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Linear algebraQuantum Error CorrectionQuantum Information·Captain: mikedeng1

Towards a Unified Framework for Approximate Quantum Error Correction: The Transpose Channel Corrects a Subsystem Code up to the Operator Norm of the PerturbationResearch Paper

Motivation

Quantum error correction protects quantum information from noise by storing it in a code and undoing the damage with a recovery operation. The textbook theory, the Knill–Laflamme conditions, characterizes codes that can be corrected perfectly. Real noise rarely admits perfect correction, and codes that are only approximately correctable can perform better than perfect ones: they can use fewer physical resources for a given target fidelity. Approximate quantum error correction (AQEC) asks for algebraic conditions that tell, from the noise and the code alone, how well a code can be corrected.

Mandayam and Ng (arXiv:1202.5139, Phys. Rev. A 2012) extend an earlier AQEC framework for subspace codes (Ng and Mandayam, arXiv:0909.0931, 2010) to subsystem codes, where information is stored in one tensor factor AAA of a subspace HA⊗HB\mathcal H_A\otimes\mathcal H_BHA​⊗HB​ and the factor BBB is a gauge whose state does not matter. Subsystem codes include noiseless subsystems and the Bacon–Shor family, and they are the natural setting for operator quantum error correction (Kribs, Laflamme and Poulin, arXiv:quant-ph/0412076, 2005).

Setting

The system space is H=HA⊗HB⊕K\mathcal H=\mathcal H_A\otimes\mathcal H_B\oplus\mathcal KH=HA​⊗HB​⊕K, with HA\mathcal H_AHA​, HB\mathcal H_BHB​ finite dimensional; PPP is the projector onto HAB=HA⊗HB\mathcal H_{AB}=\mathcal H_A\otimes\mathcal H_BHAB​=HA​⊗HB​ and PA,PBP_A,P_BPA​,PB​ the identities of the factors. The code C\mathcal CC is the set of all product states ρA⊗ρB\rho_A\otimes\rho_BρA​⊗ρB​, with ρA,ρB\rho_A,\rho_BρA​,ρB​ density operators.

The noise E\mathcal EE is a completely positive, trace-preserving (CPTP) map with Kraus operators E1,…,EN:HAB→HE_1,\dots,E_N:\mathcal H_{AB}\to\mathcal HE1​,…,EN​:HAB​→H:

E(ρ)=∑iEiρEi†,∑iEi†Ei=P.\mathcal E(\rho)=\sum_iE_i\rho E_i^\dagger,\qquad \sum_iE_i^\dagger E_i=P .E(ρ)=i∑​Ei​ρEi†​,i∑​Ei†​Ei​=P.

Write PE\mathcal P_{\mathcal E}PE​ for the support of E(P)=∑iEiEi†\mathcal E(P)=\sum_iE_iE_i^\daggerE(P)=∑i​Ei​Ei†​. A recovery is a CP map R:B(PE)→B(HAB)\mathcal R:\mathcal B(\mathcal P_{\mathcal E})\to\mathcal B(\mathcal H_{AB})R:B(PE​)→B(HAB​) that is trace preserving on PE\mathcal P_{\mathcal E}PE​.

The fidelity of states is F(ρ,σ)=trρ1/2σρ1/2F(\rho,\sigma)=\mathrm{tr}\sqrt{\rho^{1/2}\sigma\rho^{1/2}}F(ρ,σ)=trρ1/2σρ1/2​. The fidelity loss of the code state ρ\rhoρ under E\mathcal EE and R\mathcal RR compares the information in AAA before and after:

ηR{ρ}=1−F2(trB ρ, trB[(R∘E)(ρ)]).\eta_{\mathcal R}\{\rho\}=1-F^2\big(\mathrm{tr}_B\,\rho,\ \mathrm{tr}_B[(\mathcal R\circ\mathcal E)(\rho)]\big).ηR​{ρ}=1−F2(trB​ρ, trB​[(R∘E)(ρ)]).

The code is ϵ\epsilonϵ-correctable on AAA under E\mathcal EE when some recovery has ηR{ρ}≤ϵ\eta_{\mathcal R}\{\rho\}\le\epsilonηR​{ρ}≤ϵ for every ρ∈C\rho\in\mathcal Cρ∈C.

The transpose channel RP\mathcal R_PRP​ is the recovery with Kraus operators

RiP=P Ei† E(P)−1/2,R^P_i=P\,E_i^\dagger\,\mathcal E(P)^{-1/2},RiP​=PEi†​E(P)−1/2,

the inverse square root being taken on the support of E(P)\mathcal E(P)E(P).

Formalization targets

Goal: Corollary 3

Suppose that, for all i,ji,ji,j,

PEi†E(P)−1/2EjP=PA⊗Bij+Δij(12)PE_i^\dagger\mathcal E(P)^{-1/2}E_jP=P_A\otimes B_{ij}+\Delta_{ij}\qquad(12)PEi†​E(P)−1/2Ej​P=PA​⊗Bij​+Δij​(12)

with BijB_{ij}Bij​ operators on HB\mathcal H_BHB​ and Δij\Delta_{ij}Δij​ operators on HAB\mathcal H_{AB}HAB​. Then the transpose channel is a recovery, and for every ρ∈C\rho\in\mathcal Cρ∈C

ηRP{ρ}≤∥∑ijΔij†Δij∥,\eta_{\mathcal R_P}\{\rho\}\le\Big\|\sum_{ij}\Delta_{ij}^\dagger\Delta_{ij}\Big\|,ηRP​​{ρ}≤​ij∑​Δij†​Δij​​,

so C\mathcal CC is ϵ\epsilonϵ-correctable on AAA whenever ϵ≥∥∑ijΔij†Δij∥\epsilon\ge\|\sum_{ij}\Delta_{ij}^\dagger\Delta_{ij}\|ϵ≥∥∑ij​Δij†​Δij​∥ (operator norm). The statement holds for every choice of the operators BijB_{ij}Bij​; each choice determines Δij\Delta_{ij}Δij​ and gives a bound.

Theorem 2

Under (12), C\mathcal CC is ϵ\epsilonϵ-correctable on AAA for every ϵ≥ηP\epsilon\ge\eta_Pϵ≥ηP​, where

ηP=max⁡∣ψA,ϕB⟩⟨ϕB∣∑ij[⟨ψA∣Δij†Δij∣ψA⟩−⟨ψA∣Δij†∣ψA⟩⟨ψA∣Δij∣ψA⟩]∣ϕB⟩\eta_P=\max_{|\psi_A,\phi_B\rangle}\langle\phi_B|\sum_{ij}\Big[\langle\psi_A|\Delta^\dagger_{ij}\Delta_{ij}|\psi_A\rangle-\langle\psi_A|\Delta^\dagger_{ij}|\psi_A\rangle\langle\psi_A|\Delta_{ij}|\psi_A\rangle\Big]|\phi_B\rangleηP​=∣ψA​,ϕB​⟩max​⟨ϕB​∣ij∑​[⟨ψA​∣Δij†​Δij​∣ψA​⟩−⟨ψA​∣Δij†​∣ψA​⟩⟨ψA​∣Δij​∣ψA​⟩]∣ϕB​⟩

is the fidelity loss of the transpose channel. Theorem 2 is sharper than Corollary 3; the corollary trades sharpness for a quantity that is easy to compute.

Milestones

The milestones follow the paper's own steps: the pure-state form (5) of the fidelity; the reduction of the worst case over C\mathcal CC to pure product states; trace preservation of RP\mathcal R_PRP​ on PE\mathcal P_{\mathcal E}PE​; the trace-preservation identity of RP∘E\mathcal R_P\circ\mathcal ERP​∘E in terms of Bij,ΔijB_{ij},\Delta_{ij}Bij​,Δij​; the fidelity formula (14) on pure product states; Theorem 2; and the bound of the expression (13) by the operator norm.

Significance

When all Δij\Delta_{ij}Δij​ vanish, (12) is the paper's perfect-correction condition (Theorem 1), and the transpose channel is a perfect recovery. Corollary 3 quantifies the robustness of that statement: a perturbation of size ∥∑Δ†Δ∥\|\sum\Delta^\dagger\Delta\|∥∑Δ†Δ∥ costs at most that much fidelity loss, with an explicit recovery. This turns the search for approximate subsystem codes into a check of a matrix inequality, and it supplies the sufficient half of a characterization whose necessary half (near-optimality of the transpose channel) the paper establishes only in restricted scenarios.

Status: the results are proved in the paper, not formalized. Prove2Me's catalog has no statement of Theorem 2, Corollary 3, or of perfect-correction conditions for subsystem codes. This mission states the subsystem-code model in Lean, with mixed code states and a possibly singular E(P)\mathcal E(P)E(P), and poses each step of the paper's proof as a target. The reduction to pure states needs the joint concavity of the fidelity, which Mathlib does not have; a proof of it is reusable across quantum information theory.

Difficulty

Two steps resist a direct computation. First, the code contains mixed product states, while the fidelity formula (14) is available only for pure ones; the passage from one to the other is the joint concavity of FFF, a consequence of Uhlmann's theorem, not a linear-algebra identity. Second, E(P)\mathcal E(P)E(P) need not be invertible: E(P)−1/2\mathcal E(P)^{-1/2}E(P)−1/2 is a pseudo-inverse, the transpose channel is trace preserving only on PE\mathcal P_{\mathcal E}PE​, and the trace-preservation identity of RP∘E\mathcal R_P\circ\mathcal ERP​∘E needs that each EjE_jEj​ maps into PE\mathcal P_{\mathcal E}PE​. Arguments that treat E(P)−1/2\mathcal E(P)^{-1/2}E(P)−1/2 as an inverse are wrong in general.

Formalization scope

  • HAB\mathcal H_{AB}HAB​ is indexed by a × b with AAA first, matching ⊗ₖ and the published partial trace; H\mathcal HH is a separate finite type o. The noise's Kraus operators are rectangular matrices Matrix o (a × b) ℂ, so PPP, PAP_APA​, PBP_BPB​ are identity matrices and PA⊗BijP_A\otimes B_{ij}PA​⊗Bij​ is 1 ⊗ₖ B i j.
  • Vectors are a → ℂ, unit when star ψ ⬝ᵥ ψ = 1; ∣ψ⟩⟨ψ∣|\psi\rangle\langle\psi|∣ψ⟩⟨ψ∣ is vecMulVec ψ (star ψ).
  • Published definitions are reused: the fidelity (WildeQIT.fidelity =F2=F^2=F2, rootFidelity =F=F=F), the partial trace WildeQIT.partialTraceRight, the channel action PeresTerno.krausUpdate, density matrices PeresTerno.IsDensityMatrix, and the support inverse square root and support projector QReversal.NearOpt.invSqrt, supportProj.
  • A recovery is any finite Kraus family RkR_kRk​ from o to a × b with PE(∑kRk†Rk)PE=PE\mathcal P_{\mathcal E}(\sum_kR_k^\dagger R_k)\mathcal P_{\mathcal E}=\mathcal P_{\mathcal E}PE​(∑k​Rk†​Rk​)PE​=PE​. Full support of E(P)\mathcal E(P)E(P) is not assumed.
  • ϵ\epsilonϵ-correctability is the existence of a recovery with fidelity loss at most ϵ\epsilonϵ on every code state; it is equivalent to the paper's ϵ≥ηop\epsilon\ge\eta_{\mathrm{op}}ϵ≥ηop​ because the minimum defining ηop\eta_{\mathrm{op}}ηop​ is attained. "ϵ≥ηP\epsilon\ge\eta_Pϵ≥ηP​" is stated as a bound on the expression (13) at every pair of unit vectors, with no supremum.
  • The norm in (15) is the operator norm, Mathlib's Matrix.Norms.L2Operator; neither the entrywise sup norm nor the Frobenius norm.

