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Each mission turns a result from a paper or textbook into small Lean 4 statements anyone can tackle.

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Campaigns group missions around a shared mathematical goal. Each one tracks a quantity, such as an upper or lower bound. Have a good candidate in mind? Ping us on Slack, Zulip, or WeChat.

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Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

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Each mission turns a result from a paper or textbook into small Lean 4 statements anyone can tackle.

Campaigns (experimental)

See all campaigns →

Campaigns group missions around a shared mathematical goal. Each one tracks a quantity, such as an upper or lower bound. Have a good candidate in mind? Ping us on Slack, Zulip, or WeChat.

Block Sensitivity vs. Sensitivity

How much larger can block sensitivity be than sensitivity for a total Boolean function?

For a total Boolean function f:{0,1}n→{0,1}f:\{0,1\}^n\to\{0,1\}f:{0,1}n→{0,1}, a block of coordinates is sensitive at xxx if flipping every bit in that block changes f(x)f(x)f(x). Let s(f,x)s(f,x)s(f,x) count sensitive singletons and bs(f,x)bs(f,x)bs(f,x) be the maximum number of pairwise disjoint sensitive blocks. Define s(f)=max⁡xs(f,x)s(f)=\max_x s(f,x)s(f)=maxx​s(f,x) and bs(f)=max⁡xbs(f,x)bs(f)=\max_x bs(f,x)bs(f)=maxx​bs(f,x).

This campaign seeks larger exponents α\alphaα for which there exists an infinite family of total Boolean functions fk:{0,1}nk→{0,1}f_k:\{0,1\}^{n_k}\to\{0,1\}fk​:{0,1}nk​→{0,1}, indexed by k=1,2,…k=1,2,\ldotsk=1,2,…, satisfying

s(fk)→∞,bs(fk)≥s(fk)α−o(1)as k→∞.s(f_k)\to\infty,\qquad bs(f_k)\ge s(f_k)^{\alpha-o(1)}\quad\text{as }k\to\infty.s(fk​)→∞,bs(fk​)≥s(fk​)α−o(1)as k→∞.

Here o(1)o(1)o(1) denotes a quantity tending to zero as k→∞k\to\inftyk→∞. Higher is better. The classical exponent is 222, and Huang's bound gives a ceiling of 444.

OpenAI's construction achieves an exponent strictly greater than 222.

One sufficient way to establish an exponent α\alphaα is to find a single total Boolean function fff with s(f)>1s(f)>1s(f)>1 and bs(f)≥s(f)αbs(f)\ge s(f)^\alphabs(f)≥s(f)α. Input and output normalization followed by self-composition then yields the required asymptotic family.

≥ 2.1308255793978239Formalized record→≥ 2.15Open frontier
9 provers on it17 of 18 missions formalized

Integer Multiplication Below n log n

Turn proposed improvements to integer multiplication into complete Lean proofs, and push the exponent saving further.

Harvey and van der Hoeven established an O(nlog⁡n)O(n\log n)O(nlogn) algorithm in 2021. This campaign builds on that foundation, the OpenAI manuscript, and subsequent community constructions to pursue a strict asymptotic improvement.

For two nnn-bit integers, the target is

T(n)=O ⁣(n L(n)1−κ),L(n)=max⁡(⌈log⁡2n⌉,1).T(n)=O\!\left(n\,L(n)^{1-\kappa}\right),\qquad L(n)=\max(\lceil\log_2 n\rceil,1).T(n)=O(nL(n)1−κ),L(n)=max(⌈log2​n⌉,1).

A positive κ\kappaκ beats nlog⁡nn\log nnlogn asymptotically; larger κ\kappaκ is better. Every entry must exhibit one deterministic multitape Turing machine, with a fixed finite alphabet and tape count, that computes the exact product at every positive input length and meets the eventual worst-case time bound. The tracked number measures an asymptotic exponent saving.

≥ 3.6 × 10−5Formalized record→≥ 5.1 × 10−5Open frontier
8 provers on it4 of 7 missions formalized

3SUM Exponent

Classical algorithms solve 3SUM in O(n2)O(n^2)O(n2) time. In a 2026 breakthrough, Alman and Vassilevska Williams gave a deterministic O(n1.9992)O(n^{1.9992})O(n1.9992) algorithm, refuting the integer 3SUM hypothesis. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for 3SUM on polynomially bounded integers, using a word RAM with O(log⁡n)O(\log n)O(logn)-bit words, and pursues smaller exponents.

≤ 1.960614Formalized record
4 provers on it7 of 7 missions formalized

All-Pairs Shortest Paths (APSP) Exponent

Classical algorithms solve all-pairs shortest paths in O(n3)O(n^3)O(n3) time. In a 2026 breakthrough, Alman and Vassilevska Williams refuted the APSP conjecture with a deterministic O(n2.99942)O(n^{2.99942})O(n2.99942) algorithm. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for exact APSP and pursues smaller exponents.

≤ 2.995561Formalized record
3 provers on it5 of 5 missions formalized

The irrationality measure of π

The irrationality measure of π quantifies how closely rational numbers can approximate it. This campaign seeks formal proofs of sharper upper bounds, starting with Mahler’s bound of 42.

≤ 7.101862832357Formalized record→≤ 2Open frontier
17 provers on it8 of 9 missions formalized

Sharp diagonal Hlawka constant

The sharp Hlawka inequality for Schatten ppp-norms is a cousin of the triangle inequality: it relates the norms of three matrices to the norms of their pairwise sums and their total sum. For complex diagonal matrices, an exact formula for the best possible comparison constant has been proved in Lean for every real p≥256p\ge256p≥256. We conjecture that the same formula holds for all p≥2p\ge2p≥2.

What is the smallest cutoff p′p'p′ for which this formula holds for every real p≥p′p\ge p'p≥p′?

References:

  • Wolfram MathWorld, Hlawka's Inequality.
  • Audenaert and Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, §8.2 (2017).
  • Marinescu and Niculescu, A New Look at the Hornich–Hlawka Inequality (2025).
  • Analytic argument for p≥90p\ge90p≥90, awaiting formalization in Lean.
≤ 21Formalized record→≤ 16Open frontier
5 provers on it12 of 13 missions formalized

Odd numbers as sums of primes

Is every odd number a sum of kkk primes? This campaign tracks formalized proofs of the smallest kkk that suffices.

Schnirelmann (1930) showed some finite kkk works. Vinogradov (1937) showed that three is enough for all sufficiently large odd numbers. Tao (2012) proved k=5k = 5k=5 unconditionally. Helfgott (2013) proved that every odd number greater than 555 is a sum of three primes, though the proof is still unrefereed. Ideally, we can formalize this statement here. Note that three is optimal: 272727 is neither prime nor 222 + prime.

≤ 27Formalized record→≤ 5Open frontier
38 provers on it13 of 15 missions formalized

Matrix multiplication exponent

Schoolbook matrix multiplication takes n3n^3n3 operations. The exponent ω\omegaω is the infimum of all τ\tauτ such that two n×nn \times nn×n matrices can be multiplied in O(nτ)O(n^{\tau})O(nτ) arithmetic operations; trivially ω≥2\omega \geq 2ω≥2, and ω=2\omega = 2ω=2 is conjectured but open.

Strassen gave the first nontrivial bound, ω<2.81\omega < 2.81ω<2.81, in 1969, and introduced the laser method in 1986 to reach ω<2.48\omega < 2.48ω<2.48. Coppersmith and Winograd's 1990 bound of 2.3762.3762.376 stood for two decades. Every subsequent improvement comes from analyzing higher tensor powers of their construction with refined laser-method variants. That line reached ω<2.371339\omega < 2.371339ω<2.371339 in 2025, and the current record is ω<2.371177\omega < 2.371177ω<2.371177, from August 2026. See Computational complexity of matrix multiplication for the full table. Can we formalize these results and even improve on them?

≤ 2.25Formalized record
16 provers on it9 of 9 missions formalized

All missions

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Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

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AlgebraAlgebraic GeometryGroup Theory·Captain: mikedeng1

Observable actions of algebraic groups: a reductive action is observable iff some closed orbit has maximal dimension, and the socle is the largest observable closed subsetResearch Paper

Motivation

An action of an affine algebraic group GGG on an affine variety XXX is observable when invariant regular functions see every nonzero GGG-stable ideal of the coordinate ring: if I⊆k[X]I\subseteq k[X]I⊆k[X] is a nonzero GGG-stable ideal, then IG≠(0)I^G\neq(0)IG=(0). The notion goes back to Grosshans' theory of observable subgroups (F. D. Grosshans, Observable groups and Hilbert's fourteenth problem, Amer. J. Math. 95, 1973): a closed subgroup H≤GH\le GH≤G is observable exactly when the action of HHH on GGG by left translations is observable (p. 2 of the paper), and observable subgroups are the ones for which G/HG/HG/H is quasi-affine.

L. Renner and A. Rittatore (arXiv:0902.0137) characterise observability geometrically. Their Theorem 3.10 states that an action on an irreducible affine variety is observable if and only if (1) every invariant rational function is a quotient of invariant regular functions, and (2) the set of closed orbits of maximal dimension contains a nonempty open set. Section 4 of the paper specialises this to reductive groups, where the answer becomes a single condition on closed orbits, and identifies a canonical closed subvariety, the socle, on which the action is observable. This mission formalizes that section.

Timeline:

  • 1970, V. L. Popov: for a reductive group acting on an affine variety, if some closed orbit has maximal dimension then the closed orbits of maximal dimension form an open set (cited by the paper as Proposition 4.4, from Popov's stability criterion paper, Theorem 4).
  • 1973, F. D. Grosshans: observable subgroups and Hilbert's fourteenth problem.
  • 2009, Renner–Rittatore: Theorem 3.10 for arbitrary affine groups; Theorems 4.6 and 4.7 for reductive groups.

Setting

Let kkk be an algebraically closed field. An affine algebraic group GGG is given by its coordinate ring k[G]k[G]k[G], a reduced, finitely generated, smooth kkk-algebra whose kkk-points G(k)G(k)G(k) form a group with regular multiplication and inversion. An affine variety XXX is given by its coordinate ring k[X]k[X]k[X], a reduced finitely generated kkk-algebra; its points are the kkk-algebra maps k[X]→kk[X]\to kk[X]→k. A regular action is a group homomorphism ρ:G(k)→Aut⁡k(k[X])\rho:G(k)\to\operatorname{Aut}_k(k[X])ρ:G(k)→Autk​(k[X]) whose evaluation is a regular function of (g,x)(g,x)(g,x); points move by g⋅x=x∘ρ(g−1)g\cdot x=x\circ\rho(g^{-1})g⋅x=x∘ρ(g−1).

  • The orbit of xxx is O(x)=G⋅x\mathcal O(x)=G\cdot xO(x)=G⋅x; its dimension is the Krull dimension of the coordinate ring of its closure.
  • Xmax⁡X_{\max}Xmax​ is the set of points whose orbit has maximal dimension, and Ω(X)⊆Xmax⁡\Omega(X)\subseteq X_{\max}Ω(X)⊆Xmax​ is the subset of points whose orbit is also closed.
  • The categorical quotient π:X→X/ ⁣ ⁣/G\pi:X\to X/\!\!/Gπ:X→X//G sends a point to its restriction to the invariant algebra k[X]Gk[X]^Gk[X]G.
  • The socle is the Zariski closure of the union of the closed orbits:
Xsoc=⋃O(x)‾=O(x)O(x)‾.X_{\mathrm{soc}}=\overline{\bigcup_{\overline{\mathcal O(x)}=\mathcal O(x)}\mathcal O(x)}.Xsoc​=O(x)​=O(x)⋃​O(x)​.
  • For a closed GGG-stable subset ZZZ with ideal I(Z)\mathcal I(Z)I(Z), the restricted action is the action on k[Z]=k[X]/I(Z)k[Z]=k[X]/\mathcal I(Z)k[Z]=k[X]/I(Z) induced through the quotient map.
  • A point g∈G(k)g\in G(k)g∈G(k) is unipotent when right translation by ggg on k[G]k[G]k[G] is locally unipotent. GGG is reductive when every closed, connected, normal subgroup of GGG consisting of unipotent elements is trivial.

Formalization targets

Goal: Theorem 4.7

For GGG reductive acting on an irreducible affine variety XXX:

the action is observable  ⟺  Ω(X)≠∅,\text{the action is observable}\iff\Omega(X)\neq\emptyset,the action is observable⟺Ω(X)=∅,

and XsocX_{\mathrm{soc}}Xsoc​ is the maximum GGG-stable closed subset Z⊆XZ\subseteq XZ⊆X such that the restricted action G×Z→ZG\times Z\to ZG×Z→Z is observable.

Milestones

  1. Theorem 3.10 (referenced, already posed on the platform): observable   ⟺  \iff⟺ [k[X]G]=[k[X]]G[k[X]^G]=[k[X]]^G[k[X]G]=[k[X]]G and Ω(X)\Omega(X)Ω(X) contains a nonempty open subset.
  2. Lemma 4.3: Ω(X)=π−1((X/ ⁣ ⁣/G)∖π(X∖Xmax⁡))\Omega(X)=\pi^{-1}\bigl((X/\!\!/G)\setminus\pi(X\setminus X_{\max})\bigr)Ω(X)=π−1((X//G)∖π(X∖Xmax​)); in particular Ω(X)\Omega(X)Ω(X) is a GGG-stable open subset.
  3. Proposition 4.4 (Popov): if Ω(X)≠∅\Omega(X)\neq\emptysetΩ(X)=∅ then Ω(X)\Omega(X)Ω(X) is open.
  4. Lemma 4.5: π∣X∖Xmax⁡\pi|_{X\setminus X_{\max}}π∣X∖Xmax​​ is dominant   ⟺  \iff⟺ it is surjective   ⟺  \iff⟺ Xmax⁡X_{\max}Xmax​ contains no closed orbit   ⟺  \iff⟺ Ω(X)=∅\Omega(X)=\emptysetΩ(X)=∅.
  5. Theorem 4.6, "Moreover" sentence: if ZZZ is GGG-stable, closed and π∣Z\pi|_Zπ∣Z​ is dominant, then Xsoc⊆ZX_{\mathrm{soc}}\subseteq ZXsoc​⊆Z, XsocX_{\mathrm{soc}}Xsoc​ is irreducible, and Ω(Xsoc)≠∅\Omega(X_{\mathrm{soc}})\neq\emptysetΩ(Xsoc​)=∅.
  6. Theorem 4.7, first sentence: observable   ⟺  Ω(X)≠∅\iff\Omega(X)\neq\emptyset⟺Ω(X)=∅.
  7. Lemma 3.1 (referenced, already posed on the platform): for connected GGG, the action is observable if and only if the restricted action on each irreducible component is.

Significance

The result. For reductive groups observability is decided by one closed orbit of maximal dimension, with no condition on invariant rational functions. This simplification fails for general groups: a Borel subgroup acting on a semisimple group by left translation has every orbit closed of maximal dimension, yet the action is not observable (Example 3.11 of the paper). The second sentence gives every reductive action a canonical observable piece, the socle, computed from the closed orbits alone, and Proposition 4.8 of the paper then identifies its ideal as the largest GGG-stable ideal without nonzero invariants.

Formalizing it. The results are proved in the paper (Proposition 4.4 is Popov's theorem, cited there). None of them is machine-checked. Theorem 3.10 and Lemma 3.1 are open goals of an existing public mission on the same paper, which covers §§2–3 and defers §4; this mission states §4 on the same definitions, so a proof of either referenced statement serves both. A complete development needs the basic geometric invariant theory of reductive groups: finite generation of invariants, separation of closed GGG-stable sets by invariants, the existence of a unique closed orbit in each orbit closure, and semicontinuity of orbit dimension. None of this is in Mathlib.

Difficulty

The direction "observable ⇒Ω(X)≠∅\Rightarrow\Omega(X)\neq\emptyset⇒Ω(X)=∅" follows from Theorem 3.10. The converse is where reductivity enters: given a nonzero GGG-stable ideal, one must produce a nonzero invariant in it, and the natural route is to separate the closed orbits in Ω(X)\Omega(X)Ω(X) from the zero set of the ideal by invariant functions. That separation is a theorem about reductive groups (closed disjoint GGG-stable sets are separated by invariants), not available for arbitrary groups, and it must be combined with the openness of Ω(X)\Omega(X)Ω(X). For the maximality of the socle, the paper reduces to irreducible components through Lemma 3.1, which assumes GGG connected; Theorem 4.7 makes no such assumption, so a disconnected GGG needs a reduction to the stabiliser of a component.

Formalization scope

All statements are built on the public definitions module QAlgorithms_Papers_Independent_Support21_P10 for this paper: points are kkk-algebra maps, GGG is a coordinate ring H with a group structure on its points (IsAffineAlgebraicGroup), XXX is a coordinate ring A (IsAffineVariety, finite type and reduced), the action is rho : Point k H →* (A ≃ₐ[k] A) with IsRegularAction. Closure is the Zariski closure V(I(S))V(\mathcal I(S))V(I(S)) on kkk-points (classicalClosure), and X/ ⁣ ⁣/GX/\!\!/GX//G is the set of kkk-points of k[X]Gk[X]^Gk[X]G with π\piπ the restriction map (quotientPoint). No finite generation of k[X]Gk[X]^Gk[X]G is assumed.

Conventions committed to:

  • Irreducibility. XXX is irreducible (IsDomain A) in Theorems 4.6 and 4.7, the paper's standing assumption for §4 (p. 2). Without it the first sentence of 4.7 is false. Lemmas 4.3, 4.5 and Proposition 4.4 are stated for arbitrary affine XXX, as printed.
  • No connectedness of GGG. Theorem 4.7 is stated as printed, for possibly disconnected GGG.
  • Reductive is a hypothesis IsReductiveGroup k H: every Zariski-closed normal subgroup of G(k)G(k)G(k) with prime vanishing ideal and consisting of unipotent points is trivial. Unipotence is local unipotence of right translation on k[G]k[G]k[G].
  • Socle: classicalClosure {x | IsClosedOrbit rho x}.
  • Restricted actions: an action rhoZ on A ⧸ coordinateVanishingIdeal Z compatible with the quotient map (IsRestrictionOf). For the socle its existence is part of the conclusion; for a competitor ZZZ, compatibility is a hypothesis. No statement quantifies over an uncoupled action.
  • Ω(X)≠∅\Omega(X)\neq\emptysetΩ(X)=∅ is (omegaLocus rho).Nonempty. This is strictly weaker than Theorem 3.10's condition that Ω(X)\Omega(X)Ω(X) contain a nonempty open set.

A trivializing reading is excluded: the socle is computed from the closed orbits and is never defined as "the largest closed set with observable restricted action", which would make the maximality claim a tautology.

Welcome contributions: proofs of the milestones, and reusable infrastructure for reductive group actions (finite generation of invariants, separation of closed invariant sets, orbit-closure structure).

Selected references

  • L. Renner, A. Rittatore, Observable actions of algebraic groups, preprint, arXiv:0902.0137v2 [math.AG], 2009. https://arxiv.org/abs/0902.0137v2
  • V. L. Popov, Stability criterion for the action of a semisimple group on a factorial manifold, Math. USSR Izv. 4 (3) (1970), 527–535 (reference [14] of the paper).
  • F. D. Grosshans, Observable groups and Hilbert's fourteenth problem, Amer. J. Math. 95 (1973), 229–253 (reference [12] of the paper).
  • W. Ferrer Santos, A. Rittatore, Actions and Invariants of Algebraic Groups, Pure and Applied Math. 268, Dekker/CRC Press, 2005 (reference [10] of the paper; Theorem 13.3.13 is Proposition 4.4).
  • V. L. Popov, E. B. Vinberg, Invariant theory, in Algebraic Geometry IV, Encyclopaedia of Mathematical Sciences 55, Springer, 1994 (reference [15] of the paper).
10 thms2 active usersReviewed
OptimizationQuantum InformationTheoretical Computer Science·Captain: mikedeng1

Optimizing Quantum Circuit Parameters via SDP: Algorithm 1 Is a 0.562-Approximation for Quantum Max CutResearch Paper

Motivation

Quantum Max Cut asks for the highest energy of a two-qubit interaction Hamiltonian placed on the edges of a weighted graph. It is a quantum analogue of Max Cut: a classical cut assigns one of two labels to each vertex, while a quantum state can use correlations and entanglement across the qubits. Lee studies an approximation algorithm that first solves a semidefinite program and then uses its vectors to choose both a bit string and the angles of a quantum circuit. The result applies to arbitrary nonnegatively weighted simple graphs, without a degree or regularity restriction. The guarantee is an approximation ratio of 0.5620.5620.562 for the energy of the algorithm's random output in expectation Lee, 2022, pp. 9–13.

The paper places this algorithm alongside earlier approaches that round a level-one or level-two quantum Lasserre program. Its distinguishing object is a circuit with one parameter per graph edge, computed from the SDP vectors rather than optimized over circuit angles after rounding. The parameter rule makes a global approximation guarantee possible even when neighboring edge gates interfere Lee, 2022, pp. 3–5, 9.

Setting

Let G=(V,E,w)G=(V,E,w)G=(V,E,w) be a finite simple graph with nonnegative weights wijw_{ij}wij​. Associate one qubit with each vertex. On qubit iii, let Xi,Yi,ZiX_i,Y_i,Z_iXi​,Yi​,Zi​ be the standard Pauli operators, and let III be the identity. Each edge contributes

Hij=14(I−XiXj−YiYj−ZiZj),H=∑(i,j)∈EwijHij.H_{ij}=\frac14(I-X_iX_j-Y_iY_j-Z_iZ_j),\qquad H=\sum_{(i,j)\in E}w_{ij}H_{ij}.Hij​=41​(I−Xi​Xj​−Yi​Yj​−Zi​Zj​),H=(i,j)∈E∑​wij​Hij​.

For a unit state ∣ψ⟩|\psi\rangle∣ψ⟩, its energy is ⟨ψ∣H∣ψ⟩\langle\psi|H|\psi\rangle⟨ψ∣H∣ψ⟩. The Quantum Max Cut optimum is the largest eigenvalue of HHH, equivalently the largest energy over all unit states Lee, 2022, Definition 2, p. 2.

The paper's canonical Lasserre program at level kkk uses a real positive semidefinite matrix MMM indexed by Pauli strings of weight at most kkk. Its constraints make matrix entries consistent with products of Pauli strings. At level two, its objective has one term for each of XiXjX_iX_jXi​Xj​, YiYjY_iY_jYi​Yj​, and ZiZjZ_iZ_jZi​Zj​ on every edge. Lemma 1 places all quantum-state energies below feasible Lasserre objectives. The paper then introduces a vector semidefinite program (S). It uses a unit vector v0v_0v0​, vectors vi,av_{i,a}vi,a​ for vertices and a∈{1,2,3}a\in\{1,2,3\}a∈{1,2,3}, and vectors vij,av_{ij,a}vij,a​ for pairs of distinct vertices. Relations (1)–(8) fix their norms and inner products. Writing vij=∑avij,av_{ij}=\sum_a v_{ij,a}vij​=∑a​vij,a​, its objective is

S(G;v)=∑(i,j)∈Ewij4(v0−vij)⋅v0.S(G;v)=\sum_{(i,j)\in E}\frac{w_{ij}}4(v_0-v_{ij})\cdot v_0.S(G;v)=(i,j)∈E∑​4wij​​(v0​−vij​)⋅v0​.

Lemma 2 shows that (S) relaxes the level-two Lasserre program Lee, 2022, Definitions 3–5 and Lemmas 1–2, pp. 3–6.

Algorithm 1 takes an optimal feasible solution of (S). It picks a∈{1,2,3}a\in\{1,2,3\}a∈{1,2,3} uniformly, chooses a random direction rrr, and sets bit ziz_izi​ by the sign of vi,a⋅rv_{i,a}\cdot rvi,a​⋅r. For each edge it computes the normalized correlation

γij=−(v0+vij)⋅v0∥v0+vij∥∥v0∥,θij=12arccos⁡(exp⁡[−0.041max⁡(γij,0)]).\gamma_{ij}=-\frac{(v_0+v_{ij})\cdot v_0}{\|v_0+v_{ij}\|\|v_0\|},\qquad \theta_{ij}=\frac12\arccos\bigl(\exp[-0.041\max(\gamma_{ij},0)]\bigr).γij​=−∥v0​+vij​∥∥v0​∥(v0​+vij​)⋅v0​​,θij​=21​arccos(exp[−0.041max(γij​,0)]).

It starts in the computational basis state ∣z⟩|z\rangle∣z⟩ and applies the commuting edge gates exp⁡(iθijP(i)P(j))\exp(i\theta_{ij}P(i)P(j))exp(iθij​P(i)P(j)), with P(i)=XiP(i)=X_iP(i)=Xi​ when zi=1z_i=1zi​=1 and P(i)=YiP(i)=Y_iP(i)=Yi​ when zi=0z_i=0zi​=0. The result is a random state ∣ϕ(θ)⟩|\phi(\theta)\rangle∣ϕ(θ)⟩ Lee, 2022, Algorithm 1, p. 9.

Formalization targets

The goal is the expectation form of Theorem 1. For every nonnegatively weighted graph, every globally optimal feasible SDP solution vvv, and every unit quantum state ∣ψ⟩|\psi\rangle∣ψ⟩,

E ⟨ϕ(θ)∣H∣ϕ(θ)⟩≥0.562 ⟨ψ∣H∣ψ⟩.\mathbb E\,\langle\phi(\theta)|H|\phi(\theta)\rangle \ge 0.562\,\langle\psi|H|\psi\rangle.E⟨ϕ(θ)∣H∣ϕ(θ)⟩≥0.562⟨ψ∣H∣ψ⟩.

The goal also states that the random energy is integrable. Because the inequality holds for every unit ∣ψ⟩|\psi\rangle∣ψ⟩, it is exactly the comparison with 0.5620.5620.562 times the maximum eigenvalue. The printed theorem omits the expectation sign, while its proof explicitly averages the rounded output Lee, 2022, Theorem 1 and proof, pp. 10–11.

The milestones are the source's relaxation lemmas, the feasible-vector identities, the star monogamy bound, the hyperplane cut-probability bound, the circuit's edge-energy bound, equations (19) and (21)–(24), the final scalar minimum, and the per-solution expected-energy bound. Their order moves from the Hamiltonian and SDP model to the output of Algorithm 1. The coefficient 0.5620.5620.562 and the parameter 0.0410.0410.041 are the paper's values, not tunable placeholders.

Significance

Together, the two relaxation lemmas connect the quantum optimum to the objective optimized by (S). The rounding results then connect a feasible SDP value to a physically represented output state. The theorem certifies a constant approximation ratio for arbitrary weighted graphs in the model of the paper. The star monogamy inequality and edge-energy lemma also isolate claims useful for analyzing related rounding circuits Lee, 2022, Lemmas 1–6, pp. 4–10.

This result is proved in the cited paper. The mission asks for machine-checked proofs of its statements and for the model that makes those statements precise. Its definitions of Pauli strings, the quantum Hamiltonian, canonical Lasserre feasibility, the vector SDP, and the rounded circuit can support later comparisons of SDP-based quantum approximation algorithms. The draft statements compile, but a compiling sorry is not a proof; the theorem and milestones remain open formalization targets.

Difficulty

Bounding the probability that a rounded bit string cuts an edge is only one part of the argument. Its circuit gate acts on the same qubits as gates at neighboring edges. Consequently, a good cut probability alone does not determine the energy on that edge. The monogamy bound limits how much SDP value can be concentrated around a vertex, while the edge-energy statement accounts for the neighboring gate parameters. A formal proof must also connect matrix feasibility, vector feasibility, Gaussian rounding, and complex matrix expectations without losing the edge weights or the factor 1/41/41/4 Lee, 2022, pp. 7–13.

Formalization scope

Vertices are Fin n, computational basis labels are bit strings Fin n → Fin 2, and Pauli strings are maps Fin n → Fin 4. The graph is simple; each edge occurs once, with its smaller endpoint first. Only that orientation's weight is read. The vector SDP uses Fin N → ℝ, and its feasibility predicate states relations (1)–(8) with distinct-index conditions. The ordered-pair implementation of vij,av_{ij,a}vij,a​ includes symmetry, making the paper's undirected edge indexing explicit. Optimality in the goal compares feasible solutions across every finite dimension, so a solution optimal only in a small dimension cannot satisfy the intended premise.

The random direction is a standard Gaussian vector. Its signs have the same distribution as the signs from a direction uniform on the sphere; a zero projection gives bit zero. The circuit uses the cosine-sine form of each Pauli-product exponential and a lexicographic edge order. Its gates commute, so the chosen order represents the paper's product. The expectation averages the three choices of aaa and integrates over the Gaussian vector. The goal includes integrability, and its universal unit-state comparison avoids a supremum with a default value on a bad domain.

Three source boundaries are stated explicitly. The Lasserre objective requires k≥2k\ge2k≥2 because it indexes two-qubit Pauli strings. Lemma 6 requires 0≤θij≤π/40\le\theta_{ij}\le\pi/40≤θij​≤π/4 on edges; the printed nonnegative-angle condition is too broad, while Algorithm 1 always gives angles in that interval. Definition 4's repeated ZiZjZ_iZ_jZi​Zj​ objective term is read as YiYjY_iY_jYi​Yj​, as required by the Hamiltonian and its appendix calculation. The Goemans–Williamson quotient uses [−1,1)[-1,1)[−1,1) since the printed closed endpoint t=1t=1t=1 gives 0/00/00/0. A single arbitrary feasible SDP solution cannot replace the globally optimal one in the final comparison with the quantum optimum, and a deterministic bound for every random outcome is not asserted.

Contributions that establish the two relaxation maps, the vector identities, the Gaussian cut bound, the circuit's local energy bound, and the final expected-energy comparison all belong to this mission. Proofs of the paper's polynomial running-time claim and cited hardness results are outside the formal statements here.

Selected references

  • Eunou Lee, Optimizing quantum circuit parameters via SDP, arXiv preprint, 2022, arXiv:2209.00789v1.
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Operations ResearchOptimizationProbability·Captain: mikedeng1

Role of Risk Aversion in Price Postponement Under Supply Random Yield: Ex Ante and Responsive Pricing Share One CVaR Risk-Aversion ThresholdResearch Paper

Motivation

Many manufacturing processes deliver only a random fraction of what they start: semiconductor wafers, biologics, agricultural produce and recycled materials all suffer random yield. A firm facing yield risk has two classical levers. It can inflate production to hedge against low yield, and it can postpone pricing until the yield is observed, so that the price clears whatever was actually produced. The operations literature has long studied both levers for a risk-neutral firm, starting from the price-setting newsvendor (Petruzzi and Dada, 1999).

Real firms, and especially small producers exposed to a single bad harvest or batch, care about low-profit outcomes more than about the mean. Kouvelis, Xiao and Yang (Management Science, 2021) model this with the conditional value-at-risk (CVaR) of profit, the criterion introduced by Rockafellar and Uryasev (2000) and used for newsvendor problems by Chen, Xu and Zhang (2009). Their first finding is that a sufficiently risk-averse firm does not produce at all, and that the risk level at which production stops is the same whether or not the firm can postpone its price. This mission formalizes that finding.

Setting

A monopoly firm sells one product to a market with deterministic demand d(p)d(p)d(p), continuous and strictly decreasing in the price p∈[0,p0]p\in[0,p_0]p∈[0,p0​], where p0>0p_0>0p0​>0 is the maximal allowable price, d(p0)=0d(p_0)=0d(p0​)=0. The inverse demand p(x)p(x)p(x) satisfies p(d(p))=pp(d(p))=pp(d(p))=p and d(p(x))=xd(p(x))=xd(p(x))=x for x∈[0,d(0)]x\in[0,d(0)]x∈[0,d(0)]. Assumption 2 of the paper requires the revenue x↦p(x) xx\mapsto p(x)\,xx↦p(x)x to be concave on [0,d(0)][0,d(0)][0,d(0)].

Producing qqq units of input costs cqcqcq and yields qξq\xiqξ sellable units. The yield factor ξ\xiξ is a continuous random variable with law ν\nuν, support [l,u][l,u][l,u] with 0≤l<u≤10\le l<u\le10≤l<u≤1, c.d.f. GGG and mean μ\muμ. The cost satisfies 0≤c≤p0μ0\le c\le p_0\mu0≤c≤p0​μ, so that production is not hopeless. Write G−1(η)=inf⁡{x:G(x)≥η}G^{-1}(\eta)=\inf\{x:G(x)\ge\eta\}G−1(η)=inf{x:G(x)≥η} for the lower quantile and

g(η)=1η∫lG−1(η)ξ dG(ξ),η∈(0,1],g(\eta)=\frac1\eta\int_l^{G^{-1}(\eta)}\xi\,dG(\xi),\qquad \eta\in(0,1],g(η)=η1​∫lG−1(η)​ξdG(ξ),η∈(0,1],

for the mean of the lowest η\etaη-fraction of yields.

For a random profit π\piπ and a risk level η∈(0,1]\eta\in(0,1]η∈(0,1],

CVaRη(π)=max⁡v∈R{v+1η Emin⁡{π−v,0}},\mathrm{CVaR}_\eta(\pi)=\max_{v\in\mathbb R}\Big\{v+\frac1\eta\,\mathbb E\min\{\pi-v,0\}\Big\},CVaRη​(π)=v∈Rmax​{v+η1​Emin{π−v,0}},

the average profit over the worst η\etaη-fraction of outcomes; η=1\eta=1η=1 is risk neutrality and smaller η\etaη means more risk aversion.

Under ex ante pricing the firm picks pa∈[0,p0]p_a\in[0,p_0]pa​∈[0,p0​] and qa≥0q_a\ge0qa​≥0 before the yield realizes and maximizes Πa(pa,qa)=CVaRη(pamin⁡{d(pa),qaξ}−cqa)\Pi_a(p_a,q_a)=\mathrm{CVaR}_\eta\big(p_a\min\{d(p_a),q_a\xi\}-cq_a\big)Πa​(pa​,qa​)=CVaRη​(pa​min{d(pa​),qa​ξ}−cqa​). Under responsive pricing it picks qr≥0q_r\ge0qr​≥0, observes ξ\xiξ, then picks the revenue-maximizing price, and maximizes

Πr(qr)=CVaRη(max⁡pr∈[0,p0]prmin⁡{d(pr),qrξ}−cqr).\Pi_r(q_r)=\mathrm{CVaR}_\eta\Big(\max_{p_r\in[0,p_0]}p_r\min\{d(p_r),q_r\xi\}-cq_r\Big).Πr​(qr​)=CVaRη​(pr​∈[0,p0​]max​pr​min{d(pr​),qr​ξ}−cqr​).

Since q=0q=0q=0 gives CVaR 000, the firm produces under a scheme when some decision has strictly positive CVaR, and otherwise not producing is optimal.

Formalization targets

Goal: one threshold for both schemes (Proposition 4(i))

There is a single η∗∈[0,1]\eta^*\in[0,1]η∗∈[0,1], either η∗=0\eta^*=0η∗=0 or a solution of p0 g(η∗)=cp_0\,g(\eta^*)=cp0​g(η∗)=c, such that for every η∈(0,1]\eta\in(0,1]η∈(0,1]

ex ante firm produces  ⟺  η>η∗  ⟺  responsive firm produces.\text{ex ante firm produces}\iff\eta>\eta^*\iff\text{responsive firm produces}.ex ante firm produces⟺η>η∗⟺responsive firm produces.

This is the paper's ηa∗(p0,c)=ηr∗(p0,c)\eta_a^*(p_0,c)=\eta_r^*(p_0,c)ηa∗​(p0​,c)=ηr∗​(p0​,c), with the boundary case η=η∗\eta=\eta^*η=η∗ stated correctly (there the optimal CVaR is 000, so the firm is indifferent and "produces" in the strict sense fails).

Milestones

  1. Property 1: for a continuously distributed profit, the maximization formula equals the tail mean E[π∣π≤VaRη(π)]\mathbb E[\pi\mid\pi\le\mathrm{VaR}_\eta(\pi)]E[π∣π≤VaRη​(π)], attained at v=VaRη(π)v=\mathrm{VaR}_\eta(\pi)v=VaRη​(π).
  2. Property 2: the CVaR of a profit concave in the decision is concave in the decision.
  3. Proposition 1: at a fixed price pap_apa​, the optimal ex ante quantity is d(pa)/δd(p_a)/\deltad(pa​)/δ above a threshold price p~\tilde pp~​ and 000 below it.
  4. The tail mean ggg: strictly increasing and continuous on (0,1](0,1](0,1], with g(1)=μg(1)=\mug(1)=μ and g(0+)=lg(0^+)=lg(0+)=l.
  5. Proposition 2: the ex ante threshold ηa∗\eta_a^*ηa∗​.
  6. Lemma 1: the responsive firm's second-stage price is p(min⁡{qrξ,d∗})p(\min\{q_r\xi,d^*\})p(min{qr​ξ,d∗}), where d∗d^*d∗ maximizes revenue.
  7. Proposition 3: Πr\Pi_rΠr​ is concave and the responsive threshold ηr∗\eta_r^*ηr∗​ exists.

