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

Campaigns (experimental)

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

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About Prove2Me

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

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

Campaigns (experimental)

See all campaigns →

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

Block Sensitivity vs. Sensitivity

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

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

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

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

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

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

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

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

Integer Multiplication Below n log n

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

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

For two nnn-bit integers, the target is

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

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

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

3SUM Exponent

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

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

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

All-Pairs Shortest Paths (APSP) Exponent

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

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

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

The irrationality measure of π

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

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

Sharp diagonal Hlawka constant

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

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

References:

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

Odd numbers as sums of primes

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

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

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

Matrix multiplication exponent

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

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

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

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About Prove2Me

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

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Quantum Information·Captain: Goku

The characterization of Gaussian operations and Distillation of Gaussian StatesResearch Paper

Motivation

We characterize the class of all physical operations that transform Gaussian states to Gaussian states. We show that this class coincides with that of all operations which can be performed on Gaussian states using linear optical elements and homodyne measurements. For bipartite systems we characterize the processes which can be implemented by local operations and classical communication, as well as those that can be implemented using positive partial transpose preserving maps. As an application, we show that Gaussian states cannot be distilled by local Gaussian operations and classical communication. We also define and characterize positive (but not completely positive) Gaussian maps.

This mission is the statement-level formalization of The characterization of Gaussian operations and Distillation of Gaussian States (arXiv:quant-ph/0204085v4). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

5 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is The Gaussian entanglement scale is positive and attained (Appendix A, Eq.(A1): well-defined attained V for finite CMs, PDF p. 5). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Abstract; Sec. IVB: no Gaussian LOGCC distillation, including assistance: Actual Gaussian LOGCC instruments with adaptive classical communication and conditional normalized outputs (hard)
  • Sec. II, Eqs.(4)–(5): the finite EPR approximating family: Actual normalized squeezed states on bosonic Hilbert space and their characteristic functions (hard)
  • Sec. IIIA: full Gaussian Choi characterization and optical implementation: Admissible generalized Choi domain, convergence and exact-versus-limit optical implementation (source-ambiguity)
  • Sec. IIIA, Eqs.(9), (10a), (13): normalized conditional covariance: Finite-resource Gaussian Choi contraction on actual trace-class states (hard)
  • Sec. IIIA, Eq.(10b): printed displacement formula: Consistent displacement parameterization in Eqs.(8),(10b),(11),(12) (source-ambiguity)
  • Sec. IIIB: pure Gaussian displacement POVMs from homodyne: Weakly countably additive normalized displaced pure-seed POVM and homodyne implementation (hard)
  • Sec. IIIB, Eq.(15a): conditional covariance of a pure Gaussian projection: Actual normalized Gaussian conditional state of a partial pure-seed projection (hard)
  • Sec. IIIB, Eqs.(14), (15b): printed measurement means: Consistent centering, factor and measurement-label convention for Eqs.(14),(15b) (source-ambiguity)
  • Sec. IIIB: infinitely squeezed projection and pseudoinverse: Specified quadrature projection, limiting finite block, outcome scaling and convergence topology (source-ambiguity)
  • Sec. IIIB, pp.3–4: noise on a Gaussian operation is output displacement noise: Degenerate Gaussian displacement laws acting on actual normalized conditional outputs (hard)
  • Sec. IIIC: deterministic realization for known covariance: Trace-preserving Bell spectral instrument with covariance-dependent displacement feedback (hard)
  • Sec. IVA: Gaussian LOCC/PPT classification by the Choi state: Generalized Gaussian Choi object supporting separable/PPT/NPT classification (source-ambiguity)
  • Sec. IVA/IVB: separable Gaussian resource maps are products plus correlated noise: Finite-resource separability as actual state separability and its product-operation/noise implementation (hard)
  • Sec. IVB, Eqs.(16)–(17): Gaussian local monotonicity of V: Actual normalized branch action of all separable Gaussian completely positive operations (hard)
  • Sec. V: boundedness, self-adjointness, positivity and trace of Gaussian operators: Convergence domain, scalar-phase quotient/sign and corrected CCR trace normalization (source-ambiguity)
  • Sec. V: general Gaussian linear kernels and Weyl action: Analytic domain and admissible generalized Gaussian operator kernels (source-ambiguity)
  • Sec. V: adjoint preservation of Gaussian maps: Scalar phase quotient in adjoint-preservation criterion (source-ambiguity)
  • Sec. V, Eqs.(20)–(21): Gaussian positivity criterion: Generalized Schur range conditions and scalar positivity for admitted singular maps (source-ambiguity)
  • Sec. V: claimed numerical efficiency of the positivity test: Numerical input representation, tolerance, promise and complexity bound (source-ambiguity)
  • Appendix A(4): V detects PPT Gaussian entanglement: Actual Gaussian separability, partial transpose and trace-class negativity (hard)
  • Appendix A(5): V as a Gaussian entanglement quantity: Actual local Gaussian operations and independently defined Gaussian entanglement (hard)
  • Appendix A(6): asserted computability of V: Effective representation and certified approximation algorithm for V (source-ambiguity)
  • Reference note [23]: proposed regularized Choi/Bell limit: Normalized regularizer, compensating scaling and a valid Bell POVM limit (source-ambiguity)

Selected references

  • The characterization of Gaussian operations and Distillation of Gaussian States, arXiv:quant-ph/0204085v4, https://arxiv.org/abs/quant-ph/0204085v4
7 thms2 active usersReviewed
Quantum Information·Captain: Goku

Advanced Alicki-Fannes-Winter method for energy-constrained quantum systems and its useResearch Paper

Motivation

We describe an universal method for quantitative continuity analysis of entropic characteristics of energy-constrained quantum systems and channels. It gives asymptotically tight continuity bounds for basic characteristics of quantum systems of wide class (including multi-mode quantum oscillators) and channels between such systems under the energy constraint. The main application of the proposed method is the advanced version of the uniform finite-dimensional approximation theorem for basic capacities of energy-constrained quantum channels.

This mission is the statement-level formalization of Advanced Alicki-Fannes-Winter method for energy-constrained quantum systems and its use (arXiv:1907.02458v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

2 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Minimal entropy majorant and spectral asymptotics (Proposition 1(A,B), PDF p. 7). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Lemma 1: completed bipartite trace-class marginals and spectral marginal rank (hard)
  • Theorem 1: general multipartite finite-energy AFW function domains and optimized tightness modulus (hard)
  • Lemma 2: locally finite-rank multipartite state domain and trace-norm uniformly continuous extensions (hard)
  • Theorem 2: canonical extension through all finite-A-rank states, including nondense Hamiltonians (hard)
  • Example 1: canonical real extension of a difference of possibly infinite mutual informations (hard)
  • Corollary 1: Fock-space oscillator Hamiltonian and general AFW-function tightness (hard)
  • Example 2: full entropy continuity statement with oscillator specialization and optimal-t tightness (hard)
  • Example 3: extended conditional entropy on arbitrary completed bipartite spaces (hard)
  • Example 4: extended QCMI finite-projection supremum for all eight energy subsystems (hard)
  • Proposition 2: infinite-dimensional channel tensor action and extended output QCMI (hard)
  • Lemma 3: purification-defined mutual and coherent information of arbitrary trace-class channels (hard)
  • Proposition 3: channel information, complementary channels and degradability in the same infinite-state model (hard)
  • Proposition 4: generalized ensemble Holevo integral and three genuine ensemble metrics (hard)
  • Proposition 5: generalized-ensemble privacy with complementary CPTP channel and subclass predicates (hard)
  • Lemma 4: correlated n-copy CPTP truncation and actual output mutual-information variation (hard)
  • Theorem 3: boundary-inclusive least-dimension certificate at zero energy excess (source-ambiguity)
  • Theorem 3, positive-excess clause: six infinite-dimensional energy-constrained capacities and their input-subspace restrictions (hard)
  • Theorem 3, ground-energy existence clause: six genuine capacities restricted to the full finite ground eigenspace (hard)

Selected references

  • Advanced Alicki-Fannes-Winter method for energy-constrained quantum systems and its use, arXiv:1907.02458v3, https://arxiv.org/abs/1907.02458v3
4 thms2 active usersReviewed
Quantum Information·Captain: Goku

A Resource Framework for Quantum Shannon TheoryResearch Paper

Motivation

Quantum Shannon theory is loosely defined as a collection of coding theorems, such as classical and quantum source compression, noisy channel coding theorems, entanglement distillation, etc., which characterize asymptotic properties of quantum and classical channels and states. In this paper we advocate a unified approach to an important class of problems in quantum Shannon theory, consisting of those that are bipartite, unidirectional and memoryless. We formalize two principles that have long been tacitly understood. First, we describe how the Church of the larger Hilbert space allows us to move flexibly between states, channels, ensembles and their purifications. Second, we introduce finite and asymptotic (quantum) information processing resources as the basic objects of quantum Shannon theory and recast the protocols used in direct coding theorems as inequalities between resources. We develop the rules of a resource calculus which allows us to manipulate and combine resource inequalities. This framework simplifies many coding theorem proofs and provides structural insights into the logical dependencies among coding theorems. We review the above-mentioned basic coding results and show how a subset of them can be unified into a family of related resource inequalities. Finally, we use this family to find optimal trade-off curves for all protocols involving one noisy quantum resource and two noiseless ones.

This mission is the statement-level formalization of A Resource Framework for Quantum Shannon Theory (arXiv:quant-ph/0512015v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

3 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Continuity of the entropic quantities (Lemma 2.1, PDF p. 8). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Lemma 2.4: four relative-operation-distance bounds: Relative operation distance with a specified constrained subsystem and arbitrary reference, together with heterogeneous tensor/composition contexts preserving every B and C factor. (hard)
  • Corollary 3.9: parallel validity: Generalized finite resources and typed protocol combs with passive Source factors, arbitrary call permutation, universal extension validity, compatible-test distance, and standard flattening. (hard)
  • Lemma 3.10: flattening preserves finite reductions: Generalized finite resources and typed protocol combs with passive Source factors, arbitrary call permutation, universal extension validity, compatible-test distance, and standard flattening. (hard)
  • Lemma 3.11: simulation respects reductions: Generalized finite resources and typed protocol combs with passive Source factors, arbitrary call permutation, universal extension validity, compatible-test distance, and standard flattening. (hard)
  • Lemma 3.12: parallel simulation errors add: Generalized finite resources and typed protocol combs with passive Source factors, arbitrary call permutation, universal extension validity, compatible-test distance, and standard flattening. (hard)
  • Lemma 3.13: composition and validity: Generalized finite resources and typed protocol combs with passive Source factors, arbitrary call permutation, universal extension validity, compatible-test distance, and standard flattening. (hard)
  • Lemma 3.14: continuity of finite protocols: Generalized finite resources and typed protocol combs with passive Source factors, arbitrary call permutation, universal extension validity, compatible-test distance, and standard flattening. (hard)
  • Lemma 3.15: sliding: Generalized finite resources and typed protocol combs with passive Source factors, arbitrary call permutation, universal extension validity, compatible-test distance, and standard flattening. (hard)
  • Lemma 3.16: finite absolutization with randomness: Generalized finite resources and typed protocol combs with passive Source factors, arbitrary call permutation, universal extension validity, compatible-test distance, and standard flattening. (hard)
  • Corollary 3.25: eventual reductions imply asymptotic simulation: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Lemma 3.26: one-way flattening: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Theorem 3.29 (Composability): transitivity, addition and scaling: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Example 3.31: ebit rank convention: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Unnumbered addition laws after Definition 3.22: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Unnumbered closure under multiplication after Definition 3.23: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Lemma 3.32: scaling algebra: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Lemma 3.34: operations descend to equivalence classes: Actual quotient of source-defined asymptotic resources by mutual operational simulation, with representative-independent order, addition and scalar operations. (hard)
  • Proposition 3.35: partial order on resource classes: Actual quotient of source-defined asymptotic resources by mutual operational simulation, with representative-independent order, addition and scalar operations. (hard)
  • Proposition 3.36: positive scalar action on resource classes: Actual quotient of source-defined asymptotic resources by mutual operational simulation, with representative-independent order, addition and scalar operations. (hard)
  • Proposition 3.37: monotonicity of quotient operations: Actual quotient of source-defined asymptotic resources by mutual operational simulation, with representative-independent order, addition and scalar operations. (hard)
  • Lemma 4.1: five elementary resource inequalities: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Lemma 4.2: closure in a positive scalar coefficient: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Lemma 4.5: remove generatable sublinear resources: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Lemma 4.6: cancellation with sublinear assistance: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Lemma 4.7: recycle decoupled shared randomness: Witnessed asymptotic protocol families with retained classical copies and coherent or incoherent decoupling, including every discarded ancilla and environment when coherent. (hard)
  • Corollary 4.8: derandomization for pure output: Witnessed asymptotic protocol families with retained classical copies and coherent or incoherent decoupling, including every discarded ancilla and environment when coherent. (hard)
  • Theorem 4.9: absolutization of standard units: Witnessed asymptotic protocol families with retained classical copies and coherent or incoherent decoupling, including every discarded ancilla and environment when coherent. (hard)
  • Lemma 4.10: fake a source absent from the target: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Lemma 4.11: proper versus improper source coding: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Theorem 4.12: extract a flagged ensemble of resources: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Unnumbered strengthened flagged-state equality (32): Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Theorem 4.13: flagged source redirection: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Corollary 4.14: stochastic preprocessing of a flagged source: Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Theorem 6.1 (Rule I): coherent classical input: Witnessed asymptotic protocol families with retained classical copies and coherent or incoherent decoupling, including every discarded ancilla and environment when coherent. (hard)
  • Proposition 6.2: incoherent Rule I: Witnessed asymptotic protocol families with retained classical copies and coherent or incoherent decoupling, including every discarded ancilla and environment when coherent. (hard)
  • Theorem 6.3 (Rule O): coherent classical output: Witnessed asymptotic protocol families with retained classical copies and coherent or incoherent decoupling, including every discarded ancilla and environment when coherent. (hard)
  • Corollary 6.4: mother from coherified hashing: The specific cited finite protocol families, their QP dilations/ancillary registers, and the decoupling and uniformity properties required for the named coherification derivation. (hard)
  • Corollary 6.5: father from coherified EAC: The specific cited finite protocol families, their QP dilations/ancillary registers, and the decoupling and uniformity properties required for the named coherification derivation. (hard)
  • Corollary 6.6: mother from coherified noisy dense coding: The specific cited finite protocol families, their QP dilations/ancillary registers, and the decoupling and uniformity properties required for the named coherification derivation. (source-ambiguity)
  • Unnumbered family child: hashing with sublinear ebits (67): Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Unnumbered family child: noisy teleportation with sublinear ebits (68): Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Unnumbered family child: quantum capacity with sublinear ebits (69): Source-defined asymptotic resources of fixed finite component depth, finite reductions, eventual monotonicity/quasi-i.i.d. conditions, and the operational simulation relation with its exact quantifier order. (hard)
  • Theorem 7.1 (Grandmother): Remote finite Kraus instruments with QP environments, their computed conditional entropies, and the source-defined signed asymptotic RI for a noisy shared input state. (hard)
  • Corollary 7.2: independent random preprocessing: The independent-ensemble special case of the grandmother operational RI, retaining both conditional half-mutual-information rates and a QP extension of each channel. (hard)
  • Theorem 7.3: noisy super-dense coding trade-off: Operational two-rate regions for one given noisy i.i.d. resource, and arbitrary finite-auxiliary single-block ensemble/instrument regions with two-coordinate regularization. (hard)
  • Theorem 7.4: mother trade-off: Operational two-rate regions for one given noisy i.i.d. resource, and arbitrary finite-auxiliary single-block ensemble/instrument regions with two-coordinate regularization. (hard)
  • Theorem 7.5: noisy teleportation trade-off: Operational two-rate regions for one given noisy i.i.d. resource, and arbitrary finite-auxiliary single-block ensemble/instrument regions with two-coordinate regularization. (hard)
  • Theorem 7.6: entanglement-distillation trade-off: Operational two-rate regions for one given noisy i.i.d. resource, and arbitrary finite-auxiliary single-block ensemble/instrument regions with two-coordinate regularization. (hard)
  • Theorem 7.7: entanglement-assisted quantum trade-off: Operational two-rate regions for one given noisy i.i.d. resource, and arbitrary finite-auxiliary single-block ensemble/instrument regions with two-coordinate regularization. (hard)
  • Theorem 7.8: entanglement-assisted classical trade-off: Operational two-rate regions for one given noisy i.i.d. resource, and arbitrary finite-auxiliary single-block ensemble/instrument regions with two-coordinate regularization. (hard)
  • Supporting unnumbered direct RI (88): Remote finite Kraus instruments with QP environments, their computed conditional entropies, and the source-defined signed asymptotic RI for a noisy shared input state. (hard)
  • Supporting unnumbered direct RI (94): Remote finite Kraus instruments with QP environments, their computed conditional entropies, and the source-defined signed asymptotic RI for a noisy shared input state. (hard)

Selected references

  • A Resource Framework for Quantum Shannon Theory, arXiv:quant-ph/0512015v1, https://arxiv.org/abs/quant-ph/0512015v1
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Quantum Information·Captain: Goku

Continuous ensembles and the chi-capacity of infinite-dimensional channelsResearch Paper

Motivation

The paper is devoted to systematic study of the χ\chiχ-capacity (underlying the classical capacity) of infinite dimensional quantum channels. An essential feature of this case is the natural appearance of the input constraints and infinite, in general, continuous'' state ensembles, defined as probability measures on the set of all quantum states. By using compactness criteria from probability theory and operator theory it is shown that the set of all generalized ensembles with the average (barycenter) in a compact set of states is itself a compact subset of the set of all probability measures. With this in hand we give a sufficient condition for the existence of an optimal generalized ensemble for a constrained quantum channel. This condition can be verified in the case of Bosonic Gaussian channels with constrained mean energy. The importance of the above condition is shown by considering example of a constrained channel with no optimal generalized ensemble. In the case of convex constraints a characterization of the optimal generalized ensemble is obtained extending the maximal distance'' property.

This mission is the statement-level formalization of Continuous ensembles and the chi-capacity of infinite-dimensional channels (arXiv:quant-ph/0408176v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

15 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is §4, unnumbered Theorem: pure-state optimal generalized ensemble (§4, unnumbered Theorem: pure-state optimal generalized ensemble, PDF p. 8). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • §2, unnumbered: existence of the Bochner average: A trace-norm Banach realization of all trace-class operators, with the inclusion of states as a strongly measurable Banach-valued function. (hard)
  • Lemma 3: compact sets have a common energy bound: A consistent finite-dimensional convention for H-operators, or an explicit infinite-dimensional hypothesis. (source-ambiguity)
  • Proposition 3: output Gibbs condition ensures attainment: Positive unbounded discrete-spectrum observables with dense domains, cutoff energy and all-positive-beta Gibbs trace. (hard)
  • §4, unnumbered: Gaussian channels with oscillator power constraints: Finite-mode Weyl/CCR systems, Gaussian dilation and oscillator Hamiltonians with their unbounded domains. (hard)
  • Appendix B: compact constraint without an optimal generalized ensemble: Classical l1 probability states with l1 topology, their Borel ensembles and bits-valued identity-channel Holevo capacity. (hard)

Selected references

  • Continuous ensembles and the chi-capacity of infinite-dimensional channels, arXiv:quant-ph/0408176v1, https://arxiv.org/abs/quant-ph/0408176v1
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Quantum Information·Captain: Goku

Measures of quantum correlations in infinite-dimensional systemsResearch Paper

Motivation

Several important measures of quantum correlations of a state of a finite-dimensional composite system are defined as linear combinations of marginal entropies of this state. This paper is devoted to the infinite-dimensional generalizations of such quantities and to the analysis of their properties. We introduce the notion of faithful extension of a linear combination of marginal entropies and consider several concrete examples starting with the quantum mutual information and the quantum conditional entropy. Then we show that the conditional mutual information can be uniquely defined as a lower semicontinuous function on the set of all states of a tripartite infinite-dimensional system possessing all the basic properties valid in finite dimensions. Infinite-dimensional generalizations of some other measures of quantum correlations in multipartite quantum systems are also considered. It is shown that almost all of these generalized measures are globally lower semicontinuous and possess local continuity properties which essentially simplify their use in analysis of quantum systems. In the second part of the paper we consider applications of the general results of its first part, in particular, to the theory of infinite-dimensional quantum channels and their capacities. We also show the existence of the Fawzi-Renner recovery channel reproducing marginal states for all tripartite states (including states with infinite marginal entropies) starting with the corresponding finite-dimensional result.

This mission is the statement-level formalization of Measures of quantum correlations in infinite-dimensional systems (arXiv:1506.06377v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

5 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Lemma 1: lifting convergent marginals to pure states (Lemma 1: lifting convergent marginals to pure states, PDF p. 7). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Lemma 2: marginal entropy convergence under local truncation: Extended spectral von Neumann entropy on the full nuclear trace-class cone and arbitrary multipartite marginals (hard)
  • Lemma 4: lower semicontinuity and local-operation monotonicity imply faithfulness: Local bounded orthogonal projections on countable Hilbert factors; tensor compressions, positive-trace normalization and faithful truncation limits (hard)
  • Lemma 5: uniqueness of faithful extension: Local bounded orthogonal projections on countable Hilbert factors; tensor compressions, positive-trace normalization and faithful truncation limits (hard)
  • Lemma 6: linearity of faithful extensions: Local bounded orthogonal projections on countable Hilbert factors; tensor compressions, positive-trace normalization and faithful truncation limits (hard)
  • Proposition 1: bounded entropy combinations extend uniformly continuously: Extended spectral von Neumann entropy on the full nuclear trace-class cone and arbitrary multipartite marginals (hard)
  • Theorem 1 A–B: local continuity of bipartite mutual information: Full trace-class Umegaki relative entropy, homogeneous bipartite/multipartite mutual information, and local-operation tensor actions (hard)
  • Corollary 1: finite-A mutual information continuity bound: Full trace-class Umegaki relative entropy, homogeneous bipartite/multipartite mutual information, and local-operation tensor actions (hard)
  • Corollary 2: faithfulness of reduced mutual information: Full trace-class Umegaki relative entropy, homogeneous bipartite/multipartite mutual information, and local-operation tensor actions (hard)
  • Corollary 3 A–B: multipartite mutual-information convergence: Full trace-class Umegaki relative entropy, homogeneous bipartite/multipartite mutual information, and local-operation tensor actions (hard)
  • Corollary 4: multipartite mutual-information continuity bound: Full trace-class Umegaki relative entropy, homogeneous bipartite/multipartite mutual information, and local-operation tensor actions (hard)
  • Proposition 2: conditioning changes an entropy combination by a finite extension: Finite-first-marginal extended conditional entropy H_e=H(first)-I(first:conditioning) with infinite-dimensional marginals and faithful-extension domains (hard)
  • Proposition 3 A–B: extended quantum conditional entropy: Finite-first-marginal extended conditional entropy H_e=H(first)-I(first:conditioning) with infinite-dimensional marginals and faithful-extension domains (hard)
  • Corollary 5: continuity bound for extended conditional entropy: Finite-first-marginal extended conditional entropy H_e=H(first)-I(first:conditioning) with infinite-dimensional marginals and faithful-extension domains (hard)
  • Proposition 4: extension via a fixed finite-entropy subsystem: Finite-first-marginal extended conditional entropy H_e=H(first)-I(first:conditioning) with infinite-dimensional marginals and faithful-extension domains (hard)
  • Corollary 6: removing a finite-entropy register: Finite-first-marginal extended conditional entropy H_e=H(first)-I(first:conditioning) with infinite-dimensional marginals and faithful-extension domains (hard)
  • Theorem 2: unique lower-semicontinuous extended conditional mutual information: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Corollary 7 A–B: local continuity and dominated convergence of CMI: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Corollary 8: bounded continuity of CMI and its unconditional correction: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Corollary 9: ambient-system faithfulness and two-parameter approximation of CMI: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Corollary 10 A–C: mutual-information difference and continuity under partial trace: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Proposition 5 A–E: multipartite conditional mutual information: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Proposition 6 A–C: faithful extension of interaction information: Finite-first-marginal extended conditional entropy H_e=H(first)-I(first:conditioning) with infinite-dimensional marginals and faithful-extension domains (hard)
  • Corollary 11: interaction-information continuity bound: Finite-first-marginal extended conditional entropy H_e=H(first)-I(first:conditioning) with infinite-dimensional marginals and faithful-extension domains (hard)
  • Proposition 7 A–E: conditional and unconditional secrecy monotone: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Proposition 8 A–E: extension of the multipartite mutual-information gap: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Corollary 12: Wilde recovery inequality in infinite dimensions: Extended CMI, root fidelity of arbitrary trace-class states, and entangled tensor application of a recovery channel with simultaneous exact marginals (hard)
  • Proposition 9 A–C: triangle continuity relations for channels: Channel mutual information from trace-class purifications; complementary/Stinespring maps; finite-domain coherent information and entropy gain (hard)
  • Corollary 13: entropy-gain continuity for finite Choi rank: Channel mutual information from trace-class purifications; complementary/Stinespring maps; finite-domain coherent information and entropy gain (hard)
  • Proposition 10 A–C: joint continuity for channel mutual information: Channel mutual information from trace-class purifications; complementary/Stinespring maps; finite-domain coherent information and entropy gain (hard)
  • Corollary 14: joint continuity of coherent information: Channel mutual information from trace-class purifications; complementary/Stinespring maps; finite-domain coherent information and entropy gain (hard)
  • Proposition 11: global continuity of constrained entanglement-assisted capacity: Extended positive-form energy expectation, feasible-state constraint set, and ENNReal supremum of full channel mutual information (hard)
  • Corollary 15: bosonic energy-constrained capacity continuity: Canonical unbounded quadratures on a many-mode bosonic Hilbert space, nondegenerate quadratic-form Hamiltonian R^T epsilon R, and constrained assisted capacity (hard)
  • Proposition 12: local constrained-capacity continuity from output-entropy convergence: Extended positive-form energy expectation, feasible-state constraint set, and ENNReal supremum of full channel mutual information (hard)
  • Proposition 13: recovery with exact marginals for arbitrary tripartite states: Extended CMI, root fidelity of arbitrary trace-class states, and entangled tensor application of a recovery channel with simultaneous exact marginals (source-ambiguity)
  • Lemma 8: CMI continuity under product-marginal admixture: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Lemma 9: invariance and data processing on the finite-overlap cone: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Unnumbered §4.1: bipartite mutual information properties and faithful extension: Full trace-class Umegaki relative entropy, homogeneous bipartite/multipartite mutual information, and local-operation tensor actions (hard)
  • Unnumbered §4.1: exact global continuity criterion for mutual information: Full trace-class Umegaki relative entropy, homogeneous bipartite/multipartite mutual information, and local-operation tensor actions (hard)
  • Example 1: MI continuity without marginal entropy continuity: Full trace-class Umegaki relative entropy, homogeneous bipartite/multipartite mutual information, and local-operation tensor actions (hard)
  • Remark 4: faithfulness of combinations of MI and marginal entropy: Full trace-class Umegaki relative entropy, homogeneous bipartite/multipartite mutual information, and local-operation tensor actions (hard)
  • Unnumbered §4.2: multipartite MI chain rule and faithful extension: Full trace-class Umegaki relative entropy, homogeneous bipartite/multipartite mutual information, and local-operation tensor actions (hard)
  • Unnumbered (29): faithful extension of a conditioned entropy combination: Finite-first-marginal extended conditional entropy H_e=H(first)-I(first:conditioning) with infinite-dimensional marginals and faithful-extension domains (hard)
  • Unnumbered (33): faithfulness of sums of extended conditional entropies: Finite-first-marginal extended conditional entropy H_e=H(first)-I(first:conditioning) with infinite-dimensional marginals and faithful-extension domains (hard)
  • Remark 5: conditioning preserves fixed-subsystem entropy representations: Finite-first-marginal extended conditional entropy H_e=H(first)-I(first:conditioning) with infinite-dimensional marginals and faithful-extension domains (hard)
  • Remark 6: six upper bounds on extended CMI: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Remark 7: interaction information as an MI–CMI difference: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Unnumbered §7.2: additional properties of extended secrecy monotone: Constructed extended CMI via finite-rank projection suprema, signed finite corrections on S3/S4, and compatible system/tensor/reduction maps (hard)
  • Unnumbered (70)–(72): coherent information and entropy-gain extensions: Channel mutual information from trace-class purifications; complementary/Stinespring maps; finite-domain coherent information and entropy gain (hard)
  • Unnumbered §8.3: lower semicontinuity of constrained assisted capacity: Extended positive-form energy expectation, feasible-state constraint set, and ENNReal supremum of full channel mutual information (hard)
  • Example 2: compact energy constraints do not ensure capacity continuity: Extended positive-form energy expectation, feasible-state constraint set, and ENNReal supremum of full channel mutual information (hard)
  • Unnumbered (88): mutual-information balance for a pure tripartite operator: Full trace-class Umegaki relative entropy, homogeneous bipartite/multipartite mutual information, and local-operation tensor actions (hard)

Selected references

  • Measures of quantum correlations in infinite-dimensional systems, arXiv:1506.06377v2, https://arxiv.org/abs/1506.06377v2
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Quantum Information·Captain: Goku

Reachability, Coolability, and Stabilizability of Open Markovian Quantum Systems with Fast Unitary ControlResearch Paper

Motivation

Open Markovian quantum systems with fast and full Hamiltonian control can be reduced to an equivalent control system on the standard simplex modelling the dynamics of the eigenvalues of the density matrix describing the quantum state. We explore this reduced control system for answering questions on reachability and stabilizability with immediate applications to the cooling of Markovian quantum systems. We show that for certain tasks of interest, the control Hamiltonian can be chosen time-independent. -- The reduction picture is an example of dissipative interconversion between equivalence classes of states, where the classes are induced by fast controls.

