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CombinatoricsGraph Theory·Captain: utkuokur

Ten Challenges 08: Ryser's hypergraph conjectureOpen Problem

Motivation

For bipartite graphs, Kőnig's theorem says that the minimum number of vertices needed to meet every edge equals the maximum number of pairwise disjoint edges: τ=ν\tau=\nuτ=ν. For hypergraphs whose edges have rrr vertices, the ratio τ/ν\tau/\nuτ/ν can be as large as rrr in general, and the bound τ≤rν\tau\le r\nuτ≤rν is trivial. Ryser's conjecture asserts that for rrr-partite rrr-uniform hypergraphs, the natural generalisation of bipartite graphs, the trivial bound can be improved by one:

τ(H)≤(r−1) ν(H).\tau(\mathcal H)\le (r-1)\,\nu(\mathcal H).τ(H)≤(r−1)ν(H).

For r=2r=2r=2 it is Kőnig's theorem. Truncated projective planes show that the factor r−1r-1r−1 cannot be lowered when r−1r-1r−1 is a prime power. The conjecture is a central problem on matchings and covers in hypergraphs (Aharoni 2001, Haxell–Scott 2012).

Timeline.

  • 1931 — Kőnig proves τ=ν\tau=\nuτ=ν for bipartite graphs, the case r=2r=2r=2.
  • 1971 — The conjecture appears in the thesis of Ryser's student Henderson; the case ν=1\nu=1ν=1 is attributed to Lovász.
  • 1983 — Tuza proves the intersecting case ν=1\nu=1ν=1 for r≤5r\le 5r≤5 (Tuza 1983).
  • 2001 — Aharoni proves the case r=3r=3r=3 using the topological Hall theorem of Aharoni and Haxell (Aharoni 2001).
  • 2012 — Haxell and Scott prove τ≤(r−ε)ν\tau\le (r-\varepsilon)\nuτ≤(r−ε)ν for r=4,5r=4,5r=4,5 and some ε>0\varepsilon>0ε>0 (Haxell–Scott 2012).
  • 2017–2021 — Francetić, Herke, McKay and Wanless, then Abu-Khazneh, Barát, Pokrovskiy and Szabó, construct families of extremal hypergraphs; Bishnoi, Das, Morris and Szabó settle the ttt-intersecting case (Abu-Khazneh et al. 2019, Bishnoi et al. 2021).

The case r=4r=4r=4 is open.

Setting

A hypergraph H\mathcal HH has a finite vertex set V(H)V(\mathcal H)V(H) and a set E(H)E(\mathcal H)E(H) of edges, each a subset of V(H)V(\mathcal H)V(H). It is rrr-uniform if every edge has exactly rrr vertices, and rrr-partite if V(H)V(\mathcal H)V(H) is the disjoint union of parts P1,…,PrP_1,\dots,P_rP1​,…,Pr​ such that every edge meets every part in exactly one vertex. A vertex cover is a set C⊆V(H)C\subseteq V(\mathcal H)C⊆V(H) meeting every edge; the cover number τ(H)\tau(\mathcal H)τ(H) is the least size of a vertex cover. A matching is a set of pairwise disjoint edges; the matching number ν(H)\nu(\mathcal H)ν(H) is the largest size of a matching. For r∈Nr\in\mathbb Nr∈N let Ry(r)\mathrm{Ry}(r)Ry(r) be the statement

r≥2  ⟹  every r-partite r-uniform hypergraph H satisfies τ(H)≤(r−1) ν(H).r\ge 2 \implies \text{every } r\text{-partite } r\text{-uniform hypergraph } \mathcal H \text{ satisfies } \tau(\mathcal H)\le (r-1)\,\nu(\mathcal H).r≥2⟹every r-partite r-uniform hypergraph H satisfies τ(H)≤(r−1)ν(H).

Formalization targets

Goal

∀r∈N:Ry(r).\forall r\in\mathbb N:\quad \mathrm{Ry}(r).∀r∈N:Ry(r).

Rungs

Ry(2)\mathrm{Ry}(2)Ry(2) is Kőnig's theorem, Ry(3)\mathrm{Ry}(3)Ry(3) is Aharoni's theorem, and Ry(4)\mathrm{Ry}(4)Ry(4) is the first open rung. For r≤1r\le 1r≤1 the statement is vacuous.

Significance

Ryser's conjecture is the hypergraph form of Kőnig's theorem and one of the standard open problems in the matching theory of hypergraphs. Its intersecting case (ν=1\nu=1ν=1) is equivalent to a question about the covering number of Latin-square-like structures and is open for r≥6r\ge 6r≥6; its fractional version, τ≤(r−1)ν∗\tau\le (r-1)\nu^*τ≤(r−1)ν∗, was proved by Füredi. A proof for r=4r=4r=4 would be the first progress on the full conjecture since Aharoni's theorem.

Formalizing the known rungs gives a theory of finite hypergraphs, covers and matchings on top of Mathlib's Finset, which currently has Kőnig's theorem only in graph form (Hall's marriage theorem is in Mathlib). Aharoni's proof for r=3r=3r=3 goes through the topological Hall theorem, so a formalization would need the connectivity of independence complexes, a sizeable but reusable piece of topological combinatorics. None of the rungs has a machine-checked proof in the hypergraph formulation; Ry(4)\mathrm{Ry}(4)Ry(4) and the goal are open.

Difficulty

The bound τ≤rν\tau\le r\nuτ≤rν comes from taking all vertices of a maximum matching; improving it by a factor (r−1)/r(r-1)/r(r−1)/r requires exploiting the partition, and no inductive or greedy argument is known to do so beyond r=3r=3r=3. Aharoni's proof for r=3r=3r=3 is non-constructive and topological, and the topological Hall theorem gives for general rrr only τ≤rν\tau\le r\nuτ≤rν-type bounds; the ε\varepsilonε-improvements of Haxell and Scott already require long case analyses. The conjecture is tight for infinitely many rrr, so no slack is available.

Formalization scope

A hypergraph is the structure FinHypergraph α with vertices : Finset α, edges : Set (Finset α) and the axiom that every edge is a subset of vertices; since edges are finite subsets of a finite set, there are finitely many. IsUniform r, IsPartite r (parts indexed by Fin r, covering the vertex set, pairwise disjoint, each meeting each edge in exactly one vertex), IsVertexCover C (a subset of the vertices meeting every edge) and IsMatching M (a Finset of edges, pairwise disjoint) are as in the Setting. coverNumber is the infimum sInf of the sizes of vertex covers, and matchingNumber the supremum sSup of the sizes of matchings; both are natural numbers, with the conventions inf⁡∅=0\inf\emptyset=0inf∅=0 and sup⁡\supsup of an unbounded set =0=0=0, which never arise since the vertex set covers every edge whenever edges are nonempty and matchings are bounded by the number of edges. RyserConjectureFor H r is τ≤(r−1)ν\tau\le(r-1)\nuτ≤(r−1)ν under the uniformity and partiteness hypotheses, statement_08 r adds the guard 2≤r2\le r2≤r and quantifies over all vertex types with decidable equality in a universe u, and the goal is ∀ r, statement_08 r.

No trivialising reading: r=0r=0r=0 and r=1r=1r=1 are excluded by the guard, uniformity with r≥2r\ge 2r≥2 makes edges nonempty, and for an edgeless hypergraph both sides are 000. The Lean definitions are copied verbatim from the Ten Challenges repository. Because the definitions are identical, a proof of the goal or of any rung produced here can also be submitted on the Ten Challenges website, https://tenchallenges.github.io/ten-challenges/, which checks submissions automatically against the same statements and records accepted ones on its public leaderboard; contributors are welcome to do both. Contributions welcome: the basic inequalities ν≤τ≤rν\nu\le\tau\le r\nuν≤τ≤rν, finiteness of the edge set, Kőnig's theorem in this formulation, and decompositions of Aharoni's theorem.

Selected references

  • Ten Challenges website: problem statements, automatic checker and leaderboard. https://tenchallenges.github.io/ten-challenges/
  • V. Bajpai, N. Bowler, J. Carmesin, U. Okur, 10 Scalable Challenges in Combinatorics: A Public Benchmark Formalised in Lean, AI4Math workshop at CICM 2026. https://cicm-conference.org/2026/ai4math/04-okur.pdf — Lean sources: https://github.com/TenChallenges/ten-challenges (challenge 8).
  • R. Aharoni, Ryser's conjecture for tripartite 3-graphs, Combinatorica 21 (2001), 1–4. https://doi.org/10.1007/s004930170001
  • Z. Tuza, Ryser's conjecture on transversals of r-partite hypergraphs, Ars Combin. 16 (1983), 201–209.
  • P. E. Haxell, A. D. Scott, On Ryser's conjecture, Electron. J. Combin. 19 (2012), P23. https://doi.org/10.37236/1175
  • A. Abu-Khazneh, J. Barát, A. Pokrovskiy, T. Szabó, A family of extremal hypergraphs for Ryser's conjecture, J. Combin. Theory Ser. A 161 (2019), 164–177. https://doi.org/10.1016/j.jcta.2018.07.011
  • A. Bishnoi, S. Das, P. Morris, T. Szabó, Ryser's conjecture for t-intersecting hypergraphs, J. Combin. Theory Ser. A 179 (2021), 105366. https://doi.org/10.1016/j.jcta.2020.105366
  • N. Francetić, S. Herke, B. D. McKay, I. M. Wanless, On Ryser's conjecture for linear intersecting multipartite hypergraphs, European J. Combin. 61 (2017), 91–105. https://doi.org/10.1016/j.ejc.2016.10.004
  • Z. Füredi, Maximum degree and fractional matchings in uniform hypergraphs, Combinatorica 1 (1981), 155–162. https://doi.org/10.1007/BF02579271
6 thms1 active userReviewed
CombinatoricsExtremal Set Theory·Captain: utkuokur

Ten Challenges 09: Union-closed sets conjectureOpen Problem

Motivation

A family of finite sets is union-closed if the union of any two members is again a member. The union-closed sets conjecture, attributed to Frankl (1979), asserts that every such family, other than the two degenerate ones ∅\emptyset∅ and {∅}\{\emptyset\}{∅}, has an element that lies in at least half of its members. Despite its elementary statement the conjecture resisted all attempts for over forty years; it is equivalent to statements about lattices and about intersection-closed families, and the first constant-fraction bound was found only in 2022 (Bruhn–Schaudt 2015).

Timeline.

  • 1979 — Frankl poses the conjecture.
  • 1994 — Knill proves that some element lies in at least (∣F∣−1)/log⁡2∣F∣(|\mathcal F|-1)/\log_2|\mathcal F|(∣F∣−1)/log2​∣F∣ members (Knill 1994).
  • 2015 — Bruhn and Schaudt survey the partial results: families with few members, few elements, or special structure (Bruhn–Schaudt 2015).
  • 2022 — Gilmer proves the first constant bound, density at least 0.010.010.01, by an entropy argument (Gilmer 2022).
  • 2022 — Within weeks, Sawin, Chase and Lovett, Alweiss, Huang and Sellke, and Pebody independently push Gilmer's method to density at least 3−52≈0.38197\frac{3-\sqrt5}{2}\approx 0.3819723−5​​≈0.38197 (Chase–Lovett 2022, Sawin 2022, Alweiss–Huang–Sellke 2022, Pebody 2022).
  • 2023 — Further refinements improve the constant slightly beyond 0.3820.3820.382 but stay below 0.390.390.39 (Liu 2023).

Setting

Let F\mathcal FF be a finite family of finite subsets of a set UUU. It is union-closed if A∪B∈FA\cup B\in\mathcal FA∪B∈F for all A,B∈FA,B\in\mathcal FA,B∈F, and nondegenerate if F≠∅\mathcal F\ne\emptysetF=∅ and F≠{∅}\mathcal F\ne\{\emptyset\}F={∅}. The density of an element x∈Ux\in Ux∈U in F\mathcal FF is

δF(x):=∣{A∈F:x∈A}∣∣F∣.\delta_{\mathcal F}(x) := \frac{|\{A\in\mathcal F: x\in A\}|}{|\mathcal F|}.δF​(x):=∣F∣∣{A∈F:x∈A}∣​.

The conjecture says that some xxx has δF(x)≥12\delta_{\mathcal F}(x)\ge\tfrac12δF​(x)≥21​. The challenge scales the bound: for r∈Nr\in\mathbb Nr∈N let UC(r)\mathrm{UC}(r)UC(r) be the statement

every nondegenerate union-closed F has an element x with δF(x) ≥ 12−1r+2.\text{every nondegenerate union-closed } \mathcal F \text{ has an element } x \text{ with } \delta_{\mathcal F}(x)\ \ge\ \frac12-\frac1{r+2}.every nondegenerate union-closed F has an element x with δF​(x) ≥ 21​−r+21​.

The bounds 12−1r+2\tfrac12-\tfrac1{r+2}21​−r+21​ increase to 12\tfrac1221​, so UC(r)\mathrm{UC}(r)UC(r) for all rrr is the full conjecture, and each UC(r)\mathrm{UC}(r)UC(r) follows from the next.

Formalization targets

Goal

every nondegenerate union-closed F has an element x with δF(x) ≥ 12,\text{every nondegenerate union-closed } \mathcal F \text{ has an element } x \text{ with } \delta_{\mathcal F}(x)\ \ge\ \tfrac12,every nondegenerate union-closed F has an element x with δF​(x) ≥ 21​,

the union-closed sets conjecture itself. It is equivalent to UC(r)\mathrm{UC}(r)UC(r) for all rrr: the densities in a fixed finite family F\mathcal FF take finitely many values, so an element of density at least 12−1r+2\tfrac12-\tfrac1{r+2}21​−r+21​ for every rrr is an element of density at least 12\tfrac1221​.

Rungs

UC(0)\mathrm{UC}(0)UC(0) is trivial. UC(r)\mathrm{UC}(r)UC(r) for 1≤r≤61\le r\le 61≤r≤6 follows from the bound 3−52≈0.382\frac{3-\sqrt5}{2}\approx 0.38223−5​​≈0.382, since 12−18=0.375\tfrac12-\tfrac18=0.37521​−81​=0.375. UC(7)\mathrm{UC}(7)UC(7) asks for density 12−19≈0.3889\tfrac12-\tfrac19\approx 0.388921​−91​≈0.3889 and is the first open rung.

Significance

The conjecture is one of the best-known open problems in extremal set theory, with equivalent forms for lattices (every finite lattice has a join-irreducible element in at most half of the elements) and for intersection-closed families. The entropy method of 2022 changed its status from "no constant known" to "within 0.1180.1180.118 of the truth", and the remaining gap is exactly what the rungs r≥7r\ge 7r≥7 measure: the constant 3−52\frac{3-\sqrt5}{2}23−5​​ is the limit of the known method, as shown by examples of Sawin and others, so UC(7)\mathrm{UC}(7)UC(7) needs a new idea.

Formalizing the entropy argument is a self-contained project: Gilmer's proof is a few pages of entropy inequalities on top of Mathlib's probability and information theory, and the 3−52\frac{3-\sqrt5}{2}23−5​​ refinement adds one optimisation. Neither has a machine-checked proof in Mathlib. The rungs r≤6r\le 6r≤6 would follow; the rungs r≥7r\ge 7r≥7 and the goal are open.

Difficulty

The entropy argument bounds the density of the best element through the entropy of a random union A∪BA\cup BA∪B of two independent random members; the constant 3−52\frac{3-\sqrt5}{2}23−5​​ is where this inequality becomes tight, and the "approximate" families constructed by Sawin and by Chase and Lovett show that the one-step entropy method cannot pass it. Elementary approaches (induction on ∣U∣|U|∣U∣ or ∣F∣|\mathcal F|∣F∣, averaging over pairs) are known to fail even for a constant bound. The naive idea, that the most frequent element of the largest set works, is false.

Formalization scope

Families are Finset (Finset U) for a type U with decidable equality, in an arbitrary universe. IsUnionClosed F says A∪B∈FA\cup B\in FA∪B∈F for all A,B∈FA,B\in FA,B∈F; occurrences F x counts the members containing xxx; density F x : ℚ is occurrences F x / max 1 F.card, so the division is by ∣F∣|F|∣F∣ when FFF is nonempty and by 111 otherwise; Nondegenerate F is F≠∅∧F≠{∅}F\ne\emptyset\wedge F\ne\{\emptyset\}F=∅∧F={∅}. The rung statement_09 r states that for every union-closed nondegenerate FFF there is an element xxx of U with density F x ≥ 1/2 - 1/((r : ℚ) + 2) in the rationals. The goal states the conjecture directly, ∃ x, density F x ≥ 1/2 for every union-closed nondegenerate F; it is equivalent to ∀ r, statement_09 r, the universal form of the benchmark.

No trivialising reading: nondegeneracy excludes exactly the two families for which the conjecture fails, the density is a genuine quotient for nonempty FFF, and an empty type U admits no nondegenerate family. The Lean definitions are copied verbatim from the Ten Challenges repository. Because the definitions are identical, a proof of the goal or of any rung produced here can also be submitted on the Ten Challenges website, https://tenchallenges.github.io/ten-challenges/, which checks submissions automatically against the same statements and records accepted ones on its public leaderboard; contributors are welcome to do both. Contributions welcome: the equivalence of density with the real-valued density of the Mathlib archive, monotonicity of the rungs in rrr, the trivial rung r=0r=0r=0, the singleton and power-set special cases, and a formalization of the entropy bound giving the rungs r≤6r\le 6r≤6.

Selected references

  • Ten Challenges website: problem statements, automatic checker and leaderboard. https://tenchallenges.github.io/ten-challenges/
  • V. Bajpai, N. Bowler, J. Carmesin, U. Okur, 10 Scalable Challenges in Combinatorics: A Public Benchmark Formalised in Lean, AI4Math workshop at CICM 2026. https://cicm-conference.org/2026/ai4math/04-okur.pdf — Lean sources: https://github.com/TenChallenges/ten-challenges (challenge 9).
  • H. Bruhn, O. Schaudt, The journey of the union-closed sets conjecture, Graphs Combin. 31 (2015), 2043–2074. https://doi.org/10.1007/s00373-014-1515-0
  • E. Knill, Graph generated union-closed families of sets, 1994. https://arxiv.org/abs/math/9409215
  • J. Gilmer, A constant lower bound for the union-closed sets conjecture, 2022. https://arxiv.org/abs/2211.09055
  • Z. Chase, S. Lovett, Approximate union closed conjecture, 2022. https://arxiv.org/abs/2211.11689
  • W. Sawin, An improved lower bound for the union-closed set conjecture, 2022. https://arxiv.org/abs/2211.11504
  • R. Alweiss, B. Huang, M. Sellke, Improved lower bound for the union-closed sets conjecture, 2022. https://arxiv.org/abs/2211.11731
  • L. Pebody, Extension of a method of Gilmer, 2022. https://arxiv.org/abs/2211.13139
  • J. Liu, Improving the lower bound for the union-closed sets conjecture via conditionally IID coupling, 2023. https://arxiv.org/abs/2306.08824
  • N. Nagel, Notes on the union closed sets conjecture, 2023. https://arxiv.org/abs/2208.03803
6 thms1 active userReviewed
CombinatoricsGraph TheoryMathematical Logic·Captain: utkuokur

Ten Challenges 10: Unfriendly partition conjectureOpen Problem

Motivation

A partition of the vertices of a graph into two classes is unfriendly if every vertex has at least as many neighbours in the other class as in its own. Every finite graph has one: a partition with the maximum number of crossing edges. For infinite graphs the question is the unfriendly partition conjecture of Cowan and Emerson: does every countable graph have an unfriendly partition? Shelah and Milner showed that uncountable graphs need not, and the countable case has been open since the 1980s, with positive answers for locally finite graphs, graphs with finitely many vertices of infinite degree, and rayless graphs (Aharoni–Milner–Prikry 1990, Shelah–Milner 1990, Bruhn–Diestel–Georgakopoulos–Sprüssel 2010).

This challenge scales the conjecture through a game. The parameter is an ordinal rrr, the clock: Challenger repeatedly names a vertex and lowers the clock, and Partitioner must extend a finite partial partition so that the named vertex becomes unfriendly. An unfriendly partition of the whole graph gives Partitioner a winning strategy for every clock, so the full conjecture implies every rung, and the rungs with transfinite clocks measure how much of an unfriendly partition can be built on demand.

Timeline.

  • 1980s — Cowan and Emerson pose the conjecture.
  • 1990 — Aharoni, Milner and Prikry prove it for graphs with only finitely many vertices of infinite degree, in particular for locally finite graphs (Aharoni–Milner–Prikry 1990).
  • 1990 — Shelah and Milner construct uncountable graphs without unfriendly partitions (Shelah–Milner 1990).
  • 2010 — Bruhn, Diestel, Georgakopoulos and Sprüssel prove it for rayless graphs of any cardinality (Bruhn–Diestel–Georgakopoulos–Sprüssel 2010).
  • 2017 — Berger proves it for graphs containing no subdivision of an infinite clique (Berger 2017).

Setting

Let GGG be a graph with vertex set VVV. A partial partition is a partial function f ⁣:V⇀{0,1}f\colon V\rightharpoonup\{0,1\}f:V⇀{0,1}; it is finite if its domain is finite, and a partition if it is total. Write N(v)N(v)N(v) for the neighbourhood of vvv. A partial partition fff is unfriendly at vvv if f(v)f(v)f(v) is defined and

∣N(v)∩f−1[1−f(v)]∣ ≥ ∣N(v)∩f−1[f(v)]∣,\big|N(v)\cap f^{-1}[1-f(v)]\big|\ \ge\ \big|N(v)\cap f^{-1}[f(v)]\big|,​N(v)∩f−1[1−f(v)]​ ≥ ​N(v)∩f−1[f(v)]​,

as cardinal numbers; neighbours outside the domain of fff are not counted. A partition is unfriendly if it is unfriendly at every vertex.

The rrr-partitioning game. For an ordinal rrr, a position is a pair (f,α)(f,\alpha)(f,α) of a partial partition and an ordinal, the initial position is (∅,r)(\emptyset,r)(∅,r). In each turn from (f,α)(f,\alpha)(f,α), Challenger names a vertex vvv and an ordinal β<α\beta<\alphaβ<α; Partitioner must answer with a finite partial partition ggg extending fff (preserving all assignments of fff) that is unfriendly at vvv; the new position is (g,β)(g,\beta)(g,β). A player unable to move loses; since ordinals have no infinite descending sequences, the game ends after finitely many turns, and Partitioner wins if Challenger runs out of moves. For an ordinal rrr let

UP(r):Partitioner has a winning strategy in the r-partitioning game on every countable graph.\mathrm{UP}(r):\quad \text{Partitioner has a winning strategy in the } r\text{-partitioning game on every countable graph.}UP(r):Partitioner has a winning strategy in the r-partitioning game on every countable graph.

Formalization targets

Goal

every countable graph has an unfriendly partition,\text{every countable graph has an unfriendly partition,}every countable graph has an unfriendly partition,

the unfriendly partition conjecture of Cowan and Emerson. A partial partition that is unfriendly at every vertex is total, so the goal is stated with the same notion of unfriendliness as the game.

The scaled form

∀r∈Ord:UP(r),\forall r\in\mathrm{Ord}:\quad \mathrm{UP}(r),∀r∈Ord:UP(r),

Partitioner wins the rrr-partitioning game on every countable graph for every ordinal clock. An unfriendly partition yields a winning strategy for every clock, so the goal implies the scaled form; the rungs are the scaled form for particular clocks and particular classes of graphs.

Rungs

Any graph with an unfriendly partition yields a winning strategy for every clock: Partitioner reveals the partition on a finite set containing the named vertex and the finitely many coloured neighbours needed. Hence every finite graph, every countable locally finite graph, and every countable rayless graph satisfies all rungs. For finite clocks r=nr=nr=n the statement is an exercise; the rung r=ωr=\omegar=ω is the first with an infinite clock.

Significance

The unfriendly partition conjecture is the basic open question about majority colourings of infinite graphs, and its scaled form isolates how the difficulty grows with the "transfinite length" of the commitment required: with clock ω\omegaω, Challenger must announce in advance how many more vertices will be challenged, with clock ω⋅2\omega\cdot 2ω⋅2 once more, and so on. The full statement is implied by the conjecture; how much of the conjecture the game recovers in return is part of what the scaled version is designed to probe.

Nothing about unfriendly partitions is formalized; Mathlib has simple graphs on arbitrary types and cardinals, but neither majority conditions nor the compactness argument for locally finite graphs. The finite-clock rungs, the finite-graph case and the locally finite case are reachable formalization projects; the infinite-clock rungs are open.

Difficulty

The max-cut argument of the finite case has no infinite analogue: a vertex of infinite degree can be unfriendly only through a cardinality comparison, and attempts to build a partition by transfinite induction run into vertices whose status is changed by later decisions. The known positive results use a careful ordering of the vertices of infinite degree or a structural decomposition (rayless graphs); none of them gives any information about graphs with infinitely many vertices of infinite degree and infinite paths. In the game, the naive strategy of colouring only the challenged vertex fails because Challenger can later challenge a coloured vertex all of whose finitely many neighbours have already been coloured badly.

Formalization scope

Graphs are Mathlib's SimpleGraph V with V in a universe u and the hypothesis Countable V; partial partitions are functions V → Option Bool, with none for undefined and some b for class bbb. NeighColored G f v b is the type of neighbours of vvv with value bbb, and UnfriendlyAt G f v requires some b with f v = some b and the cardinal inequality #(neighbours coloured b) ≤ #(neighbours coloured !b) (Mathlib's Cardinal.mk). emptyPartition V is the constant none; HasFiniteDomain, Extends and IsLegalResponse G f g v (extends, finite domain, unfriendly at vvv) are as in the Setting. PartitionerWins G f α is defined by well-founded recursion on the ordinal α : Ordinal.{v}: for every vertex vvv and every β<α\beta<\alphaβ<α there is a legal response ggg with PartitionerWins G g β. The rung statement_10 r is PartitionerWins G (emptyPartition V) r for every countable V and every G; the scaled form is ∀ r, statement_10 r. The goal is ∃ f : V → Option Bool, ∀ v, UnfriendlyAt G f v for every countable V and every G: since UnfriendlyAt requires f v to be defined, such an f assigns a class to every vertex and is an unfriendly partition in the usual sense.

No trivialising reading: with clock 000 Partitioner wins vacuously, which is the intended base case; responses must be finite, so Partitioner cannot reveal a whole infinite partition at once; and the cardinal comparison is exactly the majority condition on coloured neighbours. The universes of V and of the ordinal are independent parameters. The Lean definitions are copied verbatim from the Ten Challenges repository. Because the definitions are identical, a proof of the goal or of any rung produced here can also be submitted on the Ten Challenges website, https://tenchallenges.github.io/ten-challenges/, which checks submissions automatically against the same statements and records accepted ones on its public leaderboard; contributors are welcome to do both. Contributions welcome: the lemma that an unfriendly partition yields PartitionerWins for every clock, monotonicity of PartitionerWins in the clock, the finite-graph and locally finite cases, the finite-clock rungs, and the relation between winning for all countable clocks and the existence of an unfriendly partition.

Selected references

  • Ten Challenges website: problem statements, automatic checker and leaderboard. https://tenchallenges.github.io/ten-challenges/
  • V. Bajpai, N. Bowler, J. Carmesin, U. Okur, 10 Scalable Challenges in Combinatorics: A Public Benchmark Formalised in Lean, AI4Math workshop at CICM 2026. https://cicm-conference.org/2026/ai4math/04-okur.pdf — Lean sources: https://github.com/TenChallenges/ten-challenges (challenge 10).
  • R. Aharoni, E. C. Milner, K. Prikry, Unfriendly partitions of a graph, J. Combin. Theory Ser. B 50 (1990), 1–10. https://doi.org/10.1016/0095-8956(90)90092-E
  • S. Shelah, E. C. Milner, Graphs with no unfriendly partitions, in: A Tribute to Paul Erdős, Cambridge University Press, 1990, 373–384.
  • H. Bruhn, R. Diestel, A. Georgakopoulos, P. Sprüssel, Every rayless graph has an unfriendly partition, Combinatorica 30 (2010), 521–532. https://doi.org/10.1007/s00493-010-2590-3
  • E. Berger, Unfriendly partitions for graphs not containing a subdivision of an infinite clique, Combinatorica 37 (2017), 157–166. https://doi.org/10.1007/s00493-015-3261-1
  • R. Diestel, Graph Theory, 5th ed., Springer, 2017, Chapter 8. https://doi.org/10.1007/978-3-662-53622-3
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Functional AnalysisMathematical LogicTopology·Captain: username

Comparisons of benchmark equivalence relationsOpen Problem

Comparing the complexity of classification problems

A classification assigns invariants to objects so that two objects receive the same invariant exactly when they are equivalent. Requiring this assignment to be Borel measurable makes it possible to compare classification problems without choosing arbitrary representatives. Borel reducibility expresses this comparison: a relation EEE reduces to a relation FFF when a single Borel map preserves and reflects equivalence for every pair of inputs. Su Gao's Invariant Descriptive Set Theory, Section 15.2 and Figure 15.1, collects benchmark relations that separate several levels of classification complexity.

This mission concerns the comparisons asserted in Section 1 of Ruijun Wang's supplied manuscript Comparisons of benchmark equivalence relations. The manuscript is the source of the proposed new results. Its claims and the completeness of their Lean proofs must be distinguished: some earlier sequence-space results have accepted proofs, while the added countable-relation, jump, and operator comparisons remain formalization targets. The requested category is OpenProblem; here the outstanding tasks concern complete formal proofs of the stated manuscript results. Source and upload files are intended for the Benchmark repository.

The spaces and relations

Let X=RNX=\mathbb R^{\mathbb N}X=RN have the product Borel structure. Its elements are arbitrary real sequences. For a finite real exponent p≥1p\geq1p≥1, the relation ℓp\ell_pℓp​ identifies x,y∈Xx,y\in Xx,y∈X when ∑n∣xn−yn∣p\sum_n|x_n-y_n|^p∑n​∣xn​−yn​∣p is finite. The relation c0c_0c0​ identifies them when xn−yn→0x_n-y_n\to0xn​−yn​→0, and ℓ∞\ell_\inftyℓ∞​ identifies them when sup⁡n∣xn−yn∣\sup_n|x_n-y_n|supn​∣xn​−yn​∣ is finite. No boundedness or convergence condition is imposed on either input separately.

For a relation EEE on a space YYY, its countable product EωE^\omegaEω compares two sequences coordinate by coordinate. Its Friedman–Stanley jump E+E^+E+ compares the sets of EEE-classes represented by their coordinates: every coordinate of either sequence must be EEE-equivalent to some coordinate of the other sequence. Repetitions and ordering do not matter, and the witnessing matches need not form a bijection of indices.

The benchmark E∞E_\inftyE∞​ is presented by the full shift of the free group F2\mathbb F_2F2​ on 2F22^{\mathbb F_2}2F2​. Thus x E∞ yx\,E_\infty\,yxE∞​y means y(h)=x(g−1h)y(h)=x(g^{-1}h)y(h)=x(g−1h) for some g∈F2g\in\mathbb F_2g∈F2​ and every h∈F2h\in\mathbb F_2h∈F2​. The presentation includes points with nontrivial stabilizers. The relation ≡m\equiv_m≡m​ is mutual absolute continuity of Borel probability measures on Cantor space 2N2^{\mathbb N}2N, with the usual evaluation sigma-algebra on probabilities.

The operator and representation targets use the fixed complex Hilbert space H=ℓ2(N;C)\mathcal H=\ell^2(\mathbb N;\mathbb C)H=ℓ2(N;C). All bounded linear operators on H\mathcal HH are allowed. Representations are all unitary representations on this space, including reducible representations. Their Borel structures come from convergence on every vector, and, for representations, at every group element. The representation notation ≈Γ+\approx_\Gamma^+≈Γ+​ follows the manuscript; this superscript denotes arbitrary representations rather than the jump operation above.