The statements carry no smallness hypothesis on Δij\Delta_{ij}Δij​, quantify over all code states including mixed ones rather than over pure states only, and admit only recoveries that are trace preserving on PE\mathcal P_{\mathcal E}PE​; each of these restrictions would make the goal weaker or trivial.

Needed infrastructure: the continuous functional calculus identities for X−1/2XX−1/2X^{-1/2}XX^{-1/2}X−1/2XX−1/2 and for range inclusions of ∑iEiEi†\sum_iE_iE_i^\dagger∑i​Ei​Ei†​, Kronecker-product algebra, and joint concavity (or Uhlmann's theorem) for the fidelity. Proofs of any milestone, and general fidelity lemmas usable beyond this mission, are welcome.

Selected references

  • P. Mandayam and H. K. Ng, Towards a unified framework for approximate quantum error correction, Phys. Rev. A 86, 012335 (2012). arXiv:1202.5139 (version v2 is the one formalized).
  • H. K. Ng and P. Mandayam, Simple approach to approximate quantum error correction based on the transpose channel, Phys. Rev. A 81, 062342 (2010). arXiv:0909.0931
  • D. Kribs, R. Laflamme and D. Poulin, Unified and generalized approach to quantum error correction, Phys. Rev. Lett. 94, 180501 (2005). arXiv:quant-ph/0412076
  • E. Knill and R. Laflamme, Theory of quantum error-correcting codes, Phys. Rev. A 55, 900 (1997). arXiv:quant-ph/9604034
  • H. Barnum and E. Knill, Reversing quantum dynamics with near-optimal quantum and classical fidelity, J. Math. Phys. 43, 2097 (2002). arXiv:quant-ph/0004088
14 thms3 active usersReviewed
Quantum Information·Captain: Goku

Quantum information can be negativeResearch Paper

Motivation

Given an unknown quantum state distributed over two systems, we determine how much quantum communication is needed to transfer the full state to one system. This communication measures the "partial information" one system needs conditioned on it's prior information. It turns out to be given by an extremely simple formula, the conditional entropy. In the classical case, partial information must always be positive, but we find that in the quantum world this physical quantity can be negative. If the partial information is positive, its sender needs to communicate this number of quantum bits to the receiver; if it is negative, the sender and receiver instead gain the corresponding potential for future quantum communication. We introduce a primitive "quantum state merging" which optimally transfers partial information. We show how it enables a systematic understanding of quantum network theory, and discuss several important applications including distributed compression, multiple access channels and multipartite assisted entanglement distillation (localizable entanglement). Negative channel capacities also receive a natural interpretation.

This mission is the statement-level formalization of Quantum information can be negative (arXiv:quant-ph/0505062v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

6 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Optimal state merging has signed cost S(A|B) (Unnumbered main result: optimal quantum state merging and negative information, PDF p. 2). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Application 1; Figure 2 and all-subset inequalities: An independently operational signed m-sender compression rate region with one decoder, local encoders, free classical messages, separate Bell input/output resources for every sender, and full purifying-reference reconstruction. (hard)
  • Application 2: noiseless coding with side information: A source-consistent definition of E_p(AU:R), including the correct purification/environment channel and one-copy versus regularized rate convention for the asserted one-way iff region. (source-ambiguity)
  • Application 3, equation (2): A two-coordinate signed quantum MAC transmission code with independent reference inputs, individually local encoders, one joint memoryless channel/decoder, explicitly charged sender-decoder Bell resources and the allowed classical messages. (hard)
  • Application 4, equation (3): An arbitrary-number-of-individually-local-helpers i.i.d. EPR-distillation protocol and its asymptotic rate threshold, without initial shared assistance or quantum helper collaboration. (hard)

Selected references

  • Quantum information can be negative, arXiv:quant-ph/0505062v1, https://arxiv.org/abs/quant-ph/0505062v1
17 thms3 active usersReviewed
Quantum Information·Captain: Goku

Reversibility conditions for quantum channels and their applicationsResearch Paper

Motivation

A necessary condition for reversibility (sufficiency) of a quantum channel with respect to complete families of states with bounded rank is obtained. A full description (up to isometrical equivalence) of all quantum channels reversible with respect to orthogonal and nonorthogonal complete families of pure states is given. Some applications in quantum information theory are considered. The main results can be formulated in terms of the operator algebras theory (as conditions for reversibility of channels between algebras of all bounded operators).

This mission is the statement-level formalization of Reversibility conditions for quantum channels and their applications (arXiv:1203.0262v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

26 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 3 (seed paper result): bounded-rank reversibility and the pure-state normal form (Theorem 3 (seed paper result): bounded-rank reversibility and the pure-state normal form, 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

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

  • Theorem 5 (entire printed quantitative statement): The binder or definition of n in the quantitative Kraus-count bound for a general Borel ensemble. (source-ambiguity)
  • Theorem 2 [13], cited background: Separate scope/provenance handling of the cited complete countable-family Petz criterion, without entropy-finiteness assumptions. (hard)

Selected references

  • Reversibility conditions for quantum channels and their applications, arXiv:1203.0262v3, https://arxiv.org/abs/1203.0262v3
39 thms3 active usersReviewed
Quantum Information·Captain: Goku

Quantum states representing perfectly secure bits are always distillableResearch Paper

Motivation

It is proven that recently introduced states with perfectly secure bits of cryptographic key (private states representing secure bit) [K. Horodecki et al., Phys. Rev. Lett. 94, 160502 (2005)] as well as its multipartite and higher dimension generalizations always represent distillable entanglement. The corresponding lower bounds on distillable entanglement are provided. We also present a simple alternative proof that for any bipartite quantum state entanglement cost is an upper bound on distillable cryptographic key in bipartite scenario.

This mission is the statement-level formalization of Quantum states representing perfectly secure bits are always distillable (arXiv:quant-ph/0602176v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

9 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Every exact nontrivial private state has positive GHZ distillable entanglement (Abstract; II.A–B, PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • II.B, last paragraph, suggested POVM extension: A complete multi-outcome locally orthogonal filtering instrument, with specified support notion, failure completion, admissible key-pair family and exact efficiency conclusion. (source-ambiguity)

Selected references

  • Quantum states representing perfectly secure bits are always distillable, arXiv:quant-ph/0602176v2, https://arxiv.org/abs/quant-ph/0602176v2
19 thms3 active usersReviewed
Quantum Information·Captain: Goku

Optimal quantum source coding with quantum information at the encoder and decoderResearch Paper

Motivation

Consider many instances of an arbitrary quadripartite pure state of four quantum systems ABCD. Alice holds the AC part of each state, Bob holds B, while D represents all other parties correlated with ABC. Alice is required to redistribute the C systems to Bob while asymptotically preserving the overall purity. We prove that this is possible using Q qubits of communication and E ebits of shared entanglement between Alice and Bob, provided that Q geq I(C;D|B)/2 and Q+E geq H(C|B), proving the optimality of the Luo-Devetak outer bound. The optimal qubit rate provides the first known operational interpretation of quantum conditional mutual information. We also show how our protocol leads to a fully operational proof of strong subadditivity and uncover a general organizing principle, in analogy to thermodynamics, that underlies the optimal rates.

This mission is the statement-level formalization of Optimal quantum source coding with quantum information at the encoder and decoder (arXiv:0706.2907v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

9 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 5 (Method of types): all simultaneous typical-projection bounds (Theorem 5 (Method of types): all simultaneous typical-projection bounds, PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Theorem 1 (seed): exact quantum state-redistribution rate region: Source-preserving signed quantum/ebit redistribution achievability and exact operational region (hard)
  • Theorem 2: redistribution with generated qubits and ebits: Redistribution with separately generated forward identity channels and ebits (hard)
  • Theorem 3: redistribution with coherent communication: Redistribution with a coherently generated cobit channel (hard)
  • Theorem 4: robust one-shot redistribution protocol — source dimension defect: A uniquely specified normalized CPTP repair of the dimension-defective encoder in Theorem 4 (source-ambiguity)
  • Lemma 1 (Composition lemma [18]): Operational simulation of arbitrary finite resource bundles and their asymptotic composition (hard)
  • Lemma 2 (Cancellation lemma [18]): Operational resource addition/scaling and sublinear catalytic input (hard)
  • §V, unnumbered: optimal classical communication cost: Classical-only redistribution protocols with a finite entanglement trade (hard)
  • §I/§V, unnumbered: optimal successive redistribution: Composable two-step source-preserving redistribution and computed step costs (hard)
  • §V, unnumbered: pure bipartite source redistribution: Zero-rate redistribution with permitted sublinear communication (hard)
  • §V, unnumbered: flagged conditionally decoupled source cost: Flagged conditionally decoupled source construction and its operational cost (hard)
  • §V, unnumbered: redistribution with separate consumed and generated ebits: Source-preserving redistribution with distinct initial and final Bell resources (hard)

Selected references

  • Optimal quantum source coding with quantum information at the encoder and decoder, arXiv:0706.2907v2, https://arxiv.org/abs/0706.2907v2
20 thms3 active usersReviewed
Quantum Information·Captain: Goku

"Squashed Entanglement" - An Additive Entanglement MeasureResearch Paper

Motivation

In this paper, we present a new entanglement monotone for bipartite quantum states. Its definition is inspired by the so-called intrinsic information of classical cryptography and is given by the halved minimum quantum conditional mutual information over all tripartite state extensions. We derive certain properties of the new measure which we call "squashed entanglement": it is a lower bound on entanglement of formation and an upper bound on distillable entanglement. Furthermore, it is convex, additive on tensor products, and superadditive in general. Continuity in the state is the only property of our entanglement measure which we cannot provide a proof for. We present some evidence, however, that our quantity has this property, the strongest indication being a conjectured Fannes type inequality for the conditional von Neumann entropy. This inequality is proved in the classical case.

This mission is the statement-level formalization of "Squashed Entanglement" - An Additive Entanglement Measure (arXiv:quant-ph/0308088v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

18 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Superadditivity and tensor-product additivity (§II, Proposition 4 (p.1 seed), PDF p. 3). 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

  • "Squashed Entanglement" - An Additive Entanglement Measure, arXiv:quant-ph/0308088v3, https://arxiv.org/abs/quant-ph/0308088v3
33 thms3 active usersReviewed
Convex OptimizationOptimizationProbability·Captain: mikedeng1

Universal Barrier is n-Self-Concordant: The Universal Barrier of Every Proper Convex Domain in ℝⁿ Is an n-Self-Concordant BarrierResearch Paper

Motivation

Interior-point methods minimize a linear function over a convex set K⊆RnK\subseteq\mathbb R^nK⊆Rn by following the minimizers of t cTx+φ(x)t\,c^{\mathsf T}x+\varphi(x)tcTx+φ(x), where φ\varphiφ is a self-concordant barrier for KKK. The number of Newton steps the path-following method needs to reach accuracy ϵ\epsilonϵ is O(νlog⁡(1/ϵ))O(\sqrt{\nu}\log(1/\epsilon))O(ν​log(1/ϵ)), where ν\nuν is the barrier's self-concordance parameter. A smaller ν\nuν is a better iteration bound, and the question of the smallest ν\nuν achievable for an arbitrary convex domain is a basic question of the theory.