Significance

The result says that price postponement, although it raises the profit of a firm that does produce, does not enlarge the set of risk-averse firms willing to produce. The threshold is explicit: η∗=0\eta^*=0η∗=0 when p0l>cp_0l>cp0​l>c, and otherwise η∗\eta^*η∗ solves g(η)=c/p0g(\eta)=c/p_0g(η)=c/p0​. Because ggg depends only on the yield law, the threshold separates cost and price power (c/p0c/p_0c/p0​) from yield risk (ggg), which is what the paper's comparative statics in ccc, p0p_0p0​ and the yield distribution (Proposition 4(ii)–(iv)) build on.

The mission states the paper's threshold results and its two CVaR properties in Lean. None of them is machine-checked anywhere. Proofs of the milestones would also provide a reusable CVaR toolkit on a general probability space: the identification of the maximization formula with the lower-tail mean, and concavity of CVaR in a decision parameter.

Difficulty

The paper's argument uses densities and derivatives throughout: g′(η)>0g'(\eta)>0g′(η)>0, a first-order condition at q=0q=0q=0, L'Hospital's rule for g(0+)g(0^+)g(0+). The model here assumes only an atomless law with full support, so every such step has to be replaced by a measure-theoretic one. CVaR is a supremum of integrals over an unbounded index, so comparisons between the two schemes cannot be read off a closed form. The responsive profit is itself a maximum over prices inside an expectation inside a supremum. Finally, the two schemes have different optimal decisions everywhere except in the limit of vanishing production, so an argument that compares optimal values fails: the content is in comparing whether positive CVaR is attainable at all.

Formalization scope

  • The yield is its law ν : Measure ℝ: a probability measure without atoms (NullSingletonClass), with ν [l,u]ᶜ = 0 and positive mass on every open subinterval of [l,u]. The paper's density is not assumed. Expectations are Bochner integrals against ν.
  • p0p_0p0​ is a finite positive real (the paper also allows p0=∞p_0=\inftyp0​=∞). Demand d and inverse demand P are two functions with both inverse identities on their intervals.
  • CVaR (RiskPostpone.Threshold.cvar) is the real supremum over v∈Rv\in\mathbb Rv∈R of the bracket. The model's profits are bounded on the support, so the supremum is genuine there; the general CVaR properties assume integrability. VaR and the yield quantile use the published MultistageStochastic.valueAtRisk.
  • The responsive maximum is the sSup of the image of [0,p0][0,p_0][0,p0​], which is nonempty and bounded.
  • "Produces" is strict: some decision has CVaR >0>0>0. With ≥\ge≥ the statement would be trivially true at q=0q=0q=0; with a CVaR supremum that could be junk 000, or with two separate thresholds for the two schemes, the goal would lose its content. All three formalizations are ruled out.
  • Assumption 1 of the paper (an IGFR-type condition and increasing price elasticity) is used only for the uniqueness of the optimal ex ante price and is not assumed. Assumption 2 is stated without "twice differentiable". In Lemma 1, d∗d^*d∗ is any maximizer of revenue on [0,d(0)][0,d(0)][0,d(0)] rather than the root of the first-order condition. Proposition 1 excludes the degenerate case c=0=lc=0=lc=0=l (there the optimal quantity does not exist). Property 1 assumes the profit is integrable, essentially bounded above and atomless.
  • Not formalized: the first-order conditions of Propositions 2(ii) and 3(ii), Proposition 4(ii)–(iv), Corollaries 1–4, the linear-demand comparisons of §5.2–§5.4, and the extensions of §7.

Contributions welcome: proofs of the milestones, especially the general CVaR facts (Properties 1 and 2) and the measure-theoretic properties of ggg, which are reusable beyond this model.

Selected references

  • P. Kouvelis, G. Xiao, N. Yang, Role of Risk Aversion in Price Postponement under Supply Random Yield, Management Science 67(8), 4826–4844, 2021. https://doi.org/10.1287/mnsc.2020.3755 (formalized from the accepted manuscript MS-OPM-18-01273.R2)
  • R. T. Rockafellar, S. Uryasev, Optimization of conditional value-at-risk, Journal of Risk 2(3), 21–41, 2000. https://doi.org/10.21314/JOR.2000.038
  • R. T. Rockafellar, S. Uryasev, Conditional value-at-risk for general loss distributions, Journal of Banking & Finance 26(7), 1443–1471, 2002. https://doi.org/10.1016/S0378-4266(02)00271-6
  • Y. Chen, M. Xu, Z. G. Zhang, A risk-averse newsvendor model under the CVaR criterion, Operations Research 57(4), 1040–1044, 2009. https://doi.org/10.1287/opre.1080.0603
  • N. C. Petruzzi, M. Dada, Pricing and the newsvendor problem: a review with extensions, Operations Research 47(2), 183–194, 1999. https://doi.org/10.1287/opre.47.2.183
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Analysis·Captain: mikedeng1

Generalized Stieltjes Transforms: Basic Aspects: A Criterion of Exactness for the Stieltjes Order via Monotonicity of a Fractional Transform of the Representing MeasureResearch Paper

Motivation

The generalized Stieltjes transform of order α>0\alpha>0α>0 of a non-negative measure μ\muμ on [0,∞)[0,\infty)[0,∞) is the function z↦∫[0,∞)μ(du)/(u+z)αz\mapsto\int_{[0,\infty)}\mu(du)/(u+z)^\alphaz↦∫[0,∞)​μ(du)/(u+z)α. For α=1\alpha=1α=1 this is the classical Stieltjes transform, whose functions (Stieltjes functions) appear in moment problems, in the theory of completely monotone and Bernstein functions, in the spectral theory of positive operators, and in the functional calculus of sectorial operators. The classes of order α≠1\alpha\ne1α=1 were studied by Widder, Hirschman and Widder, Sokal, and Schwarz, among others, and appear in work on functional calculi of sectorial operators (Batty, Gomilko and Tomilov, arXiv:1309.0318).

D. Karp and E. Prilepkina, Generalized Stieltjes transforms: basic aspects (arXiv:1111.4271), collect and prove the basic real- and complex-variable properties of these classes. One elementary but structural fact is that the classes are nested: a function of order α\alphaα is also of every larger order β\betaβ. This raises a natural question that the paper answers: given fff in the class of order β\betaβ, is β\betaβ the smallest order available, or can it be lowered? The paper introduces the exact Stieltjes order and gives a criterion of exactness phrased purely in terms of the representing measure of fff. This mission formalizes that criterion (Theorem 16) together with the results its proof relies on.

Setting

For α>0\alpha>0α>0, write Mα\mathcal M_\alphaMα​ for the set of non-negative Borel measures μ\muμ on [0,∞)[0,\infty)[0,∞) with

∫[0,∞)μ(dt)(1+t)α<∞.(2)\int_{[0,\infty)}\frac{\mu(dt)}{(1+t)^\alpha}<\infty. \tag{2}∫[0,∞)​(1+t)αμ(dt)​<∞.(2)

The generalized Stieltjes class SαS_\alphaSα​ consists of the functions f:(0,∞)→Rf:(0,\infty)\to\mathbb Rf:(0,∞)→R of the form

f(z)=μ∞+∫[0,∞)μα(du)(u+z)α,z>0,f(z)=\mu_\infty+\int_{[0,\infty)}\frac{\mu_\alpha(du)}{(u+z)^\alpha},\qquad z>0,f(z)=μ∞​+∫[0,∞)​(u+z)αμα​(du)​,z>0,

with a constant μ∞≥0\mu_\infty\ge0μ∞​≥0 and μα∈Mα\mu_\alpha\in\mathcal M_\alphaμα​∈Mα​. The paper writes the atom of μα\mu_\alphaμα​ at 000 separately as a term μ0/zα\mu_0/z^\alphaμ0​/zα (its formula (1)); here it is part of μα\mu_\alphaμα​. The pair (μ∞,μα)(\mu_\infty,\mu_\alpha)(μ∞​,μα​) is a representation of fff in SαS_\alphaSα​, and μα\mu_\alphaμα​ is its representing measure. Write S∞=⋃α>0SαS_\infty=\bigcup_{\alpha>0}S_\alphaS∞​=⋃α>0​Sα​.

For a measure μ\muμ on [0,∞)[0,\infty)[0,∞), its left-continuous distribution function is Fμ(y)=μ([0,y))F_\mu(y)=\mu([0,y))Fμ​(y)=μ([0,y)), so Fμ(0)=0F_\mu(0)=0Fμ​(0)=0. For η>0\eta>0η>0, the left-sided Riemann–Liouville fractional integral Iη+μI^+_\eta\muIη+​μ (Definition A1) is the measure on [0,∞)[0,\infty)[0,∞) with Lebesgue density

y⟼1Γ(η)∫[0,y)μ(du)(y−u)1−η(y>0).y\longmapsto\frac{1}{\Gamma(\eta)}\int_{[0,y)}\frac{\mu(du)}{(y-u)^{1-\eta}}\qquad(y>0).y⟼Γ(η)1​∫[0,y)​(y−u)1−ημ(du)​(y>0).

The exact Stieltjes order of f∈S∞f\in S_\inftyf∈S∞​ is

α∗[f]=inf⁡{α>0: f∈Sα}.(24)\alpha^*[f]=\inf\{\alpha>0:\ f\in S_\alpha\}. \tag{24}α∗[f]=inf{α>0: f∈Sα​}.(24)

Finally, for f∈Sβf\in S_\betaf∈Sβ​ with representing measure μβ\mu_\betaμβ​ and a parameter ε\varepsilonε, set

Φ(y)=∫[0,y)μβ(du)(y−u)ε,y≥0.(25)\Phi(y)=\int_{[0,y)}\frac{\mu_\beta(du)}{(y-u)^{\varepsilon}},\qquad y\ge0. \tag{25}Φ(y)=∫[0,y)​(y−u)εμβ​(du)​,y≥0.(25)

Formalization targets

Goal: Theorem 16 (criterion of exactness)

For β>0\beta>0β>0 and f∈Sβf\in S_\betaf∈Sβ​ with representing measure μβ\mu_\betaμβ​,

β>α∗[f]  ⟺  Φ is non-decreasing on (0,∞) for some ε∈(0,min⁡{β,1}).\beta>\alpha^*[f]\iff \Phi\ \text{is non-decreasing on }(0,\infty)\ \text{for some}\ \varepsilon\in(0,\min\{\beta,1\}).β>α∗[f]⟺Φ is non-decreasing on (0,∞) for some ε∈(0,min{β,1}).

The order β\betaβ is exact precisely when no admissible ε\varepsilonε makes Φ\PhiΦ monotone.

Milestones

  1. Formula (12). For 0<α<β0<\alpha<\beta0<α<β, z>0z>0z>0, u≥0u\ge0u≥0:
1(u+z)α=Γ(β)Γ(α)Γ(β−α)∫(0,∞)tβ−α−1 dt(z+u+t)β.\frac{1}{(u+z)^\alpha}=\frac{\Gamma(\beta)}{\Gamma(\alpha)\Gamma(\beta-\alpha)}\int_{(0,\infty)}\frac{t^{\beta-\alpha-1}\,dt}{(z+u+t)^\beta}.(u+z)α1​=Γ(α)Γ(β−α)Γ(β)​∫(0,∞)​(z+u+t)βtβ−α−1dt​.
  1. Theorem 3, first part. For 0<α<β0<\alpha<\beta0<α<β, Sα⊂SβS_\alpha\subset S_\betaSα​⊂Sβ​; explicitly, f∈Sαf\in S_\alphaf∈Sα​ is represented in SβS_\betaSβ​ with the same μ∞\mu_\inftyμ∞​ and
μβ(dy)=Γ(β) dyΓ(α)Γ(β−α)∫[0,y)μα(du)(y−u)α+1−β.(10)\mu_\beta(dy)=\frac{\Gamma(\beta)\,dy}{\Gamma(\alpha)\Gamma(\beta-\alpha)}\int_{[0,y)}\frac{\mu_\alpha(du)}{(y-u)^{\alpha+1-\beta}}. \tag{10}μβ​(dy)=Γ(α)Γ(β−α)Γ(β)dy​∫[0,y)​(y−u)α+1−βμα​(du)​.(10)
  1. Theorem A1, first part. Iη+I^+_\etaIη+​ maps Mα\mathcal M_\alphaMα​ into Mα+η\mathcal M_{\alpha+\eta}Mα+η​.
  2. Theorem A1, inversion (29), case 0<η<10<\eta<10<η<1. Fμ(y)=1Γ(1−η)∫[0,y)(Iη+μ)(du)(y−u)ηF_\mu(y)=\frac{1}{\Gamma(1-\eta)}\int_{[0,y)}\frac{(I^+_\eta\mu)(du)}{(y-u)^{\eta}}Fμ​(y)=Γ(1−η)1​∫[0,y)​(y−u)η(Iη+​μ)(du)​ for all y≥0y\ge0y≥0.
  3. Theorem 3, inversion (11), case 0<β−α<10<\beta-\alpha<10<β−α<1. If f∈Sαf\in S_\alphaf∈Sα​ has representing measure μα\mu_\alphaμα​ and any representation (μ∞′,μβ)(\mu'_\infty,\mu_\beta)(μ∞′​,μβ​) in SβS_\betaSβ​, then μ∞′=μ∞\mu'_\infty=\mu_\inftyμ∞′​=μ∞​ and
Fμα(y)=Γ(α)Γ(β)Γ(α−β+1)∫[0,y)μβ(du)(y−u)β−α.F_{\mu_\alpha}(y)=\frac{\Gamma(\alpha)}{\Gamma(\beta)\Gamma(\alpha-\beta+1)}\int_{[0,y)}\frac{\mu_\beta(du)}{(y-u)^{\beta-\alpha}}.Fμα​​(y)=Γ(β)Γ(α−β+1)Γ(α)​∫[0,y)​(y−u)β−αμβ​(du)​.
  1. Claim (26). If Φ=Fν\Phi=F_\nuΦ=Fν​ and ∫[0,∞)Φ(y) dy/(1+y)α+1<∞\int_{[0,\infty)}\Phi(y)\,dy/(1+y)^{\alpha+1}<\infty∫[0,∞)​Φ(y)dy/(1+y)α+1<∞, then ∫[0,∞)dΦ(y)/(1+y)α<∞\int_{[0,\infty)}d\Phi(y)/(1+y)^\alpha<\infty∫[0,∞)​dΦ(y)/(1+y)α<∞ and Φ(t)(1+t)−α→0\Phi(t)(1+t)^{-\alpha}\to0Φ(t)(1+t)−α→0.

Significance

The result. Theorem 16 reduces the question "is the order of fff optimal?" to a monotonicity test on a single function built from the representing measure. The paper derives two practical corollaries from it: if Φ(2y)/Φ(y)\Phi(2y)/\Phi(y)Φ(2y)/Φ(y) has a limit below 111, then β\betaβ is exact (Corollary 1), and if μβ\mu_\betaμβ​ has compact support, then β\betaβ is exact (Corollary 2). Both are immediate once Theorem 16 is available and are natural follow-up targets. The milestones are of independent use: Theorem 3 is the nesting of the classes with an explicit formula for the new representing measure, and Theorem A1 is the integrability and inversion theory of fractional integrals of measures, which the paper's appendix develops because the authors found no reference treating measures rather than functions.

Formalizing it. The results are proved in the paper; none is formalized. The platform has the generalized Stieltjes class itself (a published definition from the Batty–Gomilko–Tomilov formalization) and the half-line Beta integral, but no fractional integrals of measures, no inversion formula, and nothing on the exact order. A complete development provides a reusable Riemann–Liouville calculus for measures on the half-line and the uniqueness of the representing measure in SβS_\betaSβ​, which milestone 5 contains.

Difficulty

The forward direction of Theorem 16 looks like a computation: pass from β\betaβ to a smaller order and read off the measure. The obstacle is that one must know that the representing measure in SβS_\betaSβ​ is unique, since Φ\PhiΦ is built from the representing measure and the inversion formula (11) must apply to it; milestone 5 states the inversion for an arbitrary representing measure for this reason. The converse direction must produce a measure from a function: a non-decreasing Φ\PhiΦ is a distribution function, and one must show the resulting measure satisfies (2) at the lower order, which is claim (26) and needs a careful tail estimate rather than a direct comparison. Throughout, interchanges of integration are carried out for measures with atoms (including an atom at 000), where the naive differentiation formula of (11) and (29) for higher nnn breaks down at jumps.

Formalization scope

Functions are real-valued on (0,∞)(0,\infty)(0,∞) (PositiveReal), and the classes and representations are the published StieltjesClass and StieltjesRepresentation (QAlgorithms_Papers_Independent_Renew46_P11), reused unchanged. Representing measures are measures on ℝ≥0; the paper's atom at +∞+\infty+∞ is the constant μ∞\mu_\inftyμ∞​. All orders α,β,η\alpha,\beta,\etaα,β,η are positive. All kernel integrals and the functions FμF_\muFμ​ and Φ\PhiΦ take values in [0,∞][0,\infty][0,∞] (lower Lebesgue integrals), so a divergent integral is +∞+\infty+∞, not 000; "non-decreasing" is monotonicity in [0,∞][0,\infty][0,∞]. The exact order is the real infimum of {α>0:f∈Sα}\{\alpha>0: f\in S_\alpha\}{α>0:f∈Sα​}, which is nonempty and bounded below whenever f∈Sβf\in S_\betaf∈Sβ​. Densities are with respect to Lebesgue measure on (0,∞)(0,\infty)(0,∞) pushed to ℝ≥0.

Corrected readings, each disclosed in the item: (25) is taken over [0,y)[0,y)[0,y), while the paper prints (0,y)(0,y)(0,y); with (0,y)(0,y)(0,y) the theorem fails for f(z)=z−βf(z)=z^{-\beta}f(z)=z−β, whose representing measure is the unit mass at 000. Formulas (11) and (29) are stated only for n=0n=0n=0, the case Theorem 16 uses; as printed for n≥1n\ge1n≥1 they differentiate a function at its jumps. Claim (26) is stated for the distribution function of an arbitrary measure, the generality its proof gives.

A trivializing formalization is ruled out: Φ\PhiΦ must be built from the representing measure of the given fff (not from an arbitrary measure), over [0,y)[0,y)[0,y) (over (0,y)(0,y)(0,y) an atom at 000 makes Φ\PhiΦ identically 000), and in [0,∞][0,\infty][0,∞] (a real-valued Bochner Φ\PhiΦ would be 000 wherever the integral diverges).

Contributions welcome: proofs of any milestone, a reusable Riemann–Liouville integral of measures on ℝ≥0 with its Tonelli computations, uniqueness of generalized Stieltjes representations, and the corollaries of Theorem 16.

Selected references

  • D. Karp, E. Prilepkina, Generalized Stieltjes transforms: basic aspects, arXiv:1111.4271v2, 2012. https://arxiv.org/abs/1111.4271
  • C. Batty, A. Gomilko, Yu. Tomilov, Product formulas in functional calculi for sectorial operators, arXiv:1309.0318. https://arxiv.org/abs/1309.0318
  • A. D. Sokal, Real-variables characterization of generalized Stieltjes functions, Expositiones Mathematicae 28 (2010), 179–185.
  • J. H. Schwarz, The generalized Stieltjes transform and its inverse, J. Math. Phys. 46, 013501 (2005).
  • D. V. Widder, The Stieltjes transform, Trans. Amer. Math. Soc. 43 (1938), 7–60.
  • S. G. Samko, A. A. Kilbas, O. I. Marichev, Fractional Integrals and Derivatives: Theory and Applications, Gordon and Breach, 1993.
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Entanglement measures and their properties in quantum field theory: In a CFT the Vacuum Relative Entanglement Entropy of a Ball and the Outside of a Larger Concentric Ball Is ≤ ln Tr (r/R)^{½(P⁰+K⁰)}Research Paper

Motivation

In quantum field theory the vacuum is entangled between any two regions of space, and the amount of entanglement between nearby regions is infinite: the algebras of observables of regions that touch admit no normal separable state at all. For regions at a positive distance the question becomes quantitative. How much entanglement does the vacuum carry between a region and a second region at distance δ\deltaδ, and how does it depend on δ\deltaδ and on the field content of the theory? Questions of this type underlie area laws for entanglement entropy, the thermodynamics of black holes, and the information-theoretic approach to quantum field theory.

S. Hollands and K. Sanders, Entanglement measures and their properties in quantum field theory (arXiv:1702.04924, SpringerBriefs in Mathematical Physics, 2018), define entanglement measures directly on the von Neumann algebras of local observables, without assuming a tensor product structure, and prove upper and lower bounds for them in several classes of theories. For conformal field theories in d+1d+1d+1 dimensions, d>1d>1d>1, they bound the relative entanglement entropy of the vacuum between a ball of radius rrr and the outside of a concentric ball of radius R>rR>rR>r by the partition function of the conformal Hamiltonian (Theorem 13, p. 79).

Setting

Let H\mathcal HH be a Hilbert space and AA,AB⊆B(H)\mathfrak A_A,\mathfrak A_B\subseteq B(\mathcal H)AA​,AB​⊆B(H) commuting von Neumann algebras, with join AA∨AB=(AA∪AB)′′\mathfrak A_A\vee\mathfrak A_B=(\mathfrak A_A\cup\mathfrak A_B)''AA​∨AB​=(AA​∪AB​)′′. A normal state σ\sigmaσ on the join is separable if σ(ab)=∑jφj(a)ψj(b)\sigma(ab)=\sum_j\varphi_j(a)\psi_j(b)σ(ab)=∑j​φj​(a)ψj​(b) for a∈AAa\in\mathfrak A_Aa∈AA​, b∈ABb\in\mathfrak A_Bb∈AB​, with positive normal functionals φj,ψj\varphi_j,\psi_jφj​,ψj​ and ∑jφj(1)ψj(1)<∞\sum_j\varphi_j(1)\psi_j(1)<\infty∑j​φj​(1)ψj​(1)<∞. Araki's relative entropy H(ω,σ)∈(−∞,∞]H(\omega,\sigma)\in(-\infty,\infty]H(ω,σ)∈(−∞,∞] of two positive normal functionals generalizes Tr⁡ρ(ln⁡ρ−ln⁡ρ′)\operatorname{Tr}\rho(\ln\rho-\ln\rho')Trρ(lnρ−lnρ′). The relative entanglement entropy of a normal state ω\omegaω is

ER(ω)=inf⁡{H(ω,σ):σ a separable state},E_R(\omega)=\inf\{H(\omega,\sigma):\sigma\text{ a separable state}\},ER​(ω)=inf{H(ω,σ):σ a separable state},

equal to +∞+\infty+∞ when there is no separable state. Two auxiliary measures enter: the logarithmic dominance EN(ω)=inf⁡{ln⁡σ(1):σ⩾ω, σ separable}E_N(\omega)=\inf\{\ln\sigma(1):\sigma\geqslant\omega,\ \sigma\text{ separable}\}EN​(ω)=inf{lnσ(1):σ⩾ω, σ separable}, and the modular entanglement measure EM(ω)=ln⁡min⁡(∥ΨA∥1,∥ΨB∥1)E_M(\omega)=\ln\min(\|\Psi^A\|_1,\|\Psi^B\|_1)EM​(ω)=lnmin(∥ΨA∥1​,∥ΨB∥1​), where ΨA(a)=Δ1/4aΩ\Psi^A(a)=\Delta^{1/4}a\OmegaΨA(a)=Δ1/4aΩ, Δ\DeltaΔ is the modular operator of AB′\mathfrak A_B'AB′​ at the vector Ω\OmegaΩ of ω\omegaω, and ∥⋅∥1\|\cdot\|_1∥⋅∥1​ is the 1-nuclear norm.

A conformal field theory in d+1d+1d+1 dimensions is given, in its vacuum representation, by a net O↦A(O)O\mapsto\mathfrak A(O)O↦A(O) of von Neumann algebras on a Hilbert space H0\mathcal H_0H0​ indexed by causal diamonds OOO of Minkowski space Rd,1\mathbb R^{d,1}Rd,1, a unitary representation UUU of a covering group G~\tilde GG~ of the conformal group SO+(d+1,2)/Z2SO_+(d+1,2)/\mathbb Z_2SO+​(d+1,2)/Z2​ that acts covariantly on the net, and an invariant vacuum vector ∣0⟩|0\rangle∣0⟩ with vacuum state ω0\omega_0ω0​. The conformal Hamiltonian 12(P0+K0)\tfrac12(P^0+K^0)21​(P0+K0) is the generator of the rotation M0(d+2)M_{0(d+2)}M0(d+2)​ of so(d+1,2)\mathfrak{so}(d+1,2)so(d+1,2), the sum of the energy P0≥0P^0\geq0P0≥0 and the generator K0K^0K0 of special conformal transformations in the time direction; DDD generates dilations. For R>r>0R>r>0R>r>0, AA\mathfrak A_AAA​ is the algebra of the double cone over the ball of radius rrr about the origin, and AB\mathfrak A_BAB​ that of the domain of dependence of the complement of the ball of radius RRR.

Formalization targets

Goal: Theorem 13

ER(ω0)⩽ln⁡Tr⁡(rR)12(P0+K0)(210)E_R(\omega_0)\leqslant\ln\operatorname{Tr}\Big(\frac rR\Big)^{\frac12(P^0+K^0)}\qquad(210)ER​(ω0​)⩽lnTr(Rr​)21​(P0+K0)(210)

for every conformal field theory satisfying the axioms, every d≥2d\ge2d≥2 and every 0<r<R0<r<R0<r<R. The right side is +∞+\infty+∞ when the trace diverges.

Milestones

  1. Theorem 3: ER(ω)≤EN(ω)E_R(\omega)\le E_N(\omega)ER​(ω)≤EN​(ω).
  2. Lemma 3: if ∥ΨA∥1<∞\|\Psi^A\|_1<\infty∥ΨA∥1​<∞, then ω(ab)=∑jφj(a)ψj(b)\omega(ab)=\sum_j\varphi_j(a)\psi_j(b)ω(ab)=∑j​φj​(a)ψj​(b) with normal φj,ψj\varphi_j,\psi_jφj​,ψj​ and ∑j∥φj∥∥ψj∥<∥ΨA∥1+ε\sum_j\|\varphi_j\|\|\psi_j\|<\|\Psi^A\|_1+\varepsilon∑j​∥φj​∥∥ψj​∥<∥ΨA∥1​+ε.
  3. Lemma 4: such a decomposition yields a separable σ⩾ω\sigma\geqslant\omegaσ⩾ω with ∥σ∥=∑j∥φj∥∥ψj∥\|\sigma\|=\sum_j\|\varphi_j\|\|\psi_j\|∥σ∥=∑j​∥φj​∥∥ψj​∥.
  4. Theorem 4: EN(ω)≤EM(ω)E_N(\omega)\le E_M(\omega)EN​(ω)≤EM​(ω).
  5. ∥ΨA∥1≤∥ΦA∥1\|\Psi^A\|_1\le\|\Phi^A\|_1∥ΨA∥1​≤∥ΦA∥1​, with ΦA(a)=ΔB′1/4a∣0⟩\Phi^A(a)=\Delta_{B'}^{1/4}a|0\rangleΦA(a)=ΔB′1/4​a∣0⟩ for the larger algebra AB′⊆AB′\mathfrak A_{B'}\subseteq\mathfrak A_B'AB′​⊆AB′​ (p. 56).
  6. ∥Δ1/4aΩ∥≤∥a∥\|\Delta^{1/4}a\Omega\|\le\|a\|∥Δ1/4aΩ∥≤∥a∥ for any von Neumann algebra with cyclic and separating Ω\OmegaΩ (proof of Theorem 13, p. 80).
  7. Lemma 13: ΔB′iteisDΔB′−it=exp⁡[−is2sinh⁡(2πt)(P0+K0)+iscosh⁡(2πt)D]\Delta_{B'}^{it}e^{isD}\Delta_{B'}^{-it}=\exp[-\tfrac{is}2\sinh(2\pi t)(P^0+K^0)+is\cosh(2\pi t)D]ΔB′it​eisDΔB′−it​=exp[−2is​sinh(2πt)(P0+K0)+iscosh(2πt)D].
  8. (219): ΔA=e−i(ln⁡r)DΔB′ei(ln⁡r)D\Delta_A=e^{-i(\ln r)D}\Delta_{B'}e^{i(\ln r)D}ΔA​=e−i(lnr)DΔB′​ei(lnr)D.
  9. (212): ΔB′1/4ΔA−1/4=r12(P0+K0)riD\Delta_{B'}^{1/4}\Delta_A^{-1/4}=r^{\frac12(P^0+K^0)}r^{iD}ΔB′1/4​ΔA−1/4​=r21​(P0+K0)riD.

Significance

Theorem 13 bounds the vacuum entanglement of two regions by a quantity of the theory's spectrum alone. Combined with the paper's identification of Tr⁡r12(P0+K0)\operatorname{Tr}r^{\frac12(P^0+K^0)}Trr21​(P0+K0) with ∑OrdO\sum_{O}r^{d_O}∑O​rdO​ over the spectrum of operator dimensions (Theorem 14, p. 83), it shows that for R≫rR\gg rR≫r the entanglement decays like (r/R)dO(r/R)^{d_O}(r/R)dO​ with dOd_OdO​ the smallest non-zero dimension, and for r→Rr\to Rr→R it diverges at most like (ln⁡(R/r))−d(\ln(R/r))^{-d}(ln(R/r))−d. The general results on the way, ER≤EN≤EME_R\le E_N\le E_MER​≤EN​≤EM​ and the nuclearity estimates, apply to any pair of commuting von Neumann algebras and underlie all upper bounds of the paper, including those for free and integrable models.

The results are proved in the paper, at the level of rigour of mathematical physics, with some steps cited (the Hislop–Longo theorem, the Heinz–Löwner inequality for unbounded operators, the edge-of-the-wedge theorem, the Reeh–Schlieder theorem). None of them is machine-checked. A formal proof would also make precise which axioms each step uses, for instance where statistical independence of AA\mathfrak A_AAA​ and AB\mathfrak A_BAB​, which is not an axiom here, enters.

Difficulty

The obvious route, comparing the vacuum with product states through a tensor product decomposition H0=HA⊗HB\mathcal H_0=\mathcal H_A\otimes\mathcal H_BH0​=HA​⊗HB​, is not available: the local algebras are type III factors and there is no such decomposition. Every step must work with modular operators of the local algebras and normal functionals on their join. The analytic core is the operator identity (212): ΔB′1/4\Delta_{B'}^{1/4}ΔB′1/4​ and ΔA−1/4\Delta_A^{-1/4}ΔA−1/4​ are unbounded, Lemma 13 holds for real ttt only, and reaching t=−i/4t=-i/4t=−i/4 requires analytic continuation in a strip, domain control through the Heinz–Löwner inequality, and the edge-of-the-wedge theorem. Separately, EN≤EME_N\le E_MEN​≤EM​ needs that products of normal functionals on AA\mathfrak A_AAA​ and AB\mathfrak A_BAB​ are normal on the join, which in the conformal setting follows from modular nuclearity rather than from an axiom.

Formalization scope

The general layer (Definitions 5, 7, 10–13) is stated for von Neumann algebras AA,AB⊆B(H)\mathfrak A_A,\mathfrak A_B\subseteq B(\mathcal H)AA​,AB​⊆B(H) in Mathlib's VonNeumannAlgebra, with functionals as maps B(H)→CB(\mathcal H)\to\mathbb CB(H)→C of which only the values on the relevant algebra matter. Normal functionals are given by vector sums ∑n⟨ξn,aηn⟩\sum_n\langle\xi_n,a\eta_n\rangle∑n​⟨ξn​,aηn​⟩. The relative entropy is Araki's, in Kosaki's variational form, which is defined for all pairs of positive normal functionals. HHH, ERE_RER​, ENE_NEN​, EME_MEM​ take values in EReal and norms in ℝ≥0∞, so empty infima are +∞+\infty+∞, as Definitions 5, 12 and 13 require. Separability is defined on the join, as in Theorem 2 c); no split property is assumed in the goal. Lemma 4 and Theorem 4 carry the §3 standing assumption of statistical independence, in the form that products of positive normal functionals are normal on the join. Modular operators are the published StandardModularData of BoundedRecovery; Δ1/4\Delta^{1/4}Δ1/4 is the limit of spectral cut-offs.

The conformal layer is a structure CFTVacuum d H₀: the net with isotony and locality (the algebra of a region such as OBO_BOB​ contains those of the double cones inside it and commutes with those spacelike to it, without an additivity assumption the paper does not make) and weak additivity; a covering group of SO+(d+1,2)SO_+(d+1,2)SO+​(d+1,2) presented by a covering homomorphism with discrete kernel and an exponential map; a strongly continuous unitary representation with local covariance a3′); a unique invariant vacuum vector, cyclic for the quasi-local algebra (the GNS representation of a4′)); the generators P0≥0P^0\ge0P0≥0, 12(P0+K0)\tfrac12(P^0+K^0)21​(P0+K0) and DDD as spectral calculi; and the Hislop–Longo theorem for the unit double cone as a disclosed field. The projective representation of the paper is taken as a true representation of the cover (Bargmann). Generator signs are fixed so that P0P^0P0 generates forward time translations and eisDe^{isD}eisD shrinks regions, consistent with (217), (219) and p. 84. (r/R)12(P0+K0)(r/R)^{\frac12(P^0+K^0)}(r/R)21​(P0+K0) is the bounded function u↦(r/R)max⁡(u,0)u\mapsto(r/R)^{\max(u,0)}u↦(r/R)max(u,0) of the conformal Hamiltonian, whose spectrum is non-negative (footnote 42), and the trace is taken in [0,∞][0,\infty][0,∞]. The goal assumes d≥2d\ge2d≥2 (§4.4, p. 78).

No conclusion of the paper is a field of the structure: not modular nuclearity a5′), not the split property, not (212) or (219), so the goal is not a restatement of its hypotheses. Theorem 14 (the field-content form ln⁡∑O∈Φ(r/R)dO\ln\sum_{O\in\Phi}(r/R)^{d_O}ln∑O∈Φ​(r/R)dO​) is not stated: a faithful encoding of the operator-valued fields, their conformal transformation law (224) and descendants is left for a later mission.

Reusable beyond this mission: the entanglement measures on general von Neumann algebras, the 1-nuclear norm, Δ1/4\Delta^{1/4}Δ1/4, and the conformal structure. Contributions are welcome on the Kosaki formula (scaling, monotonicity, H(ω,ω)=0H(\omega,\omega)=0H(ω,ω)=0), on Heinz–Löwner for unbounded operators, and on the analytic continuation of modular groups.

Selected references

  • S. Hollands, K. Sanders, Entanglement measures and their properties in quantum field theory, SpringerBriefs in Mathematical Physics, 2018. arXiv:1702.04924v3
  • H. Araki, Relative entropy of states of von Neumann algebras, Publ. RIMS 11 (1976). doi:10.2977/prims/1195191148
  • H. Kosaki, Relative entropy of states: a variational expression, J. Operator Theory 16 (1986). jot
  • P. D. Hislop, R. Longo, Modular structure of the local algebras associated with the free massless scalar field theory, Comm. Math. Phys. 84 (1982). doi:10.1007/BF01208373
  • R. Brunetti, D. Guido, R. Longo, Modular structure and duality in conformal quantum field theory, Comm. Math. Phys. 156 (1993). doi:10.1007/BF02096738
  • D. Buchholz, C. D'Antoni, R. Longo, Nuclear maps and modular structures I, J. Funct. Anal. 88 (1990). doi:10.1016/0022-1236(90)90104-S
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AnalysisFunctional AnalysisLinear algebra·Captain: mikedeng1

Noncommutative Lp modules: Every Lp Module over a Finite-Dimensional von Neumann Algebra Is Isometrically Isomorphic, as a Module, to a Principal Column Sum of Projected Lp SpacesResearch Paper

Motivation

A Hilbert space has an orthonormal basis, so every Hilbert space is isometric to some ℓ2(I)\ell^2(I)ℓ2(I). Hilbert C∗^*∗-modules, the analogue of Hilbert spaces in which the inner product takes values in an operator algebra, have no such basis in general. Over a von Neumann algebra M\mathcal MM, Paschke showed that the self-dual Hilbert C∗^*∗-modules are exactly the "ultraweak direct sums" of corners qαMq_\alpha\mathcal Mqα​M cut by projections qα∈Mq_\alpha\in\mathcal Mqα​∈M (Paschke, Trans. AMS 182, 1973).