The formalization targets

The goal is the conjunction of the six main comparisons in the introduction. Each component is also a named milestone:

  1. E∞ω≤Bc0E_\infty^\omega\leq_B c_0E∞ω​≤B​c0​, and E∞⊥BℓpE_\infty\perp_B\ell_pE∞​⊥B​ℓp​ for every finite real p≥1p\geq1p≥1.
  2. For every 1≤p≤∞1\leq p\leq\infty1≤p≤∞, ℓp≤B≡m\ell_p\leq_B\equiv_mℓp​≤B​≡m​ if and only if p≤2p\leq2p≤2.
  3. c0̸≤B≡mc_0\not\leq_B\equiv_mc0​≤B​≡m​.
  4. c0̸≤Bℓ∞+c_0\not\leq_B\ell_\infty^+c0​≤B​ℓ∞+​ and ≡m̸≤Bℓ∞+\equiv_m\not\leq_B\ell_\infty^+≡m​≤B​ℓ∞+​.
  5. ≡m<B≃u\equiv_m<_B\simeq_u≡m​<B​≃u​, where ≃u\simeq_u≃u​ is unitary equivalence of bounded operators.
  6. ≈Z+∼B≡m<B≈F∞+∼B≃u\approx_{\mathbb Z}^+\sim_B\equiv_m<_B\approx_{F_\infty}^+\sim_B\simeq_u≈Z+​∼B​≡m​<B​≈F∞​+​∼B​≃u​.

The symbol ⊥B\perp_B⊥B​ requires both nonreductions; <B<_B<B​ requires a reduction in the forward direction and a nonreduction in the reverse direction. Significant established comparisons are retained as literature milestones, including the classical positive range 1≤p≤21\leq p\leq21≤p≤2 and Thomas's nonreduction E∞̸≤Bℓ2E_\infty\not\leq_B\ell_2E∞​≤B​ℓ2​.

History and mathematical significance

  • 1948: Kakutani established the equivalence criterion for infinite product measures that underlies the classical positive measure coding.
  • 1999: Dougherty and Hjorth determined the reducibility hierarchy of the finite-exponent sequence relations.
  • 2006: Gao surveyed the Banach-space benchmarks, posed related questions, and recorded (c0)ω∼Bc0(c_0)^\omega\sim_B c_0(c0​)ω∼B​c0​ in Lemma 7.3. Kanovei's Question 4.7 asks about reductions of E∞E_\inftyE∞​ to c0c_0c0​ and finite-exponent sequence relations.
  • 2009: Gao's monograph organized the benchmark diagram and recorded unresolved comparisons at that time.
  • 2014–2015: Ding and Gao, page 735, and Thomas, Question 8.2, posed the operator and arbitrary-representation comparisons. Thomas's Theorem 6.12 already proves E∞̸≤Bℓ2E_\infty\not\leq_B\ell_2E∞​≤B​ℓ2​; this part is an established input, not a new claim of the supplied manuscript.
  • 2026: The supplied manuscript asserts the six displayed results. Previously submitted finite-exponent threshold and null-sequence nonreduction proofs have status Proved on Prove2Me. The remaining components require their own complete proofs and verdicts.

The comparisons describe which benchmark classifications admit invariants of another specified kind. The operator result, if fully formalized, rules out scalar measure classes as Borel complete invariants for arbitrary bounded operators. It makes no claim against other kinds of spectral analysis or operator-valued invariants. Formalization must establish the comparisons themselves, rather than infer them from a shared Borel complexity bound.

What makes the formal proofs difficult

A nonreduction quantifies over every Borel map. Checking a coordinate formula, a continuous family, or a finite collection of inputs cannot establish it. The countable-relation result requires the descriptive and analytic infrastructure connecting its source action to sequence-space equivalence. The jump assertions require control of arbitrary countable sets of target classes. The operator comparisons additionally require measurability, exact preservation and reflection of equivalence, and transport to the fixed Hilbert space. Each of these requirements is part of the target, even when supporting theory is absent from Mathlib.

Formalization scope and checked evidence

The common definitions use actual free groups, actual real sequences, real powers, convergence, probability measures, bounded complex-linear maps, and surjective complex-linear isometries. An infinite exponent is represented by the top element of WithTop applied to the reals; its relation is bounded difference. Measurable structures for operators and representations are specified explicitly to avoid accidental use of a stronger operator topology.

The target environment is Lean 4.30.0 with supported Mathlib revision c5ea00351c28e24afc9f0f84379aa41082b1188f. Exact definition and statement files are compiled locally before upload. A compiling open statement is an elaboration check, not a proof. Completed solutions must contain no proof placeholders or additional mathematical axioms. In particular, assuming a reduction, a rigidity conclusion, a local-row property, or a classification theorem that the argument is meant to establish does not complete the corresponding headline result.

The existing accepted theorem identities are reused where they already express the intended result. Reusable work includes Hellinger affinity, absolute continuity, probability kernels, compact quotient obstructions, sequence codings, unitary representations, countable-row arguments, and operator intertwiners. Further contributions should preserve the exact quantifiers, endpoint cases, and source and target Borel structures.

Selected references

  • S. Kakutani, On equivalence of infinite product measures, Annals of Mathematics 49 (1948), 214–224. DOI.
  • R. Dougherty and G. Hjorth, Reducibility and nonreducibility between ℓp\ell^pℓp equivalence relations, Transactions of the AMS 351 (1999), 1835–1844. DOI.
  • S. Gao, Equivalence relations and classical Banach spaces, Mathematical Logic in Asia (2006), 70–89. DOI.
  • V. Kanovei, Varia: Ideals and Equivalence Relations, beta version (2006), Question 4.7. arXiv.
  • S. Gao, Invariant Descriptive Set Theory, Chapman & Hall/CRC (2009), Sections 8.5 and 15.2. DOI.
  • L. Ding and S. Gao, Is there a spectral theory for all bounded linear operators?, Notices of the AMS 61 (2014), 730–735. DOI.
  • S. Thomas, A descriptive view of unitary group representations, Journal of the EMS 17 (2015), 1761–1787. Publisher text.
  • R. Wang, Comparisons of benchmark equivalence relations, supplied Benchmark.tex, Section 1, Theorems 1.1–1.6. Repository designated for sources.
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Mathematical LogicModel Theory·Captain: username

Friedman Stanley cofinality without Borel completenessOpen Problem

Motivation and historical context

Classification of countable structures asks whether objects have the same structure and whether one problem can supply definable invariants for another. Borel reducibility makes this comparison precise: a Borel map must preserve and reflect isomorphism. A class is Borel complete when every countable-structure isomorphism problem reduces to it. Friedman and Stanley introduced a hierarchy of bounded-rank tree problems and asked whether receiving every countable level already forces completeness. The question is stated in their original paper, page 899. Friedman–Stanley, 1989.

The relevant chronology distinguishes that general question from particular examples:

  • 1989: Friedman and Stanley develop Borel comparison of countable structures, establish their tree hierarchy, and ask whether completeness for all countable ranks implies Borel completeness. Original article, pages 899–902.
  • 2019: Shelah and Ulrich restate the question for infinitary sentences. Their Theorem 1.2 recalls Hjorth's result that every countable Friedman–Stanley level reduces to torsion-free abelian group isomorphism. Shelah–Ulrich, page 276.
  • 2024: Paolini and Shelah prove torsion-free abelian groups Borel complete. This settles that particular group example, while the general implication concerns arbitrary invariant Borel classes. Annals of Mathematics.
  • 2024: Shani studies the finite and omega Friedman–Stanley jumps through Borel homomorphism dichotomies. The supplied manuscript distinguishes these published levels from its proposed construction at arbitrary countable ordinals. arXiv:2405.18360.
  • 2 November 2026: the supplied research draft proposes a counterexample to the general implication. It reports internal checking only, with no claim of independent mathematical verification.

Setting

A countable relational language has at most countably many symbols, each with finite arity. A structure on the natural numbers assigns a truth value to each symbol and each tuple of the appropriate length. Nullary symbols are allowed. The resulting countable product of two-point spaces has its canonical Borel sigma algebra. Two structures are isomorphic when a single permutation of the natural numbers preserves all relation values.

An invariant Borel class is a Borel subset of that structure space closed under isomorphism. Borelness of the class does not assert Borelness of its isomorphism relation. Graphs are simple undirected graphs on the fixed vertex set of natural numbers.

For relations EEE and FFF, the notation E≤BFE\leq_B FE≤B​F means that some measurable map between their specified Borel code spaces satisfies

E(x,y)⟺F(f(x),f(y))E(x,y)\quad\Longleftrightarrow\quad F(f(x),f(y))E(x,y)⟺F(f(x),f(y))

for every pair of source points. Neither relation is assumed Borel merely by writing this comparison.

The benchmark J0\mathsf J_0J0​ is equality on Cantor space 2N2^{\mathbb N}2N. At successors, Jα+1\mathsf J_{\alpha+1}Jα+1​ compares enumerated countable sets of Jα\mathsf J_\alphaJα​ classes, with a distinct empty-set code; order and repetitions are ignored. At nonzero countable limits, the benchmark is a coordinatewise product along a fixed increasing cofinal sequence of smaller ordinals. Codes remain actual measurable sequence spaces, rather than quotient spaces of invariants.

Formalization targets

The goal is Theorem 1.2 of the supplied manuscript, not Question 1.1, which shares its numbering counter. There should be one fixed countable language LLL and one invariant Borel class K⊆Str⁡L(N)\mathcal K\subseteq\operatorname{Str}_L(\mathbb N)K⊆StrL​(N) such that

∀α<ω1,Jα≤B≅K,≅Graph̸≤B≅K,\forall\alpha<\omega_1,\qquad \mathsf J_\alpha\leq_B\cong_{\mathcal K}, \qquad \cong_{\mathrm{Graph}}\not\leq_B\cong_{\mathcal K},∀α<ω1​,Jα​≤B​≅K​,≅Graph​≤B​≅K​,

and, including the theorem's additional conclusion,

∀ 0<α<ω1,≅Tα≤B≅K.\forall\,0<\alpha<\omega_1,\qquad \cong_{\mathfrak T_\alpha}\leq_B\cong_{\mathcal K}.∀0<α<ω1​,≅Tα​​≤B​≅K​.

Here Tα\mathfrak T_\alphaTα​ denotes bounded-rank rooted well-founded tree codes, including finite and empty trees. The manuscript compares its product-limit benchmarks with the usual hierarchy conventions in Proposition 4.13 and with the original tree hierarchy in Proposition 4.15. No identification of ordinal indices between different presentations is asserted.

The milestones retain the source's attack path: the classical Borelness of bounded-rank tree isomorphism from Friedman–Stanley Section 1.2.1; Proposition 3.6 on invariant real-valued graph parameters; Theorem 4.1 on cofinality of Polishable subgroup coset relations; and Proposition 4.15 comparing the original tree hierarchy with the product-limit tower. The first is published background; the other three are targets from the proposed research draft.

Significance and current status

The target distinguishes being above every countable benchmark from being universal for all countable-structure classification problems. In the source's sentence formulation, it would give a negative answer to the question restated by Shelah and Ulrich. The structure-class formulation is the goal here; the infinitary-sentence corollary and the appendix's forcing and thickness claims are outside this mission.

The requested formalization is open. Local compilation validates the definitions and theorem interfaces, with explicit open-target placeholders; it does not verify the proposed mathematical proof. A completed development would provide reusable code-space constructions, ordinal-indexed comparison relations, bounded-tree interfaces, and permutation-group coset machinery.

Central difficulty

The quantifier ranges over every countable ordinal, while the language and target class must remain fixed. Results restricted to finitely many jumps, or even to the omega level, do not settle this claim. The distinction between countable sets and countable multisets is also substantive: the original tree codes retain multiplicities, while the set jump forgets them. Friedman–Stanley, Section 1.2.

The class of structures must itself be Borel and invariant. Replacing that requirement by Borelness of its isomorphism graph changes the problem. Individual reductions may depend on the ordinal; the theorem does not require a single Borel selection of reductions over all codes for countable well-orders.

Formalization scope

The Lean language bundle represents actual relational structures on N\mathbb NN by Boolean truth tables. The source allows functions and constants to be represented by relations; no structural axioms are imposed on the ambient space. A proposed target class must supply its own Borelness and invariance. Empty languages and empty classes are admitted by the interfaces, and no nontriviality is hidden in those definitions.

The tower uses native ordinal recursion below ω1\omega_1ω1​, equality on Cantor space, option-valued sequence codes for the set jump, and dependent countable products at limits. Fundamental sequences are fixed once; their strict increase and cofinality in the countable range are proved in the definition layer. This commits to the manuscript's product-limit presentation.

Tree codes are prefix-closed subsets of finite natural-number sequences. Isomorphisms are actual node bijections preserving and reflecting immediate parenthood. A global bound is expressed by an ordinal ranking into the bound, strictly decreasing along children; the empty tree has height zero and a single vertex height one. This specifies reverse-tree height explicitly and does not conflate the original convention with the separate leaf-zero padding convention. Finite and infinite branch multiplicities are retained.

The coset interface uses the actual group of permutations of N\mathbb NN with its standard Polish topology and the source convention pEHq  ⟺  q−1p∈HpE_Hq\iff q^{-1}p\in HpEH​q⟺q−1p∈H. No normality or closedness of the image subgroup is assumed. Contributions developing the ordinal, measurable-space, tree, and topological-group prerequisites are welcome.

Selected references

  • Friedman–Stanley cofinality and Borel completeness: A proposed negative answer to the Friedman–Stanley question, supplied research draft dated 2 November 2026, FriedmanStanleyQuestion.tex, Theorem 1.2; Proposition 3.6; Theorem 4.1; Propositions 4.13 and 4.15. Author field empty; no public manuscript URL supplied.
  • H. Friedman and L. Stanley, A Borel reducibility theory for classes of countable structures, Journal of Symbolic Logic 54 (1989), 894–914. DOI.
  • S. Shelah and D. Ulrich, Torsion-free abelian groups are consistently aΔ21\mathrm a\Delta^1_2aΔ21​-complete, Fundamenta Mathematicae 247 (2019), 275–297. Author-hosted paper.
  • G. Paolini and S. Shelah, Torsion-free abelian groups are Borel complete, Annals of Mathematics 199 (2024), 1177–1224. DOI.
  • A. Shani, The finite Friedman–Stanley jumps: generic dichotomies for Borel homomorphisms, 2024. arXiv:2405.18360.
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Mathematical LogicTopology·Captain: username

No Borel upper bound for the FσF_\sigmaFσ​ equivalence relationsOpen Problem

Motivation and historical context

Borel reducibility compares classification problems by asking whether one can assign invariants for one problem using the equivalence classes of another. The comparison is sensitive to the definability of the assignment: the coding map must be Borel measurable and must preserve and reflect equivalence. It is a standard organizing principle in invariant descriptive set theory, where the objects being classified often live in Polish spaces. Marker's course notes introduce this perspective and the underlying descriptive set theory.

An upper bound for a family of equivalence relations is a single relation receiving a Borel reduction from every member of that family. The distinction between countable unions of compact sets and countable unions of closed sets is essential here. Rosendal's work established universal behavior for the more restrictive compact-union setting. The present target asks how far the closed-union class can be bounded when the target may have arbitrary Borel complexity. Rosendal, 2005.

The relevant chronology is:

  • 2002: Marker's notes present standard Borel spaces, analytic sets, and the non-Borel set of ill-founded trees, providing classical background for the source note. Course notes, Sections 4–5.
  • 2005: Rosendal studies cofinal families and universal examples for Borel reducibility, including the compact-union setting. Journal of Symbolic Logic 70, 1325–1340.
  • 22 October 2026: Wang's preprint states that every equivalence relation with an FσF_\sigmaFσ​ graph is escaped by an FσF_\sigmaFσ​ real linear coset relation on ℓ2\ell_2ℓ2​, even for Baire-measurable reductions. The corresponding public theorem on Prove2Me is already marked Proved and is included as a reference milestone. arXiv:2610.31052.
  • 1 November 2026: the supplied research proof note, No Borel upper bound for the FσF_\sigmaFσ​ equivalence relations, states the stronger Theorem 1 targeted here. Its author field is empty and its provenance does not claim external peer review. The open work in this mission is formalization of that stated result.

Setting

A Polish space is a topological space admitting a complete compatible metric and a countable dense subset. An FσF_\sigmaFσ​ set is a countable union of closed sets. A binary relation has an FσF_\sigmaFσ​ graph when its set of related pairs is FσF_\sigmaFσ​ in the product topology. A Borel equivalence relation is an equivalence relation whose graph belongs to the Borel sigma algebra generated by that product topology.

For equivalence relations EEE on XXX and FFF on YYY, write E≤BFE\leq_B FE≤B​F if there is a Borel measurable map f:X→Yf:X\to Yf:X→Y satisfying

∀x,x′∈X,E(x,x′)  ⟺  F(f(x),f(x′)).\forall x,x'\in X,\qquad E(x,x')\iff F(f(x),f(x')).∀x,x′∈X,E(x,x′)⟺F(f(x),f(x′)).

The domain and target sigma algebras are the Borel sigma algebras of the specified topologies. All Polish source spaces are admitted, including spaces that are neither compact nor sigma-compact.

For a subgroup HHH of a group GGG, the coset relation is gEHGg′gE_H^Gg'gEHG​g′ exactly when g−1g′∈Hg^{-1}g'\in Hg−1g′∈H, with classes gHgHgH. The subgroup need not be normal. For a real linear subspace, the additive convention is xEHyxE_HyxEH​y exactly when y−x∈Hy-x\in Hy−x∈H.

Formalization targets

The main target is precisely Theorem 1 of the supplied note:

¬∃(Y,F)[Y Polish, F a Borel equivalence relation on Y, ∀(X,E) (E an Fσ equivalence relation on Polish X⇒E≤BF)].\neg\exists(Y,F)\quad \bigl[Y\text{ Polish},\ F\text{ a Borel equivalence relation on }Y, \ \forall(X,E)\ (E\text{ an }F_\sigma\text{ equivalence relation on Polish }X \Rightarrow E\leq_B F)\bigr].¬∃(Y,F)[Y Polish, F a Borel equivalence relation on Y, ∀(X,E) (E an Fσ​ equivalence relation on Polish X⇒E≤B​F)].

In Lean the assertion is stated for every Polish target YYY. The target graph may belong to any Borel level.

Two new supporting milestones retain the source numbering. Lemma 2 is the category-transfer statement: for standard-Borel parameters and countably many jointly Borel families of continuous group homomorphisms, a common Borel upper bound for the coset relations outside a generated-subgroup membership set forces that membership set to be Borel. Corollary 4 states that the counterexamples can be coset relations of FσF_\sigmaFσ​ real linear subspaces in one fixed real ℓ1\ell_1ℓ1​. The earlier FσF_\sigmaFσ​-target obstruction is a separate, already-published reference milestone.

Significance and current status

The main statement rules out a single Borel classifier for the whole FσF_\sigmaFσ​ class, even when no fixed bound is imposed on the complexity of that classifier's graph. This is stronger than requiring the proposed upper bound itself to have an FσF_\sigmaFσ​ graph. The supplied note also draws consequences for higher levels of the Borel hierarchy; those consequences are outside the present goal.

The formalization would connect topological groups, descriptive set theory and real Banach-space coset relations in a reusable Lean development. The earlier reference result already has an accepted machine-checked proof. The new theorem and its new milestones are open formal statements: successful compilation of their interfaces checks their well-formedness and does not supply their proofs.

Central difficulty

Increasing the permitted complexity of the target changes the problem materially. The earlier theorem's hypothesis on the target graph no longer applies. For the category-transfer milestone, the individual reductions are only assumed to exist; a Borel selection of them is not part of the hypotheses. For the Banach-space milestone, an algebraic linear image need not be closed, and the source imposes injectivity without assuming a closed range or a bounded inverse. These distinctions must survive the formalization.

Formalization scope

The mission reuses the public definitions of FσF_\sigmaFσ​ graphs, Borel maps and relation reductions from the earlier mission. New definitions specify Borel graphs explicitly using borel (X × X), upper bounds over all Polish sources represented in Lean's ordinary type universe, algebraically generated subgroups, and native real lp with exponent 111. Targets are universe-polymorphic. Empty targets and empty Polish source spaces are included.

The category-transfer parameter space carries its given standard Borel structure. Group factors carry their own Polish group topologies; joint measurability uses the product of the parameter sigma algebra and each group's Borel sigma algebra. Generated subgroups are algebraic closures under group operations. No normality, compactness, sigma-compactness or measurable selection hypothesis is added.

The definitions contain no proof placeholders. The three new theorem interfaces deliberately use the platform's open-target placeholder. Contributions proving these targets or developing their measurable-category and Banach-space prerequisites are welcome. Baire-category coding, analytic separation, countable closed covers and the tensor-image analysis are reusable infrastructure needed by a complete development.

Selected references

  • No Borel upper bound for the FσF_\sigmaFσ​ equivalence relations, research proof note dated 1 November 2026, Theorem 1, Lemma 2 and Corollary 4. Supplied manuscript: UniversalBorelEquivalence-20261101.tex; no public manuscript URL was supplied.
  • D. Marker, Descriptive Set Theory, UIC course notes, Fall 2002. Author's PDF.
  • C. Rosendal, Cofinal families of Borel equivalence relations and quasiorders, Journal of Symbolic Logic 70 (2005), 1325–1340. DOI.
  • R. Wang, There is no universal FσF_\sigmaFσ​ equivalence relation, preprint, 22 October 2026. arXiv:2610.31052.
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Complexity TheoryTheoretical Computer Science·Captain: marwahaha

A 2o(n)2^{o(n)}2o(n) Time Algorithm for 3-SAT: Refuting ETHResearch Paper

Motivation

The Exponential Time Hypothesis (ETH) asserts that deciding whether a Boolean formula with at most three literals per clause has a satisfying assignment requires a positive exponential rate in its number of variables. It is a benchmark assumption in computational complexity. The paper A 2o(n)2^{o(n)}2o(n) Time Algorithm for 3-SAT, attributed to Claude (Anthropic), supplies a deterministic counting algorithm and a Lean development establishing a negation of ETH in a precise finite-alphabet machine model. This mission records the two public statements of that development at commit 16a5ce41304fcdaea4e0be7c132e1c361dc26da5.

Formulas, assignments, and machines

A literal is a variable or its negation. A clause is a finite ordered list of literals, interpreted as their disjunction; a CNF formula is a finite ordered list of clauses, interpreted as their conjunction. A satisfying assignment gives a Boolean value to each of the declared variables and makes at least one literal true in every clause. Counting means returning the number of such assignments, among all 2n2^n2n assignments to the nnn declared variables.

A kkk-CNF has at most kkk literals in each clause and no repeated clause as an ordered literal list. Repeated literals within one clause and clauses containing both signs of a variable are allowed. Distinct permutations of a clause can appear as distinct clauses. Empty clauses are allowed and make the formula unsatisfiable. These are the exact conventions of MainResults.lean.

The computation model is Mathlib's deterministic finite-program stack-machine model Turing.FinTM2, with Boolean input and output and an explicit requirement that every stack alphabet be finite. Time is measured by TM2OutputsInTime. Input encodings write the variable count in unary and each literal in a fixed-width binary slot; the counting problem also supplies kkk in unary. Missing literal positions are padded by zero. Outputs are a single decision bit or the exact assignment count in n+1n+1n+1 bits, least significant bit first.

Formalization targets

For a nonnegative rate δ\deltaδ, let InTime⁡(3,δ)\operatorname{InTime}(3,\delta)InTime(3,δ) mean that some machine and natural constant ccc decide every admissible 3-CNF on nnn variables within ⌊c2δn⌋\lfloor c2^{\delta n}\rfloor⌊c2δn⌋ steps. The machine and constant precede the quantification over inputs. Define

s3=inf⁡{δ≥0:InTime⁡(3,δ)}.s_3=\inf\{\delta\ge0:\operatorname{InTime}(3,\delta)\}.s3​=inf{δ≥0:InTime(3,δ)}.

The infimum is taken in the extended nonnegative reals, with the empty infimum equal to infinity. The mission goal is the source theorem MainResults.ethIsFalse:

¬(0<s3),equivalently s3=0.\neg(0<s_3),\qquad\text{equivalently }s_3=0.¬(0<s3​),equivalently s3​=0.

This is an unconditional statement. It does not assert that rate zero is attained, and does not replace a quantified machine with an input-dependent choice. It covers all variable counts and permits unused variables. The definition of ETH and its relationship to the paper's terminology are explained in the source statement file.

The companion milestone is MainResults.mainTheorem, the paper's stronger counting result. There exist one machine and one natural constant CCC, both independent of kkk and the formula, such that every kkk-CNF with k≥1k\ge1k≥1, m≥2m\ge2m≥2 clauses, n≥4n\ge4n≥4 variables, and every variable occurring is counted within

⌊2Cmin⁡{km/log⁡2m,  k2nlog⁡2log⁡2n/log⁡2n}⌋\left\lfloor2^{C\min\{km/\sqrt{\log_2m},\;k^2n\log_2\log_2n/\sqrt{\log_2n}\}}\right\rfloor⌊2Cmin{km/log2​m​,k2nlog2​log2​n/log2​n​}⌋

steps. There is no additional factor outside this exact bound. No guarantee is asserted by this milestone for inputs outside its stated restrictions.

Significance

The ETH target rules out a strictly positive optimal exponential rate for the represented decision problem. The counting target supplies a single uniform algorithm, including its dependence on clause width and both size parameters. The result is asymptotic; neither statement promises a practically useful running time at ordinary input sizes. The repository explicitly makes this distinction in its README.

The source already contains proofs, attributed to AI models by the authors. This mission imports those proofs into a reusable dependency graph. Its public goals remain Open until Prove2me accepts their complete proof dependencies. Creating or approving the mission attests to the statements and scope, not to completion of the proof import. No claim of a new discovery by the mission captain is made.

Difficulty

An asymptotic estimate alone does not establish this result. The development must connect the computation's exact output to a finite machine, control its execution time, and preserve the order of quantifiers needed for uniformity. An input-specific procedure or a cost model that grants unbounded computations as single steps would not meet these targets. The exported statements ultimately measure the named Mathlib machine relation, regardless of intermediate cost abstractions used by the proof.

Formalization scope

The source pins Lean 4.33.1 and Mathlib revision 0df444a360eaa60ab8c11dca51a86af692955474. The shared definition bundle is the source's MainResults.lean, which imports Mathlib alone. The two theorem types are retained exactly. The counting thresholds keep the logarithmic denominators positive; small-input behavior is not silently obtained from totalized division. All machine alphabets are explicitly finite. The public definition of ETH uses the infimum over decision rates and does not hide the desired result as an assumption.

The source comments discuss simulation and input-rewriting arguments relating this machine convention to other standard models. Those explanations are outside these two Lean statements and are not presented here as separately imported theorems. The project's Challenge.lean intentionally contains proof placeholders for comparator checks; those placeholders are excluded from the proof import. The completed import must use the proofs from Solution.lean and preserve the original Apache-2.0 license and attribution notices.

Selected references

  • Claude (Anthropic), A 2o(n)2^{o(n)}2o(n) Time Algorithm for 3-SAT (2026), paper and pinned research artifact.
  • Anthropic, MainResults.lean, exact definitions and propositions; Solution.lean, exported proof terms.
  • Anthropic, PaperIndex.lean, correspondence between paper statements and Lean declarations, including documented differences.
8 thms1 active userReviewed
Dynamic ProgrammingOptimizationProbability+1·Captain: iris

Markov Decision Processes with Applications to Finance X: Terminal Wealth under Partial Observation Is Solved by a Bellman Equation in Wealth and FilterTextbook

Portfolio choice when the market regime is hidden

The distribution of stock returns is not constant: drifts and volatilities change with economic conditions that are not directly observed, and drift parameters in particular are notoriously hard to estimate. A standard way to model this in discrete time is to let the return distribution depend on an unobservable Markov chain, the hidden state or regime, while the investor sees only prices. Chapter 6 of Bäuerle and Rieder's Markov Decision Processes with Applications to Finance (Springer, 2011) treats two classical portfolio problems in this setting, terminal wealth maximization and the dynamic mean–variance problem, by reducing them, through the Bayes filter of Chapter 5, to fully observed Markov Decision Problems whose state is the wealth together with the conditional law of the hidden regime. The book notes that partially observable portfolio problems in discrete time had been sparsely studied, with binomial models with an unknown up-probability (Runggaldier et al. 2002, Favero 2001) and a hidden-Markov model with unknown drift and volatility (Taksar and Zeng 2007) as earlier examples.

Setting

A bond earns the interest rate in+1≥0i_{n+1}\ge0in+1​≥0 in period [n,n+1)[n,n+1)[n,n+1), with price Sn0=∏k≤n(1+ik)S^0_n=\prod_{k\le n}(1+i_k)Sn0​=∏k≤n​(1+ik​). There are ddd stocks with relative risk Rn+1∈RdR_{n+1}\in\mathbb R^dRn+1​∈Rd, every component above −1-1−1. A hidden process (Yn)(Y_n)(Yn​) lives on a standard Borel space EYE_YEY​, and (Rn,Yn)(R_n,Y_n)(Rn​,Yn​) is a Markov process with

P(Rn+1∈B, Yn+1∈C∣Yn=y,Rn)=QR(B∣y) QY(C∣y),\mathbb P(R_{n+1}\in B,\ Y_{n+1}\in C\mid Y_n=y,R_n)=Q^R(B\mid y)\,Q^Y(C\mid y),P(Rn+1​∈B, Yn+1​∈C∣Yn​=y,Rn​)=QR(B∣y)QY(C∣y),

where QRQ^RQR and QYQ^YQY have densities qRq^RqR, qYq^YqY with respect to σ\sigmaσ-finite measures and Y0Y_0Y0​ has the prior Q0Q_0Q0​. The investor's strategy φn\varphi_nφn​ (the amounts in the stocks) may depend only on R1,…,RnR_1,\dots,R_nR1​,…,Rn​; wealth evolves as Xn+1=(1+in+1)(Xn+φn⋅Rn+1)X_{n+1}=(1+i_{n+1})(X_n+\varphi_n\cdot R_{n+1})Xn+1​=(1+in+1​)(Xn​+φn​⋅Rn+1​).

The Bayes operator maps a belief ρ∈P(EY)\rho\in\mathbb P(E_Y)ρ∈P(EY​) and an observed return zzz to

Φ(ρ,z)(C)=∫C∫qR(z∣y)qY(y′∣y)ρ(dy) ν(dy′)∫EY∫qR(z∣y)qY(y′∣y)ρ(dy) ν(dy′),\Phi(\rho,z)(C)=\frac{\int_C\int q^R(z\mid y)q^Y(y'\mid y)\rho(dy)\,\nu(dy')}{\int_{E_Y}\int q^R(z\mid y)q^Y(y'\mid y)\rho(dy)\,\nu(dy')},Φ(ρ,z)(C)=∫EY​​∫qR(z∣y)qY(y′∣y)ρ(dy)ν(dy′)∫C​∫qR(z∣y)qY(y′∣y)ρ(dy)ν(dy′)​,

and the filter is μ0=Q0\mu_0=Q_0μ0​=Q0​, μn+1=Φ(μn,Rn+1)\mu_{n+1}=\Phi(\mu_n,R_{n+1})μn+1​=Φ(μn​,Rn+1​).

In the terminal wealth problem (6.2) the investor has a utility function UUU (strictly increasing, strictly concave, continuous) on dom⁡U=[0,∞)\operatorname{dom}U=[0,\infty)domU=[0,∞) or (0,∞)(0,\infty)(0,∞), a constant rate iii, and maximizes ExU(XN)\mathbb E_xU(X_N)Ex​U(XN​) over adapted strategies with XN∈dom⁡UX_N\in\operatorname{dom}UXN​∈domU almost surely. The admissible investments at wealth xxx are D(x)={a:(1+i)(x+a⋅R(y))∈dom⁡U a.s.}D(x)=\{a:(1+i)(x+a\cdot R(y))\in\operatorname{dom}U\text{ a.s.}\}D(x)={a:(1+i)(x+a⋅R(y))∈domU a.s.}. The filtered model has state (x,ρ)(x,\rho)(x,ρ); from it, zzz is drawn from ∫QR(⋅∣y)ρ(dy)\int Q^R(\cdot\mid y)\rho(dy)∫QR(⋅∣y)ρ(dy) and the state moves to ((1+i)(x+a⋅z),Φ(ρ,z))((1+i)(x+a\cdot z),\Phi(\rho,z))((1+i)(x+a⋅z),Φ(ρ,z)). Its value functions with nnn stages to go are Jn(x,ρ)J_n(x,\rho)Jn​(x,ρ).