  • 1994: Nesterov and Nemirovski introduced the universal barrier, defined for every convex domain without lines, and proved it is O(n)O(n)O(n)-self-concordant (Interior-Point Polynomial Algorithms in Convex Programming, SIAM, Theorem 2.5.1). They also showed that no barrier for the simplex or the cube has parameter below nnn.
  • 2015: Bubeck and Eldan introduced the entropic barrier, proved it is (1+o(1))n(1+o(1))n(1+o(1))n-self-concordant, and showed that on convex cones both the universal and the entropic barrier are nnn-self-concordant (arXiv:1412.1587).
  • 2021: Lee and Yue proved that the universal barrier is nnn-self-concordant on every proper convex domain in Rn\mathbb R^nRn, n≥1n\ge1n≥1 (arXiv:1809.03011, Mathematics of Operations Research). This mission formalizes that result.

Setting

A convex domain is a convex set K⊆RnK\subseteq\mathbb R^nK⊆Rn with non-empty interior; it is proper if it contains no line {x+tv:t∈R}\{x+tv:t\in\mathbb R\}{x+tv:t∈R} with v≠0v\neq0v=0. KKK need not be closed or bounded. For x∈int⁡(K)x\in\operatorname{int}(K)x∈int(K) the polar set of KKK with respect to xxx is

K∘(x)={y∈Rn: yT(z−x)≤1  for all z∈K},K^\circ(x)=\{y\in\mathbb R^n:\ y^{\mathsf T}(z-x)\le1\ \text{ for all } z\in K\},K∘(x)={y∈Rn: yT(z−x)≤1  for all z∈K},

a convex body, and the universal barrier is φ(x)=log⁡Voln(K∘(x))\varphi(x)=\log\mathrm{Vol}_n(K^\circ(x))φ(x)=logVoln​(K∘(x)).

A function φ\varphiφ on int⁡(K)\operatorname{int}(K)int(K) is a barrier if φ(x)→+∞\varphi(x)\to+\inftyφ(x)→+∞ as x→∂Kx\to\partial Kx→∂K. A convex, three times continuously differentiable φ\varphiφ is self-concordant if, for all x∈int⁡(K)x\in\operatorname{int}(K)x∈int(K) and h∈Rnh\in\mathbb R^nh∈Rn,

∣D3φ(x)[h,h,h]∣≤2 (D2φ(x)[h,h])3/2,(1)|D^3\varphi(x)[h,h,h]|\le2\,(D^2\varphi(x)[h,h])^{3/2},\tag{1}∣D3φ(x)[h,h,h]∣≤2(D2φ(x)[h,h])3/2,(1)

and ν\nuν-self-concordant if moreover ∣Dφ(x)[h]∣≤(ν D2φ(x)[h,h])1/2|D\varphi(x)[h]|\le(\nu\,D^2\varphi(x)[h,h])^{1/2}∣Dφ(x)[h]∣≤(νD2φ(x)[h,h])1/2 (2).

The proof works with one-dimensional laws. For a convex body LLL and h≠0h\neq0h=0, the marginal density p(L,h;⋅)p(L,h;\cdot)p(L,h;⋅) is the density of yThy^{\mathsf T}hyTh for yyy uniform on LLL. For a density ppp on R\mathbb RR, μ1(p)\mu_1(p)μ1​(p) is its mean, μ22(p)\mu_2^2(p)μ22​(p) its variance and μ33(p)\mu_3^3(p)μ33​(p) its third central moment; μ23(p)=(μ22(p))3/2\mu_2^3(p)=(\mu_2^2(p))^{3/2}μ23​(p)=(μ22​(p))3/2. A density is 1m\tfrac1mm1​-concave if p1/mp^{1/m}p1/m is concave on its support (for m=0m=0m=0: ppp is constant on its support, up to endpoints).

Formalization targets

Goal: Theorem 2

For n≥1 and every proper convex domain K⊆Rn,  φ(x)=log⁡Voln(K∘(x)) is an n-self-concordant barrier for K.\text{For } n\ge1 \text{ and every proper convex domain } K\subseteq\mathbb R^n,\ \ \varphi(x)=\log\mathrm{Vol}_n(K^\circ(x)) \text{ is an } n\text{-self-concordant barrier for } K.For n≥1 and every proper convex domain K⊆Rn,  φ(x)=logVoln​(K∘(x)) is an n-self-concordant barrier for K.

The parameter nnn is exact, so the goal carries no constant to improve.

Milestones

  1. The barrier property of φ\varphiφ.
  2. Brunn's concavity principle for hyperplane sections (Theorem 1 with F=h⊥F=h^\perpF=h⊥): p(L,h;⋅)p(L,h;\cdot)p(L,h;⋅) is 1n−1\tfrac1{n-1}n−11​-concave.
  3. Lemma 2: a non-increasing density on [0,1][0,1][0,1] has mean at most 12\tfrac1221​.
  4. The polynomial inequality f0(γ)≥0f_0(\gamma)\ge0f0​(γ)≥0 for γ≥1\gamma\ge1γ≥1 (§4.1.7).
  5. Proposition 1, inequality (5): for a 1k−1\tfrac1{k-1}k−11​-concave density with 0∈Supp⁡(p)0\in\operatorname{Supp}(p)0∈Supp(p), μ12(p)≤k(k+2)μ22(p)\mu_1^2(p)\le k(k+2)\mu_2^2(p)μ12​(p)≤k(k+2)μ22​(p).
  6. Lemma 3: affine invariance of the family Q\mathcal QQ and of Ξ(p)=∣μ33(p)/μ23(p)∣\Xi(p)=|\mu_3^3(p)/\mu_2^3(p)|Ξ(p)=∣μ33​(p)/μ23​(p)∣.
  7. Lemma 4: the polynomial inequality g(γ,k)≥0g(\gamma,k)\ge0g(γ,k)≥0 for γ≥1\gamma\ge1γ≥1, k≥2k\ge2k≥2.
  8. Proposition 1, inequality (4): for a 1k−1\tfrac1{k-1}k−11​-concave density,
∣μ33(p)∣≤2k+2k k−1k+3 μ23(p).|\mu_3^3(p)|\le2\sqrt{\tfrac{k+2}{k}}\,\tfrac{k-1}{k+3}\,\mu_2^3(p).∣μ33​(p)∣≤2kk+2​​k+3k−1​μ23​(p).
  1. Lemma 1: DφD\varphiDφ, D2φD^2\varphiD2φ, D3φD^3\varphiD3φ at xxx along hhh as polynomials in the moments of p(K∘(x),h;⋅)p(K^\circ(x),h;\cdot)p(K∘(x),h;⋅).
  2. Inequality (9): ℓ(t)=(2t3+6t+4cn)/(1+t2)3/2≤2n+1\ell(t)=(2t^3+6t+4c_n)/(1+t^2)^{3/2}\le2\sqrt{n+1}ℓ(t)=(2t3+6t+4cn​)/(1+t2)3/2≤2n+1​, with cn=(n−1)/(2n)c_n=(n-1)/(2\sqrt n)cn​=(n−1)/(2n​).

Significance

The theorem settles the self-concordance parameter of the universal barrier for every proper convex domain: it is nnn, and by the lower bound of Nesterov and Nemirovski no barrier does better in general. It implies the nnn-self-concordance results for cones as special cases, and it gives a canonical barrier attaining the optimal iteration bound O(nlog⁡(1/ϵ))O(\sqrt n\log(1/\epsilon))O(n​log(1/ϵ)) on any domain. Proposition 1, a pair of sharp moment inequalities for sss-concave distributions, is of independent interest; it extends the third-moment bound for log-concave laws used by Bubeck and Eldan.

The result is proved on paper; none of it is formalized. A complete development would give machine-checked statements of the universal barrier, its derivative formulas, Brunn's principle for hyperplane sections, and the moment inequalities, all of which are reusable for other barrier constructions (the entropic barrier missions on the platform use the same definitions of barrier and self-concordance). The two polynomial inequalities (milestones 4 and 7) are self-contained and the appendix proof of Lemma 4 is long elementary calculus, a natural target for automation.

Difficulty

The derivative formulas reduce nnn-self-concordance to moment inequalities for the marginal of the polar body. The obvious argument uses only log-concavity of marginals (Prékopa–Leindler) and the log-concave third-moment bound; it yields ν=O(n)\nu=O(n)ν=O(n) and loses a constant. Exactness requires the stronger 1n−1\tfrac1{n-1}n−11​-concavity and moment bounds that are sharp for every kkk, attained by k tk−1k\,t^{k-1}ktk−1 on [0,1][0,1][0,1]. Proposition 1 is an extremal problem over an infinite-dimensional class of densities, and the sharp constants surface only as polynomial inequalities in a parameter γ≥1\gamma\ge1γ≥1 whose degree grows with kkk (milestones 4 and 7); Lemma 4 must hold uniformly in the integer k≥2k\ge2k≥2, and small kkk behave differently. The localization lemma the paper cites for the reduction is not in Mathlib. On the analytic side, Lemma 1 requires differentiating log⁡Voln(K∘(x))\log\mathrm{Vol}_n(K^\circ(x))logVoln​(K∘(x)) three times under the integral for a possibly unbounded KKK.

Formalization scope

The space is EuclideanSpace ℝ (Fin n) with Lebesgue measure volume. The goal's conclusion is the published predicate EntropicBarrier.Universal.IsNuSelfConcordantBarrier K φ n: barrier limits at every frontier point within int⁡(K)\operatorname{int}(K)int(K); convexity, C3C^3C3 and inequality (1) on int⁡(K)\operatorname{int}(K)int(K) through the published line-restriction form ConvexOptimization.IsSelfConcordantOn; and (2) in one-sided form, equivalent to the two-sided one. Lemma 1 uses Fréchet derivatives iteratedFDeriv. The universal barrier is a total function; its values off int⁡(K)\operatorname{int}(K)int(K) are junk and never read. All of KKK's standing assumptions (convex, non-empty interior, no line) are bundled in IsProperConvexDomain, together with n≥1n\ge1n≥1.

Three conventions correct slips of the page and are disclosed in each item:

  • sss-concavity is quantified over support points. Definition 5 read literally (for all t1,t2∈Rt_1,t_2\in\mathbb Rt1​,t2​∈R) is satisfied by no probability density, which would make Proposition 1 vacuously true and Brunn's principle false. The formalization uses the paper's own usage, "on its support". This trivializing reading is ruled out by design, and a sanity check exhibits a density satisfying every hypothesis of Proposition 1.
  • Marginals are normalized by their own integral, since Voln−1(slice)/Voln(L)\mathrm{Vol}_{n-1}(\text{slice})/\mathrm{Vol}_n(L)Voln−1​(slice)/Voln​(L) integrates to 1/∥h∥1/\|h\|1/∥h∥; the published section measure is an unnormalized Hausdorff measure, and the normalization removes its constant. Milestones 2 and 9 assume h≠0h\neq0h=0.
  • The family Q\mathcal QQ requires a<ba<ba<b; the degenerate case is the Dirac case the paper treats separately.