This mission is the statement-level formalization of Reachability, Coolability, and Stabilizability of Open Markovian Quantum Systems with Fast Unitary Control (arXiv:2308.00561v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

61 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 4.7: Asymptotic cooling equals constant-Hamiltonian pure-state global attraction (Theorem 4.7: Asymptotic cooling equals constant-Hamiltonian pure-state global attraction, PDF p. 17). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Theorem 2.4: Equivalence Theorem: A consistent full statement of Theorem 2.4: Equivalence Theorem (source-ambiguity)
  • Proposition 2.6: Lie saturate of the full system: A consistent full statement of Proposition 2.6: Lie saturate of the full system (source-ambiguity)
  • Proposition 3.2: Strong stabilization and compensating Hamiltonian: A consistent full statement of Proposition 3.2: Strong stabilization and compensating Hamiltonian (source-ambiguity)
  • Proposition 3.5: Eight criteria for viability of a face: A consistent full statement of Proposition 3.5: Eight criteria for viability of a face (source-ambiguity)
  • Lemma 4.11: Rank-d global attraction and non-enclosing lazy subspaces: A consistent full statement of Lemma 4.11: Rank-d global attraction and non-enclosing lazy subspaces (source-ambiguity)
  • Corollary 4.13: Non-enclosing lazy subspace criterion for direct reachability: A consistent full statement of Corollary 4.13: Non-enclosing lazy subspace criterion for direct reachability (source-ambiguity)
  • Proposition 4.19: Direct versus indirect face reachability: A consistent full statement of Proposition 4.19: Direct versus indirect face reachability (source-ambiguity)
  • Lemma C.3: Freedom of CP-generator representation: A consistent full statement of Lemma C.3: Freedom of CP-generator representation (source-ambiguity)
  • Lemma C.19: Attractive support via Hamiltonian control: A consistent full statement of Lemma C.19: Attractive support via Hamiltonian control (source-ambiguity)
  • Unnumbered reduced/full Lie-saturate relations: A consistent full statement of Unnumbered reduced/full Lie-saturate relations (source-ambiguity)
  • Unnumbered uniqueness of the Hamiltonian part: A consistent full statement of Unnumbered uniqueness of the Hamiltonian part (source-ambiguity)

Selected references

  • Reachability, Coolability, and Stabilizability of Open Markovian Quantum Systems with Fast Unitary Control, arXiv:2308.00561v1, https://arxiv.org/abs/2308.00561v1
65 thms2 active usersReviewed
Quantum Information·Captain: Goku

Quantum Interference between a Single-Photon Fock State and a Coherent StateResearch Paper

Motivation

We derive analytical expressions for the single mode quantum field state at the individual output ports of a beam splitter when a single-photon Fock state and a coherent state are incident on the input ports. The output states turn out to be a statistical mixture between a displaced Fock state and a coherent state. Consequently we are able to find an analytical expression for the corresponding Wigner function. Because of the generality of our calculations the obtained results are valid for all passive and lossless optical four port devices. We show further how the results can be adapted to the case of the Mach-Zehnder interferometer. In addition we consider the case for which the single-photon Fock state is replaced with a general input state: a coherent input state displaces each general quantum state at the output port of a beam splitter with the displacement parameter being the amplitude of the coherent state.

This mission is the statement-level formalization of Quantum Interference between a Single-Photon Fock State and a Coherent State (arXiv:1009.1844v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

3 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is MZI composition and full reciprocity relations (§III/A, Eqs.(21)–(22), PDF p. 6). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Abstract and §II/A, Eqs.(5)–(10): A complete single-mode Weyl displacement on lp (fun _ : ℕ => ℂ) 2 and two-mode passive unitary, coherent input, and countable reduced-state constructions (hard)
  • §II/A, sentence after Eq.(7): A nondegeneracy restriction absent from the universal entanglement assertion (source-ambiguity)
  • §II/B, Eqs.(11)–(15): An independently defined position-kernel Wigner transform and its connection to countable Fock reduced states (hard)
  • §II/B, paragraph after Eq.(15): The actual output Wigner transform of the normalized balanced device (hard)
  • §II/C, Eqs.(16)–(18): A continuous passive two-mode Fock isometry and Weyl covariance on arbitrary normalized lp inputs (hard)
  • §II/C, highly reflective limit paragraph: A limiting reflection-phase convention absent from the claimed limit (source-ambiguity)
  • §III/B, Eqs.(23)–(25) and Wigner sentence: A complete single-mode Weyl displacement on lp (fun _ : ℕ => ℂ) 2 and two-mode passive unitary, coherent input, and countable reduced-state constructions and the independent Wigner transform (hard)
  • §III/B, last sentence: Full-lp MZI output and countable reduced-state displacement covariance (hard)
  • §III/C, Eqs.(27)–(30): Actual coherent/displaced-Fock component and marginal states with photon occupation moments (hard)
  • §III/C, Eq.(31): Actual coherent-MZI occupation distributions with first and second moments (hard)
  • §III/D, Eqs.(32)–(34): Coherent balanced-MZI output with finite photon-number moments (hard)
  • §III/D, Fig.4 and endpoint-purity paragraph; §IV: Actual coherent-input MZI reduced states, moments and purity at phase endpoints (hard)

Selected references

  • Quantum Interference between a Single-Photon Fock State and a Coherent State, arXiv:1009.1844v2, https://arxiv.org/abs/1009.1844v2
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Quantum Information·Captain: Goku

Attainability and lower semi-continuity of the relative entropy of entanglement, and variations on the themeResearch Paper

Motivation

The relative entropy of entanglement ERE_RER​ is defined as the distance of a multi-partite quantum state from the set of separable states as measured by the quantum relative entropy. We show that this optimisation is always achieved, i.e. any state admits a closest separable state, even in infinite dimensions; also, ERE_RER​ is everywhere lower semi-continuous. We use this to derive a dual variational expression for ERE_RER​ in terms of an external supremum instead of infimum. These results, which seem to have gone unnoticed so far, hold not only for the relative entropy of entanglement and its multi-partite generalisations, but also for many other similar resource quantifiers, such as the relative entropy of non-Gaussianity, of non-classicality, of Wigner negativity \unicode8212\unicode{8212}\unicode8212 more generally, all relative entropy distances from the sets of states with non-negative λ\lambdaλ-quasi-probability distribution. The crucial hypothesis underpinning all these applications is the weak*-closedness of the cone generated by free states, and for this reason the techniques we develop involve a bouquet of classical results from functional analysis. We complement our analysis by giving explicit and asymptotically tight continuity estimates for ERE_RER​ and closely related quantities in the presence of an energy constraint.

This mission is the statement-level formalization of Attainability and lower semi-continuity of the relative entropy of entanglement, and variations on the theme (arXiv:2105.08091v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

10 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 5 (seed): attainability, lower semicontinuity, compactness and uniqueness (Theorem 5 (seed): attainability, lower semicontinuity, compactness and uniqueness, PDF p. 7). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Theorem 9: dual variational formula for resource relative entropy: support-compressed exponential and log-partition (hard)
  • Lemma 11: Gibbs variational formula without faithfulness: log-partition at singular and zero positive trace-class operators (hard)
  • Lemma 13: duality for a weak*-compact convex subnormalised set: support-compressed log-partition and extended inner supremum (hard)
  • Remark 14: Petz dual formula without faithfulness: nonfaithful Petz log-partition functional (hard)
  • Corollary 20: bipartite relative entropy of entanglement: completed bipartite state space, closed-hull separability and log-partition (hard)
  • Corollary 22: weak*-closed cones for partition separability: partition-indexed completed tensor products and closed-hull pi-separability (hard)
  • Corollary 23: multipartite relative entropy of partition entanglement: multipartite pi-separable distance and log-partition (hard)
  • Lemma 24: weak*-closed PPT cone: partial transposition T(H_A tensor H_B) to B(H_A tensor H_B) (hard)
  • Corollary 25: relative entropy of NPT entanglement: PPT state space, extended distance and log-partition (hard)
  • Lemma 30: photon-number attenuation preserves lambda positivity: concrete Weyl representation, lambda-positive states and number attenuation (hard)
  • Corollary 31: weak*-closed lambda-positive cone: lambda-positive cone on the actual m-mode Hilbert space (hard)
  • Corollary 32: relative entropy of lambda negativity: lambda-positive distance and support-compressed dual formula (hard)
  • Lemma 33 (cited): quantum Darmois–Skitovich characterisation as printed: a corrected quantum Darmois-Skitovich statement and unitary beam splitter (source-ambiguity)
  • Lemma 34: weak*-closed cone of Gaussian states: all displaced m-mode Gaussian states as actual trace-class states (hard)
  • Corollary 35: attainability and lower semicontinuity of non-Gaussianity: Gaussian-state set, Gaussification and moment-defined entropy identity (hard)
  • Unnumbered consequence after Corollary 35: entropy of Gaussification: actual Gaussification on the finite-number-energy state set (hard)
  • Unnumbered result (124): finite-local-dimension continuity bounds: six bipartite entanglement measures and tensor-power regularizations (hard)
  • Proposition 36: bipartite energy continuity estimates (125),(127): all six resource measures, energy moduli and oscillator specialization (hard)
  • Proposition 36: generic-G asymptotic-tightness clause: a valid hypothesis set for generic-G asymptotic tightness (source-ambiguity)
  • Remark 37: faithfulness of the bipartite continuity modulus: the source-admissible G and actual generalized-inverse continuity modulus (hard)
  • Corollary 38: uniform and asymptotic continuity of six bipartite measures: six bipartite measures on correlated n-copy states and additive energy (hard)
  • Unnumbered multipartite entropy upper bounds (149),(150), proved in Appendix C: multipartite marginals and extended local entropy upper bounds (hard)
  • Unnumbered result (151): finite-dimensional multipartite continuity: partition separability, one unrestricted final factor and singleton-only regularization (hard)
  • Proposition 39: multipartite energy continuity estimates (155)–(157): multipartite energy budgets and the complete three continuity moduli (hard)
  • Proposition 39: asymptotic-tightness clause for m=2: partition-restricted large-energy tightness (source-ambiguity)
  • Remark 40: faithfulness of multipartite continuity moduli: the actual H[s] entropy capacity and multipartite moduli (hard)
  • Corollary 41: uniform and asymptotic multipartite continuity: grouped multipartite copies, additive local energies and partition measures (hard)
  • Lemma 43: infinite-dimensional Lieb three-operator inequality: support-compressed exponential of log A+log B-log C (hard)
  • Lemma 44: countably decomposable separable approximation to a pure state: actual countable pure-product mixture with all prescribed marginals (hard)

Selected references

  • Attainability and lower semi-continuity of the relative entropy of entanglement, and variations on the theme, arXiv:2105.08091v3, https://arxiv.org/abs/2105.08091v3
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Quantum Information·Captain: Goku

Comparison of Quantum Channels by SuperchannelsResearch Paper

Motivation

We extend the definition of the conditional min-entropy from bipartite quantum states to bipartite quantum channels. We show that many of the properties of the conditional min-entropy carry over to the extended version, including an operational interpretation as a guessing probability when one of the subsystems is classical. We then show that the extended conditional min-entropy can be used to fully characterize when two bipartite quantum channels are related to each other via a superchannel (also known as supermap or a comb) that is acting on one of the subsystems. This relation is a pre-order that extends the definition of "quantum majorization" from bipartite states to bipartite channels, and can also be characterized with semidefinite programming. As a special case, our characterization provides necessary and sufficient conditions for when a set of quantum channels is related to another set of channels via a single superchannel. We discuss the applications of our results to channel discrimination, and to resource theories of quantum processes. Along the way we study channel divergences, entropy functions of quantum channels, and noise models of superchannels, including random unitary superchannels, and doubly-stochastic superchannels. For the latter we give a physical meaning as being completely-uniformity preserving.

This mission is the statement-level formalization of Comparison of Quantum Channels by Superchannels (arXiv:1808.02607v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

21 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Quantum majorization of channels by all paired entropy tests (Theorem 7, continued p.19, PDF p. 18). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Selected references

  • Comparison of Quantum Channels by Superchannels, arXiv:1808.02607v3, https://arxiv.org/abs/1808.02607v3
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Algorithmic Game TheoryEconomicsOperations Research·Captain: mikedeng1

Two-Sided Platform Competition in a Sharing Economy: Which Wage Scheme Maximizes Platform Profit Is Decided by Demand- versus Supply-Side CompetitionResearch Paper

Motivation

Sharing-economy platforms (ride-sharing, car-sharing, peer-to-peer lending) sit between two groups. They charge consumers a price and pay self-scheduling workers a wage, and they compete with rival platforms on both sides at once. How a platform pays its workers is a design choice that varies across the industry: some announce a fixed wage per job, some a fixed commission rate on the consumer price, and some, as Uber did in its "upfront pricing" experiments, set prices and wages job by job. Drivers and regulators have argued over these schemes, and whether the choice matters for the platforms' own profits is a question in its own right.

Zhang, Chen and Raghunathan (SSRN 3555993, published in Management Science, 2022) answer it in a parsimonious duopoly model with linear demand and supply. Their main comparison, Proposition 3, shows that every scheme can be the most profitable one. Which one wins depends on whether consumers or workers switch more readily between the platforms. Many two-sided platform models, for example ones in which supply does not respond to the rival's wage, find no such reversal.

Setting

Two platforms i∈{1,2}i \in \{1,2\}i∈{1,2}, with iˉ=3−i\bar i = 3-iiˉ=3−i, charge consumer prices pip_ipi​ and pay wages wiw_iwi​ per transaction. Six parameters a,b,c,k,l,m>0a, b, c, k, l, m > 0a,b,c,k,l,m>0 define

di=a−b(pi−piˉ)−c pi,si=−k+l(wi−wiˉ)+m wi,d_i = a - b(p_i - p_{\bar i}) - c\,p_i, \qquad s_i = -k + l(w_i - w_{\bar i}) + m\,w_i,di​=a−b(pi​−piˉ​)−cpi​,si​=−k+l(wi​−wiˉ​)+mwi​,

the demand and the worker supply of platform iii. Here bbb measures how readily consumers switch platforms, ccc the price sensitivity of loyal consumers, lll how readily workers switch, and mmm the wage sensitivity of loyal workers. A transaction needs both a consumer and a worker, so the transaction volume is max⁡{0,min⁡{di,si}}\max\{0,\min\{d_i,s_i\}\}max{0,min{di​,si​}} and the profit is

πi=(pi−wi) max⁡{0,min⁡{di,si}}.\pi_i = (p_i - w_i)\,\max\{0,\min\{d_i, s_i\}\}.πi​=(pi​−wi​)max{0,min{di​,si​}}.

The standing assumptions are Assumption 1, a/c>k/ma/c > k/ma/c>k/m, and Assumption 2, l≤2c+c2/bl \le 2c + c^2/bl≤2c+c2/b.

Three wage schemes define three games:

  1. DCR (dynamic commission rate). The platforms simultaneously choose a price pip_ipi​ and a commission rate αi\alpha_iαi​. The wage is wi=(1−αi)piw_i = (1-\alpha_i)p_iwi​=(1−αi​)pi​, so profit is αipimax⁡{0,min⁡{di,si}}\alpha_i p_i \max\{0,\min\{d_i,s_i\}\}αi​pi​max{0,min{di​,si​}}.
  2. FCR (fixed commission rate). The platforms first announce commission rates αi\alpha_iαi​, then, having observed both, set prices.
  3. FW (fixed wage). The platforms first announce wages wiw_iwi​, then set prices.

DCR is solved by Nash equilibrium. FCR and FW are solved by subgame-perfect equilibrium: a stage-2 price rule must give a Nash equilibrium of the pricing game after every pair of stage-1 announcements, and no stage-1 announcement may be improved on. The paper studies symmetric equilibria with positive demand and supply. Write πD∗,πF∗,πW∗\pi^{D*}, \pi^{F*}, \pi^{W*}πD∗,πF∗,πW∗ for the resulting platform profits.

Formalization targets

Goal: Proposition 3

Write αD∗\alpha^{D*}αD∗ for the DCR equilibrium commission rate and

Q=b+c+l+m(b+c)(l+m)αD∗−b+(1−αD∗)l(1−αD∗)(cl−bm)Q = \frac{b+c+l+m}{(b+c)(l+m)\alpha^{D*}} - \frac{b + (1-\alpha^{D*})l}{(1-\alpha^{D*})(cl-bm)}Q=(b+c)(l+m)αD∗b+c+l+m​−(1−αD∗)(cl−bm)b+(1−αD∗)l​

for the left side of the paper's Inequality (13). For every symmetric equilibrium of each game with positive demand and supply:

(a)  bc>lm⟹ πW∗>πF∗>πD∗,(b)  bc<lm, Q>0⟹ πF∗>πD∗>πW∗,(c)  bc<lm, Q<0⟹ πD∗>πF∗>πW∗.\begin{aligned} &\text{(a)}\ \ \tfrac{b}{c} > \tfrac{l}{m} &&\Longrightarrow\ \pi^{W*} > \pi^{F*} > \pi^{D*},\\ &\text{(b)}\ \ \tfrac{b}{c} < \tfrac{l}{m},\ Q > 0 &&\Longrightarrow\ \pi^{F*} > \pi^{D*} > \pi^{W*},\\ &\text{(c)}\ \ \tfrac{b}{c} < \tfrac{l}{m},\ Q < 0 &&\Longrightarrow\ \pi^{D*} > \pi^{F*} > \pi^{W*}. \end{aligned}​(a)  cb​>ml​(b)  cb​<ml​, Q>0(c)  cb​<ml​, Q<0​​⟹ πW∗>πF∗>πD∗,⟹ πF∗>πD∗>πW∗,⟹ πD∗>πF∗>πW∗.​

The goal is stated about the equilibria of the three games, not about the closed-form prices.

Milestones

  • Lemma 1 (p. 10): the DCR game has exactly one symmetric equilibrium with positive demand and supply, given by the closed forms (4) and (5), and 0<αD∗<10 < \alpha^{D*} < 10<αD∗<1.
  • Lemma 2 (p. 11): the FCR equilibrium commission rate is the unique zero in (αˉ,1)(\bar\alpha, 1)(αˉ,1) of the quadratic fff of (44), equivalently the solution of (6). The price is (a+k)/(c+m(1−α∗))(a+k)/(c + m(1-\alpha^*))(a+k)/(c+m(1−α∗)), (7).
  • Lemma 3 (p. 12): the FW equilibrium wage and price are (8) and (9).
  • Profit increases in price (A.8, p. 52): with demand equal to supply, profit is a concave quadratic in the equilibrium price. All three equilibrium prices lie on its increasing branch.
  • Three price comparisons (A.8, pp. 52–53):
    • pW∗−pD∗p^{W*} - p^{D*}pW∗−pD∗ has the sign of bm−clbm - clbm−cl;
    • αD∗<αF∗\alpha^{D*} < \alpha^{F*}αD∗<αF∗ if and only if (13) holds;
    • αW∗<αF∗\alpha^{W*} < \alpha^{F*}αW∗<αF∗ if and only if cl>bmcl > bmcl>bm.

Significance

Proposition 3 makes the choice of wage scheme a substantive strategic variable. The fixed-wage scheme is either the best or the worst for the platforms, and the fixed-commission scheme is never the worst. The ranking of profits equals the ranking of equilibrium prices and reverses that of wages. The paper's welfare results (Propositions 4 and 5) build on it, since consumer and worker surplus orderings are read off the same price ranking.

Formalizing it adds three things:

  • A checked equilibrium analysis. The appendix's equilibrium analysis is partly written out and partly asserted ("we can verify that neither platform has incentive to deviate").
  • Corrected statements. The printed comparisons contain slips; see Formalization scope.
  • A model for later work. The definitions give a reusable formal model of two-stage price competition with endogenous two-sided supply.

The result is proved in the paper; nothing in it has been machine-checked.

Difficulty

The comparison itself, once the equilibria are known, is rational-function algebra. The difficulty is the equilibrium characterizations.

  • The payoff is kinked. Profit is a product of a margin and a minimum of demand and supply, so each best response must be analysed region by region: supply exceeding demand, matching it, or falling short.
  • FCR and FW need the whole subgame. Their stage-2 pricing games must be solved after every pair of announcements, including off-path pairs in which a rival's supply is non-positive.
  • Local optimality is not enough. The obvious argument, setting the derivative of the stage-1 profit to zero along the matched-supply branch, gives only a necessary condition. Existence needs global deviations ruled out, in particular a platform raising its wage enough that its own supply exceeds demand. That is exactly where Assumption 2 enters.

Formalization scope

  • Parameters. All six parameters are reals and strictly positive (R+\mathbb R^+R+ read as >0>0>0). Assumptions 1 and 2 are bundled in Params.Standing.
  • Strategies.
    • Actions range over all of R\mathbb RR: prices, commission rates and wages alike. No bound such as 0≤α≤10 \le \alpha \le 10≤α≤1 is imposed.
    • DCR actions are pairs (price, commission rate).
    • A two-stage profile is a pair of stage-1 actions together with stage-2 price rules Pi:R2→RP_i : \mathbb R^2 \to \mathbb RPi​:R2→R. "Symmetric" means equal stage-1 actions and equal on-path prices; off-path play is unrestricted.
  • Truncated volume. The paper writes the volume as min⁡{di,si}\min\{d_i,s_i\}min{di​,si​}. With negative values allowed, the profit is unbounded above and no equilibrium exists, so the formalization uses max⁡{0,min⁡{di,si}}\max\{0,\min\{d_i,s_i\}\}max{0,min{di​,si​}}.
  • Non-trivial equilibria. Equilibria are required to have positive demand and supply on the path (p. 9). Zero-volume symmetric equilibria exist and are excluded.
  • Continuity on the path. Two-stage equilibria are required to have stage-2 price rules continuous at the equilibrium stage-1 pair. The appendix presupposes this when it differentiates the subgame prices in the stage-1 actions. It is necessary: without it, zero-profit equilibria of nearby pricing subgames can punish every deviation, and other FCR commission rates become subgame-perfect outcomes.
  • Corrections to the printed statements.
    • Case (c). It is stated with "Q<0Q < 0Q<0" where the paper says "(13) does not hold". At Q=0Q = 0Q=0 the DCR and FCR outcomes coincide and the strict ranking fails.
    • αW∗\alpha^{W*}αW∗. It is defined as 1−wW∗/pW∗1 - w^{W*}/p^{W*}1−wW∗/pW∗, because the appendix's displayed closed form has the sign of kkk reversed.
    • Denominators. Real divisions occur in (6) and (13), and their denominators are carried or proved nonzero.

A formalization that compares only the closed-form prices, or uses the literal untruncated payoff (which makes every statement about equilibria vacuous), is not this mission.

  • Contributions welcome:
    • best-response lemmas for the kinked profit;
    • existence of pricing equilibria in every subgame;
    • the global no-deviation arguments behind Lemmas 2 and 3;
    • the algebra of the price comparisons.

Selected references

  • C. Zhang, J. Chen, S. Raghunathan, Two-Sided Platform Competition in a Sharing Economy, SSRN working paper 3555993; published in Management Science, 2022. https://ssrn.com/abstract=3555993, https://doi.org/10.1287/mnsc.2022.4302
  • D. M. Kreps, J. A. Scheinkman, Quantity Precommitment and Bertrand Competition Yield Cournot Outcomes, Bell Journal of Economics 14(2), 1983. https://doi.org/10.2307/3003636
  • S. C. Choi, Price Competition in a Channel Structure with a Common Retailer, Marketing Science 10(4), 271–296, 1991, the source the paper cites for its linear demand model (p. 7). https://doi.org/10.1287/mksc.10.4.271
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Graph TheoryQuantum Error CorrectionQuantum Information·Captain: mikedeng1

Decoding Quantum Tanner Codes: The Parallel Decoder Corrects Every Error of Weight Linear in the Code Length in Logarithmically Many RoundsResearch Paper

Why decoding good quantum LDPC codes matters

Quantum computers must correct errors faster than they accumulate, and quantum low-density parity-check (LDPC) codes are the leading candidates for doing so with little overhead: every check involves a bounded number of qubits, so syndromes can be measured by local circuits. In 2021–2022 the first asymptotically good quantum LDPC codes appeared, with dimension and minimum distance both linear in the code length nnn: the expander lifted product codes of Panteleev and Kalachev (arXiv:2111.03654) and the quantum Tanner codes of Leverrier and Zémor (arXiv:2202.13641). A code is only useful if errors can be corrected efficiently. Leverrier and Zémor (arXiv:2208.05537) give two decoders for quantum Tanner codes that correct every error of weight up to a constant fraction of nnn: a sequential one running in linear time, and a parallel decoder running in a logarithmic number of rounds of local updates. This mission is about the parallel decoder.

Timeline:

  • 2021, Panteleev–Kalachev: asymptotically good quantum LDPC codes and locally testable classical codes (arXiv:2111.03654).
  • 2022, Leverrier–Zémor: quantum Tanner codes, a simpler construction on left-right Cayley complexes (arXiv:2202.13641).
  • 2022, Gu–Pattison–Tang, Leverrier–Zémor and Dinur–Hsieh–Lin–Vidick: efficient decoders for linear-distance quantum LDPC codes (arXiv:2206.06557, arXiv:2206.07571, arXiv:2206.07750).
  • 2022, Leverrier–Zémor, Decoding quantum Tanner codes: sequential and parallel decoders up to a constant fraction of nnn, with a revised parallel analysis in v3 (arXiv:2208.05537v3).

The code and the decoder

Let GGG be a finite group and A=A−1A=A^{-1}A=A−1, B=B−1⊆GB=B^{-1}\subseteq GB=B−1⊆G with ∣A∣=∣B∣=Δ|A|=|B|=\Delta∣A∣=∣B∣=Δ. The quadripartite left-right Cayley complex has four copies of GGG as vertices, Vij=G×{ij}V_{ij}=G\times\{ij\}Vij​=G×{ij}, and one square {(g,00),(ag,01),(gb,10),(agb,11)}\{(g,00),(ag,01),(gb,10),(agb,11)\}{(g,00),(ag,01),(gb,10),(agb,11)} for every (g,a,b)∈G×A×B(g,a,b)\in G\times A\times B(g,a,b)∈G×A×B. The set of squares QQQ has n=∣G∣Δ2n=|G|\Delta^2n=∣G∣Δ2 elements, and every vertex vvv sees its QQQ-neighbourhood Q(v)Q(v)Q(v) as an A×BA\times BA×B array: columns are indexed by bbb, rows by aaa. The left Cayley graph Cay(G,A)\mathrm{Cay}(G,A)Cay(G,A) and the right Cayley graph Cay(G,B)\mathrm{Cay}(G,B)Cay(G,B) are assumed to be non-bipartite Ramanujan graphs: every adjacency eigenvalue other than ±Δ\pm\Delta±Δ has absolute value at most 2Δ−12\sqrt{\Delta-1}2Δ−1​.

Two local codes CA⊆F2AC_A\subseteq\mathbb F_2^ACA​⊆F2A​, CB⊆F2BC_B\subseteq\mathbb F_2^BCB​⊆F2B​ with dim⁡CA+dim⁡CB=Δ\dim C_A+\dim C_B=\DeltadimCA​+dimCB​=Δ are fixed. Write V0=V00∪V11V_0=V_{00}\cup V_{11}V0​=V00​∪V11​ and V1=V01∪V10V_1=V_{01}\cup V_{10}V1​=V01​∪V10​. The code C1⊆F2Q\mathcal C_1\subseteq\mathbb F_2^QC1​⊆F2Q​ consists of the vectors whose view on every Q(v)Q(v)Q(v), v∈V1v\in V_1v∈V1​, lies in the dual tensor code CA⊗F2B+F2A⊗CBC_A\otimes\mathbb F_2^B+\mathbb F_2^A\otimes C_BCA​⊗F2B​+F2A​⊗CB​: every local view is a sum of a word whose columns are in CAC_ACA​ and a word whose rows are in CBC_BCB​. C0\mathcal C_0C0​ is defined in the same way on V0V_0V0​ with CA⊥C_A^\perpCA⊥​, CB⊥C_B^\perpCB⊥​. The local codes and their duals have distance at least δΔ\delta\DeltaδΔ. Both dual tensor codes are κ\kappaκ-product-expanding: every codeword xxx splits as x=c+rx=c+rx=c+r with ∣x∣≥κΔ(∥c∥+∥r∥)|x|\ge\kappa\Delta(\|c\|+\|r\|)∣x∣≥κΔ(∥c∥+∥r∥), where ∥c∥\|c\|∥c∥ counts non-zero columns and ∥r∥\|r\|∥r∥ non-zero rows.

A σx\sigma_xσx​-type error e∈F2Qe\in\mathbb F_2^Qe∈F2Q​ is decoded in three phases. In the preprocessing phase every v∈V1v\in V_1v∈V1​ chooses a minimum-weight local error εv\varepsilon_vεv​ with the local syndrome of eee; the mismatch is Z=∑v∈V1εvZ=\sum_{v\in V_1}\varepsilon_vZ=∑v∈V1​​εv​. The mismatch decomposition writes Z=C^0+R^0+C^1+R^1Z=\hat C_0+\hat R_0+\hat C_1+\hat R_1Z=C^0​+R^0​+C^1​+R^1​, with C^j\hat C_jC^j​ a sum of CAC_ACA​-columns and R^i\hat R_iR^i​ a sum of CBC_BCB​-rows. Postprocessing outputs e^=∑v∈V10εv+C^0+R^1\hat e=\sum_{v\in V_{10}}\varepsilon_v+\hat C_0+\hat R_1e^=∑v∈V10​​εv​+C^0​+R^1​. The parallel decoder (Algorithm 3) runs rounds of four substeps, one for each of V00,V01,V10,V11V_{00},V_{01},V_{10},V_{11}V00​,V01​,V10​,V11​. In a substep, every vertex vvv of the current class simultaneously looks for a non-zero local dual tensor codeword xvx_vxv​ on Q(v)Q(v)Q(v) with ∣Z^∣−∣Z^+xv∣≥∣xv∣/2|\hat Z|-|\hat Z+x_v|\ge|x_v|/2∣Z^∣−∣Z^+xv​∣≥∣xv​∣/2, picks one of maximum weight, splits it as cv+rvc_v+r_vcv​+rv​ with ∥cv∥+∥rv∥\|c_v\|+\|r_v\|∥cv​∥+∥rv​∥ minimal, and updates C^j\hat C_jC^j​, R^i\hat R_iR^i​ and Z^\hat ZZ^.

Formalization targets

Goal: Theorem 20 (= Theorem 3)

Fix ε∈(0,1/6)\varepsilon\in(0,1/6)ε∈(0,1/6) and δ,κ>0\delta,\kappa>0δ,κ>0. For all Δ\DeltaΔ large enough, every error with

∣e∣<1212min⁡(ε316,κ4)δ2κ2nΔ|e|<\frac1{2^{12}}\min\Big(\frac{\varepsilon^3}{16},\frac\kappa4\Big)\delta^2\kappa^2\frac n\Delta∣e∣<2121​min(16ε3​,4κ​)δ2κ2Δn​

is corrected by every run of the parallel decoder. With θ=14(14−32ε)\theta=\frac14\big(\frac14-\frac32\varepsilon\big)θ=41​(41​−23​ε), each round satisfies ∣Z^k+1∣≤(1−θ)∣Z^k∣|\hat Z_{k+1}|\le(1-\theta)|\hat Z_k|∣Z^k+1​∣≤(1−θ)∣Z^k​∣, so Z^k=0\hat Z_k=0Z^k​=0 once (1−θ)k⋅4∣e∣<1(1-\theta)^k\cdot4|e|<1(1−θ)k⋅4∣e∣<1, and then e+e^e+\hat ee+e^ lies in the span C0⊥\mathcal C_0^\perpC0⊥​ of the σx\sigma_xσx​-generators.