Formalization targets

Goal: Theorem 6.1.1

Under the no-arbitrage, common-support and moment assumption (FM), and with D(x)D(x)D(x) independent of the hidden state:

  1. x↦Jn(x,ρ)x\mapsto J_n(x,\rho)x↦Jn​(x,ρ) is finite, strictly increasing, strictly concave and continuous on dom⁡U\operatorname{dom}UdomU;
  2. J0(x,ρ)=U(x)J_0(x,\rho)=U(x)J0​(x,ρ)=U(x) and
Jn(x,ρ)=sup⁡a∈D(x)∫ ⁣ ⁣∫Jn−1((1+i)(x+a⋅z),Φ(ρ,z))QR(dz∣y)ρ(dy);J_n(x,\rho)=\sup_{a\in D(x)}\int\!\!\int J_{n-1}\big((1+i)(x+a\cdot z),\Phi(\rho,z)\big)Q^R(dz\mid y)\rho(dy);Jn​(x,ρ)=a∈D(x)sup​∫∫Jn−1​((1+i)(x+a⋅z),Φ(ρ,z))QR(dz∣y)ρ(dy);
  1. the value of (6.2) from wealth x>0x>0x>0 is JN(x,Q0)J_N(x,Q_0)JN​(x,Q0​);
  2. maximizers fn∗f^*_nfn∗​ of Jn−1J_{n-1}Jn−1​ exist when dom⁡U=[0,∞)\operatorname{dom}U=[0,\infty)domU=[0,∞), D(x)D(x)D(x) is closed, or U′(0+)=∞U'(0+)=\inftyU′(0+)=∞, and for any maximizers fn(hn)=fN−n∗(xn,μn(⋅∣hn))f_n(h_n)=f^*_{N-n}(x_n,\mu_n(\cdot\mid h_n))fn​(hn​)=fN−n∗​(xn​,μn​(⋅∣hn​)) is optimal for (6.2).

Theorem 6.1.2 (power utility)

For U(x)=xγ/γU(x)=x^\gamma/\gammaU(x)=xγ/γ, 0<γ<10<\gamma<10<γ<1: Jn(x,ρ)=(xSn0)γdn(ρ)J_n(x,\rho)=(xS^0_n)^\gamma d_n(\rho)Jn​(x,ρ)=(xSn0​)γdn​(ρ) with d0≡1/γd_0\equiv1/\gammad0​≡1/γ and

dn(ρ)=sup⁡α∈A~∫ ⁣ ⁣∫dn−1(Φ(ρ,z))(1+α⋅z)γQR(dz∣y)ρ(dy),d_n(\rho)=\sup_{\alpha\in\tilde A}\int\!\!\int d_{n-1}(\Phi(\rho,z))(1+\alpha\cdot z)^\gamma Q^R(dz\mid y)\rho(dy),dn​(ρ)=α∈A~sup​∫∫dn−1​(Φ(ρ,z))(1+α⋅z)γQR(dz∣y)ρ(dy),

and the optimal amounts are αn∗(ρ)x\alpha^*_n(\rho)xαn∗​(ρ)x.

Theorem 6.2.3 (mean–variance)

For Var⁡(XN)→min⁡\operatorname{Var}(X_N)\to\minVar(XN​)→min subject to EXN≥μ\mathbb E X_N\ge\muEXN​≥μ, with x0SN0<μx_0S^0_N<\mux0​SN0​<μ: the strategy fn∗(x,ρ)=(μ−d0(Q0)x0SN01−d0(Q0)Sn0SN0−x)Cn+1−1(ρ)ℓn+1(ρ)f^*_n(x,\rho)=\big(\tfrac{\mu-d_0(Q_0)x_0S^0_N}{1-d_0(Q_0)}\tfrac{S^0_n}{S^0_N}-x\big)C^{-1}_{n+1}(\rho)\ell_{n+1}(\rho)fn∗​(x,ρ)=(1−d0​(Q0​)μ−d0​(Q0​)x0​SN0​​SN0​Sn0​​−x)Cn+1−1​(ρ)ℓn+1​(ρ) applied to the filter is optimal, and the minimal variance is

d0(Q0)1−d0(Q0)(μ−x0SN0)2,\frac{d_0(Q_0)}{1-d_0(Q_0)}\big(\mu-x_0S^0_N\big)^2,1−d0​(Q0​)d0​(Q0​)​(μ−x0​SN0​)2,

with dn,ℓn,Cnd_n,\ell_n,C_ndn​,ℓn​,Cn​ given by the backward recursion (6.7).

Significance

Theorem 6.1.1 is the structural result of the chapter: it says that a hidden regime costs no more than one extra state variable, the filter, and that the investor who uses the whole price history does no better than one who uses only current wealth and current belief. Theorems 6.1.2 and 6.2.3 turn this into explicit recursions: for power utility the wealth dependence factors out and only a function of the belief remains; for mean–variance the efficient frontier keeps the same shape as under full observation, with the constant d0(Q0)d_0(Q_0)d0​(Q0​) computed from the filter. The comparison results of the chapter (Theorem 6.1.5, partial versus complete observation in the binomial model) and the logarithmic case (Theorem 6.1.7) build on these.

The results are proved in the book by combining the general reduction of Chapter 5 (Theorems 5.3.2, 5.3.3) with the structure theorems of Chapter 4. Those general POMDP theorems are formalized on the platform for models whose observable transition has a density; the financial model here does not (the next wealth is a deterministic function of the return), so this mission states the financial results directly on the market, with no reduction built into the definitions. None of the three theorems is formalized yet; earlier platform statements of them were retired as unfaithful.

Difficulty

The value of (6.2) is a supremum over strategies that are arbitrary measurable functions of the observed history, computed under the law of the hidden chain; JNJ_NJN​ is defined from a different process, the filtered model, in which returns are drawn from predictive laws. Equality of the two requires the filter property: the conditional law of YnY_nYn​ given R1,…,RnR_1,\dots,R_nR1​,…,Rn​ is μn\mu_nμn​, and the conditional law of Rn+1R_{n+1}Rn+1​ is the predictive mixture. On top of this, the Bellman equation needs measurability of the value functions on the space of probability measures and the existence of measurable maximizers, which the book obtains from compactness of D(x)D(x)D(x) under no arbitrage and the upper bounding function 1+x1+x1+x. Applying the one-period existence theorem pointwise in ρ\rhoρ does not give a measurable selection by itself.

Formalization scope

Rd\mathbb R^dRd is Fin d → ℝ; EYE_YEY​ is a standard Borel space and beliefs are ProbabilityMeasure E_Y with the Giry σ\sigmaσ-algebra. Return paths are 0-indexed vectors. Strategies are measurable functions of the return path; the market law of the returns is built recursively from (6.1). JnJ_nJn​ is a supremum over Markov policies of measurable decision rules on R×P(EY)\mathbb R\times\mathbb P(E_Y)R×P(EY​) of the expected utility under the filtered model's law of returns. Expectations of utilities are extended reals, ∫f+−∫f−\int f^+-\int f^-∫f+−∫f−. The Bayes operator returns ρ\rhoρ on the null set where its normalizing constant is 000 or ∞\infty∞.

The hypothesis that D(x)D(x)D(x) does not depend on yyy is part of the goal: for dom⁡U=(0,∞)\operatorname{dom}U=(0,\infty)domU=(0,∞) it does not follow from equal supports, and without it part 4 fails. The existence of maximizers is also corrected: for dom⁡U=(0,∞)\operatorname{dom}U=(0,\infty)domU=(0,∞) with U(0+)U(0+)U(0+) and U′(0+)U'(0+)U′(0+) finite, for instance U(x)=log⁡(1+x)U(x)=\log(1+x)U(x)=log(1+x), the set D(x)D(x)D(x) can be open with the supremum approached at its boundary, so part 4 asserts existence only under the stated conditions, which cover [0,∞)[0,\infty)[0,∞), logarithmic and negative power utility. For the mean–variance theorem the first-moment condition is used in its uniform L2L^2L2 form, which the book's covariance matrices for every belief require. A formalization in which competitors are restricted to filter-based Markov rules would make part 3 trivial and is not used.

Needed infrastructure: filtering for hidden Markov models (conditional laws of YnY_nYn​ under the recursive path law), Markov Decision Processes on Borel spaces with measurable selection, and the one-period no-arbitrage existence theorem; all of these are reusable beyond this mission. Contributions of lemmas on the filter, the predictive law and the compactness of D(x)D(x)D(x) are welcome.

Selected references

  • N. Bäuerle, U. Rieder, Markov Decision Processes with Applications to Finance, Universitext, Springer, 2011; Chapter 5 (pp.147–174) and Chapter 6 (pp.175–189). https://doi.org/10.1007/978-3-642-18324-9
  • W. Runggaldier, B. Trivellato, T. Vargiolu, A Bayesian adaptive control approach to risk management in a binomial model, in Seminar on Stochastic Analysis, Random Fields and Applications III (Ascona, 1999), Birkhäuser, 2002, 243–258 (as cited in the book's bibliography).
  • G. Favero, Shortfall risk minimization under model uncertainty in the binomial case: adaptive and robust approaches, Mathematical Methods of Operations Research 53, 2001, 493–503 (as cited in the book's bibliography).
  • M. Taksar, X. Zeng, Optimal terminal wealth under partial information: both the drift and the volatility driven by a discrete-time Markov chain, SIAM Journal on Control and Optimization 46, 2007, 1461–1482 (as cited in the book's bibliography).
32 thms1 active userReviewed
Functional AnalysisLinear algebraQuantum Information·Captain: iris

From Wigner-Yanase-Dyson conjecture to Carlen-Frank-Lieb conjecture: the full range of (p, q, s) where Tr(B^{q/2}K*A^pKB^{q/2})^s is jointly concave or jointly convexResearch Paper

Motivation

Convexity and concavity of trace functions of matrices are a basic tool of mathematical physics and quantum information. Lieb's concavity theorem (Lieb 1973), that (A,B)↦Tr⁡K∗ApKB1−p(A,B)\mapsto\operatorname{Tr}K^*A^pKB^{1-p}(A,B)↦TrK∗ApKB1−p is jointly concave for 0<p≤10<p\le10<p≤1, settled the Wigner–Yanase–Dyson conjecture on the concavity of skew information and underlies the strong subadditivity of quantum entropy. Ando's convexity theorem (Ando 1979) is its counterpart for −1≤p<0-1\le p<0−1≤p<0.

In quantum information the same functions govern the data processing inequality for Rényi-type divergences. The α\alphaα-zzz Rényi relative entropies of Audenaert–Datta 2015 are monotone under completely positive trace preserving maps exactly when a two-variable trace function of the form below is jointly convex or concave with exponent s=1/(p+q)s=1/(p+q)s=1/(p+q).

Timeline:

  • 1973: Epstein proves concavity of A↦Tr⁡(K∗ApK)1/pA\mapsto\operatorname{Tr}(K^*A^pK)^{1/p}A↦Tr(K∗ApK)1/p for 0<p≤10<p\le10<p≤1 by complex analysis; Lieb proves joint concavity of Tr⁡K∗ApKB1−p\operatorname{Tr}K^*A^pKB^{1-p}TrK∗ApKB1−p.
  • 1979: Ando proves the joint convexity for −1≤p<0-1\le p<0−1≤p<0.
  • 2008: Carlen and Lieb prove convexity of Tr⁡(K∗ApK)1/p\operatorname{Tr}(K^*A^pK)^{1/p}Tr(K∗ApK)1/p for 1≤p≤21\le p\le21≤p≤2 by a variational method (arXiv:0710.4167).
  • 2013: Hiai proves convexity of Tr⁡(K∗ApK)s\operatorname{Tr}(K^*A^pK)^sTr(K∗ApK)s for −1≤p<0-1\le p<0−1≤p<0, 0<s≤10<s\le10<s≤1.
  • 2015: Audenaert and Datta conjecture the range of (α,z)(\alpha,z)(α,z) for monotonicity.
  • 2018: Carlen, Frank and Lieb survey the area and pose a stronger conjecture covering all s≥1/(p+q)s\ge1/(p+q)s≥1/(p+q) (arXiv:1806.03985).
  • 2018–2020: Zhang proves the full range (arXiv:1811.01205), the paper of this mission.

Setting

Fix a finite index type nnn, so matrices are elements of Cn×n\mathbb C^{n\times n}Cn×n. A matrix AAA is positive definite if it is Hermitian with strictly positive eigenvalues; for such AAA and real ppp, the real power ApA^pAp is defined by applying x↦xpx\mapsto x^px↦xp to the eigenvalues (Lean: OgawaNagaoka.matPow A p). Fix an invertible matrix KKK and real numbers p,q,sp,q,sp,q,s. The trace function of the paper is

Ψp,q,s(A,B)=Tr⁡(Bq/2K∗ApKBq/2)s\Psi_{p,q,s}(A,B)=\operatorname{Tr}\big(B^{q/2}K^*A^pKB^{q/2}\big)^sΨp,q,s​(A,B)=Tr(Bq/2K∗ApKBq/2)s

on pairs (A,B)(A,B)(A,B) of positive definite matrices (Lean: ZhangCFL.Psi p q s K A B). Its one-variable specialization is Υp,s(A)=Tr⁡(K∗ApK)s\Upsilon_{p,s}(A)=\operatorname{Tr}(K^*A^pK)^sΥp,s​(A)=Tr(K∗ApK)s (Lean: ZhangCFL.Upsilon p s K A). For any matrix XXX, write ∣X∣=(X∗X)1/2|X|=(X^*X)^{1/2}∣X∣=(X∗X)1/2 and Tr⁡∣X∣r=Tr⁡(X∗X)r/2\operatorname{Tr}|X|^r=\operatorname{Tr}(X^*X)^{r/2}Tr∣X∣r=Tr(X∗X)r/2 (Lean: ZhangCFL.trAbsPow r X).

Ψp,q,s\Psi_{p,q,s}Ψp,q,s​ is jointly concave if for all pairs (A1,B1),(A2,B2)(A_1,B_1),(A_2,B_2)(A1​,B1​),(A2​,B2​) and λ∈[0,1]\lambda\in[0,1]λ∈[0,1], Ψ(λA1+(1−λ)A2,λB1+(1−λ)B2)≥λΨ(A1,B1)+(1−λ)Ψ(A2,B2)\Psi(\lambda A_1+(1-\lambda)A_2,\lambda B_1+(1-\lambda)B_2)\ge\lambda\Psi(A_1,B_1)+(1-\lambda)\Psi(A_2,B_2)Ψ(λA1​+(1−λ)A2​,λB1​+(1−λ)B2​)≥λΨ(A1​,B1​)+(1−λ)Ψ(A2​,B2​), and jointly convex with the inequality reversed.

Formalization targets

Goal: Theorem 1.1

Assume p≥qp\ge qp≥q and s>0s>0s>0. Then Ψp,q,s\Psi_{p,q,s}Ψp,q,s​ is

(1) jointly concave if 0≤q≤p≤1, 0<s≤1p+q;(2) jointly convex if −1≤q≤p≤0, s>0;(3) jointly convex if −1≤q≤0, 1≤p≤2, (p,q)≠(1,−1), s≥1p+q.\begin{aligned} &\text{(1) jointly concave if } 0\le q\le p\le1,\ 0<s\le\tfrac1{p+q};\\ &\text{(2) jointly convex if } -1\le q\le p\le0,\ s>0;\\ &\text{(3) jointly convex if } -1\le q\le0,\ 1\le p\le2,\ (p,q)\ne(1,-1),\ s\ge\tfrac1{p+q}. \end{aligned}​(1) jointly concave if 0≤q≤p≤1, 0<s≤p+q1​;(2) jointly convex if −1≤q≤p≤0, s>0;(3) jointly convex if −1≤q≤0, 1≤p≤2, (p,q)=(1,−1), s≥p+q1​.​

The normalization p≥qp\ge qp≥q, s>0s>0s>0 loses nothing by symmetry, and the ranges are sharp (Proposition 2.3 of the paper, cited).

Milestones, in attack order

  1. Lemma 3.1 (Lieb, Ando): joint concavity of Tr⁡K∗ApKB1−p\operatorname{Tr}K^*A^pKB^{1-p}TrK∗ApKB1−p for 0<p≤10<p\le10<p≤1, joint convexity for −1≤p<0-1\le p<0−1≤p<0.
  2. Lemma 3.2: pointwise suprema of convex functions are convex, partial infima of jointly convex functions are convex, and the concave analogues.
  3. Theorem 3.3: the variational formulas
Tr⁡∣XY∣r0=min⁡Z{r0r1Tr⁡∣XZ∣r1+r0r2Tr⁡∣Z−1Y∣r2},Tr⁡∣XY∣r1=max⁡Z{r1r0Tr⁡∣XZ∣r0−r1r2Tr⁡∣Y−1Z∣r2}\operatorname{Tr}|XY|^{r_0}=\min_{Z}\Big\{\tfrac{r_0}{r_1}\operatorname{Tr}|XZ|^{r_1}+\tfrac{r_0}{r_2}\operatorname{Tr}|Z^{-1}Y|^{r_2}\Big\},\quad \operatorname{Tr}|XY|^{r_1}=\max_{Z}\Big\{\tfrac{r_1}{r_0}\operatorname{Tr}|XZ|^{r_0}-\tfrac{r_1}{r_2}\operatorname{Tr}|Y^{-1}Z|^{r_2}\Big\}Tr∣XY∣r0​=Zmin​{r1​r0​​Tr∣XZ∣r1​+r2​r0​​Tr∣Z−1Y∣r2​},Tr∣XY∣r1​=Zmax​{r0​r1​​Tr∣XZ∣r0​−r2​r1​​Tr∣Y−1Z∣r2​}

for 1r0=1r1+1r2\frac1{r_0}=\frac1{r_1}+\frac1{r_2}r0​1​=r1​1​+r2​1​, ZZZ ranging over invertible matrices. 4. Z↦Tr⁡ZrZ\mapsto\operatorname{Tr}Z^rZ↦TrZr is convex on positive definite matrices for every r<0r<0r<0 (used in the proof of Theorem 3.7). 5. Theorem 3.7 (Epstein, Hiai, Carlen–Lieb): concavity of Υp,1/p\Upsilon_{p,1/p}Υp,1/p​ for 0<p≤10<p\le10<p≤1; convexity of Υp,s\Upsilon_{p,s}Υp,s​ for −1≤p<0-1\le p<0−1≤p<0, 0<s≤10<s\le10<s≤1; convexity of Υp,1/p\Upsilon_{p,1/p}Υp,1/p​ for 1≤p≤21\le p\le21≤p≤2. 6. Theorem 3.5 (Carlen–Frank–Lieb): Υp,s\Upsilon_{p,s}Υp,s​ is concave for 0<p≤10<p\le10<p≤1, 0<s≤1/p0<s\le1/p0<s≤1/p; convex for −1≤p≤0-1\le p\le0−1≤p≤0, s>0s>0s>0; convex for 1≤p≤21\le p\le21≤p≤2, s≥1/ps\ge1/ps≥1/p. 7. The identity Ψp,q,s(A,B)=Tr⁡∣Ap/2KBq/2∣2s\Psi_{p,q,s}(A,B)=\operatorname{Tr}|A^{p/2}KB^{q/2}|^{2s}Ψp,q,s​(A,B)=Tr∣Ap/2KBq/2∣2s that opens the proof of Theorem 1.1.

Significance

Theorem 1.1 gives the complete region of (p,q,s)(p,q,s)(p,q,s) in which Ψp,q,s\Psi_{p,q,s}Ψp,q,s​ is jointly concave or convex for every invertible KKK. Part (3) confirms the conjecture of Carlen, Frank and Lieb, and its case s=1/(p+q)s=1/(p+q)s=1/(p+q) the Audenaert–Datta conjecture; together with known necessity results this yields the exact set of (α,z)(\alpha,z)(α,z) for which the α\alphaα-zzz Rényi relative entropy satisfies the data processing inequality (Theorem 1.2 of the paper, not part of this mission). The same theorem recovers the concavity results of Lieb and Epstein and the convexity results of Ando, Carlen–Lieb and Hiai as special cases.

The result is proved; as far as is recorded on the platform, none of it is formalized. A machine-checked development would supply real powers of positive definite matrices with their calculus, trace Hölder and Young inequalities for Schatten quasi-norms, the variational formulas of Theorem 3.3, and Lieb's concavity theorem, all of which are reusable throughout quantum information theory (relative entropies, recoverability, entropy inequalities).

Difficulty

The variational reduction itself is short once its inputs exist; the weight lies in the inputs. Lemma 3.1 is Lieb's concavity theorem and Ando's convexity theorem, which rest on operator concavity and convexity of A↦ApA\mapsto A^pA↦Ap and are absent from Mathlib. Theorem 3.3 requires Hölder's inequality for Schatten rrr-quasi-norms with rrr possibly below 111, together with polar decompositions to exhibit the extremizers. The tempting shortcut of proving convexity separately in AAA and in BBB does not work: separate convexity does not imply joint convexity, and the theorem is about the pair.

Formalization scope

Matrices are Matrix n n ℂ over a finite index type n : Type with decidable equality; the dimension is arbitrary, including 000. Positive definite means Matrix.PosDef (with open scoped ComplexOrder), and invertibility of KKK is IsUnit K. Real powers are the published OgawaNagaoka.matPow (continuous functional calculus with Real.rpow), and traces are the real part of Matrix.trace, which is the trace itself on the positive definite matrices involved. Joint concavity and convexity are ConcaveOn ℝ/ConvexOn ℝ on the set of pairs of positive definite matrices. In Theorem 1.1 the bound s≤1/(p+q)s\le1/(p+q)s≤1/(p+q) is written s(p+q)≤1s(p+q)\le1s(p+q)≤1, so that at p=q=0p=q=0p=q=0 the clause is not vacuous; Lemma 3.2 takes suprema and infima in EReal, with no boundedness hypothesis; minima and maxima in Theorem 3.3 are IsLeast/IsGreatest, so they are attained.

Positive semidefinite inputs are not a substitute for positive definite ones: on singular matrices matPow at a negative exponent is a generalized inverse power, and the statements change meaning.

Contributions welcome: proofs of the milestones in any order; Lieb's concavity theorem and the trace Hölder inequality are the reusable cores.

Selected references

  • H. Zhang, From Wigner-Yanase-Dyson conjecture to Carlen-Frank-Lieb conjecture, Adv. Math. 365 (2020); arXiv:1811.01205v2. https://arxiv.org/abs/1811.01205
  • E. A. Carlen, R. L. Frank, E. H. Lieb, Inequalities for quantum divergences and the Audenaert–Datta conjecture, J. Phys. A 51 (2018). https://arxiv.org/abs/1806.03985
  • E. H. Lieb, Convex trace functions and the Wigner-Yanase-Dyson conjecture, Adv. Math. 11 (1973). https://doi.org/10.1016/0001-8708(73)90011-X
  • T. Ando, Concavity of certain maps on positive definite matrices and applications to Hadamard products, Linear Algebra Appl. 26 (1979). https://doi.org/10.1016/0024-3795(79)90179-4
  • E. A. Carlen, E. H. Lieb, A Minkowski type trace inequality and strong subadditivity of quantum entropy II, Lett. Math. Phys. 83 (2008). https://arxiv.org/abs/0710.4167
  • K. M. R. Audenaert, N. Datta, α-z-Rényi relative entropies, J. Math. Phys. 56 (2015). https://doi.org/10.1063/1.4906367
12 thms1 active userReviewed
Bandit AlgorithmsLinear OptimizationMachine Learning+1·Captain: iris

Blind Network Revenue Management and Bandits with Knapsacks Under Limited Switches: LS-2SLP and a Matching Lower Bound Pin the Optimal Regret at T^(1/(2-2^(-ν(s,d))))Research Paper

Selling with few price changes

Network revenue management studies a firm that sells several products made from shared, limited resources over a finite season: airline seats on connected legs, hotel room nights, retail items that share inventory. In the blind version the firm does not know how demand responds to price and has to learn it while selling. Besbes and Zeevi (2012) posed this problem, and later work reached regret of order T\sqrt TT​ over TTT periods (Agrawal and Devanur 2014, Badanidiyuru, Kleinberg and Slivkins 2013). Almost all of those algorithms change prices order-TTT times, which retailers usually cannot do. Simchi-Levi, Xu and Zhao ask how much regret a limit on the number of price changes costs, and how that cost depends on the number of resources.

Setting

A BNRM problem has a horizon of TTT periods, ddd resources with inventories BiB_iBi​, nnn products, a consumption matrix A=(aij)A=(a_{ij})A=(aij​) and KKK price vectors pk=(pj,k)j\mathbf p_k=(p_{j,k})_jpk​=(pj,k​)j​. Each period the firm posts one price vector ztz_tzt​. Under price vector kkk the demand of product jjj is a random variable Qj,k∈[0,1]Q_{j,k}\in[0,1]Qj,k​∈[0,1] with an unknown law, independent across products and fresh each period. A unit of demand for product jjj earns pj,kp_{j,k}pj,k​ and uses aija_{ij}aij​ of resource iii. Selling stops as soon as the cumulative consumption of some resource exceeds its inventory.

A switch is a period with zt≠zt+1z_t\ne z_{t+1}zt​=zt+1​. A non-anticipating policy ϕ\phiϕ picks ztz_tzt​ from a probability kernel on the past actions and demands. Φ[s]\Phi[s]Φ[s] is the set of policies with at most sss switches almost surely under every demand law, and ΠQ[s]\Pi_Q[s]ΠQ​[s] is the set of policies with at most sss switches under the law QQQ. The sss-switch regret and the regret are

Rsϕ(T)=sup⁡Q(sup⁡π∈ΠQ[s]RevQ(π)−RevQ(ϕ)),Rϕ(T)=sup⁡Q(sup⁡πRevQ(π)−RevQ(ϕ)).R^\phi_s(T)=\sup_Q\Big(\sup_{\pi\in\Pi_Q[s]}\mathrm{Rev}_Q(\pi)-\mathrm{Rev}_Q(\phi)\Big),\qquad R^\phi(T)=\sup_Q\Big(\sup_{\pi}\mathrm{Rev}_Q(\pi)-\mathrm{Rev}_Q(\phi)\Big).Rsϕ​(T)=Qsup​(π∈ΠQ​[s]sup​RevQ​(π)−RevQ​(ϕ)),Rϕ(T)=Qsup​(πsup​RevQ​(π)−RevQ​(ϕ)).

The deterministic LP JDLPJ^{\mathrm{DLP}}JDLP maximizes ∑k,jpj,kqj,kxk\sum_{k,j}p_{j,k}q_{j,k}x_k∑k,j​pj,k​qj,k​xk​ subject to ∑k,jaijqj,kxk≤Bi\sum_{k,j}a_{ij}q_{j,k}x_k\le B_i∑k,j​aij​qj,k​xk​≤Bi​, ∑kxk≤T\sum_k x_k\le T∑k​xk​≤T, x≥0x\ge0x≥0, where qj,k=E[Qj,k]q_{j,k}=\mathbb E[Q_{j,k}]qj,k​=E[Qj,k​]. Its role is that of the benchmark. The rate is governed by the integer

ν(s,d)=⌊s−d−1K−1⌋.\nu(s,d)=\Big\lfloor\frac{s-d-1}{K-1}\Big\rfloor .ν(s,d)=⌊K−1s−d−1​⌋.

Formalization targets

Goal: the optimal rate

With Bi/T∈[b,1]B_i/T\in[b,1]Bi​/T∈[b,1], K≥2(d+1)K\ge2(d+1)K≥2(d+1), n≥d+1n\ge d+1n≥d+1 and T≥2T\ge2T≥2, there is a problem with these TTT and B\mathbf BB (entries of PPP at most 111, of AAA at most 222) such that, for every sss, the minimax regret over Φ[s]\Phi[s]Φ[s] satisfies

min⁡{cLb,cL′} K−32−a(d+1)3(log⁡T)5/2 Ta ≤ inf⁡ϕ∈Φ[s]Rsϕ(T),a=12−2−ν(s,d),\min\{c_Lb,c_L'\}\,\frac{K^{-\frac32-a}}{(d+1)^{3}(\log T)^{5/2}}\,T^{a}\ \le\ \inf_{\phi\in\Phi[s]}R^\phi_s(T),\qquad a=\frac1{2-2^{-\nu(s,d)}},min{cL​b,cL′​}(d+1)3(logT)5/2K−23​−a​Ta ≤ ϕ∈Φ[s]inf​Rsϕ​(T),a=2−2−ν(s,d)1​,

while on every problem with these TTT and B\mathbf BB and entries bounded by pmax⁡p_{\max}pmax​, amax⁡a_{\max}amax​, the algorithm LS-2SLP exists, is in Φ[s]\Phi[s]Φ[s], and, when n≤(d+1)log⁡[(d+1)KT](log⁡T)2n\le(d+1)\log[(d+1)KT](\log T)^2n≤(d+1)log[(d+1)KT](logT)2,

Rϕ(T)≤max⁡{cU/b,cU′} n3(d+1)log⁡[(d+1)KT] K1−alog⁡T  Ta.R^\phi(T)\le\max\{c_U/b,c_U'\}\,\sqrt{n^3(d+1)\log[(d+1)KT]}\,K^{1-a}\log T\;T^{a}.Rϕ(T)≤max{cU​/b,cU′​}n3(d+1)log[(d+1)KT]​K1−alogTTa.

cL,cL′c_L,c_L'cL​,cL′​ are numerical; cU,cU′c_U,c_U'cU​,cU′​ depend only on amax⁡,pmax⁡a_{\max},p_{\max}amax​,pmax​. This is the Θ~(T1/(2−2−ν(s,d)))\tilde\Theta(T^{1/(2-2^{-\nu(s,d)})})Θ~(T1/(2−2−ν(s,d))) of §4.3.

Milestones

  • Theorem 3 (upper bound) with its preparations: Lemma EC.1 on the epoch grid, and the DLP bound of §3.1.
  • Theorem 4 (lower bound) with its preparations: Lemmas EC.3–EC.7, the comparator bound (EC.46), and the bandit bound CMABKTC_{\mathrm{MAB}}\sqrt{KT}CMAB​KT​.

Significance

The result. The optimal regret is a step function of sss. Roughly log⁡log⁡T\log\log TloglogT switches suffice for Θ~(T)\tilde\Theta(\sqrt T)Θ~(T​), and with s≤d+1s\le d+1s≤d+1 the regret is linear. Each extra resource costs one more switch, the first result, according to the authors, that shows how the dimension of the constraints makes a stochastic online learning problem harder. Theorem 3 also shows that a small number of LPs replaces the elimination over mixtures of Badanidiyuru et al.

Formalizing it. The result is proved on paper and, to the extent we could determine, has no machine-checked proof. The platform has switching-limited bandits without resources (BwSC.LowerBound.theorem_2) and bandits with knapsacks without switch limits, but nothing with both. Formalization also records corrections to the printed statements. Theorem 3 fails at T=1T=1T=1, and its proof hides epoch-1 consumption of order n amax⁡t1n\,a_{\max}t_1namax​t1​, so the printed bound fails for nnn growing like (log⁡T)5(\log T)^5(logT)5. For fixed nnn the rate in TTT is untouched. The DLP does not bound revenue exactly under the paper's stopping rule, so a factor 1+max⁡i∑jaij/Bi1+\max_i\sum_ja_{ij}/B_i1+maxi​∑j​aij​/Bi​ appears. Lemmas EC.1, EC.3, EC.4 and EC.7 carry smaller corrections, each with a counterexample in its item.

Difficulty

For the upper bound, single-arm elimination and uniform exploration both fail, because the optimal play is a mixture of arms. The epoch lengths are fixed, but the number of plays nkn_knk​ of each arm comes out of LPs with data-dependent values and has no closed form. The natural analysis, which plugs a confidence radius into a fixed sample count, therefore does not apply.

For the lower bound, the argument for bandits with limited switches tracks the cover times of an arbitrary policy and gives ⌊(s−1)/(K−1)⌋\lfloor(s-1)/(K-1)\rfloor⌊(s−1)/(K−1)⌋. Moving to ⌊(s−d−1)/(K−1)⌋\lfloor(s-d-1)/(K-1)\rfloor⌊(s−d−1)/(K−1)⌋ requires instances whose LP optimum has d+1d+1d+1 non-zeros at every shift, such that any policy that neglects a family of arms loses linear revenue, under a benchmark that itself has at most sss switches.