Densities are non-negative functions with integral 111, and moments are Bochner integrals; a 1k−1\tfrac1{k-1}k−11​-concave density has bounded support, so they are genuine. Not formalized: Brunn's principle for general kkk, the localization lemma (Theorem 3) and its corollaries, the limiting reductions of §4.1.1–§4.1.5 and §4.2.1, and the internals of Appendix A. Contributions of any of these as supporting lemmas, of Brunn–Minkowski-type tools for sections, and of differentiation-under-the-integral results for polar volumes are welcome.

Selected references

  • Y. T. Lee and M.-C. Yue, Universal Barrier is n-Self-Concordant, Mathematics of Operations Research 46(3), 2021; arXiv:1809.03011v4. https://arxiv.org/abs/1809.03011
  • Yu. Nesterov and A. Nemirovski, Interior-Point Polynomial Algorithms in Convex Programming, SIAM, 1994. https://doi.org/10.1137/1.9781611970791
  • S. Bubeck and R. Eldan, The entropic barrier: a simple and optimal universal self-concordant barrier, COLT 2015; arXiv:1412.1587. https://arxiv.org/abs/1412.1587
  • M. Fradelizi and O. Guédon, The extreme points of subsets of s-concave probabilities and a geometric localization theorem, Discrete & Computational Geometry 31(2), 2004. https://doi.org/10.1007/s00454-003-2868-y
  • S. Brazitikos, A. Giannopoulos, P. Valettas and B.-H. Vritsiou, Geometry of Isotropic Convex Bodies, AMS, 2014. https://doi.org/10.1090/surv/196
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An Optimal Policy for Dynamic Assortment Planning Under Uncapacitated Multinomial Logit Models: The Adaptive-Confidence Trisection Policy Has N-Independent Regret at Most C√TResearch Paper

Learning which products to offer

A retailer that sells NNN substitutable products must decide, for each arriving customer, which subset of products to display. Customer preferences are unknown at the start and have to be learned from purchases, while every suboptimal display costs revenue. This is dynamic assortment planning, a standard problem of revenue management in e-commerce and online advertising, and its learning version is a bandit problem whose arms are the 2N2^N2N subsets of products.

Under the multinomial logit (MNL) choice model the problem has been studied through the regret of a policy over TTT customers (Chen, Wang and Zhou, §2 and Table 1):

  • Rusmevichientong, Shen and Shmoys (2010) analysed the same revenue potential as this paper with a golden-ratio search; their bound involves log⁡N\log NlogN and needs a separability (gap) assumption between candidate assortments.
  • Sauré and Zeevi (2013) also cast MNL assortment learning as regret minimization.
  • Agrawal, Avadhanula, Goyal and Zeevi gave UCB and Thompson-sampling policies with regret O~(NT+N)\tilde O(\sqrt{NT} + N)O~(NT​+N) for assortments of capacity KKK.
  • Chen and Wang (2018) proved an Ω(NT)\Omega(\sqrt{NT})Ω(NT​) lower bound in the capacitated model when K≤N/4K \le N/4K≤N/4.

In the capacitated model the regret must grow with NNN. Chen, Wang and Zhou (arXiv:1805.04785v2, Mathematics of Operations Research 2021) show that without a capacity constraint it need not: a trisection policy achieves regret C1TC_1\sqrt TC1​T​ with a universal constant, and T/384\sqrt T/384T​/384 is a lower bound. This mission formalizes the upper bound.

Setting

There are NNN items with known revenues r1,…,rN∈[0,1]r_1,\dots,r_N \in [0,1]r1​,…,rN​∈[0,1] and unknown utilities v1,…,vN≥0v_1,\dots,v_N \ge 0v1​,…,vN​≥0; the no-purchase option has utility v0=1v_0 = 1v0​=1. In each period t=1,…,Tt = 1,\dots,Tt=1,…,T the retailer offers an assortment St⊆[N]S_t \subseteq [N]St​⊆[N], and the customer buys j∈Stj \in S_tj∈St​ with probability vj/(1+∑i∈Stvi)v_j/(1+\sum_{i\in S_t} v_i)vj​/(1+∑i∈St​​vi​) or buys nothing with probability 1/(1+∑i∈Stvi)1/(1+\sum_{i\in S_t} v_i)1/(1+∑i∈St​​vi​), independently of the past. The expected revenue of SSS is

R(S)=∑j∈Srjvj1+∑j∈Svj,R(S) = \frac{\sum_{j\in S} r_j v_j}{1 + \sum_{j\in S} v_j},R(S)=1+∑j∈S​vj​∑j∈S​rj​vj​​,

and the regret of a policy is Regret=E∑t=1TR(S∗)−R(St)\mathrm{Regret} = \mathbb E\sum_{t=1}^T R(S^*) - R(S_t)Regret=E∑t=1T​R(S∗)−R(St​), where S∗S^*S∗ maximizes RRR over all 2N2^N2N subsets.

The policy rests on two objects. The level set Lθ={i:ri≥θ}\mathcal L_\theta = \{i : r_i \ge \theta\}Lθ​={i:ri​≥θ} collects the items whose revenue is at least θ\thetaθ. The revenue potential F(θ)=R(Lθ)F(\theta) = R(\mathcal L_\theta)F(θ)=R(Lθ​) is a piecewise-constant function of one real variable. Its maximum is F∗=sup⁡θ≥0F(θ)F^* = \sup_{\theta \ge 0} F(\theta)F∗=supθ≥0​F(θ), its right limit is F(θ+)F(\theta^+)F(θ+), and θ∗\theta^*θ∗ denotes the fixed point θ∗=F(θ∗)=F∗\theta^* = F(\theta^*) = F^*θ∗=F(θ∗)=F∗.

The adaptive-confidence trisection policy keeps an interval [aτ,bτ][a_\tau, b_\tau][aτ​,bτ​], starting from [0,1][0,1][0,1]. In epoch τ\tauτ it forms the points xτ=23aτ+13bτx_\tau = \tfrac23 a_\tau + \tfrac13 b_\tauxτ​=32​aτ​+31​bτ​ and yτ=13aτ+23bτy_\tau = \tfrac13 a_\tau + \tfrac23 b_\tauyτ​=31​aτ​+32​bτ​, at distance ετ=yτ−xτ=13(23)τ\varepsilon_\tau = y_\tau - x_\tau = \tfrac13(\tfrac23)^\tauετ​=yτ​−xτ​=31​(32​)τ, and runs nτ=8⌈ετ−2ln⁡(8Tετ2)⌉n_\tau = 8\lceil\varepsilon_\tau^{-2}\ln(8T\varepsilon_\tau^2)\rceilnτ​=8⌈ετ−2​ln(8Tετ2​)⌉ inner iterations. Each inner iteration does two things:

  • while yτy_\tauyτ​ lies inside the current confidence interval [ℓ,u][\ell, u][ℓ,u] for F(yτ)F(y_\tau)F(yτ​), it explores: it offers Lyτ\mathcal L_{y_\tau}Lyτ​​, adds the revenue to the running sum ρt\rho_tρt​, and sets [ℓt,ut]=ρt/t±2ln⁡(8T/t)/t[\ell_t, u_t] = \rho_t/t \pm \sqrt{2\ln(8T/t)/t}[ℓt​,ut​]=ρt​/t±2ln(8T/t)/t​;
  • it then exploits by offering Laτ\mathcal L_{a_\tau}Laτ​​.

At the end of the epoch the policy sets bτ+1=yτb_{\tau+1} = y_\taubτ+1​=yτ​ if u<yτu < y_\tauu<yτ​, and aτ+1=xτa_{\tau+1} = x_\tauaτ+1​=xτ​ otherwise. The policy knows rrr and TTT but never vvv.

Formalization targets

Goal: Theorem 3

There is a universal constant C1>0C_1 > 0C1​>0 such that for every NNN, every horizon TTT, all vi≥0v_i \ge 0vi​≥0 and all ri∈[0,1]r_i \in [0,1]ri​∈[0,1], the adaptive-confidence trisection policy satisfies

E∑t=1TR(S∗)−R(St)≤C1T.\mathbb E\sum_{t=1}^T R(S^*) - R(S_t) \le C_1\sqrt T.Et=1∑T​R(S∗)−R(St​)≤C1​T​.

No gap condition and no bound on vvv is assumed. The constant is left unspecified, as in the paper.

Milestones

  • Structure of FFF. Lemma 1 (revenue-ordered optimality), Corollary 1 (F∗=R(S∗)F^* = R(S^*)F∗=R(S∗)), Lemma 2 (the fixed point, under F∗>0F^* > 0F∗>0), the jump identity (S4)/(S8), and Lemmas 3–4 (FFF is below the diagonal to the right of θ∗\theta^*θ∗ and above it to the left).
  • Concentration. Hoeffding's inequality (Lemma 15, already proved on the platform), the uniform inequality with growing confidence levels (Lemma 8, (11)), and the two tail bounds (S32) and (S33) used in the proof of Lemma 10.
  • Recursion. With ψτω(α,β)\psi^\omega_\tau(\alpha,\beta)ψτω​(α,β) the expected regret of epochs τ,…,τ0\tau,\dots,\tau_0τ,…,τ0​ conditioned on the relative position of aτa_\tauaτ​, bτb_\taubτ​ and θ∗\theta^*θ∗ ((14)): Lemma 11 (Case 3, ψτ3≤αT\psi^3_\tau \le \alpha Tψτ3​≤αT), Lemma 9 (Case 1) and Lemma 10 (Case 2).

Significance

Theorem 3, together with the lower bound of Theorem 4, settles the minimax regret of uncapacitated MNL assortment learning at Θ(T)\Theta(\sqrt T)Θ(T​), independent of the number of products. The policy uses no estimate of the individual utilities, and its cost per period is one level-set offer, so it applies to catalogues where NNN is large compared with TTT. The structural lemmas on the revenue potential (Lemmas 1–4) are standard tools for MNL assortment problems and are reusable by other missions on static and dynamic assortment optimization. Lemma 8 is a MOSS-style concentration inequality whose confidence level grows with the sample size; it is the device that removes the log⁡T\sqrt{\log T}logT​ factor of the paper's baseline bound (Theorem 2).

The result is proved in the paper and is not presented as open; no machine-checked proof of any part of it is known. The platform has the MNL model, the UCB policy of Agrawal et al. (whose bound depends on NNN) and Hoeffding's inequality, but no level-set or trisection analysis. A formal proof would also check the paper's argument, whose printed slips are recorded in the scope section.