Milestones

  • Lemma 4 (expander mixing) and Lemma 5: λ(G0□),λ(G1□)≤4Δ\lambda(\mathcal G^\square_0),\lambda(\mathcal G^\square_1)\le4\Deltaλ(G0□​),λ(G1□​)≤4Δ.
  • Lemmas 7, 10, 11, 8 and Theorem 9: the minimum distance, dmin⁡≥δ2κ2n/(1024Δ)d_{\min}\ge\delta^2\kappa^2n/(1024\Delta)dmin​≥δ2κ2n/(1024Δ).
  • Lemmas 14, 15, 16 and Theorem 12: if a minimum decomposition of a non-zero mismatch has few active vertices, some local codeword lowers ∣Z∣|Z|∣Z∣ by (1−ε)∣xv∣(1-\varepsilon)|x_v|(1−ε)∣xv​∣.
  • Lemma 17: ∣Z∣≤4∣e∣|Z|\le4|e|∣Z∣≤4∣e∣ and ∥Z∥≤4∣e∣/(κΔ)\|Z\|\le4|e|/(\kappa\Delta)∥Z∥≤4∣e∣/(κΔ).
  • Lemma 19: below 2−16ε3κ2δ2n/Δ2^{-16}\varepsilon^3\kappa^2\delta^2n/\Delta2−16ε3κ2δ2n/Δ, sequential decoding with parameter 1/21/21/2 never stalls, and switching to ε\varepsilonε still converges.
  • Lemma 18: if the ε\varepsilonε-sequential decoder converges, one parallel round removes at least θ∣Z∣\theta|Z|θ∣Z∣.

Significance

The theorem shows that asymptotically good quantum LDPC codes can be decoded against adversarial errors of linear weight by O(log⁡n)O(\log n)O(logn) rounds of local computation, each vertex acting only on its own QQQ-neighbourhood. This matters for fault tolerance, where decoding latency is a bottleneck. The milestones carry independent value. Theorem 9 is a linear minimum distance bound for quantum Tanner codes in the quadripartite setting. Theorem 12 is the local-to-global "weight reduction" principle on which both decoders rest. Lemmas 4–5 are spectral facts about Cayley graphs and square complexes that are reusable for any expander-based code.

The paper's results are proved, not open; none has been machine-checked. The sequential decoder's correctness (Theorem 13) is posed separately on the platform as an open goal in the mission Decoding quantum Tanner codes (Leverrier, Zemor), which shares this mission's published definitions; this mission does not restate it. Formalizing the present chain would give a complete, checked proof that a parallel decoder exists for good quantum LDPC codes, and would expose the constants. Two printed constants are corrected here (see the scope section), and sharper constants or simpler arguments are welcome.

Difficulty

The obvious argument is to bound the mismatch and its norm, apply Theorem 12 repeatedly, and let all vertices of a class flip at once. That argument fails because parallel flips are not sequential flips. A vertex's best local move against the mismatch at its turn need not be the move a converging sequential run would make, and a round could stall even though a sequential run never does. Lemma 18 resolves this with a virtual sequential run, a partition of its increments into "good" and "bad" ones (Claim 1), and the maximum-weight rule at every vertex. Without that rule the lemma is false. Theorem 12 itself is a counting contradiction. It uses robustness, the expander mixing lemma twice, and two notions of "exceptional" vertices, and it needs Δ\DeltaΔ large. Theorem 9 needs the coset-minimization of Lemma 7 before the same counting can start.

Formalization scope

The development builds on the published layers QAlgorithms_Defs_TensorCode and QAlgorithms_Defs_TannerDecoder. These define the complex, φv\varphi_vφv​, C0\mathcal C_0C0​, C1\mathcal C_1C1​, the σx\sigma_xσx​ span, minimum local corrections, the mismatch, Algorithm 2 and the output e^\hat ee^. The conventions are:

  • A vertex (g,ij)(g,ij)(g,ij) is (g, (i, j)) : G × (Bool × Bool), squares are G × A × B, and weights are hammingNorm cast to ℝ.
  • One new definitions file holds Algorithm 3 (admissible move, parallel choice, substep, round, run), decompositions and their norm, active, exceptional and ordinary vertices, the clustering sets TTT, stalled and converging sequential decoders, C1⊥\mathcal C_1^\perpC1⊥​, and the square graphs Gk□\mathcal G^\square_kGk□​.
  • "Δ\DeltaΔ large enough" is ∃Δ0 ∀Δ≥Δ0\exists\Delta_0\,\forall\Delta\ge\Delta_0∃Δ0​∀Δ≥Δ0​, with Δ0\Delta_0Δ0​ depending only on the constants fixed before it.
  • Only σx\sigma_xσx​-type errors are treated; the σz\sigma_zσz​ case is symmetric.
  • Non-bipartiteness of the Cayley graphs (the standing choice of p. 10) is assumed wherever spectral bounds are used.
  • Theorem 12 assumes Z≠0Z\ne0Z=0 and asks for a non-zero xvx_vxv​.

Corrected constants. Theorem 9 is stated with 102410241024 instead of the printed 256256256, because Lemma 8 and the proof's ∣x∣≥κΔ2∥x∥|x|\ge\frac{\kappa\Delta}2\|x\|∣x∣≥2κΔ​∥x∥ give 102410241024. The goal's error bound uses min⁡(ε3/16,κ/4)\min(\varepsilon^3/16,\kappa/4)min(ε3/16,κ/4) instead of min⁡(ε3/16,κ)\min(\varepsilon^3/16,\kappa)min(ε3/16,κ), which is what the corrected distance supports. Both corrected statements are weaker than the printed ones.

No trivialization. Every vertex must flip a maximum-weight admissible move whenever one exists, and runs range over all such choices. "Logarithmic time" is the per-round contraction factor, not mere eventual termination. Validity is membership of e+e^e+\hat ee+e^ in the σx\sigma_xσx​-generator span, with e^\hat ee^ the paper's postprocessing output. A formalization that lets vertices idle, drops the maximum-weight rule, or proves only eventual termination does not prove this theorem.

Needed and reusable infrastructure:

  • spectral graph theory for regular multigraphs (expander mixing, eigenvalues of commuting Cayley adjacencies);
  • product expansion and local minimality of decompositions;
  • the combinatorics of the left-right complex (shared rows and columns).

Contributions proving the graph lemmas or Lemma 18, whose proof is pure counting, are especially welcome.

Selected references

  • A. Leverrier, G. Zémor, Decoding quantum Tanner codes, IEEE Transactions on Information Theory; arXiv:2208.05537v3, 2022. https://arxiv.org/abs/2208.05537
  • A. Leverrier, G. Zémor, Quantum Tanner codes, FOCS 2022; arXiv:2202.13641. https://arxiv.org/abs/2202.13641
  • P. Panteleev, G. Kalachev, Asymptotically good quantum and locally testable classical LDPC codes, STOC 2022; arXiv:2111.03654. https://arxiv.org/abs/2111.03654
  • S. Gu, C. A. Pattison, E. Tang, An efficient decoder for a linear distance quantum LDPC code, STOC 2023; arXiv:2206.06557. https://arxiv.org/abs/2206.06557
  • A. Leverrier, G. Zémor, Efficient decoding up to a constant fraction of the code length for asymptotically good quantum codes, SODA 2023; arXiv:2206.07571. https://arxiv.org/abs/2206.07571
  • I. Dinur, M.-H. Hsieh, T.-C. Lin, T. Vidick, Good quantum LDPC codes with linear time decoders, arXiv:2206.07750, 2022. https://arxiv.org/abs/2206.07750
  • G. Kalachev, P. Panteleev, Two-sided robustly testable codes, arXiv:2206.09973, 2022. https://arxiv.org/abs/2206.09973
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Information TheoryQuantum Information·Captain: mikedeng1

Quantum Uncertainty Relation Using Coherence: For Every Qubit State, the Relative Entropies of Coherence in Two Measurement Bases Sum to at Least a Bound Set by Purity and Maximal OverlapResearch Paper

Motivation

An uncertainty relation bounds how sharply two incompatible measurements can both be predicted on one quantum state. The entropic form of Maassen and Uffink (1988), H(X)+H(Z)≥−log⁡2cmax⁡H(X) + H(Z) \ge -\log_2 c_{\max}H(X)+H(Z)≥−log2​cmax​, measures unpredictability by the Shannon entropies of the outcomes of two measurement bases X\mathbb XX and Z\mathbb ZZ, and incompatibility by their maximal overlap cmax⁡c_{\max}cmax​. It underlies security proofs in quantum key distribution and entanglement witnesses, and it has been sharpened repeatedly, for example by Berta et al. (2010) with quantum memory.

The resource theory of quantum coherence (Baumgratz, Cramer and Plenio, 2014) quantifies how far a state is from being diagonal in a fixed basis. Coherence is basis dependent, so a state cannot be incoherent in two incompatible bases at once. Yuan, Bai, Peng and Ma (arXiv:1612.02573v2, 2017) turn this into quantitative quantum uncertainty relations: lower bounds on the sum of the coherences of one state in two bases. For the relative entropy of coherence on a qubit, their Theorem 2 gives a bound depending on the purity of the state and the overlap of the bases, which they show numerically to improve on bounds obtained from the Maassen–Uffink and Sánchez-Ruiz relations.

Setting

A qubit state is a 2×22\times 22×2 complex positive semidefinite matrix ρ\rhoρ with Tr⁡ρ=1\operatorname{Tr}\rho = 1Trρ=1. A measurement basis X={∣x0⟩,∣x1⟩}\mathbb X = \{|x_0\rangle, |x_1\rangle\}X={∣x0​⟩,∣x1​⟩} is an orthonormal basis of C2\mathbb C^2C2, recorded as the unitary matrix UUU whose columns are ∣x0⟩,∣x1⟩|x_0\rangle, |x_1\rangle∣x0​⟩,∣x1​⟩. Measuring ρ\rhoρ in X\mathbb XX gives outcome iii with probability pi=⟨xi∣ρ∣xi⟩p_i = \langle x_i|\rho|x_i\ranglepi​=⟨xi​∣ρ∣xi​⟩; the outcome entropy is H(X)=−∑ipilog⁡2piH(X) = -\sum_i p_i\log_2 p_iH(X)=−∑i​pi​log2​pi​.

The dephased state ρdiag=∑i⟨xi∣ρ∣xi⟩ ∣xi⟩⟨xi∣\rho_{\mathrm{diag}} = \sum_i \langle x_i|\rho|x_i\rangle\,|x_i\rangle\langle x_i|ρdiag​=∑i​⟨xi​∣ρ∣xi​⟩∣xi​⟩⟨xi​∣ is ρ\rhoρ with its off-diagonal part (in X\mathbb XX) removed. The relative entropy of coherence is

CREX(ρ)=H(ρdiag)−H(ρ),C^{\mathbb X}_{\mathrm{RE}}(\rho) = H(\rho_{\mathrm{diag}}) - H(\rho),CREX​(ρ)=H(ρdiag​)−H(ρ),

where H(ρ)=−∑λλlog⁡2λH(\rho) = -\sum_\lambda \lambda\log_2\lambdaH(ρ)=−∑λ​λlog2​λ (over the eigenvalues of ρ\rhoρ) is the von Neumann entropy. All logarithms are base 222, and 0log⁡0=00\log 0 = 00log0=0.

The purity of ρ\rhoρ is P=Tr⁡[ρ2]∈[1/2,1]P = \operatorname{Tr}[\rho^2] \in [1/2, 1]P=Tr[ρ2]∈[1/2,1], equal to 111 exactly for pure states. For two bases X\mathbb XX and Z\mathbb ZZ, the maximal overlap is c=cmax⁡(X,Z)=max⁡∣x⟩∈X, ∣z⟩∈Z∣⟨x∣z⟩∣2c = c_{\max}(\mathbb X, \mathbb Z) = \max_{|x\rangle\in\mathbb X,\,|z\rangle\in\mathbb Z}|\langle x|z\rangle|^2c=cmax​(X,Z)=max∣x⟩∈X,∣z⟩∈Z​∣⟨x∣z⟩∣2, and cmin⁡c_{\min}cmin​ is the corresponding minimum. On a scalar t∈[0,1]t\in[0,1]t∈[0,1], H(t)=−tlog⁡2t−(1−t)log⁡2(1−t)H(t) = -t\log_2 t - (1-t)\log_2(1-t)H(t)=−tlog2​t−(1−t)log2​(1−t) is the binary entropy. In the proof the authors use f(x)=H(xp+(1−x)(1−p))f(x) = H(xp + (1-x)(1-p))f(x)=H(xp+(1−x)(1−p)), where ppp is an eigenvalue of ρ\rhoρ.

Formalization targets

Goal: Theorem 2 (p. 8, Eq. (14))

For every qubit state ρ\rhoρ and every pair of measurement bases X,Z\mathbb X, \mathbb ZX,Z of C2\mathbb C^2C2,

CREX(ρ)+CREZ(ρ) ≥ H ⁣(2P−1 (2c−1)+12)−H(ρ).C^{\mathbb X}_{\mathrm{RE}}(\rho) + C^{\mathbb Z}_{\mathrm{RE}}(\rho) \ \ge\ H\!\left(\frac{\sqrt{2P-1}\,(2\sqrt c - 1) + 1}{2}\right) - H(\rho).CREX​(ρ)+CREZ​(ρ) ≥ H(22P−1​(2c​−1)+1​)−H(ρ).

Milestones

In the paper's order:

  1. CREX(ρ)=H(X)−H(ρ)C^{\mathbb X}_{\mathrm{RE}}(\rho) = H(X) - H(\rho)CREX​(ρ)=H(X)−H(ρ) (p. 8), the step from (14) to the conventional form (15).
  2. The spectral form (16): with ρ=p∣r⟩⟨r∣+(1−p)∣r⊥⟩⟨r⊥∣\rho = p|r\rangle\langle r| + (1-p)|r_\perp\rangle\langle r_\perp|ρ=p∣r⟩⟨r∣+(1−p)∣r⊥​⟩⟨r⊥​∣ and a=∣⟨r∣x⟩∣2a = |\langle r|x\rangle|^2a=∣⟨r∣x⟩∣2, H(X)=H(ap+(1−a)(1−p))H(X) = H(ap + (1-a)(1-p))H(X)=H(ap+(1−a)(1−p)). Also P=2p2−2p+1P = 2p^2 - 2p + 1P=2p2−2p+1 and H(ρ)=H(p)H(\rho) = H(p)H(ρ)=H(p).
  3. Lemma 1, Eq. (17): for unit vectors in Cd\mathbb C^dCd, a+b≤1+ca + b \le 1 + \sqrt ca+b≤1+c​ and ∣a−b∣≤1−c|a-b| \le \sqrt{1-c}∣a−b∣≤1−c​.
  4. Lemma 1, Eq. (18): in C2\mathbb C^2C2, 1−c≤a+b1 - \sqrt c \le a + b1−c​≤a+b.
  5. Eq. (22): fff is concave on [0,1][0,1][0,1] and f(x)=f(1−x)f(x) = f(1-x)f(x)=f(1−x).
  6. For qubit bases, c=1−cmin⁡c = 1 - c_{\min}c=1−cmin​ and c≥1/2c \ge 1/2c≥1/2 (pp. 8, 11).
  7. Eq. (25): ∣c−12∣≥∣1−c−12∣|\sqrt c - \tfrac12| \ge |\sqrt{1-c} - \tfrac12|∣c​−21​∣≥∣1−c​−21​∣ for c≥1/2c \ge 1/2c≥1/2, hence f(c)≤f(1−c)f(\sqrt c) \le f(\sqrt{1-c})f(c​)≤f(1−c​).
  8. The minimum of g=f(a)+f(b)g = f(a) + f(b)g=f(a)+f(b) over the region cut out by Lemma 1 is f(0)+f(c)f(0) + f(\sqrt c)f(0)+f(c​) (pp. 11–12).

Significance

The result. Theorem 2 is a state-dependent uncertainty relation for coherence. Through milestone 1 it is equivalent to the entropic relation H(X)+H(Z)≥H((2P−1(2c−1)+1)/2)+H(ρ)H(X) + H(Z) \ge H\big((\sqrt{2P-1}(2\sqrt c-1)+1)/2\big) + H(\rho)H(X)+H(Z)≥H((2P−1​(2c​−1)+1)/2)+H(ρ) (Eq. (15)), which involves the state only through its purity and entropy. The bound is attained by the maximally mixed state. It reduces to a pure-state relation when P=1P = 1P=1, and it is compared numerically with earlier entropic bounds in §IV of the paper. Lemma 1 is a self-contained inequality on three unit vectors in Cd\mathbb C^dCd that can be reused in other overlap arguments.

Formalizing it. The theorem has a pen-and-paper proof in the paper; no machine-checked version of it or of any entropic uncertainty relation is known on Prove2Me or in Mathlib. The mission yields a checked proof together with a reusable qubit layer: dephasing in an arbitrary basis, the relative entropy of coherence in bits, outcome entropies, purity and basis overlaps, built on the published von Neumann entropy and binary entropy definitions. The proof in the paper also contains a printed slip on p. 11, where f(c)f(\sqrt c)f(c​) is written as H(pc+(1−p)c)H(p\sqrt c + (1-p)\sqrt c)H(pc​+(1−p)c​); a formal proof settles the correct expression.

Difficulty

There are three separate obstacles.

  • Matrices and entropies. The relative entropy of coherence is defined through eigenvalues of the dephased matrix. Relating it to outcome probabilities means identifying the spectrum of Udiag⁡(p0,p1)U†U\operatorname{diag}(p_0,p_1)U^\daggerUdiag(p0​,p1​)U† through Mathlib's IsHermitian.eigenvalues, which are given only up to an unspecified ordering.
  • Lemma 1. The lemma is a statement about three unit vectors in arbitrary dimension, with a separate lower bound (18) that holds only in dimension 2. It fails in C3\mathbb C^3C3: three orthonormal vectors give a=b=c=0a = b = c = 0a=b=c=0.
  • Non-convex minimization. The final minimization is of a concave function over a polygon. A concave function attains its minimum at extreme points, so local or first-order arguments do not apply; the extreme points of the region must be identified and compared, which is the role of Eq. (25) and c≥1/2c \ge 1/2c≥1/2.

Formalization scope

  • States, bases and entropies. States are Matrix (Fin 2) (Fin 2) ℂ with PosSemidef and trace 111. Bases are elements of Matrix.unitaryGroup (Fin 2) ℂ, whose columns are the basis vectors; this covers every orthonormal basis of C2\mathbb C^2C2, and global phases of the columns change no quantity. Entropies are in bits through Real.logb 2, with 0log⁡0=00\log 0 = 00log0=0. The von Neumann entropy is the published ShadowTomography.QuantumLB.vnEntropy and the binary entropy is the published WildeQIT.binaryEntropy.
  • Coherence and overlaps. CREXC^{\mathbb X}_{\mathrm{RE}}CREX​ is defined from the dephased matrix, as in Eq. (6), and not by the closed form H(X)−H(ρ)H(X) - H(\rho)H(X)−H(ρ); using that closed form as the definition would make milestone 1 true by unfolding. ccc is a maximum over all four pairs of basis vectors and cmin⁡c_{\min}cmin​ the corresponding minimum.
  • Domains. Lemma 1, Eq. (17), is stated on EuclideanSpace ℂ (Fin d) for every ddd, and Eq. (18) on C2\mathbb C^2C2 only. Statements that vary the argument of fff restrict a,b,c,pa, b, c, pa,b,c,p to the intervals the paper uses, because the binary-entropy formula has no meaning outside [0,1][0,1][0,1].
  • No added hypotheses. The goal assumes nothing beyond "a qubit state" and "two measurement bases". On these objects 2P−1≥02P - 1 \ge 02P−1≥0 and c≤1c \le 1c≤1, so no square root is evaluated at a negative number.

A complete development needs spectral facts for 2×22\times 22×2 Hermitian matrices, concavity of the binary entropy in bits, and an extreme-point argument for concave functions on a polygon. The qubit layer and Lemma 1 are reusable beyond this mission. Proofs of any milestone, and alternative proofs of the goal, are welcome.

Selected references

  • X. Yuan, G. Bai, T. Peng, X. Ma, Quantum uncertainty relation using coherence, arXiv:1612.02573v2, 2017; Phys. Rev. A 96, 032313 (2017). https://arxiv.org/abs/1612.02573v2, https://doi.org/10.1103/PhysRevA.96.032313
  • T. Baumgratz, M. Cramer, M. B. Plenio, Quantifying coherence, Phys. Rev. Lett. 113, 140401 (2014). https://arxiv.org/abs/1311.0275
  • H. Maassen, J. B. M. Uffink, Generalized entropic uncertainty relations, Phys. Rev. Lett. 60, 1103 (1988). https://doi.org/10.1103/PhysRevLett.60.1103
  • M. Berta, M. Christandl, R. Colbeck, J. M. Renes, R. Renner, The uncertainty principle in the presence of quantum memory, Nature Physics 6, 659 (2010). https://arxiv.org/abs/0909.0950
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Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

Fluid Limits for Multiclass Many-Server Queues with General Reneging Distributions and Head-of-the-Line Scheduling: Fluid-Scaled States Are Tight and Their Limit Points Are Fluid Model SolutionsResearch Paper

Motivation

Call centers, hospital wards and other service systems with many agents serve several customer classes, and customers who wait too long hang up or leave. The standard model is the multiclass many-server queue with reneging: NNN identical servers, JJJ classes, class-dependent service-time and patience-time distributions, and a control policy that decides when an idle server takes a customer and from which class. Exact analysis is out of reach once service and patience times are not exponential, so performance is studied through fluid limits: the limit of the system scaled by 1/N1/N1/N as N→∞N\to\inftyN→∞.

A. L. Puha and A. R. Ward (MOR 2022, doi:10.1287/moor.2021.1166) prove such a limit theorem for general service and patience distributions, batch arrivals and an arbitrary admissible head-of-the-line policy, including policies that idle or randomize. Earlier results covered one class without reneging (Kaspi and Ramanan, Ann. Appl. Probab. 2011), one class with reneging and unit arrivals (Kang and Ramanan, Ann. Appl. Probab. 2010), and static priority policies (Atar, Kaspi and Shimkin, Math. Oper. Res. 2014).

Setting

Fix J≥1J\ge1J≥1 classes. Class jjj has a service-time distribution GjsG^s_jGjs​ on R+\mathbb R_+R+​ with density gjsg^s_jgjs​, and a patience-time distribution GjrG^r_jGjr​ on [0,∞][0,\infty][0,∞] with density gjrg^r_jgjr​ on R+\mathbb R_+R+​, so a customer may never abandon. For a distribution GGG with density ggg, H=sup⁡{x:G(x)<1}H=\sup\{x:G(x)<1\}H=sup{x:G(x)<1} is the right edge of its support and h=g/(1−G)h=g/(1-G)h=g/(1−G) on [0,H)[0,H)[0,H) is its hazard function.

In the NNN-th queue, class-jjj customers arrive by a counting process EjNE^N_jEjN​ that may jump by more than one. The state is (αN,XN,νN,ηN)(\alpha^N,X^N,\nu^N,\eta^N)(αN,XN,νN,ηN): XjNX^N_jXjN​ counts class-jjj customers in system; νjN\nu^N_jνjN​ is the age-in-service measure, a unit atom at the service age of each class-jjj customer in service; and ηjN\eta^N_jηjN​ is the potential-queue measure, a unit atom at the time in system of each class-jjj customer whose patience has not run out. The control enters only through the entry-into-service times. A head-of-the-line (HL) policy serves each class in order of arrival. It is admissible when the entry-into-service process KNK^NKN is adapted to the filtration generated by the state history and the policy's own independent uniform random variables.

The fluid model works on the state space X=R+J×∏jM[0,Hjs)×∏jM[0,Hjr)\mathbb X=\mathbb R^J_+\times\prod_j\mathbf M[0,H^s_j)\times\prod_j\mathbf M[0,H^r_j)X=R+J​×∏j​M[0,Hjs​)×∏j​M[0,Hjr​) of finite measures with the weak topology. Given an arrival function EEE (nondecreasing, rcll, E(0)=0E(0)=0E(0)=0), a path (X,ν,η)(X,\nu,\eta)(X,ν,η) defines the auxiliary functions Bj=⟨1,νj⟩B_j=\langle1,\nu_j\rangleBj​=⟨1,νj​⟩, Qj=Xj−BjQ_j=X_j-B_jQj​=Xj​−Bj​, Dj(t)=∫0t⟨hjs,νj(u)⟩duD_j(t)=\int_0^t\langle h^s_j,\nu_j(u)\rangle duDj​(t)=∫0t​⟨hjs​,νj​(u)⟩du, Kj=Bj+Dj−Bj(0)K_j=B_j+D_j-B_j(0)Kj​=Bj​+Dj​−Bj​(0), I=1−∑jBjI=1-\sum_jB_jI=1−∑j​Bj​, and the reneging function

Rj(t)=∫0t∫0Qj(u)hjr((Fj,u)−1(y)) dy du,Fj,u(x)=⟨1[0,x],ηj(u)⟩.R_j(t)=\int_0^t\int_0^{Q_j(u)}h^r_j\big((F_{j,u})^{-1}(y)\big)\,dy\,du,\qquad F_{j,u}(x)=\langle1_{[0,x]},\eta_j(u)\rangle .Rj​(t)=∫0t​∫0Qj​(u)​hjr​((Fj,u​)−1(y))dydu,Fj,u​(x)=⟨1[0,x]​,ηj​(u)⟩.

A fluid model solution for EEE satisfies the constraints (35)–(37), the monotonicity of KKK, the balance law Xj=Xj(0)+Ej−Rj−DjX_j=X_j(0)+E_j-R_j-D_jXj​=Xj​(0)+Ej​−Rj​−Dj​, and the transport equations (46)–(47) for νj\nu_jνj​ and ηj\eta_jηj​ driven by dKjdK_jdKj​ and dEjdE_jdEj​.

Formalization targets

Goal: Theorem 1 (p. 17)

Under Assumptions 4 and 5, for every sequence of admissible HL policies:

{(XˉN,νˉN,ηˉN)}N is tight in D(X),\{(\bar X^N,\bar\nu^N,\bar\eta^N)\}_{N}\ \text{is tight in }\mathbf D(\mathbb X),{(XˉN,νˉN,ηˉ​N)}N​ is tight in D(X),

and every distributional limit point (X,ν,η)(X,\nu,\eta)(X,ν,η) is, almost surely, a continuous fluid model solution for EEE started from (X0,ν0,η0)(X^0,\nu^0,\eta^0)(X0,ν0,η0), with continuous auxiliary functions and each ηj(t)\eta_j(t)ηj​(t) charging no points. Assumptions 1–3 ask that the scaled arrivals and initial states converge. Assumption 4 asks that the hazards be bounded or lower semicontinuous near the right edges Hjs,HjrH^s_j,H^r_jHjs​,Hjr​. Assumption 5 adds continuity of EEE, an atomless η0\eta^0η0, and control of KˉN\bar K^NKˉN by C-tightness or by inequality (55).

Milestones

  1. Lemma 1, (24) and (26): the prelimit dynamic equations for ⟨f,νjN⟩\langle f,\nu^N_j\rangle⟨f,νjN​⟩ and ⟨ς,ηjN⟩\langle\varsigma,\eta^N_j\rangle⟨ς,ηjN​⟩.
  2. Lemma 6, (61): ⟨1[0,x]hjr,ηjN(t)⟩=∫0Fj,tN(x)hjr((Fj,tN)−1(y)) dy\langle1_{[0,x]}h^r_j,\eta^N_j(t)\rangle=\int_0^{F^N_{j,t}(x)}h^r_j((F^N_{j,t})^{-1}(y))\,dy⟨1[0,x]​hjr​,ηjN​(t)⟩=∫0Fj,tN​(x)​hjr​((Fj,tN​)−1(y))dy.
  3. Lemma 7: the compensator bounds ∣As,jN(φ,t)∣≤∥φ∥∞(XjN(0)+EjN(t))∫0mhjs|\mathcal A^N_{s,j}(\varphi,t)|\le\|\varphi\|_\infty(X^N_j(0)+E^N_j(t))\int_0^mh^s_j∣As,jN​(φ,t)∣≤∥φ∥∞​(XjN​(0)+EjN​(t))∫0m​hjs​ and the reneging analogue.
  4. Lemma 8: relative compactness in D(R+)\mathbf D(\mathbb R_+)D(R+​) of the fluid-scaled real processes, and their C-tightness under Assumption 5.
  5. Lemma 2 (i) and (iii): continuity and the absence of atoms propagate along fluid model solutions.

Significance

Theorem 1 characterizes fluid limits for every admissible HL policy at once. To get the fluid limit of a specific policy, one adds the equations that policy imposes and proves uniqueness for the resulting system; the paper does this for weighted random buffer selection (its Theorems 3–5). The reneging equation (40) is the main new feature: abandonment depends on the whole distribution of waiting times in queue, not only on the queue length. Allowing batch arrivals means the reneging count can only be sandwiched between two compensators, which is why Lemma 6 is needed.

The results are proved in the paper, with parts of the tightness argument delegated to Kang–Ramanan and Kaspi–Ramanan. None of them is formalized. The mission defines from scratch a measure-valued queue with abandonment, the Skorokhod space D(X)\mathbf D(\mathbb X)D(X) with J1J_1J1​ convergence, and the fluid model of §3. These definitions are reusable for the single-class models of Kaspi–Ramanan and Kang–Ramanan, for the WRBS and static-priority policies, and for other measure-valued fluid limits.

