg, Goldman & Newman (1968) to Powers (1990) and Rinott & Scarsini 2000, studies the number of PNE when the payoffs are i.i.d. with a continuous law, so that ties have probability zero. The number of PNE then has mean one and is asymptotically Poisson. Amiet, Collevecchio, Scarsini & Zhong (2021) drop the continuity assumption. They show that the single parameter governing the asymptotics is the tie probability α\alphaα, and they relate the game to bond percolation on the hypercube. Their headline result is that, for NNN binary players and small positive α\alphaα, BRD started from a fixed profile reaches a PNE with a failure probability that is summable in NNN.

Setting

There are NNN players [N]={1,…,N}[N]=\{1,\dots,N\}[N]={1,…,N}, each with strategies {0,1}\{0,1\}{0,1}. A profile is s∈{0,1}N\boldsymbol s\in\{0,1\}^Ns∈{0,1}N, and 0=(0,…,0)\mathbf 0=(0,\dots,0)0=(0,…,0). In the random game ΞN\Xi_NΞN​ the payoff of player iii at profile s\boldsymbol ss is ZisZ^{\boldsymbol s}_iZis​, and the family (Zis)i,s(Z^{\boldsymbol s}_i)_{i,\boldsymbol s}(Zis​)i,s​ is i.i.d. with a law μ\muμ on R\mathbb RR that may have atoms. With Z1,Z2Z_1,Z_2Z1​,Z2​ i.i.d. of law μ\muμ,

α=P(Z1=Z2),β=P(Z1<Z2)=1−α2.\alpha=\mathsf P(Z_1=Z_2),\qquad \beta=\mathsf P(Z_1<Z_2)=\tfrac{1-\alpha}{2}.α=P(Z1​=Z2​),β=P(Z1​<Z2​)=21−α​.

Two profiles that differ only in coordinate iii are joined by an edge of the hypercube HN\mathscr H_NHN​. The edge is oriented from s\boldsymbol ss to t\boldsymbol tt when Zis<ZitZ^{\boldsymbol s}_i<Z^{\boldsymbol t}_iZis​<Zit​, and is unoriented when the two payoffs tie; this gives the random partially oriented hypercube H⃗Nβ\vec{\mathscr H}^\beta_NHNβ​. The set D(s)\mathscr D(\boldsymbol s)D(s) of strictly profitable deviations consists of the heads of the arrows leaving s\boldsymbol ss, and s\boldsymbol ss is a PNE iff D(s)=∅\mathscr D(\boldsymbol s)=\varnothingD(s)=∅. BRD, BR(N)\mathsf{BR}^{(N)}BR(N), starts at 0\mathbf 00 and at each step moves to a uniformly random element of D\mathscr DD of the current profile. It converges to a PNE if D(BRk(N))=∅\mathscr D(\mathsf{BR}^{(N)}_k)=\varnothingD(BRk(N)​)=∅ for all large kkk.

A profile is accessible from s\boldsymbol ss if an oriented path leads to it, and L⃗Nβ,0\vec{\mathscr L}^{\beta,\mathbf 0}_NLNβ,0​ is the set of profiles accessible from 0\mathbf 00. A trap is a set of at least two profiles that is strongly connected and that no oriented path leaves. In bond percolation BNβ\mathscr B^\beta_NBNβ​ each edge of HN\mathscr H_NHN​ is open independently with probability β\betaβ. Its giant component is the largest open cluster, and its fragment MNβ\mathscr M^\beta_NMNβ​ is the set of vertices outside the giant component.

Formalization targets

Goal: Theorem 3.4

If α>0\alpha>0α>0 and ⌊−1/log⁡2(1/2+α/2)⌋≤3\lfloor -1/\log_2(1/2+\alpha/2)\rfloor\le 3⌊−1/log2​(1/2+α/2)⌋≤3 (equivalently 0<α<23/4−1≈0.680<\alpha<2^{3/4}-1\approx0.680<α<23/4−1≈0.68), then

∑N=1∞P(BR(N) does not converge to a PNE)<∞.\sum_{N=1}^\infty \mathsf P\bigl(\mathsf{BR}^{(N)}\text{ does not converge to a PNE}\bigr)<\infty .N=1∑∞​P(BR(N) does not converge to a PNE)<∞.

Milestones

  • Proposition 4.1: a coupling under which the open cluster of 0\mathbf 00 in a percolation BNβ\mathscr B^\beta_NBNβ​ equals L⃗Nβ,0\vec{\mathscr L}^{\beta,\mathbf 0}_NLNβ,0​.
  • Lemma 4.3: concentration of card(MNβ)\mathsf{card}(\mathscr M^\beta_N)card(MNβ​) around (2(1−β))N(1+O(N(1−β)N))(2(1-\beta))^N(1+O(N(1-\beta)^N))(2(1−β))N(1+O(N(1−β)N)), summably in NNN, for β∈(0,1/2)\beta\in(0,1/2)β∈(0,1/2).
  • Proposition 4.2, form (4.7): ∑NP(0∉giant component)<∞\sum_N\mathsf P(\mathbf 0\notin\text{giant component})<\infty∑N​P(0∈/giant component)<∞ for β∈(0,1/2]\beta\in(0,1/2]β∈(0,1/2].
  • Lemma 4.4: for some δˉ>0\bar\delta>0δˉ>0 and all δ<δˉ\delta<\bar\deltaδ<δˉ, summably in NNN, no Hamming ball of radius ⌈δN⌉\lceil\delta N\rceil⌈δN⌉ contains more than mβ=⌊1/(−log⁡2(1−β))⌋m_\beta=\lfloor 1/(-\log_2(1-\beta))\rfloormβ​=⌊1/(−log2​(1−β))⌋ profiles outside L⃗Nβ,0\vec{\mathscr L}^{\beta,\mathbf 0}_NLNβ,0​.
  • (5.8): ρTV(card(PNE(ΞN)),Poisson(2N(1−β)N))≤K1,αN(1−β)N\rho_{\mathsf{TV}}(\mathsf{card}(\mathsf{PNE}(\Xi_N)),\mathsf{Poisson}(2^N(1-\beta)^N))\le K_{1,\alpha}N(1-\beta)^NρTV​(card(PNE(ΞN​)),Poisson(2N(1−β)N))≤K1,α​N(1−β)N.
  • Theorem 2.3: a central limit theorem for card(PNE(ΞN))\mathsf{card}(\mathsf{PNE}(\Xi_N))card(PNE(ΞN​)), centred at (1+α)N(1+\alpha)^N(1+α)N and scaled by (1+α)N/2(1+\alpha)^{N/2}(1+α)N/2, with Kolmogorov error KαNmax⁡((1+α)/2,(1+α)−1/2)NK_\alpha N\max((1+\alpha)/2,(1+\alpha)^{-1/2})^NKα​Nmax((1+α)/2,(1+α)−1/2)N.
  • (5.13): ∑NP(card(PNE(ΞN))<(1+α)N−(1+ε)N(1+α)N/2)<∞\sum_N\mathsf P(\mathsf{card}(\mathsf{PNE}(\Xi_N))<(1+\alpha)^N-(1+\varepsilon)^N(1+\alpha)^{N/2})<\infty∑N​P(card(PNE(ΞN​))<(1+α)N−(1+ε)N(1+α)N/2)<∞ whenever 1+ε<(1+α)1/21+\varepsilon<(1+\alpha)^{1/2}1+ε<(1+α)1/2.
  • Trap reduction: if there is no trap, BRD converges to a PNE with probability one.
  • (5.29): summably in NNN, L⃗Nβ,0\vec{\mathscr L}^{\beta,\mathbf 0}_NLNβ,0​ contains a PNE.
  • (5.24): summably in NNN, H⃗Nβ\vec{\mathscr H}^\beta_NHNβ​ contains no trap.