Junge and Sherman (arXiv:math/0301044v2, 2003, revised 2004) carried this picture to the noncommutative LpL^pLp spaces Lp(M)L^p(\mathcal M)Lp(M), 0<p≤∞0<p\le\infty0<p≤∞. They introduced LpL^pLp modules, whose inner product takes values in Lp/2(M)L^{p/2}(\mathcal M)Lp/2(M), and proved that every LpL^pLp module is a column sum of corners qαLp(M)q_\alpha L^p(\mathcal M)qα​Lp(M). The result organizes the study of module maps between noncommutative LpL^pLp spaces (the paper's §5–§6 on commutants and LpL^pLp bimodules build on it), and it is the LpL^pLp form of the orthonormal-basis theorem. Earlier, Junge had proved a version for a special class of LpL^pLp modules ([J1, Prop. 2.8]).

Setting

Let n∈Nn\in\mathbb Nn∈N and let M\mathcal MM be a unital ∗*∗-subalgebra of the matrix algebra Mn(C)M_n(\mathbb C)Mn​(C); these are exactly the finite-dimensional von Neumann algebras. For real 0<p<∞0<p<\infty0<p<∞, Lp(M)L^p(\mathcal M)Lp(M) is M\mathcal MM with the tracial (quasi)norm

∥a∥p=(Tr (a∗a)p/2)1/p.\|a\|_p=\big(\mathrm{Tr}\,(a^*a)^{p/2}\big)^{1/p}.∥a∥p​=(Tr(a∗a)p/2)1/p.

In the Lean files this is lpNorm p a, the published Schatten norm schattenNorm.

Let X\mathfrak XX be a complex vector space with a right action (ξ,x)↦ξx(\xi,x)\mapsto\xi x(ξ,x)↦ξx of M\mathcal MM (act). An Lp/2L^{p/2}Lp/2-valued inner product (Definition 2.1) is a map ⟨⋅,⋅⟩:X×X→M\langle\cdot,\cdot\rangle:\mathfrak X\times\mathfrak X\to\mathcal M⟨⋅,⋅⟩:X×X→M (ip). It is conjugate linear in the first variable and linear in the second, and satisfies

⟨ξ,ηx⟩=⟨ξ,η⟩x,⟨ξ,η⟩=⟨η,ξ⟩∗,⟨ξ,ξ⟩≥0,⟨ξ,ξ⟩=0  ⟺  ξ=0.\langle\xi,\eta x\rangle=\langle\xi,\eta\rangle x,\qquad\langle\xi,\eta\rangle=\langle\eta,\xi\rangle^*,\qquad\langle\xi,\xi\rangle\ge0,\quad\langle\xi,\xi\rangle=0\iff\xi=0.⟨ξ,ηx⟩=⟨ξ,η⟩x,⟨ξ,η⟩=⟨η,ξ⟩∗,⟨ξ,ξ⟩≥0,⟨ξ,ξ⟩=0⟺ξ=0.

It induces

∥ξ∥=∥⟨ξ,ξ⟩1/2∥p=(Tr ⟨ξ,ξ⟩p/2)1/p\|\xi\|=\big\|\langle\xi,\xi\rangle^{1/2}\big\|_p=\big(\mathrm{Tr}\,\langle\xi,\xi\rangle^{p/2}\big)^{1/p}∥ξ∥=​⟨ξ,ξ⟩1/2​p​=(Tr⟨ξ,ξ⟩p/2)1/p

(gauge p ip ξ). By Proposition 2.2 this is a norm for p≥2p\ge2p≥2 and a p/2p/2p/2-norm for p≤2p\le2p≤2. A right LpL^pLp M\mathcal MM-module (Definition 2.3) is such an X\mathfrak XX that is complete in ∥⋅∥\|\cdot\|∥⋅∥.

Given projections (qα)α∈I(q_\alpha)_{\alpha\in I}(qα​)α∈I​ of M\mathcal MM, the column sum (2.4) is

⨁cqαLp={(ξα)α∈I: ξα∈qαLp, ∑αξα∗ξα converges},⟨(ξα),(ηα)⟩=∑αξα∗ηα.\textstyle\bigoplus_c q_\alpha L^p=\Big\{(\xi_\alpha)_{\alpha\in I}:\ \xi_\alpha\in q_\alpha L^p,\ \sum_\alpha\xi_\alpha^*\xi_\alpha\ \text{converges}\Big\},\qquad\langle(\xi_\alpha),(\eta_\alpha)\rangle=\sum_\alpha\xi_\alpha^*\eta_\alpha.⨁c​qα​Lp={(ξα​)α∈I​: ξα​∈qα​Lp, ∑α​ξα∗​ξα​ converges},⟨(ξα​),(ηα​)⟩=∑α​ξα∗​ηα​.

In Lean this is columnSumSet M q with colIp. The paper calls these modules principal.

Formalization targets

Goal: Theorem 2.5

For every right LpL^pLp M\mathcal MM-module X\mathfrak XX there are an index set III, projections (qα)(q_\alpha)(qα​) of M\mathcal MM and a map T:X→⨁cqαLpT:\mathfrak X\to\bigoplus_c q_\alpha L^pT:X→⨁c​qα​Lp with the following properties: TTT is bijective, complex linear and a module map, and

∥(∑αT(ξ)α∗T(ξ)α)1/2∥p=∥⟨ξ,ξ⟩1/2∥p(ξ∈X).\Big\|\Big(\sum_\alpha T(\xi)_\alpha^*T(\xi)_\alpha\Big)^{1/2}\Big\|_p=\big\|\langle\xi,\xi\rangle^{1/2}\big\|_p\qquad(\xi\in\mathfrak X).​(α∑​T(ξ)α∗​T(ξ)α​)1/2​p​=​⟨ξ,ξ⟩1/2​p​(ξ∈X).

This is the paper's statement as printed: "isometrically isomorphic, as a module". The index set and the projections are not fixed; they are part of the conclusion.

Milestones

  1. Lemma 1.2: Mφ1/p‾=Lps(φ)\overline{\mathcal M\varphi^{1/p}}=L^ps(\varphi)Mφ1/p​=Lps(φ) and φ1/pM‾=s(φ)Lp\overline{\varphi^{1/p}\mathcal M}=s(\varphi)L^pφ1/pM​=s(φ)Lp.
  2. Lemma 1.4: a bounded compatible net ξα=ξαpα\xi_\alpha=\xi_\alpha p_\alphaξα​=ξα​pα​, ξβpα=ξα\xi_\beta p_\alpha=\xi_\alphaξβ​pα​=ξα​ (α<β)(\alpha<\beta)(α<β) in LrL^rLr, r<∞r<\inftyr<∞, converges in norm.
  3. Proposition 2.2: ⟨ξ,η⟩=⟨ξ,ξ⟩1/2T⟨η,η⟩1/2\langle\xi,\eta\rangle=\langle\xi,\xi\rangle^{1/2}T\langle\eta,\eta\rangle^{1/2}⟨ξ,η⟩=⟨ξ,ξ⟩1/2T⟨η,η⟩1/2 with ∥T∥≤1\|T\|\le1∥T∥≤1; ∥⟨ξ,η⟩∥p/2≤∥ξ∥∥η∥\|\langle\xi,\eta\rangle\|_{p/2}\le\|\xi\|\|\eta\|∥⟨ξ,η⟩∥p/2​≤∥ξ∥∥η∥; and ∥⋅∥\|\cdot\|∥⋅∥ is a norm (p≥2p\ge2p≥2) or a p/2p/2p/2-norm (p≤2p\le2p≤2).
  4. (2.4): the column sum is a right LpL^pLp module.
  5. The cyclic case: ξM‾≅s(⟨ξ,ξ⟩1/2)Lp\overline{\xi\mathcal M}\cong s(\langle\xi,\xi\rangle^{1/2})L^pξM​≅s(⟨ξ,ξ⟩1/2)Lp.
  6. Case 2 (p>2p>2p>2): the closed span of an orthogonal family is isomorphic to a column sum, and a vector with 000 as best approximant from that span is orthogonal to the family.

Significance

Theorem 2.5 reduces questions about arbitrary LpL^pLp modules to columns of corners of Lp(M)L^p(\mathcal M)Lp(M). Two consequences follow. Module maps between LpL^pLp modules become matrices of maps between corners, and the paper identifies the commutant of the right action and describes LpL^pLp bimodules in this way. For p=2p=2p=2 the theorem is the orthonormal-basis theorem with M\mathcal MM-valued inner products; for p=∞p=\inftyp=∞ it is Paschke's theorem. In between, there is no Hilbert-space structure to fall back on.

The result is proved in the paper for every von Neumann algebra and every 0<p≤∞0<p\le\infty0<p≤∞. No part of it has been formalized. Mathlib has Hilbert C∗^*∗-modules with the C∗^*∗-norm and the Hermitian functional calculus for matrices, but no noncommutative LpL^pLp spaces, no LpL^pLp modules and no column sums. This mission produces the finite-dimensional theory: the definitions, the Cauchy–Schwarz inequality (2.1)–(2.2) for Lp/2L^{p/2}Lp/2-valued inner products, the column-sum construction and the structure theorem.

Difficulty

Even when M\mathcal MM is finite-dimensional, X\mathfrak XX need not be. An LpL^pLp module may be an infinite column of corners, and the theorem must produce the decomposition without any basis to start from. The obvious idea is to copy Gram–Schmidt and Zorn: take a maximal orthogonal family {ξα}\{\xi_\alpha\}{ξα​} and show that its closed span X0\mathfrak X_0X0​ is everything. For p≠2p\ne2p=2 this step fails as stated. Without an inner product on X\mathfrak XX there is no orthogonal projection onto X0\mathfrak X_0X0​. A best approximation from X0\mathfrak X_0X0​ exists only for p>2p>2p>2 (where X\mathfrak XX is a Banach space and X0\mathfrak X_0X0​ is reflexive), and turning "000 is a best approximant of ζ\zetaζ" into the algebraic identity ⟨ζ,ξλ⟩=0\langle\zeta,\xi_\lambda\rangle=0⟨ζ,ξλ​⟩=0 needs smoothness of the LpL^pLp norm together with the factorization (2.1). The case p<2p<2p<2 is reached by a different route through tensor products with Lq(M)L^q(\mathcal M)Lq(M). A second difficulty is that ∥⋅∥\|\cdot\|∥⋅∥ is the trace norm of ⟨ξ,ξ⟩1/2\langle\xi,\xi\rangle^{1/2}⟨ξ,ξ⟩1/2: it depends on ppp and is not the C∗^*∗-module norm, so Mathlib's C∗^*∗-module results do not apply.

Formalization scope

  • Finite-dimensional algebra. M\mathcal MM is a StarSubalgebra ℂ (Matrix (Fin n) (Fin n) ℂ). Lp(M)L^p(\mathcal M)Lp(M) is M\mathcal MM with the Schatten (quasi)norm of the trace, which is isometric to Haagerup's Lp(M)L^p(\mathcal M)Lp(M). This restriction is forced: Haagerup LpL^pLp spaces of a general von Neumann algebra exist neither in Mathlib nor on the platform. Because Lp/2(M)=ML^{p/2}(\mathcal M)=\mathcal MLp/2(M)=M as a set, the inner-product axioms do not depend on ppp; the norm does.
  • Exponents. Every item assumes 0<p<∞0<p<\infty0<p<∞, and Case 2 items assume p>2p>2p>2 as in the paper. p=∞p=\inftyp=∞ is out of scope.
  • The module. X\mathfrak XX is any complex vector space, of any dimension. The action is a function act with the right-module axioms for elements of M\mathcal MM, and the inner product is the structure LpInnerProduct. Completeness is sequential completeness for ∥⋅∥\|\cdot\|∥⋅∥ (GaugeComplete), since ∥⋅∥\|\cdot\|∥⋅∥ is only a quasi-norm for p<2p<2p<2.
  • Column sums. A column sum is a set of families I→Mn(C)I\to M_n(\mathbb C)I→Mn​(C). Convergence of ∑αξα∗ξα\sum_\alpha\xi_\alpha^*\xi_\alpha∑α​ξα∗​ξα​ is unconditional summability. In the goal, III lives in the universe of X\mathfrak XX.
  • Closures. In Lemma 1.2 and in the cyclic case the closures on the page are of finite-dimensional subspaces and are dropped. The closed span X0\mathfrak X_0X0​ of Case 2 keeps its closure.
  • No trivialization. Several formalizations would make the theorem empty or a different theorem, and none is admissible: measuring X\mathfrak XX in the C∗^*∗-norm ∥⟨ξ,ξ⟩∥1/2\|\langle\xi,\xi\rangle\|^{1/2}∥⟨ξ,ξ⟩∥1/2 (which makes the statement the p=∞p=\inftyp=∞ theorem), assuming X\mathfrak XX finite-dimensional or given with a basis, or asking only for a non-bijective or non-linear TTT.
  • Infrastructure. The development needs the Hermitian functional calculus on matrices (square roots, powers, support projections), Hölder's inequality and the p/2p/2p/2-triangle inequality for Schatten quasinorms, and summability of positive matrix families. These pieces are reusable beyond this mission. Proofs of any milestone are welcome, as are proofs of Theorem 2.5 by routes other than the paper's.

Selected references

  • M. Junge and D. Sherman, Noncommutative LpL^pLp modules, preprint arXiv:math/0301044v2, 2003, revised 14 Sep 2004. arXiv:math/0301044v2
  • W. L. Paschke, Inner product modules over B∗^*∗-algebras, Trans. Amer. Math. Soc. 182 (1973), 443–468 (reference [Pa] of the paper; cited as [P] on p. 10).
  • H. Kosaki, Applications of the complex interpolation method to a von Neumann algebra: noncommutative LpL^pLp-spaces, J. Funct. Anal. 56 (1984), 29–78 (reference [K1] of the paper).
  • U. Haagerup, LpL^pLp-spaces associated with an arbitrary von Neumann algebra, Algèbres d’opérateurs et leurs applications en physique mathématique, CNRS 15 (1979), 175–184 (reference [H] of the paper).
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AlgebraCombinatoricsRepresentation Theory·Captain: mikedeng1

On Central Idempotents in the Brauer Algebra: The Equation uX = −u Is Uniquely Solvable in Orbit Sums with Coefficients in K, and 1 + X Is the Splitting Idempotent of J_n(ℓ)Research Paper

Motivation

The Brauer algebra packages pairings of points into an algebra whose multiplication records how pairings join when diagrams are stacked. It was introduced by Brauer as the centralizer algebra of orthogonal and symplectic groups acting on tensor powers of their natural representation (Brauer 1937), and is semisimple for generic δ\deltaδ (Wenzl 1988). It provides an example where diagram combinatorics and the choice of coefficient ring affect the same algebraic question. King, Martin, and Parker study central idempotents that separate the diagrams with few propagating lines from the remaining part of the algebra. Their construction works over a ring KKK designed to retain useful specializations of the parameter δ\deltaδ; a solution obtained only in the field Q(δ)\mathbb Q(\delta)Q(δ) would lose that arithmetic information. King–Martin–Parker, §1–§2

The mission concerns their main result, Theorem 14. It asks for the precise bridge between a diagram equation, coefficients constrained to KKK, and an idempotent that splits an ideal quotient. The source is the 2016 arXiv version; all page and result numbers here refer to that version. King–Martin–Parker, Theorem 14

Setting

A Brauer diagram on nnn strands is a perfect matching of two rows of nnn nodes. A strand joining the rows is a propagating line; a strand within one row is a horizontal arc. The set of all such diagrams is a basis for BnB_nBn​, here over F=Q(δ)F=\mathbb Q(\delta)F=Q(δ), where δ\deltaδ is an indeterminate. To multiply diagrams AAA and BBB, place AAA over BBB and identify the adjacent rows. The resulting outer pairing is another diagram CCC. If v(A,B)v(A,B)v(A,B) connected components close entirely in the middle row, then

AB=δv(A,B)C.AB=\delta^{v(A,B)}C.AB=δv(A,B)C.

This loop factor is part of the algebra, even when no loop is visible in a particular example. The span Jn(ℓ)J_n(\ell)Jn​(ℓ) of diagrams with at most ℓ\ellℓ propagating lines is a two-sided ideal. Simultaneous relabelling of the upper and lower rows by Sn\mathfrak S_nSn​ partitions diagrams into orbits OOO. The orbit sum DO=∑A∈OAD_O=\sum_{A\in O}ADO​=∑A∈O​A uses each original, unnormalised diagram once. King–Martin–Parker, §2.2–§2.3

The source works with a coefficient ring inside FFF:

K={f/g:f,g∈Z[δ], g monic, deg⁡f≤deg⁡g}.K=\{f/g:f,g\in\mathbb Z[\delta],\ g\text{ monic},\ \deg f\leq\deg g\}.K={f/g:f,g∈Z[δ], g monic, degf≤degg}.

For ℓ<n\ell<nℓ<n and even n−ℓn-\elln−ℓ, let uuu be the diagram with cups at (1,2),(3,4),…,(n−ℓ−1,n−ℓ)(1,2),(3,4),\ldots,(n-\ell-1,n-\ell)(1,2),(3,4),…,(n−ℓ−1,n−ℓ) in each row and vertical lines elsewhere. The paper uses the normalized element uˉ=δ−(n−ℓ)/2u\bar u=\delta^{-(n-\ell)/2}uuˉ=δ−(n−ℓ)/2u. Its required equation uˉX=−uˉ\bar uX=-\bar uuˉX=−uˉ has the same solutions as uX=−uuX=-uuX=−u over FFF. King–Martin–Parker, §2.2, equation (4), and §3, equation (5)

Formalization targets

The goal is Theorem 14. For orbit coefficients cOc_OcO​ and Xc=∑OcODOX_c=\sum_Oc_OD_OXc​=∑O​cO​DO​, it asserts a unique solution with cO∈Kc_O\in KcO​∈K to

uXc=−u.uX_c=-u.uXc​=−u.

It further asserts that φ=1+Xc\varphi=1+X_cφ=1+Xc​ satisfies φ−1∈Jn(ℓ)\varphi-1\in J_n(\ell)φ−1∈Jn​(ℓ) and φJn(ℓ)=Jn(ℓ)φ=0\varphi J_n(\ell)=J_n(\ell)\varphi=0φJn​(ℓ)=Jn​(ℓ)φ=0, and is central and idempotent. By Lemma 10, these properties identify the splitting of 0→Jn(ℓ)→Bn→Bn/Jn(ℓ)→00\to J_n(\ell)\to B_n\to B_n/J_n(\ell)\to00→Jn​(ℓ)→Bn​→Bn​/Jn​(ℓ)→0. King–Martin–Parker, Lemma 10 and Theorem 14

The milestones follow the paper's proof, in attack order: the general bimodule splitting criterion (Lemma 10); the basis of the Sn\mathfrak S_nSn​-centralizer ZSn(Bn)Z_{\mathfrak S_n}(B_n)ZSn​​(Bn​) given by the orbit sums (Lemma 11); the paper's assertion that for ℓ<n\ell<nℓ<n the splitting idempotent φn(ℓ)\varphi_n(\ell)φn​(ℓ) exists with coefficients in KKK (p. 8); the fact that uˉ\bar uuˉ fixes every diagram AtA_{\mathfrak t}At​ carrying its cups and maps no other diagram onto AtA_{\mathfrak t}At​ without a negative power of δ\deltaδ (Proposition 12); the independence of the linear equations in the ctc_{\mathfrak t}ct​, i.e. injectivity of X↦uXX\mapsto uXX↦uX on orbit-sum combinations (equation (6)); and membership of every solution coefficient in KKK (Proposition 13). Lemma 10 is reusable beyond diagram algebras. King–Martin–Parker, §3

Significance

The idempotent separates the ideal of diagrams with few propagating lines from the quotient as bimodules. Its centrality means this separation is compatible with multiplication on either side. Specifying the coefficients in KKK also preserves information about specializations of δ\deltaδ that a field-only existence statement would omit. The paper uses the resulting splitting idempotents in its discussion of primitive central idempotents and Brauer algebra representations. King–Martin–Parker, §4

The theorem is proved in the cited paper. This mission supplies a machine-checkable interface for its definitions and statements; the theorem proofs remain open. A completed development would verify the diagram multiplication, the ideal and orbit descriptions, the ring-theoretic splitting criterion, and the coefficient claim in one Lean environment. These components can support later formalizations involving diagram algebras or central idempotents.

Difficulty

An equation over FFF alone does not give a splitting idempotent with coefficients in KKK. The coefficient restriction is sensitive to the exact loop factor in multiplication and to whether orbit sums use normalized or original diagrams. The equations indexed by diagrams also need to determine the orbit coefficients uniquely, while the two-sided annihilation requirement concerns every element of the ideal, not just the displayed cup diagram. These are distinct claims in the source; checking one of them does not silently establish the others. King–Martin–Parker, §3

Formalization scope

Lean represents a diagram as a fixed-point-free involution on Fin n ⊕ Fin n; the left summand is the upper row. A three-row graph defines its composite and loop count. The Brauer space is the finite-dimensional function space Diagram n → RatFunc ℚ, with an explicit bilinear multiplication bmul; the statements do not assume a ring instance whose associativity has not yet been proved. The parameter is RatFunc.X, representing the indeterminate δ\deltaδ. The ideal is the FFF-span of exactly the basis diagrams with propagating count at most ℓ\ellℓ.

The goal fixes ℓ<n\ell<nℓ<n and additionally assumes even n−ℓn-\elln−ℓ (the existence milestone, stated on the page for every ℓ<n\ell<nℓ<n, does not). That parity condition makes the paper's displayed product uˉ1uˉ3⋯uˉn−ℓ−1\bar u_1\bar u_3\cdots\bar u_{n-\ell-1}uˉ1​uˉ3​⋯uˉn−ℓ−1​ well defined. Lean uses zero-based indices, so the paper's cup (2j+1,2j+2)(2j+1,2j+2)(2j+1,2j+2) is represented by (2j,2j+1)(2j,2j+1)(2j,2j+1). The equation uses unnormalised uuu but has the same solutions as the paper's normalized equation because δ\deltaδ is nonzero in FFF. Orbit sums are unnormalised, as in the printed Theorem 14. The centralizer ZSn(Bn)Z_{\mathfrak S_n}(B_n)ZSn​​(Bn​) is the set of elements commuting with every diagram having nnn propagating lines. The index set of the goal consists only of orbits of diagrams with at most ℓ\ellℓ propagating lines; it is equivalent to the paper's Spore-tableau index set, without introducing that classification into this mission.

The statement constructs φ\varphiφ as 1+Xc1+X_c1+Xc​ from coefficients ccc, rather than postulating an arbitrary splitting idempotent. Neither the ideal nor the equation is replaced with a degenerate special case: with J=BnJ=B_nJ=Bn​ condition (ii) would force φ=0\varphi=0φ=0, and with J=0J=0J=0 it would be vacuous, so the ideal is exactly the span of the diagrams with at most ℓ\ellℓ propagating lines, and the loop factor δv(A,B)\delta^{v(A,B)}δv(A,B) is kept in the product. The main reusable infrastructure comprises finite diagrams, the loop-weighted product, orbit sums, and the generic bimodule splitting lemma. Contributions may establish these structural facts, the milestone statements, and the final theorem.

Selected references

  • O. H. King, P. P. Martin, and A. E. Parker, On central idempotents in the Brauer algebra, Journal of Algebra, 2016; arXiv:1609.01183v1. Page references use the arXiv version.
  • R. Brauer, On algebras which are connected with the semisimple continuous groups, Annals of Mathematics 38 (1937), 857–872. https://doi.org/10.2307/1968843
  • H. Wenzl, On the structure of Brauer's centralizer algebras, Annals of Mathematics 128 (1988), 173–193. https://doi.org/10.2307/1971466
8 thms2 active usersReviewed
AlgebraCombinatoricsRepresentation Theory·Captain: mikedeng1

Representations of Temperley–Lieb Algebras: Closed Product Formula for the Gram Determinants of the Cell ModulesResearch Paper

Motivation

The Temperley–Lieb algebra is a family of algebras built from generators that satisfy local relations. It appears in diagrammatic representation theory and provides a tractable setting in which to study cellular bases and Gram determinants. A Gram determinant tests whether the bilinear form on a module is degenerate after specializing its parameter. Thus an explicit determinant formula records information about when a cell module may cease to be simple. Enyang's 2007 paper develops a Murphy-style basis, a commuting family of operators and an orthogonal basis, then gives a closed product for these determinants. The mission targets that final product, with the preceding statements retained as milestones. Enyang, 2007

The generic cellular-algebra definitions and spectral-projector construction have already been formalized in the published package associated with Mathas's work. This mission specializes those objects to the actual Temperley–Lieb presentation and computes its explicit polynomial factors. Mathas, 2006

Setting

Let R=Z[x]R=\mathbb Z[x]R=Z[x], with xxx an indeterminate. For n≥1n\ge1n≥1, the algebra An(x)A_n(x)An​(x) has generators e1,…,en−1e_1,\ldots,e_{n-1}e1​,…,en−1​ and relations

ei2=xei,eiei±1ei=ei,eiej=ejeiwhen ∣i−j∣≥2.e_i^2=xe_i,\qquad e_ie_{i\pm1}e_i=e_i,\qquad e_ie_j=e_je_i\quad\text{when }|i-j|\ge2.ei2​=xei​,ei​ei±1​ei​=ei​,ei​ej​=ej​ei​when ∣i−j∣≥2.

A shape at level nnn is a pair λ=(f,n−2f)\lambda=(f,n-2f)λ=(f,n−2f) with 0≤2f≤n0\le2f\le n0≤2f≤n. A standard up–down tableau of shape λ\lambdaλ is a path of shapes from (0,0)(0,0)(0,0) to λ\lambdaλ: at each level its cup count stays fixed or increases by one. Write Tn(λ)\mathfrak T_n(\lambda)Tn​(λ) for the set of these paths and dim⁡(λ)=∣Tn(λ)∣\dim(\lambda)=|\mathfrak T_n(\lambda)|dim(λ)=∣Tn​(λ)∣. The paper orders paths by comparing their cup counts at every level; u▹tu\triangleright tu▹t means strict pointwise dominance. Enyang, §§1–2

For each shape, mλm_\lambdamλ​ is the product e1e3⋯e2f−1e_1e_3\cdots e_{2f-1}e1​e3​⋯e2f−1​. Ordered generator products wi,jw_{i,j}wi,j​ and their tableau products vt,vt∗v_t,v_t^*vt​,vt∗​ give the Murphy elements muv=vu∗mλvvm_{uv}=v_u^*m_\lambda v_vmuv​=vu∗​mλ​vv​. Lemma 2.3 asserts that they form a cellular basis. The cellular multiplication law computes a Gram form on each cell module CλC^\lambdaCλ. The determinant det⁡(λ)\det(\lambda)det(λ) is the determinant of this computed form in the Murphy basis; it is not assigned the desired closed product by definition. Enyang, Lemma 2.3 and §5

The Jucys–Murphy elements TkT_kTk​ form a commuting family in An(x)A_n(x)An​(x). Their triangular action on a tableau ttt has content rt(k)∈Rr_t(k)\in Rrt​(k)∈R. Over the fraction field F=Frac⁡(R)F=\operatorname{Frac}(R)F=Frac(R), the spectral product FtF_tFt​ produces a vector ft=mtFtf_t=m_tF_tft​=mt​Ft​. These vectors form an orthogonal basis, with squared norms ⟨ft,ft⟩\langle f_t,f_t\rangle⟨ft​,ft​⟩ whose product equals det⁡(λ)\det(\lambda)det(λ). The auxiliary polynomials are fixed by p0=0p_0=0p0​=0, p1=1p_1=1p1​=1 and pi+1=xpi−pi−1p_{i+1}=xp_i-p_{i-1}pi+1​=xpi​−pi−1​. Enyang, §§3–5

Formalization targets

The milestones follow the paper's own sequence: the Murphy cellular basis (Lemma 2.3) and the neighbour criterion for the elements vtv_tvt​ (Corollary 2.2); the basic properties of TiT_iTi​ and ziz_izi​ (Lemma 3.1), the sum identities for pip_ipi​ (Lemma 3.4), the action of ziz_izi​ on the generator of a cell module (Lemma 3.5), the triangular action of TkT_kTk​ and zkz_kzk​ with diagonals rt(k)r_t(k)rt​(k) and zt(k)=pipk−i+1z_t(k)=p_ip_{k-i+1}zt​(k)=pi​pk−i+1​ (Corollaries 3.6, 3.7) and the alternative recursion for Ti+1T_{i+1}Ti+1​ (Corollary 4.2); the seminormal basis (Lemma 4.4), the diagonal coefficients of eke_kek​ on it (Corollary 4.6) and the norm ratio of neighbouring seminormal vectors (Lemma 4.7); the identification of det⁡(λ)\det(\lambda)det(λ) with ∏t⟨ft,ft⟩\prod_t\langle f_t,f_t\rangle∏t​⟨ft​,ft​⟩ (§5) and the branching law (Lemma 5.1). The goal is Lemma 5.2, the closed product. When n>2fn>2fn>2f,

det⁡(f,n−2f)=∏i=1f(pn−2f+i+1pi)dim⁡(f−i,n−2f+2i).\det(f,n-2f)=\prod_{i=1}^{f}\left(\frac{p_{n-2f+i+1}}{p_i}\right)^{\dim(f-i,n-2f+2i)}.det(f,n−2f)=i=1∏f​(pi​pn−2f+i+1​​)dim(f−i,n−2f+2i).

When n=2fn=2fn=2f, the predecessor shape μ=(f−1,1)\mu=(f-1,1)μ=(f−1,1) lies at level n−1n-1n−1, and the target is

det⁡(f,0)=det⁡(μ)xdim⁡(f,0).\det(f,0)=\det(\mu)x^{\dim(f,0)}.det(f,0)=det(μ)xdim(f,0).

The quotient in the first formula is evaluated in FFF; the second equality is in RRR. Both clauses occur in the printed Lemma 5.2. Enyang, Lemma 5.2, p. 20

Significance

The result turns a determinant of a matrix indexed by all tableaux of a shape into a finite product of explicit recursive polynomials. It makes the factors that can vanish under specialization visible and lets later representation-theoretic questions be asked in terms of those factors. The branching law supplies a compatible description across levels of the algebra tower. Enyang, §5

The paper proves the formulas mathematically. The statements in this mission are compiled Lean targets with proof holes; they do not yet constitute machine-checked proofs of Enyang's results. A complete development would supply the cellular-basis theorem, establish the paper's explicit content action, connect the integral and field Gram forms, and prove the norm and determinant formulas. The quotient presentation, tableau encoding and cellular package can be reused for related specializations and diagram-algebra calculations.

Difficulty

The generator relations make local products manageable, but a determinant does not expose its factors directly. The cell module is indexed by whole paths, and the operators act triangularly rather than diagonally in the Murphy basis. Passing to seminormal vectors changes the basis while keeping track of the bilinear form; this requires the local coefficient and norm statements, not just the commutation of the operators. At the boundary n=2fn=2fn=2f, one of the two possible predecessor shapes disappears, so a uniform two-factor branching formula would introduce a nonexistent module. Enyang, §§3–5

Formalization scope

The Lean algebra is a quotient of a free algebra by all three defining relation families. It uses one-based generators; an out-of-range generator is set to zero, and every stated result guards its meaningful indices. Shapes are finite cup-count indices and tableaux are finite paths with a pointwise order. The unrolled products defining vtv_tvt​ and vt∗v_t^*vt∗​ follow the page's multiplication order. The integral statements use R=Z[x]R=\mathbb Z[x]R=Z[x]; seminormal vectors use F=Frac⁡(R)F=\operatorname{Frac}(R)F=Frac(R) and the published cellular-algebra package's coordinate-space cell module and Gram form. Existence of the required Murphy and JM data is asserted, preventing a theorem about an empty class of such data from passing vacuously.

Several printed details need explicit treatment. The page-2 endpoint e2f+1e_{2f+1}e2f+1​ in mλm_\lambdamλ​ is replaced by e2f−1e_{2f-1}e2f−1​, giving exactly fff factors and m(0,n)=1m_{(0,n)}=1m(0,n)​=1. The missing z0z_0z0​ is zero by the paper's sum formula. The rs(k)r_s(k)rs​(k) denominator in the definition of FtF_tFt​ means rt(k)r_t(k)rt​(k). Lemma 4.4(3) says “orthonormal,” but later nonunit norms show that the valid conclusion is pairwise orthogonality. The direction of ▹\triangleright▹ in the printed definition of gλ,μg_{\lambda,\mu}gλ,μ​ and Lemma 5.2 is reversed relative to the formula's denominator and the proof; the target product runs over shapes with fewer cups. Identity (3.3) of Lemma 3.4 is false as printed (at i=j=2i=j=2i=j=2, k=1k=1k=1 it reads x3−2x=xx^3-2x=xx3−2x=x); the target is the form its proof derives, with last factor pj+k−1p_{j+k-1}pj+k−1​. The goal and the cellular milestones take n≥1n\ge1n≥1, since the paper's tower starts at A1(x)=RA_1(x)=RA1​(x)=R; for n=0n=0n=0 the even case of Lemma 5.2 would refer to the non-existent shape (−1,1)(-1,1)(−1,1). Enyang, pp. 2, 10, 17, 19–20

Useful contributions include proofs of the algebraic Murphy-basis statement, the content formulas, the seminormal basis properties, the integral-to-field determinant identification and the branching law. Each has a separate mission item and source index.

Selected references

  • John Enyang, Representations of Temperley–Lieb Algebras, arXiv preprint arXiv:0710.3218v1, 2007. arXiv
  • Andrew Mathas, Seminormal forms and Gram determinants for cellular algebras, arXiv preprint arXiv:math/0604108v4, 2006. arXiv
18 thms2 active usersReviewed
Functional AnalysisMathematical PhysicsQuantum Information·Captain: mikedeng1

On Singular Perturbations of Quantum Dynamical Semigroups: For the Left Shift with Rank-One Rebound to Ω, Every X in the Domain Algebra Satisfies (X − Tr(ΩX)I)Ω = Ω(X − Tr(ΩX)I) = 0Research Paper

Motivation

A quantum dynamical semigroup describes the irreversible evolution of an open quantum system: a family TtT_tTt​, t≥0t \ge 0t≥0, of normal completely positive maps on the algebra B(H)\mathfrak B(\mathcal H)B(H) of bounded operators, with T0=IdT_0 = \mathrm{Id}T0​=Id and t↦Tt[X]t \mapsto T_t[X]t↦Tt​[X] weakly continuous. When the generator is bounded its structure is given by the Lindblad–Gorini–Kossakowski–Sudarshan form (Lindblad 1976). For unbounded generators, the bounded-generator formula alone does not settle trace preservation or describe the generator's domain.

W. Arveson (The domain algebra of a CP-semigroup, 2002) attached to every such semigroup its domain algebra, the set of observables XXX for which XXX, X∗XX^*XX∗X and XX∗XX^*XX∗ all lie in the domain of the generator. This is the largest set on which the generator can be handled algebraically, through derivations and the "dissipation function". Arveson computed it for one explicit example built from the shift on L2(R+)L^2(\mathbb R_+)L2(R+​) with a rank-one rebound to a pure state ∣f⟩⟨f∣|f\rangle\langle f|∣f⟩⟨f∣, found that its strong closure consists of the operators commuting with ∣f⟩⟨f∣|f\rangle\langle f|∣f⟩⟨f∣, and asked whether there exist dynamical semigroups whose domain algebra is as small as C⋅I\mathbb C \cdot IC⋅I.

A. S. Holevo (arXiv:1706.04866v5, §2) generalizes Arveson's example to a rebound into an arbitrary density operator Ω\OmegaΩ and answers the question positively: when Ω\OmegaΩ is nondegenerate, the domain algebra is C⋅I\mathbb C\cdot IC⋅I.

Setting

Let H=L2(R+)\mathcal H = L^2(\mathbb R_+)H=L2(R+​) and let Wtφ(x)=φ(x+t)W_t\varphi(x) = \varphi(x+t)Wt​φ(x)=φ(x+t) be the semigroup of left shifts. On trace-class operators ω\omegaω put St0[ω]=Wt ω Wt∗S^0_t[\omega] = W_t\,\omega\,W_t^*St0​[ω]=Wt​ωWt∗​, with dual semigroup Tt0[X]=Wt∗XWtT^0_t[X] = W_t^* X W_tTt0​[X]=Wt∗​XWt​ on bounded operators, and let K0\mathcal K_0K0​ be the generator of St0S^0_tSt0​. The shift moves probability out of R+\mathbb R_+R+​ through the endpoint 000, so St0S^0_tSt0​ is not trace preserving.