Difficulty

Each milestone is a known argument, but the obvious route to the goal breaks at the reneging term. A naive limit passage in the prelimit reneging count RjNR^N_jRjN​ fails: with batch arrivals, RjNR^N_jRjN​ is not a functional of ηjN\eta^N_jηjN​ and QjNQ^N_jQjN​ alone, because customers with equal waiting times may be split between queue and service. Identifying the limit as the nonlinear function (40) requires bounds from above and below by marked point processes. It also requires showing that the compensators of these processes converge to a common limit, which uses that η\etaη charges no points along the limit. The tightness part needs Kurtz–Jakubowski criteria for measure-valued processes on spaces [0,H)[0,H)[0,H) whose right end may carry escaping mass. Lemma 6 is a pathwise identity for finite counting measures, and Lemma 7 is a pathwise bound.

Formalization scope

Classes are Fin J with J≥1J\ge1J≥1. Time is ℝ≥0. Customers are indexed by integers as in the paper. Event times are extended reals: a patience of ∞\infty∞ keeps a customer in the potential queue forever, and an entry time of ∞\infty∞ means the customer is never served. M[0,H)\mathbf M[0,H)M[0,H) is FiniteMeasure on the subtype [0,H)[0,H)[0,H) of ℝ≥0. J1J_1J1​ convergence uses one time change for all coordinates, with the maximum of the sup-norm and Lévy–Prokhorov distances on X\mathbb XX. Convergence in distribution, distributional limit points, relative compactness and C-tightness are stated in coupling form; on the Polish space D(X)\mathbf D(\mathbb X)D(X) these are equivalent to the usual notions. Hazards take values in [0,∞][0,\infty][0,∞] and are 000 off [0,H)[0,H)[0,H). The integrals in (37), (40), (41), Lemma 6 and Lemma 7 are integrals of nonnegative functions. The derivative indicators that define the departure, reneging and marked processes are written as explicit counts.

Four readings are disclosed in the items. The goal's initial condition is stated through a coupling carrying (E,X0,ν0,η0)(E,X^0,\nu^0,\eta^0)(E,X0,ν0,η0) jointly, because the limit point lives on its own probability space. Gs,GrG^s,G^rGs,Gr in (46)–(47) are read as Gjs,GjrG^s_j,G^r_jGjs​,Gjr​. In Lemma 8, the (K.2) branch of Assumption 2 is read as relative compactness of KˉjN\bar K^N_jKˉjN​, because the printed (K.2) does not imply it. The goal encodes Assumption 2 as printed. The head-of-the-line order is the HL condition stated in words on pp. 8–9 rather than inequality (10) alone, which would let a policy skip a waiting customer for good and serve younger ones.

The statement admits trivializing formalizations, and they are excluded here. The HL predicate contains only the defining constraints of Definitions 1–3: entry no earlier than arrival and before abandonment (9), the head-of-the-line order (the HL condition of pp. 8–9, which contains (10): a customer can enter service only after every earlier customer of its class has entered or abandoned), the state constraints (S.1), (S.2), (15) and (16), and rcll paths. The identities (18)–(26) are not in it. All standing independence and distributional hypotheses and the adaptedness of KNK^NKN are explicit. The auxiliary functions R,D,B,Q,K,IR,D,B,Q,K,IR,D,B,Q,K,I are computed from the path, never chosen. The policy is not specialized: idling and randomization are allowed.

Not posed: Lemmas 3–5, 9 and 10, Theorem 2, and Lemma 2 (ii) and (iv). Lemma 4 needs a server-assignment filtration, Lemma 5 needs predictable quadratic variations, and Theorem 2, Lemma 9 and Lemma 10 need measure-valued marked point processes on [0,H)×R+[0,H)\times\mathbb R_+[0,H)×R+​. Formalizing these, or a sorry-free construction of an admissible system satisfying Assumptions 1–5, is welcome.

Selected references

  • A. L. Puha, A. R. Ward, Fluid limits for multiclass many-server queues with general reneging distributions and head-of-the-line scheduling, Mathematics of Operations Research, Articles in Advance, 2021 (2022). https://doi.org/10.1287/moor.2021.1166
  • H. Kaspi, K. Ramanan, Law of large numbers limits for many-server queues, Annals of Applied Probability 21 (2011) 33–114. https://doi.org/10.1214/10-AAP681
  • W. Kang, K. Ramanan, Fluid limits of many-server queues with reneging, Annals of Applied Probability 20 (2010) 2204–2260. https://doi.org/10.1214/10-AAP683
  • R. Atar, H. Kaspi, N. Shimkin, Fluid limits for many-server systems with reneging under a priority policy, Mathematics of Operations Research 39 (2014) 672–696. https://doi.org/10.1287/moor.2013.0632
  • S. N. Ethier, T. G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986. https://doi.org/10.1002/9780470316658
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Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

Large Fork-Join Queues with Nearly Deterministic Arrival and Service Times: Fluid Limit of the Maximum Queue Length with a Non-Zero Initial ConditionResearch Paper

Motivation

A fork-join queue splits every incoming job into tasks, sends one task to each of NNN parallel servers, and declares the job complete only when all tasks are done. The model describes assembly systems in which a manufacturer orders parts from NNN suppliers and can only start production when every part has arrived, as well as parallel computing and storage systems in which a request is answered only after all sub-requests return. Because a job waits for its slowest task, the performance of the system is governed by the maximum queue length over the NNN servers, and the question of interest is how this maximum behaves when NNN is large and the system is heavily loaded.

Schol, Vlasiou and Zwart (arXiv:1912.11661, Mathematics of Operations Research 47(2), 2022) study this question in a nearly deterministic regime: arrivals and services happen in almost every time slot, and the traffic intensity of each server tends to 111 at rate N−2N^{-2}N−2. Even in the empty-start case the queue lengths of different servers are dependent, because every server sees the same arrival process; the maximum of NNN dependent random walks has to be analysed directly.

Timeline. Early work treats two service stations and obtains exact asymptotics (Flatto and Hahn, 1984; Baccelli, 1985; Wright, 1992). For more stations the literature turned to approximations and bounds: Nelson and Tantawi (1988) and Baccelli and Makowski (1989) bound the mean response time, and Ko and Serfozo (2004) approximate the response-time distribution in M/M/s fork-join queues. Heavy-traffic process limits for a fixed number of stations were obtained by Varma (1990) and Nguyen (1993, 1994), with reflected Brownian motion limits, and by Lu and Pang (2015–2017) for many-server stations. Sigman and Whitt (2011) analysed nearly deterministic G/G/1 and G/D/N queues. The paper of this mission gives a process-level (fluid) limit for the largest queue when the number of servers NNN itself grows, in the nearly deterministic regime and with a non-zero initial condition.

Setting

Fix α,β>0\alpha,\beta>0α,β>0. For each NNN the system runs in discrete time slots j=1,2,…j=1,2,\dotsj=1,2,…. In slot jjj a task arrives at all NNN servers with probability p(N)=1−α/N−β/N2p^{(N)}=1-\alpha/N-\beta/N^2p(N)=1−α/N−β/N2 (indicator X(N)(j)X^{(N)}(j)X(N)(j)), and server iii completes a task with probability q(N)=1−α/Nq^{(N)}=1-\alpha/Nq(N)=1−α/N (indicator Yi(N)(j)Y_i^{(N)}(j)Yi(N)​(j)), all indicators being independent. The arrival process is A(N)(n)=∑j=1nX(N)(j)A^{(N)}(n)=\sum_{j=1}^{n}X^{(N)}(j)A(N)(n)=∑j=1n​X(N)(j) and the service process of server iii is Si(N)(n)=∑j=1nYi(N)(j)S_i^{(N)}(n)=\sum_{j=1}^{n}Y_i^{(N)}(j)Si(N)​(n)=∑j=1n​Yi(N)​(j).

Server iii starts with Qi(N)(0)=⌊rNUi⌋Q_i^{(N)}(0)=\lfloor r_NU_i\rfloorQi(N)​(0)=⌊rN​Ui​⌋ tasks, where U1,U2,…U_1,U_2,\dotsU1​,U2​,… are i.i.d. random variables, the initial queue lengths are non-negative, and rN≥0r_N\ge0rN​≥0 is a scaling sequence. By Lindley's recursion the maximum queue length at time nnn is

Q(α,β)(N)(n)=max⁡i≤Nmax⁡(sup⁡0≤k≤n[(A(N)(n)−A(N)(k))−(Si(N)(n)−Si(N)(k))],  Qi(N)(0)+A(N)(n)−Si(N)(n)).Q^{(N)}_{(\alpha,\beta)}(n)=\max_{i\le N}\max\Big(\sup_{0\le k\le n}\big[(A^{(N)}(n)-A^{(N)}(k))-(S_i^{(N)}(n)-S_i^{(N)}(k))\big],\;Q_i^{(N)}(0)+A^{(N)}(n)-S_i^{(N)}(n)\Big).Q(α,β)(N)​(n)=i≤Nmax​max(0≤k≤nsup​[(A(N)(n)−A(N)(k))−(Si(N)​(n)−Si(N)​(k))],Qi(N)​(0)+A(N)(n)−Si(N)​(n)).

The first term alone is the maximum queue length of the system started empty. The initial condition is assumed to satisfy Q(α,β)(N)(0)/(Nlog⁡N)→q(0)≥0Q^{(N)}_{(\alpha,\beta)}(0)/(N\log N)\to q(0)\ge0Q(α,β)(N)​(0)/(NlogN)→q(0)≥0 in probability (Assumption 2.3), and either UiU_iUi​ has a finite right endpoint (Assumption 2.4) or UiU_iUi​ is continuous with −log⁡P(Ui>vt)/−log⁡P(Ui>t)→h(v)-\log\mathbb P(U_i>vt)/-\log\mathbb P(U_i>t)\to h(v)−logP(Ui​>vt)/−logP(Ui​>t)→h(v) as t→∞t\to\inftyt→∞ for all v∈[0,1]v\in[0,1]v∈[0,1] (Assumption 2.5, the Gumbel-domain case).

The fluid limit is

q(t)=max⁡((2αt−βt)1(t<α2β2)+α2β1(t≥α2β2),  g(t,q(0))−βt),q(t)=\max\Big(\big(\sqrt{2\alpha t}-\beta t\big)\mathbb 1\big(t<\tfrac{\alpha}{2\beta^2}\big)+\tfrac{\alpha}{2\beta}\mathbb 1\big(t\ge\tfrac{\alpha}{2\beta^2}\big),\;g(t,q(0))-\beta t\Big),q(t)=max((2αt​−βt)1(t<2β2α​)+2βα​1(t≥2β2α​),g(t,q(0))−βt),

with g(t,q(0))=q(0)+2αtg(t,q(0))=q(0)+\sqrt{2\alpha t}g(t,q(0))=q(0)+2αt​ under Assumption 2.4 and g(t,q(0))=sup⁡{2αt u+q(0)v:u2+h(v)≤1, 0≤u,v≤1}g(t,q(0))=\sup\{\sqrt{2\alpha t}\,u+q(0)v : u^2+h(v)\le1,\ 0\le u,v\le1\}g(t,q(0))=sup{2αt​u+q(0)v:u2+h(v)≤1, 0≤u,v≤1} under Assumption 2.5. In Lean these are fluid, fluidEmpty, gFinite and gGumbel; the queue is maxQueue and the empty-start queue maxQueueEmpty.

Formalization targets

Goal: Theorem 2.1 (fluid limit)

For every T>0T>0T>0 and ϵ>0\epsilon>0ϵ>0,

P(sup⁡0≤t≤T∣Q(α,β)(N)(tN3log⁡N)Nlog⁡N−q(t)∣>ϵ)→N→∞0,\mathbb P\left(\sup_{0\le t\le T}\left|\frac{Q^{(N)}_{(\alpha,\beta)}(tN^3\log N)}{N\log N}-q(t)\right|>\epsilon\right)\xrightarrow{N\to\infty}0,P​0≤t≤Tsup​​NlogNQ(α,β)(N)​(tN3logN)​−q(t)​>ϵ​N→∞​0,

under Assumptions 2.1–2.3 and either Assumption 2.4 or Assumption 2.5 (one conjunct per case).

Milestones

  1. Section 4.2 tools. The pathwise oscillation bound of Lemma 4.1; the non-uniform Berry–Esseen rate of Lemma 4.2 for the standardized service process; the moment bound of Lemma 4.3; the extreme-value Lemma B.1 for sums of independent relatively stable variables and its consequence Lemma 4.4 for the Gaussian surrogate of the initial condition.
  2. Pointwise convergence (Section 4.3). Lemmas 4.6 and 4.8 (bounds for the empty-start system), Lemma 4.5 (its pointwise limit), Lemma 4.9 (the initial-condition part) and Theorem 4.1: Q(α,β)(N)(tN3log⁡N)/(Nlog⁡N)→q(t)Q^{(N)}_{(\alpha,\beta)}(tN^3\log N)/(N\log N)\to q(t)Q(α,β)(N)​(tN3logN)/(NlogN)→q(t) in probability for each t>0t>0t>0.
  3. Tightness (Section 4.4). Lemma 4.10 (maxima preserve uniform convergence), Lemmas 4.11–4.12 (moduli of continuity of the two parts) and Corollary 4.1 (tightness of the scaled process on [0,T][0,T][0,T]).

Significance

The result. Theorem 2.1 identifies the scaling under which the maximum queue length of a large, heavily loaded fork-join system follows a deterministic curve: time of order N3log⁡NN^3\log NN3logN and space of order Nlog⁡NN\log NNlogN. The limit separates the contribution of the empty-start dynamics, which saturate at the steady-state level α/(2β)\alpha/(2\beta)α/(2β) after time α/(2β2)\alpha/(2\beta^2)α/(2β2), from the contribution of the initial backlog, which is governed by the extreme-value class of the initial condition. For instance, with h(v)=vh(v)=vh(v)=v and q(0)=α/(2β)q(0)=\alpha/(2\beta)q(0)=α/(2β) the system "starts and stays in steady state" on an initial interval (p. 12). The theorem gives the transient behaviour needed to judge how long a backlog at the slowest supplier persists.

Formalizing it. The result is proved in the paper; no part of it has a machine-checked proof. The mission produces a formal statement of the model and of the fluid limit, and the intermediate results of Section 4. The proof combines a non-uniform Berry–Esseen inequality, extreme-value theory for maxima of sums, Doob's maximal inequality and a tightness criterion; formalizing it would give reusable Lean versions of several of these tools.

Difficulty

The obvious argument treats the NNN queues as independent reflected random walks and applies extreme-value theory to their maximum. It fails because all servers share the arrival process, so the queues are dependent. The paper handles this by splitting each queue into a common arrival term and an individual service term, but the individual terms are maxima of NNN centred random walks evaluated at a time of order N3log⁡NN^3\log NN3logN, and their Gaussian approximation must be accurate at the scale of the maximum: a uniform Berry–Esseen bound is too weak, and a non-uniform bound with the right rate in NNN is needed (Lemma 4.2). Upgrading pointwise convergence to uniform convergence on [0,T][0,T][0,T] requires a modulus-of-continuity estimate for a maximum of NNN processes (Lemmas 4.11–4.12), where the number of processes grows with NNN. The initial-condition term requires an extreme-value result for maxima of sums of two independent coordinates with different tails (Lemma B.1).

Formalization scope

All objects are defined in one module, LargeForkJoin.FluidLimit.Model. Times are natural numbers, and Q(tN3log⁡N)Q(tN^3\log N)Q(tN3logN) is evaluated at ⌊tN3log⁡N⌋\lfloor tN^3\log N\rfloor⌊tN3logN⌋, which is the paper's own convention Q(n)=Q(⌊n⌋)Q(n)=Q(\lfloor n\rfloor)Q(n)=Q(⌊n⌋). Servers are indexed 0,…,N−10,\dots,N-10,…,N−1. All variables live on one probability space; the Bernoulli laws are imposed for N≥N0N\ge N_0N≥N0​ (for small NNN, p(N)p^{(N)}p(N) can be negative), and within each N≥N0N\ge N_0N≥N0​ the arrival indicators, service indicators and initial-condition variables UiU_iUi​ used by that system are mutually independent. The independence of (Ui)(U_i)(Ui​) from arrivals and services is an added assumption: the paper uses it in its proofs but does not state it. Initial queue lengths are non-negative almost surely. Assumption 2.5 adds P(Ui>t)>0\mathbb P(U_i>t)>0P(Ui​>t)>0 for all ttt, without which its ratio is undefined; "continuous" means "no atoms". Convergence in probability to a constant is written with ϵ\epsilonϵ-events, and sup⁡0≤t≤T∣⋅∣>ϵ\sup_{0\le t\le T}|\cdot|>\epsilonsup0≤t≤T​∣⋅∣>ϵ as "some t∈[0,T]t\in[0,T]t∈[0,T] has ∣⋅∣>ϵ|\cdot|>\epsilon∣⋅∣>ϵ", the same event. Lemmas 4.4 and 4.9 speak of Gaussian variables outside the model; they are stated for the law of NNN independent pairs (standard normal, law of U1U_1U1​).

The goal is stated about the maximum queue length built from the Bernoulli indicators through (2.3), uniformly on [0,T][0,T][0,T]. A statement about a Gaussian or reflected-Brownian surrogate (the heuristics of Sections 2.2–2.3), or a pointwise statement (Theorem 4.1), would not be Theorem 2.1.

Not included: Propositions 2.1–2.3 (other scalings and the steady state), the variant of Theorem 2.1 under Assumption 2.6, Theorem 4.2 (finite-dimensional distributions, a generic fact), and Lemma 4.7, whose statement includes the stationary case t=∞t=\inftyt=∞ and needs a stationary-queue object. Contributions of general tools are welcome: a non-uniform Berry–Esseen inequality for Bernoulli sums, extreme-value results for maxima of i.i.d. sequences (relative stability, Gumbel-domain tails), and the tightness criterion of Billingsley's Theorem 7.3.

Selected references

  • D. Schol, M. Vlasiou, B. Zwart, Large fork-join queues with nearly deterministic arrival and service times, Mathematics of Operations Research 47(2), 2022; arXiv:1912.11661v3. https://arxiv.org/abs/1912.11661v3
  • L. Flatto, S. Hahn, Two parallel queues created by arrivals with two demands I, SIAM Journal on Applied Mathematics 44(5), 1984. https://doi.org/10.1137/0144072
  • F. Baccelli, A. M. Makowski, Queueing models for systems with synchronization constraints, Proceedings of the IEEE 77(1), 1989. https://doi.org/10.1109/5.21076
  • R. Nelson, A. N. Tantawi, Approximate analysis of fork/join synchronization in parallel queues, IEEE Transactions on Computers 37(6), 1988. https://doi.org/10.1109/12.2212
  • K. Sigman, W. Whitt, Heavy-traffic limits for nearly deterministic queues, Journal of Applied Probability 48(3), 2011. https://doi.org/10.1239/jap/1316796905
  • S.-S. Ko, R. F. Serfozo, Response times in M/M/s fork-join networks, Advances in Applied Probability 36(3), 2004. https://doi.org/10.1239/aap/1093962240
  • P. Billingsley, Convergence of Probability Measures, 2nd ed., Wiley, 1999. https://doi.org/10.1002/9780470316962
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Discrete Dividend Payments in Continuous Time: The Value Function Is the Unique Fixed Point of the One-Period Dividend-and-Issuance OperatorResearch Paper

Why periodic dividends matter

A firm can return cash to shareholders by paying dividends, but a payment reduces the reserves available to survive future losses. If cash can be distributed only at scheduled dates while equity can be raised between those dates, the firm must coordinate a discrete dividend decision with a continuous-time financing decision. Keppo, Reppen and Soner study this combination for a firm whose cash flow is a Brownian motion with drift. Their preprint identifies the firm's optimal value through an operator that first solves the financing problem between dividend dates and then chooses the next dividend. The mission concerns that characterization, Theorem 3.4, together with the regularity results on which it depends.

The cash reserve model

Let x≥0x\ge0x≥0 be the initial reserve and let Ct=μt+σWtC_t=\mu t+\sigma W_tCt​=μt+σWt​, where WWW is a one-dimensional Brownian motion, μ>0\mu>0μ>0 is profitability, and σ>0\sigma>0σ>0 is volatility. Dividends of amounts ℓn≥0\ell_n\ge0ℓn​≥0 may be paid at dates nTnTnT, with T>0T>0T>0. Equity issues have sizes ζk≥0\zeta_k\ge0ζk​≥0 and occur at stopping times τk\tau_kτk​; the issue times are locally finite. A positive issue costs

c(ζ)=λf+(1+λp)ζ,λf,λp>0,c(\zeta)=\lambda_f+(1+\lambda_p)\zeta,\qquad \lambda_f,\lambda_p>0,c(ζ)=λf​+(1+λp​)ζ,λf​,λp​>0,

while no issue costs zero. The cash reserve after actions at time ttt is Xt=x+Ct−Lt+ItX_t=x+C_t-L_t+I_tXt​=x+Ct​−Lt​+It​. The ruin time θ\thetaθ is the first strictly positive time that Xt<0X_t<0Xt​<0. A dividend cannot exceed the reserve immediately before its date, and no action is taken after ruin. These conditions define the admissible controls Ax\mathcal A_xAx​.

The firm's value function is the supremum, over admissible controls, of expected discounted dividends less expected discounted issue costs:

V(x)=sup⁡(L,I)∈AxEx[∑n≥0e−ρnTℓn−∑ke−ρτkc(ζk)],ρ>0.V(x)=\sup_{(L,I)\in\mathcal A_x}\mathbb E_x\left[\sum_{n\ge0}e^{-\rho nT}\ell_n-\sum_k e^{-\rho\tau_k}c(\zeta_k)\right],\qquad \rho>0.V(x)=(L,I)∈Ax​sup​Ex​[n≥0∑​e−ρnTℓn​−k∑​e−ρτk​c(ζk​)],ρ>0.

The first sum includes a possible dividend at time zero, following the displayed objective in §3.1 of the preprint. An issue at time TTT belongs to the next period. Thus the one-period financing operator Lϕ\mathcal L\phiLϕ charges issues on [0,T)[0,T)[0,T) and evaluates its continuation reward ϕ\phiϕ at the reserve immediately before TTT. The dividend operator is

Dϕ(x)=sup⁡0≤ℓ≤x{ϕ(x−ℓ)+ℓ},T=D∘L.\mathcal D\phi(x)=\sup_{0\le\ell\le x}\{\phi(x-\ell)+\ell\},\qquad \mathcal T=\mathcal D\circ\mathcal L.Dϕ(x)=0≤ℓ≤xsup​{ϕ(x−ℓ)+ℓ},T=D∘L.

The continuation class CA\mathcal C_ACA​ consists of the continuous, nondecreasing functions ϕ:[0,∞)→[0,∞)\phi:[0,\infty)\to[0,\infty)ϕ:[0,∞)→[0,∞) that satisfy the issuance boundary condition of Definition 3.2, are bounded above by x+Ax+Ax+A, and have ϕ(x)−x\phi(x)-xϕ(x)−x nondecreasing and bounded in absolute value by AAA. Its larger class C^A\widehat{\mathcal C}_ACA​ omits the last condition. The intervention value in the boundary condition is Iϕ(x)=sup⁡ζ>0{ϕ(x+ζ)−c(ζ)}\mathcal I\phi(x)=\sup_{\zeta>0}\{\phi(x+\zeta)-c(\zeta)\}Iϕ(x)=supζ>0​{ϕ(x+ζ)−c(ζ)}.

Formalization targets

The first target is the mapping statement in Theorem 3.3: D:C^A→CA\mathcal D:\widehat{\mathcal C}_A\to\mathcal C_AD:CA​→CA​ for A≥0A\ge0A≥0. With

A∗=μTeρT−1,A^*=\frac{\mu T}{e^{\rho T}-1},A∗=eρT−1μT​,

the next targets are the one-period bound 0≤Lϕ(x)≤e−ρTx+A0\le\mathcal L\phi(x)\le e^{-\rho T}x+A0≤Lϕ(x)≤e−ρTx+A for A≥A∗A\ge A^*A≥A∗, the classical one-period characterization of Theorem 3.6, and the remaining mapping and contraction assertions of Theorem 3.3. In particular, T\mathcal TT contracts the uniform distance between functions in CA\mathcal C_ACA​ by the factor e−ρTe^{-\rho T}e−ρT.

The goal is Theorem 3.4:

V∈CA∗,TV=V,ϕ∈CA∗ and Tϕ=ϕ ⟹ ϕ=V.V\in\mathcal C_{A^*},\qquad \mathcal T V=V,\qquad \phi\in\mathcal C_{A^*}\ \text{and}\ \mathcal T\phi=\phi\ \Longrightarrow\ \phi=V.V∈CA∗​,TV=V,ϕ∈CA∗​ and Tϕ=ϕ ⟹ ϕ=V.

This identifies the fixed point with the value defined from admissible controls. It also asserts that the value is finite at every nonnegative initial reserve.

What the characterization gives

Theorem 3.4 turns an infinite-horizon control problem into repeated one-period calculations. Since Theorem 3.3 makes T\mathcal TT a strict contraction on CA∗\mathcal C_{A^*}CA∗​, iterating it determines the value in that class. The source connects this characterization to a numerical method when the one-period financing problem can be computed efficiently. A proof in Lean would also provide reusable statements about locally finite impulse controls, periodic actions, ruin, and discounted extended-real objectives. The preprint proves the mathematical results; this mission records their statements as open Lean theorems for machine-checked proofs.

Where the difficulty lies

The dividend operator is an elementary supremum over one payment, but the financing operator ranges over adapted impulses before ruin. Its regularity is central: the paper invokes Theorem 3.6 to show that Lϕ\mathcal L\phiLϕ is continuous and satisfies the issuance boundary condition. That theorem characterizes the arbitrary-maturity issuance value as the unique classical solution of a parabolic equation with a nonlocal boundary condition. The fixed-point conclusion alone would leave an additional gap: Theorem 3.4 must identify that fixed point with the original control supremum, including the limit over dividend periods and its terminal reward.

Formalization scope

Lean represents nonnegative reserves by R≥0\mathbb R_{\ge0}R≥0​ and the discount, costs and function values by real numbers. Control values and one-period rewards are suprema in extended real numbers, with dividends and issue costs integrated separately as nonnegative quantities. The L\mathcal LL bound proves the finiteness needed before converting to real values. An expression with both expected dividends and expected costs infinite takes the extended-real value −∞-\infty−∞ and cannot improve a supremum with a finite admissible alternative.

The paper's cumulative processes are represented by nonnegative dividend amounts and a locally finite impulse sequence of nonnegative issues. This makes explicit that equity cannot be supplied by an uncharged continuous component. Simultaneous impulses are allowed; merging them cannot increase the cost. The Brownian cash flow uses the published AtaBarjesteh23.Workload.IsDriftBM definition. The model requires a probability measure, adaptation to a filtration, and positive ρ,μ,σ,λf,λp,T\rho,\mu,\sigma,\lambda_f,\lambda_p,Tρ,μ,σ,λf​,λp​,T. The filtration is right-continuous and its initial σ-algebra contains all subsets of ambient null measurable sets, as required by the usual conditions. A dividend at time zero follows the objective's sum. In L\mathcal LL, the continuation value uses XT−X_{T-}XT−​, resolving the free-issue-at-TTT ambiguity in the printed formula. The arbitrary-maturity problem retains its separately printed non-strict survival indicator.

The value VVV is defined solely from admissible controls, never from T\mathcal TT or its iterates. Theorem 3.6 uses time to maturity and states smoothness only on the interior rectangle; uniqueness is restricted to the closed nonnegative time-state rectangle. Reusable work includes stopping-time measurability, impulse summation and parabolic regularity. Contributions proving the goal or the four listed milestones are within scope; §4's random-profitability model and §3.4's numerical experiments are outside this mission.

Selected references

  • J. Keppo, A. M. Reppen and H. M. Soner, Discrete Dividend Payments in Continuous Time, Mathematics of Operations Research, 2021; preprint arXiv:1805.05077v2, 2019. https://arxiv.org/abs/1805.05077v2
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On Computing the Nonlinearity Interval in Parametric Semidefinite Optimization: The Set of Transition Points of the Optimal Partition Is FiniteResearch Paper

Motivation

Sensitivity analysis asks how the solution of an optimization problem changes when its data move. For linear optimization the answer has been known since the 1990s: as the objective is perturbed along a fixed direction, the optimal partition (which variables can be positive at an optimum and which slacks can) stays constant on open intervals and changes only at finitely many breakpoints, and the optimal value is piecewise linear with breakpoints exactly there (Adler and Monteiro, Algorithmica 8, 1992; Jansen, Roos and Terlaky, 1993). Semidefinite optimization (SDO) is used throughout control, combinatorial relaxations and polynomial optimization, and its parametric behaviour is less regular. The optimal partition can stay constant while the optimal sets move (a nonlinearity interval), and the optimal value need not be piecewise linear.

Mohammad-Nezhad and Terlaky (Optimization 69, 2020) defined invariancy intervals, nonlinearity intervals and transition points for parametric SDO. Hauenstein, Mohammad-Nezhad, Tang and Terlaky (arXiv:1908.10499v3; Mathematics of Operations Research, 2022) prove that there are only finitely many transition points (Theorem 1, p. 8) and then compute nonlinearity intervals with numerical algebraic geometry. Finiteness is what makes a computational description possible: without it, the interior of the domain need not decompose into finitely many intervals of each kind.

Timeline:

  • 1992–1993: Adler and Monteiro, and Jansen, Roos and Terlaky, start the optimal partition approach to parametric linear optimization.
  • 1999: Goldfarb and Scheinberg extend the optimal partition approach to parametric SDO (Applied Numerical Mathematics 29).
  • 2020: Mohammad-Nezhad and Terlaky introduce the optimal partition approach to parametric SDO (Definitions 3–5 of the present paper are taken from there).
  • 2019–2022: Hauenstein, Mohammad-Nezhad, Tang and Terlaky prove that the transition points are finite (Theorem 1) and give the nonlinearity-interval algorithm.

Setting

Let Sn\mathbb S^nSn be the real symmetric n×nn\times nn×n matrices with ⟨M,X⟩=tr⁡(MX)\langle M,X\rangle=\operatorname{tr}(MX)⟨M,X⟩=tr(MX). Data: A1,…,Am,C,Cˉ∈SnA^1,\dots,A^m,C,\bar C\in\mathbb S^nA1,…,Am,C,Cˉ∈Sn and b∈Rmb\in\mathbb R^mb∈Rm. For a real parameter ϵ\epsilonϵ consider

(Pϵ) inf⁡X{⟨C+ϵCˉ,X⟩: ⟨Ai,X⟩=bi, X⪰0},(Dϵ) sup⁡(y,S){bTy: ∑iyiAi+S=C+ϵCˉ, S⪰0}.(\mathrm P_\epsilon)\ \inf_X\{\langle C+\epsilon\bar C,X\rangle:\ \langle A^i,X\rangle=b_i,\ X\succeq0\},\qquad (\mathrm D_\epsilon)\ \sup_{(y,S)}\Big\{b^Ty:\ \textstyle\sum_i y_iA^i+S=C+\epsilon\bar C,\ S\succeq0\Big\}.(Pϵ​) Xinf​{⟨C+ϵCˉ,X⟩: ⟨Ai,X⟩=bi​, X⪰0},(Dϵ​) (y,S)sup​{bTy: ∑i​yi​Ai+S=C+ϵCˉ, S⪰0}.