Significance

The theorem shows that the failure of BRD described in the game-theory literature, cycling in a trap, is asymptotically rare when payoffs tie with small positive probability. By Borel–Cantelli there is then a finite random N∗N^*N∗ beyond which BRD always reaches a PNE. The threshold 23/4−12^{3/4}-123/4−1 is where the expected number of trapping 4-cycles stops being summable. The percolation coupling (Proposition 4.1) is the paper's new tool: it turns questions about accessibility under BRD into questions about clusters of the hypercube, where the results of McDiarmid, Scott & Withers apply. The same coupling yields the paper's phase transition at α=1/2\alpha=1/2α=1/2 for the accessibility of all PNE (Theorem 3.3, not part of this mission).

The paper results are proved on paper, except for one gap. The paper derives (5.8), and through it Theorem 2.3, from the claim that the number of PNE has the same law as the number of isolated vertices of the percolation. That identity is false: the two laws already differ at N=2N=2N=2. Statement (5.8) and Theorem 2.3 are nevertheless true; (5.8) follows from the Chen–Stein method (Arratia, Goldstein & Gordon 1989). Both are posed here as printed, and a correct proof of them is a contribution in its own right. None of these results has a machine-checked proof.

Difficulty

The obvious argument is a first-moment bound: count expected traps and sum over NNN. The 4-cycles that are traps alone have expected number of order N2((1+α)4/8)NN^2((1+\alpha)^4/8)^NN2((1+α)4/8)N, summable exactly when α<23/4−1\alpha<2^{3/4}-1α<23/4−1, but traps can have any size up to 2N2^N2N, and the number of candidate vertex sets grows far faster than any single-shape first moment decays. Controlling traps of every size requires global information about which profiles BRD can reach from 0\mathbf 00, and about how the exponentially many PNE sit relative to that set. That information comes from the component structure of percolation on the hypercube at a fixed edge probability, a deep theory (McDiarmid–Scott–Withers) of which nothing is in Mathlib.

Formalization scope

Players are Fin N and profiles are Fin N → Bool; the payoffs of ΞN\Xi_NΞN​ live on Fin N → Profile N → ℝ with the product law gameMeasure μ N. Each NNN has its own probability space; every target is a per-NNN bound or a sum over NNN of per-NNN probabilities, so no coupling across NNN is needed. Sums of probabilities are ∑' in ℝ≥0∞ and are required to be ≠ ⊤. The BRD chain is built from the PMF iterates of its one-step kernel. At a PNE, where the page leaves the step undefined, the chain stays put. The probability of non-convergence is then 1−sup⁡kP(BRk(N)∈PNE)1-\sup_k\mathsf P(\mathsf{BR}^{(N)}_k\in\mathsf{PNE})1−supk​P(BRk(N)​∈PNE), averaged with a lower Lebesgue integral. Percolation configurations are Edge N → Bool under a product of Bernoulli laws. "0\mathbf 00 is not in the giant component" is read conservatively: on a tie for the largest cluster, 0\mathbf 00 counts as outside. Theorem 2.3 and (5.8) assume N≥1N\ge 1N≥1, as the page's [N][N][N] does (both fail at N=0N=0N=0). Their constants are uniform over all payoff laws with the given α\alphaα. Lemma 4.3's O(⋅)O(\cdot)O(⋅) is two-sided.

Trivializing encodings are excluded: no probability is a Bochner integral of a possibly non-measurable integrand, convergence is not defined by fiat, and a trap needs at least two vertices and closedness, so a single PNE is not a trap. The hypothesis (3.8) is kept literally. At α=1\alpha=1α=1 it holds through Lean's −1/0=0-1/0=0−1/0=0, but the goal is then true for a genuine reason (every profile is a PNE).

A complete development needs the theory of finite Markov chains (absorption), Poisson approximation by Chen–Stein, a Berry–Esseen bound, and the component structure of percolation on the hypercube. The last of these is reusable well beyond this mission. Contributions of independent pieces, such as the trap reduction or the first-moment bounds, are welcome.

Selected references

  • B. Amiet, A. Collevecchio, M. Scarsini, Z. Zhong, Pure Nash Equilibria and Best-Response Dynamics in Random Games, Mathematics of Operations Research 46(4), 2021; arXiv:1905.10758v4. https://arxiv.org/abs/1905.10758
  • C. McDiarmid, A. Scott, P. Withers, The component structure of dense random subgraphs of the hypercube, arXiv:1806.06433, 2018 (cited by the paper as 2020). https://arxiv.org/abs/1806.06433
  • R. Arratia, L. Goldstein, L. Gordon, Two moments suffice for Poisson approximations: the Chen–Stein method, Annals of Probability 17(1), 1989. https://doi.org/10.1214/aop/1176991491
  • Y. Rinott, M. Scarsini, On the number of pure strategy Nash equilibria in random games, Games and Economic Behavior 33(2), 2000. https://doi.org/10.1006/game.1999.0775
  • M. Goemans, V. Mirrokni, A. Vetta, Sink equilibria and convergence, FOCS 2005. https://doi.org/10.1109/SFCS.2005.68
  • D. Monderer, L. S. Shapley, Potential games, Games and Economic Behavior 14(1), 1996. https://doi.org/10.1006/game.1996.0044
15 thms2 active usersReviewed
Bandit AlgorithmsMachine LearningOperations Research+1·Captain: mikedeng1

Contextual Bandits with Cross-Learning: UCB1.CL Has Expected Regret O(Kκ̄ log T/Δ*) and O(√(κ̄KT log T)) with Stochastic Rewards and Adversarial ContextsResearch Paper

Motivation

In a contextual bandit a learner plays TTT rounds; in round ttt it observes a context ctc_tct​, pulls one of KKK arms and receives the reward of that arm in that context. In many applications the learner also learns what the pulled arm would have paid in other contexts. The motivating example of Balseiro, Golrezaei, Mahdian, Mirrokni and Schneider (arXiv:1809.09582) is a bidder in repeated first-price auctions: the context is the bidder's private value, the arm is the bid, and after the auction the bidder can compute the utility the same bid would have earned at every other value. Similar cross-learning structure appears in dynamic pricing with variable costs and in multi-armed bandits with side information about contexts.

Treating each context as a separate bandit problem costs regret of order CKT\sqrt{CKT}CKT​, which is useless when the number of contexts CCC is large or continuous. The paper shows that cross-learning removes, or reduces, this dependence on CCC. For stochastic rewards it analyses UCB1.CL, a version of UCB1 that updates its statistics in every context it learns about, and bounds its regret by a graph quantity, the clique covering number of the cross-learning graphs. The authors describe this analysis as the main technical contribution of the paper (p. 5).

Setting

There are arms i∈[K]i\in[K]i∈[K] and contexts c∈[C]c\in[C]c∈[C]. On a probability space, the reward ri,t(c)∈[0,1]r_{i,t}(c)\in[0,1]ri,t​(c)∈[0,1] of arm iii in context ccc at round ttt is random; the reward vectors of different rounds are independent (rewards may be correlated within a round), and ri,t(c)r_{i,t}(c)ri,t​(c) has the same law Fi(c)\mathcal F_i(c)Fi​(c), with mean μi(c)\mu_i(c)μi​(c), in every round. The best mean in context ccc is μ⋆(c)=max⁡iμi(c)\mu^\star(c)=\max_i\mu_i(c)μ⋆(c)=maxi​μi​(c) and the gap of arm iii is Δi(c)=μ⋆(c)−μi(c)\Delta_i(c)=\mu^\star(c)-\mu_i(c)Δi​(c)=μ⋆(c)−μi​(c). The contexts c1,c2,…c_1,c_2,\dotsc1​,c2​,… form an arbitrary sequence fixed before the game (adversarial, oblivious contexts).

For each arm iii a directed cross-learning (CL) graph GiG_iGi​ on the contexts is known: an edge c→c′c\to c'c→c′ means that pulling arm iii in context ccc reveals ri,t(c′)r_{i,t}(c')ri,t​(c′). Every GiG_iGi​ contains all self-loops. The clique covering number κ(G)\kappa(G)κ(G) is the least number of subcliques (sets with an edge u→vu\to vu→v between any two members) that partition the contexts; κˉ=1K∑iκ(Gi)\bar\kappa=\frac1K\sum_i\kappa(G_i)κˉ=K1​∑i​κ(Gi​).