Difficulty

The regret concerns a stateful algorithm whose epochs end at random times: an inner iteration takes two periods while exploration is active and one afterwards, and the policy's internal state must be recomputed from the purchase history alone. The obvious argument fixes a confidence level 1/T21/T^21/T2, bounds each epoch's regret on the event that all confidence intervals hold, and sums a geometric series. That argument loses a log⁡T\sqrt{\log T}logT​ factor, and it is the paper's own Theorem 2. Removing the factor needs confidence levels that weaken as data accumulate. A failure is then no longer rare enough to be ignored, so the analysis has to track its cost. This is done by a recursion on conditional expected regrets across three cases (interval to the right of, containing, or to the left of θ∗\theta^*θ∗), in which a wrong decision in one epoch passes to another case with controlled probability. Within an epoch, the purchases made while exploring a level set must be shown to behave like i.i.d. samples with mean F(yτ)F(y_\tau)F(yτ​), although the number of explorations is itself random.

Formalization scope

  • Model. The model is the published MNLBandit.UCB.Setting with every subset admissible: histories are sequences of choices in Option (Fin N) (none = no purchase), policies are deterministic functions of the past choices, and expectations are finite sums over histories. Items and periods are 0-based in Lean; epochs and inner iterations are as on the page.
  • Policy. The policy is defined exactly. Confidence radius 2ln⁡(8T/t)/t\sqrt{2\ln(8T/t)/t}2ln(8T/t)/t​ (δ = 1/T in (12)); nτ=max⁡(1,8⌈(yτ−xτ)−2ln⁡(8T(yτ−xτ)2)⌉)n_\tau = \max(1, 8\lceil(y_\tau-x_\tau)^{-2}\ln(8T(y_\tau-x_\tau)^2)\rceil)nτ​=max(1,8⌈(yτ​−xτ​)−2ln(8T(yτ​−xτ​)2)⌉); trisection weights 2/3,1/32/3, 1/32/3,1/3; the update b←yτb \leftarrow y_\taub←yτ​ if and only if u<yτu < y_\tauu<yτ​; exploitation of Laτ\mathcal L_{a_\tau}Laτ​​ in every inner iteration; exploration only while ℓ≤yτ≤u\ell \le y_\tau \le uℓ≤yτ​≤u.
  • Conventions.
    • The max⁡(1,⋅)\max(1,\cdot)max(1,⋅) matters only for tiny TTT, where the printed nτn_\taunτ​ is 000.
    • The empty assortment is allowed (§3 asks St≠∅S_t \neq \varnothingSt​=∅; R(∅)=0R(\varnothing) = 0R(∅)=0).
    • §3's ri>0r_i > 0ri​>0 is relaxed to Theorem 3's ri∈[0,1]r_i \in [0,1]ri​∈[0,1].
    • FFF is defined on all of R\mathbb RR, and F(θ+)F(\theta^+)F(θ+) is Mathlib's Function.rightLim.
    • θ∗\theta^*θ∗ is defined as F∗F^*F∗.
    • ψ\psiψ is a ratio of finite sums and is 000 on a conditioning event of probability 000.
    • Every O(⋅)O(\cdot)O(⋅) and ≲\lesssim≲ is an existential constant chosen before all other quantities.
  • Added hypotheses. Lemma 2 assumes F∗>0F^* > 0F∗>0, which its proof uses. Lemmas 9 and 10 and (S33) assume T≥25T \ge 25T≥25 and that epoch τ\tauτ can start (∑τ′<τnτ′<T\sum_{\tau'<\tau} n_{\tau'} < T∑τ′<τ​nτ′​<T); without these, log⁡(Tε2)\log(T\varepsilon^2)log(Tε2) can be negative.
  • Repairs. Two printed statements are repaired.
    • (S32) is stated with exp⁡{−nτΔ2/2}\exp\{-n_\tau\Delta^2/2\}exp{−nτ​Δ2/2}, which its printed justification gives; the printed exp⁡{−nτΔ2}\exp\{-n_\tau\Delta^2\}exp{−nτ​Δ2} fails on an explicit instance.
    • Lemma 9 sums from τ′=τ\tau' = \tauτ′=τ, as its proof does, with exponent nτ′n_{\tau'}nτ′​ and the deterministic last epoch τˉ(T)\bar\tau(T)τˉ(T) as upper limit.
  • Ruled out. Three formalizations would make the goal trivial, and none is admissible: a policy that receives vvv (it could offer S∗S^*S∗ in every period); a constant C1C_1C1​ that depends on TTT, NNN or the instance (the regret is at most TTT); and an abstract "trisection oracle" with assumed guarantees in place of the algorithm above.
  • Not included. Theorem 4 (the T/384\sqrt T/384T​/384 lower bound) and its Lemmas 12–14 are not part of the mission, and neither are Theorem 2 and its Lemmas 5–7 (the baseline policy) or Proposition 1.
  • Contributions welcome. Lemmas 1–4 need only finite sums; Lemma 8 and (S32)/(S33) need Hoeffding's inequality and a union bound over sample sizes; the reduction of exploration purchases to i.i.d. samples is reusable for other level-set policies.

Selected references

  • X. Chen, Y. Wang, Y. Zhou, An Optimal Policy for Dynamic Assortment Planning Under Uncapacitated Multinomial Logit Models, arXiv:1805.04785v2, 2019; Mathematics of Operations Research 46(4), 2021. https://arxiv.org/abs/1805.04785
  • S. Agrawal, V. Avadhanula, V. Goyal, A. Zeevi, MNL-Bandit: A Dynamic Learning Approach to Assortment Selection, Operations Research 67(5), 2019. https://arxiv.org/abs/1706.03880
  • X. Chen, Y. Wang, A note on tight lower bound for MNL-bandit assortment selection models, Operations Research Letters 46(5), 534–537, 2018.
  • P. Rusmevichientong, Z.-J. M. Shen, D. B. Shmoys, Dynamic Assortment Optimization with a Multinomial Logit Choice Model and Capacity Constraint, Operations Research 58(6), 2010. https://doi.org/10.1287/opre.1100.0866
  • D. Sauré, A. Zeevi, Optimal Dynamic Assortment Planning with Demand Learning, Manufacturing & Service Operations Management 15(3), 2013. https://doi.org/10.1287/msom.2013.0429
  • K. Talluri, G. van Ryzin, Revenue Management Under a General Discrete Choice Model of Consumer Behavior, Management Science 50(1), 2004. https://doi.org/10.1287/mnsc.1030.0147
  • J.-Y. Audibert, S. Bubeck, Minimax Policies for Adversarial and Stochastic Bandits, COLT 2009.
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Offline Pricing and Demand Learning with Censored Data: a data-driven pricing problem is identifiable if and only if the optimistic and pessimistic prices coincideResearch Paper

Pricing from censored sales data

A retailer who sets a price for a product with limited inventory usually learns about demand from past sales. When the shelf runs empty, sales record the inventory level rather than the demand. Demand above the stock is lost and never observed. This demand censoring is pervasive in retail and inventory data, and it biases naive estimators of demand curves (Besbes and Muharremoglu, Management Science 2013; Ban, Operations Research 2020). Bu, Simchi-Levi and Wang (SSRN 3619625; Management Science, doi:10.1287/mnsc.2022.4382) ask a basic question about offline (historical) data. The retailer has censored sales at a few past prices and must choose a single new price. When can it, with enough data, guarantee near-optimal revenue no matter what the unobserved part of the demand distribution looks like? The paper answers this exactly, and gives an algorithm that achieves the guarantee whenever it is achievable.

Setting

The retailer has y≥0y \ge 0y≥0 units of inventory and chooses a price ppp in a known interval [p‾,pˉ]⊂(0,∞)[\underline p, \bar p] \subset (0,\infty)[p​,pˉ​]⊂(0,∞). Demand is linear: D(p)=ξ−bpD(p) = \xi - bpD(p)=ξ−bp, where the base demand ξ\xiξ is random with c.d.f. FξF_\xiFξ​, and the price sensitivity bbb lies in a known interval [b‾,bˉ]⊂(0,∞)[\underline b, \bar b] \subset (0,\infty)[b​,bˉ]⊂(0,∞). Demand is nonnegative almost surely at every feasible price. Sales are min⁡{D(p),y}\min\{D(p), y\}min{D(p),y}, and under a c.d.f. FFF of ξ\xiξ the expected revenue is RF(p)=p EF[min⁡{ξ−bp,y}]R_F(p) = p\,\mathbb E_F[\min\{\xi - bp, y\}]RF​(p)=pEF​[min{ξ−bp,y}].

Offline data. K≥2K \ge 2K≥2 different historical prices pi∈[p‾,pˉ]p_i \in [\underline p, \bar p]pi​∈[p​,pˉ​] were used with inventories yiy_iyi​. At pair iii there are NiN_iNi​ independent censored sales Sij=min⁡{ξij−bpi, yi}S^j_i = \min\{\xi^j_i - bp_i,\ y_i\}Sij​=min{ξij​−bpi​, yi​}. The data size is N=min⁡iNiN = \min_i N_iN=mini​Ni​. A value of ξ\xiξ is observable only below the observable boundary λ=max⁡i{yi+bpi}\lambda = \max_i\{y_i + bp_i\}λ=maxi​{yi​+bpi​}. Write γ=P[ξ<λ]\gamma = \mathbb P[\xi < \lambda]γ=P[ξ<λ], which is assumed positive. Assumption 1 asks that, below λ\lambdaλ, ξ\xiξ is either discrete with finitely many atoms or has a density, with a slope or density lower bound g‾>0\underline g > 0g​>0.

Ambiguity set. No amount of censored data reveals FξF_\xiFξ​ on [λ,∞)[\lambda,\infty)[λ,∞). The set of distributions consistent with the data is F={F:F(x)=Fξ(x) ∀x<λ}\mathcal F = \{F : F(x) = F_\xi(x)\ \forall x < \lambda\}F={F:F(x)=Fξ​(x) ∀x<λ}. The optimistic and pessimistic revenues are Rmax⁡(p)=max⁡F∈FRF(p)R_{\max}(p) = \max_{F\in\mathcal F} R_F(p)Rmax​(p)=maxF∈F​RF​(p) and Rmin⁡(p)=min⁡F∈FRF(p)R_{\min}(p) = \min_{F\in\mathcal F} R_F(p)Rmin​(p)=minF∈F​RF​(p). Their largest maximizers on [p‾,pˉ][\underline p,\bar p][p​,pˉ​] are the optimistic price pmax⁡∗p^*_{\max}pmax∗​ and the pessimistic price pmin⁡∗p^*_{\min}pmin∗​. With pF∗p^*_FpF∗​ the largest maximizer of RFR_FRF​, the worst-case revenue loss of a price ppp is max⁡F∈F{RF(pF∗)−RF(p)}\max_{F\in\mathcal F}\{R_F(p^*_F) - R_F(p)\}maxF∈F​{RF​(pF∗​)−RF​(p)}.

Identifiability. A data-driven algorithm maps the censored data and the public inputs (yyy, the two intervals, the pairs (pi,yi)(p_i, y_i)(pi​,yi​)) to a feasible price pAp^{\mathcal A}pA. The problem is identifiable (Definition 1) if some algorithm satisfies lim⁡N→∞P[max⁡F∈F{RF(pF∗)−RF(pA)}<ε]=1\lim_{N\to\infty}\mathbb P[\max_{F\in\mathcal F}\{R_F(p^*_F) - R_F(p^{\mathcal A})\} < \varepsilon] = 1limN→∞​P[maxF∈F​{RF​(pF∗​)−RF​(pA)}<ε]=1 for every ε>0\varepsilon > 0ε>0.