The primal feasible set P\mathcal PP does not depend on ϵ\epsilonϵ; the dual one is D(ϵ)\mathcal D(\epsilon)D(ϵ). The optimal value function v(ϵ)∈R∪{±∞}v(\epsilon)\in\mathbb R\cup\{\pm\infty\}v(ϵ)∈R∪{±∞} is the infimum of (Pϵ)(\mathrm P_\epsilon)(Pϵ​), its domain is E={ϵ: v(ϵ)>−∞}\mathcal E=\{\epsilon:\ v(\epsilon)>-\infty\}E={ϵ: v(ϵ)>−∞}, and the optimal sets are P∗(ϵ)={X∈P:⟨C+ϵCˉ,X⟩=v(ϵ)}\mathcal P^*(\epsilon)=\{X\in\mathcal P:\langle C+\epsilon\bar C,X\rangle=v(\epsilon)\}P∗(ϵ)={X∈P:⟨C+ϵCˉ,X⟩=v(ϵ)} and D∗(ϵ)={(y,S)∈D(ϵ):bTy=v(ϵ)}\mathcal D^*(\epsilon)=\{(y,S)\in\mathcal D(\epsilon):b^Ty=v(\epsilon)\}D∗(ϵ)={(y,S)∈D(ϵ):bTy=v(ϵ)}.

Standing assumptions (p. 2): Assumption 1, the AiA^iAi are linearly independent; Assumption 2, there are X∘∈PX^\circ\in\mathcal PX∘∈P, (y∘,S∘)∈D(0)(y^\circ,S^\circ)\in\mathcal D(0)(y∘,S∘)∈D(0) with X∘,S∘≻0X^\circ,S^\circ\succ0X∘,S∘≻0.

For ϵ∈int⁡(E)\epsilon\in\operatorname{int}(\mathcal E)ϵ∈int(E), a maximally complementary optimal solution (X∗(ϵ),y∗(ϵ),S∗(ϵ))(X^*(\epsilon),y^*(\epsilon),S^*(\epsilon))(X∗(ϵ),y∗(ϵ),S∗(ϵ)) has X∗(ϵ)∈ri⁡P∗(ϵ)X^*(\epsilon)\in\operatorname{ri}\mathcal P^*(\epsilon)X∗(ϵ)∈riP∗(ϵ) and (y∗(ϵ),S∗(ϵ))∈ri⁡D∗(ϵ)(y^*(\epsilon),S^*(\epsilon))\in\operatorname{ri}\mathcal D^*(\epsilon)(y∗(ϵ),S∗(ϵ))∈riD∗(ϵ) (Definition 1). A point ϵˉ∈int⁡(E)\bar\epsilon\in\operatorname{int}(\mathcal E)ϵˉ∈int(E) is a transition point if every interval (ϵˉ−δ,ϵˉ+δ)∩int⁡(E)(\bar\epsilon-\delta,\bar\epsilon+\delta)\cap\operatorname{int}(\mathcal E)(ϵˉ−δ,ϵˉ+δ)∩int(E) contains an ϵ\epsilonϵ with rank⁡X∗(ϵ)≠rank⁡X∗(ϵˉ)\operatorname{rank}X^*(\epsilon)\ne\operatorname{rank}X^*(\bar\epsilon)rankX∗(ϵ)=rankX∗(ϵˉ) or rank⁡S∗(ϵ)≠rank⁡S∗(ϵˉ)\operatorname{rank}S^*(\epsilon)\ne\operatorname{rank}S^*(\bar\epsilon)rankS∗(ϵ)=rankS∗(ϵˉ) (Definition 5).

Formalization targets

Goal: Theorem 1 (p. 8)

{ϵˉ∈R: ϵˉ is a transition point} is finite.\{\bar\epsilon\in\mathbb R:\ \bar\epsilon\ \text{is a transition point}\}\ \text{is finite.}{ϵˉ∈R: ϵˉ is a transition point} is finite.

The statement names no bound on the number of transition points; it asserts finiteness only.

Milestones, in the order of the paper's argument

  1. Remark 1 (p. 2): strictly feasible primal and dual solutions exist at every ϵ∈int⁡(E)\epsilon\in\operatorname{int}(\mathcal E)ϵ∈int(E).
  2. p. 2: E\mathcal EE is an interval with at least two points; vvv is finite and concave on E\mathcal EE and continuous on int⁡(E)\operatorname{int}(\mathcal E)int(E).
  3. p. 2: for ϵ∈int⁡(E)\epsilon\in\operatorname{int}(\mathcal E)ϵ∈int(E), P∗(ϵ)\mathcal P^*(\epsilon)P∗(ϵ) and D∗(ϵ)\mathcal D^*(\epsilon)D∗(ϵ) are nonempty and compact (strong duality).
  4. (1), p. 2: on int⁡(E)\operatorname{int}(\mathcal E)int(E), a primal–dual triple is optimal iff it is feasible and XS=0XS=0XS=0.
  5. Appendix, p. 22: the ranks at relative-interior optimal points are maximal on the optimal sets.
  6. (19), p. 22: int⁡(E)=⋃θ+σ≤nS(θ,σ)\operatorname{int}(\mathcal E)=\bigcup_{\theta+\sigma\le n}\mathcal S_{(\theta,\sigma)}int(E)=⋃θ+σ≤n​S(θ,σ)​, where S(θ,σ)\mathcal S_{(\theta,\sigma)}S(θ,σ)​ is the set of ϵ∈int⁡(E)\epsilon\in\operatorname{int}(\mathcal E)ϵ∈int(E) at which some (X,y,S)∈ri⁡(P∗(ϵ)×D∗(ϵ))(X,y,S)\in\operatorname{ri}(\mathcal P^*(\epsilon)\times\mathcal D^*(\epsilon))(X,y,S)∈ri(P∗(ϵ)×D∗(ϵ)) has ranks (θ,σ)(\theta,\sigma)(θ,σ).
  7. p. 22: ϵˉ\bar\epsilonϵˉ is a transition point iff ϵˉ∈bd⁡(S(θ,σ))∩int⁡(E)\bar\epsilon\in\operatorname{bd}(\mathcal S_{(\theta,\sigma)})\cap\operatorname{int}(\mathcal E)ϵˉ∈bd(S(θ,σ)​)∩int(E) for some θ+σ≤n\theta+\sigma\le nθ+σ≤n.
  8. p. 23: every S(θ,σ)\mathcal S_{(\theta,\sigma)}S(θ,σ)​ is a semi-algebraic subset of R\mathbb RR.
  9. [Basu–Pollack–Roy, Theorem 5.22], cited p. 22: a semi-algebraic subset of R\mathbb RR has finitely many boundary points.

Significance

The result. Theorem 1 implies that int⁡(E)\operatorname{int}(\mathcal E)int(E) is a finite union of invariancy intervals, nonlinearity intervals and transition points (p. 8). This is the structural fact behind the paper's algorithm, which follows the optimal solution along a nonlinearity interval and detects its end points, and it extends to SDO the finite-breakpoint picture of parametric linear optimization. Without finiteness, a sensitivity report would have no finite description.

Formalizing it. The theorem is proved in the paper; nothing here is open. It has no machine-checked proof that we know of. A complete development would bring parametric conic duality into Lean (the interior point condition moving along a direction, strong duality with attainment, compactness of optimal sets), and it would connect convex analysis to semi-algebraic geometry: relative interiors, ranks of positive semidefinite matrices, and the one-dimensional case of Tarski–Seidenberg. Each of these is useful beyond this paper.

Difficulty

The obvious argument says that ranks are integers between 000 and nnn, so they can change only finitely often. That is false for arbitrary integer-valued functions on an interval: a rank pair could alternate on a sequence accumulating at a point, producing infinitely many transition points. Finiteness needs a structural reason why each level set S(θ,σ)\mathcal S_{(\theta,\sigma)}S(θ,σ)​ is a finite union of points and intervals. That reason is semi-algebraicity. Proving it requires showing that the relative interior of the optimal set, and the parameter values where a rank is attained there, can be described by a first-order formula over the reals, and then eliminating the quantifiers. Mathlib has no Tarski–Seidenberg theorem, and the one-variable structure theorem for semi-algebraic sets (milestone 9) is itself missing.

A second difficulty is the parametric duality: strict feasibility is assumed only at ϵ=0\epsilon=0ϵ=0, and propagating it to all of int⁡(E)\operatorname{int}(\mathcal E)int(E) (Remark 1) uses a theorem of the alternative for SDO.

Formalization scope

Matrices are Matrix (Fin n) (Fin n) ℝ; X⪰0X\succeq0X⪰0 is PosSemidef (which includes symmetry) and X≻0X\succ0X≻0 is PosDef. Symmetry of AiA^iAi, CCC, Cˉ\bar CCˉ is a hypothesis of every theorem, as are Assumptions 1–2. The optimal value vvv is an EReal infimum over P\mathcal PP, so v=−∞v=-\inftyv=−∞ is represented faithfully and E\mathcal EE is not a junk set. D∗(ϵ)\mathcal D^*(\epsilon)D∗(ϵ) compares bTyb^TybTy with the primal value v(ϵ)v(\epsilon)v(ϵ), as printed. The relative interior is Mathlib's intrinsicInterior. Definition 1 lets X∗(ϵ)X^*(\epsilon)X∗(ϵ) be any maximally complementary solution. The formalization removes this choice by taking the supremum of ranks over relative-interior points, and milestone 5 shows that every such point has that rank. S(θ,σ)\mathcal S_{(\theta,\sigma)}S(θ,σ)​ uses the relative interior of the product, as printed. A subset of R\mathbb RR is semi-algebraic when its copy in R1\mathbb R^1R1 is a finite union of sets {p=0, g<0}\{p=0,\ g<0\}{p=0, g<0} with real polynomials.

Trivializing formalizations are excluded:

  • ranks are taken at relative-interior points only, never at arbitrary optimal points;
  • vvv is an extended-real infimum, never a real sInf (which would make an unbounded problem look finite with value 000);
  • transition points are defined by Definition 5 itself, not as boundary points of S(θ,σ)\mathcal S_{(\theta,\sigma)}S(θ,σ)​.

The paper also states that E\mathcal EE is closed. Under Assumptions 1–2 this is false: n=2n=2n=2, m=1m=1m=1, A1=diag⁡(1,0)A^1=\operatorname{diag}(1,0)A1=diag(1,0), b=1b=1b=1, C=(0111)C=\begin{pmatrix}0&1\\1&1\end{pmatrix}C=(01​11​), Cˉ=diag⁡(0,1)\bar C=\operatorname{diag}(0,1)Cˉ=diag(0,1) gives E=(−1,∞)\mathcal E=(-1,\infty)E=(−1,∞). Milestone 2 omits closedness. The paper's proof of Theorem 1 does not use it.

Contributions welcome: proofs of any milestone; a semi-algebraic toolkit in Lean (closure under Boolean operations, projections from RN+1\mathbb R^{N+1}RN+1 to R\mathbb RR, the one-dimensional structure theorem); conic duality for standard-form SDO.

Selected references

  • J. D. Hauenstein, A. Mohammad-Nezhad, T. Tang, T. Terlaky, On computing the nonlinearity interval in parametric semidefinite optimization, Mathematics of Operations Research, 2022. arXiv:1908.10499v3
  • A. Mohammad-Nezhad, T. Terlaky, Parametric analysis of semidefinite optimization, Optimization 69 (2020), 187–216.
  • I. Adler, R. D. C. Monteiro, A geometric view of parametric linear programming, Algorithmica 8 (1992), 161–176.
  • D. Goldfarb, K. Scheinberg, On parametric semidefinite programming, Applied Numerical Mathematics 29 (1999), 361–377.
  • S. Basu, R. Pollack, M.-F. Roy, Algorithms in Real Algebraic Geometry, Springer, 2006.
  • R. T. Rockafellar, Convex Analysis, Princeton University Press, 1970.
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Operations ResearchOptimization·Captain: mikedeng1

Optimal Use and Replenishment of Two Substitutable Raw Materials in a Stochastic Capacitated Make-to-Order Production System: A Use-Down-To/Balancing Production Policy Is OptimalResearch Paper

Motivation

Make-to-order manufacturers may use two substitutable raw materials to satisfy demand when production capacity and material deliveries are uncertain. A cheaper material may yield less finished product per unit, and the firm must decide how much of each material to preserve for later periods. A production rule based only on current unit costs can be wrong because using one material changes the inventory state from which future orders and production will be chosen. Chen, Duenyas, and Jasin study this coupled replenishment and production problem and characterize the form of an optimal production decision. Their result gives a state-dependent rule described by four curves, rather than requiring a separate optimization for every inventory state. This mission formalizes that production result from the 2016 working-paper version of their study.

Setting

There are T≥1T\ge1T≥1 periods and two substitutable materials. A unit of finished product requires aj>0a^j>0aj>0 units of type-jjj material, with a1<a2a^1<a^2a1<a2. Before production in period ttt, the available material is a vector yt=(yt1,yt2)∈R+2y_t=(y_t^1,y_t^2)\in\mathbb R_+^2yt​=(yt1​,yt2​)∈R+2​. Demand DtD_tDt​ and production capacity RtR_tRt​ are nonnegative random quantities with finite support. A unit of satisfied demand earns revenue ete_tet​; a unit of lost demand incurs penalty σt>0\sigma_t>0σt​>0. Holding costs are htjh_t^jhtj​ and material purchasing costs are ctjc_t^jctj​. Ordered amounts are limited by random availabilities qtjq_t^jqtj​, whose finite supports may include +∞+\infty+∞.

The production decision is the remaining inventory wtw_twt​ after material use. The feasible set E2(yt,Dt,Rt)E_2(y_t,D_t,R_t)E2​(yt​,Dt​,Rt​) contains vectors satisfying 0≤wt≤yt0\le w_t\le y_t0≤wt​≤yt​, the demand limit, and the capacity limit:

a1wt1+a2wt2≥a1yt1+a2yt2−Dt,wt1+wt2≥yt1+yt2−Rt.a^1w_t^1+a^2w_t^2\ge a^1y_t^1+a^2y_t^2-D_t,\qquad w_t^1+w_t^2\ge y_t^1+y_t^2-R_t.a1wt1​+a2wt2​≥a1yt1​+a2yt2​−Dt​,wt1​+wt2​≥yt1​+yt2​−Rt​.

The objective Jt(wt)J_t(w_t)Jt​(wt​) adds the current cost coefficients (ajpt+htj−ct+1j)wtj(a^jp_t+h_t^j-c_{t+1}^j)w_t^j(ajpt​+htj​−ct+1j​)wtj​, where pt=et+σtp_t=e_t+\sigma_tpt​=et​+σt​, to the next-period value Vt+1(wt)V_{t+1}(w_t)Vt+1​(wt​). The value functions are determined backward from VT+1(x)=cT+11x1+cT+12x2V_{T+1}(x)=c_{T+1}^1x^1+c_{T+1}^2x^2VT+1​(x)=cT+11​x1+cT+12​x2 by the production and replenishment equations (1)–(5). Thus JtJ_tJt​ is an object computed from the model data and the dynamic program. These definitions follow §3 of the working paper.

Formalization targets

Optimal production rule

The goal is Theorem 1, pp. 15–16. There are two nonincreasing switching curves γt1,γt2\gamma_t^1,\gamma_t^2γt1​,γt2​ and two balancing curves αt,βt\alpha_t,\beta_tαt​,βt​ meeting at wˉt\bar w_twˉt​. Together they define the use-down-to and balancing (UB) rule of Definition 1. For every nonnegative D,RD,RD,R and every y∈R+2y\in\mathbb R_+^2y∈R+2​, the prescribed decision is feasible and optimal:

wt∗(y,D,R)∈arg min⁡w∈E2(y,D,R)Jt(w).w_t^*(y,D,R)\in\operatorname*{arg\,min}_{w\in E_2(y,D,R)}J_t(w).wt∗​(y,D,R)∈w∈E2​(y,D,R)argmin​Jt​(w).

The goal also includes the theorem's four minimization characterizations: wˉt\bar w_twˉt​ minimizes JtJ_tJt​ on the whole nonnegative orthant; each γtj\gamma_t^jγtj​ minimizes a one-coordinate section; αt(x)\alpha_t(x)αt​(x) minimizes on a1w1+a2w2=xa^1w^1+a^2w^2=xa1w1+a2w2=x; and βt(x)\beta_t(x)βt​(x) minimizes on w1+w2=xw^1+w^2=xw1+w2=x, for every x≥0x\ge0x≥0. The milestones retain Lemma 3(a), Lemma 3(d), the backward-induction claim for HtH_tHt​, Proposition 1 for the strictly convex perturbation, and Proposition 2 for the limiting policy.

Significance

The theorem identifies which material-use rule solves the production stage for any observed demand, capacity, and inventory. Its curves are independent of that period's realized DDD and RRR; those realizations enter the region boundaries and the rule's arguments. This structure supports the paper's later ordering-policy and computational work without replacing the original dynamic program with an unrelated one. The same formal definitions of feasible production, finite-support expectations, and coordinatewise value-function structure can be reused in other two-resource inventory models.

The working paper proves the result mathematically; the requested machine-checked work is to prove the Lean statements. The present proposal supplies definitions and theorem targets with sorry proof bodies. It does not claim that Theorem 1 or its milestones already have Lean proofs. A completed development would connect the backward dynamic program to the curve characterization and then prove that the region-specific action is optimal.

Difficulty

The replenishment-stage objective GtG_tGt​ is generally neither convex nor supermodular even when the subsequent value function has those properties, as the paper notes after Lemma 3. Consequently, taking a minimum in the replenishment recursion does not preserve the desired shape by an immediate standard argument. At the production stage, demand and capacity impose different coupled linear constraints on the two materials. Minimizing each material coordinate separately therefore does not produce a feasible or optimal decision in general. The source's region boundaries must account for which of these constraints binds and for their changes at D=a1RD=a^1RD=a1R and D=a2RD=a^2RD=a2R.

Formalization scope

Lean uses R×R\mathbb R\times\mathbb RR×R with componentwise order for two-material vectors. Each random quantity is a finite support with nonnegative real weights summing to one; expectations are finite sums. The two availability laws are multiplied as independent laws at each period, and +∞+\infty+∞ availability is represented by WithTop ℝ. The joint law of (Dt,Rt)(D_t,R_t)(Dt​,Rt​) need not factor. The dynamic program has periods 1,…,T1,\ldots,T1,…,T, and the terminal value is set at T+1T+1T+1. Its minima are defined as infima of feasible objective images; attainment is content of the results, not part of the definitions. Lower-growth claims use eventual real inequalities for every positive error, with the other inventory coordinate fixed and nonnegative.

The paper describes revenues and costs as monetary amounts and uses sign conditions in its proof of Lemma 3. The Lean standing predicate makes explicit et,htj,ctj≥0e_t,h_t^j,c_t^j\ge0et​,htj​,ctj​≥0, ctj+htj>0c_t^j+h_t^j>0ctj​+htj​>0, aj>0a^j>0aj>0, and T>0T>0T>0, in addition to the paper's σt>0\sigma_t>0σt​>0 and a1<a2a^1<a^2a1<a2. These assumptions are disclosed because without them the stated coercivity and attainment claims may fail. The objective in the goal is precisely JtJ_tJt​ produced by the full backward recursion; allowing an arbitrary objective with assumed structural properties would omit the dynamic-programming content.

Definition 1 calls its six regions a partition. At D≤a1RD\le a^1RD≤a1R, two printed regions can overlap; a concrete Lean check is included locally. The formal policy follows the page's displayed order when more than one region matches. Region coverage is asserted for all nonnegative D,RD,RD,R, and pairwise disjointness is asserted only when a1R<Da^1R<Da1R<D. The first-match convention and corrected partition claim are documented with the counterexample for review. The piecewise formulas for KjK^jKj, LjL^jLj, and γˉj\bar\gamma^jγˉ​j retain their source inequalities. Contributions establishing feasibility, curve existence, uniqueness for the perturbed problem, and the induction step are all useful to the mission.

Selected references

  • Q. Chen, I. Duenyas, and S. Jasin, Optimal Use and Replenishment of Two Substitutable Raw Materials in a Nonstationary Capacitated Make-to-Order Production System, SSRN working paper 2801786, version of 2016-06-28. SSRN.
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Machine LearningOptimizationRandom Matrix Theory+1·Captain: mikedeng1

Nonconvex Low-Rank Tensor Completion from Noisy Data: Spectrally Initialized Vanilla Gradient Descent Recovers the Tensor Factors at a Linear Rate to Near-Optimal ℓ2 and ℓ2,∞ AccuracyResearch Paper

Motivation

A partially observed array with three indices appears when data record relationships among triples of objects. If its entries have a low-rank structure, one can hope to recover the full array from far fewer than d3d^3d3 measurements. Cai, Li, Poor and Chen study this problem when the measurements are noisy and only a random subset of entries is seen. Their result gives a statistical error bound for a concrete two-stage method: spectral initialization followed by ordinary gradient descent on a nonconvex loss. It is a known theorem, proved in the pinned preprint, rather than an open conjecture.

Setting

The unknown symmetric order-three tensor is T⋆∈Rd×d×dT^\star\in\mathbb R^{d\times d\times d}T⋆∈Rd×d×d. It has a CP decomposition T⋆=∑s=1r(us⋆)⊗3T^\star=\sum_{s=1}^r(u_s^\star)^{\otimes3}T⋆=∑s=1r​(us⋆​)⊗3, where the nonzero columns us⋆u_s^\starus⋆​ form U⋆∈Rd×rU^\star\in\mathbb R^{d\times r}U⋆∈Rd×r. Each unordered triple of coordinates is sampled independently with probability ppp; its six permutations share one sampling decision. On a sampled triple the observation is Tijk⋆+EijkT^\star_{ijk}+E_{ijk}Tijk⋆​+Eijk​, with symmetric, centered, independent sub-Gaussian noise of variance at most σ2\sigma^2σ2. The observed tensor TTT vanishes outside the sampled set Ω\OmegaΩ.

For a candidate factor matrix U=[u1,…,ur]U=[u_1,\ldots,u_r]U=[u1​,…,ur​], the objective is

f(U)=16p∥PΩ ⁣(∑s=1rus⊗3−T)∥F2.f(U)=\frac{1}{6p}\left\|P_\Omega\!\left(\sum_{s=1}^r u_s^{\otimes3}-T\right)\right\|_F^2.f(U)=6p1​​PΩ​(s=1∑r​us⊗3​−T)​F2​.

Algorithm 2 obtains a leading rrr-dimensional eigenspace from an off-diagonal Gram matrix of the mode-one unfolding of p−1Tp^{-1}Tp−1T. Algorithm 3 uses Gaussian restarts, leading singular vectors, and greedy pruning to turn that subspace into a factor matrix U0U^0U0. Algorithm 1 then applies the gradient step to fff. Eigenvalue ties, leading singular-vector choices, and pruning ties can produce several admissible executions; the result concerns every execution.

Incoherence μ\muμ measures how evenly the tensor and factors spread across coordinates and how nearly orthogonal distinct factors are. The condition number κ\kappaκ is the ratio of the largest to smallest factor norm. Write λmin⁡⋆=min⁡s∥us⋆∥23\lambda^\star_{\min}=\min_s\|u_s^\star\|_2^3λmin⋆​=mins​∥us⋆​∥23​ and λmax⁡⋆=max⁡s∥us⋆∥23\lambda^\star_{\max}=\max_s\|u_s^\star\|_2^3λmax⋆​=maxs​∥us⋆​∥23​. Distances dist⁡F\operatorname{dist}_FdistF​, dist⁡∞\operatorname{dist}_\inftydist∞​, and dist⁡2,∞\operatorname{dist}_{2,\infty}dist2,∞​ minimize their respective matrix norms over permutations of the rrr columns.

Formalization targets

The goal is Theorem 2.4, in the bounded-rank, bounded-incoherence, bounded-condition-number regime. Under its printed sampling, noise, restart, threshold and step-size conditions, for every 0≤t≤d50\le t\le d^50≤t≤d5 it asserts, with probability at least 1−δ1-\delta1−δ,

dist⁡F(Ut,U⋆)≤(C1ρt+C2σλmin⁡⋆dlog⁡dp)∥U⋆∥F,\operatorname{dist}_F(U^t,U^\star)\le\left(C_1\rho^t+C_2\frac{\sigma}{\lambda^\star_{\min}}\sqrt{\frac{d\log d}{p}}\right)\|U^\star\|_F,distF​(Ut,U⋆)≤(C1​ρt+C2​λmin⋆​σ​pdlogd​​)∥U⋆∥F​, dist⁡∞(Ut,U⋆)≤dist⁡2,∞(Ut,U⋆)≤(C3ρt+C4σλmin⁡⋆dlog⁡dp)∥U⋆∥2,∞.\operatorname{dist}_\infty(U^t,U^\star)\le\operatorname{dist}_{2,\infty}(U^t,U^\star)\le\left(C_3\rho^t+C_4\frac{\sigma}{\lambda^\star_{\min}}\sqrt{\frac{d\log d}{p}}\right)\|U^\star\|_{2,\infty}.dist∞​(Ut,U⋆)≤dist2,∞​(Ut,U⋆)≤(C3​ρt+C4​λmin⋆​σ​pdlogd​​)∥U⋆∥2,∞​.

The rate is fixed to ρ=1−λmin⁡⋆,4/3η/5\rho=1-\lambda_{\min}^{\star,4/3}\eta/5ρ=1−λmin⋆,4/3​η/5, consistent with the paper's local-convergence lemmas. Milestones formalize the gradient identity (36), local Hessian bounds (Lemma 5.1), spectral-subspace recovery (Lemma 5.7), factor retrieval (Theorem 5.9), and the paper's general-parameter recovery theorem (Theorem 2.8). The latter makes the dependence on μ\muμ and rrr explicit.

Significance

The inequalities give two guarantees at once: geometric reduction of initialization error and an explicit noise floor. The 2,∞2,\infty2,∞ bound controls the error in each coordinate row, which a Frobenius estimate alone does not supply. Together with the tensor-entry corollaries in the paper, they explain the accuracy of this practical nonconvex method under random subsampling. The authors also specify how the sample probability, noise level, rank and incoherence interact, so the result can be compared to other tensor-completion methods.

This mission asks for a machine-checked version of the known result. Its published ψ₂ norm definition is reused; the paper-specific tensor model, spectral initialization relations, loss and gradient iteration are new. The theorem statements compile with sorry, so none of their proofs is claimed as machine checked here. Proofs of the listed milestones, the main theorem, and faithful auxiliary concentration results are welcome; the paper's numerical experiments are outside this formalization.

Difficulty

The gradient loss is nonconvex, so global convexity cannot justify the iteration bound. The local Hessian estimate applies only near U⋆U^\starU⋆ in both Frobenius and rowwise norm. A Frobenius estimate alone cannot establish the rowwise condition at every iteration. The spectral initializer must also select individual factors from a subspace despite nearly tied eigenvalues and noisy tensor contractions. These are the points where a direct appeal to standard smooth-gradient-descent theory stops short of the stated result.

Formalization scope

Coordinates are Fin d and Fin r, with zero-based indexing; the PDF uses one-based indices. All logarithms are natural. Tensor and matrix norms are explicit finite-coordinate Euclidean norms. Minima over permutations range over all permutations of Fin r, and maxima in the incoherence parameters range over the indices specified by Definition 2.1. Sampling is on sorted triples, then extended by symmetry. The probability model is a single probability space carrying the sampling indicators, noise variables and Gaussian restarts, jointly independent; the paper leaves some cross-family independence implicit. Noise has mean zero, variance at most σ2\sigma^2σ2, and ψ₂ norm at most σ\sigmaσ using the published extended-nonnegative norm. The last bound makes the paper's sub-Gaussian scale explicit.

The statements use d≥d0≥2d\ge d_0\ge2d≥d0​≥2, r≥1r\ge1r≥1, nonzero true factor columns, 0<p≤10<p\le10<p≤1, and σ≥0\sigma\ge0σ≥0. Theorems 2.8 and 5.9 use r≥2r\ge2r≥2 and round their real-valued restart count up to a natural number; this handles the boundary where log⁡r=0\log r=0logr=0. Theorem 2.4 places its claimed absolute error constants before the rank and incoherence bounds and all instance data. Probability is expressed as the outer measure of the bad event, since admissible-execution predicates quantify over choices and need not be measurable. Each good event explicitly asserts that an admissible execution exists before requiring the bounds for every execution; otherwise a failed pruning run would make a universal claim vacuous.

The remaining reusable infrastructure includes concentration for symmetric sampled tensors, finite-dimensional spectral perturbation with ties, and derivative estimates for the cubic factor map. The paper's leave-one-out iteration lemmas and their auxiliary estimators are not included in this initial milestone list; they remain natural contributions toward the full proof.

Selected references

  • C. Cai, G. Li, H. V. Poor and Y. Chen, Nonconvex Low-Rank Tensor Completion from Noisy Data, arXiv:1911.04436v2, 2021; published in Operations Research 70(2), 2022. Preprint.
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Definition 2.5.6 for the ψ₂ norm. Publisher DOI.
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Algebraic TopologyAlgorithmic Game TheoryTopology·Captain: mikedeng1

Equipartition of a Segment: Every Continuous Function on Subsegments of [0, 1] Vanishing on Degenerate Segments Takes Equal Values on Some Partition of [0, 1] into m SegmentsResearch Paper

Motivation

In fair division, a value may be assigned to each interval that a cut produces. If the value is continuous in the interval's endpoints, an equal-value partition is a natural target. Some valuations are nonnegative and additive, but a difference of competing measures or a signed utility need have neither property. Avvakumov and Karasev establish equal-value partitions even when the value changes sign and is not additive, provided it vanishes on degenerate intervals. Their result is used by Bogomolnaia and Moulin in work on guarantees for fair division. Avvakumov and Karasev, pp. 1–2; Bogomolnaia and Moulin.