UCB1.CL keeps, for every arm iii and context ccc, the number τi,t(c)\tau_{i,t}(c)τi,t​(c) of rewards of arm iii in context ccc observed before round ttt and their sum σi,t(c)\sigma_{i,t}(c)σi,t​(c). In round ttt it pulls an arm ItI_tIt​ maximising

σi,t(ct)τi,t(ct)+2log⁡Tτi,t(ct)(+∞ if τi,t(ct)=0),\frac{\sigma_{i,t}(c_t)}{\tau_{i,t}(c_t)}+\sqrt{\frac{2\log T}{\tau_{i,t}(c_t)}}\qquad(+\infty\text{ if }\tau_{i,t}(c_t)=0),τi,t​(ct​)σi,t​(ct​)​+τi,t​(ct​)2logT​​(+∞ if τi,t​(ct​)=0),

breaking ties arbitrarily. The pseudo-regret is Reg=∑t=1TΔIt(ct)\mathrm{Reg}=\sum_{t=1}^T\Delta_{I_t}(c_t)Reg=∑t=1T​ΔIt​​(ct​).

Formalization targets

Goal: Theorem 1 (p. 17)

For every T≥2T\ge2T≥2, every context sequence and every UCB1.CL arm process,

E[Reg]≤16log⁡TΔ∗∑i=1Kκ(Gi)+Kπ23for every 0<Δ∗≤min⁡{Δi(c):Δi(c)>0},\mathbb E[\mathrm{Reg}]\le\frac{16\log T}{\Delta^*}\sum_{i=1}^K\kappa(G_i)+\frac{K\pi^2}{3}\quad\text{for every }0<\Delta^*\le\min\{\Delta_i(c):\Delta_i(c)>0\},E[Reg]≤Δ∗16logT​i=1∑K​κ(Gi​)+3Kπ2​for every 0<Δ∗≤min{Δi​(c):Δi​(c)>0}, E[Reg]≤17Tlog⁡T∑i=1Kκ(Gi)+Kπ23.\mathbb E[\mathrm{Reg}]\le17\sqrt{T\log T\sum_{i=1}^K\kappa(G_i)}+\frac{K\pi^2}{3}.E[Reg]≤17TlogTi=1∑K​κ(Gi​)​+3Kπ2​.

These are the paper's O(Kκˉlog⁡T/Δ∗)O(K\bar\kappa\log T/\Delta^*)O(KκˉlogT/Δ∗) and O(κˉKTlog⁡T)O(\sqrt{\bar\kappa KT\log T})O(κˉKTlogT​) with the constants of its proof.

Milestones

  1. Eq. (4) (p. 19): along any arm sequence, for contexts of a set SSS ordered by decreasing positive gap, Xi(c(1))+⋯+Xi(c(j))≤mi(c(j))+1X_i(c_{(1)})+\dots+X_i(c_{(j)})\le m_i(c_{(j)})+1Xi​(c(1)​)+⋯+Xi​(c(j)​)≤mi​(c(j)​)+1, where mi(c)=8log⁡T/Δi(c)2m_i(c)=8\log T/\Delta_i(c)^2mi​(c)=8logT/Δi​(c)2.
  2. Lemma 3 (p. 18): for any arm sequence, RegPre≤16log⁡T∑iκ(Gi)/Δmin⁡\mathrm{Reg}_{\mathrm{Pre}}\le16\log T\sum_i\kappa(G_i)/\Delta_{\min}RegPre​≤16logT∑i​κ(Gi​)/Δmin​.
  3. Hoeffding step (p. 46): the mean xˉi,n(c)\bar x_{i,n}(c)xˉi,n​(c) of the first nnn observed rewards deviates from μi(c)\mu_i(c)μi​(c) by 2log⁡T/n\sqrt{2\log T/n}2logT/n​ with probability at most T−4T^{-4}T−4 in each direction.
  4. Per-round bound (p. 46): Pr⁡[It=i, τi,t(ct)>mi(ct)]≤2t−2\Pr[I_t=i,\ \tau_{i,t}(c_t)>m_i(c_t)]\le2t^{-2}Pr[It​=i, τi,t​(ct​)>mi​(ct​)]≤2t−2 for Δi(ct)>0\Delta_i(c_t)>0Δi​(ct​)>0.
  5. Lemma 4 (p. 20): E[RegPost]≤Kπ2/3\mathbb E[\mathrm{Reg}_{\mathrm{Post}}]\le K\pi^2/3E[RegPost​]≤Kπ2/3.

Significance

With complete cross-learning (κ(Gi)=1\kappa(G_i)=1κ(Gi​)=1) Theorem 1 gives regret O(KTlog⁡T)O(\sqrt{KT\log T})O(KTlogT​), independent of the number of contexts; with no cross-learning (κ(Gi)=C\kappa(G_i)=Cκ(Gi​)=C) it recovers the O(KCTlog⁡T)O(\sqrt{KCT\log T})O(KCTlogT​) of independent UCB1 instances; in between, the clique covering number interpolates. The bound applies to bidding in first-price auctions with discretised values and bids, and the paper's lower bounds (Theorems 5–6) show that a dependence on graph invariants of the CL graphs cannot be removed in general.

The result is proved in the paper; nothing about it is formalized. A machine-checked proof would add to the platform its first contextual bandit with cross-learning, its first regret bound in terms of a clique cover, and a Hoeffding inequality for rewards sampled at rounds chosen adaptively by an algorithm, which is reusable in every UCB-type analysis. The formal statements also record corrected versions of four printed slips in the proof (listed under Formalization scope).

Difficulty

The standard UCB1 analysis counts, per arm and context, the pulls made before the arm has been observed mi(c)m_i(c)mi​(c) times, and pays Δi(c) mi(c)\Delta_i(c)\,m_i(c)Δi​(c)mi​(c) for each context. Summed over contexts this gives a bound linear in CCC, which is exactly what cross-learning should avoid. The difficulty is that an observation of arm iii in context ccc may come from a pull in another context, so the per-context counts are coupled through the CL graph and do not decrease independently. Lemma 3 handles this through a linear system over the cliques of a minimum clique cover, and Lemma 4 needs concentration for samples collected at random times determined by the algorithm itself.

Formalization scope

Arms and contexts are Fin K and Fin C with K,C≥1K,C\ge1K,C≥1. The reward process R t ω i c is defined for all t∈Nt\in\mathbb Nt∈N; the hypotheses are measurability, independence of the round vectors (iIndepFun), values in [0,1][0,1][0,1], and identical distribution of each coordinate across rounds. Contexts are a deterministic sequence ctx : ℕ → Fin C. G i c c' is the edge c→c′c\to c'c→c′ of GiG_iGi​, with all self-loops assumed. Rounds are 0-based in Lean (Lean's round ttt is the paper's round t+1t+1t+1). The UCB index is EReal-valued, +∞+\infty+∞ at τ=0\tau=0τ=0; the logarithm is natural and the algorithm knows TTT.

The selection rule is a property of the arm sequence: in every round t<Tt<Tt<T the pulled arm maximises the index, which reads only the rewards observed before round ttt; ties are arbitrary. The arm of round ttt must be a measurable function of the rewards of earlier rounds. The regret is the expected pseudo-regret of p. 17, summed over all TTT rounds.

Repairs relative to the page: Δ∗\Delta^*Δ∗ is a positive lower bound on the positive gaps (as printed it is 000); the gap-dependent constant is Lemma 3's 16log⁡T∑iκ(Gi)/Δ∗16\log T\sum_i\kappa(G_i)/\Delta^*16logT∑i​κ(Gi​)/Δ∗, without the extra factor KKK of (5); (4) carries +1+1+1 on each right-hand side; T≥2T\ge2T≥2 throughout; Lemma 3 is pathwise for any arm sequence; the Hoeffding step is restricted to the event that the nnn-th observation occurs within the horizon. Lean's 8log⁡T/0=08\log T/0=08logT/0=0, so every statement using mi(c)m_i(c)mi​(c) restricts to positive gaps.

The formalization rules out the trivializing readings: the index cannot read the means, the gaps or unobserved rewards; the selection property is satisfiable (an explicit sequence exists); κ\kappaκ is a minimum over labellings whose classes are cliques, so it equals CCC without cross-learning and 111 with complete cross-learning; all constants are absolute.