Formalization targets

Goal: Theorem 1

The problem is identifiable if and only if

pmax⁡∗=pmin⁡∗.p^*_{\max} = p^*_{\min}.pmax∗​=pmin∗​.

The Lean goal states this in three parts, for every instance satisfying the standing assumptions:

  1. the paper's algorithm D2ACD (Algorithm 1) always prices in [p‾,pˉ][\underline p,\bar p][p​,pˉ​], and if pmax⁡∗=pmin⁡∗p^*_{\max} = p^*_{\min}pmax∗​=pmin∗​ it satisfies the near-optimality limit;
  2. if pmax⁡∗≠pmin⁡∗p^*_{\max} \ne p^*_{\min}pmax∗​=pmin∗​, every feasible price has worst-case loss at least
γb(γ+1)2 (pmax⁡∗−pmin⁡∗)2>0;\frac{\gamma b}{(\sqrt\gamma+1)^2}\,(p^*_{\max} - p^*_{\min})^2 > 0;(γ​+1)2γb​(pmax∗​−pmin∗​)2>0;
  1. identifiable   ⟺  pmax⁡∗=pmin⁡∗\iff p^*_{\max} = p^*_{\min}⟺pmax∗​=pmin∗​.

Milestones

  • Structure of the robust revenues. Concavity and projection (Proposition 1); closed forms of Rmax⁡R_{\max}Rmax​, Rmin⁡R_{\min}Rmin​ with the extremal distributions (Proposition 2); pmin⁡∗≤pF∗≤pmax⁡∗p^*_{\min} \le p^*_F \le p^*_{\max}pmin∗​≤pF∗​≤pmax∗​ (Proposition 3); the worst-case loss equals max⁡{Rmax⁡(pmax⁡∗)−Rmax⁡(p), Rmin⁡(pmin⁡∗)−Rmin⁡(p)}\max\{R_{\max}(p^*_{\max}) - R_{\max}(p),\ R_{\min}(p^*_{\min}) - R_{\min}(p)\}max{Rmax​(pmax∗​)−Rmax​(p), Rmin​(pmin∗​)−Rmin​(p)} (Proposition 7); the lower bound on the minimax loss Δ\DeltaΔ (Proposition 6).
  • Concentration. Hoeffding (Lemma A.1, already proved on the platform), Dvoretzky–Kiefer–Wolfowitz for an arbitrary c.d.f. (Lemma A.2), and a uniform deviation bound for bounded monotone functions (Lemma A.3).
  • Analysis of D2ACD. Consistency of the sensitivity estimate b^\hat bb^ (Lemma 1), of the empirical revenue (Lemma D.1) and of the empirical uncensored fraction (Lemma D.2). Uniform convergence of the empirical robust revenues (Lemma 2). The sample-complexity bound N(ε,δ)=Cε−2log⁡(8K/δ)N(\varepsilon,\delta) = C\varepsilon^{-2}\log(8K/\delta)N(ε,δ)=Cε−2log(8K/δ) with the paper's explicit constant CCC (Theorem 2).

Significance

Theorem 1 separates censored-data pricing problems into two classes. In identifiable ones, more data eventually yields near-optimal prices. In the others, a positive loss persists however large the sample, and the right benchmark is the minimax loss Δ\DeltaΔ. The criterion is checkable in terms of two robust optimization problems, the maximax and the maximin. The constructive half comes with an algorithm that uses only observable data and has sample complexity O(ε−2log⁡(1/δ))O(\varepsilon^{-2}\log(1/\delta))O(ε−2log(1/δ)), matching data-driven newsvendor results without censoring (Levi, Perakis and Uichanco, Operations Research 2015).

The results are proved in the paper. None of them, and none of the model, is formalized. The mission formalizes the model, the ambiguity set, the algorithm and the full chain of the proof. It includes two concentration inequalities not yet available in Lean in the needed form: DKW with Massart's constant for distributions with atoms, and a uniform bound over monotone function classes.

Difficulty

The algorithm sees only the censored data. A proof that silently uses bbb or FξF_\xiFξ​ to pick the price does not establish the theorem. The obvious estimator of bbb, least squares on observed sales, is biased by censoring. D2ACD instead regresses empirical quantiles at the level γ^min⁡\hat\gamma_{\min}γ^​min​, below which the data are uncensored. Its analysis needs a lower bound on the slope of the c.d.f. (Assumption 1), and a uniform-in-price comparison of piecewise empirical revenues whose breakpoint p~^\hat{\tilde p}p~​^​ is itself random. On the other side, the lower bound requires the exact extremal distributions in F\mathcal FF. The optimistic one sends the unobserved mass beyond every relevant demand level. The pessimistic one puts it at the boundary λ\lambdaλ.

Formalization scope

Representation. c.d.f.s are probability measures on R\mathbb RR. F∈FF \in \mathcal FF∈F means agreement with FξF_\xiFξ​ on every half-line (−∞,x](-\infty, x](−∞,x], x<λx < \lambdax<λ, so an atom at λ\lambdaλ is allowed. Rmax⁡R_{\max}Rmax​, Rmin⁡R_{\min}Rmin​, the worst-case loss and Δ\DeltaΔ are defined as suprema and infima. Their attainment is part of the milestones, so no statement is true through a junk value. "max⁡{arg⁡max⁡}\max\{\arg\max\}max{argmax}" is the supremum of the set of maximizers. The data are base-demand samples ξij\xi^j_iξij​ under the product law, mapped to censored sales. An algorithm is a function of the sample sizes and the censored sales for fixed public inputs. Failure probabilities are outer measures. The limit N→∞N \to \inftyN→∞ is over all sample-size vectors with min⁡iNi→∞\min_i N_i \to \inftymini​Ni​→∞.

Standing assumptions and disclosed choices. The data equation is Sij=min⁡{ξij−bpi,yi}S^j_i = \min\{\xi^j_i - bp_i, y_i\}Sij​=min{ξij​−bpi​,yi​}; the page drops bbb once. The continuous branch of Assumption 1 bounds the density on [ℓ,λ)[\ell, \lambda)[ℓ,λ), with ℓ\ellℓ a lower bound of the support. The printed [0,λ)[0,\lambda)[0,λ) contradicts nonnegative demand together with γ>0\gamma > 0γ>0. The historical prices are pairwise different, as the text says. The finite-sample statements (Lemmas 1, 2, Theorem 2) are made on the data assumption γ^i>0\hat\gamma_i > 0γ^​i​>0 for all iii, as on p. 10; the goal is not. In D2ACD, b^\hat bb^ is the clamp of the least-squares slope to [b‾,bˉ][\underline b, \bar b][b​,bˉ], which is the arg min of line 9. Ties go to the largest price and the least index. The output is p‾\underline pp​ when some sample is empty.

Trivializing readings ruled out. Definition 1 fixes the instance before asking for an algorithm, so a constant algorithm returning pmax⁡∗p^*_{\max}pmax∗​ witnesses the bare equivalence. For that reason the goal names D2ACD, a definition taking only the public inputs and the censored sales, and states the quantitative lower bound for the other direction. Two sanity instances, one discrete and one uniform, satisfy every standing assumption, so the hypotheses are not vacuous.

Contributions welcome. Proofs of any milestone. The concentration lemmas A.2 and A.3 are reusable well beyond this mission. Propositions 1–3, 6 and 7 are deterministic convex-analysis arguments about the two robust revenue curves and are a natural starting point.

Selected references

  • J. Bu, D. Simchi-Levi, L. Wang, Offline Pricing and Demand Learning with Censored Data, Management Science, 2022 (SSRN 3619625, PDF of 2021-08-23). https://ssrn.com/abstract=3619625, https://doi.org/10.1287/mnsc.2022.4382
  • P. Massart, The tight constant in the Dvoretzky–Kiefer–Wolfowitz inequality, Annals of Probability 18(3), 1990. https://doi.org/10.1214/aop/1176990746
  • W. Hoeffding, Probability inequalities for sums of bounded random variables, Journal of the American Statistical Association 58, 1963. https://doi.org/10.1080/01621459.1963.10500830
  • O. Besbes, A. Muharremoglu, On implications of demand censoring in the newsvendor problem, Management Science 59(6), 1407–1424, 2013.
  • G.-Y. Ban, Confidence intervals for data-driven inventory policies with demand censoring, Operations Research 68(2), 309–326, 2020.
  • R. Levi, G. Perakis, J. Uichanco, The data-driven newsvendor problem: new bounds and insights, Operations Research 63(6), 2015.
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Complexity TheoryOperations ResearchProbability·Captain: mikedeng1

Bayesian Decision Making in Groups is Hard: In the Vertex-Cover Reduction, Small and Large Covers Force Opposite Exponentially Concentrated Beliefs at Time TwoResearch Paper

Motivation

Models of Bayesian social learning describe agents in a network who each receive a private signal about an unknown state of the world, observe the actions of their neighbours over time, and act optimally given everything they have seen. They are used in economics, operations research and the study of collective decision making to ask whether groups aggregate dispersed information, and they presuppose that every agent can carry out the Bayesian update. Hązła, Jadbabaie, Mossel and Rahimian (arXiv:1705.04770, Operations Research 2021) show that this presupposition fails in general: already at the second round of interaction, computing a Bayesian agent's action is NP-hard (their Theorem 1). The proof is a reduction from approximate VERTEX-COVER. This mission formalizes the mathematical core of that reduction: in the network built from a graph, the belief of one designated agent at time two is pushed to opposite extremes by graphs with small vertex covers and by graphs whose vertex covers are all large.

Setting

A finite set of agents is given, and every agent iii has a neighbourhood Ni\mathcal N_iNi​ of agents whose actions she observes, with i∈Nii \in \mathcal N_ii∈Ni​. The state is θ∈{0,1}\theta \in \{0,1\}θ∈{0,1}, drawn from the uniform prior ν(0)=ν(1)=12\nu(0) = \nu(1) = \tfrac12ν(0)=ν(1)=21​. Agent iii receives a private signal si∈{0,1}s_i \in \{0,1\}si​∈{0,1} with law Pi,θ\mathbb P_{i,\theta}Pi,θ​; conditionally on θ\thetaθ the signals are independent, so a signal profile sss has probability Pθ(s)=∏iPi,θ(si)\mathbb P_\theta(s) = \prod_i \mathbb P_{i,\theta}(s_i)Pθ​(s)=∏i​Pi,θ​(si​).