The paper identifies earlier special cases: a nonnegative valuation follows from the Knaster–Kuratowski–Mazurkiewicz theorem; prime-power numbers of parts with a valuation of varying sign were known through degree-theoretic results; additive valuations admit an elementary argument. The remaining case permits a sign-changing, nonadditive valuation and an arbitrary positive number of parts. The authors distinguish this from an envy-free division problem with separate valuations for several players, which they state remains open outside prime-power cases. Avvakumov and Karasev, p. 2; Avvakumov and Karasev, Envy-free division using mapping degree; Meunier and Zerbib.

Setting

Write I\mathcal II for the set of all subsegments I=[a,b]I=[a,b]I=[a,b] of [0,1][0,1][0,1] with 0≤a≤b≤10\le a\le b\le10≤a≤b≤1. An interval may be degenerate, meaning a=ba=ba=b. A real-valued function fff on I\mathcal II is continuous when its value varies continuously with the two endpoints. The required boundary condition is f([a,a])=0f([a,a])=0f([a,a])=0 for every a∈[0,1]a\in[0,1]a∈[0,1]. No sign, monotonicity, or additivity condition is imposed. A partition into mmm parts is a sequence 0=x0≤x1≤⋯≤xm=10=x_0\le x_1\le\cdots\le x_m=10=x0​≤x1​≤⋯≤xm​=1, so its parts [xj−1,xj][x_{j-1},x_j][xj−1​,xj​] may also be degenerate. Avvakumov and Karasev, Theorem 1.1, pp. 1–2.

The intermediate setting is a nice multivalued function. Its graph is a compact subset ZZZ of I×(−1,1)\mathcal I\times(-1,1)I×(−1,1). The graph separates the bottom I×{−1}\mathcal I\times\{-1\}I×{−1} from the top I×{1}\mathcal I\times\{1\}I×{1} inside the cylinder C=I×[−1,1]C=\mathcal I\times[-1,1]C=I×[−1,1]: those two sides lie in different connected components of C∖ZC\setminus ZC∖Z. A representation of a nice graph is a continuous real function φ\varphiφ on CCC that is negative on the bottom, positive on the top, and whose zero set is the graph. The paper passes between graphs and representations in Lemma 2.2. Avvakumov and Karasev, Definition 2.1 and Lemma 2.2, p. 2.

For a prime ppp, a segment I=[a,b]I=[a,b]I=[a,b], and a value yyy, a zero partition is a sequence a=x0≤⋯≤xp=ba=x_0\le\cdots\le x_p=ba=x0​≤⋯≤xp​=b such that φ([xj−1,xj],y)=0\varphi([x_{j-1},x_j],y)=0φ([xj−1​,xj​],y)=0 for each j=1,…,pj=1,\ldots,pj=1,…,p. The set Zp(φ)Z_p(\varphi)Zp​(φ) contains exactly those pairs (I,y)(I,y)(I,y) that admit a zero partition. This is the projection to the cylinder of the paper's simultaneous-solution set SSS for labeled partitions. Avvakumov and Karasev, equation (4.1) and Claim 4.4, pp. 7–9.

Formalization targets

The goal is Theorem 1.1: for every positive integer mmm and every continuous fff satisfying the degenerate-interval condition, there are possibly repeated cut points with a common value:

0=x0≤x1≤⋯≤xm=1,f([x0,x1])=⋯=f([xm−1,xm]).0=x_0\le x_1\le\cdots\le x_m=1,\qquad f([x_0,x_1])=\cdots=f([x_{m-1},x_m]).0=x0​≤x1​≤⋯≤xm​=1,f([x0​,x1​])=⋯=f([xm−1​,xm​]).

The theorem is already posed as the Open platform statement FairGuarantees.DivideChoose.theorem_of_4; this mission references that exact statement as its goal. It supplies the paper's supporting statements, including Lemma 2.2 on graph representations, Claim 4.4 on separation by projected zero partitions, and the prime-step Lemma 2.3. The latter asserts that, when φ([a,a],y)=y\varphi([a,a],y)=yφ([a,a],y)=y, there is a represented nice graph with the same degenerate identity whose zeros each yield a zero partition for φ\varphiφ. The milestone list includes the fixed-segment and continuous-family statements used to characterize Zp(φ)Z_p(\varphi)Zp​(φ), and equation (4.2) describing its degenerate boundary. Avvakumov and Karasev, Lemmas 2.2–2.3, pp. 2–3; Claims 4.3–4.4 and equation (4.2), pp. 8–9.

Significance

The theorem guarantees equal values for any positive number of consecutive parts under only endpoint continuity and the zero-on-degenerates condition. It covers valuations for which nonnegative or additive special-case results give no conclusion. It also provides the theorem invoked in the fair-guarantee application cited by the authors. Avvakumov and Karasev, pp. 1–2; Bogomolnaia and Moulin.

The mathematical result was proved in the paper; the platform's theorem statement remains Open and lacks a machine-checked proof there. Formalizing the paper's intermediate claims makes its topological assumptions and its treatment of degenerate parts explicit. The definitions of a separating graph, its representation, and zero partitions can also be reused for related partition problems. The present mission states the paper's prime-step targets, leaving the proofs and the underlying equivariant topology as work for solvers.

Difficulty

For a fixed signed valuation, continuity alone does not select one common value that works across every piece of an arbitrary partition. The nonnegative case has a simplex-covering argument, but that argument does not directly control values of both signs. In the paper's general case, the difficult claim is that the projected simultaneous-zero set separates an entire cylinder, even as the segment varies. Its source proof requires a mod-ppp statement for a space of labeled partitions and control of the resulting solution set. A further boundary issue arises on degenerate segments: a representation of the projected graph must satisfy ψ([a,a],y)=y\psi([a,a],y)=yψ([a,a],y)=y, not merely have the right zeros. Avvakumov and Karasev, pp. 2, 7–10.

Formalization scope

Lean represents I=[a,b]I=[a,b]I=[a,b] by the endpoint pair (a,b)(a,b)(a,b) with 0≤a≤b≤10\le a\le b\le10≤a≤b≤1. The cylinder uses the closed value range [−1,1][-1,1][−1,1]; a nice graph lies in its open interior (−1,1)(-1,1)(−1,1). Functions are total Lean functions, but only their values on this cylinder enter the definitions and results. Continuity is required on the cylinder. Separation uses connected components of its complement, as in Definition 2.1, and explicitly requires the bottom and top to avoid the graph. This prevents a graph containing a boundary side from satisfying separation vacuously.

Every prime-step claim assumes ppp prime, the representation's strict boundary signs, and the degenerate identity. Zero partitions have exactly ppp consecutive parts whose endpoints are pinned to the original segment; repeated cuts are allowed. The goal reference likewise permits degenerate parts and assumes m≥1m\ge1m≥1. The projected set is defined through existence of an ordinary ordered partition, independent of how the paper labels partitions in its configuration space. The needed existing Lean notions include ContinuousOn, IsCompact, connectedComponentIn, finite index types, and Nat.Prime. A complete proof development also needs results about the paper's labeled-partition complex, equivariant cycles and transverse maps. Contributions establishing that reusable topology, as well as proofs of the stated milestones, are within scope. Avvakumov and Karasev, §§2–4.

Selected references

  • Sergey Avvakumov and Roman Karasev, Equipartition of a Segment, Mathematics of Operations Research, 2023. arXiv:2009.09862v4.
  • Anna Bogomolnaia and Hervé Moulin, Guarantees in Fair Division: General or Monotone Preferences, 2019. arXiv:1911.10009v3.
  • Sergey Avvakumov and Roman Karasev, Envy-Free Division Using Mapping Degree, Mathematika 67, 2021. arXiv:1907.11183.
  • Frédéric Meunier and Shira Zerbib, Envy-Free Cake Division Without Assuming the Players Prefer Nonempty Pieces, Israel Journal of Mathematics 234, 2019. arXiv:1804.00449.
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Graph TheoryOperations ResearchProbability·Captain: mikedeng1

A Dynamic Contagion Risk Model with Recovery Features: Fluid Limit for the Final Fraction of Failed Nodes in Threshold Contagion with Growth on the Configuration ModelResearch Paper

Motivation

Financial networks, supply chains and contact networks share a failure mode: a node fails when enough of its counterparties have failed, and its failure in turn weakens its own counterparties. Threshold contagion on random graphs is the standard mathematical model of this. Amini, Cont and Minca (Resilience to contagion in financial networks, Mathematical Finance 2016) proved that on a configuration-model network the final fraction of failed nodes concentrates, as the network grows, around an explicit value determined by the smallest fixed point of a one-dimensional map.

In that model thresholds are fixed. In practice institutions recover while a crisis unfolds: capital is raised, earnings accrue, and a node that survives long enough can absorb more losses than at the start. Amini, Minca and Sulem (A Dynamic Contagion Risk Model with Recovery Features, Mathematics of Operations Research 2022; the mission follows the authors' preprint of February 2021) add this recovery feature: every surviving node's threshold grows linearly in calendar time, at a rate proportional to its connectivity. The main result, Theorem 5, identifies the scaling limit of the cascade with growth. It is the basis of the paper's analysis of equilibrium connectivity choice (§3), where agents trade off the rewards of links against contagion risk.

Setting

A network has nnn nodes. Node iii has a connectivity λi∈N\lambda_i\in\mathbb Nλi​∈N (in-degree and out-degree both equal λi\lambda_iλi​) and an integer initial threshold θi∈N\theta_i\in\mathbb Nθi​∈N. The empirical type distribution is μλ,θ(n)=#{i:θi=θ,λi=λ}/n\mu^{(n)}_{\lambda,\theta}=\#\{i:\theta_i=\theta,\lambda_i=\lambda\}/nμλ,θ(n)​=#{i:θi​=θ,λi​=λ}/n and the mean connectivity is λˉ(n)=∑λ,θλμλ,θ(n)\bar\lambda^{(n)}=\sum_{\lambda,\theta}\lambda\mu^{(n)}_{\lambda,\theta}λˉ(n)=∑λ,θ​λμλ,θ(n)​. Two regularity conditions are assumed: (C1) μλ,θ(n)→μλ,θ\mu^{(n)}_{\lambda,\theta}\to\mu_{\lambda,\theta}μλ,θ(n)​→μλ,θ​ for a probability distribution μ\muμ on N2\mathbb N^2N2; (C2) λˉ(n)→λˉ=∑λμλ,θ∈(0,∞)\bar\lambda^{(n)}\to\bar\lambda=\sum\lambda\mu_{\lambda,\theta}\in(0,\infty)λˉ(n)→λˉ=∑λμλ,θ​∈(0,∞).

Each node owns λi\lambda_iλi​ out-going and λi\lambda_iλi​ in-coming half-edges. The directed configuration model matches out-half-edges to in-half-edges by a uniformly random bijection; self-loops and multiple links are allowed.

The cascade: at time 000 the nodes with θi=0\theta_i=0θi​=0 fail. Interactions happen at times Tk(n)T^{(n)}_kTk(n)​ whose gaps are i.i.d. exponential with rate nnn. At each interaction one unrevealed out-link of a failed node, chosen uniformly, is revealed; its counterparty jjj gains one failed link and fails if its count of failed links reaches its current threshold θj+αλjTk(n)/λˉ(n)\theta_j+\alpha\lambda_jT^{(n)}_k/\bar\lambda^{(n)}θj​+αλj​Tk(n)​/λˉ(n), where 0<α<10<\alpha<10<α<1 is the growth rate. Only surviving nodes grow. The cascade stops at kstop(n)k^{(n)}_{\rm stop}kstop(n)​, when no unrevealed failed link remains; ∣Df(n)∣|\mathcal D^{(n)}_f|∣Df(n)​∣ is the number of failed nodes and Sλ,θ(n)(kstop(n))S^{(n)}_{\lambda,\theta}(k^{(n)}_{\rm stop})Sλ,θ(n)​(kstop(n)​) the number of survivors of type (λ,θ)(\lambda,\theta)(λ,θ).

The limit objects: Pλ,θ,ℓ(π)P_{\lambda,\theta,\ell}(\pi)Pλ,θ,ℓ​(π) is the probability that the order statistics of ℓ\ellℓ i.i.d. uniform variables on [0,π][0,\pi][0,π] satisfy U(u)>(u−θ)/(αλ)U_{(u)}>(u-\theta)/(\alpha\lambda)U(u)​>(u−θ)/(αλ) for u=θ+1,…,ℓu=\theta+1,\dots,\ellu=θ+1,…,ℓ; Bλ,0α=1B^\alpha_{\lambda,0}=1Bλ,0α​=1 and, for θ≥1\theta\ge1θ≥1,

Bλ,θα(π)=1−∑ℓ=0min⁡{⌈θ+αλπ⌉−1,λ}(λℓ)πℓ(1−π)λ−ℓPλ,θ,ℓ(π);B^\alpha_{\lambda,\theta}(\pi)=1-\sum_{\ell=0}^{\min\{\lceil\theta+\alpha\lambda\pi\rceil-1,\lambda\}}\binom{\lambda}{\ell}\pi^\ell(1-\pi)^{\lambda-\ell}P_{\lambda,\theta,\ell}(\pi);Bλ,θα​(π)=1−ℓ=0∑min{⌈θ+αλπ⌉−1,λ}​(ℓλ​)πℓ(1−π)λ−ℓPλ,θ,ℓ​(π);

Jα(π)=∑λ,θλμλ,θBλ,θα(π)/λˉJ^\alpha(\pi)=\sum_{\lambda,\theta}\lambda\mu_{\lambda,\theta}B^\alpha_{\lambda,\theta}(\pi)/\bar\lambdaJα(π)=∑λ,θ​λμλ,θ​Bλ,θα​(π)/λˉ; and the relaxed fixed point π∗=min⁡{π∈[0,1]:Jα(π)≤π}\pi^*=\min\{\pi\in[0,1]:J^\alpha(\pi)\le\pi\}π∗=min{π∈[0,1]:Jα(π)≤π}.

Formalization targets

Goal: Theorem 5 (corrected)

With L=∑λ,θμλ,θBλ,θα(π∗)L=\sum_{\lambda,\theta}\mu_{\lambda,\theta}B^\alpha_{\lambda,\theta}(\pi^*)L=∑λ,θ​μλ,θ​Bλ,θα​(π∗): for every ε>0\varepsilon>0ε>0, with high probability ∣Df(n)∣/n≥L−ε|\mathcal D^{(n)}_f|/n\ge L-\varepsilon∣Df(n)​∣/n≥L−ε. (i) If π∗=1\pi^*=1π∗=1 and μ0,θ=0\mu_{0,\theta}=0μ0,θ​=0 for θ≥1\theta\ge1θ≥1, then ∣Df(n)∣/n→1|\mathcal D^{(n)}_f|/n\to1∣Df(n)​∣/n→1 in probability. (ii) If π∗<1\pi^*<1π∗<1 is a stable fixed point (Jα(π)<πJ^\alpha(\pi)<\piJα(π)<π just to the right of π∗\pi^*π∗), then

∣Df(n)∣n→pL,Sλ,θ(n)(kstop(n))n→pμλ,θ(1−Bλ,θα(π∗)).\frac{|\mathcal D^{(n)}_f|}{n}\xrightarrow{p}L,\qquad\frac{S^{(n)}_{\lambda,\theta}(k^{(n)}_{\rm stop})}{n}\xrightarrow{p}\mu_{\lambda,\theta}\big(1-B^\alpha_{\lambda,\theta}(\pi^*)\big).n∣Df(n)​∣​p​L,nSλ,θ(n)​(kstop(n)​)​p​μλ,θ​(1−Bλ,θα​(π∗)).

Milestones

  1. Lemma 16: a recursion in ℓ\ellℓ for Pλ,θ,ℓ(t)P_{\lambda,\theta,\ell}(t)Pλ,θ,ℓ​(t), for 0<α<10<\alpha<10<α<1 and θ<ℓ≤λ\theta<\ell\le\lambdaθ<ℓ≤λ, valid for t≥t^λ,θ,ℓ=(ℓ−θ)λˉ/(αλ)t\ge\hat t_{\lambda,\theta,\ell}=(\ell-\theta)\bar\lambda/(\alpha\lambda)t≥t^λ,θ,ℓ​=(ℓ−θ)λˉ/(αλ).
  2. Lemma 15: for 0<α<10<\alpha<10<α<1 and 0<θ≤λ0<\theta\le\lambda0<θ≤λ, the piecewise linear system (DE) for the rescaled numbers of surviving nodes with ℓ\ellℓ failed links has a unique continuous solution on [0,λˉ)[0,\bar\lambda)[0,λˉ), in closed form.
  3. (24)–(25): the limiting failed fraction of a class is μλ,θBλ,θα(t/λˉ)\mu_{\lambda,\theta}B^\alpha_{\lambda,\theta}(t/\bar\lambda)μλ,θ​Bλ,θα​(t/λˉ), and the limiting number of unrevealed failed links is λˉ(Jα(t/λˉ)−t/λˉ)\bar\lambda(J^\alpha(t/\bar\lambda)-t/\bar\lambda)λˉ(Jα(t/λˉ)−t/λˉ).
  4. (27)–(28): for k=γλˉ(n)n+o(n)k=\gamma\bar\lambda^{(n)}n+o(n)k=γλˉ(n)n+o(n), Tk(n)→γλˉT^{(n)}_k\to\gamma\bar\lambdaTk(n)​→γλˉ in probability.
  5. Remark 6: the minimum defining π∗\pi^*π∗ is attained.

Significance

Theorem 5 gives the final size of a cascade with recovery as an explicit function of the type distribution and the growth rate. The paper uses it to define each agent's expected reward as a function of its connectivity and to study the equilibrium of the resulting connectivity game (§3). Without the theorem, the equilibrium analysis would rest on the heuristic of §2.3 alone.

On the formal side, the platform has no random graph model of configuration type, no network contagion process and no fluid limit of a random cascade. This mission introduces all three. The result is proved on paper (by Wormald's differential-equation method); none of it is machine-checked. The work is to formalize the proof, and the milestones are self-contained pieces of it: an order-statistic identity, an explicit ODE solution, an algebraic identification of the limit, a concentration bound for sums of exponentials, and a fixed-point existence result.

Difficulty

The obvious approach is to view the cascade as a Markov chain in the counts of surviving nodes by type and number of failed links, and to apply Wormald's theorem directly. Two things break. First, with growth a node's survival depends on the whole history of its failed-link count, not on its current value, so the state space grows with time: new states become relevant at each growth time t^λ,θ,ℓ\hat t_{\lambda,\theta,\ell}t^λ,θ,ℓ​, and the fluid limit has to be established inductively on successive time intervals. Second, the cascade stops at a random time, near the first zero of the limiting number of unrevealed failed links. Showing that the stopping time concentrates requires the stability condition on π∗\pi^*π∗ and a truncation of the type distribution in the degree, since μ\muμ may have infinite support. The fixed point need not be a crossing point of a smooth map, so the identification of the stopping time is delicate even when the drift is known.

Formalization scope

  • Network. Half-edges of node iii are pairs (i,a)(i,a)(i,a) with a<λia<\lambda_ia<λi​; the matching is a uniformly random permutation of the half-edges. Each nnn has its own probability space: the matching, m=nλˉ(n)m=n\bar\lambda^{(n)}m=nλˉ(n) i.i.d. Exp(n)\mathrm{Exp}(n)Exp(n) gaps, and mmm i.i.d. uniform variables on [0,1)[0,1)[0,1) that choose the revealed link (uniform among the available ones given the past). The probability of an event averages over permutations the product law of gaps and choices. "With high probability" and "in probability" are stated with explicit ε\varepsilonε and limits of these probabilities.
  • Cascade. Computed step by step from the randomness and run for mmm steps; ∣Df(n)∣|\mathcal D^{(n)}_f|∣Df(n)​∣ and Sλ,θ(n)(kstop)S^{(n)}_{\lambda,\theta}(k_{\rm stop})Sλ,θ(n)​(kstop​) are read off the final state. A node fails when its failed links reach (not exceed) its threshold, as in every formula of the paper. Initially failed nodes are those with θi=0\theta_i=0θi​=0.
  • Limit objects. Order statistics are encoded by counting (U(u)>sU_{(u)}>sU(u)​>s iff fewer than uuu variables are ≤s\le s≤s), and probabilities as Lebesgue measures of subsets of [0,π]ℓ[0,\pi]^\ell[0,π]ℓ. Sums over types are tsums with summability hypotheses; μ\muμ is nonnegative with total mass 111.
  • Corrections, all labelled. (a) Bλ,0α:=1B^\alpha_{\lambda,0}:=1Bλ,0α​:=1; the printed formula gives a value below 111 for π>0\pi>0π>0, contradicting the paper's p. 9, and makes the theorem false. (b) Part (i) assumes no isolated nodes with a positive threshold. (c) Lemma 16 assumes t≥t^λ,θ,ℓt\ge\hat t_{\lambda,\theta,\ell}t≥t^λ,θ,ℓ​. (d) Lemma 15 is stated for 0<θ≤λ0<\theta\le\lambda0<θ≤λ, with uniqueness among continuous solutions, and reads the printed λˉ−u\bar\lambda-uλˉ−u as λˉ−t\bar\lambda-tλˉ−t. (e) (24) ends in μλ,θBλ,θα(t/λˉ)\mu_{\lambda,\theta}B^\alpha_{\lambda,\theta}(t/\bar\lambda)μλ,θ​Bλ,θα​(t/λˉ), not μλ,θ(1−Bλ,θα(t/λˉ))\mu_{\lambda,\theta}(1-B^\alpha_{\lambda,\theta}(t/\bar\lambda))μλ,θ​(1−Bλ,θα​(t/λˉ)). "Stable fixed point" means Jα(π)<πJ^\alpha(\pi)<\piJα(π)<π on some interval (π∗,π∗+η)(\pi^*,\pi^*+\eta)(π∗,π∗+η).
  • No trivialization. ∣Df(n)∣|\mathcal D^{(n)}_f|∣Df(n)​∣ and Sλ,θ(n)S^{(n)}_{\lambda,\theta}Sλ,θ(n)​ are computed from the random matching, the gaps and the revelation order, never from BαB^\alphaBα or JαJ^\alphaJα; π∗\pi^*π∗ is defined from μ\muμ and α\alphaα, not taken as a parameter.
  • Not included. Theorem 3 (the case α=0\alpha=0α=0, cited from earlier work), the equilibrium results of §3, Wormald's theorem (Lemma 17, an external result), the in/out-degree extension (Theorem 18) and the displays (32)–(41) of the inductive argument.
  • Infrastructure. A complete proof needs Wormald's differential-equation method for Markov chains with bounded increments, concentration of the configuration model, and the elementary facts in the milestones. A general Wormald theorem and the configuration model are reusable well beyond this mission; contributions of either, as separate theorems, are welcome.

Selected references

  • H. Amini, A. Minca, A. Sulem, A dynamic contagion risk model with recovery features, Mathematics of Operations Research, 2022 (preprint February 2021). https://doi.org/10.1287/moor.2021.1174
  • H. Amini, R. Cont, A. Minca, Resilience to contagion in financial networks, Mathematical Finance, 2016. https://doi.org/10.1111/mafi.12051
  • N. C. Wormald, Differential equations for random processes and random graphs, Annals of Applied Probability, 1995. https://doi.org/10.1214/aoap/1177004612
  • L. Warnke, On Wormald's differential equation method, arXiv:1905.08928, 2019. https://arxiv.org/abs/1905.08928
  • B. Bollobás, A probabilistic proof of an asymptotic formula for the number of labelled regular graphs, European Journal of Combinatorics, 1980. https://doi.org/10.1016/S0195-6698(80)80030-8
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Machine LearningMarkov ChainOperations Research+1·Captain: mikedeng1

Learning Markov Models Via Low-Rank Optimization: KL Error Bound for the Rank-Constrained Maximum Likelihood Estimator of a Low-Rank Markov ChainResearch Paper

Motivation

Many systems studied in operations research and reinforcement learning are modelled as finite Markov chains with a large number of states ppp: the stops of a taxi in a city, a random walk on a network, the conformations of a molecule. Estimating the p×pp\times pp×p transition matrix from one observed trajectory needs, in general, a trajectory long compared with the p2p^2p2 unknown entries. In many such systems the transition matrix has, at least approximately, a small rank r≪pr\ll pr≪p: the observed chain is driven by a low-dimensional latent process, as in state aggregation, where P(st+1∣st)=∑zP(zt=z∣st) P(st+1∣zt=z)\mathbb P(s_{t+1}\mid s_t)=\sum_z\mathbb P(z_t=z\mid s_t)\,\mathbb P(s_{t+1}\mid z_t=z)P(st+1​∣st​)=∑z​P(zt​=z∣st​)P(st+1​∣zt​=z) (Zhu, Li, Wang & Zhang, arXiv:1907.00113, §1.1). Zhu, Li, Wang and Zhang show that a low-rank transition matrix can be estimated from a trajectory whose length is proportional to ppp (up to logarithmic factors), and they give two maximum-likelihood estimators with explicit rates. This mission formalizes the rate of the second, rank-constrained, estimator in Kullback–Leibler divergence.

Setting

Let X0,X1,…,XnX_0,X_1,\dots,X_nX0​,X1​,…,Xn​ be a Markov chain on the states [p]={s1,…,sp}[p]=\{s_1,\dots,s_p\}[p]={s1​,…,sp​} with transition matrix PPP (Pij≥0P_{ij}\ge0Pij​≥0, ∑jPij=1\sum_jP_{ij}=1∑j​Pij​=1, Pij=P(X1=sj∣X0=si)P_{ij}=\mathbb P(X_1=s_j\mid X_0=s_i)Pij​=P(X1​=sj​∣X0​=si​)) and stationary distribution π\piπ (π⊤P=π⊤\pi^\top P=\pi^\topπ⊤P=π⊤). The chain is primitive (some power of PPP has all entries positive), and X0X_0X0​ is drawn from π\piπ. Write πmin⁡=min⁡jπj\pi_{\min}=\min_j\pi_jπmin​=minj​πj​ and πmax⁡=max⁡jπj\pi_{\max}=\max_j\pi_jπmax​=maxj​πj​.

The right spectral gap is 1−ρ+1-\rho_+1−ρ+​, where, with ⟨h1,h2⟩π=∑jh1jh2jπj\langle h_1,h_2\rangle_\pi=\sum_jh_{1j}h_{2j}\pi_j⟨h1​,h2​⟩π​=∑j​h1j​h2j​πj​ and the adjoint P∗=Diag(π)−1P⊤Diag(π)P^*=\mathrm{Diag}(\pi)^{-1}P^\top\mathrm{Diag}(\pi)P∗=Diag(π)−1P⊤Diag(π),

ρ+=sup⁡⟨h,1⟩π=0, ⟨h,h⟩π=112⟨(P+P∗)h,h⟩π.\rho_+=\sup_{\langle h,1\rangle_\pi=0,\ \langle h,h\rangle_\pi=1}\tfrac12\langle(P+P^*)h,h\rangle_\pi .ρ+​=⟨h,1⟩π​=0, ⟨h,h⟩π​=1sup​21​⟨(P+P∗)h,h⟩π​.

The KL divergence of a transition matrix QQQ from PPP is DKL(P,Q)=∑i,jπiPijlog⁡(Pij/Qij)1{Pij≠0}D_{\mathrm{KL}}(P,Q)=\sum_{i,j}\pi_iP_{ij}\log(P_{ij}/Q_{ij})1_{\{P_{ij}\ne0\}}DKL​(P,Q)=∑i,j​πi​Pij​log(Pij​/Qij​)1{Pij​=0}​. From the trajectory, nijn_{ij}nij​ counts the transitions si→sjs_i\to s_jsi​→sj​, and the averaged negative log-likelihood is ℓn(Q)=−1n∑i,jnijlog⁡Qij\ell_n(Q)=-\frac1n\sum_{i,j}n_{ij}\log Q_{ij}ℓn​(Q)=−n1​∑i,j​nij​logQij​. The empirical KL divergence is D~KL(P,Q)=ℓn(Q)−ℓn(P)\widetilde D_{\mathrm{KL}}(P,Q)=\ell_n(Q)-\ell_n(P)DKL​(P,Q)=ℓn​(Q)−ℓn​(P).

Assumption 1 of the paper: rank⁡(P)=r\operatorname{rank}(P)=rrank(P)=r, and Pjk∈{0}∪[α/p,β/p]P_{jk}\in\{0\}\cup[\alpha/p,\beta/p]Pjk​∈{0}∪[α/p,β/p] for constants α,β>0\alpha,\beta>0α,β>0. The (α/p)(\alpha/p)(α/p)-minoration (Remark 2) removes the 000: α/p≤Pjk≤β/p\alpha/p\le P_{jk}\le\beta/pα/p≤Pjk​≤β/p for all j,kj,kj,k. The rank-constrained MLE (5) is any

P^r∈arg⁡min⁡{ℓn(Q): Q1p=1p, α/p≤Qij≤β/p, rank⁡(Q)≤r}.\widehat P^r\in\arg\min\big\{\ell_n(Q):\ Q1_p=1_p,\ \alpha/p\le Q_{ij}\le\beta/p,\ \operatorname{rank}(Q)\le r\big\}.Pr∈argmin{ℓn​(Q): Q1p​=1p​, α/p≤Qij​≤β/p, rank(Q)≤r}.

In Lean these objects are IsStochastic, IsStationary, IsPrimitive, piMin, piMax, trajProb, rhoPlus, klDiv, negLogLik, empKL, Assumption1, Minorated, RankFeasible and IsRankMLE in the namespace LowRankMarkov.RankMLE.

Formalization targets

Goal: Theorem 2, KL display (p. 10)

There are universal constants C1,C2>0C_1,C_2>0C1​,C2​>0 such that, for p≥2p\ge2p≥2, under minoration with rank⁡P=r\operatorname{rank}P=rrankP=r and nπmax⁡(1−ρ+)>max⁡(20log⁡p,log⁡n)n\pi_{\max}(1-\rho_+)>\max(20\log p,\log n)nπmax​(1−ρ+​)>max(20logp,logn), every rank-constrained MLE satisfies, for all ξ>0\xi>0ξ>0,

P{DKL(P,P^r)≥max⁡(C1rπmax⁡β2plog⁡pπmin⁡α3n, ξπmin⁡rpπmax⁡log⁡p)}≤C2e−ξ.\mathbb P\Big\{D_{\mathrm{KL}}(P,\widehat P^r)\ge\max\Big(\frac{C_1r\pi_{\max}\beta^2p\log p}{\pi_{\min}\alpha^3n},\ \frac{\xi\pi_{\min}}{rp\pi_{\max}\log p}\Big)\Big\}\le C_2e^{-\xi}.P{DKL​(P,Pr)≥max(πmin​α3nC1​rπmax​β2plogp​, rpπmax​logpξπmin​​)}≤C2​e−ξ.