Formalization scope

Periods, arms and products are 000-based in Lean. Actions are Option (Fin K), where none is an absorbing stop, as Algorithm 2 stops once it has run. The history law is built period by period from Markov kernels. Demand vectors have the product law of their marginals. A period earns revenue exactly when cumulative consumption through it is within every inventory. LearningClass quantifies over all DemandLaw, and clairvoyant classes over all history-dependent policies with the switch bound under that law.

Regrets are real suprema of nonempty bounded families, with integrable revenue, and the verification file proves these facts, so no statement holds through a junk value. T≥2T\ge2T≥2 excludes (log⁡T)−5/2(\log T)^{-5/2}(logT)−5/2 at T=1T=1T=1, where Lean's 0−5/2=00^{-5/2}=00−5/2=0 would trivialize the lower bound. The goal asserts that LS-2SLP exists, so its upper clause cannot hold vacuously. IsLS2SLP fixes what Algorithm 2 overlooks: rounding by ⌈γNk⌉\lceil\gamma N_k\rceil⌈γNk​⌉, sparse LP solutions, empty samples and the order of arms within an epoch.

A complete development needs the DLP layer, Hoeffding and maximal concentration for the clean events, a change-of-measure bound for the Bernoulli history laws, a measurable selection of LP solutions, and the bandit lower bound in this model. The DLP bound and the history law are reusable for other network revenue management missions. Proofs of Lemmas EC.4 and EC.1 and of the DLP bound are the natural starting points, and direct proofs of the theorems are welcome too.

Selected references

  • D. Simchi-Levi, Y. Xu, J. Zhao, Blind Network Revenue Management and Bandits with Knapsacks Under Limited Switches, arXiv:1911.01067v5, 2025; Operations Research. https://arxiv.org/abs/1911.01067
  • O. Besbes, A. Zeevi, Blind Network Revenue Management, Operations Research 60(6), 2012. https://doi.org/10.1287/opre.1120.1103
  • A. Badanidiyuru, R. Kleinberg, A. Slivkins, Bandits with Knapsacks, FOCS 2013. https://arxiv.org/abs/1305.2545
  • S. Agrawal, N. Devanur, Bandits with Concave Rewards and Convex Knapsacks, EC 2014. https://arxiv.org/abs/1402.5758
  • D. Simchi-Levi, Y. Xu, Phase Transitions in Bandits with Switching Constraints, Management Science 69(12), 2023. https://doi.org/10.1287/mnsc.2023.4755
18 thms1 active userReviewed
Algebraic TopologyDifferential Geometry·Captain: iris

Bundle gerbes: stable isomorphism and local theory: the Dixmier-Douady class is a bijection from stable isomorphism classes of bundle gerbes to H3(M,Z)H^3(M, \mathbb{Z})H3(M,Z)Research Paper

Motivation

Line bundles on a manifold MMM are classified by their Chern class in H2(M,Z)H^2(M,\mathbb Z)H2(M,Z). One degree up, gerbes as sheaves of groupoids (Brylinski 1993) realize classes in H3(M,Z)H^3(M,\mathbb Z)H3(M,Z) geometrically. Bundle gerbes, introduced by Murray (1996), do this with bundles rather than sheaves, and they appear in index theory and Hamiltonian quantization (Carey, Mickelsson, Murray 1997) and in the classifying theory of Gajer (1997).

The theory had one defect. Two bundle gerbes can have the same characteristic class and fail to be isomorphic, which never happens for line bundles. Murray and Stevenson (1999) give the repair: stable isomorphism is exactly the relation of having the same class, and the classes of bundle gerbes up to stable isomorphism are exactly H3(M,Z)H^3(M,\mathbb Z)H3(M,Z).

Setting

Let MMM be a smooth manifold. A map π:Y→M\pi:Y\to Mπ:Y→M is locally split if every point of MMM lies in an open set UUU with a smooth section s:U→Ys:U\to Ys:U→Y. Write Y[2]=Y×πYY^{[2]}=Y\times_\pi YY[2]=Y×π​Y for the pairs of points in one fibre.

A principal C×\mathbb C^\timesC× bundle over XXX is a space with a smooth projection to XXX and a fibrewise simply transitive action of C×\mathbb C^\timesC×, locally a product. Its dual Q∗Q^*Q∗ is the same space with the inverse action. The contracted product R⊗SR\otimes SR⊗S of two principal C×\mathbb C^\timesC× spaces is R×SR\times SR×S modulo the pairs (z,z−1)(z,z^{-1})(z,z−1).

A bundle gerbe over MMM is a pair (P,Y)(P,Y)(P,Y): a locally split π:Y→M\pi:Y\to Mπ:Y→M and a principal C×\mathbb C^\timesC× bundle P→Y[2]P\to Y^{[2]}P→Y[2] with a smooth, equivariant, associative product P(y1,y2)⊗P(y2,y3)→P(y1,y3)P_{(y_1,y_2)}\otimes P_{(y_2,y_3)}\to P_{(y_1,y_3)}P(y1​,y2​)​⊗P(y2​,y3​)​→P(y1​,y3​)​. Its dual is (P∗,Y)(P^*,Y)(P∗,Y), and the product of (P,Y)(P,Y)(P,Y) and (Q,Z)(Q,Z)(Q,Z) is (P⊗Q,Y×πZ)(P\otimes Q,Y\times_\pi Z)(P⊗Q,Y×π​Z).

For a C×\mathbb C^\timesC× bundle Q→YQ\to YQ→Y, the bundle gerbe δ(Q)\delta(Q)δ(Q) has fibres Qy1∗⊗Qy2Q^*_{y_1}\otimes Q_{y_2}Qy1​∗​⊗Qy2​​. A bundle gerbe isomorphic to some δ(Q)\delta(Q)δ(Q) is trivial. Two bundle gerbes are stably isomorphic if P⊗T1≅Q⊗T2P\otimes T_1\cong Q\otimes T_2P⊗T1​≅Q⊗T2​ for trivial T1,T2T_1,T_2T1​,T2​.

The Dixmier-Douady class comes from an open cover {Uα}\{U_\alpha\}{Uα​}, sections sα:Uα→Ys_\alpha:U_\alpha\to Ysα​:Uα​→Y, and σαβ:Uα∩Uβ→P\sigma_{\alpha\beta}:U_\alpha\cap U_\beta\to Pσαβ​:Uα​∩Uβ​→P over (sα,sβ)(s_\alpha,s_\beta)(sα​,sβ​). Then σαβσβγ=σαγgαβγ\sigma_{\alpha\beta}\sigma_{\beta\gamma}=\sigma_{\alpha\gamma}g_{\alpha\beta\gamma}σαβ​σβγ​=σαγ​gαβγ​ defines a C×\mathbb C^\timesC×-valued Čech cocycle, whose class lies in H2(M,C×)≃H3(M,Z)H^2(M,\mathbb C^\times)\simeq H^3(M,\mathbb Z)H2(M,C×)≃H3(M,Z). Here C×\mathbb C^\timesC× denotes smooth C×\mathbb C^\timesC×-valued functions, Z\mathbb ZZ denotes locally constant functions, and HnH^nHn is Čech cohomology.

Formalization targets

Goal: Theorem 3.3

For MMM a finite-dimensional, boundaryless, Hausdorff, paracompact smooth manifold, and any admissible class A\mathcal AA of locally split maps,

Φ:{bundle gerbes over A}/stable isomorphism→ ≃ H3(M,Z),Φ[P]=d(P).\Phi:\{\text{bundle gerbes over }\mathcal A\}/\text{stable isomorphism}\xrightarrow{\ \simeq\ }H^3(M,\mathbb Z),\qquad \Phi[P]=d(P).Φ:{bundle gerbes over A}/stable isomorphism ≃ ​H3(M,Z),Φ[P]=d(P).

The goal has three clauses: Φ\PhiΦ is bijective, Φ[P]\Phi[P]Φ[P] is exactly the class of PPP, and two gerbes have one class in the quotient exactly when they are stably isomorphic.

Milestones

δ(Q) exists;P⊗Q exists;gαβγ defines one class;H2(M,C×)≃H3(M,Z);\delta(Q)\text{ exists};\quad P\otimes Q\text{ exists};\quad g_{\alpha\beta\gamma}\text{ defines one class};\quad H^2(M,\mathbb C^\times)\simeq H^3(M,\mathbb Z);δ(Q) exists;P⊗Q exists;gαβγ​ defines one class;H2(M,C×)≃H3(M,Z); d(P)=0  ⟺  P trivial;d(P∗)=−d(P), d(P⊗Q)=d(P)+d(Q);P⊗(Q∗⊗Q)≅Q⊗(P⊗Q∗);d(P)=0\iff P\text{ trivial};\quad d(P^*)=-d(P),\ d(P\otimes Q)=d(P)+d(Q);\quad P\otimes(Q^*\otimes Q)\cong Q\otimes(P\otimes Q^*);d(P)=0⟺P trivial;d(P∗)=−d(P), d(P⊗Q)=d(P)+d(Q);P⊗(Q∗⊗Q)≅Q⊗(P⊗Q∗); stably isomorphic  ⟺  P⊗Q∗ trivial  ⟺  d(P)=d(Q);equivalence relation;every class occurs.\text{stably isomorphic}\iff P\otimes Q^*\text{ trivial}\iff d(P)=d(Q);\quad\text{equivalence relation};\quad\text{every class occurs}.stably isomorphic⟺P⊗Q∗ trivial⟺d(P)=d(Q);equivalence relation;every class occurs.

Significance

The result turns a characteristic class into a complete invariant. Bundle gerbes up to stable isomorphism are the same thing as degree-three integral classes, as line bundles are for degree two. The same paper uses this classification to obtain the local description of gerbes by transition data and the correspondence with Gajer's BC×B\mathbb C^\timesBC× bundles, and the notion of stable isomorphism underlies later work on bundle gerbe modules and twisted K-theory (Bouwknegt, Carey, Mathai, Murray, Stevenson 2002).

The theorem is proved on paper, partly by citing Murray (1996): Theorems 2.1, 2.2 and the realization of every class are stated, not proved, in this source. No formalized proof is known to this mission, and there was no formal definition of a bundle gerbe in the platform's library when the mission was drafted. The mission's output is a checked statement of the classification and a definition layer for bundle gerbes, Čech cohomology and diffeological principal bundles.

Difficulty

The algebra of the statement is short, and the proof of Proposition 3.2 fits in a few lines given the cited results. The work sits in the cited results. The Dixmier-Douady class is defined by choices on a cover, so showing it well defined requires comparing data across refinements. The passage H2(M,C×)≃H3(M,Z)H^2(M,\mathbb C^\times)\simeq H^3(M,\mathbb Z)H2(M,C×)≃H3(M,Z) needs the Čech long exact sequence on a paracompact space and smooth partitions of unity. Theorem 2.1 requires constructing a bundle on YYY from a vanishing cocycle, in a setting where Y→MY\to MY→M is only locally split. The naive identification of C×\mathbb C^\timesC×-valued functions with their logarithms fails globally, which is why a refinement is needed at each step.

Formalization scope

MMM is a finite-dimensional smooth manifold modelled on a normed space EEE, with T2Space and ParacompactSpace; there is no second countability, compactness or connectedness. Its diffeology is pinned by the class IsManifoldDiffeology E M.

YYY and PPP are diffeological spaces (Mathlib's DiffeologicalSpace), because the paper uses finite-dimensional manifolds, infinite-dimensional manifolds and differentiable spaces and leaves the category to context. A bijection for all diffeological YYY would not imply the one for manifold YYY, since the trivial gerbes would range over a larger class. So results are stated for every admissible class A\mathcal AA: a class of locally split maps closed under fibre products in which every open cover has a refinement whose nerve lies in the class. AdmissibleClass.all gives the diffeological statement, and surjective submersions from manifolds give the smooth one.

HnH^nHn is a colimit over covers, on all tuples, presented as a direct sum of cocycle groups modulo coboundaries and refinement. Stable isomorphism classes form a Quot. The contracted products P⊗QP\otimes QP⊗Q and δ(Q)\delta(Q)δ(Q) are relations IsTensor, IsDelta, given by balanced multiplicative maps, and the Dixmier-Douady class is a relation IsDixmierDouady; milestones supply existence and uniqueness. The equality in Definition 3.1 is read as isomorphism.

The trivializing readings are excluded: coefficients are locally constant and smooth (arbitrary functions make the Čech groups vanish), local triviality is by diffeomorphisms, and the goal keeps its three clauses instead of a bare cardinality statement.

Contributions to a comparison of the Čech groups with Mathlib's Sheaf.H, and to reusable diffeological bundle theory, are welcome beyond this mission.

Selected references

  • M. K. Murray, D. Stevenson, Bundle gerbes: stable isomorphism and local theory, arXiv:math/9908135v1, 1999. https://arxiv.org/abs/math/9908135v1
  • M. K. Murray, Bundle gerbes, J. London Math. Soc. (2) 54 (1996), 403–416. https://arxiv.org/abs/dg-ga/9407015
  • J.-L. Brylinski, Loop spaces, characteristic classes and geometric quantization, Birkhäuser, 1993. https://doi.org/10.1007/978-0-8176-4731-5
  • A. Carey, J. Mickelsson, M. Murray, Index theory, gerbes, and Hamiltonian quantization, Comm. Math. Phys. 183 (1997), 707–722. https://doi.org/10.1007/s002200050048
  • P. Gajer, Geometry of Deligne cohomology, Invent. Math. 127 (1997), 155–207. https://doi.org/10.1007/s002220050118
  • P. Bouwknegt, A. L. Carey, V. Mathai, M. K. Murray, D. Stevenson, Twisted K-theory and K-theory of bundle gerbes, Comm. Math. Phys. 228 (2002), 17–49. https://doi.org/10.1007/s002200200646
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CombinatoricsMachine Learning·Captain: iris

Deep Sets: Over a Countable Universe, a Function of a Finite Set Is Permutation Invariant iff It Has the Form ρ(∑x∈Xϕ(x))\rho(\sum_{x\in X}\phi(x))ρ(∑x∈X​ϕ(x))Research Paper

Motivation

Many learning problems take a set as input rather than a vector: a point cloud, the collection of words in a document, a group of users in an audience, a sample from a distribution. A model for such data must give the same answer however the elements of the set are listed. Deep Sets (Zaheer, Kottur, Ravanbakhsh, Póczos, Salakhutdinov, Smola, arXiv:1703.06114v3, NIPS 2017) asked which functions have this property and answered, for a countable universe of elements, with a structure theorem: every such function is a sum of per-element embeddings followed by a post-processing map. That structure is the "Deep Sets" architecture, in which a network ϕ\phiϕ is applied to each element, the outputs are summed, and a second network ρ\rhoρ is applied to the sum. The architecture and its sum-pooling template are now standard for set-valued inputs, and the paper's Theorem 2 is the result usually cited to justify it.

The paper also treats sets of a fixed size MMM drawn from an uncountable universe such as [0,1][0,1][0,1] (Theorem 7, p.14), where the representation requires continuity and a latent dimension M+1M+1M+1. That case is a different theorem and is not part of this mission.

Setting

Fix a universe X\mathfrak XX of elements (in Lean, a type U). A finite set X={x1,…,xM}⊆XX=\{x_1,\dots,x_M\}\subseteq\mathfrak XX={x1​,…,xM​}⊆X has M≥0M\ge 0M≥0 distinct elements; M=0M=0M=0 is the empty set. A listing of XXX is a tuple (x1,…,xM)(x_1,\dots,x_M)(x1​,…,xM​) of its distinct elements; in Lean it is an injective tuple x:Fin M→Ux:\mathrm{Fin}\,M\to Ux:FinM→U.

A function fff that assigns a real number to every listing of every size,

f:(M:N)→(Fin M→U)→R,f : (M:\mathbb N)\to(\mathrm{Fin}\,M\to U)\to\mathbb R ,f:(M:N)→(FinM→U)→R,

is permutation invariant (Property 1, eq. (7), p.12) if

f(x1,…,xM)=f(xπ(1),…,xπ(M))f(x_1,\dots,x_M)=f(x_{\pi(1)},\dots,x_{\pi(M)})f(x1​,…,xM​)=f(xπ(1)​,…,xπ(M)​)

for every MMM, every listing xxx of distinct elements and every permutation π\piπ of {1,…,M}\{1,\dots,M\}{1,…,M}. This is the Lean predicate DeepSets.IsPermInvariant f, where the reordered listing is x∘πx\circ\pix∘π. The paper calls such an fff a valid set function.

A function fff admits a sum decomposition if there are ϕ:X→R\phi:\mathfrak X\to\mathbb Rϕ:X→R and ρ:R→R\rho:\mathbb R\to\mathbb Rρ:R→R with

f(x1,…,xM)=ρ(∑m=1Mϕ(xm))f(x_1,\dots,x_M)=\rho\Bigl(\sum_{m=1}^{M}\phi(x_m)\Bigr)f(x1​,…,xM​)=ρ(m=1∑M​ϕ(xm​))

for every MMM and every listing of distinct elements. The same ϕ\phiϕ and ρ\rhoρ serve every set size.

Formalization targets

Goal: Theorem 2 (p.12; also stated on p.2)

For a countable universe UUU and every fff as above,

IsPermInvariant f  ⟺  ∃ ϕ:U→R, ∃ ρ:R→R, ∀M, ∀x injective, f M x=ρ(∑mϕ(xm)).\mathrm{IsPermInvariant}\,f\iff\exists\,\phi:U\to\mathbb R,\ \exists\,\rho:\mathbb R\to\mathbb R,\ \forall M,\ \forall x \text{ injective},\ f\,M\,x=\rho\Bigl(\sum_{m}\phi(x_m)\Bigr).IsPermInvariantf⟺∃ϕ:U→R, ∃ρ:R→R, ∀M, ∀x injective, fMx=ρ(m∑​ϕ(xm​)).

Both directions are part of the goal, for all M≥0M\ge 0M≥0, with ϕ\phiϕ and ρ\rhoρ chosen before MMM.

Milestones (the steps of the proof on p.12)

  1. An invariant function depends only on the set. If fff is permutation invariant, there is ggg on finite subsets of UUU with f(x1,…,xM)=g({x1,…,xM})f(x_1,\dots,x_M)=g(\{x_1,\dots,x_M\})f(x1​,…,xM​)=g({x1​,…,xM​}).
  2. Sufficiency. For every ϕ\phiϕ and ρ\rhoρ, X↦ρ(∑x∈Xϕ(x))X\mapsto\rho\left(\sum_{x\in X}\phi(x)\right)X↦ρ(∑x∈X​ϕ(x)) is permutation invariant.
  3. Unique representation. For an injective c:U→Nc:U\to\mathbb Nc:U→N, the map X↦∑x∈X4−c(x)X\mapsto\sum_{x\in X}4^{-c(x)}X↦∑x∈X​4−c(x) is injective on finite subsets of UUU.
  4. Construction of ρ\rhoρ. For an injective c:U→Nc:U\to\mathbb Nc:U→N and every ggg on finite subsets of UUU, there is ρ:R→R\rho:\mathbb R\to\mathbb Rρ:R→R with g(X)=ρ(∑x∈X4−c(x))g(X)=\rho\left(\sum_{x\in X}4^{-c(x)}\right)g(X)=ρ(∑x∈X​4−c(x)) for every finite XXX.

Milestones 1 and 4 give the forward direction of the goal; milestone 2 gives the backward direction.

Significance

The theorem says that, on a countable universe, nothing is lost by restricting a set model to the sum-pooling form: every permutation-invariant real function of finite sets, of all sizes at once, has it. It is the formal justification for sum pooling in set and multiset architectures, and the starting point for the later literature on the expressive power of such models, including the fixed-size uncountable case and the question of how large the latent dimension must be (Wagstaff et al., 2019).

The result is proved in the paper, in one paragraph. To the best of a search of the Prove2Me catalogue (November 2026), it has no machine-checked proof there; the closest published item, GeomDL.Sets.eq_6_invariant, proves only the sufficiency idea for sum readouts over rows of a real matrix. This mission produces a checked statement and proof of both directions for an arbitrary countable universe, together with the encoding lemma (milestone 3), which is reusable wherever a finite subset of a countable set must be coded injectively by a real number.

Difficulty

The sufficiency direction is a reindexing of a finite sum. The content is in the necessity direction, at two points.

First, Property 1 is a statement about listings, while the decomposition is about sets. Passing from one to the other requires showing that two listings of distinct elements with the same underlying set differ by a permutation and have the same length, for every size at once.

Second, a single real number ∑x∈Xϕ(x)\sum_{x\in X}\phi(x)∑x∈X​ϕ(x) must determine the whole finite set XXX, for sets of every size simultaneously, and with no bound on the elements used when the universe is infinite. Any ϕ\phiϕ that is not injective on singletons fails at once, and injectivity on singletons is far from enough. The paper fixes ϕ(x)=4−c(x)\phi(x)=4^{-c(x)}ϕ(x)=4−c(x); that its finite sums separate finite sets is the key arithmetic fact and must be proved, not assumed. A per-size decomposition (∀M ∃ ϕ,ρ\forall M\,\exists\,\phi,\rho∀M∃ϕ,ρ) would avoid this uniformity issue and is not what the paper claims.

Formalization scope

  • The universe is a type U with [Countable U], which includes finite universes. Page 12 prints ∣X∣<ℵ0|\mathfrak X|<\aleph_0∣X∣<ℵ0​; p.2 and the proof say "countable", and the countable reading is taken.
  • A finite set is presented by an injective tuple x : Fin M → U, for every M : ℕ, including M = 0. Values of f on tuples with repeated entries are not constrained by either side of the goal. Property 1 is stated on listings because on an unordered Finset it would hold trivially, and the goal would collapse to milestone 4.
  • ϕ:U→R\phi:U\to\mathbb Rϕ:U→R and ρ:R→R\rho:\mathbb R\to\mathbb Rρ:R→R, with no continuity, measurability or other regularity.
  • In milestones 1, 3 and 4, finite subsets are Finset U; the power 4−c(x)4^{-c(x)}4−c(x) is (4 : ℝ) ^ (-(c x : ℤ)); the enumeration ccc is an injective map U → ℕ, which exists for countable U by Countable.exists_injective_nat.
  • The definitions needed are only DeepSets.IsPermInvariant; everything else is Mathlib (Equiv.Perm, Finset.sum, Finset.image, zpow).

Contributions welcome: proofs of the four milestones and of the goal; the encoding lemma in greater generality (other bases, infinite subsets with tsum) as separate results.

Selected references

  • M. Zaheer, S. Kottur, S. Ravanbakhsh, B. Póczos, R. Salakhutdinov, A. J. Smola, Deep Sets, arXiv:1703.06114v3, 2018 (NIPS 2017). Theorem 2, pp.2 and 12; Property 1, eq. (7), p.12. https://arxiv.org/abs/1703.06114
  • E. Wagstaff, F. Fuchs, M. Engelcke, I. Posner, M. A. Osborne, On the Limitations of Representing Functions on Sets, ICML 2019. https://arxiv.org/abs/1901.09006
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Machine LearningQuantum InformationRepresentation Theory·Captain: iris

Representation Theory for Geometric Quantum Machine Learning: The Commutant of a Unitary Representation Is the Direct Sum of Multiplicity-Space Operators Tensored with the Identity on Each IrrepResearch Paper

Why the commutant matters in geometric quantum machine learning

Geometric quantum machine learning builds the symmetries of a learning task into a quantum model. A parametrized circuit is made equivariant when it commutes with a representation of the symmetry group, and a measurement is made invariant in the same way. The tutorial of Ragone et al., Representation Theory for Geometric Quantum Machine Learning, organizes this subject around one claim: "GQML is all about block-diagonal structures" (p.35). Its Theorem 7 is the precise form of that claim. It describes all operators commuting with a unitary representation, and equivariant circuits and measurements are among them. The theorem is classical. The paper attributes it to Simon's Representations of Finite and Compact Groups and prints no proof, saying only that it "rests fundamentally upon Schur's lemma" (p.29).

Setting

Let GGG be a group and HHH a finite dimensional complex Hilbert space. A unitary representation is a homomorphism g↦Ugg\mapsto U_gg↦Ug​ from GGG to the operators on HHH with Ug†Ug=1U_g^\dagger U_g=\mathbb 1Ug†​Ug​=1 for all ggg. A subspace is invariant when every UgU_gUg​ preserves it, and a representation is irreducible (an irrep) when its only invariant subspaces are 000 and the whole nonzero space. Two representations are equivalent when an invertible linear map intertwines them.

The commutant of an operator algebra A\mathcal AA is

C(A)={B:[A,B]=0 for all A∈A},\mathcal C(\mathcal A)=\{B:[A,B]=0\text{ for all }A\in\mathcal A\},C(A)={B:[A,B]=0 for all A∈A},

and C(U)\mathcal C(U)C(U) is the commutant of the algebra generated by the UgU_gUg​.

A decomposition into irreps is an identification of HHH with a direct sum under which

U=⨁k=1K1mk⊗Uk,U=\bigoplus_{k=1}^K\mathbb 1_{m_k}\otimes U_k ,U=k=1⨁K​1mk​​⊗Uk​,

where the UkU_kUk​ are pairwise inequivalent irreps on spaces VkV_kVk​. The integer mkm_kmk​ is the multiplicity of UkU_kUk​, the factor Cmk\mathbb C^{m_k}Cmk​ is its multiplicity space, and the factor VkV_kVk​ carries the irrep.

Formalization targets

The goal: Theorem 7, p.28

For every unitary representation UUU of a group on a finite dimensional complex Hilbert space, a decomposition into irreps exists, and for every such decomposition,

C(U)=⨁k=1KBmk⊗1dim⁡(Uk),\mathcal C(U)=\bigoplus_{k=1}^K\mathcal B_{m_k}\otimes\mathbb 1_{\dim(U_k)} ,C(U)=k=1⨁K​Bmk​​⊗1dim(Uk​)​,

where Bmk\mathcal B_{m_k}Bmk​​ denotes the operators on Cmk\mathbb C^{m_k}Cmk​. Both inclusions are part of the statement.

Milestones

  1. Theorem 4, p.23. A finite dimensional unitary representation is completely reducible, with orthogonal summands.
  2. Theorem 6, p.25. Schur's lemma, for a group and for a Lie algebra.
  3. Definition 17, p.28. TTT lies in the commutant of the algebra generated by the UgU_gUg​ if and only if TTT commutes with each UgU_gUg​.
  4. Footnote 20, p.28. A map intertwining 1m⊗ρ\mathbb 1_m\otimes\rho1m​⊗ρ and 1m′⊗σ\mathbb 1_{m'}\otimes\sigma1m′​⊗σ, for inequivalent irreps ρ,σ\rho,\sigmaρ,σ, is zero.
  5. p.29. A map intertwining 1m⊗ρ\mathbb 1_m\otimes\rho1m​⊗ρ and 1m′⊗ρ\mathbb 1_{m'}\otimes\rho1m′​⊗ρ is exactly a map B⊗1B\otimes\mathbb 1B⊗1.
  6. (31)–(32), pp.28–29. Elements of the commutant are block diagonal across kkk.
  7. p.27 (implicit). Equivalent irreducible unitary representations are unitarily equivalent.
  8. p.28. Every finite dimensional unitary representation has the form ⨁k1mk⊗Uk\bigoplus_k\mathbb 1_{m_k}\otimes U_k⨁k​1mk​​⊗Uk​ through an isometry, with mk≥1m_k\ge 1mk​≥1.

Significance

The result. Theorem 7 turns "commutes with the symmetry" into an explicit parametrization. An operator in the commutant is determined by one matrix per irrep, of size the multiplicity of that irrep, and it never connects different irreps. For a model hθ(ρ)=Tr[W(θ)ρW†(θ)M]h_\theta(\rho)=\mathrm{Tr}[W(\theta)\rho W^\dagger(\theta)M]hθ​(ρ)=Tr[W(θ)ρW†(θ)M] with equivariant WWW and MMM, the off-diagonal information of ρ\rhoρ between irrep sectors is inaccessible (pp.29–30, Fig. 10). The dimension of the commutant is ∑kmk2\sum_k m_k^2∑k​mk2​. Schur–Weyl duality, which the paper presents as an example (p.30), is the case of the tensor representation of the unitary group.

Formalizing it. The statement is proved in the literature but, as far as a search of this platform and Mathlib shows, it has no machine-checked form in this generality. Mathlib has Schur's lemma for group representations and isotypic components of modules, but neither this description of the commutant nor the Lie algebra clause of the paper's Schur lemma. The mission produces a reusable statement of the block structure for equivariant quantum models on the platform.

Difficulty

No step needs deep theory. The obstacle is bookkeeping across several identifications. Applying Schur's lemma directly does not reach the conclusion, because Theorem 7's blocks are not irreducible: 1m⊗ρ\mathbb 1_{m}\otimes\rho1m​⊗ρ is a sum of mmm copies of ρ\rhoρ. So Schur's lemma says nothing yet about a map between two such blocks, and the statement that this map is one matrix BBB tensored with the identity has to be derived from it. For the existence clause, the summands from complete reducibility must be collected into multiplicity spaces, and an equivalence between two summands is only a linear map, while the decomposition has to be an isometry.

Formalization scope

The Lean development uses the following conventions.

  • Representations are Mathlib's Representation, and irreducibility is Representation.IsIrreducible, which requires a nonzero space.
  • The field is C\mathbb CC for the goal. Over R\mathbb RR the statement fails: SO(2)SO(2)SO(2) on R2\mathbb R^2R2 is irreducible with commutant C\mathbb CC.
  • GGG is an arbitrary group. Compactness in the paper serves only to give unitarity, which is assumed here.
  • The total space is PiLp 2 of EuclideanSpace ℂ (Fin (m k)) ⊗[ℂ] V k, with the multiplicity factor first. The opposite factor order typechecks when m=dim⁡Vm=\dim Vm=dimV and is false.
  • The "===" of the source holds after an identification Φ\PhiΦ of HHH with the direct sum. Lean carries Φ\PhiΦ explicitly. It is linear in the commutant clause and isometric in the existence clause.
  • The irreps are pairwise inequivalent. Theorem 7 does not print this, but it is how the paper uses "multiplicity". Without it the theorem is false: take GGG trivial on C2\mathbb C^2C2 with two copies of the trivial representation.

The goal asserts existence as well as the description for every decomposition, so it cannot hold vacuously, and it states an if and only if, so a single inclusion does not close it.

The required library work is small: linear maps out of Cm⊗V\mathbb C^m\otimes VCm⊗V, and the passage from equivalence to unitary equivalence in milestone 7. Milestones 1, 2, 4, 5 and 7 are reusable beyond this mission. Direct proofs of the goal that bypass the milestones are welcome, as are generalizations of milestones 4 and 5 to arbitrary finite dimensional multiplicity spaces.

Selected references

  • M. Ragone, P. Braccia, Q. T. Nguyen, L. Schatzki, P. J. Coles, F. Sauvage, M. Larocca, M. Cerezo, Representation Theory for Geometric Quantum Machine Learning, arXiv preprint, 2023. https://arxiv.org/abs/2210.07980v2
  • B. Simon, Representations of Finite and Compact Groups, Graduate Studies in Mathematics, Vol. 10, American Mathematical Society, 1996. https://doi.org/10.1090/gsm/010
  • Q. T. Nguyen, L. Schatzki, P. Braccia, M. Ragone, M. Larocca, F. Sauvage, P. J. Coles, M. Cerezo, A theory for equivariant quantum neural networks, arXiv preprint, 2022. https://arxiv.org/abs/2210.08566
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Quantum Error CorrectionQuantum Information·Captain: iris

Hardware-Efficient Bosonic Quantum Error-Correcting Codes Based on Symmetry Operators: the photon-loss quantum Hamming bound (1+3n)bk≤(4q−3)n(1+3n)b^k \le (4q-3)^n(1+3n)bk≤(4q−3)nResearch Paper

Why count dimensions for bosonic codes

A quantum error-correcting code protects information by embedding it in a larger space. The quantum Hamming bound limits how small that space can be: the images of the code under the correctable errors must fit into the available space. Niu, Chuang and Shapiro (arXiv:1709.05302) design bosonic codes for hardware whose only nonlinearity is coherent χ(2)\chi^{(2)}χ(2) three-wave mixing, and their dominant error is the loss of a single photon. For such codes the usual bound, which counts all qudit rotations, is the wrong yardstick. Their Section V derives generalized Hamming bounds adapted to this setting, and the paper's abstract claims that its codes saturate the photon-loss versions. This mission formalizes the photon-loss bound, Theorem 5 of that section.