Not part of the mission: Lemmas 1–2 (comparisons of graph invariants), Theorems 2–3 (EXP3.CL and EXP3.CL-U for adversarial rewards), Theorems 4–10 (lower bounds and the learning-to-bid applications) and the conjecture of Appendix D. Contributions of the optional-skipping Hoeffding inequality as a general lemma, and of clique-cover combinatorics on Fin C, are welcome and reusable.

Selected references

  • S. Balseiro, N. Golrezaei, M. Mahdian, V. Mirrokni, J. Schneider, Contextual Bandits with Cross-Learning, Mathematics of Operations Research, 2023; arXiv:1809.09582v3 (2021). https://arxiv.org/abs/1809.09582
  • P. Auer, N. Cesa-Bianchi, P. Fischer, Finite-time Analysis of the Multiarmed Bandit Problem, Machine Learning 47, 2002. https://doi.org/10.1023/A:1013689704352
  • W. Hoeffding, Probability Inequalities for Sums of Bounded Random Variables, Journal of the American Statistical Association 58, 1963. https://doi.org/10.1080/01621459.1963.10500830
  • S. Mannor, O. Shamir, From Bandits to Experts: On the Value of Side-Observations, NeurIPS 2011. https://arxiv.org/abs/1106.2436
8 thms2 active usersReviewed
Quantum Information·Captain: Goku

Entropic characteristics of subsets of statesResearch Paper

Motivation

This paper is devoted to systematic study of properties of the quantum entropy and of the Holevo capacity considered as a function of a set of quantum states. The properties of restriction of the quantum entropy to arbitrary set of states are discussed. For some types of sets necessary and sufficient conditions of boundedness and of continuity of restriction of the quantum entropy as well as necessary and sufficient conditions of existence of the Gibbs state are obtained. The Holevo capacity of an arbitrary set of states and its general properties as a function of a set are considered. The notion of the optimal average state of an arbitrary set of states with finite Holevo capacity is introduced. The condition of existence of optimal measure for a set of states is obtained. The general results concerning the quantum entropy and the Holevo capacity are illustrated by considering the several examples of sets of states.

This mission is the statement-level formalization of Entropic characteristics of subsets of states (arXiv:quant-ph/0510073v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

41 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 1 (Theorem 1, PDF p. 24). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

30 results of the paper are not stated yet, because the library lacks an interface they need:

  • Proposition 1a: Actual unbounded H-operator with a complete eigenbasis, finite spectral multiplicities, extended form-energy, partition trace, and normalized Gibbs state/critical-parameter constructions in the same coefficient-state model (hard)
  • Lemma 3: Normalized positive-trace spectral-power state sigma_t, including the support-projection t=0 branch and its linked logarithmic energy; the scalar powerTrace/decreaseCoefficient definitions alone do not construct that state (hard)
  • Proposition 3a: Normalized positive-trace spectral-power state sigma_t, including the support-projection t=0 branch and its linked logarithmic energy; the scalar powerTrace/decreaseCoefficient definitions alone do not construct that state; distinguish critical entropy radius c_* from capacity radius c^* and handle finite-rank plateau (hard)
  • Proposition 4: Actual unbounded H-operator with a complete eigenbasis, finite spectral multiplicities, extended form-energy, partition trace, and normalized Gibbs state/critical-parameter constructions in the same coefficient-state model; simultaneous linked witnesses H, Htilde=-log(sigma), finite H-energy of sigma and finite entropy of sigma (hard)
  • Corollary 1: Actual unbounded H-operator with a complete eigenbasis, finite spectral multiplicities, extended form-energy, partition trace, and normalized Gibbs state/critical-parameter constructions in the same coefficient-state model; a shared reference state and Htilde on each fixed finite energy sublevel (hard)
  • Corollary 3: A concrete action on normalized coefficient states of arbitrary unitaries AND antiunitaries, with change of orthonormal basis and continuous parameter action; support-sensitive log-energy expectation Tr sigma(-log omega) (hard)
  • Proposition 5: Arbitrary complete-basis dephasing and its density-state image. The current Matrix.diagonal/Matrix.diag expression treats the coordinate basis only; all A-F clauses need existential versus universal quantification over actual complete bases (hard)
  • Corollary 5: Actual unbounded H-operator with a complete eigenbasis, finite spectral multiplicities, extended form-energy, partition trace, and normalized Gibbs state/critical-parameter constructions in the same coefficient-state model; relative compactness is already expressible and is not replaced by closedness (hard)
  • Theorem 2: The complete A-L contract with an independently moderated, nonvacuous correction to G and all finite-capacity domains for Omega (source-ambiguity)
  • Corollary 8: A concrete action on normalized coefficient states of arbitrary unitaries AND antiunitaries, with change of orthonormal basis and continuous parameter action; the CPTP channel clause is expressible, but the whole node also includes non-CP antiunitary automorphisms (hard)
  • Proposition 9a: Actual unbounded H-operator with a complete eigenbasis, finite spectral multiplicities, extended form-energy, partition trace, and normalized Gibbs state/critical-parameter constructions in the same coefficient-state model; all of B and its three equivalent sufficient continuity conditions must accompany A and C (hard)
  • Proposition 9b: A full indexed finite/countable probability-ensemble certificate with a normalized barycenter and positive-weight maximal-distance system, including the real nonnegative common C and the H-convergent tail infimum bound (hard)
  • Proposition 1b: Actual unbounded H-operator with a complete eigenbasis, finite spectral multiplicities, extended form-energy, partition trace, and normalized Gibbs state/critical-parameter constructions in the same coefficient-state model; canonical ground projection at h=h_m and all five regularity/optimality equivalences (hard)
  • Proposition 3b: Normalized positive-trace spectral-power state sigma_t, including the support-projection t=0 branch and its linked logarithmic energy; the scalar powerTrace/decreaseCoefficient definitions alone do not construct that state; distinct upper critical radius c^*, infinite-rank regime, and canonical endpoint states for all capacity branches (hard)
  • Lemma 7: Normalized positive-trace spectral-power state sigma_t, including the support-projection t=0 branch and its linked logarithmic energy; the scalar powerTrace/decreaseCoefficient definitions alone do not construct that state; infinite support and finite positive exponent domain must be actual operator predicates (hard)
  • Lemma 9: A valid source replacement for the printed joint-diagonal expansion and invariance claim (source-ambiguity)
  • Proposition 11: Actual operator support/range and support projections in coefficient coordinates, diagonal coupling states in specified marginal eigenbases, and normalized finite-rank uniform projectors; isomorphism of arbitrary marginal states and an optimal law with full diagonal joint support, retaining all four finite-entropy equivalents (hard)
  • Lemma 10: Actual operator support/range and support projections in coefficient coordinates, diagonal coupling states in specified marginal eigenbases, and normalized finite-rank uniform projectors; distinguish closed convex hull in clause (i) from finite mixtures in clause (iii) (hard)
  • Proposition 12: A concrete continuous compact-group projective unitary action, normalized Haar pushforward law and its actual density-state barycenter; the twirl and law must be computed from the action, not arbitrary data satisfying the conclusions (hard)
  • Remark 2: Actual unbounded H-operator with a complete eigenbasis, finite spectral multiplicities, extended form-energy, partition trace, and normalized Gibbs state/critical-parameter constructions in the same coefficient-state model; the SAME simultaneous Proposition 4 witnesses must extend to closedHull(A union {sigma}) (hard)
  • Remark 7: Actual operator support/range and support projections in coefficient coordinates, diagonal coupling states in specified marginal eigenbases, and normalized finite-rank uniform projectors; orthogonality is between the complete support spans of the sets, not just their optimal averages, and both the binary maximum and equality iff are required (hard)
  • Remark 10: Actual normalized cyclic permutation coupling states and their uniform finite law, for every d>=1, with d-dimensional uniform marginals; comparison to full quantum coupling capacity (hard)
  • Remark 12: Actual infinite-rank shared state with precisely two orthogonal pure flags in its support complement, the half-mixture set, finite-rank flag-preserving projections, and strictly increasing retained masses giving the exact log(2)/(1+eta_n) capacities (hard)
  • §5.1: binary optimal weights, finite symmetry and enlargement: A concrete action on normalized coefficient states of arbitrary unitaries AND antiunitaries, with change of orthonormal basis and continuous parameter action; actual finite orbit law/uniform average and orthogonal-support finite ensembles, together with the unique distinct-binary equal-divergence root and the equal-capacity enlargement clause (hard)
  • §5.1: full q_n,epsilon family and (45)–(46): A source-specified treatment of q_n=0, q_n=1, duplicate signals and finite-degenerate families in formulas (45)-(46) (source-ambiguity)
  • §5.1: compact countable set without optimal law: Constructed rho_n^±(q,epsilon), its entropy-defined purity interpolation, normalized states and limit signal, and the extended F_e/G_e series with a boundary-root-safe canonical parameter choice for q_n=1/log(n log^3(2n+1)) and every epsilon, with exact F_1(1)<1 rather than the printed decimal approximation (hard)
  • §5.2: no minimal closed equal-capacity subset: Actual unbounded H-operator with a complete eigenbasis, finite spectral multiplicities, extended form-energy, partition trace, and normalized Gibbs state/critical-parameter constructions in the same coefficient-state model; actual late-tail finite-cutoff Gibbs approximants (8)-(9), their entropy-limit state, and closure of their union of chosen-basis layers (hard)
  • §5.5: optimal law exists but no purely atomic one: A concrete continuous compact-group projective unitary action, normalized Haar pushforward law and its actual density-state barycenter; the actual normalized circle step vector, its complex Fourier coefficients and pure translation orbit, with nonatomic Haar law and absence of EVERY countable orbit decomposition of the twirl (hard)
  • Theorem 2G literal entropy-continuity alternative: Entropy control at ensemble barycenters in closedHull(A_1) in the literal second G alternative (source-ambiguity)
  • §5.1 (45)–(46): convergent family on the proof-used interior domain: Constructed rho_n^±(q,epsilon), its entropy-defined purity interpolation, normalized states and limit signal, and the extended F_e/G_e series with a boundary-root-safe canonical parameter choice on the explicit proof-used domain 0<q_n<1 and q_n->0, retaining roots AT the convergence threshold when F(a)=1 (hard)