At every time t=0,1,2,…t = 0, 1, 2, \dotst=0,1,2,… agent iii knows her own signal and the actions aj,τa_{j,\tau}aj,τ​ of all j∈Nij \in \mathcal N_ij∈Ni​ at times τ<t\tau < tτ<t. Her information set Ii,t(s)\mathcal I_{i,t}(s)Ii,t​(s) is the set of profiles s′s's′ that agree with sss in sis_isi​ and in all those actions. Her belief is the posterior (4)

μi,t(θ)=ν(θ)∑s′∈Ii,tPθ(s′)∑θ′ν(θ′)∑s′∈Ii,tPθ′(s′),\mu_{i,t}(\theta) = \frac{\nu(\theta)\sum_{s' \in \mathcal I_{i,t}} \mathbb P_\theta(s')}{\sum_{\theta'} \nu(\theta')\sum_{s' \in \mathcal I_{i,t}} \mathbb P_{\theta'}(s')},μi,t​(θ)=∑θ′​ν(θ′)∑s′∈Ii,t​​Pθ′​(s′)ν(θ)∑s′∈Ii,t​​Pθ​(s′)​,

and in the binary action model (utility 1(a=θ)\mathbf 1(a = \theta)1(a=θ)) her action ai,ta_{i,t}ai,t​ is the more likely state, with ties broken towards 000. Actions at time ttt depend on information sets at time ttt, which depend on actions at earlier times, so all of these are defined together by recursion on ttt. The log-belief ratio is ϕi,t=log⁡(μi,t(1)/μi,t(0))\phi_{i,t} = \log(\mu_{i,t}(1)/\mu_{i,t}(0))ϕi,t​=log(μi,t​(1)/μi,t​(0)).

The reduction network for a simple graph GGG with nnn vertices and mmm edges has n+m+2n + m + 2n+m+2 agents: a vertex agent τv\tau_vτv​ for each vertex, observing only herself, with Pτ,1(1)=pˉ=0.4\mathbb P_{\tau,1}(1) = \bar p = 0.4Pτ,1​(1)=pˉ​=0.4 and Pτ,0(1)=p‾=0.3\mathbb P_{\tau,0}(1) = \underline p = 0.3Pτ,0​(1)=p​=0.3; an edge agent εe\varepsilon_eεe​ for each edge e={u,w}e = \{u,w\}e={u,w}, observing τu\tau_uτu​, τw\tau_wτw​ and herself, with an uninformative signal; an agent κ\kappaκ observing only herself; and the agent iii, with an uninformative signal, observing κ\kappaκ and all edge agents. With qˉ(α)=pˉα(1−pˉ)1−α\bar q(\alpha) = \bar p^\alpha(1-\bar p)^{1-\alpha}qˉ​(α)=pˉ​α(1−pˉ​)1−α, q‾(α)=p‾α(1−p‾)1−α\underline q(\alpha) = \underline p^\alpha(1-\underline p)^{1-\alpha}q​(α)=p​α(1−p​)1−α and q~(α)=log⁡(qˉ(α)/q‾(α))\tilde q(\alpha) = \log(\bar q(\alpha)/\underline q(\alpha))q~​(α)=log(qˉ​(α)/q​(α)), agent κ\kappaκ's signal is chosen so that

λκ(0)=log⁡Pκ,1(0)Pκ,0(0)=−n2(q~(0.998)+q~(0.999)).\lambda_\kappa(0) = \log\frac{\mathbb P_{\kappa,1}(0)}{\mathbb P_{\kappa,0}(0)} = -\frac n2\bigl(\tilde q(0.998) + \tilde q(0.999)\bigr).λκ​(0)=logPκ,0​(0)Pκ,1​(0)​=−2n​(q~​(0.998)+q~​(0.999)).

Agent iii's observed history is: every edge agent announces aε,1=1a_{\varepsilon,1} = 1aε,1​=1, and κ\kappaκ announces aκ,0=0a_{\kappa,0} = 0aκ,0​=0.

Formalization targets

Goal: Theorem 6, belief clauses (p. 27)

There are c>0c > 0c>0 and NNN such that for every n≥Nn \ge Nn≥N, every graph GGG on nnn vertices, every admissible signal structure of κ\kappaκ, and every signal profile producing the observed history:

G has a vertex cover of size≤0.85n  ⟹  μi,2(1)<e−cn,G \text{ has a vertex cover of size} \le 0.85n \implies \mu_{i,2}(1) < e^{-cn},G has a vertex cover of size≤0.85n⟹μi,2​(1)<e−cn, every vertex cover of G has size≥0.999n  ⟹  μi,2(0)<e−cn.\text{every vertex cover of } G \text{ has size} \ge 0.999n \implies \mu_{i,2}(0) < e^{-cn}.every vertex cover of G has size≥0.999n⟹μi,2​(0)<e−cn.

The constant ccc is not fixed: the paper writes exp⁡(−Ω(n))\exp(-\Omega(n))exp(−Ω(n)).

Milestones

  1. Example 1, (3), p. 8: time-zero actions reveal informative signals, and ϕi,1=∑j∈Niλj\phi_{i,1} = \sum_{j \in \mathcal N_i}\lambda_jϕi,1​=∑j∈Ni​​λj​.
  2. Fact 1, p. 28: aε,1=1a_{\varepsilon,1} = 1aε,1​=1 iff one of the edge's endpoints has signal 111.
  3. Fact 2, p. 28: the vertices with signal 111 form a vertex cover iff all edge agents announce 111.
  4. (12), p. 29: ϕi,2\phi_{i,2}ϕi,2​ is the log-ratio of ∑Σ^pˉ∣Σ^∣(1−pˉ)n−∣Σ^∣\sum_{\hat\Sigma}\bar p^{|\hat\Sigma|}(1-\bar p)^{n-|\hat\Sigma|}∑Σ^​pˉ​∣Σ^∣(1−pˉ​)n−∣Σ^∣ and ∑Σ^p‾∣Σ^∣(1−p‾)n−∣Σ^∣\sum_{\hat\Sigma}\underline p^{|\hat\Sigma|}(1-\underline p)^{n-|\hat\Sigma|}∑Σ^​p​∣Σ^∣(1−p​)n−∣Σ^∣ over vertex covers Σ^\hat\SigmaΣ^, plus λκ(0)\lambda_\kappa(0)λκ​(0).
  5. (13), p. 29: in the NO case, ϕi,2>n2(q~(0.999)−q~(0.998))\phi_{i,2} > \frac n2(\tilde q(0.999) - \tilde q(0.998))ϕi,2​>2n​(q~​(0.999)−q~​(0.998)).
  6. Theorem 7, pp. 29–30: Pr⁡{∑ksk≥αn}≤exp⁡(−nDKL(α∥p))\Pr\{\sum_k s_k \ge \alpha n\} \le \exp(-nD_{KL}(\alpha\|p))Pr{∑k​sk​≥αn}≤exp(−nDKL​(α∥p)) for i.i.d. Bernoulli(ppp) and p≤α≤1p \le \alpha \le 1p≤α≤1.
  7. (16), p. 30: P1{∣Σ∣>0.998n}≤exp⁡(−nDKL(0.998∥0.4))<0.41n\mathbb P_1\{|\Sigma| > 0.998n\} \le \exp(-nD_{KL}(0.998\|0.4)) < 0.41^nP1​{∣Σ∣>0.998n}≤exp(−nDKL​(0.998∥0.4))<0.41n.
  8. (17), p. 30: a set of at most 0.85n0.85n0.85n vertices has P1\mathbb P_1P1​-probability at least qˉ(0.85)n>0.42n\bar q(0.85)^n > 0.42^nqˉ​(0.85)n>0.42n.
  9. (18), p. 30: in the YES case, ϕi,2<nq~(0.998)+log⁡(1+(0.41/0.42)n)−n2(q~(0.999)+q~(0.998))\phi_{i,2} < n\tilde q(0.998) + \log(1 + (0.41/0.42)^n) - \frac n2(\tilde q(0.999) + \tilde q(0.998))ϕi,2​<nq~​(0.998)+log(1+(0.41/0.42)n)−2n​(q~​(0.999)+q~​(0.998)).

Significance

Theorem 6 is the step that turns a statement about vertex covers into a statement about beliefs. Together with the NP-hardness of distinguishing graphs with a vertex cover of size 0.85n0.85n0.85n from graphs with no vertex cover smaller than 0.999n0.999n0.999n (Theorem 5, from Khot, Minzer and Safra's proof of the 2-to-2 games theorem), it shows that no polynomial-time algorithm computes the time-two action of a Bayesian agent unless P = NP, and that even approximating the belief is hard, since the two cases differ by exponentially small versus exponentially close to one. This sets a limit on rational-agent models of social learning as descriptions of behaviour and motivates bounded-rationality alternatives.

The result is proved in the paper; to the best of current knowledge it has not been formalized. The mission produces a machine-checked model of Bayesian group decision making on a network, with information sets defined by recursion on time, reusable for other results about Bayesian learning on graphs, and a finite Chernoff bound in Kullback–Leibler form. The NP-hardness itself is not part of the mission: it needs a model of computation and inherits its hardness from a cited theorem.

Difficulty

The model's information sets are defined by a recursion in which every agent simulates what every neighbour could have seen. The first obstacle is to compute the time-two information set of agent iii in closed form: one must check that the actions of agent iii and κ\kappaκ at earlier times, and of the edge agents at time zero, carry no additional information, and that the edge agents' time-one actions reveal exactly whether the vertex signals form a vertex cover. Then the posterior becomes a ratio of two weighted counts of vertex covers. A naive bound comparing the two sums term by term does not separate the YES and NO cases, because the sums are dominated by different covers; in the YES case the large covers must be discarded using a tail bound whose exponent beats the likelihood of a single small cover, which is where the constants 0.41<0.420.41 < 0.420.41<0.42 enter.

Formalization scope

States, signals and actions are Bool (false = 0). A network is BinNet (neighbourhoods with i∈Nii \in \mathcal N_ii∈Ni​, and Pi,θ(1)\mathbb P_{i,\theta}(1)Pi,θ​(1)); post, mapAct, infoSet, act, logBelief are (4), the MAP action with ties to 000, Ii,t\mathcal I_{i,t}Ii,t​, ai,ta_{i,t}ai,t​ and ϕi,t\phi_{i,t}ϕi,t​. Information sets contain the conjunct si′=sis'_i = s_isi′​=si​ from the history of (1). The reduction network is vcNet G k₀ k₁ for G : SimpleGraph (Fin n), on the agent type Agent n G (vertex agents, edge agents indexed by G.edgeSet, iAg, kap), with kθ=Pκ,θ(0)k_\theta = \mathbb P_{\kappa,\theta}(0)kθ​=Pκ,θ​(0) quantified over all pairs in (0,1)(0,1)(0,1) with log⁡(k1/k0)=λκ(0)\log(k_1/k_0) = \lambda_\kappa(0)log(k1​/k0​)=λκ​(0). Vertex covers are Mathlib's SimpleGraph.IsVertexCover. Decimals are exact rationals; 0.85n0.85n0.85n, 0.998n0.998n0.998n, 0.999n0.999n0.999n are compared as real numbers. Probabilities of events on the vertex signals are written as finite sums of p∣C∣(1−p)n−∣C∣p^{|C|}(1-p)^{n-|C|}p∣C∣(1−p)n−∣C∣ over subsets CCC. DKLD_{KL}DKL​ is the published bernoulliRelativeEntropy. nnn is the number of graph vertices, not of agents.

The goal is about the model's own posterior on the model's own information set, for every profile on which the model's actions produce the history; it is not stated about a hand-written ratio of sums, which would skip the model. The constants ccc and NNN are quantified before the graph and before κ\kappaκ's parameters, so they cannot depend on the instance. The complexity clauses of Theorem 6 (a polynomial-time reduction, the bounds (9)) and Theorem 1's NP-hardness are not formalized.