Setting: three-mode qudits and single-photon loss

A physical qudit consists of three bosonic modes, signal sss, idler iii and pump ppp, with Fock states ∣ns,ni,np⟩|n_s,n_i,n_p\rangle∣ns​,ni​,np​⟩. The χ(2)\chi^{(2)}χ(2) Hamiltonian conserves the pump-photon number, so a physical qudit of dimension qqq lives in the pump-photon subspace

Hq−1=Span{∣j,j,q−1−j⟩:0≤j≤q−1},\mathcal H_{q-1}=\mathrm{Span}\{|j,j,q-1-j\rangle:0\le j\le q-1\},Hq−1​=Span{∣j,j,q−1−j⟩:0≤j≤q−1},

and a code of nnn physical qudits is a subspace C⊆Hq−1⊗nC\subseteq\mathcal H_{q-1}^{\otimes n}C⊆Hq−1⊗n​. A code of kkk logical qudits of dimension bbb has dim⁡C=bk\dim C=b^kdimC=bk.

The annihilation operator a^ℓ,m\hat a_{\ell,m}a^ℓ,m​ of mode m∈{s,i,p}m\in\{s,i,p\}m∈{s,i,p} of qudit ℓ\ellℓ acts by a^∣r⟩=r ∣r−1⟩\hat a|r\rangle=\sqrt r\,|r-1\ranglea^∣r⟩=r​∣r−1⟩ on that mode and trivially on the others. To lowest order in the loss probability the single-photon-loss errors are the identity I^\hat II^ and the 3n3n3n operators a^ℓ,m\hat a_{\ell,m}a^ℓ,m​, in total 1+3n1+3n1+3n operators EhE_hEh​. The code satisfies the error-correction condition (23) of the paper when

⟨a~∣Eh†Ej∣b~⟩=αhjδab\langle\tilde a|E_h^\dagger E_j|\tilde b\rangle=\alpha_{hj}\delta_{ab}⟨a~∣Eh†​Ej​∣b~⟩=αhj​δab​

for all logical basis states and all h,jh,jh,j, with αhj\alpha_{hj}αhj​ independent of a~,b~\tilde a,\tilde ba~,b~. The corrupted code subspace is the span of all images Eh(C)E_h(C)Eh​(C), and its dimension is DlossD_{\mathrm{loss}}Dloss​.

Formalization targets

Goal: Theorem 5, corrected

For q≥2q\ge2q≥2 and every code C⊆Hq−1⊗nC\subseteq\mathcal H_{q-1}^{\otimes n}C⊆Hq−1⊗n​ with dim⁡C=bk\dim C=b^kdimC=bk satisfying (23) for the 1+3n1+3n1+3n errors,

(1+3n) bk≤(4q−3)n.(1+3n)\,b^k\le(4q-3)^n.(1+3n)bk≤(4q−3)n.

The printed theorem has no lower bound on qqq and is false at q=1q=1q=1: for n=1n=1n=1, b=k=1b=k=1b=k=1 and the one-dimensional code C=H0=Span{∣0,0,0⟩}C=\mathcal H_0=\mathrm{Span}\{|0,0,0\rangle\}C=H0​=Span{∣0,0,0⟩}, condition (23) holds, while 1+3=4>1=(4−3)11+3=4>1=(4-3)^11+3=4>1=(4−3)1. Every code in the paper has q≥2q\ge2q≥2, so the goal adds exactly this hypothesis. No nondegeneracy is assumed: the printed theorem has none, and the corrected bound holds without one.

Milestones

The three steps of the printed proof, stated separately.

  1. Error images of a nondegenerate code. If CCC satisfies (23) for a finite family (Eh)h∈κ(E_h)_{h\in\kappa}(Eh​)h∈κ​ and is nondegenerate for it, then
dim⁡∑hEh(C)=∣κ∣dim⁡C.\dim\sum_hE_h(C)=|\kappa|\dim C.dimh∑​Eh​(C)=∣κ∣dimC.

This is (112) with the sentence after it. The page does not assume nondegeneracy, but the step needs it. For q=n=2q=n=2q=n=2 and C=Span{∣0,0,1⟩∣0,0,1⟩}C=\mathrm{Span}\{|0,0,1\rangle|0,0,1\rangle\}C=Span{∣0,0,1⟩∣0,0,1⟩}, condition (23) holds and only three of the seven images are nonzero. 2. One qudit. The corrupted space of Hq−1\mathcal H_{q-1}Hq−1​ has dimension 4q−34q-34q−3, and the basis states ∣0,0,q−1⟩|0,0,q-1\rangle∣0,0,q−1⟩, ∣q−1,q−1,0⟩|q-1,q-1,0\rangle∣q−1,q−1,0⟩ and ∣j,j,q−1−j⟩|j,j,q-1-j\rangle∣j,j,q−1−j⟩ with 1≤j≤q−21\le j\le q-21≤j≤q−2 add one, two and three new dimensions. 3. The bound on the corrupted space. For every C⊆Hq−1⊗nC\subseteq\mathcal H_{q-1}^{\otimes n}C⊆Hq−1⊗n​,

Dloss≤(4q−3)n.D_{\mathrm{loss}}\le(4q-3)^n.Dloss​≤(4q−3)n.

What the bound says

The bound replaces the space qnq^nqn available to arbitrary codes by a budget of 4q−34q-34q−3 states per qudit, and the (q2−1)(q^2-1)(q2−1)-per-qudit error count of qudit rotations by the 1+3n1+3n1+3n loss errors. It shows, for instance, that one physical qutrit may protect a logical qubit against photon loss (2⋅4≤92\cdot4\le92⋅4≤9), whereas the rotation bound of the same paper needs n≥4n\ge4n≥4. The paper then reads off that its χ(2)\chi^{(2)}χ(2) parity-check and embedded codes saturate the bound.

The result itself is proved in the paper, up to the two corrections above. A search of the platform finds no formal statement of it. Formalizing it adds three things: a precise statement, in which the code class and the error family are pinned down; the correction at q=1q=1q=1; and a proof that also covers degenerate codes, which the printed proof does not reach. The statement is thin: the theorem is a finite dimension count. For q≥2q\ge2q≥2 the inequality (1+3n)dim⁡Hq−1⊗n≤(4q−3)n(1+3n)\dim\mathcal H_{q-1}^{\otimes n}\le(4q-3)^n(1+3n)dimHq−1⊗n​≤(4q−3)n already holds outside n=1n=1n=1 and n=q=2n=q=2n=q=2, and in those two cases the goal excludes only C=Hq−1⊗nC=\mathcal H_{q-1}^{\otimes n}C=Hq−1⊗n​. The value of the mission is a clean finite-dimensional model of multi-mode photon loss with a reusable error-correction condition, not depth.

Where the printed argument stops

The proof's first step reads "for all of these errors to be correctable, DerrD_{\mathrm{err}}Derr​ cannot exceed DlossD_{\mathrm{loss}}Dloss​", which treats the 1+3n1+3n1+3n images of the code as independent copies. Condition (23) does not imply this: the images are independent only for nondegenerate codes, and the theorem is stated for all codes. Applying the first step directly therefore proves the goal only for nondegenerate codes, and the general case cannot be obtained by adding a hypothesis. The other technical point is bookkeeping: the bound on DlossD_{\mathrm{loss}}Dloss​ must treat a loss on one qudit against product states of all the others, with the r\sqrt rr​ weights kept, since a plain shift of Fock states would change condition (23).

Formalization scope

The Hilbert space is EuclideanSpace ℂ (FockIdx n q) with FockIdx n q = Fin n → Fin 3 → Fin q, modes numbered signal, idler, pump =0,1,2=0,1,2=0,1,2. Photon numbers are truncated at q−1q-1q−1. Annihilation never raises a photon number, so this truncation changes no vector, inner product or dimension in the statements. Operators are complex matrices acting through Matrix.toEuclideanLin, and errors are indexed by Option (Fin n × Fin 3) with none the identity. Dimensions are Module.finrank ℂ. Condition (23) is SatisfiesKL, stated for all vectors of CCC and for all pairs of errors, cross terms included.

The hypothesis C≤Hq−1⊗nC\le\mathcal H_{q-1}^{\otimes n}C≤Hq−1⊗n​ cannot be dropped, since CCC would then range over a q3nq^{3n}q3n-dimensional space and the bound fails. The statement is not vacuous: every one-dimensional code satisfies (23).

SatisfiesKL, IsNondegenerate and corruptedSubspace are stated for any finite-dimensional space and any error family, and can be reused beyond this mission, as can the first milestone. Proofs of the goal, the milestones and an analogue of the first milestone for other error families are all welcome. Not included: Theorems 1–4 (qudit-rotation errors), the codes' verification of (23), and the saturation remarks.

Selected references

  • M. Y. Niu, I. L. Chuang, J. H. Shapiro, Hardware-Efficient Bosonic Quantum Error-Correcting Codes Based on Symmetry Operators, preprint, 2017. https://arxiv.org/abs/1709.05302v1
  • E. Knill, R. Laflamme, A Theory of Quantum Error-Correcting Codes, Phys. Rev. A 55, 900, 1997. https://arxiv.org/abs/quant-ph/9604034
  • D. Gottesman, Class of quantum error-correcting codes saturating the quantum Hamming bound, Phys. Rev. A 54, 1862, 1996. https://arxiv.org/abs/quant-ph/9604038
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Linear algebraMathematical PhysicsProbability+2·Captain: iris

Formalism Locality in Quantum Theory and Quantum Gravity: The Clumped Causaloid Fully Specifies the Quantum Theory of Pairwise Interacting QubitsResearch Paper

Why a theory should predict locally

General relativity has no fixed causal structure, and quantum theory has indefiniteness: a theory of quantum gravity may have to be probabilistic about causal structure itself. L. Hardy's causaloid framework addresses this by asking for predictions that make no reference to a background causal order. The 2008 paper Formalism Locality in Quantum Theory and Quantum Gravity isolates one principle behind that framework. A formulation is F-local if predictions about a space-time region use only mathematical objects pertaining to that region. The paper argues that the usual formulations of quantum theory fail this, and it closes by describing how quantum theory fits the causaloid framework for a system that can run any quantum computation: pairwise interacting qubits.

The paper describes that case "without deriving any of the results" (p.12), and states no numbered theorems. The earlier paper, Towards Quantum Gravity, introduced the framework, and its framework half is already posed on the platform as the HardyCausaloid mission. This mission takes the part left open: the qubit lattice.

The lattice and its data

There are mmm right moving qubits uuu and nnn left moving qubits vvv. Each right mover crosses each left mover at a vertex x=(u,v)x=(u,v)x=(u,v). At each vertex the two qubits pass through a box with a knob and a display panel, which together are a label α\alphaα: an instrument and one of its outcomes. A label has a superoperator \_\alpha,completelypositiveandtracenon−increasing.Givenadensitymatrix, completely positive and trace non-increasing. Given a density matrix ,completelypositiveandtracenon−increasing.Givenadensitymatrix\rho$ on the qubits, the probability of a total label is the trace after applying every box in an order compatible with the motion of the qubits.

A fiducial family is a real basis \k,, ,k\in\Omega^2,oftheHermiticity−preservingone−qubitmaps,with, of the Hermiticity-preserving one-qubit maps, with ,oftheHermiticity−preservingone−qubitmaps,with|\Omega^2|=2^4,eachmapcompletelypositiveandtracenon−increasing,andwith, each map completely positive and trace non-increasing, and with ,eachmapcompletelypositiveandtracenon−increasing,andwith$1=I. It defines two tables, by solving $$\\alpha=\sum{k_uk_v}\Lambda^{k_uk_v}{\alpha},${k_u}\otimes${k_v},\qquad ${l'}\circ$l=\sum{k}\Lambda^{1k}_{l'l},$_k.$$

For a finite set OOO of vertices, a clump is a maximal run of consecutive vertices of one qubit lying in OOO. The clumping method computes a Λ\LambdaΛ matrix for a clump by a recursion from the pair table, then multiplies the components over all clumps. The first vertex of a clump carries a free label and later vertices the identity. The list of the two tables together with this method is the causaloid of the lattice.

Formalization targets

Goal

For every m,nm,nm,n, every density matrix ρ\rhoρ, every fiducial family and all fiducial labels, the causaloid CCC of the lattice satisfies:

pα=rα(RO)⋅p(RO)for every region, label and preparation;p_\alpha=\mathbf r_\alpha(R_O)\cdot\mathbf p(R_O)\quad\text{for every region, label and preparation};pα​=rα​(RO​)⋅p(RO​)for every region, label and preparation;

the clump labels are a fiducial set in the interior of the lattice; the two-step approach holds, with

a=rα1α2,b=∑β2rα1β2,a=\mathbf r_{\alpha_1\alpha_2},\qquad b=\sum_{\beta_2}\mathbf r_{\alpha_1\beta_2},a=rα1​α2​​,b=β2​∑​rα1​β2​​,

so that a=c ba=c\,ba=cb gives the value ccc of Prob(Y2∣Y1,F1,F2)\mathrm{Prob}(Y_2\mid Y_1,F_1,F_2)Prob(Y2​∣Y1​,F1​,F2​) at every region, and the value ∣a∣/∣b∣|a|/|b|∣a∣/∣b∣ of (19) when b≠0b\ne0b=0, and in the interior the probability is well defined exactly when aaa and bbb are parallel, with value ∣a∣/∣b∣|a|/|b|∣a∣/∣b∣; and the method is F-local, in that tables agreeing on the vertices and sequential pairs of OOO give the same matrix for OOO.

Milestones

These follow the paper's order: the probabilities (6); the count ∣ΩN∣=N4|\Omega^N|=N^4∣ΩN∣=N4; the choice \_1=I$; the expansions (20) and (21); the recursions (22)–(24) and their generalization; the base case (25)–(26); the clumping method computing every probability; the fiducial clause; F-locality; and the symmetry property (27)–(28).

What the result gives

The result. A tiny list specifies the theory. Rather than one matrix per region, exponentially many, the theory is two tables and a rule. It also separates the specification of a theory from its use: the same calculation applies whatever the theory, and the conditional probabilities are decided without a causal order.

The formalization. The statements here are derived nowhere in the paper, and their proofs are not in print in this source, so the mission produces machine-checked statements for what the paper only describes. It also corrects the claim. As printed, the method is claimed for "an arbitrary region" (p.14), and with it the minimality of the fiducial set (p.9) and the "only if" of the two-step test (18). That fails at the ends of a qubit. Take a 1×11\times11×1 lattice, O1=∅O_1=\emptysetO1​=∅, O2O_2O2​ the whole lattice, and a σz\sigma_zσz​ measurement of the right mover. There is one preparation, so the probability is trivially well defined, yet aaa and bbb are not parallel. The goal keeps the computing clause and the "if" direction at every region, and states minimality and the "only if" for regions with no vertex at either end of a qubit. The counterexample is proved in Lean. Printed (24) also has an unbound index k′′′k'''k′′′, which is corrected.

Where the difficulty lies

Expanding every box and composing along each qubit is routine once the evaluation is multilinear and maps on different qubits commute. The central difficulty is minimality. Independence of the clump labels has to be exhibited by actual preparations outside the region, with one vertex in a gap serving the end of one clump and the start of the next, on each of its two qubits, and with the factors of the probabilities that come from outside the clumps kept nonzero. Trace-preserving preparations alone do not separate the labels: a numerical check at an interior vertex of a 3×33\times33×3 lattice gives rank 16 with them, against 256 with selected-outcome branches. Summability of the sums over outcomes, with countably many outcomes, is a separate step.

Formalization scope

The Lean development commits to the following. Lattices are Fin m × Fin n, for all m,nm,nm,n. Labels are 0-based, so the paper's first element of Ω2\Omega^2Ω2 is index 000 of Fin 16. An instrument is indexed by ℕ, with zero branches padding a finite one. Matrices on all the qubits are indexed by bit assignments, and the boxes are applied in lexicographic order, which is proved independent of the linear extension on a small case. The initial state is an arbitrary density matrix. Coefficients are real and solve (20) and (21) in a real basis. Tables are arguments of the clumped causaloid, so that F-locality is a statement.

The clumped Λ\LambdaΛ is computed by the recursion and a product over clumps, never characterized by the equation it should satisfy, which would make the first clause empty. The fiducial clause and the two-step clause are for the published HardyCausaloid model, with its ratio form of well-definedness, and do not use IsCausaloidOf, which demands fiducial-ness at every region.

Reused from HardyCausaloid: Model, Region, Fiducial, Causaloid, Conditional. New and reusable beyond this mission: Kraus-form superoperators with countable instruments, and the superoperator product. Proofs of any milestone are welcome, as are the framework theorems of the HardyCausaloid mission, which this mission does not pose again.

Selected references

  • L. Hardy, Formalism Locality in Quantum Theory and Quantum Gravity, arXiv preprint, 2008. https://arxiv.org/abs/0804.0054
  • L. Hardy, Towards Quantum Gravity: A Framework for Probabilistic Theories with Non-Fixed Causal Structure, J. Phys. A 40, 2007. https://arxiv.org/abs/gr-qc/0608043
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MetrologyQuantum Error CorrectionQuantum Information·Captain: iris

Optimal probes and error-correction schemes in multi-parameter quantum metrology: the minimum cost of joint error-corrected multi-parameter estimation is an explicit semidefinite programResearch Paper

Motivation

Quantum metrology studies how well unknown parameters of a physical process can be estimated when the probe is a quantum system. With NNN uncorrelated repetitions, or total interrogation time TTT under noise, the estimation error of a parameter typically scales as 1/T1/\sqrt{T}1/T​ (the standard scaling). Noiseless coherent evolution allows Heisenberg scaling (HS), an error of order 1/T1/T1/T. Under Markovian noise HS is usually lost, but a line of work showed that quantum error correction (QEC) can restore it: if the Hamiltonian is not in the Lindblad span of the noise (the HNLS condition), a suitable code removes the noise while keeping the signal (Demkowicz-Dobrzański, Czajkowski, Sekatski 2017; Zhou, Zhang, Preskill, Jiang 2018). Those results concern a single parameter.

Many sensing tasks estimate several parameters at once, for instance the three components of a magnetic field. Górecki, Zhou, Jiang and Demkowicz-Dobrzański (arXiv:1901.00896, Quantum 4, 288 (2020)) extend the HNLS condition to PPP parameters and, for protocols that protect all parameters in a single code space, give an exact finite-dimensional recipe for the optimal probe state, code and measurement. That recipe is the subject of this mission.

Setting

The probe is HS=Cd\mathcal H_S=\mathbb C^dHS​=Cd and the parameters ω=(ω1,…,ωP)\boldsymbol\omega=(\omega_1,\dots,\omega_P)ω=(ω1​,…,ωP​) enter through Hermitian generators G1,…,GPG_1,\dots,G_PG1​,…,GP​. The noise is described by a real subspace S\mathcal SS of Hermitian matrices containing 1d\mathbb 1_d1d​ (the Lindblad span). Theorem 2 fixes an orthonormal basis 1d/d,{Gi},{Si},{Ri}\mathbb 1_d/\sqrt d,\{G_i\},\{S_i\},\{R_i\}1d​/d​,{Gi​},{Si​},{Ri​} of the Hermitian d×dd\times dd×d matrices under the Hilbert–Schmidt product Tr(AB)\mathrm{Tr}(AB)Tr(AB) with S=spanR{1d,Si}\mathcal S=\mathrm{span}_{\mathbb R}\{\mathbb 1_d,S_i\}S=spanR​{1d​,Si​}; this encodes HNLS with {Gi}⊂S⊥\{G_i\}\subset\mathcal S^\perp{Gi​}⊂S⊥.

A JNT-QEC protocol chooses an ancilla HA=Ca\mathcal H_A=\mathbb C^aHA​=Ca of any dimension, a code space HC⊆HS⊗HA\mathcal H_C\subseteq\mathcal H_S\otimes\mathcal H_AHC​⊆HS​⊗HA​ with projection ΠC\Pi_CΠC​ satisfying the QEC condition ΠC(X⊗1)ΠC∝ΠC\Pi_C(X\otimes\mathbb 1)\Pi_C\propto\Pi_CΠC​(X⊗1)ΠC​∝ΠC​ for all X∈SX\in\mathcal SX∈S, and an input ∣ψin⟩∈HC|\psi_{\rm in}\rangle\in\mathcal H_C∣ψin​⟩∈HC​. Ideal error correction leaves the effective evolution

∣ψω⟩=exp⁡(−iT∑jωj ΠC(Gj⊗1)ΠC)∣ψin⟩.|\psi_{\boldsymbol\omega}\rangle=\exp\Big(-iT\sum_j\omega_j\,\Pi_C(G_j\otimes\mathbb 1)\Pi_C\Big)|\psi_{\rm in}\rangle .∣ψω​⟩=exp(−iTj∑​ωj​ΠC​(Gj​⊗1)ΠC​)∣ψin​⟩.

A POVM {Mℓ}\{M_\ell\}{Mℓ​} and an estimator ω~(ℓ)\tilde{\boldsymbol\omega}(\ell)ω~(ℓ) are applied; the estimator is locally unbiased at ω=0\boldsymbol\omega=0ω=0 when ∑ℓω~j(ℓ)pℓ(0)=0\sum_\ell\tilde\omega_j(\ell)p_\ell(0)=0∑ℓ​ω~j​(ℓ)pℓ​(0)=0 and ∑ℓω~j(ℓ)∂ipℓ(0)=δij\sum_\ell\tilde\omega_j(\ell)\partial_ip_\ell(0)=\delta_{ij}∑ℓ​ω~j​(ℓ)∂i​pℓ​(0)=δij​, where pℓ(ω)=⟨ψω∣Mℓ∣ψω⟩p_\ell(\boldsymbol\omega)=\langle\psi_{\boldsymbol\omega}|M_\ell|\psi_{\boldsymbol\omega}\ranglepℓ​(ω)=⟨ψω​∣Mℓ​∣ψω​⟩. With covariance Σij=∑ℓpℓ(0)ω~i(ℓ)ω~j(ℓ)\Sigma_{ij}=\sum_\ell p_\ell(0)\tilde\omega_i(\ell)\tilde\omega_j(\ell)Σij​=∑ℓ​pℓ​(0)ω~i​(ℓ)ω~j​(ℓ) and a real positive definite cost matrix WWW, the figure of merit is ΔW2ω~=Tr(WΣ)\Delta^2_W\tilde{\boldsymbol\omega}=\mathrm{Tr}(W\Sigma)ΔW2​ω~=Tr(WΣ).

Formalization targets

Goal: Theorem 2, corrected

With GiR,BiG^R_i,B_iGiR​,Bi​ Hermitian (P+1)×(P+1)(P+1)\times(P+1)(P+1)×(P+1) matrices, νi∈R\nu_i\in\mathbb Rνi​∈R, K,YK,YK,Y real P×PP\times PP×P matrices and Γij=Im[GjR]i0\Gamma_{ij}=\mathrm{Im}[G^R_j]_{i0}Γij​=Im[GjR​]i0​, the minimum JNT-QEC cost exists and equals

ΔW2ω~=14T2min⁡ Tr Ys.t.Q≥0, (YKK1)≥0, (K11ΓW−1)≥0,\Delta^2_W\tilde{\boldsymbol\omega}=\frac1{4T^2}\min\ \mathrm{Tr}\,Y\quad\text{s.t.}\quad Q\ge0,\ \begin{pmatrix}Y&K\\K&\mathbb 1\end{pmatrix}\ge0,\ \begin{pmatrix}K&\mathbb 1\\\mathbb 1&\Gamma\sqrt{W^{-1}}\end{pmatrix}\ge0,ΔW2​ω~=4T21​min TrYs.t.Q≥0, (YK​K1​)≥0, (K1​1ΓW−1​​)≥0, Q=1P+1⊗1dd+∑i(GiR)T⊗Gi+∑iνi1P+1⊗Si+∑iBi⊗Ri.Q=\mathbb 1_{P+1}\otimes\tfrac{\mathbb 1_d}{d}+\sum_i(G^R_i)^T\otimes G_i+\sum_i\nu_i\mathbb 1_{P+1}\otimes S_i+\sum_iB_i\otimes R_i .Q=1P+1​⊗d1d​​+i∑​(GiR​)T⊗Gi​+i∑​νi​1P+1​⊗Si​+i∑​Bi​⊗Ri​.

The printed SDP (8) is corrected. The paper writes the block w1Pw\mathbb 1_Pw1P​ and the value P4T2min⁡w\frac{P}{4T^2}\min w4T2P​minw. That is false for general WWW: take two qubits (d=4d=4d=4, P=2P=2P=2), no noise, G1=12σz⊗1G_1=\tfrac12\sigma_z\otimes\mathbb 1G1​=21​σz​⊗1, G2=121⊗σzG_2=\tfrac12\mathbb 1\otimes\sigma_zG2​=21​1⊗σz​, W=diag(1,100)W=\mathrm{diag}(1,100)W=diag(1,100). Every feasible point of the printed program has w≥400w\ge400w≥400, so it predicts a cost of at least 200/T2200/T^2200/T2, while the input ∣+⟩∣+⟩|+\rangle|+\rangle∣+⟩∣+⟩ with a σy\sigma_yσy​ measurement on each qubit is locally unbiased with cost 101/T2101/T^2101/T2. The step "Pmin⁡w=min⁡Tr(K2)P\min w=\min\mathrm{Tr}(K^2)Pminw=minTr(K2)" on p.9 fails unless K∝1K\propto\mathbb 1K∝1. Replacing w1Pw\mathbb 1_Pw1P​ by a matrix YYY and P wP\,wPw by Tr Y\mathrm{Tr}\,YTrY is exact.

Milestones

The Matsumoto bound (11) and its two halves (12)–(14), (15)–(17); its frame form (19); the derivative identity and the fixed-code program (21); the code-matrix characterization (25) with ancilla (P+1)d(P+1)d(P+1)d; the program (26); the rotation making ΓW−1≥0\Gamma\sqrt{W^{-1}}\ge0ΓW−1​≥0; the two Schur-complement relations (27), (28). The printed (19) and (21) also omit the constraint that the frame is orthogonal to the probe state, which the text imposes; without it they are false, and the milestones state the corrected forms.

Significance

Theorem 2 turns the joint optimization over input state, error-correcting code and measurement, a non-convex search over an unbounded family of ancilla dimensions and POVMs, into one semidefinite program of fixed size (P+1)d(P+1)d(P+1)d. The optimum can then be computed numerically, compared with protocols that sense each parameter in a separate code (for which joint protection gains at most a factor PPP, Eq. (29)), and used to certify optimality of explicit protocols such as those for SU(ddd) generators in Sec. 6. The derivation also gives a self-contained proof of the saturability of the Matsumoto bound for pure states.

None of this is machine-checked. The mission produces a formal statement of the corrected theorem, and of the printed slips in (8), (19) and (21), and the formal infrastructure of local unbiasedness, POVMs with countably many outcomes and pure-state estimation that other metrology results can reuse.

Difficulty

The obvious route is the quantum Cramér–Rao bound, but in the multi-parameter case it is not saturable in general, because the optimal measurements for different parameters need not be compatible; minimizing it over codes would not identify the optimal protocol. The Holevo–Cramér–Rao bound is saturable but is itself an optimization. The proof needs the pure-state Matsumoto form, a Naimark dilation of a POVM with possibly infinitely many outcomes, an isometric reduction to dimension 2P+12P+12P+1, and a purification argument that controls the ancilla dimension. The final step from (26) to an SDP needs a polar decomposition and two Schur complements; that step is where the printed (8) goes wrong.

Formalization scope

Everything is finite-dimensional: HS⊗HA\mathcal H_S\otimes\mathcal H_AHS​⊗HA​ is indexed by Fin d × Fin a, probe first, and QQQ by Fin (P+1) × Fin d, reference space first. POVMs are indexed by N\mathbb NN with unconditional sums (finite POVMs padded with zeros), and the variances are required to be summable. Derivatives ∂ipℓ\partial_ip_\ell∂i​pℓ​ are genuine Fréchet derivatives of the evolution (20); writing their closed form into the definition would make the derivative milestone definitional. The ancilla dimension is quantified over all of N\mathbb NN and never fixed. W−1\sqrt{W^{-1}}W−1​ is the positive semidefinite root. Every inverse (DTD)−1(D^TD)^{-1}(DTD)−1, (ΓTΓ)−1(\Gamma^T\Gamma)^{-1}(ΓTΓ)−1 is taken only where DDD, Γ\GammaΓ are invertible, and minima are stated as attained least elements, with the degenerate infeasible case written out where it can occur.

Contributions welcome: Schur-complement lemmas for real block matrices, a Naimark dilation for countable POVMs, purification of a positive matrix with an ancilla of dimension equal to its size, and a proof that the corrected SDP is feasible and attains its minimum.

Selected references

  • W. Górecki, S. Zhou, L. Jiang, R. Demkowicz-Dobrzański, Optimal probes and error-correction schemes in multi-parameter quantum metrology, Quantum 4, 288 (2020); arXiv:1901.00896v4. https://arxiv.org/abs/1901.00896v4
  • K. Matsumoto, A new approach to the Cramér–Rao-type bound of the pure-state model, J. Phys. A 35, 3111 (2002). https://doi.org/10.1088/0305-4470/35/13/307
  • R. Demkowicz-Dobrzański, J. Czajkowski, P. Sekatski, Adaptive quantum metrology under general Markovian noise, Phys. Rev. X 7, 041009 (2017). https://doi.org/10.1103/PhysRevX.7.041009
  • S. Zhou, M. Zhang, J. Preskill, L. Jiang, Achieving the Heisenberg limit in quantum metrology using quantum error correction, Nat. Commun. 9, 78 (2018). https://doi.org/10.1038/s41467-017-02510-3
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Linear algebraQuantum Information·Captain: iris

Towards Large-Scale Quantum Computation IV: the phase-insensitive gate distance sqrt((m − |tr(U†V)|)/m) satisfies the triangle inequality on the unitary group U(m)Textbook

Why a phase-insensitive distance between gates

A quantum computer protected by an error-correcting code can apply only a small set of gates fault-tolerantly, so every other gate must be approximated by a sequence from that set. The existence of short approximating sequences is the content of the Solovay–Kitaev theorem (Kitaev 1997; Nielsen and Chuang 2000). A practical search for the best sequence needs an objective, that is, a number saying how far a candidate sequence is from the target gate.

Fowler's 2005 thesis (arXiv:quant-ph/0506126v1, Ch. 10) searches numerically for optimal fault-tolerant approximations of single-qubit gates on the Steane code. It uses a distance that does not see the global phase of a gate, because two gates that differ by a phase act identically on states up to an unobservable factor. A distance that does see it forces the search to match an irrelevant phase, which the thesis says leads to "unnecessarily long phase correct approximating sequences". Section 10.1 introduces this distance in one display and asserts, in the following sentences, the properties for which it was chosen. This mission formalizes those properties.

The gate distance on U(m)U(m)U(m)

Fix an integer m≥1m\ge 1m≥1. The unitary group U(m)U(m)U(m) is the group of m×mm\times mm×m complex matrices UUU with U†U=IU^\dagger U=IU†U=I, where U†U^\daggerU† is the conjugate transpose. The trace of a square matrix is written tr\mathrm{tr}tr, and ∣⋅∣|\cdot|∣⋅∣ is the modulus of a complex number.

For U,V∈U(m)U,V\in U(m)U,V∈U(m), the gate distance of (10.1) is

dist(U,V)=m−∣tr(U†V)∣m.\mathrm{dist}(U,V)=\sqrt{\frac{m-|\mathrm{tr}(U^\dagger V)|}{m}} .dist(U,V)=mm−∣tr(U†V)∣​​.

The thesis writes the second argument as UlU_lUl​, a sequence of at most lll gates from a finite generating set, and applies the formula to arbitrary elements in (10.2).

A global phase is a factor eiαe^{i\alpha}eiα with α\alphaα real. For U∈U(m)U\in U(m)U∈U(m), the matrix eiαUe^{i\alpha}UeiαU again lies in U(m)U(m)U(m). In the Lean development this gate is phaseShift α U, and the distance is gateDist U V.