Selected references

  • Entropic characteristics of subsets of states, arXiv:quant-ph/0510073v2, https://arxiv.org/abs/quant-ph/0510073v2
44 thms2 active usersReviewed
Quantum Information·Captain: Goku

The structure of degradable quantum channelsResearch Paper

Motivation

Degradable quantum channels are among the only channels whose quantum and private classical capacities are known. As such, determining the structure of these channels is a pressing open question in quantum information theory. We give a comprehensive review of what is currently known about the structure of degradable quantum channels, including a number of new results as well as alternate proofs of some known results. In the case of qubits, we provide a complete characterization of all degradable channels with two dimensional output, give a new proof that a qubit channel with two Kraus operators is either degradable or anti-degradable and present a complete description of anti-degradable unital qubit channels with a new proof. For higher output dimensions we explore the relationship between the output and environment dimensions (dBd_BdB​ and dEd_EdE​ respectively) of degradable channels. For several broad classes of channels we show that they can be modeled with a environment that is "small" in the sense dE≤dBd_E \leq d_BdE​≤dB​. Perhaps surprisingly, we also present examples of degradable channels with ``large'' environments, in the sense that the minimal dimension dE>dBd_E > d_BdE​>dB​. Indeed, one can have dE>14dB2d_E > \tfrac{1}{4} d_B^2dE​>41​dB2​. In the case of channels with diagonal Kraus operators, we describe the subclass which are complements of entanglement breaking channels. We also obtain a number of results for channels in the convex hull of conjugations with generalized Pauli matrices. However, a number of open questions remain about these channels and the more general case of random unitary channels.

This mission is the statement-level formalization of The structure of degradable quantum channels (arXiv:0802.1360v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

37 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 4: complete degradable qubit-output structure (original paper seed) (Theorem 4: complete degradable qubit-output structure (original paper seed), PDF p. 12). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

6 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 19: A valid prescribed degrader for all real angles, including singular denominators (source-ambiguity)
  • §2.1: one-dimensional input bullet: An ambient-output-minimality convention justifying d_B=d_E (source-ambiguity)
  • §4: four-dimensional direct-sum example: The exact four-Kraus count for the two unrestricted summands (source-ambiguity)
  • §7: claimed Holevo additivity transfer via (16): A valid capacity identity and additivity-transfer theorem for the common-input weighted flag channel (source-ambiguity)
  • A.1: alleged unrestricted commutant lift and complement relation (62)–(68): The missing commutation-domain hypothesis for the alleged arbitrary-rho lift (source-ambiguity)
  • §3: unnumbered qubit-output classification summary: Missing degradability and parameter-domain premises in the summary bullets (source-ambiguity)

Selected references

  • The structure of degradable quantum channels, arXiv:0802.1360v2, https://arxiv.org/abs/0802.1360v2
48 thms2 active usersReviewed
Quantum Information·Captain: Goku

Tema Con Variazioni: Quantum Channel CapacityResearch Paper

Motivation

Channel capacity describes the size of the nearly ideal channels, which can be obtained from many uses of a given channel, using an optimal error correcting code. In this paper we collect and compare minor and major variations in the mathematically precise statements of this idea which have been put forward in the literature. We show that all the variations considered lead to equivalent capacity definitions. In particular, it makes no difference whether one requires mean or maximal errors to go to zero, and it makes no difference whether errors are required to vanish for any sequence of block sizes compatible with the rate, or only for one infinite sequence.

This mission is the statement-level formalization of Tema Con Variazioni: Quantum Channel Capacity (arXiv:quant-ph/0311037v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

35 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Abstract and Sections 2–7: equivalent quantum capacity definitions (Abstract and Sections 2–7: equivalent quantum capacity definitions, PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

1 results of the paper are not stated yet, because the library lacks an interface they need:

  • Section 2.2 exact-boundary sentence; compare p.29: A consistent exact-boundary version of the p.4 sporadic-rate assertion under Definition 2.1. (source-ambiguity)

Selected references

  • Tema Con Variazioni: Quantum Channel Capacity, arXiv:quant-ph/0311037v1, https://arxiv.org/abs/quant-ph/0311037v1
40 thms2 active usersReviewed
Quantum Information·Captain: Goku

Trade-off capacities of the quantum Hadamard channelsResearch Paper

Motivation

Coding theorems in quantum Shannon theory express the ultimate rates at which a sender can transmit information over a noisy quantum channel. More often than not, the known formulas expressing these transmission rates are intractable, requiring an optimization over an infinite number of uses of the channel. Researchers have rarely found quantum channels with a tractable classical or quantum capacity, but when such a finding occurs, it demonstrates a complete understanding of that channel's capabilities for transmitting classical or quantum information. Here, we show that the three-dimensional capacity region for entanglement-assisted transmission of classical and quantum information is tractable for the Hadamard class of channels. Examples of Hadamard channels include generalized dephasing channels, cloning channels, and the Unruh channel. The generalized dephasing channels and the cloning channels are natural processes that occur in quantum systems through the loss of quantum coherence or stimulated emission, respectively. The Unruh channel is a noisy process that occurs in relativistic quantum information theory as a result of the Unruh effect and bears a strong relationship to the cloning channels. We give exact formulas for the entanglement-assisted classical and quantum communication capacity regions of these channels. The coding strategy for each of these examples is superior to a naive time-sharing strategy, and we introduce a measure to determine this improvement.