The constants are not fixed numerically, so a sharper analysis does not invalidate the goal.

Milestones

  1. Lemma EC.1, both forms: DKL(u,v)≥pα2β2∥u−v∥22D_{\mathrm{KL}}(u,v)\ge\frac{p\alpha}{2\beta^2}\|u-v\|_2^2DKL​(u,v)≥2β2pα​∥u−v∥22​ for distributions with uj∈{0}∪[α/p,β/p]u_j\in\{0\}\cup[\alpha/p,\beta/p]uj​∈{0}∪[α/p,β/p], vj∈[α/p,β/p]v_j\in[\alpha/p,\beta/p]vj​∈[α/p,β/p], and its matrix form ∥P−Q∥F2≤2β2απmin⁡pDKL(P,Q)\|P-Q\|_F^2\le\frac{2\beta^2}{\alpha\pi_{\min}p}D_{\mathrm{KL}}(P,Q)∥P−Q∥F2​≤απmin​p2β2​DKL​(P,Q).
  2. The rank remark (p. 14): rank⁡(P^r−P)≤2r\operatorname{rank}(\widehat P^r-P)\le2rrank(Pr−P)≤2r and ∥P^r−P∥∗≤(2r)1/2∥P^r−P∥F\|\widehat P^r-P\|_*\le(2r)^{1/2}\|\widehat P^r-P\|_F∥Pr−P∥∗​≤(2r)1/2∥Pr−P∥F​.
  3. (EC.14): on the shell Q∈C(η)Q\in\mathcal C(\eta)Q∈C(η), l≥1l\ge1l≥1 and 2l−1η≤DKL(P,Q)≤2lη2^{l-1}\eta\le D_{\mathrm{KL}}(P,Q)\le2^l\eta2l−1η≤DKL​(P,Q)≤2lη, ∥Q−P∥∗≤2β(2lηr/(pαπmin⁡))1/2\|Q-P\|_*\le2\beta(2^l\eta r/(p\alpha\pi_{\min}))^{1/2}∥Q−P∥∗​≤2β(2lηr/(pαπmin​))1/2.
  4. (EC.15), (EC.17): Bernstein-type tails p−(ξ−1)p^{-(\xi-1)}p−(ξ−1) for Wn(1)=max⁡j∑i≤nPXi−1,jW^{(1)}_n=\max_j\sum_{i\le n}P_{X_{i-1},j}Wn(1)​=maxj​∑i≤n​PXi−1​,j​ and Wn(2)=max⁡j∑i≤n1{Xi−1=sj}W^{(2)}_n=\max_j\sum_{i\le n}1_{\{X_{i-1}=s_j\}}Wn(2)​=maxj​∑i≤n​1{Xi−1​=sj​}​.
  5. Lemma 3: with probability at least 1−C2exp⁡(−ηπmax⁡rplog⁡p/πmin⁡)1-C_2\exp(-\eta\pi_{\max}rp\log p/\pi_{\min})1−C2​exp(−ηπmax​rplogp/πmin​), ∣D~KL(P,Q)−DKL(P,Q)∣≤12DKL(P,Q)+C1πmax⁡β2rplog⁡p/(πmin⁡α3n)|\widetilde D_{\mathrm{KL}}(P,Q)-D_{\mathrm{KL}}(P,Q)|\le\frac12D_{\mathrm{KL}}(P,Q)+C_1\pi_{\max}\beta^2rp\log p/(\pi_{\min}\alpha^3n)∣DKL​(P,Q)−DKL​(P,Q)∣≤21​DKL​(P,Q)+C1​πmax​β2rplogp/(πmin​α3n) for every Q∈CQ\in\mathcal CQ∈C with DKL(P,Q)≥ηD_{\mathrm{KL}}(P,Q)\ge\etaDKL​(P,Q)≥η.
  6. (EC.3): D~KL(P,P^r)≤0\widetilde D_{\mathrm{KL}}(P,\widehat P^r)\le0DKL​(P,Pr)≤0. Together with DKL(P,P^r)=L(P^r)−L(P)D_{\mathrm{KL}}(P,\widehat P^r)=\mathcal L(\widehat P^r)-\mathcal L(P)DKL​(P,Pr)=L(Pr)−L(P) it gives (EC.4), DKL(P,P^r)≤DKL(P,P^r)−D~KL(P,P^r)D_{\mathrm{KL}}(P,\widehat P^r)\le D_{\mathrm{KL}}(P,\widehat P^r)-\widetilde D_{\mathrm{KL}}(P,\widehat P^r)DKL​(P,Pr)≤DKL​(P,Pr)−DKL​(P,Pr).

Significance

The bound says that, with high probability, the KL error of P^r\widehat P^rPr is of order rplog⁡p/nrp\log p/nrplogp/n up to the factors πmax⁡/πmin⁡\pi_{\max}/\pi_{\min}πmax​/πmin​ and β2/α3\beta^2/\alpha^3β2/α3, plus a term independent of nnn controlled by ξ\xiξ. A trajectory of length of order rplog⁡prp\log prplogp, rather than p2p^2p2, therefore suffices: the low rank is what makes the estimation problem sample-efficient. Lemma EC.1 converts the KL bound into a Frobenius-norm bound, and Lemma 3 is a uniform law for the empirical KL process of a dependent sequence over the paper’s cone class.

The result is proved in the paper; nothing in it has been machine-checked. The mission asks for a formal proof of the KL display. Two points need care beyond transcription: the printed hypotheses do not suffice (see Formalization scope), and the paper's proof of Lemma 3 symmetrizes the dependent summands as if they were independent (EC.8), so a formal proof must supply a valid argument for that step.

Difficulty

Comparing ℓn(P^r)\ell_n(\widehat P^r)ℓn​(Pr) with ℓn(P)\ell_n(P)ℓn​(P) is immediate; the difficulty is to control D~KL−DKL\widetilde D_{\mathrm{KL}}-D_{\mathrm{KL}}DKL​−DKL​ uniformly over a non-convex set of matrices, from one dependent trajectory. A union bound over a net of the feasible set loses polynomial factors in ppp, and i.i.d. empirical-process tools do not apply directly to a Markov chain. The printed Lemma 3 covers the cone class C\mathcal CC, while the appendix proof restricts its shells to rank-rrr matrices. This leaves a gap for matrices in C\mathcal CC of higher rank and for the claimed application to P^r\widehat P^rPr when r>16r>16r>16. The paper combines a tail inequality for suprema of empirical processes of Markov chains (Adamczak 2008), a contraction step, the matrix Freedman inequality (Tropp 2011) for a matrix martingale, and a Bernstein inequality for Markov chains with a spectral gap (Jiang, Fan & Sun 2018) for the quadratic variations Wn(1),Wn(2)W^{(1)}_n,W^{(2)}_nWn(1)​,Wn(2)​. None of these is in Mathlib.

Formalization scope

States are Fin p, matrices Matrix (Fin p) (Fin p) ℝ, logarithms natural. A trajectory x=(X0,…,Xn)x=(X_0,\dots,X_n)x=(X0​,…,Xn​) makes nnn transitions, and its probability is π(x0)∏k<nPxkxk+1\pi(x_0)\prod_{k<n}P_{x_kx_{k+1}}π(x0​)∏k<n​Pxk​xk+1​​; probabilities of events are finite sums, so no measure theory is needed. ρ+\rho_+ρ+​ is a real sSup; "ρ+<1\rho_+<1ρ+​<1" is not built into its definition. The nuclear and Frobenius norms come from the published definition CaiCandesShen.Convergence.Basic.

Hypotheses fixed relative to the page:

  • Minoration instead of Assumption 1(ii), in the goal and (EC.3). The printed Theorem 2 allows Pjk=0P_{jk}=0Pjk​=0, and it is false then. For even ppp, let rows 1,…,p/21,\dots,p/21,…,p/2 of PPP equal 2/p2/p2/p on columns p/2+1,…,pp/2+1,\dots,pp/2+1,…,p and 000 elsewhere, and rows p/2+1,…,pp/2+1,\dots,pp/2+1,…,p equal 1/p1/p1/p. Then rank⁡P=2\operatorname{rank}P=2rankP=2, α=1\alpha=1α=1, β=2\beta=2β=2, ρ+=0\rho_+=0ρ+​=0, π\piπ puts mass 1/31/31/3 on the first half and πmax⁡/πmin⁡=2\pi_{\max}/\pi_{\min}=2πmax​/πmin​=2. Every feasible QQQ has Qij≥1/pQ_{ij}\ge1/pQij​≥1/p, so on each of the first p/2p/2p/2 rows QQQ puts mass at most 1/21/21/2 on the support of PPP, and DKL(P,Q)≥13log⁡2D_{\mathrm{KL}}(P,Q)\ge\frac13\log2DKL​(P,Q)≥31​log2. With ξ=0.9 plog⁡p\xi=0.9\,p\log pξ=0.9plogp the threshold is below 13log⁡2\frac13\log231​log2 for all large nnn, so the probability is 111, while C2e−ξ<1C_2e^{-\xi}<1C2​e−ξ<1 for large ppp. The broken step is (EC.3), which needs PPP feasible for (5); minoration with rank⁡P=r\operatorname{rank}P=rrankP=r makes it feasible. Lemma EC.1, (EC.14), (EC.15), (EC.17) and Lemma 3 keep the printed Assumption 1.
  • X0∼πX_0\sim\piX0​∼π, stated in Theorem 1 and used by the proof of Theorem 2 through Lemma 3.
  • Ergodic is read as primitive; πi>0\pi_i>0πi​>0 is stated (it is implied); p≥2p\ge2p≥2 keeps log⁡p>0\log p>0logp>0 in denominators.
  • Lemma 3's set is the printed C(η)\mathcal C(\eta)C(η), whose cone is ∥Q−P∥∗≤4×21/2∥Q−P∥F\|Q-P\|_*\le4\times2^{1/2}\|Q-P\|_F∥Q−P∥∗​≤4×21/2∥Q−P∥F​ and which has no rank constraint. The appendix proof uses rank-restricted shells; for r>16r>16r>16 the rank remark alone does not place P^r\widehat P^rPr in C\mathcal CC. This is a proof gap, while the formal statement retains the page's quantification.
  • Lemma EC.1's matrix form and (EC.14) include the printed cone condition. (EC.14) is stated pointwise for members of Cl\mathcal C_lCl​.

The statements rule out trivializing readings: C1,C2C_1,C_2C1​,C2​ are quantified before all data; the goal holds for every selection of minimizers, not for one fixed estimator; p≥2p\ge2p≥2 and π>0\pi>0π>0 exclude the junk values x/0=0x/0=0x/0=0 and log⁡1=0\log1=0log1=0 that would collapse the thresholds; a sorry-free check shows the goal's hypotheses are jointly satisfiable (p=2p=2p=2, uniform PPP, n=28n=28n=28).

Not posed: Theorem 1 (nuclear-norm MLE), the Frobenius display of Theorem 2 (Lemma EC.1 turns the KL threshold into twice the printed Frobenius threshold, so the paper's one-line derivation gives C2e−ξ/2C_2e^{-\xi/2}C2​e−ξ/2), Theorem 3 (lower bound), and the DC-programming results of §4. Useful reusable contributions: a Bernstein inequality for finite Markov chains with a spectral gap, the matrix Freedman inequality, and the reverse-Pinsker bound of Lemma EC.1.

Selected references

  • Z. Zhu, X. Li, M. Wang, A. R. Zhang, Learning Markov models via low-rank optimization, Operations Research, 2022; preprint arXiv:1907.00113v2, 2020. https://arxiv.org/abs/1907.00113
  • B. Jiang, J. Fan, Q. Sun, Bernstein's inequality for general Markov chains, arXiv:1805.10721, 2018. https://arxiv.org/abs/1805.10721
  • J. A. Tropp, Freedman's inequality for matrix martingales, Electronic Communications in Probability 16:262–270, 2011. https://arxiv.org/abs/1101.3039
  • R. Adamczak, A tail inequality for suprema of unbounded empirical processes with applications to Markov chains, Electronic Journal of Probability 13(34):1000–1034, 2008. https://arxiv.org/abs/0709.3110
  • J. A. Fill, Eigenvalue bounds on convergence to stationarity for nonreversible Markov chains, with an application to the exclusion process, The Annals of Applied Probability 1(1):62–87, 1991. https://doi.org/10.1214/aoap/1177005981
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EconomicsOperations Research·Captain: mikedeng1

Skill Acquisition and Data Sales: Under Uncertain Skill Acquisition and Accurate Data, Higher Skill-Acquisition Costs Raise Data Clarity, Data Price and Price InformativenessResearch Paper

Motivation

Asset managers increasingly buy alternative data: satellite images, credit-card panels, web traffic. Raw data of this kind is worthless until someone has the skills to process it, and those skills are costly and uncertain to acquire. A fund can hire data scientists and still find that its models extract little. Huang, Xiong and Yang (Management Science, 2022) build an equilibrium model of a data seller who sells to investors who must first acquire such skills. They ask how the cost of acquiring skills feeds through the data market into the financial market: into how much the price reveals, the cost of capital and return volatility.

The model joins two lines of work. One is the classical noisy rational-expectations market of Grossman and Stiglitz (1980), in which prices partly reveal private information. The other is the literature on selling information started by Admati and Pfleiderer (1986, 1990), in which a monopolist seller degrades the information it sells to limit what the price leaks. The new feature is the "gold rush" of skill acquisition: an investor who pays the cost learns only afterwards whether her skill is high or low.

Setting

A risky asset pays θ~∼N(0,τθ−1)\tilde\theta\sim N(0,\tau_\theta^{-1})θ~∼N(0,τθ−1​) and there is noise demand u~∼N(0,τu−1)\tilde u\sim N(0,\tau_u^{-1})u~∼N(0,τu−1​). A data seller observes θ~+η~\tilde\theta+\tilde\etaθ~+η~​ with η~∼N(0,τη−1)\tilde\eta\sim N(0,\tau_\eta^{-1})η~​∼N(0,τη−1​); the precision τη\tau_\etaτη​ is the data accuracy. The seller chooses a clarity x∈(0,∞]x\in(0,\infty]x∈(0,∞] and passes the data with personalized noise, so that a buyer of skill zzz receives a signal of precision xzxzxz about θ~+η~\tilde\theta+\tilde\etaθ~+η~​. The value x=∞x=\inftyx=∞ means the data are sold "as is".

A continuum of CARA investors with risk aversion γ\gammaγ is indexed by i∈[0,1]i\in[0,1]i∈[0,1]. Investor iii can acquire data-processing skills at cost C(c,i)C(c,i)C(c,i), where c>0c>0c>0 is a cost parameter. The cost is continuous and strictly increasing in iii, with C(c,0)=0C(c,0)=0C(c,0)=0 and C(c,i)→∞C(c,i)\to\inftyC(c,i)→∞ as i→1i\to1i→1, and it is strictly increasing in ccc. A skilled investor turns out high-skilled (ZHZ_HZH​) or low-skilled (ZLZ_LZL​) with probability 12\tfrac1221​ each, with 0<ZL<ZH0<Z_L<Z_H0<ZL​<ZH​. A mass λ\lambdaλ of investors becomes skilled.

In the asset market, the price reveals θ~+η~\tilde\theta+\tilde\etaθ~+η~​ with precision α2τu\alpha^2\tau_uα2τu​, and α\alphaα is pinned down by the market-clearing equation (14). Skilled investors buy the data at a Nash-bargained price q=βGq=\beta Gq=βG, where G(x,α)G(x,\alpha)G(x,α) is the certainty-equivalent trading gain (15) and β∈(0,1)\beta\in(0,1)β∈(0,1) is the seller's bargaining power. Investors acquire skills until the marginal investor is indifferent, (1−β)G(x,α)=C(c,λ)(1-\beta)G(x,\alpha)=C(c,\lambda)(1−β)G(x,α)=C(c,λ) (19). The seller chooses xxx to maximize the profit λq\lambda qλq. An equilibrium is a clarity x∗x^*x∗ with its (λ∗,α∗)(\lambda^*,\alpha^*)(λ∗,α∗) such that no other feasible clarity gives more profit.

The market outcomes are:

  • the data price q∗q^*q∗;
  • price informativeness 1/Var⁡(θ~∣p~)1/\operatorname{Var}(\tilde\theta\mid\tilde p)1/Var(θ~∣p~​);
  • the cost of capital E(θ~−p~)E(\tilde\theta-\tilde p)E(θ~−p~​);
  • return volatility σ(θ~−p~)\sigma(\tilde\theta-\tilde p)σ(θ~−p~​);
  • skilled investors' performance, the average certainty-equivalent advantage (21) of a skilled over an unskilled investor.

Formalization targets

Goal: Proposition 5

Fix 0<c1<c20<c_1<c_20<c1​<c2​. There is a threshold TTT such that, for every data accuracy τη≥T\tau_\eta\ge Tτη​≥T and every pair of equilibria at c1c_1c1​ and c2c_2c2​, both clarities are finite and

λ2∗<λ1∗,x1∗<x2∗,q1∗<q2∗,1Var⁡1(θ~∣p~)<1Var⁡2(θ~∣p~),\lambda^*_2<\lambda^*_1,\quad x^*_1<x^*_2,\quad q^*_1<q^*_2,\quad \frac{1}{\operatorname{Var}_1(\tilde\theta\mid\tilde p)}<\frac{1}{\operatorname{Var}_2(\tilde\theta\mid\tilde p)},λ2∗​<λ1∗​,x1∗​<x2∗​,q1∗​<q2∗​,Var1​(θ~∣p~​)1​<Var2​(θ~∣p~​)1​, E2(θ~−p~)<E1(θ~−p~),σ2(θ~−p~)<σ1(θ~−p~),Performance1<Performance2.E_2(\tilde\theta-\tilde p)<E_1(\tilde\theta-\tilde p),\quad \sigma_2(\tilde\theta-\tilde p)<\sigma_1(\tilde\theta-\tilde p),\quad \mathrm{Performance}_1<\mathrm{Performance}_2 .E2​(θ~−p~​)<E1​(θ~−p~​),σ2​(θ~−p~​)<σ1​(θ~−p~​),Performance1​<Performance2​.

The paper writes these as signs of derivatives in ccc. The goal states them as comparisons between two cost levels, which is what the prose of the proposition asserts.

Milestones

  1. Proposition 1: for given (λ,x)(\lambda,x)(λ,x), equation (14) has a unique positive root α\alphaα.
  2. Proof of Proposition 2: for each finite clarity xxx, a unique (λ,α)(\lambda,\alpha)(λ,α) solves (14) and (19).
  3. Proposition 2 (1): an equilibrium exists.
  4. (C5): on feasible tuples the profit equals βλC(c,λ)/(1−β)\beta\lambda C(c,\lambda)/(1-\beta)βλC(c,λ)/(1−β).
  5. Proposition 3: in equilibrium, x∗<∞x^*<\inftyx∗<∞ if λ∗τη>α∗γ\lambda^*\tau_\eta>\alpha^*\gammaλ∗τη​>α∗γ and x∗=∞x^*=\inftyx∗=∞ otherwise.
  6. The clarity limit: as τη→∞\tau_\eta\to\inftyτη​→∞, every solution xxx of (14) tends to 2αγ/(λ(ZH+ZL))2\alpha\gamma/(\lambda(Z_H+Z_L))2αγ/(λ(ZH​+ZL​)).
  7. The α limit: the equilibrium α∗\alpha^*α∗ tends to τθ/τu\sqrt{\tau_\theta/\tau_u}τθ​/τu​​.
  8. (C18): the equilibrium λ∗\lambda^*λ∗ tends to a root of (C18).

Significance

The result. Proposition 5 is the paper's headline. When skills are uncertain, a rise in skill-acquisition costs makes prices more informative and lowers the cost of capital and return volatility. When skills are certain, these outcomes stay unchanged (Proposition 4). The mechanism is that the seller cannot tailor one clarity to buyers of unknown skill. To keep buyers interested as costs rise, she provides clearer data, and more information leaks into the price. The result separates the data market from a pure cost shock to information production. It gives empirical predictions for markets where skill acquisition is costlier, such as private or international equities.

Formalizing it. The proposition is proved in the paper by expansion in w=1/τηw=1/\tau_\etaw=1/τη​ around w=0w=0w=0. A machine-checked version must make "sufficiently high τη\tau_\etaτη​" precise, with a threshold that holds uniformly over all equilibria. It must also control the exact finite-τη\tau_\etaτη​ equilibrium rather than its limit. The mission also contributes the first noisy rational-expectations model with a strategic data seller on the platform: posterior variances, the equilibrium equation (14), the certainty-equivalent gain, and the seller's choice between finite clarity and selling "as is". No part of the paper has been formalized before.

Difficulty

Several comparisons follow at leading order in 1/τη1/\tau_\eta1/τη​. As τη→∞\tau_\eta\to\inftyτη​→∞ the equilibrium mass converges to the root of (C18), which is decreasing in ccc, and the clarity, the data price and performance are, to first order, functions of that mass. The price-informativeness, cost-of-capital and volatility comparisons do not follow at leading order. At τη=∞\tau_\eta=\inftyτη​=∞ the ratio α∗\alpha^*α∗ tends to τθ/τu\sqrt{\tau_\theta/\tau_u}τθ​/τu​​ whatever the cost, so these three outcomes are flat in ccc to leading order. Their signs come from the O(1/τη)O(1/\tau_\eta)O(1/τη​) correction to α∗\alpha^*α∗, and the correction must be controlled jointly with the seller's optimal clarity. A newcomer's first idea is to set τη=∞\tau_\eta=\inftyτη​=∞ in the equilibrium conditions and differentiate. That loses exactly the term that carries the result. A further difficulty is that the seller's optimum is defined by comparison with every feasible clarity, including selling "as is", not by a first-order condition.

Formalization scope

All quantities are real numbers. The parameters satisfy τθ,τu,γ>0\tau_\theta,\tau_u,\gamma>0τθ​,τu​,γ>0, 0<β<10<\beta<10<β<1, 0<ZL<ZH0<Z_L<Z_H0<ZL​<ZH​ and τη>0\tau_\eta>0τη​>0. Two of these go beyond the paper's §2 domains, and both are needed:

  • β>0\beta>0β>0: with β=0\beta=0β=0 the profit is identically zero and every clarity is optimal;
  • ZL>0Z_L>0ZL​>0: this is the paper's own condition on p. 23.

The cost family is any admissible C(c,i)C(c,i)C(c,i): continuous and strictly increasing in iii on [0,1)[0,1)[0,1), C(c,0)=0C(c,0)=0C(c,0)=0, C(c,i)→∞C(c,i)\to\inftyC(c,i)→∞ as i→1−i\to1^-i→1−, and strictly increasing in ccc on (0,1)(0,1)(0,1). "Increasing" in the paper is read as strictly increasing. Clarity is either a finite x>0x>0x>0 or "as is". At "as is", (14) becomes γα=λτη\gamma\alpha=\lambda\tau_\etaγα=λτη​ and both conditional variances given a signal equal 1/(τθ+τη)1/(\tau_\theta+\tau_\eta)1/(τθ​+τη​). These are the x→∞x\to\inftyx→∞ limits of the finite-clarity formulas. The value x=0x=0x=0 is excluded from the choice set because it gives no positive root of (14).

The posterior variances (8), (10), (12), the gain (15), the price coefficients (C1)–(C4), the cost of capital (C12), volatility (C13) and performance (21) are taken as closed-form definitions. Their CARA-normal derivation (Bayes' rule, market clearing, certainty equivalents) is not formalized. Equilibria are defined relationally: a feasible tuple whose profit is at least that of every feasible tuple, with no choice functions.

The goal concludes, rather than assumes, that the equilibrium clarities are finite. It quantifies over every equilibrium at each cost level. It does not define the equilibrium through the τη=∞\tau_\eta=\inftyτη​=∞ economy or through the paper's expansions, which would replace the theorem by its heuristic.

A complete development needs real analysis only: the intermediate value theorem, monotonicity, compactness on (0,∞](0,\infty](0,∞], and asymptotics in 1/τη1/\tau_\eta1/τη​. Contributions are welcome on any milestone, on an independent proof of Proposition 4's Δ=0\Delta=0Δ=0 counterpart, and on a formal derivation of the closed forms from Gaussian conditioning and CARA utility, which would be reusable for other rational-expectations models.

Selected references

  • S. Huang, Y. Xiong, L. Yang, Skill Acquisition and Data Sales, Management Science 68(8), 2022; working paper version of July 2019. https://doi.org/10.1287/mnsc.2021.4117
  • S. J. Grossman, J. E. Stiglitz, On the Impossibility of Informationally Efficient Markets, American Economic Review 70(3), 1980. https://www.jstor.org/stable/1805228
  • A. R. Admati, P. Pfleiderer, A Monopolistic Market for Information, Journal of Economic Theory 39(2), 1986. https://doi.org/10.1016/0022-0531(86)90049-3
  • A. R. Admati, P. Pfleiderer, Direct and Indirect Sale of Information, Econometrica 58(4), 1990. https://doi.org/10.2307/2938330
  • N. Gârleanu, L. H. Pedersen, Efficiently Inefficient Markets for Assets and Asset Management, Journal of Finance 73(4), 2018. https://doi.org/10.1111/jofi.12696
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Control TheoryOperations ResearchOptimization·Captain: mikedeng1

Managing Self-Replicating Innovative Goods: Characterization of the Optimal Production and Sales Policies under Strong ReplicabilityResearch Paper

Why self-replicating goods

Some goods can only be made by copies of themselves. RepRap and Prusa 3D printers print the parts of new printers, seed stock is grown from seed, and livestock herds breed. For such a good the inventory is also the production capacity: a unit sold today is a unit that will not replicate tomorrow. A firm launching such a good has to decide, at every instant, how much of its stock to use for replication and how much demand to serve. Demand for an innovative good is not exogenous either. It diffuses through the market by word-of-mouth, so sales held back today also slow future demand.

B. Hu and Z. Sun (Management Science) model this as a deterministic optimal control problem. Their demand side is the Bass diffusion model (Bass, 1969) in the supply-constrained form of Ho, Savin and Terwiesch (2002) and Kumar and Swaminathan (2003), where cumulative sales rather than cumulative demand drive imitation. Hu and Sun add diminishing word-of-mouth. Their main structural result, Theorem 1, says that under a condition they call Strong Replicability the optimal policy switches only once and can be found by a one-dimensional search.

The model

Time runs over [0,T][0,T][0,T], where TTT is the life cycle. The firm controls a production rate p(t)p(t)p(t) and a sales rate s(t)s(t)s(t). The state consists of the cumulative demand D(t)D(t)D(t), the adjusted cumulative sales S(t)S(t)S(t) and the inventory I(t)I(t)I(t). The demand rate is

d(t)=[α+βS(t)m][m−D(t)],d(t)=\Big[\alpha+\frac{\beta S(t)}{m}\Big]\big[m-D(t)\big],d(t)=[α+mβS(t)​][m−D(t)],

where mmm is the market size, α\alphaα the coefficient of innovation and β\betaβ the coefficient of imitation. Problem (1) of the paper is

max⁡p,s∫0T[πs(t)−cp(t)−hI(t)]e−ρt dt\max_{p,s}\int_0^T\big[\pi s(t)-cp(t)-hI(t)\big]e^{-\rho t}\,dtp,smax​∫0T​[πs(t)−cp(t)−hI(t)]e−ρtdt

subject to

D′=d,S′=s−wS,I′=p−s,0≤p≤rI,0≤s≤d,I(T)≥0,D'=d,\quad S'=s-wS,\quad I'=p-s,\qquad 0\le p\le rI,\quad 0\le s\le d,\quad I(T)\ge0,D′=d,S′=s−wS,I′=p−s,0≤p≤rI,0≤s≤d,I(T)≥0, D(0)=S(0)=0,I(0)=IL>0.D(0)=S(0)=0,\qquad I(0)=I_L>0.D(0)=S(0)=0,I(0)=IL​>0.

Here π\piπ is the price, ccc the unit replication cost, hhh the holding cost rate, rrr the replication rate, ρ≥0\rho\ge0ρ≥0 the discount rate and w≥0w\ge0w≥0 the rate at which word-of-mouth decays. Unmet demand is lost. The paper assumes π>c\pi>cπ>c and r>ρr>\rhor>ρ. Production is on when p=rIp=rIp=rI and off when p=0p=0p=0. Sales are on when s=ds=ds=d and off when s=0s=0s=0.

Strong Replicability is condition (2),

(r−ρ)π>cr+h.(r-\rho)\pi>cr+h.(r−ρ)π>cr+h.

It says that letting a unit replicate for a short time and selling the offspring later is worth more than selling the unit now.

Two levels of the launch inventory organise the answer. I‾\underline II​ is the level at which keeping production and sales always on depletes the inventory exactly at TTT. I‾\overline II is the level at which keeping production off and sales on depletes it exactly at TTT.

Formalization targets

Goal: Theorem 1

Assume Strong Replicability. Then:

  • (a) if IL<I‾I_L<\underline IIL​<I​, the policy that keeps production always on and switches sales on once, at the time that depletes the inventory exactly at TTT, is optimal;
  • (b) if I‾<IL<I‾\underline I<I_L<\overline II​<IL​<I, the policy that keeps sales always on and switches production on once, at the time that depletes the inventory exactly at TTT, is optimal;
  • (c) if IL>I‾I_L>\overline IIL​>I, the policy that keeps sales always on and production off is optimal, and it leaves inventory at TTT.

In each case, optimal means that the profit is at least

∫0T[πs~−cp~−hI~]e−ρt dt\int_0^T\big[\pi\tilde s-c\tilde p-h\tilde I\big]e^{-\rho t}\,dt∫0T​[πs~−cp~​−hI~]e−ρtdt

for every admissible trajectory (D~,S~,I~,p~,s~)(\tilde D,\tilde S,\tilde I,\tilde p,\tilde s)(D~,S~,I~,p~​,s~), not only for policies of the stated shape. The switching times are not given in closed form, and the theorem asserts only that they exist.

Milestones

  1. The thresholds are ordered, I‾<I‾\underline I<\overline II​<I (preamble of Theorem 1).
  2. Proposition 1. Once production is switched on, an optimal policy keeps it on until TTT or inventory depletion.
  3. Proposition 2, first half. Under Strong Replicability, every optimal trajectory has I(t)>0I(t)>0I(t)>0 for all t<Tt<Tt<T, whatever TTT is.