Formalization targets

Goal: the triangle inequality (10.2)

For every m≥1m\ge 1m≥1 and all U,V,W∈U(m)U,V,W\in U(m)U,V,W∈U(m),

dist(U,W)≤dist(U,V)+dist(V,W).\mathrm{dist}(U,W)\le\mathrm{dist}(U,V)+\mathrm{dist}(V,W).dist(U,W)≤dist(U,V)+dist(V,W).

The thesis, p.110, gives this as the reason the square root appears in (10.1).

Milestone: the radicand lies between 0 and 1

For every m≥1m\ge 1m≥1 and all U,V∈U(m)U,V\in U(m)U,V∈U(m),

0≤m−∣tr(U†V)∣m≤1.0\le\frac{m-|\mathrm{tr}(U^\dagger V)|}{m}\le 1 .0≤mm−∣tr(U†V)∣​≤1.

Milestone: the distance ignores global phase

For every m≥1m\ge 1m≥1, all U,V∈U(m)U,V\in U(m)U,V∈U(m) and all real α,β\alpha,\betaα,β,

dist(eiαU,eiβV)=dist(U,V).\mathrm{dist}(e^{i\alpha}U,e^{i\beta}V)=\mathrm{dist}(U,V).dist(eiαU,eiβV)=dist(U,V).

The thesis states this by contrast with the trace distance, which "does not ignore global phase". The formal statement is the reading with an independent phase on each argument.

What the result gives

The result itself. The inequality is what permits the distance to measure accumulated error. If a gate is replaced by an approximation and that by a further approximation, the total error is bounded by the sum of the two. Together with phase invariance, the inequality says that dist\mathrm{dist}dist descends to a function satisfying the triangle inequality on the projective unitary group, the group of gates modulo global phase, which is the object that matters physically.

Although the thesis calls dist\mathrm{dist}dist a metric, it is not a metric on U(m)U(m)U(m) itself, since dist(U,−U)=0\mathrm{dist}(U,-U)=0dist(U,−U)=0. No definiteness claim is part of this mission, because the source states none.

Formalizing it. The inequality is true as printed and elementary in its objects, but the thesis gives no proof, only the assertion. The remaining work is therefore to supply a proof and have it machine-checked, for every dimension rather than for the single-qubit case the chapter uses. No machine-checked proof of this inequality is known to the authors of this mission. The closest related formal statement, QAlgorithms.Papers.Independent.Intakenext100.P82.distance_controls_absolute_trace, concerns a differently normalized single-qubit distance and a different claim, and is itself unproved.

Where the difficulty lies

The obvious first attempt works directly with the radicand. It fails: (m−∣tr(U†V)∣)/m(m-|\mathrm{tr}(U^\dagger V)|)/m(m−∣tr(U†V)∣)/m does not itself satisfy the triangle inequality. In U(2)U(2)U(2), take U=IU=IU=I, V=diag(1,eiθ)V=\mathrm{diag}(1,e^{i\theta})V=diag(1,eiθ) and W=diag(1,e2iθ)W=\mathrm{diag}(1,e^{2i\theta})W=diag(1,e2iθ). The radicand from UUU to WWW is about θ2/2\theta^2/2θ2/2 for small θ\thetaθ, while the two steps give about θ2/8\theta^2/8θ2/8 each. This is the point of the thesis's remark that the overall square root "is required".

The second obstacle is that the trace is not multiplicative. The three quantities tr(U†W)\mathrm{tr}(U^\dagger W)tr(U†W), tr(U†V)\mathrm{tr}(U^\dagger V)tr(U†V) and tr(V†W)\mathrm{tr}(V^\dagger W)tr(V†W) are not related by any identity, even though U†W=(U†V)(V†W)U^\dagger W=(U^\dagger V)(V^\dagger W)U†W=(U†V)(V†W). Moreover, the modulus discards the phase of each trace independently, so the inequality cannot be read off from a single fixed norm on matrices applied to UUU, VVV and WWW.

Formalization scope

U(m)U(m)U(m) is Matrix.unitaryGroup (Fin m) ℂ, U†U^\daggerU† is Uᴴ, ∣⋅∣|\cdot|∣⋅∣ is the norm on ℂ, and the square root is Real.sqrt. Every theorem assumes 0 < m. The formula is 0/00/00/0 at m=0m=0m=0, and the Lean junk value there is 000. The definition gateDist does not build in nonnegativity of the radicand: because Real.sqrt returns 000 on negative input, the lower bound of the first milestone is what shows that the definition is the book's, and it is stated separately.

The statements cover every dimension m≥1m\ge 1m≥1 and every triple in U(m)U(m)U(m), not only the single-qubit case m=2m=2m=2 used later in the chapter. A trivializing formalization is excluded by proved sanity checks kept outside the mission: dist(I,−I)=0\mathrm{dist}(I,-I)=0dist(I,−I)=0 and dist(I,Z)=1\mathrm{dist}(I,Z)=1dist(I,Z)=1 in U(2)U(2)U(2), where Z=diag(1,−1)Z=\mathrm{diag}(1,-1)Z=diag(1,−1), so the definition is neither constant nor sensitive to phase.

A complete development needs only Mathlib's unitary group, the matrix trace and basic facts on inner product spaces. General facts about traces of unitary matrices that do not mention dist\mathrm{dist}dist are reusable beyond this mission, and contributions that factor them out are welcome. The trace distance mentioned in the source, and the numerical search procedure of §10.1, are out of scope.

Selected references

  • A. G. Fowler, Towards Large-Scale Quantum Computation, PhD thesis, School of Physics, The University of Melbourne, 2005. arXiv:quant-ph/0506126v1, §10.1, (10.1)–(10.2), p.110.
  • A. Yu. Kitaev, Quantum computations: algorithms and error correction, Russian Mathematical Surveys 52(6):1191–1249, 1997. doi:10.1070/RM1997v052n06ABEH002155
  • M. A. Nielsen and I. L. Chuang, Quantum Computation and Quantum Information, Cambridge University Press, 2000 (link: 10th anniversary edition, 2010). doi:10.1017/CBO9780511976667
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Linear algebraMathematical PhysicsQuantum Information·Captain: iris

BCS-like Modewise Entanglement of Fermion Gaussian States: under any bipartition of modes a pure Gaussian state is a product of two-mode squeezed pairs and vacuum modes in locally transformed modesResearch Paper

Motivation

Quadratic fermion Hamiltonians H=∑Cijbi†bj+∑(Aijbi†bj†+h.c.)H=\sum C_{ij}b_i^\dagger b_j+\sum(A_{ij}b_i^\dagger b_j^\dagger+\text{h.c.})H=∑Cij​bi†​bj​+∑(Aij​bi†​bj†​+h.c.) describe BCS superconductivity and the Hubbard model in mean-field approximation, and several exactly solvable spin chains after a Jordan–Wigner transformation. Their ground states, and all their eigenstates with a definite set of quasi-particle excitations, are fermion Gaussian states. Studies of entanglement in many-body systems therefore need to know how such a state is entangled across a split of its modes into two groups.

For bosons the answer was known: a pure Gaussian state is, after local symplectic transformations, a product of two-mode squeezed pairs (Botero–Reznik 2003; Giedke–Eisert–Cirac–Plenio 2003). Botero and Reznik (2004) proved the fermionic counterpart: under any bipartition, a pure fermion Gaussian state has the structure of a BCS wave function, a product of entangled mode pairs and vacuum modes, in a mode basis adapted to the state and the partition. The same paper extends the matrix form of the result to "isotropic" mixed states.

Setting

Operators are complex matrices on a finite-dimensional space Cι\mathbb C^\iotaCι. A family of modes (bi)i∈μ(b_i)_{i\in\mu}(bi​)i∈μ​ satisfies the canonical anticommutation relations if {bi,bj}=0\{b_i,b_j\}=0{bi​,bj​}=0 and {bi,bj†}=δij1\{b_i,b_j^\dagger\}=\delta_{ij}\mathbb 1{bi​,bj†​}=δij​1. Its quadratures are the 2∣μ∣2|\mu|2∣μ∣ Hermitian operators γ(i,0)=bi+bi†\gamma_{(i,0)}=b_i+b_i^\daggerγ(i,0)​=bi​+bi†​ and γ(i,1)=i(bi−bi†)\gamma_{(i,1)}=i(b_i-b_i^\dagger)γ(i,1)​=i(bi​−bi†​); the relations become the Clifford algebra {γα,γβ}=2δαβ\{\gamma_\alpha,\gamma_\beta\}=2\delta_{\alpha\beta}{γα​,γβ​}=2δαβ​.

A canonical family obtained from bbb is a family ci=∑j(uijbj+vijbj†)c_i=\sum_j(u_{ij}b_j+v_{ij}b_j^\dagger)ci​=∑j​(uij​bj​+vij​bj†​) that again satisfies the relations. On quadratures, these transformations are exactly the real orthogonal matrices O∈O(2N)O\in O(2N)O∈O(2N), improper ones included.

A unit vector ψ\psiψ is a pure fermion Gaussian state if, for some canonical family ccc and signs λk=±1\lambda_k=\pm1λk​=±1, every factor ρ~k=12(1−λk[ck†,ck])\tilde\rho_k=\frac12(\mathbb 1-\lambda_k[c_k^\dagger,c_k])ρ~​k​=21​(1−λk​[ck†​,ck​]) of the product form (4) fixes ψ\psiψ. In other words, ψ\psiψ is the vacuum of the modes ckc_kck​, except that some of them are occupied.

The fermion covariance matrix (FCM) of ψ\psiψ is the real antisymmetric matrix Mαβ=12i⟨ψ,[γα,γβ]ψ⟩M_{\alpha\beta}=\frac1{2i}\langle\psi,[\gamma_\alpha,\gamma_\beta]\psi\rangleMαβ​=2i1​⟨ψ,[γα​,γβ​]ψ⟩. With J2=(0−110)J_2=\begin{pmatrix}0&-1\\1&0\end{pmatrix}J2​=(01​−10​), every real antisymmetric matrix is orthogonally equivalent to a Williamson form ⨁iλiJ2\bigoplus_i\lambda_iJ_2⨁i​λi​J2​ with λi≥0\lambda_i\ge0λi​≥0. Pure states are characterized by M2=−1M^2=-\mathbb 1M2=−1.

A bipartition of the modes is a split b=(bA,bB)b=(b_A,b_B)b=(bA​,bB​), with AAA indexed by α\alphaα (mmm modes) and BBB by β\betaβ (nnn modes). A transformation is local if each new AAA-mode is a combination of AAA-modes and their adjoints only, and likewise for BBB.

Formalization targets

Goal: the modewise decomposition (main result, (2)–(3), p.2)

For every pure Gaussian state ψ\psiψ of the modes (bA,bB)(b_A,b_B)(bA​,bB​) there are local canonical families A~\tilde AA~ (from bAb_AbA​) and B~\tilde BB~ (from bBb_BbB​), a number s≤min⁡(m,n)s\le\min(m,n)s≤min(m,n) of disjoint pairs (A~k,B~k)(\tilde A_k,\tilde B_k)(A~k​,B~k​), angles θk∈(0,π/4]\theta_k\in(0,\pi/4]θk​∈(0,π/4] and a unit vector ∣0⟩|0\rangle∣0⟩ annihilated by every mode of A~\tilde AA~ and B~\tilde BB~, such that

ψ=∏k=1s(cos⁡θk−sin⁡θk A~k†B~k†)∣0⟩,\psi=\prod_{k=1}^s\big(\cos\theta_k-\sin\theta_k\,\tilde A_k^\dagger\tilde B_k^\dagger\big)|0\rangle,ψ=k=1∏s​(cosθk​−sinθk​A~k†​B~k†​)∣0⟩,

that is, a product of two-mode squeezed states cos⁡θk∣00⟩−sin⁡θk∣11⟩\cos\theta_k|00\rangle-\sin\theta_k|11\ranglecosθk​∣00⟩−sinθk​∣11⟩ and the vacuum of all other modes.

Milestones

The milestones follow the paper's proof:

  1. the Clifford relations (5)–(6);
  2. O(2N)O(2N)O(2N) acts canonically, with the covariance law M↦OMOTM\mapsto OMO^TM↦OMOT;
  3. the FCM is real and antisymmetric (8);
  4. the Williamson form (9);
  5. the purity criterion −M2=1-M^2=\mathbb 1−M2=1;
  6. the block identities (17), (18), (20a), (20b) and (21)–(22);
  7. the decoupling of modes with eigenvalue λ0\lambda_0λ0​;
  8. the isotropic normal form (11)–(12) for every real antisymmetric MMM with M2=−λ02M^2=-\lambda_0^2M2=−λ02​;
  9. the pure-state correspondence between an FCM and the operators that annihilate the state;
  10. the identity T∣00⟩=cos⁡θ∣00⟩−sin⁡θ∣11⟩T|00\rangle=\cos\theta|00\rangle-\sin\theta|11\rangleT∣00⟩=cosθ∣00⟩−sinθ∣11⟩ for T=exp⁡[−(a†b†+ab)θ]T=\exp[-(a^\dagger b^\dagger+ab)\theta]T=exp[−(a†b†+ab)θ], whose FCM is the block (12) at λ=cos⁡2θ\lambda=\cos2\thetaλ=cos2θ, κ=sin⁡2θ\kappa=\sin2\thetaκ=sin2θ.

Significance

The theorem settles the structure of bipartite mode entanglement for every pure fermion Gaussian state. It reduces any entanglement quantity of such a state to its values on single pairs: the entanglement of modes EME_MEM​ is the sum of the pair entropies of the Schmidt coefficients cos⁡2θk,sin⁡2θk\cos^2\theta_k,\sin^2\theta_kcos2θk​,sin2θk​. It also identifies the vacuum and the excitations with respect to which a correlated fermion state looks like a BCS state. Together with the bosonic result, it shows that pure Gaussian states are entangled pairwise whatever the statistics.

The result is proved in the paper. As far as the platform's catalog shows, no part of it has been formalized: there is no modewise decomposition, and Mathlib has no normal form of real antisymmetric matrices. A formalization yields:

  • the real skew-symmetric normal form (9), which is reusable well beyond fermions;
  • the isotropic normal form (11)–(12) as a pure matrix theorem;
  • a small, representation-independent layer for anticommutation relations, quadratures, canonical families and covariance matrices.

The printed (20b) and the symplectic clause of (22) fail when the common local eigenvalue is λ=0\lambda=0λ=0 (they divide (18) by λ\lambdaλ). The mission states them with the minimal correction λ≠0\lambda\ne0λ=0. The normal form and the main result do not depend on the correction, because at λ=0\lambda=0λ=0 the diagonal block vanishes and any orthogonal transformation works.

Difficulty

The natural first idea, a Schmidt decomposition of ψ\psiψ across the split, does not apply directly: a fermionic Fock space has no natural tensor-product structure over modes, and the Schmidt vectors need not be Gaussian. The paper works instead with the covariance matrix.

That route has two hard steps. The first is the real normal form of an antisymmetric matrix, which needs spectral theory of normal real matrices that Mathlib does not package. The second is the simultaneous normal form (11): after local Williamson forms, the off-diagonal block must be shown to pair equal eigenvalues, the degeneracies must be shown to match for λ≠λ0\lambda\ne\lambda_0λ=λ0​, and a single local orthogonal transformation must straighten each block while keeping the diagonal block intact. Doing this needs regrouping of modes by eigenvalue and careful reindexing. Turning the matrix normal form back into a statement about the vector ψ\psiψ needs a third, purely operator-level step: annihilators of ψ\psiψ read off from the eigenvectors of MMM, and an explicit computation with commuting entangling unitaries.

Formalization scope

All operators are Matrix ι ι ℂ on an arbitrary finite type, so the statements hold in every finite-dimensional representation of the anticommutation relations, not only the Fock space. Mode sets are arbitrary finite types and may be empty; the partition is α ⊕ β.

The conventions are fixed throughout:

  • quadratures are indexed by μ × Fin 2;
  • the FCM carries the prefactor 1/(2i)1/(2i)1/(2i) and is stored as its real part;
  • covariance matrices on a bipartition are indexed by (α × Fin 2) ⊕ (β × Fin 2);
  • pairs are injective maps Fin s ↪ α, Fin s ↪ β instead of a re-ordering;
  • ∣11⟩=a†b†∣00⟩|11\rangle=a^\dagger b^\dagger|00\rangle∣11⟩=a†b†∣00⟩;
  • the relation tan⁡2θ=κ/λ\tan2\theta=\kappa/\lambdatan2θ=κ/λ is stated as λ=cos⁡2θ\lambda=\cos2\thetaλ=cos2θ, κ=sin⁡2θ\kappa=\sin2\thetaκ=sin2θ.

Improper canonical transformations are allowed, as the paper allows them: a single occupied mode on side AAA forces A~=b†\tilde A=b^\daggerA~=b†.

Two formalizations of the goal would be trivial, and both are excluded. If the new modes were not required to be local, s=0s=0s=0 would always work. If the vector ∣0⟩|0\rangle∣0⟩ were not required to be killed by every new mode, any vector could serve.

All definitions are local to this mission. The published fermionic layers fix a qubit representation, use other Gaussianity predicates or the opposite covariance sign, so they are not reused. Contributions are welcome on the normal form (9), which is self-contained linear algebra, on the block lemmas (17)–(22), and on the operator identities of the last two milestones.

Selected references

  • A. Botero, B. Reznik, BCS-like Modewise Entanglement of Fermion Gaussian States, Phys. Lett. A 331 (2004) 39–44; arXiv:quant-ph/0404176v3. https://arxiv.org/abs/quant-ph/0404176
  • A. Botero, B. Reznik, Modewise entanglement of Gaussian states, Phys. Rev. A 67 (2003) 052311. https://arxiv.org/abs/quant-ph/0209026
  • G. Giedke, J. Eisert, J. I. Cirac, M. B. Plenio, Entanglement transformations of pure Gaussian states, Quantum Inf. Comput. 3 (2003) 211–223. https://arxiv.org/abs/quant-ph/0301038
  • P. Zanardi, Quantum entanglement in fermionic lattices, Phys. Rev. A 65 (2002) 042101. https://arxiv.org/abs/quant-ph/0104114
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Functional AnalysisHarmonic AnalysisProbability·Captain: iris

A Class of Gaussian Processes with Fractional Spectral Measures: The Wick-Ito Integral Against the Derivative Process Is the Limit of Wick Riemann SumsResearch Paper

Motivation

A centered Gaussian process with stationary increments is determined by a spectral measure σ\sigmaσ on R\mathbb RR: its covariance is ∫χt(u)χs(u)‾ dσ(u)\int\chi_t(u)\overline{\chi_s(u)}\,d\sigma(u)∫χt​(u)χs​(u)​dσ(u) with χt(u)=(eitu−1)/u\chi_t(u)=(e^{itu}-1)/uχt​(u)=(eitu−1)/u. Brownian motion corresponds to Lebesgue measure and fractional Brownian motion to a power density. When σ\sigmaσ has a density mmm, a stochastic calculus for such processes can be built inside Hida's white noise space, with Wick products replacing pointwise products and Kondratiev spaces of stochastic distributions as the ambient space (Alpay–Attia–Levanony, arXiv:1008.0186). In that setting the derivative of the process exists only as a stochastic distribution.

Alpay, Jorgensen and Levanony (arXiv:1009.0233) treat the opposite case: singular spectral measures, such as the Cantor-type measures σm\sigma_mσm​ of Jorgensen and Pedersen, which have Hausdorff dimension 1/21/21/2 and nevertheless admit an orthonormal basis of exponentials in L2(dσ)L^2(d\sigma)L2(dσ) (Jorgensen–Pedersen 1998). They show that for this class the derivative process lives in the white noise space itself, and they use this to obtain a sharper Wick–Itô integration formula. That formula, Theorem 7.1, is the goal of this mission.

Setting

A spectral setting is a finite Borel measure σ\sigmaσ on R\mathbb RR supported in [−12,12][-\tfrac12,\tfrac12][−21​,21​] with a sequence λ0=0,λ1,λ2,…\lambda_0=0,\lambda_1,\lambda_2,\dotsλ0​=0,λ1​,λ2​,… such that the exponentials eλn(u)=eiλnue_{\lambda_n}(u)=e^{i\lambda_nu}eλn​​(u)=eiλn​u form an orthonormal basis of L2(dσ)L^2(d\sigma)L2(dσ). Fourier transforms carry a plus sign and no 2π2\pi2π: ψ^(u)=∫eiuxψ(x) dx\widehat\psi(u)=\int e^{iux}\psi(x)\,dxψ​(u)=∫eiuxψ(x)dx and σ^(t)=∫eitu dσ(u)\widehat\sigma(t)=\int e^{itu}\,d\sigma(u)σ(t)=∫eitudσ(u).

Let (hn)n≥0(h_n)_{n\ge0}(hn​)n≥0​ be a real orthonormal basis of L2(R,dx)L^2(\mathbb R,dx)L2(R,dx) (the paper uses the Hermite functions). The unitary W:L2(dσ)→L2(R,dx)W:L^2(d\sigma)\to L^2(\mathbb R,dx)W:L2(dσ)→L2(R,dx) with W(eλn)=hnW(e_{\lambda_n})=h_nW(eλn​​)=hn​ transports multiplication by uuu to a bounded self-adjoint operator T=WMuW∗T=WM_uW^*T=WMu​W∗, and for a Schwartz function ψ\psiψ one sets Qσψ=ψ^(T)h0Q_\sigma\psi=\widehat\psi(T)h_0Qσ​ψ=ψ​(T)h0​. An isometry property, ∥Qσψ∥2=∫∣ψ^∣2dσ\|Q_\sigma\psi\|^2=\int|\widehat\psi|^2d\sigma∥Qσ​ψ∥2=∫∣ψ​∣2dσ, extends QσQ_\sigmaQσ​ to functions that are uniform limits of sn^\widehat{s_n}sn​​, in particular to ft=1[0,t]^f_t=\widehat{1_{[0,t]}}ft​=1[0,t]​​.

The white noise measure PPP on Ω=S′\Omega=\mathcal S'Ω=S′ has characteristic functional ∫e−i⟨ω,s⟩dP(ω)=e−∥s∥2/2\int e^{-i\langle\omega,s\rangle}dP(\omega)=e^{-\|s\|^2/2}∫e−i⟨ω,s⟩dP(ω)=e−∥s∥2/2. The map s↦s~=⟨⋅,s⟩s\mapsto\widetilde s=\langle\cdot,s\rangles↦s=⟨⋅,s⟩ extends to an isometry f↦f~f\mapsto\widetilde ff↦f​ of L2(R,dx)L^2(\mathbb R,dx)L2(R,dx) into the white noise space W=L2(P)\mathcal W=L^2(P)W=L2(P). Put Zn=hn~Z_n=\widetilde{h_n}Zn​=hn​​. The two processes are

Xσ(t)=Qσ1[0,t]~=∑n≥0(∫0tσ^(y−λn) dy)Zn,Wσ(t)=∑n≥0σ^(t−λn) Zn.X_\sigma(t)=\widetilde{Q_\sigma1_{[0,t]}}=\sum_{n\ge0}\Big(\int_0^t\widehat\sigma(y-\lambda_n)\,dy\Big)Z_n,\qquad W_\sigma(t)=\sum_{n\ge0}\widehat\sigma(t-\lambda_n)\,Z_n .Xσ​(t)=Qσ​1[0,t]​​=n≥0∑​(∫0t​σ(y−λn​)dy)Zn​,Wσ​(t)=n≥0∑​σ(t−λn​)Zn​.

The chaos basis is Hα=∏khαk(Zk)H_\alpha=\prod_k\mathbf h_{\alpha_k}(Z_k)Hα​=∏k​hαk​​(Zk​) over finitely supported multi-indices α\alphaα, with hj\mathbf h_jhj​ the probabilists' Hermite polynomials; E[HαHβ]=δαβ α!E[H_\alpha H_\beta]=\delta_{\alpha\beta}\,\alpha!E[Hα​Hβ​]=δαβ​α!. A formal series ∑fαHα\sum f_\alpha H_\alpha∑fα​Hα​ lies in the Hilbert space Hk′\mathcal H'_kHk′​ when ∥f∥k2=∑∣fα∣2(2N)−kα<∞\|f\|_k^2=\sum|f_\alpha|^2(2\mathbb N)^{-k\alpha}<\infty∥f∥k2​=∑∣fα​∣2(2N)−kα<∞, and the Kondratiev space S−1S_{-1}S−1​ is the union of the Hk′\mathcal H'_kHk′​. The Wick product is F⋄G=∑γ(∑α+β=γfαgβ)HγF\diamond G=\sum_\gamma\big(\sum_{\alpha+\beta=\gamma}f_\alpha g_\beta\big)H_\gammaF⋄G=∑γ​(∑α+β=γ​fα​gβ​)Hγ​.

Formalization targets

Goal: Theorem 7.1

For every spectral setting, every a<ba<ba<b and every Y:[a,b]→S−1Y:[a,b]\to S_{-1}Y:[a,b]→S−1​ continuous in the strong topology of S−1S_{-1}S−1​, there is p≥1p\ge1p≥1 such that t↦Y(t)⋄Wσ(t)t\mapsto Y(t)\diamond W_\sigma(t)t↦Y(t)⋄Wσ​(t) is a continuous Hp′\mathcal H'_pHp′​-valued map and

∫abY(t)⋄Wσ(t) dt=lim⁡∣Δ∣→0∑k=0n−1Y(tk)⋄(Xσ(tk+1)−Xσ(tk))in Hp′.\int_a^bY(t)\diamond W_\sigma(t)\,dt=\lim_{|\Delta|\to0}\sum_{k=0}^{n-1}Y(t_k)\diamond\big(X_\sigma(t_{k+1})-X_\sigma(t_k)\big)\quad\text{in }\mathcal H'_p .∫ab​Y(t)⋄Wσ​(t)dt=∣Δ∣→0lim​k=0∑n−1​Y(tk​)⋄(Xσ​(tk+1​)−Xσ​(tk​))in Hp′​.

Milestones

In proof order: the spectral-pair criterion ∑λ∣σ^(t−λ)∣2=1\sum_\lambda|\widehat\sigma(t-\lambda)|^2=1∑λ​∣σ(t−λ)∣2=1 (Theorem 3.1) and the Lipschitz bound for t↦ett\mapsto e_tt↦et​ (Lemma 3.2); the white noise isometry (4.2), the chaos basis (4.3) and Våge's inequality (4.7); the expansion of QσψQ_\sigma\psiQσ​ψ (Lemma 5.1), the isometry and continuity of QσQ_\sigmaQσ​ (Theorem 5.2), its extension (Proposition 5.4) and the approximation of χt\chi_tχt​ (p.16); the law of the ZnZ_nZn​ and the expansion (6.2); the bound ∥Xσ(t)−Xσ(s)∥W≤∣t−s∣\|X_\sigma(t)-X_\sigma(s)\|_{\mathcal W}\le|t-s|∥Xσ​(t)−Xσ​(s)∥W​≤∣t−s∣ and Xσ′=WσX_\sigma'=W_\sigmaXσ′​=Wσ​ (Theorem 6.2); continuity, stationarity and unit variance of WσW_\sigmaWσ​ (Theorem 6.4); and the three steps of the proof of Theorem 7.1.

Significance

Theorem 7.1 identifies the Wick–Itô integral against the derivative process with a limit of Wick–Riemann sums of the process itself, in a single Hilbert space Hp′\mathcal H'_pHp′​. Because Wσ(t)∈WW_\sigma(t)\in\mathcal WWσ​(t)∈W, Våge's inequality is applied with the white noise norm on one factor, which is what makes the statement sharper than its counterpart for absolutely continuous σ\sigmaσ, where WWW lies only in a larger Kondratiev space. The same machinery underlies the paper's Itô formula (Theorem 8.2), which is not part of this mission.

The result is proved in the paper, partly by citation: STEP 1 refers to arXiv:1008.0186, Våge's inequality to Holden–Øksendal–Ubøe–Zhang, and Theorem 3.1 to Jorgensen–Pedersen. None of it is formalized. The mission produces machine-checked statements of the whole chain, and two printed statements are corrected along the way: Theorem 3.1 needs σ(R)=1\sigma(\mathbb R)=1σ(R)=1, and Lemma 3.2 holds with K\sqrt KK​ in place of KKK.

Difficulty

STEP 1 is the functional-analytic core: a strongly continuous curve in the inductive limit S−1S_{-1}S−1​ must lie in a single Hp′\mathcal H'_pHp′​ and be uniformly continuous there. This is a regularity property of the inductive limit (a compact subset of a DFS space is contained and compact in one step), not a pointwise estimate, and the natural attempt of choosing ppp for each ttt separately gives no uniform ppp. Våge's inequality needs the summability of ∑α(2N)−qα\sum_\alpha(2\mathbb N)^{-q\alpha}∑α​(2N)−qα for q>1q>1q>1, a combinatorial estimate over infinitely many coordinates. On the probabilistic side, the white noise measure itself requires the Bochner–Minlos theorem, and the differentiability of XσX_\sigmaXσ​ in W\mathcal WW rests on the exact identity (3.1), which fails for measures without a spectrum.

Formalization scope

Coefficients are complex throughout: Schwartz functions S(R,C)\mathcal S(\mathbb R,\mathbb C)S(R,C), L2(R;C)L^2(\mathbb R;\mathbb C)L2(R;C), L2(P;C)L^2(P;\mathbb C)L2(P;C), and formal series as families (ℕ →₀ ℕ) → ℂ. Coordinate n=0,1,…n=0,1,\dotsn=0,1,… of a multi-index carries ZnZ_nZn​ and the weight 2(n+1)2(n+1)2(n+1); it is the paper's coordinate k=n+1k=n+1k=n+1. Hk′\mathcal H'_kHk′​ is realized in ℓ2\ell^2ℓ2 through f↦(fα(2N)−kα/2)αf\mapsto(f_\alpha(2\mathbb N)^{-k\alpha/2})_\alphaf↦(fα​(2N)−kα/2)α​, so integrals are Bochner integrals in a Hilbert space. QσQ_\sigmaQσ​ is defined by the continuous functional calculus of TTT, not by its expansion; Xσ(t)X_\sigma(t)Xσ​(t) uses ft(u)=∫0teiuxdxf_t(u)=\int_0^te^{iux}dxft​(u)=∫0t​eiuxdx (an oriented integral, value ttt at u=0u=0u=0). The white noise measure PPP and the isometry f↦f~f\mapsto\widetilde ff↦f​ are parameters fixed by (4.1) and (4.2), which determine them; Bochner–Minlos is not assumed. The strong topology of S−1S_{-1}S−1​ is uniform convergence on bounded subsets of S1S_1S1​ under ⟨f,g⟩=∑α!fαgα\langle f,g\rangle=\sum\alpha!f_\alpha g_\alpha⟨f,g⟩=∑α!fα​gα​.

The basis (hn)(h_n)(hn​) is any real orthonormal basis, and the paper's condition λn∈πN0\lambda_n\in\pi\mathbb N_0λn​∈πN0​ is dropped; both are generalizations that contain the paper's case. The goal asserts continuity of the integrand and membership of the Riemann sums, so neither the integral nor the norm can take a junk value, and XσX_\sigmaXσ​, WσW_\sigmaWσ​ are constructed from σ\sigmaσ, not arbitrary processes with X′=WX'=WX′=W.

Reusable infrastructure: Kondratiev spaces and the Wick product, Våge's inequality, the Wiener–Itô chaos basis of white noise, and Fourier frames for spectral measures. Contributions of any milestone, of the Bochner–Minlos theorem for S′\mathcal S'S′, and of the summability of ∑(2N)−qα\sum(2\mathbb N)^{-q\alpha}∑(2N)−qα are welcome.