This mission is the statement-level formalization of Trade-off capacities of the quantum Hadamard channels (arXiv:1001.1732v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

26 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Unnumbered main result: Hadamard CQE single-letterization (Unnumbered main result: Hadamard CQE single-letterization, PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

6 results of the paper are not stated yet, because the library lacks an interface they need:

  • Lemma-2: An unstated feasibility or tie-breaking qualification on every lambda=0 CQ optimizer. (source-ambiguity)
  • Theorem-6: Full countably infinite flagged-cloner channel, both unrestricted-block CQ/CE regions, and summable entropy adapters for arbitrary finite-reference block inputs. (hard)
  • Unruh-time-sharing-gain: Both full infinite-output Unruh CQ/CE regions and their own endpoint time-sharing hulls. (hard)
  • CQE-time-sharing-gain: A common three-resource endpoint-protocol time-sharing hull and the full Unruh positive-consumption CQE region. (hard)
  • Unruh-common-ensemble: One shared binary purified input optimizing both unrestricted infinite-output Unruh rate boundaries, with summable weighted entropy objectives. (hard)
  • relative-gain-numerics: Exact threshold domains or certified numerical error bounds for the qualitative Figure 6 rankings. (source-ambiguity)

Selected references

  • Trade-off capacities of the quantum Hadamard channels, arXiv:1001.1732v2, https://arxiv.org/abs/1001.1732v2
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The Conley-Zehnder index for a path of symplectic matricesResearch Paper

Motivation

We give here a self contained and elementary introduction to the Conley-Zehnder index for a path of symplectic matrices. We start from the definition of the index as the degree of a map into the circle for a path starting at the identity and ending at a matrix for which 1 is not an eigenvalue. We prove some properties which characterize this index using normal forms for symplectic matrices obtained from geometrical considerations. We explore the relations to Robbin-Salamon index for paths of Lagrangians. We give an axiomatic characterization of the generalization of the Conley-Zehnder index for any continuous path of symplectic matrices defined by Robbin and Salamon.

This mission is the statement-level formalization of The Conley-Zehnder index for a path of symplectic matrices (arXiv:1201.3728v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

43 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Classical integer Conley–Zehnder index: degree construction, independence and determinant parity (Classical integer Conley–Zehnder index: degree construction, independence and determinant parity, PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

8 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 23: Symplectic bases of the constructed real primary subspace and dependent Jordan block sums (hard)
  • Theorem 24: Signed Jordan block representation on the real lambda-primary symplectic space (hard)
  • Theorem 25: Unambiguous unit-circle odd-block columns, dimensions and block count (source-ambiguity)
  • Proposition 42: Constructed complementary-Lagrangian chart and its differentiable transition (hard)
  • Lemma 43: Transported tangent form on the smooth Lagrangian Grassmannian (hard)
  • Unnumbered: complementary Lagrangian chart and tangent identification: Lagrangian Grassmannian chart and actual tangent-space identification (hard)
  • Theorem 45: Arbitrary-reference Lagrangian index on the actual topological Lagrangian Grassmannian (hard)
  • Cited regularization and crossing-sum invariance: Regular representatives and homotopy-invariant crossing sums for arbitrary Lagrangian paths (hard)

Selected references

  • The Conley-Zehnder index for a path of symplectic matrices, arXiv:1201.3728v2, https://arxiv.org/abs/1201.3728v2
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Conditions for the local manipulation of Gaussian statesResearch Paper

Motivation

We present a general necessary and sufficient criterion for the possibility of a state transformation from one mixed Gaussian state to another of a bi-partite continuous-variable system with two modes. The class of operations that will be considered is the set of local Gaussian completely positive trace-preserving maps.

This mission is the statement-level formalization of Conditions for the local manipulation of Gaussian states (arXiv:quant-ph/0109126v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

6 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Proposition 2: exact LOG conversion criterion (Proposition 2, PDF p. 2). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

6 results of the paper are not stated yet, because the library lacks an interface they need:

  • Minimal-noise characterization: A justified minimal-noise definition and a valid equivalence to f1=0 at zero commutator defect (source-ambiguity)
  • Composition of two minimal LOG: Operational factorization using independently defined minimal local noise (source-ambiguity)
  • Zero-correlation one-sided continuation: Correct one-sided criterion at xi4=0 including product states (source-ambiguity)
  • Zero-correlation two-sided criterion: Correct two-sided criterion at xi4=0 and unambiguous target indices (source-ambiguity)
  • Partial, non-total order assertion: A specified domain or equivalence quotient on which antisymmetry is intended (source-ambiguity)
  • Note [14]: single ancillary mode: A valid bound on ancillary modes for singular Gaussian channels (source-ambiguity)

Selected references

  • Conditions for the local manipulation of Gaussian states, arXiv:quant-ph/0109126v2, https://arxiv.org/abs/quant-ph/0109126v2
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On Shor's channel extension and constrained channelsResearch Paper

Motivation

In this paper we give several equivalent formulations of the additivity conjecture for constrained channels, which formally is substantially stronger than the unconstrained additivity. To this end a characteristic property of the optimal ensemble for such a channel is derived, generalizing the maximal distance property. It is shown that the additivity conjecture for constrained channels holds true for certain nontrivial classes of channels. Recently P. Shor showed that conjectured additivity properties for several quantum information quantities are in fact equivalent. After giving an algebraic formulation for the Shor's channel extension, its main asymptotic property is proved. It is then used to show that additivity for two constrained channels can be reduced to the same problem for unconstrained channels, and hence, "global" additivity for channels with arbitrary constraints is equivalent to additivity without constraints.

This mission is the statement-level formalization of On Shor's channel extension and constrained channels (arXiv:quant-ph/0306196v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

21 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 2: constrained versus asymptotic extension additivity (Theorem 2: constrained versus asymptotic extension additivity, PDF p. 13). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Selected references

  • On Shor's channel extension and constrained channels, arXiv:quant-ph/0306196v2, https://arxiv.org/abs/quant-ph/0306196v2
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Continuity bounds on the quantum relative entropyResearch Paper

Motivation

The quantum relative entropy is frequently used as a distance, or distinguishability measure between two quantum states. In this paper we study the relation between this measure and a number of other measures used for that purpose, including the trace norm distance. More precisely, we derive lower and upper bounds on the relative entropy in terms of various distance measures for the difference of the states based on unitarily invariant norms. The upper bounds can be considered as statements of continuity of the relative entropy distance in the sense of Fannes. We employ methods from optimisation theory to obtain bounds that are as sharp as possible.

This mission is the statement-level formalization of Continuity bounds on the quantum relative entropy (arXiv:quant-ph/0503218v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

25 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is §VI, Theorem 4: sharp lower bound for every UI norm (seed headline) (§VI, Theorem 4: sharp lower bound for every UI norm (seed headline), PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

4 results of the paper are not stated yet, because the library lacks an interface they need:

  • §V.B, Theorem 3: printed logarithmic continuity bound (deferred): A corrected Fannes modulus or a source-justified local distance domain for the logarithmic continuity bound; the unrestricted printed inequality cannot be asserted. (source-ambiguity)
  • §VII.A, unnumbered printed series (48) (deferred): A corrected Taylor series for (46): powers beta^(k-1) and (1-beta)^(k-1), with a plus (-1)^k term. The independently valid leading coefficient is already stated. (source-ambiguity)
  • §VII.B, Theorem 6: complete bound plus fixed-dimension sharpness wording (deferred): An exact fixed-dimension, fixed-actual-minimum sharpness domain, including the residual-eigenvalue condition, or a corrected dimension-independent sharpness claim. (source-ambiguity)
  • §VIII, Theorem 7: full asymptotic statement (converse deferred): A support-reducing/invariance hypothesis with an audited converse, or a bound using the minimum positive eigenvalue of the full sigma_n instead of its compression. (source-ambiguity)

Selected references

  • Continuity bounds on the quantum relative entropy, arXiv:quant-ph/0503218v3, https://arxiv.org/abs/quant-ph/0503218v3
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Strong Converse and Stein's Lemma in the Quantum Hypothesis TestingResearch Paper

Motivation

The hypothesis testing problem of two quantum states is treated. We show a new inequality between the error of the first kind and the second kind, which complements the result of Hiai and Petz to establish the quantum version of Stein's lemma. The inequality is also used to show a bound on the first kind error when the power exponent for the second kind error exceeds the quantum relative entropy, and the bound yields the strong converse in the quantum hypothesis testing. Finally, we discuss the relation between the bound and the power exponent derived by Han and Kobayashi in the classical hypothesis testing.