Fix an arbitrary density operator Ω\OmegaΩ (positive, trace class, Tr⁡Ω=1\operatorname{Tr}\Omega = 1TrΩ=1). The rank-one reset

Λ[ω]=− Ω Tr⁡K0[ω],ω∈dom⁡K0,\Lambda[\omega] = -\,\Omega\,\operatorname{Tr}\mathcal K_0[\omega], \qquad \omega \in \operatorname{dom}\mathcal K_0,Λ[ω]=−ΩTrK0​[ω],ω∈domK0​,

re-injects the lost probability in the state Ω\OmegaΩ. For ω=∣ψ⟩⟨φ∣\omega = |\psi\rangle\langle\varphi|ω=∣ψ⟩⟨φ∣ with φ,ψ\varphi,\psiφ,ψ absolutely continuous with square-integrable derivative (φ,ψ∈D=AC1(R+)\varphi, \psi \in \mathcal D = AC^1(\mathbb R_+)φ,ψ∈D=AC1(R+​)), Λ[ω]=Ω ψ(0) φ(0)‾\Lambda[\omega] = \Omega\,\psi(0)\,\overline{\varphi(0)}Λ[ω]=Ωψ(0)φ(0)​. Let StS_tSt​ be the minimal perturbed semigroup generated by K0+Λ\mathcal K_0 + \LambdaK0​+Λ (constructed by a resolvent series), Tt=(St)∗T_t = (S_t)^*Tt​=(St​)∗ its dual, and L\mathcal LL the ultraweak generator of TtT_tTt​: L[X]=Y\mathcal L[X] = YL[X]=Y means t−1(Tr⁡ρ Tt[X]−Tr⁡ρX)→Tr⁡ρYt^{-1}(\operatorname{Tr}\rho\,T_t[X] - \operatorname{Tr}\rho X) \to \operatorname{Tr}\rho Yt−1(TrρTt​[X]−TrρX)→TrρY as t↓0t \downarrow 0t↓0 for every trace-class ρ\rhoρ. The generator L0\mathcal L_0L0​ of Tt0T^0_tTt0​ is defined in the same way. Arveson's domain algebra is

A={X∈dom⁡L:X∗X∈dom⁡L, XX∗∈dom⁡L}.\mathcal A = \{X \in \operatorname{dom}\mathcal L : X^*X \in \operatorname{dom}\mathcal L,\ XX^* \in \operatorname{dom}\mathcal L\}.A={X∈domL:X∗X∈domL, XX∗∈domL}.

Formalization targets

Goal: Theorem 2 (p. 4)

For every X∈AX \in \mathcal AX∈A,

[X−(Tr⁡ΩX) I] Ω=Ω [X−(Tr⁡ΩX) I]=0,[X - (\operatorname{Tr}\Omega X)\,I]\,\Omega = \Omega\,[X - (\operatorname{Tr}\Omega X)\,I] = 0,[X−(TrΩX)I]Ω=Ω[X−(TrΩX)I]=0,

and if Ω\OmegaΩ is nondegenerate, A=C⋅I\mathcal A = \mathbb C \cdot IA=C⋅I. The goal is the existing Open platform theorem QAlgorithms.Papers.Independent.Renew46.P06.shiftReset_domainAlgebra, which this mission references rather than restates.

Milestones

The milestones follow the paper's proof, in order:

  1. (11), p. 5: Arveson's criterion, for an arbitrary quantum dynamical semigroup: X∈dom⁡LX \in \operatorname{dom}\mathcal LX∈domL iff sup⁡t>0t−1∥Tt[X]−X∥<∞\sup_{t>0} t^{-1}\|T_t[X] - X\| < \inftysupt>0​t−1∥Tt​[X]−X∥<∞.
  2. Lemma 3, p. 5: dom⁡L0\operatorname{dom}\mathcal L_0domL0​ is a ∗*∗-algebra and I∉dom⁡L0I \notin \operatorname{dom}\mathcal L_0I∈/domL0​ (existing Open theorem shiftDual_nonunitalStarDomain).
  3. p. 4: TtT_tTt​ is unital, Tt[I]=IT_t[I] = ITt​[I]=I.
  4. (12), p. 5: the integral equation ⟨φ∣Tt[X]∣ψ⟩=⟨φ∣Tt0[X]∣ψ⟩+∫0tψ(s)φ(s)‾Tr⁡ΩTt−s[X] ds\langle\varphi|T_t[X]|\psi\rangle = \langle\varphi|T^0_t[X]|\psi\rangle + \int_0^t \psi(s)\overline{\varphi(s)}\operatorname{Tr}\Omega T_{t-s}[X]\,ds⟨φ∣Tt​[X]∣ψ⟩=⟨φ∣Tt0​[X]∣ψ⟩+∫0t​ψ(s)φ(s)​TrΩTt−s​[X]ds for φ,ψ∈D\varphi,\psi \in \mathcal Dφ,ψ∈D.
  5. Lemma 4, p. 5: if X∈dom⁡LX \in \operatorname{dom}\mathcal LX∈domL then X0=X−(Tr⁡ΩX)I∈dom⁡L0X_0 = X - (\operatorname{Tr}\Omega X)I \in \operatorname{dom}\mathcal L_0X0​=X−(TrΩX)I∈domL0​ and L[X]=L0[X0]\mathcal L[X] = \mathcal L_0[X_0]L[X]=L0​[X0​] (existing Open theorem shiftReset_centeredGenerator).
  6. Proof of Theorem 2, p. 6: for X∈AX \in \mathcal AX∈A, Tr⁡ΩX∗X=∣Tr⁡ΩX∣2\operatorname{Tr}\Omega X^*X = |\operatorname{Tr}\Omega X|^2TrΩX∗X=∣TrΩX∣2 and Tr⁡ΩXX∗=∣Tr⁡ΩX∗∣2\operatorname{Tr}\Omega XX^* = |\operatorname{Tr}\Omega X^*|^2TrΩXX∗=∣TrΩX∗∣2.
  7. Proof of Theorem 2, p. 6: the noncommutative Cauchy–Schwarz inequality Tr⁡ΩX∗X≥∣Tr⁡ΩX∣2\operatorname{Tr}\Omega X^*X \ge |\operatorname{Tr}\Omega X|^2TrΩX∗X≥∣TrΩX∣2 and its equality case [X−(Tr⁡ΩX)I]Ω=0[X - (\operatorname{Tr}\Omega X)I]\Omega = 0[X−(TrΩX)I]Ω=0, on an arbitrary Hilbert space.

The goal and Lemmas 3 and 4 are Open platform theorems posed from this paper without a mission; this mission supplies the remaining milestones of the paper's proof and the attack path connecting them.

Significance

Theorem 2 answers Arveson's question: there are quantum dynamical semigroups on B(L2(R+))\mathfrak B(L^2(\mathbb R_+))B(L2(R+​)) whose domain algebra contains only the scalars. For such a semigroup, no non-scalar XXX lies in the generator domain together with both X∗XX^*XX∗X and XX∗XX^*XX∗, so algebraic tools built on the domain algebra (derivations, the dissipation function) see only scalars. For degenerate Ω\OmegaΩ the theorem still forces every element of A\mathcal AA to act as a scalar on the range of Ω\OmegaΩ, extending Arveson's computation for a pure Ω\OmegaΩ to every density operator.

The result is proved in the paper; nothing here is open mathematically. None of it has a machine-checked proof. The mission produces, on top of Mathlib, a formal account of weak∗^*∗ generators of semigroups on B(H)\mathfrak B(\mathcal H)B(H) (the Favard-class criterion (11)), a Duhamel formula for a minimal perturbation, and the equality case of the Cauchy–Schwarz inequality for density operators, each of which is reusable outside this paper.

Difficulty

The algebra of the proof of Theorem 2 is short once its inputs are available; the inputs are the work. Criterion (11) is a statement about the ultraweak generator: with the operator-norm derivative in its place it is false, since the bounded difference quotients describe the Favard class, which is in general larger than the norm domain. Its reverse direction must connect uniform operator-norm bounds with a limit against every trace-class operator. Unitality of TtT_tTt​ depends on the minimal resolvent series of the perturbation actually conserving trace, which can fail for general unbounded perturbations (explosion). The integral equation (12) requires knowing that the minimal semigroup satisfies the Dyson-type equation on rank-one operators ∣ψ⟩⟨φ∣|\psi\rangle\langle\varphi|∣ψ⟩⟨φ∣ built from AC1AC^1AC1 functions, together with the evaluation Λ[Ss0[∣ψ⟩⟨φ∣]]=Ω ψ(s)φ(s)‾\Lambda[S^0_s[|\psi\rangle\langle\varphi|]] = \Omega\,\psi(s)\overline{\varphi(s)}Λ[Ss0​[∣ψ⟩⟨φ∣]]=Ωψ(s)φ(s)​, which uses boundary values of L2L^2L2 functions that only continuous representatives possess.

Formalization scope

All statements use the published definitions module QAlgorithms_Papers_Independent_Renew46_P06 and its imports: H\mathcal HH is HalfLine =L2(R+)= L^2(\mathbb R_+)=L2(R+​) as an Lp space; semigroups are Evolution (normal, CP, subunital, weakly continuous) with times in NNReal, real times entering through t.toNNReal only for t≥0t \ge 0t≥0; trace-class operators and density operators are TraceClass and State b, with the trace operatorTrace b taken in a fixed Hilbert basis bbb; dom⁡L\operatorname{dom}\mathcal LdomL and the graph of L\mathcal LL are the ultraweak dualGeneratorDomain and InDualGeneratorGraph; the shift, the pair (St0,Tt0)(S^0_t, T^0_t)(St0​,Tt0​) and the reset construction are IsLeftShift, IsShiftPair and IsResetConstruction; A\mathcal AA is domainAlgebra; III is identityObservable. Every semigroup milestone uses exactly the goal's binders, so the milestones compose with the goal. In (12), φ,ψ∈AC1(R+)\varphi,\psi \in AC^1(\mathbb R_+)φ,ψ∈AC1(R+​) are encoded by L2L^2L2 classes with named locally absolutely continuous representatives, and only those representatives are evaluated at a point; ⟨φ∣A∣ψ⟩\langle\varphi|A|\psi\rangle⟨φ∣A∣ψ⟩ is Mathlib's inner product, conjugate-linear in the first slot. The Cauchy–Schwarz milestone is stated on an arbitrary complex Hilbert space.

A formalization that takes a local semigroup in place of the published construction, an operator-norm generator in place of the ultraweak one, or that turns (12) into a definition of TtT_tTt​, would not state the paper's results and is ruled out.

The setting of the semigroup milestones is satisfiable exactly when a reset construction exists, which is part of the separate Open platform theorem shiftReset_standard_nonclosable; contributions proving that existence are welcome alongside the milestones. Also welcome: general Favard-class results for weak∗^*∗-continuous semigroups, Duhamel formulas for minimal perturbations in the sense of the published IsMinimalPerturbation, and trace inequalities for State.

Selected references

  • A. S. Holevo, On singular perturbations of quantum dynamical semigroups, Mathematical Notes, 2017; arXiv:1706.04866v5, 2018. https://arxiv.org/abs/1706.04866
  • W. Arveson, The domain algebra of a CP-semigroup, Pacific J. Math. 203(1), 67–77, 2002. https://doi.org/10.2140/pjm.2002.203.67
  • G. Lindblad, On the generators of quantum dynamical semigroups, Commun. Math. Phys. 48, 119–130, 1976. https://doi.org/10.1007/BF01608499
  • A. M. Chebotarev, F. Fagnola, Sufficient conditions for conservativity of quantum dynamical semigroups, J. Funct. Anal. 118, 131–153, 1993. https://doi.org/10.1006/jfan.1993.1140
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Functional AnalysisHarmonic AnalysisRepresentation Theory·Captain: mikedeng1

On the Characterization of Trace Class Representations and Schwartz Operators: A Unitary Lie Group Representation Is Trace Class iff Some (1 − dπ(Δ))⁻ᵏ Is Trace Class iff π(Cᵐ_c(G)) ⊆ B₁ for Some mResearch Paper

Why trace class representations matter

A strongly continuous unitary representation turns each group element into a unitary operator on a Hilbert space. Averaging those operators against a smooth, compactly supported function gives a bounded operator. When every such average is trace class, its trace defines a distribution character. The trace condition is therefore a bridge from an operator representation to a scalar distribution that can be studied by harmonic analysis. Van Dijk, Neeb, Salmasian and Zellner collect and extend characterizations of this condition for finite-dimensional Lie groups in their 2015 preprint. Their Theorem 1.3 is the target here.

The authors identify one of the equivalences, between the trace class property and a trace class negative power of the Nelson Laplacian, with an earlier statement of Cartier that had appeared without a proof or reference. Their further conclusion that one finite degree of differentiability suffices is presented as a new result; it gives finite order for the distribution character. These are claims about the cited preprint, not claims of prior machine verification. Source: introduction and Theorem 1.3, pp. 2–5.

The representation and its test functions

Let GGG be a finite-dimensional real Lie group, let HHH be a complex Hilbert space, and let π:G→U(H)\pi:G\to\mathrm U(H)π:G→U(H) be a strongly continuous unitary representation. Fix a left Haar measure μ\muμ. For a compactly supported continuous function f:G→Cf:G\to\mathbb Cf:G→C, the integrated operator is π(f)v=∫Gf(g)π(g)v dμ(g)\pi(f)v=\int_G f(g)\pi(g)v\,d\mu(g)π(f)v=∫G​f(g)π(g)vdμ(g) for each v∈Hv\in Hv∈H. Write Ccm(G)C^m_c(G)Ccm​(G) for compactly supported functions with mmm continuous derivatives and Cc∞(G)C^\infty_c(G)Cc∞​(G) for smooth compactly supported functions. Write B1(H)B_1(H)B1​(H) and B2(H)B_2(H)B2​(H) for the trace class and Hilbert–Schmidt ideals of bounded operators on HHH.

Choose a basis X1,…,XnX_1,\ldots,X_nX1​,…,Xn​ of the Lie algebra g\mathfrak gg. The Nelson Laplacian is Δ=∑j=1nXj2\Delta=\sum_{j=1}^n X_j^2Δ=∑j=1n​Xj2​ in the enveloping algebra. The derived representation applies dπ(Δ)d\pi(\Delta)dπ(Δ) on smooth vectors. Its closure D=dπ(Δ)‾D=\overline{d\pi(\Delta)}D=dπ(Δ)​ is a non-positive self-adjoint operator, and (1−D)−1(1-D)^{-1}(1−D)−1 is bounded. The choice of basis determines DDD, while the theorem holds for an arbitrary fixed basis. Source: §1 and proof of Theorem 1.3, pp. 3–4.

Formalization targets

Five equivalent conditions

The mission goal is the complete five-way equivalence in Theorem 1.3:

(i)  ∃m≥1: π(Ccm(G))⊆B1(H) and π:Ccm(G)→B1(H) is continuous;(ii)  π(Cc∞(G))⊆B1(H) and π:Cc∞(G)→B1(H) is continuous;(iii)  π(Cc∞(G))⊆B1(H);(iv)  π(Cc∞(G))⊆B2(H);(v)  ∃k≥1: (1−D)−k∈B1(H).\begin{aligned} \text{(i)}\;&\exists m\ge1:\ \pi(C^m_c(G))\subseteq B_1(H) \text{ and }\pi:C^m_c(G)\to B_1(H)\text{ is continuous};\\ \text{(ii)}\;&\pi(C^\infty_c(G))\subseteq B_1(H) \text{ and }\pi:C^\infty_c(G)\to B_1(H)\text{ is continuous};\\ \text{(iii)}\;&\pi(C^\infty_c(G))\subseteq B_1(H);\\ \text{(iv)}\;&\pi(C^\infty_c(G))\subseteq B_2(H);\\ \text{(v)}\;&\exists k\ge1:\ (1-D)^{-k}\in B_1(H). \end{aligned}(i)(ii)(iii)(iv)(v)​∃m≥1: π(Ccm​(G))⊆B1​(H) and π:Ccm​(G)→B1​(H) is continuous;π(Cc∞​(G))⊆B1​(H) and π:Cc∞​(G)→B1​(H) is continuous;π(Cc∞​(G))⊆B1​(H);π(Cc∞​(G))⊆B2​(H);∃k≥1: (1−D)−k∈B1​(H).​

The continuity clauses are part of the target; they cannot be inferred merely from the displayed inclusions. The milestone list includes the four nontrivial implications named in the paper's proof, its finite-order claim and the two displayed identities needed to connect the function and operator Laplacians. Source: Theorem 1.3 and proof, pp. 3–5.

What the equivalence gives

Condition (iii) is formulated using every smooth compactly supported function. Condition (i) replaces smoothness by one finite differentiability order that works uniformly for the representation, while retaining continuity into the trace class ideal. This is the form needed to conclude that the distribution character has finite order. Condition (v) tests the same property with one operator associated with the Lie algebra basis. These consequences are stated by the authors in the introduction and derived in §1. Source: pp. 2–5.

A formal proof would connect Lie-group differentiation, Bochner integration, Schatten ideals and the topology of compactly supported function spaces in one reusable development. The target and milestones here are open Lean statements: compilation checks their types, not their proofs. The previously posed Lemmas 1.1 and 1.2 of the same paper remain separate open platform items, and can be used by solvers without being re-posed here.

Where the difficulty lies

Showing that each π(f)\pi(f)π(f) is trace class does not immediately give continuity of f↦π(f)f\mapsto\pi(f)f↦π(f) in trace norm: operator-norm convergence alone does not control trace norm. The paper also needs to pass from trace class images of smooth functions to an operator statement about (1−D)−k(1-D)^{-k}(1−D)−k, and then back to functions with only finitely many derivatives. The obvious shortcut of treating dπ(Δ)d\pi(\Delta)dπ(Δ) as a bounded operator fails because its natural domain is the smooth-vector space and its closure is generally unbounded. The proof therefore has substantial analytic content beyond elementary ideal inclusions. Source: proof of Theorem 1.3, pp. 4–5.

Formalization scope

Lean represents GGG as a Hausdorff finite-dimensional Lie group modelled on a finite-dimensional real normed space EEE, equipped with a regular left Haar measure. It represents HHH as a complete complex inner-product space, without a separability assumption, and the representation by a strongly continuous monoid homomorphism into unitary continuous linear equivalences. The Lie algebra is the tangent space EEE at the identity, and the basis is an arbitrary finite basis of EEE. The quantifiers for mmm and kkk include explicit lower bounds 1≤m1\le m1≤m and 1≤k1\le k1≤k, matching the paper's convention N0=N∪{0}\mathbb N_0=\mathbb N\cup\{0\}N0​=N∪{0}.

Smooth vectors are exactly those whose orbit maps are smooth. The derived action is the manifold derivative of that orbit map at the identity, used only on smooth vectors. The function-side Laplacian uses right-invariant directional derivatives; its second-order sign agrees with the paper's action. A bounded operator RRR is characterized by R(w−dπ(Δ)w)=wR(w-d\pi(\Delta)w)=wR(w−dπ(Δ)w)=w on every smooth vector. The paper's essential self-adjointness and density statement identifies this RRR uniquely with (1−D)−1(1-D)^{-1}(1−D)−1; the theorem carries that characterization as a hypothesis. The hypothesis must be satisfiable, and the interpretation must remain the paper's resolvent.

Continuity on Ccm(G)C^m_c(G)Ccm​(G) is encoded by a bound on the Schatten 111-norm for every compact support set, with one constant for all functions supported there. For Cc∞(G)C^\infty_c(G)Cc∞​(G), the derivative order may depend on the compact set. The Schatten norms and classes are reused published definitions, with norm values in [0,∞][0,\infty][0,∞]; no alternate trace norm is introduced. Equation (1) is an identity of distributions tested against smooth compactly supported functions. A complete proof needs the smooth-vector integration lemma, Lie-group test-function approximation, the function-side parametrix and operator ideal estimates. These components are useful beyond this mission.

Selected references

  • G. van Dijk, K.-H. Neeb, H. Salmasian and C. Zellner, On the characterization of trace class representations and Schwartz operators, arXiv preprint, 2015, arXiv:1512.02451v1.
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Information TheoryMathematical PhysicsQuantum Information·Captain: mikedeng1

Capacities of Quantum Channels for Massive Bosons and Fermions: Under Average Energy and Particle-Number Constraints the Capacity Is the Grand-Canonical Entropy, Attained by Fock StatesResearch Paper

Motivation

Classical information can be sent by choosing a quantum state, transmitting it, and asking a receiver to measure it. An ideal noiseless channel seems to have no finite information limit if its carrier can occupy arbitrarily many quantum states. A physical carrier, however, has a limited average energy, and a channel carrying massive particles also has a limited average particle number. Sen(De), Sen, Gromek, Bruß, and Lewenstein ask for the greatest information transfer compatible with both constraints. Their answer connects the channel's information capacity to the entropy of the grand-canonical ensemble familiar from statistical mechanics. Sen(De) et al., pp. 1–2.

The paper also studies how capacities of Bose and Fermi systems respond to condensation and pairing. This mission concerns the result that supports those comparisons: the capacity formula for an ideal, noiseless channel under fixed average energy and particle number. Its finite-dimensional form gives a precise setting in which the optimization and its attaining ensemble can both be stated. Sen(De) et al., pp. 2–4.

Setting

The carrier has a finite-dimensional complex state space. Its Hamiltonian H\mathcal HH assigns energy, and its number operator N^\hat NN^ counts particles. The two Hermitian operators commute, so the system has an orthonormal basis of states with definite energy and particle number. These are the Fock states used as signals. For inverse temperature β\betaβ and chemical potential μ\muμ, the grand-canonical state is

ρGCE=exp⁡[−β(H−μN^)]Z,Z=tr⁡exp⁡[−β(H−μN^)].\rho_{\mathrm{GCE}}=\frac{\exp[-\beta(\mathcal H-\mu\hat N)]}{Z}, \qquad Z=\operatorname{tr}\exp[-\beta(\mathcal H-\mu\hat N)].ρGCE​=Zexp[−β(H−μN^)]​,Z=trexp[−β(H−μN^)].

A sender chooses one state ρi\rho_iρi​ from a finite ensemble E={(pi,ρi)}\mathcal E=\{(p_i,\rho_i)\}E={(pi​,ρi​)} with probability pip_ipi​. Each state may be mixed. The mean state is ρˉ=∑ipiρi\bar\rho=\sum_i p_i\rho_iρˉ​=∑i​pi​ρi​. A receiver chooses a finite quantum measurement and observes its outcome. The accessible information Iacc(E)I_{\mathrm{acc}}(\mathcal E)Iacc​(E) is the largest mutual information between the sender's label and the receiver's outcome among these measurements. The Holevo quantity is χ(E)=S(ρˉ)−∑ipiS(ρi)\chi(\mathcal E)=S(\bar\rho)-\sum_i p_iS(\rho_i)χ(E)=S(ρˉ​)−∑i​pi​S(ρi​), where SSS is von Neumann entropy. All information and entropy values use base-two logarithms, so their units are bits. Sen(De) et al., p. 1.

Fix EEE and NNN. An ensemble is admissible when its mean state obeys the two exact constraints tr⁡(ρˉH)=E\operatorname{tr}(\bar\rho\mathcal H)=Etr(ρˉ​H)=E and tr⁡(ρˉN^)=N\operatorname{tr}(\bar\rho\hat N)=Ntr(ρˉ​N^)=N. The paper defines CE,NC_{E,N}CE,N​ as the maximum accessible information among admissible ensembles. For the theorem here, EEE and NNN are the expectations of H\mathcal HH and N^\hat NN^ in ρGCE\rho_{\mathrm{GCE}}ρGCE​; no claim of a global inverse from (E,N)(E,N)(E,N) to (β,μ)(\beta,\mu)(β,μ) is needed. Sen(De) et al., p. 2.

Formalization targets

The first targets are the paper's entropy bounds: the Holevo bound Iacc(E)≤χ(E)I_{\mathrm{acc}}(\mathcal E)\leq\chi(\mathcal E)Iacc​(E)≤χ(E) and χ(E)≤S(ρˉ)\chi(\mathcal E)\leq S(\bar\rho)χ(E)≤S(ρˉ​). The grand-canonical variational principle says that, under the two fixed expectations, no state has greater entropy than ρGCE\rho_{\mathrm{GCE}}ρGCE​. The first and third targets correspond to existing Open platform statements; the second is drafted here. Sen(De) et al., pp. 1–2.

The goal combines the value of the capacity with its attainment:

CE,N=S(ρGCE),Iacc(EFock)=CE,N,C_{E,N}=S(\rho_{\mathrm{GCE}}), \qquad I_{\mathrm{acc}}(\mathcal E_{\mathrm{Fock}})=C_{E,N},CE,N​=S(ρGCE​),Iacc​(EFock​)=CE,N​,

where EFock\mathcal E_{\mathrm{Fock}}EFock​ consists of joint energy and number eigenstates with probabilities supplied by ρGCE\rho_{\mathrm{GCE}}ρGCE​. Two further milestones record that this ensemble has mean ρGCE\rho_{\mathrm{GCE}}ρGCE​ and that orthogonal pure signals make their classical label information accessible to a measurement. The goal includes an actual maximizing ensemble; an equality involving a supremum alone would leave the paper's attainment claim unstated. Sen(De) et al., p. 2 and abstract.

Significance

The result turns a channel optimization over encodings and measurements into a thermodynamic quantity, while specifying signals that reach the bound. The second constraint matters: energy by itself selects a canonical ensemble, whereas fixed average energy together with fixed average particle number selects a grand-canonical ensemble in the paper's setting. This is the connection the authors use when comparing massive Bose and Fermi carriers. Sen(De) et al., pp. 1–2.

A formalization would add a reusable statement linking three kinds of objects: operational accessible information, entropy maximization with conserved quantities, and a concrete optimal ensemble. The shared quantum definitions already exist on the platform; the Holevo and grand-canonical variational statements are Open goals, rather than machine-checked results claimed by this mission. The present draft has compile-checked statements, not proofs of the capacity theorem or those Open goals.

Difficulty

The accessible information is itself an optimization over measurements, while capacity optimizes it again over every admissible ensemble. Merely diagonalizing the grand-canonical state does not establish that no other ensemble, including an ensemble of mixed or noncommuting states, carries more accessible information. The matching attainment assertion also needs an ensemble of the paper's Fock states that obeys both average constraints. The comparison must use the same bit-valued entropy convention throughout, even though one existing grand-canonical platform theorem states its variational principle using natural logarithms.

Formalization scope

Lean represents states and observables by complex matrices indexed by a finite nonempty type, with H\mathcal HH and N^\hat NN^ Hermitian and commuting. The grand-canonical state uses the published Gibbs-state definition. Expected values are real parts of traces, and both constraints are equalities. The finite-dimensional model is exact for finitely many fermionic levels; it is a truncation of the unbounded bosonic Fock space, so this mission does not claim the paper's infinite-dimensional bosonic formula. The theorem permits every real β\betaβ and μ\muμ, with EEE and NNN defined from the resulting state.

The capacity domain includes all finite ensemble sizes and arbitrary mixed density matrices, and accessible information optimizes over all finite POVMs. Restricting the ensemble to Fock-diagonal or pure states, fixing its label type to the Fock basis, or fixing the measurement would turn the capacity claim into a different problem. The maximum is expressed as a greatest element of the value set, which records membership and hence attainment. The reusable work includes the ensemble entropy bound, the joint-eigenbasis interface, and the link between orthogonal signals and accessible information. Contributions that establish these links for the stated definitions or connect the existing Open reference theorems to this interface fit the mission. The paper's separately labelled comparison theorem for bosons and fermions, its asymptotic expansions, and its numerical figures are outside this mission.

Selected references

  • A. Sen(De), U. Sen, B. Gromek, D. Bruß, and M. Lewenstein, Capacities of Quantum Channels for Massive Bosons and Fermions, Physical Review Letters 2005; pinned preprint arXiv:quant-ph/0505028v2, 2006. arXiv
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Category TheoryDifferential Geometry·Captain: mikedeng1

Convenient Categories of Smooth Spaces: For Every Concrete Site, the Category of Concrete Sheaves Is a Quasitopos with All Small Limits and ColimitsResearch Paper

Motivation

Many spaces used in differential geometry are described by the maps permitted into them from simple domains. For a diffeological space, the domains are open subsets of Euclidean space; for a Chen space, they are convex subsets. A map between spaces is smooth when it sends permitted plots to permitted plots. Baez and Hoffnung use the language of concrete sheaves to put these examples in one setting and to explain why their categories share certain categorical properties (Baez–Hoffnung, §§1 and 4). A common theorem matters because it identifies which properties follow from the site of domains and its covers, without relying on a coordinate presentation of either kind of smooth space.

The paper first defines a quasitopos in Definition 8 and states the smooth-space application as Theorem 9, both on page 17. It then builds the general theory of concrete sites and DDD spaces in §§4–5. Theorem 52 on page 40 is the general result from which the smooth-space application follows, using the paper's identifications of Chen and diffeological spaces with suitable categories of DDD spaces (Baez–Hoffnung, Theorems 9 and 52). This mission targets that general theorem.

Setting

A site consists of a category DDD of domains and a coverage KKK. A covering family of a domain XXX is a family of arrows into XXX. The coverage requires that a cover can be refined after pulling it back along any arrow. A presheaf P:Dop→SetP:D^{\mathrm{op}}\to\mathrm{Set}P:Dop→Set assigns a set P(X)P(X)P(X) of plots to each domain and restricts plots along arrows. It is a sheaf when every compatible family of plots over a cover has exactly one amalgamating plot. Compatibility tests equality after further restriction along arrows into two members of the cover (Baez–Hoffnung, Definitions 10–15).

A concrete site has a terminal domain TTT. Maps T→XT\to XT→X are the points of XXX, and maps between domains are determined by their action on points. Every point of a covered domain must lift through some covering arrow. The site is also subcanonical: each representable presheaf Hom⁡(−,X)\operatorname{Hom}(-,X)Hom(−,X) is a sheaf. These are exactly the conditions of Definition 18, including the subcanonicity of Definition 17 (Baez–Hoffnung, p. 19).

A plot ϕ∈P(X)\phi\in P(X)ϕ∈P(X) has an underlying function ϕ‾:Hom⁡(T,X)→P(T)\underline\phi:\operatorname{Hom}(T,X)\to P(T)ϕ​:Hom(T,X)→P(T), defined by ϕ‾(d)=P(d)(ϕ)\underline\phi(d)=P(d)(\phi)ϕ​(d)=P(d)(ϕ). The presheaf is concrete if no two distinct plots have the same underlying function. A DDD space is a concrete sheaf, and a map of DDD spaces is a natural transformation of presheaves. Their category is written DSpace(D)\mathrm{DSpace}(D)DSpace(D) (Baez–Hoffnung, Definitions 19–20). Its underlying-set functor evaluates a DDD space at TTT.

Formalization targets

The goal is the full assertion of Theorem 52:

For every concrete site (D,K,T),DSpace(D) is a quasitopos with all small limits and colimits.\text{For every concrete site }(D,K,T),\quad \mathrm{DSpace}(D)\text{ is a quasitopos with all small limits and colimits.}For every concrete site (D,K,T),DSpace(D) is a quasitopos with all small limits and colimits.

A quasitopos is locally cartesian closed, has finite colimits, and has a weak subobject classifier. A weak classifier consists of an object Ω\OmegaΩ and a truth arrow ⊤:1→Ω\top:1\to\Omega⊤:1→Ω; each strong monomorphism i:A→Xi:A\to Xi:A→X is the pullback of ⊤\top⊤ along a unique characteristic arrow χi:X→Ω\chi_i:X\to\Omegaχi​:X→Ω. Local cartesian closure means that for every DDD space BBB, the slice DSpace(D)/B\mathrm{DSpace}(D)/BDSpace(D)/B is cartesian closed: it has finite products, and product with any object over BBB has a right adjoint. The paper gives these notions in Definitions 8, 38, 42, and 43 (Baez–Hoffnung, pp. 17, 30, 32–33).

The milestones follow the paper's proof, in order. Four of them are the results cited in the proof of Theorem 52: Proposition 39 (all small limits, computed pointwise), Proposition 40 (the weak subobject classifier), Proposition 45 (local cartesian closure), and Proposition 50 (all small colimits). Together they cover every clause of the target. The others are the results these four rest on:

  • Proposition 28: the underlying-set functor X↦X(T)X\mapsto X(T)X↦X(T) on DSpace(D)\mathrm{DSpace}(D)DSpace(D) is faithful;
  • Proposition 29: every representable presheaf is a DDD space;
  • Proposition 30: the presheaf Ω(X)={0,1}Hom⁡(T,X)\Omega(X)=\{0,1\}^{\operatorname{Hom}(T,X)}Ω(X)={0,1}Hom(T,X) is a DDD space;
  • Proposition 31: a map of DDD spaces is a monomorphism (epimorphism) exactly when its underlying function is injective (surjective);
  • Proposition 34: a map of DDD spaces is a strong monomorphism exactly when it makes its domain a subspace of its codomain;
  • Lemma 44: the comparison map X×AY→X×YX\times_A Y\to X\times YX×A​Y→X×Y is a strong monomorphism;
  • Lemma 47: concretization, which identifies plots with the same underlying function, is left adjoint to the inclusion of concrete presheaves;
  • Lemma 48: a concrete presheaf is separated for every cover;
  • Lemma 49: Grothendieck's plus construction turns a concrete presheaf into a DDD space.

The classifier in Proposition 40 is the paper's Ω\OmegaΩ of Proposition 30; the milestone states the existence property (Baez–Hoffnung, pp. 24–40).

Significance

The theorem provides a single categorical setting for several plot-based smooth-space constructions. All small limits and colimits allow diagrams of DDD spaces to be assembled within the same category. Local cartesian closure gives parametrized mapping spaces over an arbitrary base, while the weak classifier describes strong subspaces through characteristic maps. These are the specific convenient properties singled out by the paper, and Theorem 9 transfers them to the paper's smooth-space examples (Baez–Hoffnung, §§3 and 5).

The mathematical theorem is already proved in the cited preprint. This mission supplies Lean statements for its general hypotheses, categorical notions, the thirteen results of §5 its proof uses, and its final conclusion. The drafted theorem bodies contain sorry; the work remaining is to prove them and build reusable support for concrete sheaves, pointwise limits, parametrized mapping spaces, and concrete sheafification. A machine-checked development would permit later applications to particular sites without restating the same categorical infrastructure. The present draft does not claim a machine-checked proof.

Difficulty

Presheaf categories already have pointwise limits and colimits, but a pointwise construction need not visibly retain both the sheaf and concreteness conditions. In particular, pointwise colimits of concrete sheaves do not by themselves establish Proposition 50; the result must return to the category of concrete sheaves. For local cartesian closure, constructing a mapping object in the unsliced category handles only the case of a terminal base. Proposition 45 requires the corresponding statement in each slice and for each object over that base. A classifier for every monomorphism would ask for a different property: the paper classifies strong monomorphisms, while it gives examples showing that arbitrary monomorphisms need not be subspaces (Baez–Hoffnung, pp. 10 and 26–37).

Formalization scope

The Lean development fixes a universe uuu, a small category DDD with SmallCategory D, a coverage KKK, and a chosen terminal domain TTT with proof that it is terminal. Presheaves are Dop→TypeuD^{\mathrm{op}}\to\mathrm{Type}_uDop→Typeu​. A covering family is represented by a Mathlib presieve; repeated arrows have no effect on the sheaf or point-covering conditions. The sheaf predicate uses Presieve.IsSheafFor for each member of the coverage. Subcanonicity, faithfulness of Hom⁡(T,−)\operatorname{Hom}(T,-)Hom(T,−), and pointwise surjectivity of covers are all clauses of the concrete-site predicate. The smallness restriction and choice of Typeu\mathrm{Type}_uTypeu​ are explicit scope decisions: the preprint states its theorem for any concrete site, while this development works in Mathlib's small-site setting.

DSpace is the full subcategory of presheaves satisfying the sheaf and concreteness predicates. Its morphisms are natural transformations. The truth-value object uses Bool; the paper's set 2={0,1}2=\{0,1\}2={0,1} has the same two elements. Concretization is represented by the image of the map sending a plot to its underlying function, which is canonically the quotient described in Definition 46. The weak-classifier predicate carries a terminal object as existence data; the quasitopos predicate takes finite limits as an instance, reflecting the ambient assumption in Definition 38. The goal's limits clause supplies this instance. In the slice predicate, X×B−X\times_B-X×B​− is used; symmetry identifies it with the paper's −×BX-\times_B X−×B​X.