Selected references

  • D. Alpay, P. Jorgensen, D. Levanony, A class of Gaussian processes with fractional spectral measures, arXiv preprint (v1), 2010; J. Funct. Anal. 261 (2011). https://arxiv.org/abs/1009.0233
  • D. Alpay, H. Attia, D. Levanony, White noise based stochastic calculus associated with a class of Gaussian processes, arXiv preprint, 2010. https://arxiv.org/abs/1008.0186
  • P. E. T. Jorgensen, S. Pedersen, Dense analytic subspaces in fractal L2L^2L2-spaces, J. Anal. Math. 75 (1998), 185–228. https://doi.org/10.1007/BF02788699
  • H. Holden, B. Øksendal, J. Ubøe, T. Zhang, Stochastic Partial Differential Equations, Birkhäuser, 1996 (Definition 2.4.1, §2.3, Proposition 3.3.2). https://doi.org/10.1007/978-1-4684-9215-6
  • I. M. Gelfand, N. Ya. Vilenkin, Generalized Functions, Vol. 4: Applications of Harmonic Analysis, Academic Press, 1964 (Bochner–Minlos theorem).
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Operations ResearchOptimizationProbability·Captain: iris

Good Prophets Know When the End Is Near: A Heads-Up T^(1/2+ε) Periods Before the End Gives Expected Loss Against the Clairvoyant Optimum Bounded Independently of the HorizonResearch Paper

Motivation

Many online decision problems in operations research have the same shape. Requests of finitely many types arrive one per period, and each must be answered at once by an irrevocable action: an item is packed into a bin configuration, a payment is routed to a processor, a booking is accepted or rejected. The cost of the whole run depends only on how many times each action was used for each type. Bin packing, payment routing, network revenue management and AdWords-style allocation all fit this pattern.

The performance of an online policy is measured against a clairvoyant that knows the whole sample path in advance. A policy has uniform loss if its expected excess cost over the clairvoyant is bounded by a constant that does not grow with the horizon. Such guarantees were first obtained when the horizon is known (Vera and Banerjee, 2021; Arlotto and Gurvich, 2019). In practice the horizon is often not known: a selling season, a shift or a batch window may end earlier or later than planned.

S. Banerjee and D. Freund (Management Science, 2024) ask how much warning about the end is needed. Their answer: a heads-up revealing the horizon TTT at a time T^\hat TT^ with T−T^>T1/2+ϵT-\hat T>T^{1/2+\epsilon}T−T^>T1/2+ϵ suffices for uniform loss, even when the arrival distribution is also unknown. They also show that a heads-up of order T\sqrt TT​ periods is not enough.

Setting

There are kkk types θ\thetaθ and, for each type, ℓ\ellℓ actions aθ1,…,aθℓa_{\theta1},\dots,a_{\theta\ell}aθ1​,…,aθℓ​. In each period t=1,…,Tt=1,\dots,Tt=1,…,T a type θt\theta_tθt​ arrives, drawn independently from an unknown distribution p⃗\vec pp​ with

pθ≥β>0for every θ(Assumption 1).p_\theta\ge\beta>0\quad\text{for every }\theta\qquad\text{(Assumption 1)}.pθ​≥β>0for every θ(Assumption 1).

Nθ(t)N_\theta(t)Nθ​(t) counts the type-θ\thetaθ arrivals in periods [1,t][1,t][1,t], Nˉθ(t)\bar N_\theta(t)Nˉθ​(t) those in [t+1,T][t+1,T][t+1,T], and NθN_\thetaNθ​ those over the whole horizon. The algorithm's type-action counts xθjx_{\theta j}xθj​ record how often action aθja_{\theta j}aθj​ was used on a type-θ\thetaθ arrival.

The objective is a linear program in the counts,

fN⃗(x⃗)=min⁡z⃗≥0 c⃗1⋅x⃗+c⃗2⋅z⃗s.t.∑jxθj=Nθ,Ax⃗−Dz⃗≤B⃗∑θNθ,f_{\vec N}(\vec x)=\min_{\vec z\ge0}\ \vec c_1\cdot\vec x+\vec c_2\cdot\vec z\quad\text{s.t.}\quad\sum_jx_{\theta j}=N_\theta,\qquad A\vec x-D\vec z\le\vec B\sum_\theta N_\theta,fN​(x)=z≥0min​ c1​⋅x+c2​⋅zs.t.j∑​xθj​=Nθ​,Ax−Dz≤Bθ∑​Nθ​,

with D≥0D\ge0D≥0 having a positive entry in every row. The analysis uses two properties of fff (Proposition 1):

  • (i) fN⃗f_{\vec N}fN​ is λ\lambdaλ-Lipschitz;
  • (ii) optimal solutions are stable: an optimal x⃗\vec xx of min⁡x⃗≥y⃗fN⃗\min_{\vec x\ge\vec y}f_{\vec N}minx≥y​​fN​ has a counterpart for N⃗′\vec N'N′ within δ∣N⃗−N⃗′∣∞\delta|\vec N-\vec N'|_\inftyδ∣N−N′∣∞​.

A tie-breaking rule σ(N⃗,y⃗)\sigma(\vec N,\vec y)σ(N,y​) selects one optimal solution of min⁡x⃗≥y⃗fN⃗(x⃗)\min_{\vec x\ge\vec y}f_{\vec N}(\vec x)minx≥y​​fN​(x) and is δ\deltaδ-Lipschitz in N⃗\vec NN (Assumption 2).

The horizon TTT is revealed at a heads-up time T^\hat TT^, unknown in advance, with

T−T^>T1/2+ϵ(Assumption 3).T-\hat T>T^{1/2+\epsilon}\qquad\text{(Assumption 3)}.T−T^>T1/2+ϵ(Assumption 3).

The benchmark is OPT(N⃗)=min⁡x⃗≥0fN⃗(x⃗)\mathrm{OPT}(\vec N)=\min_{\vec x\ge0}f_{\vec N}(\vec x)OPT(N)=minx≥0​fN​(x), and the loss of an algorithm is

LALG=E[fN⃗(x⃗ALG)−OPT(N⃗)].L_{\mathrm{ALG}}=\mathbb E\big[f_{\vec N}(\vec x^{\mathrm{ALG}})-\mathrm{OPT}(\vec N)\big].LALG​=E[fN​(xALG)−OPT(N)].

Formalization targets

Goal: Theorem 2.2

For every ϵ>0\epsilon>0ϵ>0 there is a constant M(β,λ,δ,ϵ,ℓ)M(\beta,\lambda,\delta,\epsilon,\ell)M(β,λ,δ,ϵ,ℓ) such that, for every instance and every tie-breaking rule, some online algorithm satisfies

LALG≤M(β,λ,δ,ϵ,ℓ)L_{\mathrm{ALG}}\le M(\beta,\lambda,\delta,\epsilon,\ell)LALG​≤M(β,λ,δ,ϵ,ℓ)

for every arrival distribution with pθ≥βp_\theta\ge\betapθ​≥β, every horizon TTT and every heads-up time T^\hat TT^ allowed by Assumption 3. The constant does not depend on TTT, T^\hat TT^, p⃗\vec pp​, kkk or the constraint data. The theorem fixes no value of MMM.

Milestones

In the paper's order:

  • Lemma 2.1: Hoeffding plus a union bound, P[max⁡θ∣Nˉθ(t)−tˉpθ∣>αtˉlog⁡tˉ]≤2ktˉ−2α\mathbb P[\max_\theta|\bar N_\theta(t)-\bar tp_\theta|>\sqrt{\alpha\bar t\log\bar t}]\le2k\bar t^{-2\alpha}P[maxθ​∣Nˉθ​(t)−tˉpθ​∣>αtˉlogtˉ​]≤2ktˉ−2α.
  • Lemma 3.1: the hindsight optimum OPTt\mathrm{OPT}^tOPTt does not change while the actions taken stay below an optimal solution.
  • Lemma 3.2: with high probability some clairvoyant solution uses each action at least T DLPθj−[Tlog⁡T](1+ϵ)/2T\,\mathrm{DLP}_{\theta j}-[T\log T]^{(1+\epsilon)/2}TDLPθj​−[TlogT](1+ϵ)/2 times, where DLP\mathrm{DLP}DLP solves min⁡x⃗≥0fp⃗\min_{\vec x\ge0}f_{\vec p}minx≥0​fp​​.
  • Lemma 3.3: bad events StS_tSt​ are rare, and off them the empirical program EDLP(t)\mathrm{EDLP}(t)EDLP(t) is close to DLP\mathrm{DLP}DLP.
  • Lemma 3.5: after T/2T/2T/2, the program TDLP(t)\mathrm{TDLP}(t)TDLP(t) with the known horizon gives lower confidence bounds on the hindsight solution.

Significance

The result. Theorem 2.2 separates two kinds of uncertainty. Not knowing the arrival distribution costs only a constant, because it can be learned on the fly. Not knowing the horizon costs only a constant as long as the end is announced T1/2+ϵT^{1/2+\epsilon}T1/2+ϵ periods ahead. The impossibility results of the paper's Section 4 show that each assumption is needed:

  • a heads-up of order T\sqrt TT​ forces Ω(T)\Omega(\sqrt T)Ω(T​) loss in bin packing;
  • rare types (no lower bound β\betaβ) force loss growing with TTT;
  • an objective without the stability property (ii) forces loss growing with TTT.

The framework covers online bin packing, online payment routing, packing problems with budgets, and egalitarian welfare objectives.

Formalizing it. The theorem is proved in the paper and has no machine-checked proof. The mission states it at full strength: the constant depends only on (β,λ,δ,ϵ,ℓ)(\beta,\lambda,\delta,\epsilon,\ell)(β,λ,δ,ϵ,ℓ), every heads-up time allowed by Assumption 3 is covered, and the algorithm is chosen before the arrival distribution, the horizon and the heads-up time. The paper's printed proof does not establish this as written. Its Lemma 3.4 introduces a threshold T0T_0T0​ that depends on the smallest positive entry of DLP\mathrm{DLP}DLP, which varies with B⃗\vec BB and p⃗\vec pp​. A complete formal proof therefore requires either repairing that step or a different algorithm. Either outcome is a contribution. The milestones isolate the parts of the proof that are sound as stated: Lemma 3.3 is stated at t=2t=2t=2 only for ϵ≤1/2\epsilon\le1/2ϵ≤1/2, the range Assumption 3 allows.

Difficulty

The obvious algorithm resolves the deterministic program with the empirical frequencies N⃗(t)/t\vec N(t)/tN(t)/t in every period and randomizes according to its solution. The paper shows (Figure 1, p.11) that this alone incurs Ω(T)\Omega(\sqrt T)Ω(T​) loss. Actions that the true program never uses receive empirical weight of order 1/t1/\sqrt t1/t​, and these mistakes add up. Removing low-weight actions creates the opposite risk: the remaining actions are used too often, and the gap T−T^T-\hat TT−T^ must absorb that excess. This is where the exponent 1/2+ϵ1/2+\epsilon1/2+ϵ enters.

The constant must also be uniform over every instance with the same (β,λ,δ,ϵ,ℓ)(\beta,\lambda,\delta,\epsilon,\ell)(β,λ,δ,ϵ,ℓ). Bounds that hold "for TTT large enough", with a threshold depending on the instance, do not suffice. Neither does a bound that assumes T^≥T/2\hat T\ge T/2T^≥T/2, unless the reduction is carried out.

Formalization scope

Types are Fin k and actions Fin ℓ; periods are 1-based in the paper and the indices of Fin T. Probabilities are finite sums over arrival sequences with the product law. The loss is a finite sum over trajectories of arrivals and actions. All counts are natural numbers cast to ℝ.

The conventions fixed in Lean:

  • OPT\mathrm{OPT}OPT is over real (fractional) x⃗≥0\vec x\ge0x≥0.
  • Proposition 1 (i) is in the ℓ1\ell_1ℓ1​ norm.
  • Proposition 1 (ii) is required only when both feasible sets are non-empty; without that guard it is unsatisfiable for k≥2k\ge2k≥2, and every hypothesis set would be empty.
  • Assumption 2 is a δ\deltaδ-Lipschitz selection, with no homogeneity.
  • fN⃗f_{\vec N}fN​ is assumed real-valued (Bounded).
  • An algorithm is a map from the history, the current type and the horizon information (none up to T^\hat TT^, some T afterwards) to a distribution over actions. It receives nothing else.

A statement in which the algorithm may depend on TTT, T^\hat TT^ or p⃗\vec pp​, or in which MMM is chosen after the instance, is a different and much weaker theorem. The quantifier order of the goal rules both out.

A complete development needs:

  • Hoeffding's inequality for sums of indicators on the finite product space;
  • linear-programming homogeneity and stability;
  • an online algorithm in the policy class (the paper's Algorithm 1, or a repaired variant).

The concentration lemmas and the policy and trajectory model are reusable for other online resource-allocation missions. Proofs of the milestones are welcome independently of the goal. So is a repaired version of Lemma 3.4: as printed it fails at small ttt, where the empirical maximizer can be an action of zero DLP weight without a bad event.

Selected references

  • S. Banerjee, D. Freund, Good prophets know when the end is near, Management Science, 2024. https://doi.org/10.1287/mnsc.2023.04307
  • A. Vera, S. Banerjee, The Bayesian prophet: a low-regret framework for online decision making, Management Science 67(3), 2021. https://doi.org/10.1287/mnsc.2020.3624
  • A. Arlotto, I. Gurvich, Uniformly bounded regret in the multisecretary problem, Stochastic Systems 9(3), 2019. https://doi.org/10.1287/stsy.2018.0028
  • O. L. Mangasarian, T.-H. Shiau, Lipschitz continuity of solutions of linear inequalities, programs and complementarity problems, SIAM Journal on Control and Optimization 25(3), 1987. https://doi.org/10.1137/0325033
  • W. Hoeffding, Probability inequalities for sums of bounded random variables, Journal of the American Statistical Association 58(301), 1963. https://doi.org/10.1080/01621459.1963.10500830
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🏆Completed
ProbabilityRandom Matrix Theory·Captain: Hix_Lab

Singh Theorem: cN=π215(1−4N2)c_N = \frac{\pi^2}{15}\left(1 - \frac{4}{N^2}\right)cN​=15π2​(1−N24​)Research Paper

Motivation

The local statistics of eigenvalues of Haar distributed unitary matrices (the circular unitary ensemble) are a standard model for spacings of zeros of the Riemann zeta function. This mission concerns the characteristic polynomial Λ(θ)=det⁡(I−e−iθU)\Lambda(\theta) = \det(I - e^{-i\theta}U)Λ(θ)=det(I−e−iθU) at two adjacent eigenangles, and how the difference of log⁡∣Λ′∣\log|\Lambda'|log∣Λ′∣ at those two eigenangles fluctuates when the two eigenangles nearly collide.

Setting

Let UUU be Haar distributed in U(N)U(N)U(N), N≥2N \ge 2N≥2, with adjacent eigenangles θ1<θ2\theta_1 < \theta_2θ1​<θ2​ and normalized gap s=N(θ2−θ1)/(2π)s = N(\theta_2 - \theta_1)/(2\pi)s=N(θ2​−θ1​)/(2π). Set

X=log⁡∣Λ′(θ1)∣−log⁡∣Λ′(θ2)∣,VN(s)=Var⁡(X∣s).X = \log|\Lambda'(\theta_1)| - \log|\Lambda'(\theta_2)|, \qquad V_N(s) = \operatorname{Var}(X \mid s).X=log∣Λ′(θ1​)∣−log∣Λ′(θ2​)∣,VN​(s)=Var(X∣s).

By rotation invariance one may place the pair at ±δ/2\pm\delta/2±δ/2 with δ=2πs/N\delta = 2\pi s/Nδ=2πs/N. The remaining n=N−2n = N - 2n=N−2 eigenangles θ∈(δ/2,2π−δ/2)n\theta \in (\delta/2, 2\pi - \delta/2)^nθ∈(δ/2,2π−δ/2)n then have density proportional to

∏a<bsin⁡2θa−θb2∏ksin⁡2θk−δ/22 sin⁡2θk+δ/22,\prod_{a<b}\sin^2\frac{\theta_a-\theta_b}{2}\prod_{k}\sin^2\frac{\theta_k-\delta/2}{2}\,\sin^2\frac{\theta_k+\delta/2}{2},a<b∏​sin22θa​−θb​​k∏​sin22θk​−δ/2​sin22θk​+δ/2​,

and X=∑k(log⁡sin⁡θk+δ/22−log⁡sin⁡θk−δ/22)X = \sum_k \left(\log\sin\frac{\theta_k+\delta/2}{2} - \log\sin\frac{\theta_k-\delta/2}{2}\right)X=∑k​(logsin2θk​+δ/2​−logsin2θk​−δ/2​). In Lean, VN(s)V_N(s)VN​(s) is cueV N s.

Target

The goal is the Singh Theorem: for every N≥2N \ge 2N≥2,

lim⁡s→0+VN(s)s2=cN,cN=π215(1−4N2).\lim_{s\to 0^+}\frac{V_N(s)}{s^2} = c_N, \qquad c_N = \frac{\pi^2}{15}\left(1 - \frac{4}{N^2}\right).s→0+lim​s2VN​(s)​=cN​,cN​=15π2​(1−N24​).

Milestones:

  1. Little o form: VN(s)=cNs2+o(s2)V_N(s) = c_N s^2 + o(s^2)VN​(s)=cN​s2+o(s2) as s→0+s \to 0^+s→0+.
  2. Circle moment: with weight w0(θ)=∏a<bsin⁡2θa−θb2∏ksin⁡4θk2w_0(\theta) = \prod_{a<b}\sin^2\frac{\theta_a-\theta_b}{2}\prod_k\sin^4\frac{\theta_k}{2}w0​(θ)=∏a<b​sin22θa​−θb​​∏k​sin42θk​​ on (0,2π)N−2(0,2\pi)^{N-2}(0,2π)N−2 and S=12∑kcot⁡θk2S = \frac12\sum_k\cot\frac{\theta_k}{2}S=21​∑k​cot2θk​​, Ew0[S2]=N2−460E_{w_0}[S^2] = \frac{N^2-4}{60}Ew0​​[S2]=60N2−4​.
  3. Hua second moment: for the probability measure Pn,2P_{n,2}Pn,2​ on Rn\mathbb{R}^nRn with density proportional to ∏j<k(uj−uk)2∏k(1+uk2)−(n+2)\prod_{j<k}(u_j-u_k)^2\prod_k(1+u_k^2)^{-(n+2)}∏j<k​(uj​−uk​)2∏k​(1+uk2​)−(n+2), E[(∑kuk)2]=n(n+4)15E\left[(\sum_k u_k)^2\right] = \frac{n(n+4)}{15}E[(∑k​uk​)2]=15n(n+4)​.

Significance

The constant cNc_NcN​ is exact for every finite NNN, and its limit π2/15\pi^2/15π2/15 as N→∞N \to \inftyN→∞ gives the small gap behaviour of the corresponding quantity for the sine kernel process. A complete Lean development of all four statements exists and checks with only the standard axioms.

Difficulty

As s→0s \to 0s→0 the conditioning weight degenerates, so VN(s)V_N(s)VN​(s) is a ratio of integrals that both vanish to leading order; the expansion has to be carried to second order in δ\deltaδ with uniform control of integrability near the colliding pair.

Formalization scope

All objects are real valued integrals over Rn\mathbb{R}^nRn (functions Fin n → ℝ) with Lebesgue measure, restricted to explicit open boxes by indicator functions; conditional variance is written as a ratio of integrals. Natural subtraction N−2N - 2N−2 is harmless under N≥2N \ge 2N≥2. Definitions live in Definitions.Def_Singh.

Selected references

  • J. Singh, Singh Theorem formalization, https://github.com/jjsingh88/singh-constant
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EconomicsOperations Research·Captain: iris

Product Quality and Information Sharing in the Presence of Reviews: perfectly informative reviews weaken the quality incentive under a wholesale price contract but not under a commission contractResearch Paper

Motivation

Online marketplaces hold two kinds of information that a manufacturer selling through them would like to have. Product reviews tell customers about a product's quality. Customer data tell the platform how strongly the market responds to quality, and the platform can sell that signal to the manufacturer, as Amazon does with Brand Analytics, which Shin and Zeevi discuss. Both kinds of information affect what the manufacturer decides to build.

Shin and Zeevi (SSRN 3886954; published in Management Science, doi:10.1287/mnsc.2023.4746) ask how reviews change a manufacturer's incentive to invest in quality once the platform's information sharing is endogenous. Their answer depends on the contract: under a wholesale price contract, where the firms price in sequence, reviews can make the platform unwilling to share; under a commission contract, where the manufacturer sets the retail price and pays a share of revenue, they do not. Proposition 7 of the paper states this contrast, and this mission formalizes it.

Setting

A manufacturer sells through a platform over two stages. Before selling, it chooses a quality q∈{q‾,qˉ}q\in\{\underline q,\bar q\}q∈{q​,qˉ​}, 0<q‾<qˉ0<\underline q<\bar q0<q​<qˉ​, with unit cost cq∈{c‾,cˉ}c_q\in\{\underline c,\bar c\}cq​∈{c​,cˉ}, c‾<cˉ\underline c<\bar cc​<cˉ. Demand is d1=α+θq−p1d_1=\alpha+\theta q-p_1d1​=α+θq−p1​ in the first stage and d2=α+θq^2−p2d_2=\alpha+\theta\hat q_2-p_2d2​=α+θq^​2​−p2​ in the second, where θ\thetaθ is an unknown quality sensitivity with mean μθ>0\mu_\theta>0μθ​>0 and variance σθ2>0\sigma_\theta^2>0σθ2​>0, and q^2\hat q_2q^​2​ is the customers' posterior mean quality.

The propensity signal sθs_\thetasθ​ reaches the platform before the second stage. It is an unbiased estimator of θ\thetaθ with variance σm2>0\sigma_m^2>0σm2​>0, and the posterior mean is linear,

θ^=E[θ∣sθ]=(1−ϕ)μθ+ϕsθ,ϕ=σθ2σm2+σθ2.\hat\theta=E[\theta\mid s_\theta]=(1-\phi)\mu_\theta+\phi s_\theta,\qquad \phi=\frac{\sigma_\theta^2}{\sigma_m^2+\sigma_\theta^2}.θ^=E[θ∣sθ​]=(1−ϕ)μθ​+ϕsθ​,ϕ=σm2​+σθ2​σθ2​​.

The product's true value is Q=q+ϵQ=q+\epsilonQ=q+ϵ, where ϵ\epsilonϵ has mean 000 and variance σp2>0\sigma_p^2>0σp2​>0 and is independent of (θ,sθ)(\theta,s_\theta)(θ,sθ​). The rate γ\gammaγ measures how informative reviews are. The two regimes compared here are no reviews, γ=0\gamma=0γ=0, where q^2=q\hat q_2=qq^​2​=q, and perfectly informative reviews, γ=∞\gamma=\inftyγ=∞, where q^2=q+ϵ\hat q_2=q+\epsilonq^​2​=q+ϵ.

Under the wholesale contract the manufacturer sets wtw_twt​ and the platform then sets ptp_tpt​ in each stage. Under the commission contract, with rate uuu, the manufacturer sets ptp_tpt​ and pays the platform uptup_tupt​ per unit. The information arrangement i∈{s,ns}i\in\{s,ns\}i∈{s,ns} says whether the manufacturer subscribes to the signal; without it the manufacturer prices on μθ\mu_\thetaμθ​ in place of θ^\hat\thetaθ^. Prices come from backward induction, and Πik(q)\Pi^k_i(q)Πik​(q) is the resulting two-stage expected profit of firm kkk, gross of the fee.

The manufacturer's quality qiq_iqi​ maximizes ΠiM\Pi^M_iΠiM​, a tie going to low quality, and its incentive is ΔqΠiM=ΠiM(qˉ)−ΠiM(q‾)\Delta_q\Pi^M_i=\Pi^M_i(\bar q)-\Pi^M_i(\underline q)Δq​ΠiM​=ΠiM​(qˉ​)−ΠiM​(q​). The platform chooses a fee ρ≥0\rho\ge0ρ≥0; the manufacturer subscribes iff ΠsM(qs)−ΠnsM(qns)>ρ\Pi^M_s(q_s)-\Pi^M_{ns}(q_{ns})>\rhoΠsM​(qs​)−ΠnsM​(qns​)>ρ. The equilibrium arrangement is i∗=si^*=si∗=s if some fee makes the manufacturer subscribe and leaves the platform strictly better off, and i∗=nsi^*=nsi∗=ns otherwise. Commission quantities carry a bar.

With π(q)=(α+μθq−cq)2\pi(q)=(\alpha+\mu_\theta q-c_q)^2π(q)=(α+μθ​q−cq​)2, the thresholds are

Φi0=2(π(q‾)−π(qˉ))σθ2(qˉ2−43q‾2),Ψi0=q‾23,Φi∞=2(π(q‾)−π(qˉ))σθ2(qˉ2−43q‾2−13σp2),Ψi∞=q‾2+σp23.\Phi^0_i=\frac{2(\pi(\underline q)-\pi(\bar q))}{\sigma_\theta^2(\bar q^2-\frac43\underline q^2)},\quad\Psi^0_i=\frac{\underline q^2}{3},\quad \Phi^\infty_i=\frac{2(\pi(\underline q)-\pi(\bar q))}{\sigma_\theta^2(\bar q^2-\frac43\underline q^2-\frac13\sigma_p^2)},\quad\Psi^\infty_i=\frac{\underline q^2+\sigma_p^2}{3}.Φi0​=σθ2​(qˉ​2−34​q​2)2(π(q​)−π(qˉ​))​,Ψi0​=3q​2​,Φi∞​=σθ2​(qˉ​2−34​q​2−31​σp2​)2(π(q​)−π(qˉ​))​,Ψi∞​=3q​2+σp2​​.

Formalization targets

Goal: Proposition 7 (pp.27–28), corrected

For every family of pricing equilibria: if π(qˉ)<π(q‾)\pi(\bar q)<\pi(\underline q)π(qˉ​)<π(q​), then under the wholesale contract

ΔqΠi∗M∣γ=0 ≥ ΔqΠi∗M∣γ=∞,\Delta_q\Pi^M_{i^*}\big|_{\gamma=0}\ \ge\ \Delta_q\Pi^M_{i^*}\big|_{\gamma=\infty},Δq​Πi∗M​​γ=0​ ≥ Δq​Πi∗M​​γ=∞​,

with strict inequality iff qˉ2−q‾2>Ψi0\bar q^2-\underline q^2>\Psi^0_iqˉ​2−q​2>Ψi0​ and ϕ>Φi0\phi>\Phi^0_iϕ>Φi0​, but not both qˉ2−q‾2>Ψi∞\bar q^2-\underline q^2>\Psi^\infty_iqˉ​2−q​2>Ψi∞​ and ϕ>Φi∞\phi>\Phi^\infty_iϕ>Φi∞​. If πu(qˉ)<πu(q‾)\pi_u(\bar q)<\pi_u(\underline q)πu​(qˉ​)<πu​(q​) and u∈(0,uˉ)u\in(0,\bar u)u∈(0,uˉ), with πu\pi_uπu​, uˉ\bar uuˉ of (17), then under the commission contract

ΔqΠˉi∗M∣γ=0=ΔqΠˉi∗M∣γ=∞.\Delta_q\bar\Pi^M_{i^*}\big|_{\gamma=0}=\Delta_q\bar\Pi^M_{i^*}\big|_{\gamma=\infty}.Δq​Πˉi∗M​​γ=0​=Δq​Πˉi∗M​​γ=∞​.

Three printed statements are corrected, each with a counterexample satisfying the paper's assumptions. "Fix an information fee ρ≥0\rho\ge0ρ≥0" is removed: at a fixed fee (23) can fail, so i∗i^*i∗ is the equilibrium arrangement in each regime. The printed strictness clause "ϕ∈(Φi0,Φi∞)\phi\in(\Phi^0_i,\Phi^\infty_i)ϕ∈(Φi0​,Φi∞​) and/or qˉ2−q‾2∈(Ψi0,Ψi∞)\bar q^2-\underline q^2\in(\Psi^0_i,\Psi^\infty_i)qˉ​2−q​2∈(Ψi0​,Ψi∞​)" is replaced by the iff above, since its second branch alone does not give strictness. Display (15), Φi0<Φi∞\Phi^0_i<\Phi^\infty_iΦi0​<Φi∞​, is stated for qˉ2−q‾2\bar q^2-\underline q^2qˉ​2−q​2 outside [Ψi0,Ψi∞][\Psi^0_i,\Psi^\infty_i][Ψi0​,Ψi∞​], since it fails between them; qˉ2−q‾2>Ψi∞\bar q^2-\underline q^2>\Psi^\infty_iqˉ​2−q​2>Ψi∞​ is the range where Φi∞\Phi^\infty_iΦi∞​ is a threshold.

Milestones

  1. (5), (6): second- and first-stage wholesale prices.
  2. (38), (39): platform and manufacturer profits at γ∈{0,∞}\gamma\in\{0,\infty\}γ∈{0,∞}.
  3. Proofs of Proposition 1 and Theorems 1, 2: the quality decision and the threshold strategies in the two regimes.
  4. (15)–(16): the order of the thresholds.
  5. §4.1, (62)–(63): commission prices and profits.
  6. Proofs of Proposition 2 and Theorem 3: under commission, sharing is always arranged, and quality is high iff ϕ>Φˉq\phi>\bar\Phi_qϕ>Φˉq​.

Significance

The result. For a fixed arrangement, reviews do not move the quality threshold under either contract. The whole effect runs through information sharing. Under a wholesale price contract reviews raise the double-marginalization loss from sharing, the platform may then refuse to share, and quality falls. This is why the proposition compares contracts, and it supports the paper's conclusion that information sharing is more favorable under a commission contract when reviews are informative.

Formalizing it. The result is proved on paper; no machine-checked proof is known. The formal development makes explicit what the paper leaves implicit: the fee rule behind i∗i^*i∗, the moment computation Var⁡θ^=ϕσθ2\operatorname{Var}\hat\theta=\phi\sigma_\theta^2Varθ^=ϕσθ2​, and the region where a threshold's denominator is not positive, which is where the printed clauses fail.

Difficulty

The obvious route computes each profit and compares. Two steps resist it. The profit formulas need second moments of θ^\hat\thetaθ^, θ\thetaθ and ϵ\epsilonϵ jointly, and Var⁡θ^\operatorname{Var}\hat\thetaVarθ^ follows from the tower property, not from a formula in the paper. The comparison then cannot simply subtract thresholds: Φi0\Phi^0_iΦi0​ and Φi∞\Phi^\infty_iΦi∞​ are meaningful only when the matching gap condition holds, so the case analysis must follow the fee rule rather than the printed intervals.

Formalization scope

Equilibria are predicates built from IsMaxOn, subgame perfect in the estimate and the belief; no price, profit or arrangement is defined by a closed form. The goal quantifies over every family of pricing equilibria, and milestones give their existence and uniqueness. Expected profits are Bochner integrals on a probability space; the L2L^2L2 and independence hypotheses make each integrand integrable. Conditional expectations are Mathlib's, with respect to the σ-algebras generated by θ\thetaθ and sθs_\thetasθ​.

The conventions are these. γ=0\gamma=0γ=0 and γ=∞\gamma=\inftyγ=∞ are the boundary models, with exact statements in place of the paper's limits. Finite-γ\gammaγ results (Lemmas 3, 4 and the finite-γ\gammaγ parts of Propositions 1, 2 and Theorems 1–3) are not part of this mission, because the paper does not specify how the law of sθs_\thetasθ​ varies with ϕ\phiϕ. The plain ccc of (5) is cqc_qcq​. Without sharing the manufacturer's problem is read at μθ\mu_\thetaμθ​. The model drops normality of ϵ\epsilonϵ, the supports of θ\thetaθ and sθs_\thetasθ​ and positivity of demand, and keeps μθ>0\mu_\theta>0μθ​>0; these are generalizations. Commission clauses add (α+μθq‾)2<(α+μθqˉ)2(\alpha+\mu_\theta\underline q)^2<(\alpha+\mu_\theta\bar q)^2(α+μθ​q​)2<(α+μθ​qˉ​)2 and c‾2≤cˉ2\underline c^2\le\bar c^2c​2≤cˉ2 so that (17) is defined; both follow from 0<α0<\alpha0<α and 0≤c‾0\le\underline c0≤c​. Each standing assumption sits on the clause that uses it.

Defining i∗i^*i∗ by the thresholds, or prices by their formulas, would reduce the goal to algebra on transcribed expressions; the definitions rule this out. The weak inequality alone would also be empty when i∗i^*i∗ does not change, so the strictness iff is part of the goal, and a proved finite model confirms that the signal hypotheses are satisfiable and that the strict case occurs.

Everything is built on Mathlib primitives. The fee game, stated on a table of profits, is reusable for other information-sale models. Proofs of any milestone are welcome, as are alternative arguments for the profit formulas.