This mission is the statement-level formalization of Strong Converse and Stein's Lemma in the Quantum Hypothesis Testing (arXiv:quant-ph/9906090v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

10 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Quantum Stein lemma at every fixed positive error (§3, Theorem 2, (10): quantum Stein lemma, corrected positive-error domain, PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

1 results of the paper are not stated yet, because the library lacks an interface they need:

  • §5, unnumbered quantum variational identity and Golden–Thompson comparison: A source-specified quantum active-rate attainment domain, singular-state log-exponential convention, and nonzero-order equality-case domain for the combined p.8 identity. (source-ambiguity)

Selected references

  • Strong Converse and Stein's Lemma in the Quantum Hypothesis Testing, arXiv:quant-ph/9906090v1, https://arxiv.org/abs/quant-ph/9906090v1
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Quantum broadcast channelsResearch Paper

Motivation

We consider quantum channels with one sender and two receivers, used in several different ways for the simultaneous transmission of independent messages. We begin by extending the technique of superposition coding to quantum channels with a classical input to give a general achievable region. We also give outer bounds to the capacity regions for various special cases from the classical literature and prove that superposition coding is optimal for a class of channels. We then consider extensions of superposition coding for channels with a quantum input, where some of the messages transmitted are quantum instead of classical, in the sense that the parties establish bipartite or tripartite GHZ entanglement. We conclude by using state merging to give achievable rates for establishing bipartite entanglement between different pairs of parties with the assistance of free classical communication.

This mission is the statement-level formalization of Quantum broadcast channels (arXiv:quant-ph/0603098v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

16 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 1 and its explicit nonregularization limitation (seed paper result) (Theorem 1 and its explicit nonregularization limitation (seed paper result), PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

5 results of the paper are not stated yet, because the library lacks an interface they need:

  • Unnumbered remark: regularized two-EPR capacity formula: Capacity converse and zero-resource completion of the regularized two-EPR witness union (source-ambiguity)
  • §II-C unnumbered quantum outer bound: less noisy: Source-pinned quantum less-noisy comparison domain supporting quantum conditioning (source-ambiguity)
  • §II-C unnumbered quantum outer bound: more capable: Source-pinned quantum more-capable comparison domain supporting quantum conditioning (source-ambiguity)
  • §IV unnumbered strengthening: strong subspace transmission: Broadcast-specific strong-subspace error criteria for Theorems 3–6 (source-ambiguity)
  • Appendix A unnumbered result: support reduction preserving all three information quantities: A true same-finite-T support-reduction assertion preserving all three information quantities (source-ambiguity)

Selected references

  • Quantum broadcast channels, arXiv:quant-ph/0603098v2, https://arxiv.org/abs/quant-ph/0603098v2
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Properties of Conjugate Channels with Applications to Additivity and MultiplicativityResearch Paper

Motivation

Quantum channels can be described via a unitary coupling of system and environment, followed by a trace over the environment state space. Taking the trace instead over the system state space produces a different mapping which we call the conjugate channel. We explore the properties of conjugate channels and describe several different methods of construction. In general, conjugate channels map M_d to M_d' with d < d', and different constructions may differ by conjugation with a partial isometry. We show that a channel and its conjugate have the same minimal output entropy and maximal output p-norm. It then follows that the additivity and multiplicativity conjectures for these measures of optimal output purity hold for a product of channels if and only if they also hold for the product of their conjugates. This allows us to reduce these conjectures to the special case of maps taking M_d to M_d' with a minimal representation of dimension at most d. We find explicit expressions for the conjugates for a number of well-known examples, including entanglement-breaking channels, unital qubit channels, the depolarizing channel, and a subclass of random unitary channels. For the entanglement-breaking channels, channels this yields a new class of channels for which additivity and multiplicativity of optimal output purity can be established. For random unitary channels using the generalized Pauli matrices, we obtain a new formulation of the multiplicativity conjecture. The conjugate of the completely noisy channel plays a special role and suggests a mechanism for using noise to transmit information.

This mission is the statement-level formalization of Properties of Conjugate Channels with Applications to Additivity and Multiplicativity (arXiv:quant-ph/0509126v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

30 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 5 / paper headline: conjugation preserves multiplicativity and entropy additivity (Theorem 5 / paper headline: conjugation preserves multiplicativity and entropy additivity, PDF p. 8). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

17 results of the paper are not stated yet, because the library lacks an interface they need:

  • Corollary 11: filtered noisy complement for Pauli-diagonal channels: A consistent full source statement: Corollary 11: filtered noisy complement for Pauli-diagonal channels (source-ambiguity)
  • Theorem 14: explicit shift-clock formula (58): A consistent full source statement: Theorem 14: explicit shift-clock formula (58) (source-ambiguity)
  • Theorem 15: additional equality/decomposability assertion: A consistent full source statement: Theorem 15: additional equality/decomposability assertion (source-ambiguity)
  • Theorem 16: subgroup/coset equality characterization: A consistent full source statement: Theorem 16: subgroup/coset equality characterization (source-ambiguity)
  • Theorem 18 (Stinespring): cited general C-star dilation theorem: A consistent full source statement: Theorem 18 (Stinespring): cited general C-star dilation theorem (source-ambiguity)
  • Unnumbered CQ extremality claim (cited [16]): A consistent full source statement: Unnumbered CQ extremality claim (cited [16]) (source-ambiguity)
  • Unnumbered formulas (37)–(40): diagonal Weyl action: A consistent full source statement: Unnumbered formulas (37)–(40): diagonal Weyl action (source-ambiguity)
  • Unnumbered cyclic axis-state formula (46)–(47): A consistent full source statement: Unnumbered cyclic axis-state formula (46)–(47) (source-ambiguity)
  • Example 1: composite-dimensional decomposable image: A consistent full source statement: Example 1: composite-dimensional decomposable image (source-ambiguity)
  • Example 2: eight-label support and formula (49): A consistent full source statement: Example 2: eight-label support and formula (49) (source-ambiguity)
  • Example 3: combinations of axis QC channels: A consistent full source statement: Example 3: combinations of axis QC channels (source-ambiguity)
  • Unnumbered: Pauli support subgroups determine block decompositions: A consistent full source statement: Unnumbered: Pauli support subgroups determine block decompositions (source-ambiguity)
  • Unnumbered corollary (59): set representation of the pure image: A consistent full source statement: Unnumbered corollary (59): set representation of the pure image (source-ambiguity)
  • Example 5: depolarizing bound attainment and product nonattainment: A consistent full source statement: Example 5: depolarizing bound attainment and product nonattainment (source-ambiguity)
  • Unnumbered appendix claim: strict product-bound nonattainment: A consistent full source statement: Unnumbered appendix claim: strict product-bound nonattainment (source-ambiguity)
  • Unnumbered appendix classification and Bell/product comparison: A consistent full source statement: Unnumbered appendix classification and Bell/product comparison (source-ambiguity)
  • Example 6: basis dependence of decomposability: A consistent full source statement: Example 6: basis dependence of decomposability (source-ambiguity)

Selected references

  • Properties of Conjugate Channels with Applications to Additivity and Multiplicativity, arXiv:quant-ph/0509126v3, https://arxiv.org/abs/quant-ph/0509126v3
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Monogamy of entanglement and other correlationsResearch Paper

Motivation

It has been observed by numerous authors that a quantum system being entangled with another one limits its possible entanglement with a third system: this has been dubbed the "monogamous nature of entanglement". In this paper we present a simple identity which captures the trade-off between entanglement and classical correlation, which can be used to derive rigorous monogamy relations. We also prove various other trade-offs of a monogamy nature for other entanglement measures and secret and total correlation measures.