The classifier must classify strong monomorphisms, and local cartesian closure must range over every slice. Mathlib's Classifier, which classifies all monomorphisms, would make the goal false: the paper's example of the reals with the discrete structure mapping to the standard reals (p. 10) is a monomorphism that is not a subspace. Ordinary cartesian closure is only the case of a terminal base. A model with functions between underlying sets as morphisms would not be Definition 20 and would make Proposition 28 trivial. The complete proof will need Mathlib's coverage and sheaf APIs, strong monomorphisms, pullbacks, slice categories, adjunctions, and limit and colimit interfaces. The concrete-site and DDD-space definitions can be reused for further results of this paper. Lemma 44 takes the existence of the pullback and product as instance arguments, which Proposition 39 supplies; Lemma 47 states the adjunction as the universal property of the quotient map P→L(P)P\to L(P)P→L(P); Lemma 49 uses Mathlib's plus construction for the Grothendieck topology generated by KKK, as the paper's proof does. Contributions toward the milestone proofs are in scope; the site-specific equivalences used for Theorem 9 are outside this mission.

Selected references

  • John C. Baez and Alexander E. Hoffnung, Convenient categories of smooth spaces, arXiv:0807.1704v4, 2008 preprint (version dated 8 October 2009). arXiv
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Graph TheoryQuantum InformationTheoretical Computer Science·Captain: mikedeng1

Beyond product state approximations for a quantum analogue of Max Cut: Tensor Products of One- and Two-Qubit States Reach 0.55 of the Maximum Energy on Every Weighted GraphResearch Paper

Motivation

Classical Max Cut asks for a partition of the vertices of a weighted graph that maximises the total weight of edges crossing it. Its best-known approximation algorithm, due to Goemans and Williamson, rounds a semidefinite relaxation and guarantees ratio 0.8780.8780.878. Quantum Max Cut is the analogous problem for a family of local Hamiltonians: each edge contributes a two-qubit term that rewards the two qubits for being antisymmetric, and one asks for the maximum energy of the sum. Estimating it precisely is QMA-complete (Piddock and Montanaro), so attention has turned to efficient approximation algorithms, and to the question of which classes of quantum states can certify a good fraction of the optimum.

A short history of the approximation ratio on weighted graphs:

  • 2010. Briët, de Oliveira Filho and Vallentin give an efficient algorithm approximating the best product-state energy within 0.9560.9560.956; combined with the 1/21/21/2 bound of the next item, this approximates the optimum within 0.4780.4780.478, as observed by Gharibian and Liu.
  • 2012, product states, ratio 1/21/21/2. The best product state always has energy at least half the optimum (Gharibian and Kempe), and this is tight: on a single edge the optimum is the entangled singlet while every product state gets at most half its energy.
  • 2019. Gharibian and Parekh round an SDP relaxation of the quantum problem to product states, reaching 0.4980.4980.498.
  • 2020. Anshu, Gosset and Morenz (arXiv:2003.14394) show that allowing two-qubit entangled blocks breaks the 1/21/21/2 barrier on every weighted graph: some tensor product of one- and two-qubit states reaches 0.550.550.55 of the optimum. This mission formalizes that result.

Setting

Let G=(V,E,w)G=(V,E,w)G=(V,E,w) be a simple graph on V={0,…,n−1}V=\{0,\dots,n-1\}V={0,…,n−1} with nonnegative edge weights we≥0w_e\ge0we​≥0 (the paper's standing assumption). Each vertex carries a qubit; a state is a vector ψ∈C{0,1}n\psi\in\mathbb C^{\{0,1\}^n}ψ∈C{0,1}n, and it is a unit state if ∑x∣ψ(x)∣2=1\sum_x|\psi(x)|^2=1∑x​∣ψ(x)∣2=1. With the Pauli matrices X,Y,ZX,Y,ZX,Y,Z acting on qubit iii written Xi,Yi,ZiX_i,Y_i,Z_iXi​,Yi​,Zi​, the quantum Max Cut Hamiltonian is

HG=∑{i,j}∈Ewij hij,hij=12(I−XiXj−YiYj−ZiZj),H_G=\sum_{\{i,j\}\in E}w_{ij}\,h_{ij},\qquad h_{ij}=\tfrac12\bigl(I-X_iX_j-Y_iY_j-Z_iZ_j\bigr),HG​={i,j}∈E∑​wij​hij​,hij​=21​(I−Xi​Xj​−Yi​Yj​−Zi​Zj​),

each edge counted once. The term hijh_{ij}hij​ equals twice the projector onto the singlet (∣01⟩−∣10⟩)/2(|01\rangle-|10\rangle)/\sqrt2(∣01⟩−∣10⟩)/2​, so HGH_GHG​ is positive semidefinite, and

OPT(G)=∥HG∥=max⁡ψ unit⟨ψ∣HG∣ψ⟩.\mathrm{OPT}(G)=\|H_G\|=\max_{\psi\ \text{unit}}\langle\psi|H_G|\psi\rangle .OPT(G)=∥HG​∥=ψ unitmax​⟨ψ∣HG​∣ψ⟩.

Two weight statistics appear throughout: the total weight W=∑e∈EweW=\sum_{e\in E}w_eW=∑e∈E​we​ and, for a vertex vvv, max⁡e∼vwe\max_{e\sim v}w_emaxe∼v​we​, the largest weight of an edge incident to vvv (zero for an isolated vertex).

A tensor product of 1- and 2-qubit states φ=φ1⊗⋯⊗φL\varphi=\varphi_1\otimes\cdots\otimes\varphi_Lφ=φ1​⊗⋯⊗φL​ is obtained by partitioning the qubits into blocks of size one or two (a pair need not be an edge of GGG), choosing a unit vector of C2\mathbb C^2C2 or C4\mathbb C^4C4 for each block, and multiplying the block amplitudes. Product states (all blocks of size one) and singlets placed on a matching are examples; a generic entangled state of three qubits is not.

Formalization targets

Goal: Theorem 3 (p. 5)

For every graph with nonnegative weights there is a tensor product φ\varphiφ of 1- and 2-qubit states such that

⟨φ∣HG∣φ⟩OPT(G)  ≥  0.55.\frac{\langle\varphi|H_G|\varphi\rangle}{\mathrm{OPT}(G)}\;\ge\;0.55 .OPT(G)⟨φ∣HG​∣φ⟩​≥0.55.

The constant is the exact minimum of the optimisation problem (28) of the paper.

Milestones

The proof combines an upper bound on OPT(G)\mathrm{OPT}(G)OPT(G) with three candidate states:

  1. Eq. (10) and Lemma 1 (pp. 6–7): on a star with nonnegative weights, ∥L(G)∥≤∑ewe+max⁡ewe\|L(G)\|\le\sum_ew_e+\max_ew_e∥L(G)∥≤∑e​we​+maxe​we​ for the weighted Laplacian, and ∥HG∥≤max⁡ewe+∑ewe\|H_G\|\le\max_ew_e+\sum_ew_e∥HG​∥≤maxe​we​+∑e​we​.
  2. Weighted eq. (15) (p. 9): OPT(G)≤W+12∑vmax⁡e∼vwe\mathrm{OPT}(G)\le W+\frac12\sum_{v}\max_{e\sim v}w_eOPT(G)≤W+21​∑v​maxe∼v​we​.
  3. Weighted eqs. (18)–(19) and eq. (24) (pp. 8, 10): a computational basis state ∣z⟩|z\rangle∣z⟩ with ⟨z∣HG∣z⟩/OPT(G)≥13+23 W/(2W+∑vmax⁡e∼vwe)\langle z|H_G|z\rangle/\mathrm{OPT}(G)\ge\frac13+\frac23\,W/\bigl(2W+\sum_v\max_{e\sim v}w_e\bigr)⟨z∣HG​∣z⟩/OPT(G)≥31​+32​W/(2W+∑v​maxe∼v​we​).
  4. Lemma 2 (p. 10): a matching MMM and a forest FFF in EEE with ∑vmax⁡e∼vwe=∑e∈Mwe+∑e∈Fwe\sum_v\max_{e\sim v}w_e=\sum_{e\in M}w_e+\sum_{e\in F}w_e∑v​maxe∼v​we​=∑e∈M​we​+∑e∈F​we​.
  5. Eq. (25) (p. 10): singlets on MMM and uniformly random bits elsewhere have average energy 32m+12W\frac32m+\frac12W23​m+21​W, m=∑e∈Mwem=\sum_{e\in M}w_em=∑e∈M​we​.
  6. Eq. (26) (p. 11): a basis state with energy at least f=∑e∈Fwef=\sum_{e\in F}w_ef=∑e∈F​we​.
  7. Eq. (27) (p. 11): the best of the three states has ratio at least max⁡{2f, 3m+W, (4W+f+m)/3}/(2W+f+m)\max\{2f,\,3m+W,\,(4W+f+m)/3\}/(2W+f+m)max{2f,3m+W,(4W+f+m)/3}/(2W+f+m).
  8. Eqs. (28)–(29) (p. 11): max⁡{2y,3x+1,(4+x+y)/3}≥0.55 (2+x+y)\max\{2y,3x+1,(4+x+y)/3\}\ge0.55\,(2+x+y)max{2y,3x+1,(4+x+y)/3}≥0.55(2+x+y) for 0≤x≤y≤10\le x\le y\le10≤x≤y≤1.

Significance

The result shows that the 1/21/21/2 limitation of product states for quantum Max Cut is not a limitation of efficiently describable states: allowing entanglement only within disjoint pairs of qubits already guarantees a fraction strictly above 1/21/21/2 on every weighted graph, including those (a single heavy edge) where product states are stuck at exactly 1/21/21/2. The accompanying algorithmic statement (an efficient randomized algorithm with ratio ≥0.53\ge0.53≥0.53) improved the best known efficient approximation ratio at the time. The upper bound of Lemma 1 is a quantitative form of monogamy of entanglement on a star: the centre qubit cannot be maximally entangled with all of its neighbours.

The theorem is proved in the paper; none of it is formalized. A complete development gives a machine-checked model of a frustrated quantum spin Hamiltonian on arbitrary weighted graphs, a formal upper bound on its ground-state energy, and an explicit certified family of entangled states. The final step, (28)–(29), is evaluated in the paper "by a computer"; a formal proof replaces that evaluation.

Difficulty

The obvious upper bound, ∥HG∥≤∑ewe∥he∥=2W\|H_G\|\le\sum_ew_e\|h_e\|=2W∥HG​∥≤∑e​we​∥he​∥=2W, is too weak: it allows every edge to be maximally entangled simultaneously, and with it no ratio above 1/21/21/2 follows. The improvement needs the star bound of Lemma 1, which the paper derives from the Lieb–Mattis theorem on the spin of the ground state of bipartite antiferromagnets, restricting the problem to the Hamming-weight-one sector where the Hamiltonian becomes a weighted graph Laplacian. Neither Lieb–Mattis nor the angular-momentum decomposition of (C2)⊗n(\mathbb C^2)^{\otimes n}(C2)⊗n is available in Mathlib. The combinatorial side (Lemma 2) needs a careful choice of a maximal incident edge at each vertex and an argument that these edges form no cycle. Eq. (25) is an exact energy computation for a state that is entangled across a matching.

Formalization scope

  • Representation. Qubits are Fin n, basis configurations Fin n → Fin 2, states (Fin n → Fin 2) → ℂ, operators complex matrices indexed by configurations; onSite i σ places a 2×22\times22×2 matrix on qubit iii. The graph is a SimpleGraph (Fin n); weights are w : Sym2 (Fin n) → ℝ with ∀ e, 0 ≤ w e in every statement. HGH_GHG​ sums over the ordered representatives i<ji<ji<j of the edges, so each edge is counted once. The energy is the real part of ⟨ψ∣H∣ψ⟩\langle\psi|H|\psi\rangle⟨ψ∣H∣ψ⟩.
  • No OPT\mathrm{OPT}OPT as a supremum. OPT(G)\mathrm{OPT}(G)OPT(G) is not defined. Since HG⪰0H_G\succeq0HG​⪰0, a bound ⟨φ∣HG∣φ⟩≥c OPT(G)\langle\varphi|H_G|\varphi\rangle\ge c\,\mathrm{OPT}(G)⟨φ∣HG​∣φ⟩≥cOPT(G) is stated as c ⟨ψ∣HG∣ψ⟩≤⟨φ∣HG∣φ⟩c\,\langle\psi|H_G|\psi\rangle\le\langle\varphi|H_G|\varphi\ranglec⟨ψ∣HG​∣ψ⟩≤⟨φ∣HG​∣φ⟩ for every unit ψ\psiψ, with φ\varphiφ chosen before ψ\psiψ. Ratios are cleared of denominators; 0.550.550.55 is the real 11/2011/2011/20. Where the paper bounds PROD(G)\mathrm{PROD}(G)PROD(G) (eqs. (19), (24)), the item exhibits a computational basis state, which is a product state.
  • The class. A tensor product of 1- and 2-qubit states is given by an involution ppp of the qubits (the block of iii is {i,p(i)}\{i,p(i)\}{i,p(i)}), a unit vector of C2\mathbb C^2C2 for every fixed point, a unit vector of C4\mathbb C^4C4 for every pair, and the product of block amplitudes. The norm and disjointness conditions are part of the definition, so the class does not contain every state and the goal cannot be met by a top eigenvector.
  • Conventions. max⁡e∼vwe=0\max_{e\sim v}w_e=0maxe∼v​we​=0 for an isolated vertex and max⁡e∈Ewe=0\max_{e\in E}w_e=0maxe∈E​we​=0 for an edgeless graph. A star is a graph all of whose edges contain one centre; other vertices may be isolated. A forest is an edge set whose spanning subgraph is acyclic; a matching is an edge set whose distinct edges are disjoint. The singlet on {i,j}\{i,j\}{i,j}, i<ji<ji<j, is (∣01⟩−∣10⟩)/2(|01\rangle-|10\rangle)/\sqrt2(∣01⟩−∣10⟩)/2​ with qubit iii first.
  • Weighted forms. Eqs. (15) and (18)–(19) are written in the paper for unit weights and reused in weighted form in the proof of Theorem 3; the items state the weighted forms.
  • Not formalized. The second sentence of Theorem 3 (an efficient randomized algorithm with ratio ≥0.53\ge0.53≥0.53), the words "efficiently compute" in Lemma 2 and eq. (26) (existence only), the polynomial bound on the maximum weight (relevant only to running time), Theorems 1, 2, 4 and 5.
  • Infrastructure. Useful general results include the Pauli algebra of onSite, energies of computational basis states (equal to cut values), partial-trace style computations for tensor products of blocks, and a Laplacian/Gershgorin bound; the Hamiltonian layer is reusable for later quantum Max Cut missions. Contributions of any of these as separate lemmas are welcome.

Selected references

  • A. Anshu, D. Gosset, K. Morenz, Beyond product state approximations for a quantum analogue of Max Cut, TQC 2020; arXiv:2003.14394v1 (2020). https://arxiv.org/abs/2003.14394
  • S. Gharibian, O. Parekh, Almost optimal classical approximation algorithms for a quantum generalization of Max-Cut, APPROX/RANDOM 2019. https://arxiv.org/abs/1909.08846
  • J. Briët, F. M. de Oliveira Filho, F. Vallentin, The positive semidefinite Grothendieck problem with rank constraint, ICALP 2010. https://arxiv.org/abs/0910.5765
  • S. Gharibian, J. Kempe, Approximation algorithms for QMA-complete problems, SIAM J. Comput. 41(4) (2012). https://arxiv.org/abs/1101.3884
  • M. X. Goemans, D. P. Williamson, Improved approximation algorithms for maximum cut and satisfiability problems using semidefinite programming, J. ACM 42 (1995). https://doi.org/10.1145/227683.227684
  • S. Piddock, A. Montanaro, The complexity of antiferromagnetic interactions and 2D lattices, arXiv preprint (2015). https://arxiv.org/abs/1506.04014
  • E. Lieb, D. Mattis, Ordering energy levels of interacting spin systems, J. Math. Phys. 3 (1962). https://doi.org/10.1063/1.1724276
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AlgebraMathematical PhysicsQuantum Information·Captain: mikedeng1

Permutation and Its Partial Transpose: A Linear Combination of Identity, Permutation and Its Partial Transpose Solves the Braid Relation and the Yang–Baxter Equations Only in Dimension TwoResearch Paper

Why these operators matter

Permutation of tensor factors is a basic operation in quantum information and in the algebra of braids. A braid representation assigns an operator to each crossing so that different drawings of the same braid act identically. A Yang–Baxter equation adds spectral parameters to this local consistency condition; such families appear in integrable lattice models and in constructions of quantum gates. The paper by Zhang, Kauffman, and Werner asks when one operator family built from permutation and partial transpose can meet both requirements. It connects two familiar operations on bipartite matrices with algebraic relations on three tensor factors.

The article studies several related representations and two main theorems. This mission concerns Theorem 1 in §6.3 and the source equations that support it. The theorem is a classification of a specific three-term family, not a claim about arbitrary Yang–Baxter solutions. The paper's printed wording has degenerate counterexamples already present elsewhere in the same article. The target here makes their exclusions explicit, so that the formal statement records the intended classification. The source is the first arXiv version, quant-ph/0606005v1; page and equation numbers below refer to that version.

Operators and equations

Fix an integer d≥2d\ge2d≥2 and let V=CdV=\mathbb C^dV=Cd with its standard basis. The permutation operator PPP acts on V⊗VV\otimes VV⊗V by P∣ij⟩=∣ji⟩P|ij\rangle=|ji\rangleP∣ij⟩=∣ji⟩. The partial transpose Θ2\Theta_2Θ2​ transposes the matrix index belonging to the second copy of VVV. Write P∗=Θ2(P)P_*=\Theta_2(P)P∗​=Θ2​(P). This operator is ∑i,j∣ii⟩⟨jj∣\sum_{i,j}|ii\rangle\langle jj|∑i,j​∣ii⟩⟨jj∣ and satisfies P∗2=dP∗P_*^2=dP_*P∗2​=dP∗​. In dimension two the paper also uses P∗=1−P∗P^*=\mathbf1-P_*P∗=1−P∗​; the star's position matters, since P∗P^*P∗ and P∗P_*P∗​ are different matrices. These definitions and identities are in §2.1, pp. 5–6.

For fixed complex coefficients aaa and bbb, the family under study is

Rˇ(u)=a1+uP+bP∗.\check R(u)=a\mathbf1+uP+bP_*.Rˇ(u)=a1+uP+bP∗​.

Here u∈Cu\in\mathbb Cu∈C is the spectral parameter: it is the coefficient of PPP. On V⊗3V^{\otimes3}V⊗3, the subscripts iii and i+1i+1i+1 mean that an operator acts on the first two or last two factors, with the identity on the unused factor. The braid relation is RˇiRˇi+1Rˇi=Rˇi+1RˇiRˇi+1\check R_i\check R_{i+1}\check R_i=\check R_{i+1}\check R_i\check R_{i+1}Rˇi​Rˇi+1​Rˇi​=Rˇi+1​Rˇi​Rˇi+1​. The paper considers two parameterized versions, with multiplicative law xyxyxy in equation (14) and additive law u+vu+vu+v in equation (15):

Rˇi(x)Rˇi+1(xy)Rˇi(y)=Rˇi+1(y)Rˇi(xy)Rˇi+1(x),Rˇi(u)Rˇi+1(u+v)Rˇi(v)=Rˇi+1(v)Rˇi(u+v)Rˇi+1(u).\begin{aligned} \check R_i(x)\check R_{i+1}(xy)\check R_i(y)&=\check R_{i+1}(y)\check R_i(xy)\check R_{i+1}(x),\\ \check R_i(u)\check R_{i+1}(u+v)\check R_i(v)&=\check R_{i+1}(v)\check R_i(u+v)\check R_{i+1}(u). \end{aligned}Rˇi​(x)Rˇi+1​(xy)Rˇi​(y)Rˇi​(u)Rˇi+1​(u+v)Rˇi​(v)​=Rˇi+1​(y)Rˇi​(xy)Rˇi+1​(x),=Rˇi+1​(v)Rˇi​(u+v)Rˇi+1​(u).​

The equations are identities for all indicated parameter pairs, with a,ba,ba,b fixed. The source gives the braid relation as (54), defines the family in (69), and states the two Yang–Baxter forms in §3.1 and §5.

Formalization targets

Corrected Theorem 1

For d≥2d\ge2d≥2 and a≠0a\ne0a=0, classify this family by three equivalences. At every nonzero uuu,

Rˇ(u) satisfies (54)⟺d=2 and (a=−b or a=b=−u).\check R(u)\text{ satisfies (54)}\quad\Longleftrightarrow\quad d=2\text{ and }\bigl(a=-b\text{ or }a=b=-u\bigr).Rˇ(u) satisfies (54)⟺d=2 and (a=−b or a=b=−u).

If b≠0b\ne0b=0, the family satisfies the additive equation (15) for all u,vu,vu,v exactly when d=2d=2d=2 and a=−ba=-ba=−b. The family satisfies the multiplicative equation (14) for all x,yx,yx,y exactly under the same dimension and coefficient condition. The source's “only for” statement and the sufficiency part of its proof support equivalences; the explicit guards correct the printed exceptions. This is the mission goal.

Supporting equations

The milestones capture the source's operator identities PP∗=P∗P=P∗PP_*=P_*P=P_*PP∗​=P∗​P=P∗​ and P∗2=dP∗P_*^2=dP_*P∗2​=dP∗​; the dimension-two braid and mixed relations (66)–(67) for PPP and P∗P^*P∗; the second dimension-two braid branch displayed in (70); the coloured identity (74) for aP∗+uPaP^*+uPaP∗+uP; the necessary coefficient system (127) above dimension two; and Appendix B's higher-dimensional exclusions, stated with the same corrected guards. These are the source's own named or displayed claims in the order useful to a reader of the goal.

What the classification gives

The result locates the precise dimension in which this particular linear combination supplies braid and spectral-parameter solutions simultaneously. It also distinguishes two braid branches: a=−ba=-ba=−b gives the parameterized family aP∗+uPaP^*+uPaP∗+uP, while a=b=−ua=b=-ua=b=−u gives another fixed braid matrix. Above dimension two, with the stated nonzero conditions, neither branch survives as a solution of the three requested relations. This keeps a tempting general-dimensional extrapolation from being treated as a theorem.

The source result is a published mathematical argument, but these Lean statements are proposed open goals. A completed mission would produce machine-checked proofs for the classification and its selected intermediate identities in one reusable matrix representation. The definitions of permutation, partial transpose, and the two three-factor placements may also serve later formalizations of braid and Yang–Baxter calculations. This mission does not claim to formalize the paper's second theorem, its full virtual braid group development, or its later applications to gates and Hamiltonians.

Where the mathematical work lies

The dimension-two formulas are finite matrix identities, but the classification asks for necessity as well as sufficiency. Verifying the displayed solution matrices alone cannot rule out other coefficients. In higher dimension the paper compares terms in an expansion on three tensor factors. Its observation that the ambient vector space has dimension d3>15d^3>15d3>15 does not by itself establish independence of the 15 operators being compared; a formal proof must justify every coefficient conclusion that it uses. Appendix B's sentence about a unique solution at fixed parameters also has degenerate counterexamples, so the milestone records only the necessary equations (127). These issues make the source's computational looking argument a substantive formalization task.

Formalization scope

The Lean model takes V=CdV=\mathbb C^dV=Cd and represents two-factor and three-factor operators by matrices indexed by Fin d × Fin d and Fin d × Fin d × Fin d. Fin d starts at zero while the paper labels basis vectors from one; this only changes names of indices. Tensor placement is defined entrywise, with the identity matrix on the unused factor. Scalars and spectral parameters are complex. The goal quantifies over every natural-number dimension d≥2d\ge2d≥2, every fixed a,ba,ba,b with a≠0a\ne0a=0, and every indicated spectral parameter. In (14), the paper introduces x=eux=e^ux=eu and y=evy=e^vy=ev, hence initially nonzero. The Lean predicate quantifies over all complex x,yx,yx,y; for polynomial matrix identities these formulations are equivalent.

The definition P∗=Θ2(P)P_*=\Theta_2(P)P∗​=Θ2​(P) is retained explicitly. Replacing it by an unrelated matrix with a convenient identity, fixing the dimension to two in every definition, or varying the coefficient bbb as the spectral parameter would change the problem. The guard u≠0u\ne0u=0 excludes the higher-dimensional braid family 1+vP∗\mathbf1+vP_*1+vP∗​ from §6.1, (60), and b≠0b\ne0b=0 excludes the rational additive solution a1+uPa\mathbf1+uPa1+uP in §3.2, (21). At d=1d=1d=1, all three basic matrices are scalar, so the paper's implicit d≥2d\ge2d≥2 convention is stated. Contributions that establish the shared identities, the two-dimensional coefficient classification, or the uniform higher-dimensional exclusions all advance the target.

Selected references

  • Y. Zhang, L. H. Kauffman, and R. F. Werner, Permutation and Its Partial Transpose, International Journal of Quantum Information, 2006; arXiv:quant-ph/0606005v1. This mission cites the pinned preprint's numbering.
8 thms2 active usersReviewed
Group TheoryQuantum Error CorrectionQuantum Information·Captain: mikedeng1

Restrictions on Transversal Encoded Quantum Gate Sets: For Any Nontrivial Local-Error-Detecting Quantum Code, the Transversal Logical Unitary Operators Are Not UniversalResearch Paper

Motivation

A quantum computer that runs long computations must protect its data with a quantum error-correcting code and must compute on the encoded data without letting errors spread. The simplest gates with that property are transversal gates: a code is laid out in several code blocks, and a transversal gate couples each physical subsystem of one block only to the corresponding subsystem of the other blocks, so a single fault never becomes several faults inside one block (Gottesman 1997; Aliferis, Gottesman, Preskill 2006). Every known code has some encoded gate that is not transversal, and fault-tolerant schemes pay for the missing gates with expensive constructions such as magic-state distillation. Whether some code has a universal transversal gate set was a long-standing question.

Timeline.

  • 2007: Zeng, Cross and Chuang show that transversal gates are not universal for stabilizer codes on qubits (arXiv:0706.1382).
  • 2008: Chen, Chung, Cross, Zeng and Chuang extend this to stabilizer codes on qudits (arXiv:0801.2360).
  • 2008–2009: Eastin and Knill prove the statement for every code that detects an arbitrary error on any single subsystem, stabilizer or not (arXiv:0811.4262; Phys. Rev. Lett. 102, 110502, 2009). This is the result of the present mission, now called the Eastin–Knill theorem.

Setting

A composite quantum system Q\mathcal QQ consists of finitely many physical subsystems jjj, subsystem jjj having dimension djd_jdj​. Operators on Q\mathcal QQ are complex matrices on Cd1⊗⋯⊗Cdn\mathbb C^{d_1}\otimes\cdots\otimes\mathbb C^{d_n}Cd1​⊗⋯⊗Cdn​. A product operator is ⨂jUj\bigotimes_j U_j⨂j​Uj​ with UjU_jUj​ acting on subsystem jjj, and T\mathcal TT is the group of unitary product operators (Uj∈U(dj)U_j \in \mathcal U(d_j)Uj​∈U(dj​)).

A quantum code is a subspace of the state space, represented by the orthogonal projector PPP onto it; its dimension rank⁡P\operatorname{rank} PrankP is the dimension of the encoded system, and the code is nontrivial when this dimension is at least 222. An error EEE is detectable when PEP∝PPEP \propto PPEP∝P. The code is local-error-detecting when every error on any single subsystem is detectable: P (I⊗E⊗I) P∝PP\,(I\otimes E\otimes I)\,P \propto PP(I⊗E⊗I)P∝P for every operator EEE acting on one subsystem.

A unitary UUU is logical when it preserves the code space,

(I−P) U P=0(Eq. (1)),(I-P)\,U\,P = 0 \qquad \text{(Eq. (1))},(I−P)UP=0(Eq. (1)),

and G\mathcal GG denotes the logical unitary product operators. An encoded unitary is a unitary operator WWW of the code space (PWP=WPWP = WPWP=W, W†W=WW†=PW^\dagger W = WW^\dagger = PW†W=WW†=P). A set SSS of unitaries is universal when every encoded unitary is approximated to arbitrary accuracy by the actions PUPPUPPUP, U∈SU \in SU∈S, on the code space.

For a code made of blocks bbb, each with subsystems at the same positions jjj and a block code PbP_bPb​, the joint code is P=⨂bPbP = \bigotimes_b P_bP=⨂b​Pb​. The transversal part jjj collects subsystem jjj of every block, and a transversal unitary is a product of unitaries, one on each transversal part.

Formalization targets

Goal: Corollary 1

For block codes PbP_bPb​, each local-error-detecting, with rank⁡⨂bPb≥2\operatorname{rank}\bigotimes_b P_b \ge 2rank⨂b​Pb​≥2, the set G\mathcal GG of transversal logical unitaries is not universal:

{ W:PWP=W, W†W=WW†=P } ⊈ { PUP:U∈G }‾.\{\,W : PWP = W,\ W^\dagger W = WW^\dagger = P\,\}\ \not\subseteq\ \overline{\{\,PUP : U \in \mathcal G\,\}}.{W:PWP=W, W†W=WW†=P} ⊆ {PUP:U∈G}​.

Theorem 1 (milestone)

The same conclusion for product operators on the physical subsystems of a single local-error-detecting code with rank⁡P≥2\operatorname{rank} P \ge 2rankP≥2.

Milestones on the way

In attack order: Lemma 1 (logical unitaries form a group); Lemma 2 (logical unitaries in a closed group of unitaries form a closed subgroup); T\mathcal TT is a compact group; the derivative step (I−P)DP=0(I-P)DP = 0(I−P)DP=0; elements of the Lie algebra of T\mathcal TT are sums of local Hermitian operators; DP∝PDP \propto PDP∝P for a logical sum of local Hermitians; the identity component C\mathcal CC of G\mathcal GG acts on the code space as a scalar; G\mathcal GG has finitely many actions on the code space up to phase; Theorem 1; and the detectability of an error on a single transversal part.

Significance

The result. The theorem rules out the simplest route to fault tolerance for every code that detects single-subsystem errors, which includes every code of distance at least 222. It explains why every fault-tolerant architecture needs a non-transversal ingredient (state injection and distillation, code switching, gauge fixing, measurements with feed-forward), and it is the starting point for later refinements: approximate and covariant versions for continuous symmetries (Faist et al. 2020), and restrictions on the level of the Clifford hierarchy reachable transversally (Bravyi–König 2013).

Formalizing it. The result is proved; no machine-checked proof of it is known to exist. The mission produces a checked statement of the theorem for arbitrary finite-dimensional subsystems and arbitrary (non-stabilizer) codes, together with a reusable layer: tensor-product operators on index-typed subsystems, codes as projectors, logical operators, local error detection, encoded universality and block codes. Related platform items are QAlgorithms_Defs_QECC (qubit stabilizer codes, detectability for submodule codes) and QAlgorithms.GottesmanIntro.knillLaflamme (the error-correction criterion), which use a different model of codes and are not imported here.

Difficulty

The paper's argument runs through Lie theory: G\mathcal GG is a closed subgroup of the compact group T\mathcal TT, so it is a compact Lie group with finitely many connected components; its identity component is generated by exponentials of its Lie algebra, and local error detection forces that Lie algebra to act on the code space by scalars. None of this is about the code alone; the difficulty is the passage from a closed matrix group to its Lie algebra and back (exponential coordinates, connectedness of the identity component, finiteness of the component group of a compact Lie group). Mathlib has the matrix exponential and compactness of the unitary group but not Cartan's closed-subgroup theorem or the Lie algebra of a closed matrix group.

A frequent first idea, that G\mathcal GG itself is a finite group, is false: every global phase eiθIe^{i\theta}IeiθI is a logical product unitary, so G\mathcal GG always contains a circle. Only the action of G\mathcal GG on the code space is finite, and only up to phase; a statement that ignores the phase is false.

Formalization scope

Subsystem jjj is a finite index type αj\alpha_jαj​ (so dj=∣αj∣d_j = |\alpha_j|dj​=∣αj​∣), and the system has basis ∏jαj\prod_j \alpha_j∏j​αj​; operators are Matrix over ℂ, unitaries are Matrix.unitaryGroup. A code is its projector (Hermitian, idempotent) and its dimension is Matrix.rank; "nontrivial" is 2≤rank⁡P2 \le \operatorname{rank} P2≤rankP. Closure is in the standard topology on complex matrices, which is the topology of any norm. Exponentials are NormedSpace.exp with the factor iii of the physics convention (footnote 1).

Disclosed restatements:

  1. "Lie group/Lie subgroup" (Lemma 2, T\mathcal TT) is stated as closed or compact subgroup; Cartan's theorem is not in Mathlib.
  2. "DDD in the Lie algebra" is stated through the one-parameter group t↦eitDt\mapsto e^{itD}t↦eitD.
  3. The real coefficients αj\alpha_jαj​ in D=∑jαjHjD = \sum_j \alpha_j H_jD=∑j​αj​Hj​ are absorbed into the Hermitian HjH_jHj​.
  4. The page's "the constant of proportionality must be one" is a slip (global phases lie in C\mathcal CC); the identity-component and finite-actions milestones state CP∝PCP \propto PCP∝P and GP=c FPGP = c\,FPGP=cFP.
  5. Corollary 1's code blocks are a tensor product of block codes PbP_bPb​ with common positions jjj and possibly different codes and dimensions; a single block is Theorem 1.

Universality is defined only through approximation of encoded unitaries, local error detection quantifies over every matrix on one subsystem, and G\mathcal GG is the full intersection of T\mathcal TT with the logical unitaries, so no hypothesis trivializes the conclusion; at rank 111 the conclusion is false, which is why the rank hypothesis is ≥2\ge 2≥2 and not P≠0P \ne 0P=0.

A complete development needs the Lie algebra of a closed subgroup of Matrix.unitaryGroup, connectedness of the identity component via exponentials, and finiteness of the component group of a compact matrix group. These parts are reusable far beyond this mission, and contributions of them, as well as alternative proofs of Theorem 1 that avoid Lie theory, are welcome.

Selected references

  • B. Eastin, E. Knill, Restrictions on Transversal Encoded Quantum Gate Sets, Phys. Rev. Lett. 102, 110502 (2009). https://arxiv.org/abs/0811.4262
  • B. Zeng, A. Cross, I. L. Chuang, Transversality versus Universality for Additive Quantum Codes, IEEE Trans. Inf. Theory 57 (2011). https://arxiv.org/abs/0706.1382
  • X. Chen, H. Chung, A. W. Cross, B. Zeng, I. L. Chuang, Subsystem stabilizer codes cannot have a universal set of transversal gates for even one encoded qudit, Phys. Rev. A 78, 012353 (2008). https://arxiv.org/abs/0801.2360
  • D. Gottesman, Stabilizer Codes and Quantum Error Correction, PhD thesis, Caltech (1997). https://arxiv.org/abs/quant-ph/9705052
  • S. Bravyi, R. König, Classification of topologically protected gates for local stabilizer codes, Phys. Rev. Lett. 110, 170503 (2013). https://arxiv.org/abs/1206.1609
  • P. Faist et al., Continuous symmetries and approximate quantum error correction, Phys. Rev. X 10, 041018 (2020). https://arxiv.org/abs/1902.07714
12 thms2 active usersReviewed
EconomicsOperations Research·Captain: mikedeng1

Curtailing Bank Loan and Loan Insurance Under Risk Regulations in Supply Chain Finance: In the Insurance-Cooperation Region a Lower Initial Loan Limit and a Higher Fixed Bank Fee Benefit the SupplierResearch Paper

Why bank credit limits matter in supply chain finance

Small retailers often cannot pay for their orders out of their own capital and borrow from banks to do so. Banks in turn are regulated: risk-control rules such as value-at-risk caps limit how much they may lend against an uncertain revenue, and they charge fixed fees to process a loan. Loan insurance, offered by insurers or guaranteed by governments, relaxes those caps for a premium. The common view, in practice and in policy discussions of financing for small firms, is that a higher credit limit and a cheaper loan help every firm in the supply chain.

Wang and Cai (Management Science, 2023) study a supplier selling to such a capital-constrained buyer and show that the common view fails in a precise region of parameters. They build on the capital-constrained newsvendor literature, which studies how financing frictions distort ordering and pricing (Buzacott and Zhang, 2004; Kouvelis and Zhao, 2012), and on the price-only wholesale contract of Lariviere and Porteus (2001), whose equilibrium price wEw^EwE and quantity QEQ^EQE are the benchmark without any capital constraint.

Setting

Demand ξ\xiξ for a product with retail price 111 has distribution function FFF, complementary distribution Fˉ=1−F\bar F = 1 - FFˉ=1−F, density fff on [0,∞)[0, \infty)[0,∞) and failure rate h=f/Fˉh = f/\bar Fh=f/Fˉ, and satisfies the increasing generalized failure rate (IGFR) property: xh(x)x h(x)xh(x) is increasing. The expected sales of an order QQQ are S(Q)=Emin⁡(ξ,Q)=Q−∫0QF(x) dxS(Q) = \mathbb E\min(\xi, Q) = Q - \int_0^Q F(x)\,dxS(Q)=Emin(ξ,Q)=Q−∫0Q​F(x)dx.