Significance

Theorem 1 turns an infinite-dimensional control problem into a choice of one switching time. Its managerial content is that a firm with a replicating good should, when stock is scarce, run replication at full capacity and hold back sales, losing some early customers, as long as the stock built up will eventually be sold. Proposition 2 says that under Strong Replicability the firm never sells out before the end of the life cycle. The paper's numerical study (§4) and its extensions (§5: backlogged demand, liquidity, stochastic diffusion) are built on this characterization.

The result has a published informal proof (pp. 36–37 of the manuscript), which applies necessary conditions from Pontryagin's maximum principle and then a perturbation and exchange argument. None of it is machine-checked. A complete formal proof would establish global optimality, against all integrable controls, for a nonlinear controlled ODE with mixed state–control constraints. That is a sufficiency statement, which the necessary conditions alone do not give.

Difficulty

The maximum principle gives necessary conditions only, and Problem (1) is not concave: the dynamics of DDD are bilinear in SSS and DDD, and the constraint p≤rIp\le rIp≤rI couples control and state. So the obvious route, solving the Pontryagin system and reading off the optimum, does not prove optimality. The paper's own argument is an exchange argument. It postpones sales or shifts production forward and claims each change improves profit, and it applies the change recursively ("by making the same argument recursively"). Making it rigorous requires comparison results for the Bass system under perturbed sales, which are delicate. Postponing sales lowers the adjusted sales SSS, and with it all future demand. The existence of the switching times also needs a continuity argument on the depletion time as a function of the switch.

Formalization scope

The Lean development lives in the namespace SelfReplic.Strong and uses real numbers throughout.

  • Parameters form a structure Params with fields m, price, c, h, r, alpha, beta, rho, w, T, IL. The predicate Params.Standing collects the page's assumptions IL>0I_L>0IL​>0, π>c\pi>cπ>c, r>ρ≥0r>\rho\ge0r>ρ≥0, w≥0w\ge0w≥0. It adds the sign conditions m>0m>0m>0, T>0T>0T>0, α>0\alpha>0α>0, β≥0\beta\ge0β≥0, c≥0c\ge0c≥0, h≥0h\ge0h≥0, which the paper uses but never states. Params.StrongRepl is condition (2).
  • Admissible trajectories (IsAdmissible) have integrable controls p,sp,sp,s and continuous states D,S,ID,S,ID,S,I on [0,T][0,T][0,T]. The three ODEs hold in integral form at every t∈[0,T]t\in[0,T]t∈[0,T], the constraints 0≤p≤rI0\le p\le rI0≤p≤rI, 0≤s≤d0\le s\le d0≤s≤d hold at every t∈[0,T]t\in[0,T]t∈[0,T], and I(T)≥0I(T)\ge0I(T)≥0. The integral form is used because bang-bang controls are discontinuous. Continuity and integrability prevent any integral from silently taking Lean's default value 000. Nonnegativity of III follows from 0≤p≤rI0\le p\le rI0≤p≤rI, as on p. 8.
  • Optimality (IsOptimal) compares the discounted profit with every admissible trajectory of the same parameters.
  • Policy shapes are pointwise statements on [0,T][0,T][0,T], and a switch instant counts as "on". The thresholds I‾,I‾\underline I,\overline II​,I enter as real numbers with their defining property (IsLowLevel, IsHighLevel), evaluated at the same parameters with ILI_LIL​ replaced.
  • Proposition 1 is read up to null sets ("production has run before t0t_0t0​", conclusion almost everywhere). It carries the added hypothesis ρc+h>0\rho c+h>0ρc+h>0, which the paper's proof uses. Without it (ρ=h=0\rho=h=0ρ=h=0), pausing production is costless and the statement fails.

A formalization that states Theorem 1 inside its own policy class (the best policy of shape (a) is the best of shape (a)) would be empty. Here the competitor in every case ranges over all admissible trajectories.

Not formalized: Theorem 2 (Weak Replicability), whose closed form (3) for the production interval is inexact when ρ>0\rho>0ρ>0; Corollaries 1–2; the second half of Proposition 2, which fails when IL≥mI_L\ge mIL​≥m; the unnumbered bang-bang claim of p. 9; Propositions 3–4 (§5).

Contributions that would be reusable beyond this mission include existence and uniqueness for the controlled Bass system in integral form, a comparison lemma for DDD and SSS under pointwise-ordered sales, and a sufficiency (verification) theorem for bang-bang controls of problems that are linear in the control.

Selected references

  • B. Hu, Z. Sun, Managing self-replicating innovative goods, Management Science (doi:10.1287/mnsc.2020.3936); authors' manuscript of 2020-10-18. https://doi.org/10.1287/mnsc.2020.3936
  • F. M. Bass, A new product growth for model consumer durables, Management Science 15(5), 215–227, 1969. https://doi.org/10.1287/mnsc.15.5.215
  • T.-H. Ho, S. Savin, C. Terwiesch, Managing demand and sales dynamics in new product diffusion under supply constraint, Management Science 48(2), 187–206, 2002. https://doi.org/10.1287/mnsc.48.2.187.255
  • S. Kumar, J. M. Swaminathan, Diffusion of innovations under supply constraints, Operations Research 51(6), 866–879, 2003. https://doi.org/10.1287/opre.51.6.866.24918
  • S. P. Sethi, Optimal Control Theory: Applications to Management Science and Economics, 3rd ed., Springer, 2019. https://doi.org/10.1007/978-3-319-98237-3
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Algorithmic Game TheoryEconomicsOperations Research·Captain: mikedeng1

Supplier Encroachment in a Non-Exclusive Reselling Channel: The Encroaching Supplier May Sell Only Directly at a Positive Direct Cost, or Through Both Channels at a Negative OneResearch Paper

Why encroachment through a shared reseller matters

Manufacturers that sell through retailers increasingly also sell directly to consumers, through their own web stores or outlets. The operations literature calls this supplier encroachment. The classical analysis (Arya, Mittendorf and Sappington, 2007) assumes an exclusive reseller: the reseller carries only the encroaching supplier's product. In that setting a supplier whose direct channel costs more per unit than the reseller's still sells through the reseller, and a supplier whose direct channel is cheaper never does.

Real resellers are rarely exclusive. A retailer that carries one brand usually carries competing brands too, and its order from one supplier depends on its order from the others. Hotkar and Gilbert (Management Science, 2021) study what changes when the reseller is non-exclusive. Their headline finding, Proposition 5, is that both conclusions of the exclusive model can reverse.

Setting

Two suppliers, i∈{1,2}i\in\{1,2\}i∈{1,2}, sell partially substitutable products through one reseller. Supplier 1 can also sell directly. The reseller orders q1q_1q1​ and q2q_2q2​; supplier 1 sells yyy units directly. The substitutability between the two suppliers' products is θ12∈(0,1)\theta_{12}\in(0,1)θ12​∈(0,1), written θ\thetaθ below. Supplier 1's direct product is a perfect substitute for her product at the reseller. Prices clear the market linearly:

p1=1−q1−θq2−y,p2=1−q2−θq1−θy,pd=1−y−q1−θq2.p_1=1-q_1-\theta q_2-y,\qquad p_2=1-q_2-\theta q_1-\theta y,\qquad p_d=1-y-q_1-\theta q_2 .p1​=1−q1​−θq2​−y,p2​=1−q2​−θq1​−θy,pd​=1−y−q1​−θq2​.

Production and reselling cost nothing. A direct sale costs supplier 1 an extra ccc per unit, and ccc may be negative: the direct channel can be more efficient than the reseller. With wholesale prices w1,w2≥0w_1,w_2\ge0w1​,w2​≥0, the reseller earns q1(p1−w1)+q2(p2−w2)q_1(p_1-w_1)+q_2(p_2-w_2)q1​(p1​−w1​)+q2​(p2​−w2​), supplier 1 earns y(pd−c)+q1w1y(p_d-c)+q_1w_1y(pd​−c)+q1​w1​, and supplier 2 earns q2w2q_2w_2q2​w2​.

The game has three stages:

  1. the suppliers set w1w_1w1​ and w2w_2w2​ simultaneously, and neither observes the other's price;
  2. the reseller, who sees both prices, orders q1q_1q1​ and q2q_2q2​;
  3. supplier 1 observes q1q_1q1​, but not q2q_2q2​ or w2w_2w2​, and chooses yyy.

Supplier 1 holds a belief w2′w_2'w2′​ about supplier 2's price. In stage III her quantity yyy and her conjecture q2′q_2'q2′​ of the reseller's order from supplier 2 are mutual best responses computed with w2′w_2'w2′​ (Lemma 1). In an equilibrium (the paper's (4.7)–(4.16)), beliefs equal the actual prices. The reseller best-responds at every price pair, anticipating supplier 1's reaction. Neither supplier gains from a unilateral price change. After a deviation by supplier 2, supplier 1's belief stays where it was. This is not a subgame-perfect equilibrium, because supplier 1 cannot observe w2w_2w2​.

The paper restricts the direct cost to c0(θ)<c<c3(θ)c_0(\theta)<c<c_3(\theta)c0​(θ)<c<c3​(θ) (p. 9). It identifies thresholds c0≤c1≤c2≤c3c_0\le c_1\le c_2\le c_3c0​≤c1​≤c2​≤c3​ (Table 2) that separate three regimes:

  • Direct Only (c≤c1c\le c_1c≤c1​) and Direct Only Boundary (c1≤c≤c2c_1\le c\le c_2c1​≤c≤c2​), in which the reseller orders nothing from supplier 1;
  • Reseller & Direct (c>c2c>c_2c>c2​), in which supplier 1 uses both channels.

The sign of c2c_2c2​ is that of

Num1(θ)=32−θ(80+θ(32+θ(14+θ(8−(4−θ)θ)))),\mathrm{Num1}(\theta)=32-\theta\Big(80+\theta\big(32+\theta(14+\theta(8-(4-\theta)\theta))\big)\Big),Num1(θ)=32−θ(80+θ(32+θ(14+θ(8−(4−θ)θ)))),

which has a unique root θ^≈0.3443\hat\theta\approx0.3443θ^≈0.3443 in (0,1)(0,1)(0,1).

Formalization targets

Goal: Proposition 5 (p. 22)

∃ θ^∈(0,1), Num1(θ^)=0, such that\exists\,\hat\theta\in(0,1),\ \mathrm{Num1}(\hat\theta)=0,\ \text{such that}∃θ^∈(0,1), Num1(θ^)=0, such that
  • for 0<θ<θ^0<\theta<\hat\theta0<θ<θ^: c2(θ)>0c_2(\theta)>0c2​(θ)>0, and for every c∈(0,c2(θ)]c\in(0,c_2(\theta)]c∈(0,c2​(θ)] an equilibrium exists and every equilibrium has q1∗=0<y∗q_1^*=0<y^*q1∗​=0<y∗. Supplier 1 sells only directly, although her direct channel is less efficient;
  • for θ^<θ<1\hat\theta<\theta<1θ^<θ<1: c2(θ)<0c_2(\theta)<0c2​(θ)<0. For θ^<θ≤9/10\hat\theta<\theta\le 9/10θ^<θ≤9/10 and every c∈(c2(θ),0)c\in(c_2(\theta),0)c∈(c2​(θ),0) there is an equilibrium with q1∗>0q_1^*>0q1∗​>0 and y∗>0y^*>0y∗>0. Supplier 1 sells through both channels, although her direct channel is more efficient.

Milestones

  • Lemma 1: the stage-III pair (yIII,q2′)(y^{III},q_2')(yIII,q2′​), which is unique.
  • Lemma 2: the reseller's conditionally optimal q2IIIq_2^{III}q2III​.
  • Corollary 1: q2III=q2′q_2^{III}=q_2'q2III​=q2′​ when w2=w2′w_2=w_2'w2​=w2′​.
  • Lemma 4: the threshold order c0≤c1≤c2≤c3c_0\le c_1\le c_2\le c_3c0​≤c1​≤c2​≤c3​.
  • Lemma 4: for c≤c2c\le c_2c≤c2​, the Direct Only and Direct Only Boundary prices are equilibria, and every equilibrium has q1∗=0<y∗q_1^*=0<y^*q1∗​=0<y∗.
  • Lemma 4: the Reseller & Direct equilibrium for c2<c<0c_2<c<0c2​<c<0 (stated for θ≤9/10\theta\le 9/10θ≤9/10).
  • The sign facts about Num1\mathrm{Num1}Num1 used in the proof of Proposition 5.

Significance

With an exclusive reseller, efficiency alone decides channel use: a costlier direct channel is used alongside the reseller, and a cheaper one replaces it. Proposition 5 shows that this rule fails once the reseller also carries a competitor.

  • When the products are weakly substitutable, supplier 1 may abandon the reseller although it is the cheaper channel. Supplier 2 then prices just low enough to keep her out.
  • When they are strongly substitutable, supplier 1 keeps selling through the reseller although her own channel is cheaper. The reseller's order shields her from supplier 2.

The result explains why observed channel structures need not reflect relative channel costs. It also shows which assumption of the exclusive model drives its conclusions.

As far as the mission's searches found, no part of this model has been machine-checked. The mission formalizes a game with unobservable prices and belief-based stage-III conjectures. Such games occur throughout the supply-chain contracting literature, and the equilibrium predicate here can be reused for them. The paper's proofs are algebraic, but they verify deviation incentives across a piecewise-defined reseller response, with polynomials of degree eight in θ\thetaθ. A formal proof has to check every branch.

Difficulty

The reseller's best response is piecewise in q1q_1q1​: supplier 1 sells directly only while q1q_1q1​ is below a threshold, and her conjecture about q2q_2q2​ can hit zero. The paper analyzes the reseller's choice under a restriction (Lemmas 1–3) that rules out the conjecture q2′=0q_2'=0q2′​=0 for small q1q_1q1​, and argues that the excluded region cannot occur in equilibrium. Deviation prices, however, can push the reseller into that region. There the reseller's objective is not concave in q1q_1q1​, and supplier 1 may find a price cut that triggers a jump in the reseller's order. A proof of Lemma 4 cannot simply cite first-order conditions inside the restricted region: it has to rule out such jumps for every deviation price. Numerically this succeeds for θ≤9/10\theta\le 9/10θ≤9/10, but it fails for θ\thetaθ close to 111.

The uniqueness claim in part (a) is a statement about every strategy profile, including the reseller's off-path rules. It cannot be obtained by exhibiting one profile. The equilibrium prices themselves are not unique for c≤c2c\le c_2c≤c2​, so this claim concerns the channel use q1∗=0<y∗q_1^*=0<y^*q1∗​=0<y∗ only.

Formalization scope

Everything is real-valued and lives in NonExclEncroach.Channels. The conventions are:

  • the paper's case θ1d=1\theta_{1d}=1θ1d​=1 (§4), hence θ2d=θ\theta_{2d}=\thetaθ2d​=θ; §5 (θ1d=0.8\theta_{1d}=0.8θ1d​=0.8) is out of scope;
  • the standing range 0<θ<10<\theta<10<θ<1 and c0<c<c3c_0<c<c_3c0​<c<c3​ (p. 9), with ccc allowed to be negative;
  • prices and quantities in [0,∞)[0,\infty)[0,∞);
  • best responses as argmaxes over [0,∞)[0,\infty)[0,∞), with no tie-breaking rule;
  • a strategy profile made of the two prices, supplier 1's direct-quantity and conjecture rules as functions of the observed q1q_1q1​, and the reseller's order rule at every price pair. Supplier 1's belief is the equilibrium price of supplier 2 and does not move after supplier 2 deviates.

The goal quantifies over this equilibrium predicate. Stating Proposition 5 with the quantities read off Table 1, or as the sign of c2c_2c2​ alone, would reduce it to the sign of Num1\mathrm{Num1}Num1, and is ruled out.

Three statements depart from the page, and each departure is disclosed in its Formalization Note:

  • Part (b) of the goal and the Direct Only/Boundary part of Lemma 4 are stated for θ≤9/10\theta\le 9/10θ≤9/10. The Reseller & Direct part of Lemma 4 is stated for θ≤9/10\theta\le 9/10θ≤9/10 and c2<c<0c_2<c<0c2​<c<0. A numerical solution of the game shows that the paper's equilibrium prices fail outside these ranges: for θ\thetaθ near 111, for θ≥0.85\theta\ge 0.85θ≥0.85 with c>0.3c>0.3c>0.3, and just below c3c_3c3​ (where supplier 2 gains by raising her price until the reseller shuts down the direct channel). The paper also announces that the Direct Only and Direct Only Boundary prices are the unique equilibrium prices for c≤c2c\le c_2c≤c2​. That is false: a lower w2w_2w2​, with w1w_1w1​ at the reseller's threshold, can also be an equilibrium. Those prices are therefore stated as existence.
  • "There exist positive (negative) values of ccc" is strengthened to every ccc in (0,c2](0,c_2](0,c2​] (in (c2,0)(c_2,0)(c2​,0)).
  • Lemma 2 assumes that the upper branch of (4.19) is non-negative.

Not formalized: Lemma 3, whose threshold 2c−12c-12c−1 is correct only when w2=w2′w_2=w_2'w2​=w2′​; the appendix lemma eliminating equilibria with q2′=0q_2'=0q2′​=0; and Propositions 1–4 and 6–8.

Contributions welcome: proofs of the milestones, a general existence theorem for the reseller's order rule, and an analysis of the game for θ\thetaθ near 111.

Selected references

  • P. Hotkar and S. M. Gilbert, Supplier Encroachment in a Non-Exclusive Reselling Channel, Management Science, 2021; SSRN working paper 3238502. https://ssrn.com/abstract=3238502 , https://doi.org/10.1287/mnsc.2020.3786
  • A. Arya, B. Mittendorf and D. E. M. Sappington, The Bright Side of Supplier Encroachment, Marketing Science 26(5), 2007. https://doi.org/10.1287/mksc.1070.0280
  • D. G. Pearce, Rationalizable Strategic Behavior and the Problem of Perfection, Econometrica 52(4), 1984. https://doi.org/10.2307/1911197
  • B. D. Bernheim, Rationalizable Strategic Behavior, Econometrica 52(4), 1984. https://doi.org/10.2307/1911196
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EconomicsOperations ResearchStochastic Systems·Captain: mikedeng1

Design and Pricing of Discretionary Service Lines: Under SPT Without Customer Heterogeneity, the Optimal Service Line Has Variety, No Cutoff and a Concave Price Falling at the TopResearch Paper

Motivation

Many services are discretionary: the provider chooses how long to spend with a customer, and a longer service is worth more to the customer. Medical consultations, legal and tax advice, repair and diagnostic work, and personal services such as hair styling all have this shape. A firm offering such services designs a service line, a menu of service durations with a price for each, and runs it on one shared resource. Longer services are more valuable, but they also slow the queue for everyone else, and customers dislike waiting.

L. Debo and C. Li, in Design and Pricing of Discretionary Service Lines (SSRN 3054741, 2017; later published in Management Science, doi:10.1287/mnsc.2020.3670), study this problem by combining a Mussa–Rosen style product-line model with a single-server queue. A central question is whether congestion alone, with all customers identical, can make variety optimal. Under first-in-first-out (FIFO) service the answer is no: with homogeneous customers the optimal line collapses to a single service. Under the shortest-processing-time (SPT) priority rule the paper shows that the optimal line does offer variety. This mission formalizes that result.

Setting

Customers arrive as a Poisson process of rate Λ>0\Lambda>0Λ>0. A customer who receives a service of duration ttt gets value V(t,θˉ)=θˉt−bt2V(t,\bar\theta)=\bar\theta t-bt^2V(t,θˉ)=θˉt−bt2 with b>0b>0b>0, and pays a waiting cost ccc per unit of sojourn time, waiting plus service. All customers have the same quality sensitivity θˉ\bar\thetaθˉ: the paper's heterogeneity parameter Δ\DeltaΔ is 000. The standing assumption is 0<c<θˉ0<c<\bar\theta0<c<θˉ.

A service line is a shortest duration t‾\underline tt​, a longest duration tˉ\bar ttˉ, and a demand measure μ\muμ on [t‾,tˉ]⊆[0,∞)[\underline t,\bar t]\subseteq[0,\infty)[t​,tˉ]⊆[0,∞). When demand has a density λ(t)\lambda(t)λ(t), customers choosing durations in [t,t+dt][t,t+dt][t,t+dt] arrive at rate λ(t) dt\lambda(t)\,dtλ(t)dt. Its moments are

Λk=∫τk μ(dτ),k=0,1,2,\Lambda_k=\int\tau^k\,\mu(d\tau),\qquad k=0,1,2,Λk​=∫τkμ(dτ),k=0,1,2,

so Λ0\Lambda_0Λ0​ is the throughput and Λ1\Lambda_1Λ1​ the load on the server. A line is feasible if Λ0≤Λ\Lambda_0\le\LambdaΛ0​≤Λ (customers may be turned away) and Λ1<1\Lambda_1<1Λ1​<1 (the queue is stable).

The server uses non-preemptive SPT: whenever it frees up, it starts the shortest waiting service. By Phipps and Van Voorhis (1956), a customer with duration ttt waits in queue for

W(t)=Λ2/2(1−∫t‾tτλ(τ) dτ)2W(t)=\frac{\Lambda_2/2}{\big(1-\int_{\underline t}^{t}\tau\lambda(\tau)\,d\tau\big)^2}W(t)=(1−∫t​t​τλ(τ)dτ)2Λ2​/2​

on average, which is eq. (7) of the paper. The expected queue length is Q=∫W dμQ=\int W\,d\muQ=∫Wdμ. With Δ=0\Delta=0Δ=0 the paper's mechanism-design problem (its Proposition 1) reduces to the firm's problem

max⁡ Π=(θˉΛ1−bΛ2)−c (Λ1+Q)over feasible service lines,(9)\max\ \Pi=(\bar\theta\Lambda_1-b\Lambda_2)-c\,(\Lambda_1+Q)\quad\text{over feasible service lines},\tag{9}max Π=(θˉΛ1​−bΛ2​)−c(Λ1​+Q)over feasible service lines,(9)

and the price of duration ttt is

P(t)=θˉt−bt2−c (t+W(t)),P(t)=\bar\theta t-bt^2-c\,(t+W(t)),P(t)=θˉt−bt2−c(t+W(t)),

which leaves every customer zero surplus.

Formalization targets

Goal: Proposition 5

For every Λ>0\Lambda>0Λ>0, problem (9) has an optimal service line, and every optimal line has

  1. service variety, t‾<tˉ\underline t<\bar tt​<tˉ;
  2. no customer cutoff, Λ0=Λ\Lambda_0=\LambdaΛ0​=Λ;
  3. a price PPP that is concave on [t‾,tˉ][\underline t,\bar t][t​,tˉ], with
ddtP(tˉ)<0.\frac{d}{dt}P(\bar t)<0 .dtd​P(tˉ)<0.

There are also thresholds Λ‾,Λˉ>0\underline\Lambda,\bar\Lambda>0Λ​,Λˉ>0, depending on (θˉ,b,c)(\bar\theta,b,c)(θˉ,b,c), such that

ddtP(t‾)<0  for Λ∈(0,Λ‾),ddtP(t‾)>0  for Λ∈(Λˉ,∞).\frac{d}{dt}P(\underline t)<0\ \text{ for }\Lambda\in(0,\underline\Lambda),\qquad \frac{d}{dt}P(\underline t)>0\ \text{ for }\Lambda\in(\bar\Lambda,\infty).dtd​P(t​)<0  for Λ∈(0,Λ​),dtd​P(t​)>0  for Λ∈(Λˉ,∞).

The thresholds are existential, so the goal does not commit to their values.

Milestones

  • Corollary 1. For every feasible line, Q≥12{ln⁡(1−Λ1)}2Q\ge\tfrac12\{\ln(1-\Lambda_1)\}^2Q≥21​{ln(1−Λ1​)}2. The bound does not depend on Λ0\Lambda_0Λ0​, and it is attained by λ(t)∝1/t3\lambda(t)\propto1/t^3λ(t)∝1/t3 on a line with t‾<tˉ\underline t<\bar tt​<tˉ.
  • Root of (A–35). The equation F(ω)=0F(\omega)=0F(ω)=0 of the paper's Lemma A7 has a root ω∈(0,1)\omega\in(0,1)ω∈(0,1).
  • Lemma A7. Every optimal line is given in closed form by a root ω\omegaω of (A–35): Λ0=Λ\Lambda_0=\LambdaΛ0​=Λ, Λ1=1−ω\Lambda_1=1-\sqrt\omegaΛ1​=1−ω​, and explicit Λ2\Lambda_2Λ2​, t‾\underline tt​, tˉ\bar ttˉ.
  • Quadratic waiting time. At an optimum, W(t)=−α0+α2t2W(t)=-\alpha_0+\alpha_2t^2W(t)=−α0​+α2​t2 on [t‾,tˉ][\underline t,\bar t][t​,tˉ] with α2>0\alpha_2>0α2​>0 and 2α2tˉ=θˉ/c−12\alpha_2\bar t=\bar\theta/c-12α2​tˉ=θˉ/c−1.
  • Proposition 5 split into its parts: (i)–(ii), (iii) at the top end, and (iii) at the bottom end.

Significance

The result separates two sources of variety. Classical product-line theory obtains variety from heterogeneous tastes. Proposition 5 obtains it from operations alone: under SPT, short services jump the queue, so a spread of durations lowers total waiting below what any single duration achieves (Corollary 1 makes this exact). This outweighs the loss in service value from moving away from a single duration. The price result is the operational counterpart. Customers who choose the longest services wait the longest, so the price falls at the top of the line, and in small markets it falls along the whole line. This contrasts with FIFO, where the price always increases in duration.

Formalizing these results adds the following. The paper's proofs are long first-order-condition calculations over a constrained calculus-of-variations problem. They take existence of an optimum for granted, and they argue the bottom-end sign through Taylor approximations in the limits 2b/(Λc)→02b/(\Lambda c)\to02b/(Λc)→0 and →∞\to\infty→∞. A machine-checked proof would establish existence, rigorously derive the optimality conditions over all demand measures, and turn the asymptotic sign argument into a proof. As far as is known, none of these results, nor the SPT waiting-time formula, has a machine-checked proof.

Difficulty

The obvious approach is to optimize pointwise in λ(t)\lambda(t)λ(t). This fails because WWW at duration ttt depends on the whole demand below ttt through the cumulative load, and on Λ2\Lambda_2Λ2​, so the objective is a nonlocal, nonconvex functional of the demand schedule. A second obvious idea is to compare with the best single service. That comparison shows only that some non-degenerate line beats one particular collapsed line. It neither produces an optimum nor rules out an optimum with an atom. Existence also needs an argument: the feasible set of measures is not compact in any naive sense, because the support can drift and the load constraint is strict. Finally, the sign of P′(t‾)P'(\underline t)P′(t​) depends on where the root of the transcendental equation (A–35) lies, and the paper controls this only asymptotically.

Formalization scope

Everything is real-valued. A service line is a Lean structure with endpoints lo, hi and a measure μ : Measure ℝ. Admissibility requires:

  • μ\muμ is finite and lives on [t‾,tˉ][\underline t,\bar t][t​,tˉ] with 0≤t‾≤tˉ0\le\underline t\le\bar t0≤t​≤tˉ;
  • μ\muμ charges every right-neighbourhood of t‾\underline tt​ and every left-neighbourhood of tˉ\bar ttˉ, so the endpoints are the shortest and longest services actually offered;
  • Λ1<1\Lambda_1<1Λ1​<1.

Feasibility adds Λ0≤Λ\Lambda_0\le\LambdaΛ0​≤Λ. The waiting time is

W(t)=Λ2/2(1−L−(t))(1−L+(t)),W(t)=\frac{\Lambda_2/2}{(1-L^-(t))(1-L^+(t))},W(t)=(1−L−(t))(1−L+(t))Λ2​/2​,

with L−L^-L− and L+L^+L+ the loads of durations <t<t<t and ≤t\le t≤t. This is eq. (7) for densities. At atoms it is Cobham's non-preemptive priority wait, with ties served FIFO, and for a single service it is the M/D/1 value Λ2/(2(1−Λ1))\Lambda_2/(2(1-\Lambda_1))Λ2​/(2(1−Λ1​)).

Point masses are allowed on purpose. If demand were restricted to densities, a collapsed line would be infeasible and t‾<tˉ\underline t<\bar tt​<tˉ would hold by construction. Letting the endpoints float freely, beyond the support, would trivialize it in the same way. Both encodings are therefore excluded.

The following conventions are committed:

  • the reduced problem (9) is used instead of the mechanism of Proposition 1;
  • Δ=0\Delta=0Δ=0 is built in, with no parameter for θ‾\underline\thetaθ​;
  • VVV is uncapped;
  • the price derivatives at t‾\underline tt​ and tˉ\bar ttˉ are one-sided, taken within [t‾,tˉ][\underline t,\bar t][t​,tˉ], because PPP has a kink at tˉ\bar ttˉ;
  • existence of an optimum is stated explicitly;
  • uniqueness of the optimum or of the root of (A–35) is not claimed;
  • the hypotheses b>0b>0b>0 and Λ>0\Lambda>0Λ>0 are added, since they are implicit in the paper.

A complete development needs: integration against finite measures on R\mathbb RR; existence of optimal measures under moment and load constraints; first-order conditions for the nonlocal functional QQQ; and real analysis of FFF. The SPT waiting-time functional and Corollary 1's queue-length bound are reusable for other priority-queue design problems. Contributions are welcome on any milestone, in particular Corollary 1 and the existence part of Lemma A7.

Selected references

  • L. Debo and C. Li, Design and Pricing of Discretionary Service Lines, SSRN working paper 3054741, October 2017. https://ssrn.com/abstract=3054741 (published in Management Science, https://doi.org/10.1287/mnsc.2020.3670)
  • T. E. Phipps Jr. and W. R. Van Voorhis, Machine repair as a priority waiting-line problem, Operations Research 4(1), 76–86, 1956. https://doi.org/10.1287/opre.4.1.76
  • A. Cobham, Priority assignment in waiting line problems, Journal of the Operations Research Society of America 2(1), 70–76, 1954. https://doi.org/10.1287/opre.2.1.70
  • M. Mussa and S. Rosen, Monopoly and product quality, Journal of Economic Theory 18(2), 301–317, 1978. https://doi.org/10.1016/0022-0531(78)90085-6
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