Selected references

  • D. Shin, A. Zeevi, Product Quality and Information Sharing in the Presence of Reviews, working paper, SSRN 3886954. https://ssrn.com/abstract=3886954
  • D. Shin, A. Zeevi, Product Quality and Information Sharing in the Presence of Reviews, Management Science, 2023. https://doi.org/10.1287/mnsc.2023.4746
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Dynamic ProgrammingOperations ResearchProbability+1·Captain: iris

Online Policies for Efficient Volunteer Crowdsourcing: The Sparse Notification Policy Is 12−q(1−1e)\frac{1}{2-q}(1-\frac{1}{e})2−q1​(1−e1​)-CompetitiveResearch Paper

Why volunteer notifications are an online decision problem

Nonprofit crowdsourcing platforms rely on volunteers to perform time-sensitive tasks. On Food Rescue U.S., for example, a task is a scheduled pickup of a perishable donation, and when a task goes unclaimed the platform can push a notification to a subset of volunteers. Notifying more volunteers raises the chance that the current task gets done, but excessive notifications lead volunteers to stop paying attention, which costs future tasks. Manshadi and Rodilitz model this trade-off as the online volunteer notification problem, a generalization of online stochastic bipartite matching. Their Theorem 1 gives a constant-factor guarantee for a randomized policy that never observes volunteers' states.

The model

An instance I\mathcal II has VVV volunteers, SSS task types and TTT periods. In period ttt a task of type sss arrives with known probability λs,t\lambda_{s,t}λs,t​, with ∑sλs,t≤1\sum_s\lambda_{s,t}\le 1∑s​λs,t​≤1; arrivals are independent across periods. Every volunteer starts active. If an active volunteer vvv is notified about a task of type sss, she responds with probability pv,sp_{v,s}pv,s​ and, whether or not she responds, becomes inactive for Z>0Z>0Z>0 periods, where ZZZ has known law ggg on {1,2,… }\{1,2,\dots\}{1,2,…}. An inactive volunteer ignores notifications. The task is completed if at least one notified active volunteer responds. The platform sees neither states nor the future, and POLI\mathrm{POL}_{\mathcal I}POLI​ denotes the expected number of completed tasks.

Let GGG be the CDF of ggg. The minimum discrete hazard rate (MDHR) of ggg is

q=inf⁡τ≥1g(τ)1−G(τ−1),q=\inf_{\tau\ge1}\frac{g(\tau)}{1-G(\tau-1)},q=τ≥1inf​1−G(τ−1)g(τ)​,

with 0/0=10/0=10/0=1. The benchmark LPI\mathrm{LP}_{\mathcal I}LPI​ maximizes ∑t,sλs,tmin⁡{∑vxv,s,tpv,s,1}\sum_{t,s}\lambda_{s,t}\min\{\sum_v x_{v,s,t}p_{v,s},1\}∑t,s​λs,t​min{∑v​xv,s,t​pv,s​,1} over the set P\mathcal PP of x∈[0,1]V×S×Tx\in[0,1]^{V\times S\times T}x∈[0,1]V×S×T with

1≥∑τ≤t∑sλs,τxv,s,τ(1−G(t−τ))for all v,t.1\ge\sum_{\tau\le t}\sum_s\lambda_{s,\tau}x_{v,s,\tau}(1-G(t-\tau))\quad\text{for all }v,t.1≥τ≤t∑​s∑​λs,τ​xv,s,τ​(1−G(t−τ))for all v,t.

The sparse notification (SN) policy has an offline and an online phase. Offline it computes an ex ante solution x∗x^*x∗, the best under f(x)=∑t,sλs,t(1−∏v(1−xv,s,tpv,s))f(x)=\sum_{t,s}\lambda_{s,t}(1-\prod_v(1-x_{v,s,t}p_{v,s}))f(x)=∑t,s​λs,t​(1−∏v​(1−xv,s,t​pv,s​)) of three candidates: an optimum of the benchmark, the output of a Frank–Wolfe variant for maximizing fff over P\mathcal PP, and the solution of VVV sequential linear programs. It then sparsifies x∗x^*x∗ into x~\tilde xx~ with a sequence of one-dimensional dynamic programs with value-to-go Jv,tJ_{v,t}Jv,t​, one per volunteer, in priority order. Online, when a task of type sss arrives at ttt, it notifies each vvv independently with probability x~v,s,t\tilde x_{v,s,t}x~v,s,t​.

Formalization targets

Goal: Theorem 1

For every instance,

POLI≥12−q(1−1e)LPI.\mathrm{POL}_{\mathcal I}\ge\frac{1}{2-q}\Bigl(1-\frac1e\Bigr)\mathrm{LP}_{\mathcal I}.POLI​≥2−q1​(1−e1​)LPI​.

There are no bounds on V,S,TV,S,TV,S,T and no condition on ggg beyond being a proper law on the positive integers.

Online half

For x∈Px\in\mathcal Px∈P, the contribution of vvv under the index-based priority scheme is at least Jv,1J_{v,1}Jv,1​ (Lemma 2), and

Jv,1≥12−qfv(x)J_{v,1}\ge\frac{1}{2-q}f_v(x)Jv,1​≥2−q1​fv​(x)

(Lemma 3), through dual feasibility (12)–(16) and the weak-duality bound (17). With f=∑vfvf=\sum_vf_vf=∑v​fv​ (Lemma 1) this gives POLI≥f(x∗)/(2−q)\mathrm{POL}_{\mathcal I}\ge f(x^*)/(2-q)POLI​≥f(x∗)/(2−q).

Offline half

For x∈Px\in\mathcal Px∈P,

1−∏v(1−xv,s,tpv,s)≥(1−1e)min⁡{∑vxv,s,tpv,s,1},1-\prod_v(1-x_{v,s,t}p_{v,s})\ge\Bigl(1-\frac1e\Bigr)\min\Bigl\{\sum_vx_{v,s,t}p_{v,s},1\Bigr\},1−v∏​(1−xv,s,t​pv,s​)≥(1−e1​)min{v∑​xv,s,t​pv,s​,1},

through Claims 1 and 2, so f(x∗)≥(1−1/e)LPIf(x^*)\ge(1-1/e)\mathrm{LP}_{\mathcal I}f(x∗)≥(1−1/e)LPI​ (Proposition 2).

Significance

The result gives a guarantee of at least 12(1−1e)\frac12(1-\frac1e)21​(1−e1​) for every inter-activity distribution, one that improves with qqq, against a benchmark that bounds the clairvoyant solution. It extends the 1−1/e1-1/e1−1/e style of guarantee for online matching to resources that return after a random time and react to notifications they cannot be seen to receive. The paper also tests the policy on Food Rescue U.S. data, which is outside this mission.

The theorem is proved on paper and, as far as the catalog shows, has no machine-checked proof. A formalization adds a precise model of the process, including the independence structure the informal proof relies on. The paper's proof of Lemma 2 passes through a recursion for a conditional value that treats it as independent of the history; the lemma itself stands, and a formal proof has to establish it without that shortcut. It also fixes which readings of the printed statements hold: Lemma 3 is meant with JJJ built from the same xxx.

Difficulty

The volunteers' states are correlated through the common arrival sequence and the policy cannot see them, so the natural idea of analyzing each volunteer's state as an independent chain fails: a lower-priority volunteer's chance of completing a task depends on the states of those before her. The constraint defining P\mathcal PP holds only in expectation, so feasibility of x∗x^*x∗ says nothing about a single sample path, and following x∗x^*x∗ directly is only qqq-competitive. The hazard rate has to convert the expected constraint into a per-volunteer bound through a dual solution, and the online loss 1/(2−q)1/(2-q)1/(2−q) and the offline loss 1−1/e1-1/e1−1/e must hold for the same x∗x^*x∗.

Formalization scope

Volunteers, types and periods are Fin-indexed, with paper index equal to the value plus one; xxx has type Fin V → Fin S → Fin T → ℝ so that fderiv gives ∇f\nabla f∇f. J has T + 1 time slots, with the last one 0. The law ggg is real-valued on N\mathbb NN, with g(0)=0g(0)=0g(0)=0 and sum 111; it may have unbounded support and infinite mean. The MDHR is an infimum, because the printed minimum need not exist, and the fraction 0/00/00/0 is coded as 111.

The process is stated on an arbitrary probability space carrying measurable N\mathbb NN-valued primitives: arrivals AtA_tAt​, notification coins, response coins and inter-activity times Zv,tZ_{v,t}Zv,t​, all jointly independent as one family. The dynamics are a deterministic function of a realization. Notifying an inactive volunteer changes nothing.

The goal is stated for x∗x^*x∗ of (5), not for an arbitrary point of P\mathcal PP: at x=0x=0x=0 the policy does nothing, so the statement would be false. All three candidates are defined as printed, and any optimizer and tie-break is allowed. (x~,J)(\tilde x,J)(x~,J) is a predicate whose solutions exist and are unique. No result is restricted to finitely supported ggg.

Everything is built on Mathlib: iIndepFun, fderiv and the Bochner integral. The hazard-rate definitions and the process with independent primitives are reusable for other models of reusable resources. Proofs of the milestones in any order are welcome, as are direct proofs of the offline half, which needs no probability.

Selected references

  • V. Manshadi, S. Rodilitz, Online Policies for Efficient Volunteer Crowdsourcing, arXiv:2002.08474v7, 2021. https://arxiv.org/abs/2002.08474
  • S. Alaei, M. Hajiaghayi, V. Liaghat, Online prophet-inequality matching with applications to ad allocation, Proceedings of the 13th ACM Conference on Electronic Commerce, pp. 18–35, 2012. https://doi.org/10.1145/2229012.2229018
  • A. Bian, B. Mirzasoleiman, J. M. Buhmann, A. Krause, Guaranteed Non-convex Optimization: Submodular Maximization over Continuous Domains, AISTATS 2017. https://arxiv.org/abs/1606.05615
19 thms1 active userReviewed
Dynamic ProgrammingLinear OptimizationOperations Research·Captain: iris

Self-Adapting Network Relaxations for Weakly Coupled Markov Decision Processes: Every Feasibility Network Relaxation Bound Lies Between the Optimal Value and the Lagrangian BoundResearch Paper

Motivation

Many sequential decision problems in operations research consist of a number of independent subsystems that interact only through shared resources: assortment and inventory decisions under a common budget, multi-armed bandits with a cap on the number of arms pulled, scheduling with capacity limits. Such problems are modelled as weakly coupled Markov decision processes (WDPs) (Hawkins 2003; Adelman and Mersereau 2008). The joint state and action spaces grow exponentially in the number of subsystems, so the optimal policy value is out of reach, and upper bounds on it are used both to assess heuristic policies and to derive policies of their own.

The standard bound is the Lagrangian relaxation, which dualizes the linking constraints and decomposes the problem into one small MDP per subsystem. Its weakness is that it enforces the linking constraints only on average. Nadarajah and Cire (SSRN 4081430, 2023) propose to replace the averaged constraints by an exact representation of the feasible joint actions as paths in a layered network, the feasibility network, and to impose flow conservation on that network inside the linear program. The resulting feasibility network relaxation (FNR) stays decomposable and, as this mission formalizes, never gives a worse bound than the Lagrangian one.

Setting

A WDP has JJJ component MDPs indexed by j∈{1,…,J}j\in\{1,\dots,J\}j∈{1,…,J} and decision periods t∈T={0,…,T−1}t\in\mathcal T=\{0,\dots,T-1\}t∈T={0,…,T−1}. In period ttt, component jjj is in a state sjs_jsj​ of a finite set St,j\mathcal S_{t,j}St,j​, chooses an action aja_jaj​ from a finite set At,j(sj)\mathcal A_{t,j}(s_j)At,j​(sj​), earns rt,j(sj,aj)r_{t,j}(s_j,a_j)rt,j​(sj​,aj​) and moves to sj′s'_jsj′​ with probability P(sj′∣sj,aj)\mathbb P(s'_j\mid s_j,a_j)P(sj′​∣sj​,aj​). The joint action a=(a1,…,aJ)a=(a_1,\dots,a_J)a=(a1​,…,aJ​) must satisfy KKK linking constraints ∑jCt,k,j(sj,aj)≤bk\sum_j C_{t,k,j}(s_j,a_j)\le b_k∑j​Ct,k,j​(sj​,aj​)≤bk​; the joint feasible action set is At(s)\mathcal A_t(s)At​(s) and Ft\mathscr F_tFt​ is the set of feasible pairs (s,a)(s,a)(s,a) of period ttt. The initial state is a single point s0s^0s0, and every state of a decision period has a feasible action.

The value function VtV_tVt​ is defined by the Bellman equations Vt(s)=max⁡a∈At(s){rt(s,a)+∑s′P(s′∣s,a)Vt+1(s′)}V_t(s)=\max_{a\in\mathcal A_t(s)}\{r_t(s,a)+\sum_{s'}\mathbb P(s'\mid s,a)V_{t+1}(s')\}Vt​(s)=maxa∈At​(s)​{rt​(s,a)+∑s′​P(s′∣s,a)Vt+1​(s′)} with VT=0V_T=0VT​=0, where the joint transition is the product of the component transitions and rtr_trt​ the sum of the component rewards. V0(s0)V_0(s^0)V0​(s0) is the optimal policy value. Its LP dual DLP optimizes over joint state–action frequencies xt(s,a)x_t(s,a)xt​(s,a).

D-LAG is the Lagrangian flow program: component frequencies xt,j(sj,aj)x_{t,j}(s_j,a_j)xt,j​(sj​,aj​) satisfying per-component flow conservation (7)–(8), nonnegativity (10), and the averaged linking constraints (9) ∑j∑sj,ajCt,k,j(sj,aj)xt,j(sj,aj)≤bk\sum_j\sum_{s_j,a_j}C_{t,k,j}(s_j,a_j)x_{t,j}(s_j,a_j)\le b_k∑j​∑sj​,aj​​Ct,k,j​(sj​,aj​)xt,j​(sj​,aj​)≤bk​. Its optimal value is zLAGz^{\mathrm{LAG}}zLAG.

A feasibility network Nt\mathcal N_tNt​ of Ft\mathscr F_tFt​ has J+1J+1J+1 layers of nodes, a single root, and arcs from layer jjj to layer j+1j+1j+1 labelled by component pairs (sj,aj)(s_j,a_j)(sj​,aj​); every root-to-last-layer path spells out a pair (s,a)(s,a)(s,a), and the map from paths to pairs is a bijection onto Ft\mathscr F_tFt​. The slack network, whose nodes record the remaining capacity of each linking constraint, is one example. FNR keeps the component flow constraints, introduces arc flows yt,j(v,sj,aj)y_{t,j}(v,s_j,a_j)yt,j​(v,sj​,aj​) with xt,j(sj,aj)=∑vyt,j(v,sj,aj)x_{t,j}(s_j,a_j)=\sum_v y_{t,j}(v,s_j,a_j)xt,j​(sj​,aj​)=∑v​yt,j​(v,sj​,aj​) (18), and imposes flow conservation at every interior node (19); its optimal value is zFNRz^{\mathrm{FNR}}zFNR.

Formalization targets

Goal: Proposition 4 (Bound Ordering)

For every WDP and every family (Nt)t∈T(\mathcal N_t)_{t\in\mathcal T}(Nt​)t∈T​ of feasibility networks,

zLAG ≥ zFNR ≥ V0(s0).z^{\mathrm{LAG}}\ \ge\ z^{\mathrm{FNR}}\ \ge\ V_0(s^0).zLAG ≥ zFNR ≥ V0​(s0).

Both inequalities are part of the goal. No network is fixed: the statement covers the slack network, the minimal network and every other feasibility network.

Milestones

  1. Proposition 1: the linking constraints are equivalent to a chain of slack equalities ending in a nonnegative slack.
  2. Corollary 1: the slack network is a feasibility network, so FNR is always available.
  3. §2.1: the optimal value of DLP is V0(s0)V_0(s^0)V0​(s0).
  4. Lemma EC.2: the arc flow y′y'y′ of any FNR solution is a convex combination of path indicators.
  5. Proof of Proposition 4, (EC.20)–(EC.25): every FNR solution is D-LAG feasible.
  6. Proof of Proposition 4, (EC.27)–(EC.37): every DLP solution yields an FNR solution with the same objective.

Significance

Proposition 4 is what makes FNR a valid relaxation: its value is an upper bound on the optimal policy value, and it is never weaker than the Lagrangian bound, whichever feasibility network is used. This is what justifies building FNR on the smallest feasibility network, the paper's self-adapting network, whose size reflects how hard the linking constraints are to represent. In the paper's knapsack-bandit illustration (§4.3, pp.21–23) the Lagrangian bound is 69.667 while FNR attains the optimal value 49.

The result is proved in the paper; no machine-checked proof exists. Formalizing it gives a checked model of finite-horizon weakly coupled MDPs with their linear programs, and the first formal statement of flow decomposition on layered networks in this setting. Beyond Proposition 4, a formal proof requires LP duality for the finite-horizon MDP (milestone 3), which is reusable for any finite MDP development.

Difficulty

The first inequality looks like a monotonicity statement, but the two programs have different variables: FNR's linking information lives in the arc flows yyy, and the averaged constraint (9) holds only after the flow is decomposed into paths (Lemma EC.2) and the linking constraints of each path are summed. For periods after the first, the total flow of one is not given by any single constraint; it propagates through the component flow constraints and the stochasticity of the transitions. The decomposition uses the single root and the fact that each node–state–action triple carries one arc.

The second inequality cannot be obtained from the first: it goes through the joint program DLP, whose variables are indexed by exponentially many joint pairs, and through LP duality for the Bellman equations. Mapping a DLP solution to FNR needs the bijection between paths and feasible pairs in both directions, and checking the component flow constraints (8) needs the product form of the joint transitions.

Formalization scope

All objects are finite. Components, layers and constraints are 0-based (Fin J, Fin (J+1), Fin K); periods are natural numbers with decision periods t<Tt<Tt<T. A WDP is a structure carrying the component spaces, action sets, transitions (nonnegative, summing to one), rewards, linking data, the singleton initial state and the nonemptiness of At(s)\mathcal A_t(s)At​(s). VtV_tVt​ is defined by the Bellman recursion with a maximum over a nonempty finite set. Optimal values of D-LAG, FNR and DLP are suprema in EReal, so an empty or unbounded program cannot be read as 000. A layered network has finite layers, a unique root, and arcs given by a partial successor map on node–state–action triples; a feasibility network is one whose path-to-label map is injective with range Ft\mathscr F_tFt​. LP variables are functions of all indices, and only those of the paper appear in constraints and objectives.

The statement is not trivial on degenerate data: the coefficients and right-hand sides have no sign restriction, K=0K=0K=0 and J=1J=1J=1 are allowed, and the verification files exhibit a WDP with a feasibility network whose FNR value is finite.

Contributions welcome: the flow decomposition of Lemma EC.2, the duality argument for DLP, and the proof of Corollary 1 for the slack network. Related platform work: the Brown–Zhang mission on weakly coupled DPs (WeaklyCoupledDP.*), which uses a different model with exogenous states and is not reused here.

Selected references

  • S. Nadarajah, A. A. Cire, Self-Adapting Network Relaxations for Weakly Coupled Markov Decision Processes, SSRN 4081430, version of August 2023. https://ssrn.com/abstract=4081430 (published in Management Science, https://doi.org/10.1287/mnsc.2022.01108).
  • J. T. Hawkins, A Langrangian decomposition approach to weakly coupled dynamic optimization problems and its applications, PhD thesis, Massachusetts Institute of Technology, 2003.
  • D. Adelman, A. J. Mersereau, Relaxations of weakly coupled stochastic dynamic programs, Operations Research 56(3), 2008. https://doi.org/10.1287/opre.1070.0445
  • D. P. Bertsekas, Dynamic Programming and Optimal Control, Vol. II, 4th ed., Athena Scientific, 2012.
  • R. K. Ahuja, T. L. Magnanti, J. B. Orlin, Network Flows: Theory, Algorithms, and Applications, Prentice Hall, 1993.
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Operations ResearchProbabilityRevenue Management and Pricing·Captain: iris

Technical Note—A Note on State-Independent Policies in Network Revenue Management: the make-to-stock policy has optimality gap O(k)O(\sqrt{k})O(k​) under non-separable demandResearch Paper

Motivation

An airline, a hotel chain or an online retailer sells many products that draw on a shared, limited stock of resources: seats on flight legs, rooms on nights, units of a component. Choosing prices in real time from the current stock is the network revenue management problem, and it is intractable in general. A practical answer is a state-independent policy, whose prices depend on time only and are read off a deterministic relaxation. The central question is how much revenue such a simple policy gives up.

Timeline:

  • Gallego and van Ryzin (1994) solved the single-product problem and showed that a fixed price, computed from the deterministic problem, is asymptotically optimal (doi:10.1287/mnsc.40.8.999).
  • Gallego and van Ryzin (1997) introduced the multiproduct network problem and the make-to-stock (MTS) and make-to-order policies, and showed that their optimality gaps scale like k\sqrt kk​ when demand and capacity are scaled by kkk (doi:10.1287/opre.45.1.24).
  • Manchiraju, Dawande and Janakiraman observed that the 1997 analysis implicitly assumes that the demand for a product depends only on its own price, and proved the k\sqrt kk​ rate without that assumption (SSRN 3831496; published in Operations Research, doi:10.1287/opre.2023.2471).

This mission formalizes the last result for the continuous-price problem. All numbering refers to the SSRN version.

Setting

There are MMM resources and NNN products. One unit of product nnn uses am,n≥0a_{m,n}\ge0am,n​≥0 units of resource mmm, and resource mmm has capacity bm∈Nb_m\in\mathbb Nbm​∈N. Time runs over [0,T][0,T][0,T], which is cut into finitely many pieces. On each piece the set Λt\Lambda_tΛt​ of feasible rate vectors is convex and contains 000, and the revenue rate RtR_tRt​ is concave on Λt\Lambda_tΛt​. Choosing a price vector is the same as choosing a rate vector λt∈Λt\lambda_t\in\Lambda_tλt​∈Λt​: sales of product nnn are Poisson at rate λn,t\lambda_{n,t}λn,t​, and λn,t\lambda_{n,t}λn,t​ may depend on the prices of all products.

A policy chooses λt\lambda_tλt​ without looking ahead and must respect capacity. The optimal value ΠC\Pi_CΠC​ is the supremum of its expected revenue E∫0TRt(λt) dt\mathbb E\int_0^TR_t(\lambda_t)\,dtE∫0T​Rt​(λt​)dt.

The deterministic problem PDet\mathbb P_{\mathrm{Det}}PDet​ maximizes ∫0TRt(λt) dt\int_0^TR_t(\lambda_t)\,dt∫0T​Rt​(λt​)dt subject to A∫0Tλt dt≤bA\int_0^T\lambda_t\,dt\le bA∫0T​λt​dt≤b. Let λ∗\lambda^*λ∗ be an optimal solution, rt∗=Rt(λt∗)r^*_t=R_t(\lambda^*_t)rt∗​=Rt​(λt∗​), Λn∗[0,T]=∫0Tλn,t∗ dt\Lambda^*_n[0,T]=\int_0^T\lambda^*_{n,t}\,dtΛn∗​[0,T]=∫0T​λn,t∗​dt and Dn=⌊Λn∗[0,T]⌋D_n=\lfloor\Lambda^*_n[0,T]\rfloorDn​=⌊Λn∗​[0,T]⌋. Assume λn,t∗≥λ‾n>0\lambda^*_{n,t}\ge\underline\lambda_n>0λn,t∗​≥λ​n​>0 and rt∗≤rˉ∗r^*_t\le\bar r^*rt∗​≤rˉ∗ on [0,T][0,T][0,T].

The MTS policy follows λ∗\lambda^*λ∗ until the first time τ\tauτ at which some product nnn has sold DnD_nDn​ units, and then sets the rate to zero. The kkk-scaled problem PC,k\mathbb P_{C,k}PC,k​ multiplies the rates and the capacities by kkk. Write ΠC,k\Pi_{C,k}ΠC,k​ for its optimal value and ΠC,kMTS\Pi^{MTS}_{C,k}ΠC,kMTS​ for the expected revenue of MTS in it.

Formalization targets

Goal: Theorem 1

For every k≥1k\ge1k≥1, the MTS policy is admissible for PC,k\mathbb P_{C,k}PC,k​, and

ΠC,k−ΠC,kMTS≤(rˉ∗∑n=1Nπ Λn∗[0,T]2 λ‾n)k+∑n=1Nrˉ∗λ‾n,ΠC,k−ΠC,kMTS=O(k).\Pi_{C,k}-\Pi^{MTS}_{C,k}\le\Big(\bar r^*\sum_{n=1}^N\frac{\sqrt{\pi\,\Lambda^*_n[0,T]}}{\sqrt2\,\underline\lambda_n}\Big)\sqrt k+\sum_{n=1}^N\frac{\bar r^*}{\underline\lambda_n}, \qquad \Pi_{C,k}-\Pi^{MTS}_{C,k}=O(\sqrt k).ΠC,k​−ΠC,kMTS​≤(rˉ∗n=1∑N​2​λ​n​πΛn∗​[0,T]​​)k​+n=1∑N​λ​n​rˉ∗​,ΠC,k​−ΠC,kMTS​=O(k​).

The paper prints DnD_nDn​ where this display has Λn∗[0,T]\Lambda^*_n[0,T]Λn∗​[0,T]. That version is false: for N=M=1N=M=1N=M=1, a=b=T=1a=b=T=1a=b=T=1, Λ=[0,12]\Lambda=[0,\tfrac12]Λ=[0,21​], R(λ)=2λ−λ2R(\lambda)=2\lambda-\lambda^2R(λ)=2λ−λ2, one has D=0D=0D=0, so the printed bound is 1.51.51.5 for all kkk, while the gap is at least 2.982.982.98 at k=50k=50k=50. The reason is that the floor DnD_nDn​ does not scale by kkk. The display above is the minimal correction, and it coincides with the printed bound when Λn∗[0,T]\Lambda^*_n[0,T]Λn∗​[0,T] is an integer.

Milestones

In proof order:

ΠC≤∫0Trt∗ dt  (1),ΠC,k≤k∫0Trt∗ dt,ΠC−ΠCMTS≤Δ  (4),\Pi_C\le\int_0^Tr^*_t\,dt\ \ (1),\qquad \Pi_{C,k}\le k\int_0^Tr^*_t\,dt,\qquad \Pi_C-\Pi_C^{MTS}\le\Delta\ \ (4),ΠC​≤∫0T​rt∗​dt  (1),ΠC,k​≤k∫0T​rt∗​dt,ΠC​−ΠCMTS​≤Δ  (4), Δ≤rˉ∗ E[(T−τ)+]  (7),E[(T−τ)+]≤∑nE[(T−τn)+]  (8),\Delta\le\bar r^*\,\mathbb E[(T-\tau)^+]\ \ (7),\qquad \mathbb E[(T-\tau)^+]\le\sum_n\mathbb E[(T-\tau_n)^+]\ \ (8),Δ≤rˉ∗E[(T−τ)+]  (7),E[(T−τ)+]≤n∑​E[(T−τn​)+]  (8),

the Poisson tail bound (12), the integral bound (11), Lemma 1

E[(T−τn)+]≤πDn2 λ‾n+1λ‾n,\mathbb E[(T-\tau_n)^+]\le\frac{\sqrt{\pi D_n}}{\sqrt2\,\underline\lambda_n}+\frac1{\underline\lambda_n},E[(T−τn​)+]≤2​λ​n​πDn​​​+λ​n​1​,

and the non-asymptotic bound of p.13, ΠC−ΠCMTS≤rˉ∗∑n(πDn/(2 λ‾n)+1/λ‾n)\Pi_C-\Pi_C^{MTS}\le\bar r^*\sum_n\big(\sqrt{\pi D_n}/(\sqrt2\,\underline\lambda_n)+1/\underline\lambda_n\big)ΠC​−ΠCMTS​≤rˉ∗∑n​(πDn​​/(2​λ​n​)+1/λ​n​).

Significance

The result. The theorem extends the square-root rate from separable to general demand models, which covers substitutes and complements, including multinomial logit and linear demand with cross-price effects. Since ΠC,k\Pi_{C,k}ΠC,k​ is of order kkk, the relative loss of a time-only policy vanishes at rate k−1/2k^{-1/2}k−1/2. The paper uses the same technique for its discrete-price and assortment results, which are outside this mission.

The formalization. The result is proved on paper, and to our knowledge none of it is machine-checked. A formal proof would add a continuous-time controlled Poisson model with an explicit policy class and would certify the constant, which the printed statement gets wrong. Inequalities (1) and (12) are cited by the paper without proof, so their proofs here are new work relative to the source.

Difficulty

The obvious route follows each product until its own stock runs out. It fails here: once one product stocks out and its price changes, the rates of the other products change too, so no product's sales stay Poisson at rate λn∗\lambda^*_nλn∗​ after the first stock-out. A second obstacle is that a hitting time of a non-homogeneous Poisson process is not a sum of i.i.d. exponentials, so distribution-free newsvendor bounds do not apply. A third is (1): a Jensen argument for a concave RtR_tRt​ on a convex Λt\Lambda_tΛt​ that is neither closed nor continuous, against policies that may depend on the whole past. Mathlib's Jensen inequality asks for closedness and continuity. Finally, admissibility of MTS needs optional stopping in continuous time, which Mathlib only has in discrete time.

Formalization scope

Products and resources are Fin N, Fin M, counted from 000. An Instance holds the data above, with Rj(0)=0R_j(0)=0Rj​(0)=0 and Λj\Lambda_jΛj​ in the nonnegative orthant; closedness of Λj\Lambda_jΛj​ and continuity of RjR_jRj​ are not assumed, and prices are not modelled. Pieces are half-open with the last one closed.

A policy is formalized as a PricingSystem: a filtration indexed by Set.Icc 0 T, a progressively measurable rate process and counting processes with unit jumps, such that Xn(t)−∫0tλn,s dsX_n(t)-\int_0^t\lambda_{n,s}\,dsXn​(t)−∫0t​λn,s​ds is a martingale on [0,T][0,T][0,T], capacity holds almost surely at TTT, and the revenue rate is integrable. The compensator condition excludes look-ahead and keeps every non-anticipatory policy. Revenue is E∫0TRt(λt) dt\mathbb E\int_0^TR_t(\lambda_t)\,dtE∫0T​Rt​(λt​)dt, and ΠC\Pi_CΠC​ is a real sSup over sample spaces in Type. The value set is nonempty by the null policy and bounded above by (1).

MTS is the §3 p.9 policy (zero rate after τ\tauτ), not the p.7 one. Its demand process is a hypothesis of the theorem, IsPoissonDemand, with every path a counting path. The stock-out set always contains TTT, so sInf ∅ = 0 never occurs, and Dn=0D_n=0Dn​=0 gives τ=0\tau=0τ=0 as on the page. The rate bounds λ‾n\underline\lambda_nλ​n​, rˉ∗\bar r^*rˉ∗ are the paper's p.10 assumption; the upper rate bound λˉn\bar\lambda_nλˉn​ is unused and dropped.

No trivialization is available: the goal is stated about the supremum over all admissible policies and about the policy itself, never through Δ\DeltaΔ, τ\tauτ or the relaxed problem.

A complete development needs joint measurability and Jensen without closedness in RN\mathbb R^NRN, continuous-time optional stopping for right-continuous martingales, and Poisson tail bounds. The first two are reusable well beyond this mission. Proofs of any milestone are welcome, as are general lemmas on counting processes.

Selected references

  • C. Manchiraju, M. Dawande, G. Janakiraman, Technical Note—A Note on State-Independent Policies in Network Revenue Management, SSRN 3831496; Operations Research, 2023. https://ssrn.com/abstract=3831496, https://doi.org/10.1287/opre.2023.2471
  • G. Gallego, G. van Ryzin, A Multiproduct Dynamic Pricing Problem and Its Applications to Network Yield Management, Operations Research 45(1), 1997. https://doi.org/10.1287/opre.45.1.24
  • G. Gallego, G. van Ryzin, Optimal Dynamic Pricing of Inventories with Stochastic Demand over Finite Horizons, Management Science 40(8), 1994. https://doi.org/10.1287/mnsc.40.8.999
  • C. Canonne, A short note on Poisson tail bounds, 2019. http://www.cs.columbia.edu/~ccanonne/files/misc/2017-poissonconcentration.pdf
  • D. Pollard, MiniEmpirical, 2015. http://www.stat.yale.edu/~pollard/Books/Mini/Basic.pdf
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