A supplier with unit cost c∈(0,1)c \in (0, 1)c∈(0,1) sets a wholesale price www. A buyer with initial capital lll then chooses an order QQQ and how to finance it:

  1. with its own capital, spending wQ≤lwQ \le lwQ≤l, for an expected profit S(Q)−wQS(Q) - wQS(Q)−wQ;
  2. with a bank loan, spending wQ≤u+l−τwQ \le u + l - \tauwQ≤u+l−τ, for S(Q)−wQ−τS(Q) - wQ - \tauS(Q)−wQ−τ, where uuu is the initial loan limit and τ\tauτ the fixed bank fee;
  3. with an insured bank loan, spending wQ≤v+l−τ−twQ \le v + l - \tau - twQ≤v+l−τ−t, for S(Q)−wQ−τ−tS(Q) - wQ - \tau - tS(Q)−wQ−τ−t, where vvv is the insured loan limit and ttt the fixed insurance premium.

The supplier earns (w−c)Q(w - c)Q(w−c)Q. The game is a Stackelberg game solved backwards, with the paper's goodwill tie-breaking rule: a firm indifferent between choices picks the one better for the other firm. ΠSI∗\Pi^{I*}_SΠSI∗​ and ΠBI∗\Pi^{I*}_BΠBI∗​ denote the supplier's and the buyer's equilibrium profits.

The equilibrium is described through explicit thresholds. tk(w)t_k(w)tk​(w) is the buyer's additional revenue from insurance at price www (the paper's equation (A-7)); the buyer insures exactly when t≤tk(w)t \le t_k(w)t≤tk​(w). w1t<w2tw^t_1 < w^t_2w1t​<w2t​ are the two roots of tk(w)=tt_k(w) = ttk​(w)=t. With w2aw^a_2w2a​, wsw_sws​ and wminw_{min}wmin​ defined in the paper's appendix, wI=max⁡(w2a,wE)w_I = \max(w^a_2, w^E)wI​=max(w2a​,wE) and wII=max⁡(ws,wmin)w_{II} = \max(w_s, w_{min})wII​=max(ws​,wmin​). The insurance-cooperation region (Area II) is

tk(wI)<t≤tk(wII).t_k(w_I) < t \le t_k(w_{II}).tk​(wI​)<t≤tk​(wII​).

In it, the equilibrium price is w2tw^t_2w2t​: the supplier lowers its price just enough for the buyer to be willing to insure.

Formalization targets

Goal: Proposition 2 part 2

Assume u+l−τ<wEQEu + l - \tau < w^E Q^Eu+l−τ<wEQE, v>uv > uv>u and the paper's global assumptions, and Area II. Then

ΠSI∗ strictly decreases in u,ΠBI∗ strictly increases in u,\Pi^{I*}_S \text{ strictly decreases in } u, \qquad \Pi^{I*}_B \text{ strictly increases in } u,ΠSI∗​ strictly decreases in u,ΠBI∗​ strictly increases in u, ΠBI∗ strictly decreases in τ,ΠSI∗ strictly increases in τ  if v+l−τ−t≥w2tFˉ−1(w2t).\Pi^{I*}_B \text{ strictly decreases in } \tau, \qquad \Pi^{I*}_S \text{ strictly increases in } \tau \ \text{ if } v + l - \tau - t \ge w^t_2\bar F^{-1}(w^t_2).ΠBI∗​ strictly decreases in τ,ΠSI∗​ strictly increases in τ  if v+l−τ−t≥w2t​Fˉ−1(w2t​).

The monotonicity is stated along every segment of uuu (or τ\tauτ) on which the hypotheses hold at each point, and for every equilibrium at the two ends.

Milestones

In attack order: the buyer's best response and the threshold tkt_ktk​ (Lemma A.7), its monotonicity and unimodality (Lemma A.7, "Moreover"), the shape of the supplier's profit in www (Lemma A.8), the monotonicity of wsw_sws​ (Lemma A.9), the equilibrium in Area II (Proposition 1 item 1(b), including existence), the comparative statics of w2tw^t_2w2t​ (Proposition A.8, "Moreover"), and the closed-form equilibrium profits in Area II (proof of Proposition 2).

Significance

The result reverses an intuition that regulators and firms rely on: a tighter or costlier bank loan, normally a loss for everyone, here benefits the supplier, because the buyer is pushed towards insurance and the supplier then needs to cut its price less to keep the buyer insuring. The buyer loses at the same time, so the two firms' interests over bank credit terms conflict in this region. The paper builds on this a parallel statement about curtailing loan insurance (Proposition 3) and a Stackelberg prisoner's dilemma (Proposition 5); both are outside this mission.

The paper's proofs are derivative computations through the implicit function theorem applied to piecewise-defined thresholds, with several details left to figures. A machine-checked proof would pin down the exact hypotheses under which the region exists and the claims hold, settle the role of the tie-breaking rule (without which no equilibrium exists in Area II), and give a reusable formal model of a capital-constrained newsvendor with several financing modes. No part of the paper has been formalized before.

Difficulty

The obvious argument differentiates the closed-form equilibrium profits in uuu and τ\tauτ. It requires first knowing that the equilibrium is the price w2tw^t_2w2t​ throughout a segment of parameters, which in turn needs the full best-response analysis of the buyer (three financing modes, two binding regimes for each loan cap), the unimodality of tkt_ktk​, and the comparison of the supplier's profit at w2tw^t_2w2t​ with its profit at the competing price w2uw^u_2w2u​. Each threshold is defined as a root of an equation involving Fˉ−1\bar F^{-1}Fˉ−1 and S−1S^{-1}S−1, and the region boundaries tk(wI)t_k(w_I)tk​(wI​) and tk(wII)t_k(w_{II})tk​(wII​) themselves move with uuu and τ\tauτ. The implicit function theorem gives local derivative signs; turning them into strict monotonicity along a segment needs continuity of the thresholds across the switches between regimes.

Formalization scope

All quantities are real numbers. Demand is a probability measure on R\mathbb RR with a density that vanishes on (−∞,0)(-\infty, 0)(−∞,0), is continuous and positive on the positive open support, with finite mean and the IGFR property; continuity, positivity and the finite mean are added to the paper and disclosed. Expected sales use the published SupplyChainTheory.expSales. IGFR is imposed where the failure rate is defined, on the positive support with Fˉ>0\bar F>0Fˉ>0; this includes bounded-support demand laws such as the uniform distribution. Prices range over (0,1](0, 1](0,1]. The loan limits u,vu, vu,v are parameters; their value-at-risk derivation is not modelled. In the supplier's threshold wsw_sws​, an inverse of expected sales above its range is treated as +∞+\infty+∞ inside the minimum with the finite unconstrained order. Lemma A.8's buyer profit is nonincreasing in price; strict decrease additionally requires positive initial capital, since with zero capital and a positive bank fee the buyer can earn zero throughout a high-price interval.

Every threshold is defined from the paper's own equation as an infimum or supremum of an explicitly named set, never passed as a free parameter. The goal is about the game's equilibria (IsEquilibrium) on the region AreaII; restating it about w2tw^t_2w2t​ and the closed-form profits, or defining the profits or Area II through the equilibrium's expected shape, would trivialize it and is excluded. Proposition 1 item 1(b) asserts existence of an equilibrium in Area II, so the goal is not vacuous.

A complete development needs the inverse functions Fˉ−1\bar F^{-1}Fˉ−1 and S−1S^{-1}S−1 and their continuity and derivatives, the newsvendor with a spending cap, and the implicit-function arguments for the roots. The capped newsvendor and the financing-mode best response are reusable for other supply-chain-finance missions. Contributions to any milestone, and to the missing lemmas about Fˉ−1\bar F^{-1}Fˉ−1 under IGFR, are welcome.

Selected references

  • W. Wang and G. Cai, Curtailing bank loan and loan insurance under risk regulations in supply chain finance, Management Science, 2023 (authors' accepted version, SSRN 3760840). https://ssrn.com/abstract=3760840
  • M. A. Lariviere and E. L. Porteus, Selling to the newsvendor: An analysis of price-only contracts, Manufacturing & Service Operations Management 3(4), 2001. https://doi.org/10.1287/msom.3.4.293.9971
  • J. A. Buzacott and R. Q. Zhang, Inventory management with asset-based financing, Management Science 50(9), 2004. https://doi.org/10.1287/mnsc.1040.0278
  • P. Kouvelis and W. Zhao, Financing the newsvendor: Supplier vs. bank, and the structure of optimal trade credit contracts, Operations Research 60(3), 2012. https://doi.org/10.1287/opre.1120.1051
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EconomicsOperations Research·Captain: mikedeng1

Sales Information Transparency and Trust in Repeated Vertical Relationships: Sharing Past Sales Information Benefits the Retailer if and only if Its Discount Factor Is at Most 1/(1+√(1+p))Research Paper

Why past sales information matters in a repeated supply relationship

A manufacturer that sells through a retailer usually knows less about end-customer demand than the retailer does. In the classical one-shot screening model (Laffont and Martimort, 2002) the manufacturer offers a menu of quantity–payment pairs, pays the well-informed retailer an information rent to reveal high demand, and distorts the low-demand quantity downward to keep that rent small. Real vertical relationships are repeated, and after each selling season the retailer can choose whether to share its past sales data (point-of-sale data, sell-through reports) with the manufacturer. Such data says nothing about future demand when demand is i.i.d., yet it lets the manufacturer check, after the fact, whether the retailer reported truthfully.

Shamir and Yehezkel (2023) ask when the retailer, who owns the data, wants to share it. The manufacturer can never lose from more information, since it can ignore it. The retailer's side is the interesting one: sharing lets the manufacturer punish misreports and so cut the retailer's rent for a given quantity, but it also lets the manufacturer raise the low-demand quantity, which increases the rent. The paper's main result, Proposition 3, gives an explicit threshold on the discount factor that separates the two cases. The question belongs to the literature on trust and information sharing in supply chains (for example Özer, Zheng and Chen, 2011).

The model

In every period demand is high (HHH) with probability ppp and low (LLL) with probability 1−p1-p1−p, independently across periods. The inverse demand is linear, P(q;θ)=Vθ−qP(q;\theta) = V_\theta - qP(q;θ)=Vθ​−q with VH>VLV_H > V_LVH​>VL​, so the retailer's revenue from quantity qqq in state θ\thetaθ is πR(q;θ)=(Vθ−q)q\pi_R(q;\theta) = (V_\theta - q)qπR​(q;θ)=(Vθ​−q)q, and Δ(q)=πR(q;H)−πR(q;L)\Delta(q) = \pi_R(q;H) - \pi_R(q;L)Δ(q)=πR​(q;H)−πR​(q;L). The retailer observes the state before ordering; the manufacturer does not.

The manufacturer offers a menu {(qH,TH),(qL,TL)}\{(q_H,T_H),(q_L,T_L)\}{(qH​,TH​),(qL​,TL​)}: quantity qθq_\thetaqθ​ for the payment TθT_\thetaTθ​. The per-period expected profits are

ΠR=p(πR(qH;H)−TH)+(1−p)(πR(qL;L)−TL),ΠM=pTH+(1−p)TL.\Pi_R = p(\pi_R(q_H;H) - T_H) + (1-p)(\pi_R(q_L;L) - T_L), \qquad \Pi_M = pT_H + (1-p)T_L.ΠR​=p(πR​(qH​;H)−TH​)+(1−p)(πR​(qL​;L)−TL​),ΠM​=pTH​+(1−p)TL​.

Both firms discount future periods by δ\deltaδ.

In the static problem the manufacturer maximizes ΠM\Pi_MΠM​ subject to participation πR(qθ;θ)−Tθ≥0\pi_R(q_\theta;\theta) - T_\theta \ge 0πR​(qθ​;θ)−Tθ​≥0 and incentive compatibility πR(qθ;θ)−Tθ≥πR(qθ~;θ)−Tθ~\pi_R(q_\theta;\theta) - T_\theta \ge \pi_R(q_{\tilde\theta};\theta) - T_{\tilde\theta}πR​(qθ​;θ)−Tθ​≥πR​(qθ~​;θ)−Tθ~​. Its solution has qHS=VH/2q^S_H = V_H/2qHS​=VH​/2 and qLS=VL2−p1−pVH−VL2q^S_L = \frac{V_L}{2} - \frac{p}{1-p}\frac{V_H - V_L}{2}qLS​=2VL​​−1−pp​2VH​−VL​​, and the retailer's expected profit is ΠRS=pΔ(qLS)\Pi^S_R = p\Delta(q^S_L)ΠRS​=pΔ(qLS​). The paper assumes pVH<VLpV_H < V_LpVH​<VL​, so that qLS>0q^S_L > 0qLS​>0.

In the repeated game, the manufacturer offers the same menu every period and reverts to the static menu forever after a deviation. The dynamic participation constraint, common to both regimes, is

πR(qθ;θ)−Tθ+δ1−δΠR ≥ δ1−δpΔ(qLS).\pi_R(q_\theta;\theta) - T_\theta + \tfrac{\delta}{1-\delta}\Pi_R \ \ge\ \tfrac{\delta}{1-\delta}p\Delta(q^S_L).πR​(qθ​;θ)−Tθ​+1−δδ​ΠR​ ≥ 1−δδ​pΔ(qLS​).

Without sales information a misreport cannot be detected, so incentive compatibility stays static. With sales information a misreport is detected at the end of the period and punished:

πR(qθ;θ)−Tθ+δ1−δΠR ≥ πR(qθ~;θ)−Tθ~+δ1−δpΔ(qLS).\pi_R(q_\theta;\theta) - T_\theta + \tfrac{\delta}{1-\delta}\Pi_R \ \ge\ \pi_R(q_{\tilde\theta};\theta) - T_{\tilde\theta} + \tfrac{\delta}{1-\delta}p\Delta(q^S_L).πR​(qθ​;θ)−Tθ​+1−δδ​ΠR​ ≥ πR​(qθ~​;θ)−Tθ~​+1−δδ​pΔ(qLS​).

In each regime the manufacturer chooses a menu that maximizes ΠM\Pi_MΠM​ among all menus satisfying that regime's constraints. Write ΠRD,ne\Pi^{D,ne}_RΠRD,ne​ and ΠRD,e\Pi^{D,e}_RΠRD,e​ for the retailer's expected profit at the optimal menu without and with sales information.

Formalization targets

Goal: Proposition 3

For 0<p<10<p<10<p<1, VL<VHV_L<V_HVL​<VH​, pVH<VLpV_H<V_LpVH​<VL​ and 0≤δ<10\le\delta<10≤δ<1, and for every optimal menu of each program,

ΠRD,e ≥ ΠRD,ne⟺δ ≤ δ~=11+1+p.\Pi^{D,e}_R \ \ge\ \Pi^{D,ne}_R \quad\Longleftrightarrow\quad \delta \ \le\ \tilde\delta = \frac{1}{1+\sqrt{1+p}}.ΠRD,e​ ≥ ΠRD,ne​⟺δ ≤ δ~=1+1+p​1​.

Milestones

  1. The static optimal menu (4)–(5), and ΠRS=pΔ(qLS)\Pi^S_R = p\Delta(q^S_L)ΠRS​=pΔ(qLS​).
  2. Without sales information: the transfers that make the low-state participation and high-state incentive constraints bind, (27), and the reduced profit (10); the other two constraints are slack (Appendix C).
  3. Proposition 1: the unique optimal no-sharing menu (11)–(12).
  4. The retailer's no-sharing profit (15).
  5. With sales information: the binding transfers (29), the reduced profit (19), and slackness of the other constraints (Appendix C).
  6. Proposition 2: the unique optimal sharing menu (20)–(21).
  7. The retailer's sharing profit (30) and the gap (31),
ΠRD,e−ΠRD,ne=δp3(1−δ)(VH−VL)22(1−p)(1+δp)2 [1−δ(2+δp)].\Pi^{D,e}_R - \Pi^{D,ne}_R = \frac{\delta p^3(1-\delta)(V_H - V_L)^2}{2(1-p)(1+\delta p)^2}\,\big[1 - \delta(2+\delta p)\big].ΠRD,e​−ΠRD,ne​=2(1−p)(1+δp)2δp3(1−δ)(VH​−VL​)2​[1−δ(2+δp)].

Significance

Proposition 3 answers the paper's central question: sharing past sales data can arise voluntarily, and it does so exactly when the retailer is impatient enough, δ≤δ~\delta \le \tilde\deltaδ≤δ~. For patient retailers the repeated relationship already sustains a large low-demand quantity without verification, and the retailer loses more rent from detection than it gains from the higher quantity. Since the manufacturer always gains, δ≤δ~\delta \le \tilde\deltaδ≤δ~ is also the region where sharing is a Pareto improvement for the channel. The threshold depends on ppp alone, not on VHV_HVH​ or VLV_LVL​.

The results are proved in the paper by first-order conditions on the reduced profits and direct substitution. Nothing in this mission is machine-checked yet. The formalization would turn the paper's chain (binding constraints, slack constraints, reduced profit, maximizer, retailer profit, sign of the gap) into one verified argument, including the step the paper treats informally: that the relaxed program with two binding constraints has the same optimum as the full four-constraint program, and that the optimum is unique.

Difficulty

The algebra of (15), (30) and (31) is long but mechanical. The substantive step is optimality over all menus. The paper drops two of the four constraints, solves the remaining two with equality, and maximizes the resulting quadratic. A rigorous version must show that no feasible menu, at any quantities, earns more than the reduced profit, that the reduced profit has a unique maximizer, and that the two dropped constraints hold at the candidate (Appendix C). Proposition 3 itself is stated about any optimal menu, so it needs uniqueness, not only existence, before the closed forms can be substituted. The naive route of evaluating (31) at the closed-form menus proves the comparison only for those menus, not for the optimum of the program.

Formalization scope

Everything is over R\mathbb RR with the linear demand of the paper. Parameters form a structure Params with fields p, VH, VL, δ; the predicate Params.Standing collects 0<p<10<p<10<p<1, VL<VHV_L<V_HVL​<VH​, pVH<VLpV_H<V_LpVH​<VL​ (footnote 2 of the paper) and 0≤δ<10\le\delta<10≤δ<1. The bound δ<1\delta<1δ<1 is added to the paper's 0≤δ≤10\le\delta\le10≤δ≤1 because the constraints divide by 1−δ1-\delta1−δ. A menu is a structure Menu with fields qH, TH, qL, TL; every program also requires qH,qL≥0q_H, q_L \ge 0qH​,qL​≥0, a condition that does not bind at the optima. Constraints are weak inequalities as printed. "Optimal" means feasible and maximizing pTH+(1−p)TLpT_H + (1-p)T_LpTH​+(1−p)TL​ over all feasible menus (IsOptimalNE, IsOptimalE). The retailer's profit is the ex-ante per-period ΠR\Pi_RΠR​, not the discounted sum.

The goal must not be stated at the closed-form menus menuNE, menuE: that version is the algebraic identity (31) and skips the optimization entirely. Likewise the retailer's profit is defined from the menu, never by the formulas (15) or (30).

All definitions live in one file, SalesTrust.Sharing.Model. Contributions are welcome on any milestone; the two relaxation arguments (milestones 2 and 5 with Appendix C) and the uniqueness parts of Propositions 1 and 2 are where the work is. The relaxation step is common to two-type screening models, so a general statement of it would be reusable beyond this mission.

Selected references

  • N. Shamir and Y. Yehezkel, Sales Information Transparency and Trust in Repeated Vertical Relationships, Manufacturing & Service Operations Management, 2023. https://doi.org/10.1287/msom.2023.1208
  • J.-J. Laffont and D. Martimort, The Theory of Incentives: The Principal-Agent Model, Princeton University Press, 2002. https://doi.org/10.1515/9781400829453
  • Ö. Özer, Y. Zheng and K.-Y. Chen, Trust in Forecast Information Sharing, Management Science 57(6), 2011. https://doi.org/10.1287/mnsc.1110.1348
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Convex OptimizationEconomicsOptimization·Captain: mikedeng1

Discrete Choice Prox-Functions on the Simplex: The Convex Conjugate of an Additive Random Utility Surplus Function Is a Prox-Function on the SimplexResearch Paper

Motivation

Prox-functions determine how subgradient and mirror-type optimization methods turn a direction of improvement into the next feasible point. On a probability simplex, that step should respect the geometry of probability vectors and be computable from the current direction. The entropic prox-function gives the softmax rule, familiar from the logit model of discrete choice. Müller, Nesterov and Shikhman ask whether a wider family of random-utility choice models supplies prox-functions with the same operational link between optimization and choice probabilities. Their 2019 preprint, published in Mathematics of Operations Research in 2022, states that it does: the convex conjugate of the model's surplus is a prox-function on the simplex.

This question matters to optimization because the random-utility law specifies a geometry and a computable update together. It matters to discrete-choice modeling because the update from an optimization problem can be interpreted as a vector of probabilities of choosing each alternative. The mission covers the general result in Section 2 of the preprint, rather than its later specialized generalized-extreme-value parameters or economic application.

Setting

There are n≥1n\ge1n≥1 alternatives. A deterministic utility vector u∈Rnu\in\mathbb R^nu∈Rn is perturbed by a random shock vector ϵ∈Rn\epsilon\in\mathbb R^nϵ∈Rn with law μ\muμ. Assumption 1 requires a finite mean, absolute continuity with respect to Lebesgue measure, and full support in Rn\mathbb R^nRn. The surplus function is the expected best perturbed utility,

E(u)=Eμ ⁣[max⁡1≤i≤n(ui+ϵi)].E(u)=\mathbb E_\mu\!\left[\max_{1\le i\le n}\bigl(u_i+\epsilon_i\bigr)\right].E(u)=Eμ​[1≤i≤nmax​(ui​+ϵi​)].

The convex conjugate of this function is taken over every utility vector, with extended-real values:

E∗(p)=sup⁡u∈Rn{⟨p,u⟩−E(u)},⟨p,u⟩=∑ipiui.E^*(p)=\sup_{u\in\mathbb R^n}\{\langle p,u\rangle-E(u)\},\qquad \langle p,u\rangle=\sum_i p_i u_i.E∗(p)=u∈Rnsup​{⟨p,u⟩−E(u)},⟨p,u⟩=i∑​pi​ui​.

The candidate domain is the simplex Δ={p∈Rn:pi≥0, ∑ipi=1}\Delta=\{p\in\mathbb R^n:p_i\ge0,\ \sum_i p_i=1\}Δ={p∈Rn:pi​≥0, ∑i​pi​=1}. The model's choice probability Pi(u)P_i(u)Pi​(u) is the chance that ui+ϵiu_i+\epsilon_iui​+ϵi​ attains the largest perturbed utility. Absolute continuity makes ties null, so including ties in this event does not change its probability. The paper identifies Pi(u)P_i(u)Pi​(u) with the iiith derivative of EEE in equation (1).

A prox-function on Δ\DeltaΔ is continuous and strongly convex there, and the optimization step that maximizes ⟨p,u⟩−E∗(p)\langle p,u\rangle-E^*(p)⟨p,u⟩−E∗(p) over p∈Δp\in\Deltap∈Δ has a unique, directly available answer. Here strong convexity uses ∥p−q∥1=∑i∣pi−qi∣\|p-q\|_1=\sum_i|p_i-q_i|∥p−q∥1​=∑i​∣pi​−qi​∣. The relevant smoothness of EEE uses the dual norm ∥u∥∞=max⁡i∣ui∣\|u\|_\infty=\max_i|u_i|∥u∥∞​=maxi​∣ui​∣.

Formalization targets

The goal combines the three claims that form the paper's Section 2 main result. First, Theorem 1 says that the finite domain of E∗E^*E∗ is exactly Δ\DeltaΔ, and that E∗E^*E∗ is continuous even at the boundary of that simplex. Second, Theorem 2 supplies an explicit strong-convexity parameter. For distinct alternatives i,ji,ji,j, let gijg_{ij}gij​ be a density of ϵj−ϵi\epsilon_j-\epsilon_iϵj​−ϵi​ and let zˉij\bar z_{ij}zˉij​ be a mode of that density. Then

E∗(αp+(1−α)q)≤αE∗(p)+(1−α)E∗(q)−β2α(1−α)∥p−q∥12,β=12∑i∑j≠igij(zˉij)E^*(\alpha p+(1-\alpha)q)\le \alpha E^*(p)+(1-\alpha)E^*(q) -\frac{\beta}{2}\alpha(1-\alpha)\|p-q\|_1^2, \quad \beta=\frac{1}{2\sum_i\sum_{j\ne i}g_{ij}(\bar z_{ij})}E∗(αp+(1−α)q)≤αE∗(p)+(1−α)E∗(q)−2β​α(1−α)∥p−q∥12​,β=2∑i​∑j=i​gij​(zˉij​)1​

for p,q∈Δp,q\in\Deltap,q∈Δ and α∈[0,1]\alpha\in[0,1]α∈[0,1]. The double sum is over ordered pairs. Third, under the strong-convexity premise stated at the opening of §2.2.3, Theorem 4 identifies the optimizer and the attained value:

argmax⁡p∈Δ(⟨p,u⟩−E∗(p))=P(u),max⁡p∈Δ(⟨p,u⟩−E∗(p))=E(u).\underset{p\in\Delta}{\operatorname{argmax}} \bigl(\langle p,u\rangle-E^*(p)\bigr)=P(u), \qquad \max_{p\in\Delta}\bigl(\langle p,u\rangle-E^*(p)\bigr)=E(u).p∈Δargmax​(⟨p,u⟩−E∗(p))=P(u),p∈Δmax​(⟨p,u⟩−E∗(p))=E(u).

The milestones record Lemmas 1, 2, 3 and 5, equation (1), and Theorems 1, 2 and 4. They cover the paper's elementary surplus properties, the choice-probability identity, the relation between strong convexity and strong smoothness, the Hessian norm criterion, the matrix trace bound, and the three final clauses.

Significance

The result gives a family of simplex prox-functions indexed by shock laws, rather than by a single entropy formula. The optimizer in the auxiliary problem is a choice-probability vector, so a prox update has an explicit behavioral interpretation. The strong-convexity bound supplies the geometric constant used when such a function enters first-order optimization estimates. The paper's later sections derive parameters for generalized extreme-value models and apply the update to a consumption cycle; those consequences motivate the general theorem but are outside this mission's goal.

The result is proved in the cited paper; this mission asks for its Lean formalization. The current draft has compile-checked statements with proof placeholders. A complete development would add machine-checked proofs of the listed lemmas and goal, together with reusable results about conjugacy, probability laws of differences, and norms of finite matrices. No proof of this specific paper result is claimed here.

Difficulty

Continuity in the relative interior of a simplex does not by itself establish continuity at its boundary, which is part of Theorem 1. The choice-probability formula connects differentiation of an expected maximum with an event defined by inequalities; ties, measurability, and integrability must all be handled. The strong-convexity constant then depends on controlling the Hessian with the norm induced from ℓ∞\ell_\inftyℓ∞​ to ℓ1\ell_1ℓ1​, while retaining the ordered-pair sum of density values. A direct substitution of the default norm on finite coordinate functions would change the theorem because that norm is ℓ∞\ell_\inftyℓ∞​.

Formalization scope

Alternatives are Fin n with [NeZero n]; vectors are Fin n → ℝ. The law μ\muμ is a probability measure on shock vectors. Assumption 1 explicitly includes coordinate integrability, absolute continuity and full support. Its integrability clause keeps the Bochner integral defining EEE meaningful, rather than allowing the integral's default value on a nonintegrable function. The choice event includes ties, which have zero measure under Assumption 1. The conjugate is EReal valued and takes its supremum over all utility vectors; defining it by a maximum over the simplex or by an entropy formula would change the result.

The real value of E∗E^*E∗ is used only alongside its finiteness on Δ\DeltaΔ. Strong convexity uses an explicit ℓ1\ell_1ℓ1​ sum, while Mathlib's norm on Fin n → ℝ represents ℓ∞\ell_\inftyℓ∞​. Coordinate derivatives and the Hessian are formed from Fréchet derivatives. The differences ϵj−ϵi\epsilon_j-\epsilon_iϵj​−ϵi​ have fixed, nonnegative measurable density versions tied to their pushforward laws; each mode maximizes its selected version pointwise. Theorem 4 carries the positive strong-convexity premise stated in its section preamble. The paper uses twice differentiability of EEE on page 7 without deriving it from Assumption 1. This mission explicitly adds ContDiff ℝ 2 E to the Hessian-dependent result and the goal. It is a necessary disclosed strengthening of the paper's stated assumptions.

For one alternative the simplex is a point, and the displayed denominator in β\betaβ is zero. Lean evaluates the reciprocal as zero. The strong-convexity inequality is then vacuous between distinct points; the draft asserts positivity of the displayed β\betaβ only when n≥2n\ge2n≥2 and separately asserts that some positive parameter exists for every n≥1n\ge1n≥1, as Definition 1 requires. No empty set of alternatives is admitted. Contributions should keep the unrestricted conjugate, the law-dependent densities, the exact ℓ1\ell_1ℓ1​ inequality, and the paper's constants. General finite-dimensional convex duality and induced matrix-norm lemmas would be reusable beyond this model.

Selected references

  • D. Müller, Yu. Nesterov and V. Shikhman, Discrete choice prox-functions on the simplex, arXiv:1909.05591v1, 2019; published in Mathematics of Operations Research, 2022. Preprint.
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Dynamic ProgrammingEconomicsMarkov Chain+1·Captain: mikedeng1

An Analysis of “Buy X, Get One Free” Reward Programs: Without Transaction Utility, a Redemption Threshold Alone Cannot Raise the Firm's Long-Run Profit Above max{λqv, λ(v − v̄)}Research Paper

Why reward programs that give away a free unit

"Buy XXX, get one free" (BXGO) programs are among the most common loyalty schemes: coffee shops, car washes, golf courses and hotel chains hand out a free unit after a fixed number of paid purchases. A long empirical literature documents that such programs change behaviour, most visibly through point pressure, the acceleration of purchases as a customer approaches the redemption threshold (Kopalle et al. 2012; Lewis 2004). Whether that acceleration is worth the free units given away is a question for the firm's pricing and marketing operations.

Liu, Sun and Zhang (2021) study the question in a fully rational model. A forward-looking consumer facing a BXGO program solves a dynamic program, and her optimal decisions induce a Markov chain on her point inventory. The paper shows that discounting alone produces point pressure, and then asks whether the program raises the firm's long-run profit. Its answer without transaction utility (the consumer's extra enjoyment of a free unit) is negative under explicit conditions: Proposition 3. This mission formalizes that result together with the structural lemmas its proof rests on.

Setting

A monopolist sells a nondurable product at marginal cost 000, so revenue and profit coincide. A BXGO program is a pair (p,X)(p,X)(p,X): a fixed price ppp and a threshold X≥1X\ge1X≥1. A consumer earns one point per purchase, and holding XXX points she may redeem them for a free unit, returning to 000 points.

In each period the consumer is in the market with probability λ\lambdaλ. In the market she values the product at vvv and has an outside option v0v_0v0​, equal to 000 with probability qqq and to vˉ\bar vvˉ otherwise, where v≥vˉ≥0v\ge\bar v\ge0v≥vˉ≥0. A redemption gives her a transaction utility k≥0k\ge0k≥0 on top of vvv. She discounts with factor δ∈(0,1)\delta\in(0,1)δ∈(0,1).

Her value function JJJ on the point inventories x∈{0,…,X}x\in\{0,\dots,X\}x∈{0,…,X} solves the optimality equations

J(x)=λqmax⁡{v−p+δJ(x+1),δJ(x)}+λ(1−q)max⁡{v−p+δJ(x+1),vˉ+δJ(x)}+(1−λ)δJ(x)J(x)=\lambda q\max\{v-p+\delta J(x+1),\delta J(x)\}+\lambda(1-q)\max\{v-p+\delta J(x+1),\bar v+\delta J(x)\}+(1-\lambda)\delta J(x)J(x)=λqmax{v−p+δJ(x+1),δJ(x)}+λ(1−q)max{v−p+δJ(x+1),vˉ+δJ(x)}+(1−λ)δJ(x)

for x<Xx<Xx<X, and the analogous equation at XXX with v+k+δJ(0)v+k+\delta J(0)v+k+δJ(0) (redemption) in place of v−p+δJ(x+1)v-p+\delta J(x+1)v−p+δJ(x+1). She buys, or redeems, when this is at least as good as the outside option. Her decisions turn the point inventory into a Markov chain on {0,…,X}\{0,\dots,X\}{0,…,X} that moves from xxx to x+1x+1x+1 (from XXX to 000) or stays put. The firm's profit is ppp times the long-run purchase probability per period.

Two constants recur throughout:

A=λqδ1−δ+λqδ,A1=λδ1−δ+λδ.A=\frac{\lambda q\delta}{1-\delta+\lambda q\delta},\qquad A_1=\frac{\lambda\delta}{1-\delta+\lambda\delta}.A=1−δ+λqδλqδ​,A1​=1−δ+λδλδ​.

So do the boundary prices pB(τ)p^B(\tau)pB(τ) and pD(τ)p^D(\tau)pD(τ) of the paper's p. 10, which separate the price ranges of the consumer's four response patterns (Proposition 2). The benchmark is the profit of the best price without a program, max⁡{λqv, λ(v−vˉ)}\max\{\lambda qv,\ \lambda(v-\bar v)\}max{λqv, λ(v−vˉ)}: selling to the consumer only when her outside option is 000, or always, at the price v−vˉv-\bar vv−vˉ.

Formalization targets

Goal: Proposition 3

Assume k=0k=0k=0 and either (a) q≤12q\le\tfrac12q≤21​ and δ≥22+λ\delta\ge\tfrac{2}{2+\lambda}δ≥2+λ2​, or (b) q>12q>\tfrac12q>21​ and v−vˉ≤min⁡{Av, v1+A1}v-\bar v\le\min\{Av,\ \tfrac{v}{1+A_1}\}v−vˉ≤min{Av, 1+A1​v​}. Then for every program (p,X)(p,X)(p,X) and every solution JJJ of the optimality equations, the average expected revenue RˉN\bar R_NRˉN​ over the first NNN periods, of a consumer who starts with 000 points, satisfies

lim sup⁡N→∞RˉN ≤ max⁡{λqv, λ(v−vˉ)}.\limsup_{N\to\infty}\bar R_N\ \le\ \max\{\lambda qv,\ \lambda(v-\bar v)\}.N→∞limsup​RˉN​ ≤ max{λqv, λ(v−vˉ)}.

The statement covers every price, including those between the ranges of Proposition 2, where the paper asserts but does not show that the consumer drops out.

Milestones

  • Structure of the value function. Proposition 1 (JJJ increasing and convex for p≥0p\ge0p≥0), Corollaries 1–2 (purchase decisions are monotone in the point inventory), Lemmas 4–5 (redemption at the low outside option, and at the high one whenever she buys in state X−1X-1X−1).
  • The consumer's response. Proposition 2: four price ranges and the purchase and redemption rule in each. Its converse, from the proofs of Lemmas 6–9: each observed behaviour forces the price into its range.
  • Demand. Lemma 1 and the analogous case (c) computation: the stationary distribution of the induced chain and the purchase probabilities λqX/(τ+q(X−τ+1))\lambda qX/(\tau+q(X-\tau+1))λqX/(τ+q(X−τ+1)) and λqX/(X+q)\lambda qX/(X+q)λqX/(X+q).
  • Profit bounds. πa∗≤λ(v−vˉ)\pi^*_a\le\lambda(v-\bar v)πa∗​≤λ(v−vˉ) and πd∗≤λqv\pi^*_d\le\lambda qvπd∗​≤λqv; Lemmas 2 and 3, which bound the profit of the threshold cases (b) and (c); and the inequality q≤Aq\le Aq≤A under condition (a).

Significance

Proposition 3 separates two effects of a reward program. Point pressure raises the purchase probability above that of a consumer who never accelerates. Discounting forces the firm to lower its price to keep her in the program, and without transaction utility the second effect dominates. The paper's Proposition 4 shows that a small positive kkk reverses the conclusion, and its §6 shows that an expiration term reverses it too. The result therefore locates exactly where the profitability of BXGO programs comes from: transaction utility or expiration, not the threshold alone.

The result is proved on paper but not machine-checked. The paper's proof of Proposition 3 works with the closed-form profits of four behavioural cases. Formalizing it requires connecting those closed forms to the consumer's dynamic program and to the long-run behaviour of the chain her decisions induce, and that connection is part of the mission. Machine-checked proofs of Propositions 1–2 also give a reusable template for monotone threshold policies in discounted point-accumulation problems.