This mission is the statement-level formalization of Monogamy of entanglement and other correlations (arXiv:quant-ph/0310037v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

17 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 1, Eqs. (2)–(3): complementarity of entanglement and classical correlation (Theorem 1, Eqs. (2)–(3): complementarity of entanglement and classical correlation, PDF p. 2). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

1 results of the paper are not stated yet, because the library lacks an interface they need:

  • Section III: two-way secret-key sandwich: Operational two-way public-discussion secret-key capacity on finite tripartite states with evaluated Eve-plus-transcript security and arbitrary private local memory. (hard)

Selected references

  • Monogamy of entanglement and other correlations, arXiv:quant-ph/0310037v1, https://arxiv.org/abs/quant-ph/0310037v1
24 thms2 active usersReviewed
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On Quantum Fidelities and Channel CapacitiesResearch Paper

Motivation

We show the equivalence of two different notions of quantum channel capacity: that which uses the entanglement fidelity as its criterion of success in transmission, and that which uses the minimum fidelity of pure states in a subspace of the input Hilbert space as its criterion. As a corollary, any source with entropy rate less than the capacity may be transmitted with high entanglement fidelity. We also show that a restricted class of encodings is sufficient to transmit any quantum source which may be transmitted on a given channel. This enables us to simplify a known upper bound for the channel capacity. It also enables us to show that the availability of an auxiliary classical channel from encoder to decoder does not increase the quantum capacity.

This mission is the statement-level formalization of On Quantum Fidelities and Channel Capacities (arXiv:quant-ph/9809010v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

23 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Entanglement and minimum-subspace capacities coincide (Abstract; Theorem 1 and Corollary 1, PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

2 results of the paper are not stated yet, because the library lacks an interface they need:

  • Lemma 3, Eq.(29): A correct source-specified sequential-fidelity estimate replacing the false printed 2 eta bound. (source-ambiguity)
  • Lemma 4, Eq.(35): A correct source-specified two-output squared-fidelity bound replacing the false 1-epsilon1-epsilon2 estimate. (source-ambiguity)

Selected references

  • On Quantum Fidelities and Channel Capacities, arXiv:quant-ph/9809010v1, https://arxiv.org/abs/quant-ph/9809010v1
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Majorization theory approach to the Gaussian channel minimum entropy conjectureResearch Paper

Motivation

A longstanding open problem in quantum information theory is to find the classical capacity of an optical communication link, modeled as a Gaussian bosonic channel. It has been conjectured that this capacity is achieved by a random coding of coherent states using an isotropic Gaussian distribution in phase space. We show that proving a Gaussian minimum entropy conjecture for a quantum-limited amplifier is actually sufficient to confirm this capacity conjecture, and we provide a strong argument towards this proof by exploiting a connection between quantum entanglement and majorization theory.

This mission is the statement-level formalization of Majorization theory approach to the Gaussian channel minimum entropy conjecture (arXiv:1111.1986v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

14 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Single-use reduction: C1 iff C2 iff C3; C4 is sufficient (C1–C4; Appendix 1, PDF p. 2). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

2 results of the paper are not stated yet, because the library lacks an interface they need:

  • Infinitesimal two-mode squeezer, (6),(8)–(9): A quantified exact infinitesimal majorization statement with a controlled approximation remainder (source-ambiguity)
  • (16)–(17), Appendix 4d, A.34–A.50: A consistent explicit positive row-subunital, column-stochastic beta-function kernel for general k (source-ambiguity)

Selected references

  • Majorization theory approach to the Gaussian channel minimum entropy conjecture, arXiv:1111.1986v1, https://arxiv.org/abs/1111.1986v1
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Multipartite quantum correlations and local recoverabilityResearch Paper

Motivation

Characterizing genuine multipartite quantum correlations in quantum physical systems has historically been a challenging problem in quantum information theory. More recently however, the total correlation or multipartite information measure has been helpful in accomplishing this goal, especially with the multipartite symmetric quantum (MSQ) discord [Piani et al., Phys. Rev. Lett. 100, 090502, 2008] and the conditional entanglement of multipartite information (CEMI) [Yang et al., Phys. Rev. Lett. 101, 140501, 2008]. Here we apply a recent and significant improvement of strong subadditivity of quantum entropy [Fawzi and Renner, arXiv:1410.0664] in order to develop these quantities further. In particular, we prove that the MSQ discord is nearly equal to zero if and only if the multipartite state for which it is evaluated is approximately locally recoverable after performing measurements on each of its systems. Furthermore, we prove that the CEMI is a faithful entanglement measure, i.e., it vanishes if and only if the multipartite state for which it is evaluated is a fully separable state. Along the way we provide an operational interpretation of the MSQ discord in terms of the partial state distribution protocol, which in turn, as a special case, gives an interpretation for the original discord quantity. Finally, we prove an inequality that could potentially improve upon the Fawzi-Renner inequality in the multipartite context, but it remains an open question to determine whether this is so.

This mission is the statement-level formalization of Multipartite quantum correlations and local recoverability (arXiv:1412.0333v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

8 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is §2, (2.1); §3: local recoverability from the multipartite information gap (§2, (2.1); §3: local recoverability from the multipartite information gap, PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

6 results of the paper are not stated yet, because the library lacks an interface they need:

  • §2, unnumbered: approximate local recovery implies a small information gap: Uniform converse to approximate JOINT local recovery with unprimed-only dimensions (source-ambiguity)
  • Proposition 4, (5.7): quantitative fourth-power CEMI faithfulness bound: Exact quantitative CEMI prefactor and valid integer extension-order rounding (source-ambiguity)
  • §8, unnumbered: geometric CEMI is faithful: Faithfulness of the unrestricted extension/recovery fidelity supremum in (8.1) (source-ambiguity)
  • §§6–6.1, unnumbered: exact optimal total communication cost: Multipartite partial-state-distribution protocol and operational infimum in nats (hard)
  • §6.2: MSQ discord is twice the coherence-restoration and loss cost: Measurement Stinespring outputs connected to forward/reverse multipartite communication costs (hard)
  • §6.3: one-sided discord is twice the state-redistribution coherence cost: Measurement coherence restoration by actual two-party redistribution with passive B (hard)

Selected references

  • Multipartite quantum correlations and local recoverability, arXiv:1412.0333v3, https://arxiv.org/abs/1412.0333v3
15 thms2 active usersReviewed
Quantum Information·Captain: Goku

Quantum majority voteResearch Paper

Motivation

Majority vote is a basic method for amplifying correct outcomes that is widely used in computer science and beyond. While it can amplify the correctness of a quantum device with classical output, the analogous procedure for quantum output is not known. We introduce quantum majority vote as the following task: given a product state ∣ψ1⟩⊗⋯⊗∣ψn⟩|ψ_1\rangle \otimes \dots \otimes |ψ_n\rangle∣ψ1​⟩⊗⋯⊗∣ψn​⟩ where each qubit is in one of two orthogonal states ∣ψ⟩|ψ\rangle∣ψ⟩ or ∣ψ⊥⟩|ψ^\perp\rangle∣ψ⊥⟩, output the majority state. We show that an optimal algorithm for this problem achieves worst-case fidelity of 1/2+Θ(1/n)1/2 + Θ(1/\sqrt{n})1/2+Θ(1/n​). Under the promise that at least 2/32/32/3 of the input qubits are in the majority state, the fidelity increases to 1−Θ(1/n)1 - Θ(1/n)1−Θ(1/n) and approaches 111 as nnn increases. We also consider the more general problem of computing any symmetric and equivariant Boolean function f:{0,1}n→{0,1}f: \{0,1\}^n \to \{0,1\}f:{0,1}n→{0,1} in an unknown quantum basis, and show that a generalization of our quantum majority vote algorithm is optimal for this task. The optimal parameters for the generalized algorithm and its worst-case fidelity can be determined by a simple linear program of size O(n)O(n)O(n). The time complexity of the algorithm is O(n4log⁡n)O(n^4 \log n)O(n4logn) where nnn is the number of input qubits.

This mission is the statement-level formalization of Quantum majority vote (arXiv:2211.11729v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

61 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Quantum majority vote: Theorem 1.2 (Quantum majority vote: Theorem 1.2, PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

3 results of the paper are not stated yet, because the library lacks an interface they need:

  • Lemma 2.1 (Schur’s Lemma).: A specified identifying intertwiner between isomorphic coordinate representations. (source-ambiguity)
  • Corollary 2.12.: Compatibility of arbitrary input/output representations with entrywise complex conjugation. (source-ambiguity)
  • Theorem C.3.: The continuity convention for the cited classification of finite-dimensional SU(2) representations. (source-ambiguity)

Selected references

  • Quantum majority vote, arXiv:2211.11729v1, https://arxiv.org/abs/2211.11729v1
73 thms2 active usersReviewed
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