Difficulty

The value function has no closed form until the consumer's behaviour is known, and her behaviour is defined by the value function. The paper breaks the circularity case by case: assume a behaviour, solve the linear equations it induces, and read off the price range in which that behaviour is consistent. A formal proof has to show that the four ranges, together with the gaps between them, account for every price. At a gap price the consumer either never buys from 000 points or behaves as in a neighbouring case.

Reading profit as "price times stationary demand" also needs care. At high prices, at λ=0\lambda=0λ=0 or at q=0q=0q=0 the induced chain is reducible, and the long-run revenue from 000 points need not equal the revenue under an arbitrary stationary law. Lemmas 2 and 3 bound only the four closed forms; turning them into a bound on the Cesàro averages of the actual chain is the remaining step.

Formalization scope

All quantities are real. Params bundles (λ,q,δ,v,vˉ,k)(\lambda,q,\delta,v,\bar v,k)(λ,q,δ,v,vˉ,k), and Params.Standing is the list of standing assumptions: λ,q∈[0,1]\lambda,q\in[0,1]λ,q∈[0,1], δ∈(0,1)\delta\in(0,1)δ∈(0,1), v≥vˉ≥0v\ge\bar v\ge0v≥vˉ≥0, k≥0k\ge0k≥0. The value function is a hypothesis, IsValueFn P p X J, meaning that J : ℕ → ℝ satisfies the optimality equations on {0,…,X}\{0,\dots,X\}{0,…,X}. The equations have exactly one solution there, and its values beyond XXX play no role. Decisions break ties in favour of buying or redeeming, as in the paper's Corollary 1 and Proposition 2. The chain lives on Fin (X+1). Profit is the Cesàro average avgRevenue of expected revenues from state 000, computed from the transition matrix of the consumer's own decisions. Stationary distributions use the published MarkovChain.IsStationary.

The goal cannot be made true by construction. Profit is computed from the decisions of JJJ, never from the paper's closed forms, and the goal quantifies over every price and every threshold with no assumed behaviour.

Hypotheses added to the paper's statements:

  • p≥0p\ge0p≥0 on Proposition 1 and Corollary 2. Both fail for negative prices.
  • λ>0\lambda>0λ>0, q>0q>0q>0 on Proposition 2 and its converse. There the boundary prices divide by quantities that vanish when A=0A=0A=0.
  • Pointwise statements. Lemmas 2–3 and the case (a)/(d) bounds are stated at every feasible price, because πb∗\pi^*_bπb∗​ and the other optimal profits are suprema over possibly empty sets.
  • Uniqueness only for λ,q>0\lambda,q>0λ,q>0. The stationary laws of Lemma 1 and case (c) are asserted unique only in that range, since at λ=0\lambda=0λ=0 or q=0q=0q=0 other stationary laws exist.

Proofs of individual milestones are welcome. So are general lemmas about Cesàro averages of finite stochastic matrices and the two-sided comparison of discounted value functions, both of which are reusable beyond this mission.

Selected references

  • Y. Liu, Y. Sun, D. Zhang, An Analysis of "Buy X, Get One Free" Reward Programs, Operations Research 69(6):1823–1841, 2021 (cited from the accepted manuscript of March 26, 2021). https://doi.org/10.1287/opre.2021.2128
  • P. K. Kopalle, Y. Sun, S. A. Neslin, B. Sun, V. Swaminathan, The joint sales impact of frequency reward and customer tier components of loyalty programs, Marketing Science 31(2):216–235, 2012. https://doi.org/10.1287/mksc.1110.0687
  • M. Lewis, The influence of loyalty programs and short-term promotions on customer retention, Journal of Marketing Research 41(3):281–292, 2004. https://doi.org/10.1509/jmkr.41.3.281.35986
  • Y. Sun, D. Zhang, A model of customer reward programs with finite expiration terms, Management Science 65(8):3889–3903, 2019. https://doi.org/10.1287/mnsc.2018.3115
  • M. L. Puterman, Markov Decision Processes: Discrete Stochastic Dynamic Programming, Wiley, 1994. https://doi.org/10.1002/9780470316887
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EconomicsMechanism DesignOperations Research·Captain: mikedeng1

Simple and Approximately Optimal Contracts for Payment for Ecosystem Services: A Linear Contract with Per-Unit Price k/2 Achieves at Least Half of the Optimal Contract PayoffResearch Paper

Motivation

Payments for ecosystem services compensate landowners for conservation that a program values but cannot directly provide. A contract designer must decide how to pay when landowners differ in the amount of forest they would conserve without a payment. That baseline conservation type is privately known, so a contract can pay for forest that would have remained anyway. Li, Ashlagi and Lo study this problem for forest conservation and ask how much payoff a simple, uniform price can guarantee relative to an optimally tailored contract (Li, Ashlagi and Lo, 2022, §§1–2).

The paper's Theorem 1 establishes a guarantee that does not depend on the type distribution: a price equal to half the program's value per unit secures at least half of the optimal contract payoff. This matters to a designer who can estimate the conservation value but cannot reliably estimate the distribution of landowners' private baselines. The guarantee concerns the principal's payoff after payments, rather than the total area conserved or the agent's utility (Li, Ashlagi and Lo, 2022, §4, Theorem 1).

Setting

An agent owns an initial forest area a0>0a_0>0a0​>0. Their type θ\thetaθ is the fraction of that area they would conserve without incentives. The publicly known type distribution μ\muμ is supported on [θ‾,θˉ]⊆[0,1][\underline\theta,\bar\theta]\subseteq[0,1][θ​,θˉ]⊆[0,1]. The agent selects a conserved area a∈[0,a0]a\in[0,a_0]a∈[0,a0​]. Conservation above the baseline θa0\theta a_0θa0​ has cost ch(a−θa0)c_h(a-\theta a_0)ch​(a−θa0​), where h>0h>0h>0 and

ch(x)={(h/2)x2,x≥0,0,x<0.c_h(x)=\begin{cases}(h/2)x^2,&x\geq0,\\0,&x<0.\end{cases}ch​(x)={(h/2)x2,0,​x≥0,x<0.​

The principal values each conserved unit at k>0k>0k>0. A direct revelation contract specifies an action a(θ)a(\theta)a(θ) and payment P(θ)P(\theta)P(θ) for each reported type. It is feasible when the action respects the forest-area bounds, payments are nonnegative, truthful participation gives nonnegative utility (individual rationality, IR), and truthfully reporting the type maximizes utility among all reports in the type interval (incentive compatibility, IC). Its payoff is Eμ[ka(θ)−P(θ)]\mathbb E_\mu[k a(\theta)-P(\theta)]Eμ​[ka(θ)−P(θ)]. These are the model and contract constraints on pages 4–5 of the source preprint.

A linear contract pays the same price p≥0p\geq0p≥0 for every unit of conserved area, including area the agent would conserve without incentives. The agent's action at price ppp is aL(θ;p)=min⁡{θa0+p/h,a0}a_L(\theta;p)=\min\{\theta a_0+p/h,a_0\}aL​(θ;p)=min{θa0​+p/h,a0​} on the type interval. The principal then receives Obj⁡L(p)=(k−p)Eμ[aL(θ;p)]\operatorname{Obj}^L(p)=(k-p)\mathbb E_\mu[a_L(\theta;p)]ObjL(p)=(k−p)Eμ​[aL​(θ;p)]; the best such payoff is Obj⁡L∗=sup⁡p≥0Obj⁡L(p)\operatorname{Obj}^{L*}=\sup_{p\geq0}\operatorname{Obj}^L(p)ObjL∗=supp≥0​ObjL(p). The price and payment apply to the whole action aaa, as in Equation (3) of the source preprint.

Formalization targets

Distribution-free half guarantee

For every probability law μ\muμ on the stated type interval, every feasible direct contract (a,P)(a,P)(a,P) with a defined expected payoff, and every best-response action aLa_LaL​ to the price k/2k/2k/2, Theorem 1 gives

Eμ[ka(θ)−P(θ)]≤2Eμ[(k−k/2)aL(θ)].\mathbb E_\mu[k a(\theta)-P(\theta)] \leq 2\mathbb E_\mu[(k-k/2)a_L(\theta)].Eμ​[ka(θ)−P(θ)]≤2Eμ​[(k−k/2)aL​(θ)].

It follows that every feasible direct-contract payoff is at most 2Obj⁡L∗2\operatorname{Obj}^{L*}2ObjL∗. The universal bound expresses the comparison with an optimal contract even if a maximum over contracts is not attained. The milestone list contains the linear best response, the doubled payoff identity of Equation (7), the information-rent-free upper bound of Equations (4)–(5), and the pointwise comparison from Appendix A.4. All four come from the paper's §4 and Appendix A.4.

Significance

The guarantee makes the price k/2k/2k/2 a distribution-independent benchmark for this conservation model. The paper's Example 3 gives a single type at θ=0\theta=0θ=0 where the factor of two is attained, so a larger universal fraction cannot be claimed under the same assumptions (Li, Ashlagi and Lo, 2022, p. 9). The result also implies the best linear contract has the same worst-case guarantee, even though finding its maximizing price may depend on the distribution.

The result is proved in the paper but is not yet machine checked in this mission. Formalizing it will give a reusable definition of this conservation-contract model, with explicit IR and IC constraints, and Lean statements for the price guarantee and its central comparisons. It can also support later formalizations of the paper's conditional contracts and convex-cost extensions, which are outside this mission.

Difficulty

The benchmark is the payoff of an optimally designed contract with actual payments, under private information. Replacing those payments by conservation cost changes the benchmark: the agent may receive an information rent. Likewise, optimizing ka−ch(a−θa0)k a-c_h(a-\theta a_0)ka−ch​(a−θa0​) independently for each type describes an unconstrained surplus, not the direct contract in Theorem 1. A formal statement that uses either quantity as the goal's “optimal payoff” would miss the paper's claim. The paper compares the linear payoff with a bound on the contract payoff, and its Appendix treats type distributions that need not satisfy the monotone-hazard-rate condition used in the shorter proof sketch (Li, Ashlagi and Lo, 2022, pp. 10, 24–26).

Formalization scope

Lean represents types, areas, prices and payoffs as real numbers. The law μ\muμ is any probability measure on the reals concentrated on [θ‾,θˉ][\underline\theta,\bar\theta][θ​,θˉ]; atoms, including a point mass, are allowed. The standing parameter conditions are a0>0a_0>0a0​>0, h>0h>0h>0 and 0≤θ‾≤θˉ≤10\leq\underline\theta\leq\bar\theta\leq10≤θ​≤θˉ≤1. Positive a0a_0a0​ is made explicit because the paper uses 1−p/(ha0)1-p/(ha_0)1−p/(ha0​). The theorem adds k>0k>0k>0 as stated in Theorem 1. Feasibility and best-response conditions range over supported types, and IC compares every pair of types in that interval. The contract's action and payment are integrable so their expected payoff is defined. The bounded best-response action needs no separate integrability assumption.

The formalization uses a supremum over nonnegative linear prices. Under the standing conditions its values are bounded above, so this is the ordinary best-payoff bound rather than a default value of a total supremum operation. The goal ranges over feasible direct contracts with IR, IC, action bounds and nonnegative payments; it retains the actual P(θ)P(\theta)P(θ) in the payoff. A goal stated only for an unconstrained surplus or with an empty feasible class would not represent Theorem 1. Useful contributions include proofs of the four milestones, measure-theoretic facts about supported type laws, and lemmas about the price-payoff supremum.

Selected references

  • Wanyi Li, Itai Ashlagi and Iris Lo, Simple and Approximately Optimal Contracts for Payment for Ecosystem Services, Management Science, 2022. Formalization uses the SSRN preprint dated 2021-05-19: SSRN 3754041.
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Machine LearningOptimizationProbability+1·Captain: mikedeng1

Hidden Integrality and Semirandom Robustness of SDP Relaxation for Sub-Gaussian Mixture Model: The SDP Clustering Error Is at Most Twice the Oracle Integer Program ErrorResearch Paper

Why compare a clustering SDP with an oracle?

Clustering methods must infer a partition from noisy observations, while the quality of a partition is usually judged against labels that the method cannot see. Fei and Chen study a balanced sub-Gaussian mixture model in which a semidefinite program (SDP) estimates a cluster matrix from pairwise distances. Their Theorem 1 relates its error to a simpler integer program allowed to know the true cluster centers. This comparison makes the SDP's error interpretable through an explicit benchmark, even when exact recovery is unavailable. The paper also investigates semi-random perturbations, but this mission targets the Model 1 comparison on which that broader discussion builds.

The tension is that an SDP solution may be fractional. Its entries express pairwise affinities, whereas an assignment matrix places each point in exactly one cluster. The result bounds the fractional matrix's entrywise error by an integer assignment error without assuming that the SDP solution itself is integral. That is the hidden-integrality claim relevant to this mission.

The model and the two optimization problems

There are n≥4n\ge4n≥4 observations in Rd\mathbb R^dRd and k≥2k\ge2k≥2 clusters. The true label of point iii is σ∗(i)∈[k]\sigma^*(i)\in[k]σ∗(i)∈[k], and every cluster contains exactly ℓ=n/k\ell=n/kℓ=n/k points. For unknown centers μ1,…,μk\mu_1,\ldots,\mu_kμ1​,…,μk​, the observations have the form

hi=μσ∗(i)+gi.h_i=\mu_{\sigma^*(i)}+g_i.hi​=μσ∗(i)​+gi​.

The noise vectors gig_igi​ are independent, measurable, zero-mean, and sub-Gaussian. Their vector sub-Gaussian norms are at most τ>0\tau>0τ>0. The minimum center separation and signal-to-noise ratio are

Δ=min⁡a≠b∥μa−μb∥2,s=Δ/τ.\Delta=\min_{a\ne b}\|\mu_a-\mu_b\|_2,\qquad s=\Delta/\tau.Δ=a=bmin​∥μa​−μb​∥2​,s=Δ/τ.

The SDP uses the squared-distance matrix Aij=∥hi−hj∥22A_{ij}=\|h_i-h_j\|_2^2Aij​=∥hi​−hj​∥22​. It minimizes ⟨Y,A⟩=∑i,jYijAij\langle Y,A\rangle=\sum_{i,j}Y_{ij}A_{ij}⟨Y,A⟩=∑i,j​Yij​Aij​ over real n×nn\times nn×n matrices with row sums n/kn/kn/k, diagonal entries one, nonnegative entries, and symmetric positive semidefiniteness. Write Y^\widehat YY for any optimum. The true cluster matrix is Yij∗=1Y^*_{ij}=1Yij∗​=1 when σ∗(i)=σ∗(j)\sigma^*(i)=\sigma^*(j)σ∗(i)=σ∗(j) and 000 otherwise. Its error is measured by the entrywise norm ∥Y^−Y∗∥1=∑i,j∣Y^ij−Yij∗∣\|\widehat Y-Y^*\|_1=\sum_{i,j}|\widehat Y_{ij}-Y^*_{ij}|∥Y−Y∗∥1​=∑i,j​∣Yij​−Yij∗​∣.

The benchmark is an Oracle Integer Program. An assignment matrix F∈FF\in\mathcal FF∈F has zero-one entries and exactly one one in each row. The true assignment is Fja∗=1{σ∗(j)=a}F^*_{ja}=\mathbf1\{\sigma^*(j)=a\}Fja∗​=1{σ∗(j)=a}. The oracle sees the centers and augmented observations hˉj=μσ∗(j)+(2κ)−1gj\bar h_j=\mu_{\sigma^*(j)}+(2\kappa)^{-1}g_jhˉj​=μσ∗(j)​+(2κ)−1gj​ with the fixed κ=1/8\kappa=1/8κ=1/8, so its noise is four times the realized noise in hjh_jhj​. It minimizes

η(F)=∑j,a∥hˉj−μa∥22Fja.\eta(F)=\sum_{j,a}\|\bar h_j-\mu_a\|_2^2F_{ja}.η(F)=j,a∑​∥hˉj​−μa​∥22​Fja​.

The Oracle error is the largest 12∥F−F∗∥1\tfrac12\|F-F^*\|_121​∥F−F∗∥1​ among assignments satisfying η(F)≤η(F∗)\eta(F)\le\eta(F^*)η(F)≤η(F∗). The Oracle feasible set has no balance constraint. In contrast, the SDP retains the row-sum constraint inherited from balanced clustering.

Formalization targets

Main goal: Theorem 1

The goal is the paper's quantitative comparison. It asserts that universal constants Cs>0C_s>0Cs​>0 and C≥1C\ge1C≥1 exist such that, when

s2≥Cs(kdnlog⁡n+kdn+k),s^2\ge C_s\left(\sqrt{\frac{kd}{n}\log n}+\frac{kd}{n}+k\right),s2≥Cs​(nkd​logn​+nkd​+k),

an event of probability at least 1−n−C−2e−n1-n^{-C}-2e^{-n}1−n−C−2e−n has, for every realized SDP optimum Y^\widehat YY, the bound

∥Y^−Y∗∥1∥Y∗∥1≤2max⁡F∈Fη(F)≤η(F∗)∥F−F∗∥1∥F∗∥1.\frac{\|\widehat Y-Y^*\|_1}{\|Y^*\|_1} \le 2\max_{\substack{F\in\mathcal F\\\eta(F)\le\eta(F^*)}} \frac{\|F-F^*\|_1}{\|F^*\|_1}.∥Y∗∥1​∥Y−Y∗∥1​​≤2F∈Fη(F)≤η(F∗)​max​∥F∗∥1​∥F−F∗∥1​​.

The constants are independent of n,k,dn,k,dn,k,d, the centers, the labels, and the noise law. The event and the SDP optimum are chosen after the random observations are realized. The theorem fixes the factor two and the failure-probability expression exactly as printed.

Milestone results

The eight milestones follow the statements in Section 5: the six structural properties of the SDP error matrix (Fact 2), the basic inequality (16), the signal estimate (Proposition 3), the two noise estimates (Propositions 1 and 2), the representation of the remaining term (Lemma 1), the identity between the integer program and Oracle error (Lemma 2), and the final deterministic bound. Each milestone keeps the paper's constants and its own hypotheses. Together they expose the interfaces needed to close Theorem 1.

What the comparison gives

Theorem 1 transfers a question about a real matrix optimum to a finite assignment benchmark. The Oracle benchmark can itself be bounded under additional assumptions, as Fei and Chen do in their separate Theorem 2. The present target preserves the comparison even in regimes where the benchmark does not vanish. It therefore expresses an error guarantee rather than an exact-recovery assertion.

A complete Lean proof would connect a probability model, finite-dimensional semidefinite feasibility, and the paper's integer assignment comparison. At present these mission statements are draft proof obligations: compiling a statement with sorry checks its formulation but does not prove the result. The development reuses published definitions of scalar and vector sub-Gaussian norms; proving the new lemmas and the main theorem remains open within this mission.

Where the difficulty lies

SDP optimality gives an inequality for the squared-distance objective, but it does not directly bound the entrywise difference from Y∗Y^*Y∗. Noise enters that objective through both a Gram matrix and mixed center-noise terms. A direct entrywise comparison also ignores the row-sum and positive-semidefinite structure that constrains the SDP error.

On the benchmark side, replacing a fractional matrix error by an arbitrary rounded assignment would not retain the stated factor. The paper identifies an intermediate linear program whose value can be controlled at integer cardinalities. Formalizing the result requires preserving that cardinality constraint, the exact coefficient κ=1/8\kappa=1/8κ=1/8, and the distinction between the observed points and the oracle's augmented points.

Formalization scope

Points, clusters, and coordinates use finite index types; Lean indices start at zero while the paper's [n][n][n] and [k][k][k] start at one. All matrices are real. The trace inner product is represented by a double sum, the matrix ℓ1\ell_1ℓ1​ norm is entrywise, and the spectral norm in Proposition 2 uses the L2L^2L2 operator norm. The minimum separation ranges over distinct center pairs, which is nonempty when k≥2k\ge2k≥2. Oracle maxima are finite, nonempty, bounded sets; the true assignment is a feasible candidate. The normalized denominators are nonzero under n≥4n\ge4n≥4 and k≥2k\ge2k≥2 with balanced labels.

The random model uses one probability space and the same noise realization in both hhh and hˉ\bar hhˉ. Measurability, zero mean, independence, and the extended-nonnegative vector sub-Gaussian norm bound are explicit. High-probability conclusions use measurable events and quantify over every optimum at each realized data set. Deterministic milestones take a fixed realization and do not add a probability space. The universal constants occur before all model parameters. These choices rule out a vacuous instance-dependent SNR constant, a norm that assigns zero to heavy-tailed noise, and an SDP optimum chosen before observing the noise.

The scope is Theorem 1 and its selected Section 5 statements. Theorem 2's separate Oracle-error rate, the rounding algorithm, semi-random Model 2, and the stochastic-ball special case are outside this proposal. Reusable work includes the SDP and assignment interfaces, matrix-error identities, and finite integer-program comparisons. Contributions that prove the eight source milestones or establish their supporting concentration and finite-dimensional optimization results are welcome.

Selected references

  • Y. Fei and Y. Chen, Hidden Integrality and Semi-Random Robustness of SDP Relaxation for Sub-Gaussian Mixture Model, Mathematics of Operations Research, 2022. arXiv:1803.06510v2, the version and pagination used here.
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CombinatoricsEconomicsLinear Optimization·Captain: mikedeng1

Every Choice Function Is Pro-Con Rationalizable: Disjoint Sets of Pro- and Con-Orderings Under Which Each Choice Set's Chosen Alternative Is the One with More Pros Than ConsResearch Paper

Motivation

Revealed-preference theory asks which observed choices can be explained by a decision procedure. The classical answer, maximization of a single preference, explains only choice functions that satisfy consistency conditions such as the weak axiom, and observed choices, including the menu effects in Luce and Raiffa's dinner example, often violate them. A large literature therefore studies richer procedures and characterizes the behaviour each one can generate.

The pro-con model of Dogan and Yildiz formalizes Benjamin Franklin's "prudential algebra": an agent lists reasons for and against each alternative and chooses the one whose reasons for outnumber its reasons against. Each reason is an ordering of the alternatives, and an ordering counts as a reason for (or against) an alternative at a menu when it ranks that alternative first among those available. The paper's main result is that this model is universal for deterministic choice: every choice function is pro-con rationalizable. The paper also proves the random-choice analogue (every random choice function is pro-con rational with signed weights in [−1,1][-1,1][−1,1]), derives that every choice function is plurality-rationalizable, and recovers McGarvey's theorem on majority relations as a corollary.

Setting

Let XXX be a finite set of nnn alternatives. A choice set is a nonempty S⊆XS \subseteq XS⊆X, and a choice function CCC assigns to every choice set an element C(S)∈SC(S) \in SC(S)∈S. An ordering is a strict linear order ≻\succ≻ of XXX; max⁡(S,≻)\max(S, \succ)max(S,≻) is the ≻\succ≻-top-ranked alternative of SSS.

A pro-con model ⟨≻,⊳⟩\langle \succ, \rhd\rangle⟨≻,⊳⟩ consists of two sets of orderings, the pro-orderings ≻={≻1,…,≻m}\succ = \{\succ_1, \dots, \succ_m\}≻={≻1​,…,≻m​} and the con-orderings ⊳={⊳1,…,⊳q}\rhd = \{\rhd_1, \dots, \rhd_q\}⊳={⊳1​,…,⊳q​}, with no ordering in both. For x∈Sx \in Sx∈S,

Pros(x,S)={≻i∈≻:x=max⁡(S,≻i)},Cons(x,S)={⊳i∈⊳:x=max⁡(S,⊳i)}.\mathrm{Pros}(x, S) = \{\succ_i \in \succ : x = \max(S, \succ_i)\}, \qquad \mathrm{Cons}(x, S) = \{\rhd_i \in \rhd : x = \max(S, \rhd_i)\}.Pros(x,S)={≻i​∈≻:x=max(S,≻i​)},Cons(x,S)={⊳i​∈⊳:x=max(S,⊳i​)}.

CCC is pro-con rational (Definition 1) if one pro-con model serves every choice set: for every SSS and every x∈Sx \in Sx∈S, C(S)=xC(S) = xC(S)=x if and only if ∣Pros(x,S)∣>∣Cons(x,S)∣|\mathrm{Pros}(x, S)| > |\mathrm{Cons}(x, S)|∣Pros(x,S)∣>∣Cons(x,S)∣.

The proof works with signed weights on classes of orderings. For 1≤k≤n1 \le k \le n1≤k≤n, a kkk-prefix [≻k][\succ^k][≻k] is the list of the first kkk alternatives of an ordering, and Ωk\Omega_kΩk​ is the family of sets with more than n−kn - kn−k elements. A weight function λk\lambda_kλk​ on kkk-prefixes represents a random choice function ppp on Ωk\Omega_kΩk​ if p(x,S)p(x, S)p(x,S) is the total weight of the prefixes along which xxx is the first element of SSS. The Möbius transform of ppp is q(a,S)=∑S⊆T⊆X(−1)∣T∣−∣S∣p(a,T)q(a, S) = \sum_{S \subseteq T \subseteq X} (-1)^{|T|-|S|} p(a, T)q(a,S)=∑S⊆T⊆X​(−1)∣T∣−∣S∣p(a,T), extended by q(a,S)=q(a,S∪{a})q(a, S) = q(a, S \cup \{a\})q(a,S)=q(a,S∪{a}) for a∉Sa \notin Sa∈/S.

Formalization targets

Goal: Theorem 1

for every choice function C on a finite set X:C is pro-con rational.\text{for every choice function } C \text{ on a finite set } X:\quad C \text{ is pro-con rational.}for every choice function C on a finite set X:C is pro-con rational.

Milestones

The milestones follow the paper's proof, which runs the inductive construction of Section 6 and makes each step integral in Section 7:

  1. Lemma 2 (Möbius inversion over supersets) and Lemma 3: ∑a∈X∣q(a,S)∣≤2k\sum_{a \in X} |q(a, S)| \le 2^k∑a∈X​∣q(a,S)∣≤2k when ∣S∣=n−k|S| = n - k∣S∣=n−k.
  2. Theorem 4 (Ford–Fulkerson criterion), Lemma 1, and Theorem 3, the generalized Ford–Fulkerson theorem: for real ri∈[−1,1]r_i \in [-1, 1]ri​∈[−1,1], cj∈[−m,m]c_j \in [-m, m]cj​∈[−m,m] with equal sums and 2m≥∑∣ri∣+∑∣cj∣2m \ge \sum|r_i| + \sum |c_j|2m≥∑∣ri​∣+∑∣cj​∣, a matrix with entries in [−1,1][-1,1][−1,1], these margins, and column bound ∑i∣aij∣≤∣cj∣+max⁡{0,(∑∣ri∣−∑∣cj∣)/n}\sum_i |a_{ij}| \le |c_j| + \max\{0, (\sum|r_i| - \sum|c_j|)/n\}∑i​∣aij​∣≤∣cj​∣+max{0,(∑∣ri​∣−∑∣cj​∣)/n}.
  3. Steps 1–3 of the proof of Theorem 2: the system (RS)–(CS) gives the representation (15); its row and column totals agree (25); and the bound (29) ∑i∣λk([≻ik])∣+∑j∣q(xj,S)∣≤2 k!\sum_i |\lambda_k([\succ^k_i])| + \sum_j |q(x_j, S)| \le 2\,k!∑i​∣λk​([≻ik​])∣+∑j​∣q(xj​,S)∣≤2k!.
  4. Lemma 5 (Heller–Tompkins), total unimodularity of the (RS)–(CS) matrix, and Lemma 4 (Hoffman–Kruskal, corrected).
  5. The integral induction step of Section 7.
  6. Remark 1, the strongest form: a model with ∣Pros(x,S)∣−∣Cons(x,S)∣=1|\mathrm{Pros}(x, S)| - |\mathrm{Cons}(x, S)| = 1∣Pros(x,S)∣−∣Cons(x,S)∣=1 at the chosen alternative and 000 at every other alternative of SSS.

Significance

Theorem 1 says that pro-con rationality imposes no testable restriction on deterministic choice: no data set of single-valued choices can refute it. A characterization of a choice procedure is therefore informative only once the model is restricted further (fewer orderings, structured orderings), and the representation of Theorem 1 serves as a starting point for building other universal models, such as the plurality representation of Section 2.4. The paper shows that universality is delicate: it fails for multi-valued choice rules when each ordering may be used only once (Section 2.3).

The result is proved in the paper; nothing in this mission is open mathematics. No part of it has a machine-checked proof. The formal work is to verify the proof. That covers its combinatorial core (Möbius inversion, the 2k2^k2k estimate, the generalized Ford–Fulkerson theorem), the integrality step, and the corrections the formalization needed: Lemma 4 requires an integral right-hand side; the paper's description of the con-orderings in the random case (inverses of negative-weight orderings, p. 16) is not what the deterministic assembly uses; and the induction of Section 7 uses a bound for the previous step that the paper establishes only for the real-valued construction.

Difficulty

The obvious approach, assigning pro- and con-orderings menu by menu, fails because every ordering affects every menu at once: changing one ordering changes the top element of all sets. The paper therefore builds a signed measure on orderings level by level, prefix length k=1,…,nk = 1, \dots, nk=1,…,n, and each level must solve a transportation problem with signed margins and box constraints [−1,1][-1, 1][−1,1]. Classical Ford–Fulkerson theory covers nonnegative margins only. Moreover, a solution at one level has to leave the next level feasible, which is the role of the column bound in Theorem 3 and the source of the integrality gap noted above. The integrality itself rests on total unimodularity, which neither Mathlib nor the platform currently provides as a usable criterion (Heller–Tompkins) or vertex theorem (Hoffman–Kruskal).

Formalization scope

The alternative set is a type X with [Fintype X] [DecidableEq X]; it may be empty, in which case every statement holds trivially. An ordering is a rank bijection X ≃ Fin (Fintype.card X), rank 000 being the best, and x=max⁡(S,σ)x = \max(S, \sigma)x=max(S,σ) means x∈Sx \in Sx∈S and σ(x)≤σ(y)\sigma(x) \le \sigma(y)σ(x)≤σ(y) for all y∈Sy \in Sy∈S. A pro-con model is a structure with two Finsets of rank bijections and a disjointness proof. A choice function is C : Finset X → X with C S ∈ S for nonempty S; its value at ∅\emptyset∅ is irrelevant. ProConRational C includes this choice-function condition. Random choice functions are real-valued p : X → Finset X → ℝ, kkk-prefixes are injections Fin k ↪ X, and weight functions are maps from prefixes to ℝ (to ℤ in the integral step). Representation on Ωk\Omega_kΩk​ is stated with n < |S| + k to avoid natural-number subtraction. Matrices are Matrix (Fin m) (Fin n) ℝ or indexed by finite types; total unimodularity is Mathlib's Matrix.IsTotallyUnimodular, and vertices are Set.extremePoints ℝ.

The definition rules out each trivializing reading: orderings cannot be repeated (sets, not lists), cannot be both pro and con, are linear orders (unique top), count as cons at their top element, require a strict majority, and one model must serve all choice sets with the equivalence holding at every x∈Sx \in Sx∈S. A formalization that drops any of these makes Theorem 1 easier or false in a different way and is not this mission's goal.

Theorem 2 (random choice) is not a target; its proof steps appear as milestones. Reusable beyond this mission: the Möbius transform and its bound, the generalized Ford–Fulkerson theorem, Heller–Tompkins, and Hoffman–Kruskal for box-constrained systems. Proofs of any milestone, alternative proofs of Theorem 1 (for instance, a direct induction avoiding the gap in Section 7), and Lean infrastructure for total unimodularity are welcome.

Selected references

  • Dogan, S. and Yildiz, K., Every choice function is pro-con rationalizable, SSRN 3085542, version of January 10, 2021; published in Operations Research, 2022. https://ssrn.com/abstract=3085542, https://doi.org/10.1287/opre.2022.2312
  • Ford, L. R. Jr. and Fulkerson, D. R., Flows in Networks, Princeton University Press, 1962 (reissued 2015).
  • Heller, I. and Tompkins, C. B., An extension of a theorem of Dantzig's, in Linear Inequalities and Related Systems, Annals of Mathematics Studies 38, Princeton University Press, 1956.
  • Hoffman, A. J. and Kruskal, J. B., Integral boundary points of convex polyhedra, in 50 Years of Integer Programming 1958–2008, Springer, 2010. https://doi.org/10.1007/978-3-540-68279-0_3
  • McGarvey, D. C., A theorem on the construction of voting paradoxes, Econometrica 21(4), 1953. https://doi.org/10.2307/1907925
  • Stanley, R. P., Enumerative Combinatorics, Volume 1, Cambridge University Press, 1997, Section 3.7 (Möbius inversion).
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Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

On the SRPT Scheduling Discipline in Many-Server Queues with Impatient Customers: In the Overloaded Many-Server Limit, SRPT Serves Short Jobs Without Waiting While Long Jobs AbandonResearch Paper

Why SRPT in many-server queues with abandonment

Shortest remaining processing time first (SRPT) is the scheduling rule that always works on the jobs closest to completion. For a single server it minimizes the number of jobs in the system at every time, on every sample path (Schrage 1968). Service systems with many parallel servers and customers who leave when they wait too long, such as call centers, hospital wards and cloud platforms, are a different setting. There an overloaded system must turn customers away somehow, and the scheduling rule decides who. How SRPT behaves in such systems had resisted analysis: the state of the queue is a vector of remaining service and patience times of unbounded dimension, and preemptions couple all customers together.

Dong and Ibrahim (2021) analyze SRPT in the M/GI/s+GIM/GI/s+GIM/GI/s+GI queue in the overloaded many-server regime. They show that SRPT asymptotically behaves like a two-class priority system with a sharp threshold τ\tauτ on the service time. Short jobs are served with vanishing delay, long jobs almost all abandon, and the resulting waiting-time measures depend on the patience distribution only through its mean. Under first-come-first-served, by contrast, performance depends on the whole patience distribution (Whitt 2006).

Setting

Customers arrive according to a Poisson process of rate λ\lambdaλ to sss identical servers. Customer nnn brings a service time SnS_nSn​ and a patience time TnT_nTn​. The SnS_nSn​ are i.i.d. with a continuous law νS\nu_SνS​, density ggg, cdf GGG and mean 1/μ1/\mu1/μ; the TnT_nTn​ are i.i.d. with a continuous law νT\nu_TνT​ and mean 1/θ1/\theta1/θ. Arrivals, services and patience times are mutually independent.

A schedule says which customers occupy the servers at each time. From it one reads off each customer's remaining processing time Rn(t)R_n(t)Rn​(t) and cumulative time in queue Qn(t)Q_n(t)Qn​(t). Customer nnn abandons when Qn(t)Q_n(t)Qn​(t) reaches TnT_nTn​. Her patience clock keeps running across preemptions and is not reset. Under SRPT, at every time the servers are busy whenever customers are waiting, and every customer in service has remaining work no larger than that of any waiting customer. Customer nnn is served (Serv\mathrm{Serv}Serv) if she completes service and abandons (Ab\mathrm{Ab}Ab) otherwise. Her waiting time WnW_nWn​ is the total time she is present but not in service.

The traffic intensity is ρ=λ/(sμ)\rho = \lambda/(s\mu)ρ=λ/(sμ). The paper fixes ρ>1\rho > 1ρ>1 and lets λ\lambdaλ and sss grow together, with s=λ/(ρμ)s = \lambda/(\rho\mu)s=λ/(ρμ). The threshold τ\tauτ is defined by equation (1),

λ E[S 1(S≤τ)]=s,equivalentlyE[S 1(S≤τ)]=1ρμ,\lambda\,\mathbb E[S\,\mathbf 1(S \le \tau)] = s, \qquad\text{equivalently}\qquad \mathbb E[S\,\mathbf 1(S\le\tau)] = \frac{1}{\rho\mu},λE[S1(S≤τ)]=s,equivalentlyE[S1(S≤τ)]=ρμ1​,

so the work brought by jobs shorter than τ\tauτ exactly matches capacity. Class 1 consists of the customers with S≤τS \le \tauS≤τ and class 2 of those with S>τS > \tauS>τ.

The analysis couples the SRPT queue with a loss system LLL. This system has the same customers and sss servers but no waiting room. Class 1 customers preempt class 2 customers, and a class 1 customer who finds all servers busy with class 1 work is lost. Its class 1 throughput is ThL,1\mathrm{Th}_{L,1}ThL,1​.

Formalization targets

Goal: Theorem 2 (p. 10)

As s→∞s \to \inftys→∞, under SRPT and for a tagged customer ccc in steady state:

(a)P(Servc∣Sc≤τ)→1,P(Servc∣Sc>τ)→0;\text{(a)}\quad P(\mathrm{Serv}_c \mid S_c\le\tau)\to 1,\qquad P(\mathrm{Serv}_c\mid S_c>\tau)\to 0;(a)P(Servc​∣Sc​≤τ)→1,P(Servc​∣Sc​>τ)→0; (b)E[Wc∣Servc]→0,E[Wc∣Sc≤τ]→0;\text{(b)}\quad \mathbb E[W_c\mid\mathrm{Serv}_c]\to 0,\qquad \mathbb E[W_c\mid S_c\le\tau]\to 0;(b)E[Wc​∣Servc​]→0,E[Wc​∣Sc​≤τ]→0; (c)E[Wc∣Abc]→1/θ,E[Wc∣Sc>τ]→1/θ;\text{(c)}\quad \mathbb E[W_c\mid\mathrm{Ab}_c]\to 1/\theta,\qquad \mathbb E[W_c\mid S_c>\tau]\to 1/\theta;(c)E[Wc​∣Abc​]→1/θ,E[Wc​∣Sc​>τ]→1/θ; (d)E[Wc]→1−G(τ)θ.\text{(d)}\quad \mathbb E[W_c]\to \frac{1-G(\tau)}{\theta}.(d)E[Wc​]→θ1−G(τ)​.

The goal states all four parts. The constants 111, 000, 1/θ1/\theta1/θ and (1−G(τ))/θ(1-G(\tau))/\theta(1−G(τ))/θ are those of the paper.

Milestones

Proposition 1 (p. 8) is the coupling inequality ThL,1≤ThO\mathrm{Th}_{L,1}\le\mathrm{Th}_OThL,1​≤ThO​, where ThO\mathrm{Th}_OThO​ is the throughput of the SRPT queue. The capacity constraint (5) (p. 16) says that work is completed at rate at most sss. Two steps in the proof of Lemma 4 (p. 17) concern Erlang's loss formula. The first is the identity E(r,C)=(∫0∞(1+t/r)Ce−tdt)−1E(r,C) = \bigl(\int_0^\infty(1+t/r)^C e^{-t}dt\bigr)^{-1}E(r,C)=(∫0∞​(1+t/r)Ce−tdt)−1. The second is the limit E(s,s)→0E(s,s)\to 0E(s,s)→0. Lemma 4 (p. 16) gives ThL,1λ/λ→G(τ)\mathrm{Th}^\lambda_{L,1}/\lambda\to G(\tau)ThL,1λ​/λ→G(τ). Problem (7) (p. 18) is a linear program over service-probability profiles. Lemma 5 (p. 17) says the limiting service probability is γˉ(x)=1{x≤τ}\bar\gamma(x) = \mathbf 1\{x\le\tau\}γˉ​(x)=1{x≤τ}; the mission states the analytic step that concludes its proof (p. 18), not Lemma 5 itself. Theorem 2(a) is the goal's first part.

Significance

Theorem 2 is a state-space collapse: an infinite-dimensional preemptive system becomes, in the limit, a two-class priority rule with an explicit threshold. Several consequences follow from it. SRPT asymptotically minimizes the waiting time of served customers and maximizes that of abandoning ones (Corollary 1). It also asymptotically maximizes throughput among all disciplines (Proposition 3). Its performance measures are insensitive to the patience law beyond its mean.

The paper proves Theorem 2 on paper. To our knowledge none of it is machine-checked. The mission asks for a formal model of a multi-server preemptive queue with abandonment and a formal proof of the coupling. It also asks for the Erlang-formula asymptotics and the variational step that pins down γˉ\bar\gammaγˉ​. Two parts of the published argument need care in a formal proof. The proof of (b) switches to patience laws with f(0)>0f(0)>0f(0)>0, while the statement is for general patience laws. The proof of Lemma 5 presupposes that γˉ=lim⁡γλ\bar\gamma = \lim \gamma^\lambdaγˉ​=limγλ exists. A complete development must close both points or replace them with arguments that avoid them.

Difficulty

The SRPT queue has no finite-dimensional Markov description. Preemptions mean that the order in which customers are served is not their arrival order, and a preempted customer's patience keeps running. Standard fluid or diffusion limits for many-server queues track the number of customers, or a measure-valued state under first-come-first-served, and SRPT fits neither. The coupling with the loss system avoids this, but proving it requires a matching argument along the sample path that survives every preemption. Converting throughput bounds into statements about conditional waiting times then requires control of steady-state quantities that the model does not provide in closed form.

Formalization scope

The model is a single definitions file in the namespace SRPTManyServer.Collapse, with these conventions.

  • Sample paths. A path lists arrival, service and patience times (An,Sn,Tn)n≥0(A_n, S_n, T_n)_{n\ge 0}(An​,Sn​,Tn​)n≥0​. It is admissible if arrivals are strictly increasing from time ≥0\ge 0≥0 and tend to infinity, and if Sn,Tn>0S_n, T_n > 0Sn​,Tn​>0; this holds almost surely.
  • Schedules. A schedule is a measurable {0,1}\{0,1\}{0,1}-valued δn(t)\delta_n(t)δn​(t). SRPT is the relational predicate "only present customers are served; min⁡(s,#present)\min(s, \#\text{present})min(s,#present) are in service; those in service have remaining work no larger than any waiting customer". Ties are broken arbitrarily. The page describes preemption at arrivals, and the predicate also fixes who takes a freed server.
  • The loss system. It is defined by recursion over arrivals.
  • The probability model. The seeds are i.i.d. Exp(1)\mathrm{Exp}(1)Exp(1) variables EnE_nEn​, and system sss has arrivals An=(E0+⋯+En)/(ρμs)A_n = (E_0+\dots+E_n)/(\rho\mu s)An​=(E0​+⋯+En​)/(ρμs). All systems share the service and patience times. The sequence is indexed by s∈Ns\in\mathbb Ns∈N in place of λ\lambdaλ.
  • Standing assumptions. Both laws are carried by [0,∞)[0,\infty)[0,∞) and have densities. The means are 1/μ1/\mu1/μ and 1/θ1/\theta1/θ, ρ>1\rho>1ρ>1, and τ\tauτ satisfies (1).
  • Steady state. Steady-state tagged-customer quantities are read as almost-sure customer long-run averages, for example the fraction served among customers 0,…,N−10,\dots,N-10,…,N−1 with Sn≤τS_n\le\tauSn​≤τ as N→∞N\to\inftyN→∞. Their existence for each sss is a hypothesis, standing for the paper's assumption of a steady state. The theorems are about these limits as s→∞s\to\inftys→∞.
  • Pathwise and analytic forms. Proposition 1 is stated for one deterministic admissible path and every SRPT schedule of it. The capacity constraint (5) is stated pathwise: completed work by time ttt is at most sts tst. Lemma 5 itself is not stated; the final step of its proof is, analytically and ggg-almost everywhere: if ∫gγˉ≥G(τ)\int g\bar\gamma \ge G(\tau)∫gγˉ​≥G(τ) and ∫xgγˉ≤E[S1{S≤τ}]\int xg\bar\gamma \le \mathbb E[S\mathbf 1\{S\le\tau\}]∫xgγˉ​≤E[S1{S≤τ}], then γˉ=1{⋅≤τ}\bar\gamma = \mathbf 1\{\cdot\le\tau\}γˉ​=1{⋅≤τ} a.e. where g>0g>0g>0. Problem (7) is an IsLeast statement over measurable γ\gammaγ.

The discipline in the goal is SRPT on the actual arrival stream. It is not the two-class priority system, the threshold τ\tauτ does not appear in the scheduling predicate, and the throughputs and service probabilities are not free parameters: a statement in which they were would reduce the goal to Lemma 5. The non-idling clause is part of the SRPT predicate, so the empty schedule does not qualify.

A complete development needs a sample-path theory of preemptive multi-server queues with abandonment. It also needs renewal or regenerative arguments that connect time averages with customer averages, and the insensitivity of the M/G/s/sM/G/s/sM/G/s/s blocking probability, which the paper cites from the literature and does not prove. These pieces are reusable beyond this mission. Contributions to any milestone are welcome. The Erlang identities, problem (7) and the final step of the proof of Lemma 5 are self-contained analysis.

Not formalized here: Corollary 1, Proposition 3 (Appendix B), inequality (4), and the numerical comparisons of §4.

Selected references

  • J. Dong and R. Ibrahim, On the SRPT scheduling discipline in many-server queues with impatient customers, arXiv:2102.05789v1, 2021 (published in Management Science). https://arxiv.org/abs/2102.05789
  • L. Schrage, A proof of the optimality of the shortest remaining processing time discipline, Operations Research 16(3), 687–690, 1968. https://doi.org/10.1287/opre.16.3.687
  • W. Whitt, Fluid models for multiserver queues with abandonments, Operations Research 54(1), 37–54, 2006. https://doi.org/10.1287/opre.1050.0227
  • O. Garnett, A. Mandelbaum and M. Reiman, Designing a call center with impatient customers, Manufacturing & Service Operations Management 4(3), 208–227, 2002. https://doi.org/10.1287/msom.4.3.208.7753
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Algorithmic Game TheoryEconomicsOperations Research·Captain: mikedeng1

Multidimensional Targeting and Consumer Response: With a Small Ad Cost and a Click Cost Just Below the md-Equilibrium Threshold, Single-Dimensional Targeting Is Strictly More ProfitableResearch Paper

Motivation

Firms that advertise online choose whom to target from the customer data they hold, and the industry's working assumption is that more granular data can only help: a firm that knows more about each consumer can at worst ignore the extra information. Despotakis and Yu (SSRN 3900394; Management Science, 2022, doi:10.1287/mnsc.2022.4604) show that this fails once consumers draw inferences from being targeted. A consumer who receives an ad learns something about how well the product suits her, and she decides whether to spend effort clicking on that basis. When the firm uses more dimensions of data, the set of consumers it targets changes shape, and the signal that being targeted conveys becomes weaker. In equilibrium the firm can then earn strictly less with more data than with less.

The result belongs to a line of work on targeted advertising as a signal, and on the value of customer data to a firm whose actions consumers observe and interpret. It is a commitment problem: the firm would like to promise to use less information, but cannot.

Setting

A unit mass of consumers is interested in a product sold at an exogenous price p∈(0,1)p\in(0,1)p∈(0,1). A consumer's utility from the product is

u=ωα+(1−ω)β,u=\omega\alpha+(1-\omega)\beta,u=ωα+(1−ω)β,

where α,β∈[0,1]\alpha,\beta\in[0,1]α,β∈[0,1] are her matching values on two components of the product and ω∈[0,1]\omega\in[0,1]ω∈[0,1] is her private weight on the first. The three are independent and uniform on [0,1][0,1][0,1]. The consumer does not know α\alphaα and β\betaβ until she clicks.

The firm sends ads at unit ad cost cad>0c_{ad}>0cad​>0. Under single-dimensional (sd) targeting it observes α\alphaα and chooses a targeting set Σ⊆[0,1]\Sigma\subseteq[0,1]Σ⊆[0,1]; under multidimensional (md) targeting it observes (α,β)(\alpha,\beta)(α,β) and chooses Σ⊆[0,1]2\Sigma\subseteq[0,1]^2Σ⊆[0,1]2.

A targeted consumer does not see Σ\SigmaΣ but expects a set Σ~\widetilde\SigmaΣ. Her posterior is uniform: under sd targeting α\alphaα is uniform on Σ~\widetilde\SigmaΣ and β\betaβ uniform on [0,1][0,1][0,1]; under md targeting (α,β)(\alpha,\beta)(α,β) is uniform on Σ~\widetilde\SigmaΣ. She clicks at click cost cclick>0c_{click}>0cclick​>0 if and only if her posterior expected surplus E[max⁡{u−p,0};Σ~]E[\max\{u-p,0\};\widetilde\Sigma]E[max{u−p,0};Σ] is at least cclickc_{click}cclick​; the weights that click form the click set Ω(Σ~)⊆[0,1]\Omega(\widetilde\Sigma)\subseteq[0,1]Ω(Σ)⊆[0,1]. After clicking she learns uuu and buys if and only if u≥pu\ge pu≥p.

Against a click set Ω\OmegaΩ, the ad value of a consumer is ppp times the probability that she clicks and buys, minus cadc_{ad}cad​; under md targeting πmd(α,β;Ω)=p ∣{ω∈Ω:ωα+(1−ω)β≥p}∣−cad\pi^{md}(\alpha,\beta;\Omega)=p\,|\{\omega\in\Omega:\omega\alpha+(1-\omega)\beta\ge p\}|-c_{ad}πmd(α,β;Ω)=p∣{ω∈Ω:ωα+(1−ω)β≥p}∣−cad​. The firm's profit from targeting TTT is the integral of the ad value over TTT.

A non-trivial equilibrium is a targeting set Σ\SigmaΣ of positive measure that maximizes the firm's profit over all targeting sets, against the click set Ω(Σ)\Omega(\Sigma)Ω(Σ) that consumers who correctly expect Σ\SigmaΣ produce. An md equilibrium is symmetric if Σ\SigmaΣ is symmetric about the 45-degree line. Π∗sd\Pi^{*sd}Π∗sd and Π∗md\Pi^{*md}Π∗md denote equilibrium profits. Two thresholds from the paper enter the statements: the click-cost threshold cclickmax(cad,p)c^{max}_{click}(c_{ad},p)cclickmax​(cad​,p) of Equation (7), above which no non-trivial symmetric md equilibrium exists, and the ad-cost threshold cad‾(cclick,p)\overline{c_{ad}}(c_{click},p)cad​​(cclick​,p) from the proof of Proposition 1.

Formalization targets

Goal: Proposition 3

For every p∈(0,1)p\in(0,1)p∈(0,1) there is δ>0\delta>0δ>0 such that for every cad∈(0,δ)c_{ad}\in(0,\delta)cad​∈(0,δ) there is c1<cclickmax(cad,p)c_1<c^{max}_{click}(c_{ad},p)c1​<cclickmax​(cad​,p) such that for every cclick∈(c1,cclickmax(cad,p)]c_{click}\in(c_1,c^{max}_{click}(c_{ad},p)]cclick​∈(c1​,cclickmax​(cad​,p)] both a non-trivial sd equilibrium and a non-trivial symmetric md equilibrium exist, and

Π∗md<Π∗sd\Pi^{*md}<\Pi^{*sd}Π∗md<Π∗sd

for every such pair. The goal fixes neither δ\deltaδ nor c1c_1c1​; the right end of the click-cost interval is the explicit threshold of Equation (7).

Milestones

  1. Lemmas 1 and 3: the click set is [0,1][0,1][0,1] minus an interval, [0,ω‾]∪[ω‾,1][0,\underline\omega]\cup[\overline\omega,1][0,ω​]∪[ω,1], in both environments; for a symmetric md strategy it is symmetric about ω=1/2\omega=1/2ω=1/2.
  2. Claim 3 (first case): against Ω=[0,ω‾]∪[ω‾,1]\Omega=[0,\underline\omega]\cup[\overline\omega,1]Ω=[0,ω​]∪[ω,1] with cad≤pω‾c_{ad}\le p\underline\omegacad​≤pω​ and cad≤p(1−ω‾)c_{ad}\le p(1-\overline\omega)cad​≤p(1−ω), the md best response is the set bounded by two lines through (p,p)(p,p)(p,p) with slopes γ1∗=−cad/(p−cad)\gamma_1^*=-c_{ad}/(p-c_{ad})γ1∗​=−cad​/(p−cad​) and γ2∗=1/γ1∗\gamma_2^*=1/\gamma_1^*γ2∗​=1/γ1∗​.
  3. Proposition 1 (for (1−p)2/2<cclick<(1−p)/2(1-p)^2/2<c_{click}<(1-p)/2(1−p)2/2<cclick​<(1−p)/2): a unique non-trivial sd equilibrium [αˉ∗,1][\bar\alpha^*,1][αˉ∗,1].
  4. Proposition 2 (for cad<min⁡{p2,p(1−p)}c_{ad}<\min\{p^2,p(1-p)\}cad​<min{p2,p(1−p)}): a unique non-trivial symmetric md equilibrium if and only if cclick≤cclickmax(cad,p)c_{click}\le c^{max}_{click}(c_{ad},p)cclick​≤cclickmax​(cad​,p).
  5. Lemma 4: the sd equilibrium profit decreases in cclickc_{click}cclick​ on ((1−p)2/2,(1−p)/2)((1-p)^2/2,(1-p)/2)((1−p)2/2,(1−p)/2) and is 000 at (1−p)/2(1-p)/2(1−p)/2.
  6. Lemma 5: near cclickmaxc^{max}_{click}cclickmax​ the symmetric md profit tends to 000 as cad→0c_{ad}\to0cad​→0.
  7. Lemma 6: (1−p)2/2<cclickmax(cad,p)<(1−p)/2(1-p)^2/2<c^{max}_{click}(c_{ad},p)<(1-p)/2(1−p)2/2<cclickmax​(cad​,p)<(1−p)/2 for cad<min⁡{p2,p(1−p)}c_{ad}<\min\{p^2,p(1-p)\}cad​<min{p2,p(1−p)}.

Significance

The result is a clean counterexample to the monotonicity of the value of information for a firm whose actions are observed by strategic receivers. It isolates a mechanism, inference from being targeted, that does not need competition, price discrimination or privacy costs to make extra data harmful. The paper uses it to explain why firms might coarsen the data they act on, and §5 revisits the comparison with endogenous pricing and with consumers who do not know which dimension the firm targets on.

On the platform this mission is the first model of targeting with consumer inference. The model layer, uniform posteriors on an expected targeting set, click sets defined by posterior expected surplus, and equilibria defined as fixed points over arbitrary measurable targeting sets, is reusable for other signalling-through-targeting results. The result is proved on paper, with Lemmas 4 and 5 argued in sketch form; to our knowledge no part of it has a machine-checked proof.

Difficulty

Both equilibria are fixed points: the firm's best response depends on the click set, and the click set depends on the expected targeting set through a posterior average. The md firm may choose any measurable subset of the square, so the reduction to the two-line class S\mathcal SS of Equation (6) is part of the work, and Proposition 2 asks for uniqueness among all symmetric measurable equilibria, not only within S\mathcal SS.

The comparison itself is not a monotonicity argument. As cclickc_{click}cclick​ approaches cclickmaxc^{max}_{click}cclickmax​, the md click set shrinks to the threshold where the md equilibrium disappears, while the sd profit stays positive only because cclickmaxc^{max}_{click}cclickmax​ lies strictly below (1−p)/2(1-p)/2(1−p)/2, where the sd profit vanishes. Making this precise requires the piecewise closed forms of the expected surplus (with logarithms) and control of both profits uniformly as cad→0c_{ad}\to0cad​→0, which the page leaves implicit. Comparing the closed forms at a single numerical point does not give the statement for every price.

Formalization scope

All quantities are real numbers. Consumer populations are Lebesgue measure on [0,1][0,1][0,1] and [0,1]2[0,1]^2[0,1]2, so probabilities are lengths and areas. Targeting sets are measurable subsets of the unit interval or square, "non-trivial" means positive measure, "symmetric" means invariance under (α,β)↦(β,α)(\alpha,\beta)\mapsto(\beta,\alpha)(α,β)↦(β,α), and "unique" means unique up to a null set. The tie-breaks follow the page: buy at u=pu=pu=p, click at equality, and indifference is allowed in the firm's optimization. Click thresholds are arbitrary reals, so an empty click set is expressible.

Equilibria are defined as fixed points, never by the paper's closed forms [αˉ∗,1][\bar\alpha^*,1][αˉ∗,1] and Σmd(γ1∗,1/γ1∗)\Sigma^{md}(\gamma_1^*,1/\gamma_1^*)Σmd(γ1∗​,1/γ1∗​); otherwise Propositions 1 and 2 would be definitional and the goal a comparison of two formulas. The paper's cclickminc^{min}_{click}cclickmin​ is defined as the least click cost at which Π∗sd≥Π∗md\Pi^{*sd}\ge\Pi^{*md}Π∗sd≥Π∗md, which would make a literal statement nearly true by definition; the goal therefore asserts the existence of the region instead, and it includes existence of both equilibria so that the comparison is not vacuous.

Added or restricted hypotheses: Propositions 1 and 2 are stated only in the regimes Proposition 3 uses; Proposition 1 uses cad<cad‾c_{ad}<\overline{c_{ad}}cad​<cad​​ strictly (at equality the cutoff is 111 and the targeting set is null); Lemma 4 adds cad<p(1−p)c_{ad}<p(1-p)cad​<p(1−p); Lemma 5 is stated in ε\varepsilonε–δ\deltaδ form because its limit is not shown to exist; and the price is p∈(0,1)p\in(0,1)p∈(0,1) throughout.

A complete development needs set integrals and product measures from Mathlib, convexity of the expected surplus in ω\omegaω, and real analysis of the piecewise closed forms. Proofs of any milestone, and alternative arguments for Lemmas 4 and 5, are welcome.

Selected references

  • S. Despotakis and J. Yu, Multidimensional Targeting and Consumer Response, SSRN working paper 3900394 (version of October 11, 2022). https://ssrn.com/abstract=3900394
  • S. Despotakis and J. Yu, Multidimensional Targeting and Consumer Response, Management Science, 2022. https://doi.org/10.1287/mnsc.2022.4604
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Convex OptimizationLinear algebraOptimization·Captain: mikedeng1

Conic Optimization with Spectral Functions on Euclidean Jordan Algebras: The Root-Determinant Cone Barrier Is a (1 + d)-Logarithmically Homogeneous Self-Concordant BarrierResearch Paper

Motivation

Interior-point methods solve a conic optimization problem by following the minimizers of a barrier function for the cone. Their iteration count is governed by the barrier's parameter ν\nuν: the best known algorithms need O(νlog⁡(1/ε))O(\sqrt\nu\log(1/\varepsilon))O(ν​log(1/ε)) iterations to reach accuracy ε\varepsilonε (Nesterov and Todd, 1997). A cone can be used natively by a solver only once a logarithmically homogeneous self-concordant barrier (LHSCB) with a small parameter is known for it, together with efficient oracles for its derivatives.

Coey, Kapelevich and Vielma (arXiv:2103.04104v2; Mathematics of Operations Research, 2022) study cones defined by spectral functions on Euclidean Jordan algebras. This framework covers vectors, real symmetric matrices and complex Hermitian matrices at once. The paper implements the resulting cones in the solver Hypatia. One of its two new barrier results concerns the root-determinant cone, the hypograph of the geometric mean of the eigenvalues. For symmetric matrices this is the hypograph of det⁡(W)1/d\det(W)^{1/d}det(W)1/d over the positive semidefinite cone, a standard modelling device for D-optimal experimental design and for determinant maximization. Before this paper, the usual way to represent it was an extended formulation with auxiliary variables and a semidefinite constraint.

Setting

A Jordan algebra is a real vector space VVV with a bilinear product ∘\circ∘ that is commutative and satisfies the Jordan identity wa∘(wa2∘wb)=wa2∘(wa∘wb)w_a\circ(w_a^2\circ w_b)=w_a^2\circ(w_a\circ w_b)wa​∘(wa2​∘wb​)=wa2​∘(wa​∘wb​), where w2:=w∘ww^2:=w\circ ww2:=w∘w. It has a multiplicative identity eee. It is Euclidean if ⟨wa∘wb,wc⟩=⟨wb,wa∘wc⟩\langle w_a\circ w_b,w_c\rangle=\langle w_b,w_a\circ w_c\rangle⟨wa​∘wb​,wc​⟩=⟨wb​,wa​∘wc​⟩. An idempotent is a ccc with c2=cc^2=cc2=c. It is primitive if it is non-zero and is not the sum of two orthogonal non-zero idempotents. A Jordan frame is a family c1,…,cdc_1,\dots,c_dc1​,…,cd​ of pairwise orthogonal primitive idempotents summing to eee. Every Jordan frame of VVV has the same size ddd, the rank of VVV.

Every w∈Vw\in Vw∈V has a spectral decomposition w=∑i∈[ ⁣[d] ⁣]wiciw=\sum_{i\in[\![d]\!]}w_ic_iw=∑i∈[[d]]​wi​ci​ over a Jordan frame, with real eigenvalues w1,…,wdw_1,\dots,w_dw1​,…,wd​. From these, det⁡(w)=∏iwi\det(w)=\prod_iw_idet(w)=∏i​wi​, tr⁡(w)=∑iwi\operatorname{tr}(w)=\sum_iw_itr(w)=∑i​wi​, and a real function fff acts by f(w)=∑if(wi)cif(w)=\sum_if(w_i)c_if(w)=∑i​f(wi​)ci​. The inner product is the trace form ⟨wa,wb⟩=tr⁡(wa∘wb)\langle w_a,w_b\rangle=\operatorname{tr}(w_a\circ w_b)⟨wa​,wb​⟩=tr(wa​∘wb​). The cone of squares is Q={w∘w:w∈V}\mathcal Q=\{w\circ w:w\in V\}Q={w∘w:w∈V}; w≻0w\succ0w≻0 means w∈int⁡(Q)w\in\operatorname{int}(\mathcal Q)w∈int(Q). The quadratic representation is P(w)=2L(w)2−L(w2)P(w)=2L(w)^2-L(w^2)P(w)=2L(w)2−L(w2), where L(w)v=w∘vL(w)v=w\circ vL(w)v=w∘v.

The root-determinant is φ(w)=det⁡(w)1/d\varphi(w)=\det(w)^{1/d}φ(w)=det(w)1/d on Q\mathcal QQ. With E=R×Q\mathcal E=\mathbb R\times\mathcal QE=R×Q and ζ(u,w)=φ(w)−u\zeta(u,w)=\varphi(w)-uζ(u,w)=φ(w)−u, the root-determinant cone and its candidate barrier are

Krtdet={(u,w)∈R×Q: u≤det⁡(w)1/d},Γ(u,w)=−log⁡ζ(u,w)−log⁡det⁡(w).\mathcal K_{\mathrm{rtdet}}=\{(u,w)\in\mathbb R\times\mathcal Q:\ u\le\det(w)^{1/d}\},\qquad \Gamma(u,w)=-\log\zeta(u,w)-\log\det(w).Krtdet​={(u,w)∈R×Q: u≤det(w)1/d},Γ(u,w)=−logζ(u,w)−logdet(w).

A function Γ\GammaΓ is a ν\nuν-LHSCB for a cone K\mathcal KK if it is C3C^3C3 and convex on int⁡(K)\operatorname{int}(\mathcal K)int(K) and tends to +∞+\infty+∞ at the boundary. It must also satisfy Γ(θu~)=Γ(u~)−νlog⁡θ\Gamma(\theta\tilde u)=\Gamma(\tilde u)-\nu\log\thetaΓ(θu~)=Γ(u~)−νlogθ and ∣∇3Γ(u~)[p~,p~,p~]∣≤2(∇2Γ(u~)[p~,p~])3/2|\nabla^3\Gamma(\tilde u)[\tilde p,\tilde p,\tilde p]|\le2(\nabla^2\Gamma(\tilde u)[\tilde p,\tilde p])^{3/2}∣∇3Γ(u~)[p~​,p~​,p~​]∣≤2(∇2Γ(u~)[p~​,p~​])3/2, and the parameter satisfies ν≥1\nu\ge1ν≥1.

Formalization targets

Goal: Proposition 7.1 (p. 24)

Krtdet is a proper cone, and  Γ is a (1+d)-LHSCB for Krtdet.\mathcal K_{\mathrm{rtdet}}\ \text{is a proper cone, and}\ \ \Gamma\ \text{is a}\ (1+d)\text{-LHSCB for}\ \mathcal K_{\mathrm{rtdet}}.Krtdet​ is a proper cone, and  Γ is a (1+d)-LHSCB for Krtdet​.

The goal holds for every finite-dimensional Euclidean Jordan algebra of rank d≥1d\ge1d≥1, not for one matrix algebra.

Milestones, in proof order

  1. Krtdet\mathcal K_{\mathrm{rtdet}}Krtdet​ is proper (p. 23).
  2. Ψ(u,w)=−log⁡det⁡(w)\Psi(u,w)=-\log\det(w)Ψ(u,w)=−logdet(w) is a ddd-LHSCB for E\mathcal EE (p. 24).
  3. φ\varphiφ is nonnegative, concave and homogeneous on Q\mathcal QQ ((96), p. 23).
  4. ζ\zetaζ is concave and C3C^3C3 on int⁡(E)\operatorname{int}(\mathcal E)int(E) (p. 24).
  5. The derivative identities, with r^=P(w−1/2)r\hat r=P(w^{-1/2})rr^=P(w−1/2)r, σ\sigmaσ the eigenvalues of r^\hat rr^, m1=d−1∑iσim_1=d^{-1}\sum_i\sigma_im1​=d−1∑i​σi​ and δi=σi−m1\delta_i=\sigma_i-m_1δi​=σi​−m1​:
∇2Ψ(u~)[p~,p~]=tr⁡(r^2)=∥σ∥2,∇2φ(w)[r,r]=−d−1φ∑iδi2,∇3φ(w)[r,r,r]=d−1φ∑iδi2(m1+2σi),\nabla^2\Psi(\tilde u)[\tilde p,\tilde p]=\operatorname{tr}(\hat r^2)=\|\sigma\|^2,\quad \nabla^2\varphi(w)[r,r]=-d^{-1}\varphi\textstyle\sum_i\delta_i^2,\quad \nabla^3\varphi(w)[r,r,r]=d^{-1}\varphi\sum_i\delta_i^2(m_1+2\sigma_i),∇2Ψ(u~)[p~​,p~​]=tr(r^2)=∥σ∥2,∇2φ(w)[r,r]=−d−1φ∑i​δi2​,∇3φ(w)[r,r,r]=d−1φ∑i​δi2​(m1​+2σi​),

which are (105), (107) and (108). 6. The scalar inequality (109c):  d−1φ∑iδi2(∥σ∥−m1+2(∥σ∥−σi))≥0\ d^{-1}\varphi\sum_i\delta_i^2(\|\sigma\|-m_1+2(\|\sigma\|-\sigma_i))\ge0 d−1φ∑i​δi2​(∥σ∥−m1​+2(∥σ∥−σi​))≥0 for every σ∈Rd\sigma\in\mathbb R^dσ∈Rd. 7. The compatibility inequality (103) on int⁡(Krtdet)\operatorname{int}(\mathcal K_{\mathrm{rtdet}})int(Krtdet​):

∇3ζ(u~)[p~,p~,p~]≤−3(∇2Ψ(u~)[p~,p~])1/2∇2ζ(u~)[p~,p~].\nabla^3\zeta(\tilde u)[\tilde p,\tilde p,\tilde p]\le-3\big(\nabla^2\Psi(\tilde u)[\tilde p,\tilde p]\big)^{1/2}\nabla^2\zeta(\tilde u)[\tilde p,\tilde p].∇3ζ(u~)[p~​,p~​,p~​]≤−3(∇2Ψ(u~)[p~​,p~​])1/2∇2ζ(u~)[p~​,p~​].
  1. The reduction: if Ψ\PsiΨ is a ddd-LHSCB, ζ\zetaζ is C3C^3C3 and concave, and (103) holds, then Γ\GammaΓ is a (1+d)(1+d)(1+d)-LHSCB. This is the paper's application of Nesterov–Nemirovskii Proposition 5.1.7.

Significance

The result gives the root-determinant cone a barrier whose parameter 1+d1+d1+d is one more than the optimal parameter ddd of its domain R×Q\mathbb R\times\mathcal QR×Q, so it cannot be improved by more than one (p. 24). It also removes the extended formulation: a solver works with the cone in its natural dimension. The paper pairs the barrier with closed-form oracles for the gradient, Hessian product and inverse Hessian product (§7.4, Lemma 7.1), and reports computational gains in Hypatia. Because the statement is uniform over Euclidean Jordan algebras, it covers the vector, real symmetric and complex Hermitian cases at once.

The result is proved in the paper; this mission formalizes it. To the best of the curators' knowledge, it has no machine-checked proof, and Lean's Mathlib has no theory of Euclidean Jordan algebras, spectral decompositions in them, or barrier functions for their cones. Formalizing Proposition 7.1 therefore also yields a reusable layer: the Jordan-algebraic setting, the cone of squares, the quadratic representation, and an LHSCB predicate on arbitrary normed spaces.

Difficulty

The obvious route checks self-concordance of Γ\GammaΓ directly. That requires bounding the third derivative of −log⁡(det⁡(w)1/d−u)−log⁡det⁡(w)-\log(\det(w)^{1/d}-u)-\log\det(w)−log(det(w)1/d−u)−logdet(w) by the 3/23/23/2-power of its Hessian in every direction. The two logarithmic terms interact, and no simple direct estimate is available. The paper instead uses a compatibility criterion of Nesterov and Nemirovskii, which reduces the barrier property to the single inequality (103) between derivatives of ζ\zetaζ and Ψ\PsiΨ. In Lean that criterion is not available and must be established for this cone; it is the deepest milestone.

The derivative identities (105), (107) and (108) require differential calculus of spectral functions on a Jordan algebra: derivatives of det⁡\detdet, of w↦w−1w\mapsto w^{-1}w↦w−1, and of P(w−1/2)P(w^{-1/2})P(w−1/2), expressed through the eigenvalues of the scaled direction r^\hat rr^. Deriving them from the structure axioms needs, among other things, the fact that the eigenvalues of θw\theta wθw and w2w^2w2 are those of www scaled and squared, uniqueness of the spectral decomposition, and positivity of the eigenvalues on int⁡(Q)\operatorname{int}(\mathcal Q)int(Q). Only the final scalar inequality (109c) is elementary.

Formalization scope

VVV is a real finite-dimensional inner product space carrying a structure EJA V d. The structure bundles the Jordan product (bilinear, commutative, Jordan identity), the unit eee and the Euclidean property. It also bundles, for every www, eigenvalues and a Jordan frame of primitive idempotents with w=∑iwiciw=\sum_iw_ic_iw=∑i​wi​ci​, and the identity ⟨a,b⟩=tr⁡(a∘b)\langle a,b\rangle=\operatorname{tr}(a\circ b)⟨a,b⟩=tr(a∘b). The spectral theorem (Faraut–Korányi III.1.2) says such data exist for every Euclidean Jordan algebra of rank ddd, so this is the paper's setting. Primitivity forces ddd to be the rank: without it, a frame could be padded with zeros and det⁡\detdet would change.

The ambient space is R×V\mathbb R\times VR×V. Directional derivatives are iterated Fréchet derivatives on the diagonal, and "boundary" is the topological frontier. The barrier limit is taken within the interior at every frontier point.

The following conventions are fixed:

  • the rank satisfies d≥1d\ge1d≥1, since the paper divides by ddd and the goal is false at d=0d=0d=0;
  • self-concordance includes convexity, as in Nesterov–Nemirovskii Definition 2.1.1;
  • logarithmic homogeneity (38) is required for u~∈int⁡(K)\tilde u\in\operatorname{int}(\mathcal K)u~∈int(K) and θ>0\theta>0θ>0;
  • ∥σ∥\|\sigma\|∥σ∥ is the Euclidean norm;
  • (⋅)1/2(\cdot)^{1/2}(⋅)1/2 in (103) is the real square root;
  • (105) is stated in squared form;
  • φ\varphiφ, ζ\zetaζ, Γ\GammaΓ, Ψ\PsiΨ and r^\hat rr^ are total functions that are only evaluated on the relevant interiors.

Properness is a separate predicate from LHSCB, because E\mathcal EE is not pointed.

A trivializing formalization is ruled out by these choices. Specializing VVV to Rd\mathbb R^dRd or Sd\mathbb S^dSd, dropping primitivity, allowing d=0d=0d=0, dropping convexity, or imposing the barrier limit at only some boundary points would each prove a different, weaker or vacuous statement.

Proposition 6.1 (the (2+d)(2+d)(2+d)-LHSCB for the matrix monotone derivative cones) and Lemma 7.1 (the inverse Hessian oracle) are deliberately absent. The first needs matrix monotonicity and Löwner's integral representation and is independent of Proposition 7.1. The second is an oracle formula that the goal does not use.

Contributions are welcome at every level: the scalar inequality (109c); the cone and homogeneity facts; the spectral calculus behind (105)–(108); and the compatibility reduction. The Jordan-algebraic infrastructure and the LHSCB predicate are reusable beyond this mission.

Selected references

  • C. Coey, L. Kapelevich, J. P. Vielma, Conic optimization with spectral functions on Euclidean Jordan algebras, Mathematics of Operations Research, 2022. https://arxiv.org/abs/2103.04104v2
  • Y. Nesterov, A. Nemirovskii, Interior-Point Polynomial Algorithms in Convex Programming, SIAM, 1994. https://doi.org/10.1137/1.9781611970791
  • J. Faraut, A. Korányi, Analysis on Symmetric Cones, Oxford University Press, 1994 (cited in the paper as Faraut and Koranyi, 1998).
  • Y. Nesterov, M. J. Todd, Self-scaled barriers and interior-point methods for convex programming, Mathematics of Operations Research 22(1), 1997. https://doi.org/10.1287/moor.22.1.1
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