Contributions welcome: closed-form computations of early information sets in the model, the finite Chernoff bound (Theorem 7; the published Proved MassartDKW.Binom.comment_3 is the strict-tail Cramér–Chernoff bound for binomial n p), and the numerical inequalities of (16) and (17).

Selected references

  • J. Hązła, A. Jadbabaie, E. Mossel, M. A. Rahimian, Bayesian Decision Making in Groups is Hard, arXiv:1705.04770v4, 2019; Operations Research 69(2), 2021. https://arxiv.org/abs/1705.04770
  • S. Khot, D. Minzer, M. Safra, Pseudorandom sets in Grassmann graph have near-perfect expansion, FOCS 2018. https://doi.org/10.1109/FOCS.2018.00062
  • P. Massart, The tight constant in the Dvoretzky–Kiefer–Wolfowitz inequality, Annals of Probability 18(3), 1990. https://doi.org/10.1214/aop/1176990746
13 thms3 active usersReviewed
CombinatoricsOperations ResearchOptimization·Captain: Shuze Chen

Submodular Maximization over Multiple Matroids via Generalized Exchange Properties: Polynomial approximation for monotone submodular maximizationResearch Paper

Motivation

Selecting a valuable subset subject to several simultaneous restrictions is a common combinatorial optimization problem. A facility may contribute less after nearby facilities have already been selected; a collection of observations may provide overlapping information. Such diminishing returns are captured by submodular objectives. Matroid constraints describe families of admissible selections that are closed under deletion and satisfy an exchange rule. Requiring a selection to satisfy several matroids permits overlapping restrictions on the same elements.

Lee, Sviridenko and Vondrák study this model with access to objective values and independence tests through oracles. Their main monotone guarantee is a polynomial approximation factor of 1/(k+δ)1/(k+\delta)1/(k+δ) for any fixed number k≥2k\ge2k≥2 of matroids and fixed δ>0\delta>0δ>0. The source compares this with the earlier 1/(k+1)1/(k+1)1/(k+1) greedy guarantee. This mission formalizes the published monotone result and its supporting exchange statements, with the constants and algorithmic quantifiers intact (Introduction and Theorem 3.1).

Setting

The ground set is a finite set NNN of nnn elements. A submodular function assigns a real number f(S)f(S)f(S) to every subset S⊆NS\subseteq NS⊆N and satisfies

f(A∪B)+f(A∩B)≤f(A)+f(B).f(A\cup B)+f(A\cap B)\le f(A)+f(B).f(A∪B)+f(A∩B)≤f(A)+f(B).

All objective values in the faithful source statements are nonnegative. For the headline theorem the function is also nondecreasing: A⊆BA\subseteq BA⊆B implies f(A)≤f(B)f(A)\le f(B)f(A)≤f(B). The empty set need not have value zero.

A matroid on NNN is a family of independent sets containing the empty set, closed under taking subsets, and satisfying augmentation: a smaller independent set can gain an element from a larger independent set while remaining independent. There are kkk such matroids, all on the same ground set. A set is common independent, or feasible, when it is independent in every one of them. The quantity OPT\mathrm{OPT}OPT is the maximum of fff over feasible subsets. This maximum exists even when NNN is empty, since there are finitely many subsets and the empty set is feasible.

An algorithm receives a value oracle for fff and one independence oracle for each matroid. A value query specifies a subset and returns its value; an independence query specifies a matroid and a subset and returns a yes-or-no answer. Real arithmetic and comparisons use the unit-cost oracle convention. No table of all objective values is supplied (Introduction, p. 795).

Formalization targets

The goal is the first sentence of Theorem 3.1. For each fixed k≥2k\ge2k≥2 and δ>0\delta>0δ>0, there must exist one finite oracle program and polynomial constants, depending only on those fixed parameters, such that on every instance it halts and returns a feasible set SSS with

f(S)≥OPTk+δ.f(S)\ge\frac{\mathrm{OPT}}{k+\delta}.f(S)≥k+δOPT​.

The time bound includes initialization, oracle queries, subset processing, unsuccessful searches, and output. It is not merely a bound on the number of improving moves (Theorem 3.1, p. 803).

The eleven supporting milestones follow the source's numbered statements. They cover perfect matching for equal-size independent sets; irreducible cycle covers; the independence consequence of a unique perfect matching; feasibility of irreducible cycles; feasible path and cycle covers; exact-cover addition; generalized Rota exchange; bounded-multiplicity exchange for independent sets; exact-cover removal; and exact and approximate local-search inequalities. The order follows the dependencies identified in §§1–3. The exact local-search bound is

(k+1p)f(S)≥f(S∪C)+(k−1+1p)f(S∩C),\left(k+\frac1p\right)f(S)\ge f(S\cup C)+\left(k-1+\frac1p\right)f(S\cap C),(k+p1​)f(S)≥f(S∪C)+(k−1+p1​)f(S∩C),

with a factor 1+ε1+\varepsilon1+ε on the left in the approximate version. Here p≥1p\ge1p≥1 is an integer, CCC is any feasible set, and the objective may be nonmonotone (Lemmas 3.1–3.2).

Significance

The approximation theorem gives a quantitative guarantee for general matroid intersections with a submodular objective. Restricting the constraints to partition matroids, or proving that a good set exists without a polynomial computation, would lose part of the result. The supporting exchange statements also describe how independent sets can be related when individual exchanges cannot simply be combined across constraints (§§2–3).

The mathematics is a published result; this mission asks for machine-checked proofs of its formal statements. The submodularity predicate is reused from an existing published definition. Lemma 2.1 is anchored to an existing Open bijective exchange theorem through a contraction and graph interpretation, rather than posed again. Open means that its proof remains a target. The remaining statements and the operational oracle model are local drafts, and compiling their statements does not prove them.

Difficulty

A chain of individually feasible swaps need not give a feasible simultaneous exchange. The source's distinction between an arbitrary directed cycle and an irreducible one therefore matters. Feasibility of a path or cycle also includes every eligible subpath, not just the whole vertex-set swap. Losing either distinction changes the supporting exchange results (Definitions 2.1–2.2).

Polynomial computation is a separate obligation from local-optimum quality. Literal Figure 1 admits infeasible singleton initialization when loops are present and nontermination at zero value under its non-strict update test. These issues are recorded as findings about the displayed routine, while the existential headline retains all inputs. Two further findings identify missing witness properties and an invalid intermediate path-count estimate in the printed analysis; they do not establish falsity of the numbered local-search inequalities. Proofs must resolve those obligations without importing them as assumptions (pp. 802–803).

Formalization scope

Lean represents NNN by Fin n, subsets by finite sets, objective values by real numbers, and matroids by Mathlib matroids with ground set equal to the whole finite type. Indexed families preserve repeated sets and repeated paths or cycles. Paths may consist of one vertex, cycles may have two vertices, and the cover multiplicity is 2s2^s2s, including s=0s=0s=0. There is no looplessness, normalization, positive-optimum, or equal-cardinality restriction on the headline inputs.

The algorithmic goal uses a finite register-machine language whose only input-dependent operations are the two types of oracle queries. An explicit halt and a bound on the full execution cost are conclusions. Definitions contain neither an approximation guarantee nor an assumed polynomial stopping bound. The terminal predicate for Figure 1 uses strict inequality because the printed update uses greater-than-or-equal. Empty and zero-value inputs belong to the headline theorem even though the literal terminal predicate need not describe them.

The stronger linear-objective sentence of Theorem 3.1, the nonmonotone algorithm of Theorem 4.1, and the tightness examples in §5 are outside this mission. No optional variants are posed. Contributions needed here include the source theorem proofs, the exchange adapter, and the operational algorithm witness and its accounting.

Selected references

  • Jon Lee, Maxim Sviridenko and Jan Vondrák, Submodular Maximization over Multiple Matroids via Generalized Exchange Properties, Mathematics of Operations Research 35(4), 795–806, 2010. Published journal article. All result numbering and page references use this artifact; PDF pages 1–12 correspond to printed pages 795–806.
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Stochastic Networks XIV: Large Deviations for Queues with Many SourcesTextbook

Motivation

Communication connections can demand bandwidth at rates that fluctuate over time. Reserving every connection's peak rate can leave substantial capacity unused, while reserving only its mean rate allows temporary overloads and queueing delays. Effective bandwidth provides a way to express the statistical cost of a source in terms that can be used in admission decisions. Chapter 6 of Kelly and Yudovina's Stochastic Networks develops this question first for an instantaneous aggregate load and then for a resource with a buffer.

The buffered model distinguishes the number of connections from the number of connection classes. The number of classes stays fixed while capacity, buffer size, and the number of connections all grow together. The object of interest is the exponential rate of the probability that the workload exceeds the buffer level. This rate measures rare overloads on a scale where ordinary convergence of probabilities to zero loses the relevant information.

Setting

A source increment Xji[a,b]X_{ji}[a,b]Xji​[a,b] is the work arriving during an interval from connection iii of class jjj. The classes form a finite set JJJ. A source supplies nonnegative, additive increments, with no work on an interval of length zero. Each interval workload is a measurable real random variable. Different source processes are independent, copies within one class have the same process law, and increments have stationary distributions: the law of an interval's workload depends only on its duration. Independence between increments of one source is not required.

Let njn_jnj​ be the natural number of class-jjj sources in a base system. At positive integer scale NNN, there are njNn_jNnj​N copies. The aggregate arrival is

SN[a,b]=∑j∈J∑i=1njNXji[a,b].S^N[a,b]=\sum_{j\in J}\sum_{i=1}^{n_jN}X_{ji}[a,b].SN[a,b]=j∈J∑​i=1∑nj​N​Xji​[a,b].

A server of capacity CNCNCN, where C>0C>0C>0, processes this work. Its infinite-past workload at time zero is the random variable

QN(0)=sup⁡t≥0{SN[−t,0]−CNt}.Q^N(0)=\sup_{t\ge0}\{S^N[-t,0]-CNt\}.QN(0)=t≥0sup​{SN[−t,0]−CNt}.

This is the construction in equation (6.4), not an independently chosen stationary queue size. It can be infinite. With a positive base buffer BBB, the overflow probability is LN=P(QN(0)>BN)L_N=P(Q^N(0)>BN)LN​=P(QN(0)>BN).

The logarithmic moment generating function of a class-jjj increment is

Mj(s,t)=log⁡Eexp⁡(sXj1[0,t]).M_j(s,t)=\log\mathbb E\exp(sX_{j1}[0,t]).Mj​(s,t)=logEexp(sXj1​[0,t]).

Exponential moments are assumed finite locally around zero for each finite duration, following the chapter's MGF convention; a larger tilt may have infinite expectation. The quantity Mj(s,t)M_j(s,t)Mj​(s,t) is the nonsingular expression for the product stαj(s,t)st\alpha_j(s,t)stαj​(s,t) in the book's effective-bandwidth formula.

Formalization targets

The goal is Theorem 6.10, printed page 145 of the supplied Lecture Notes PDF:

lim⁡N→∞1Nlog⁡LN=sup⁡t≥0inf⁡s≥0[∑j∈JnjMj(s,t)−s(B+Ct)].\lim_{N\to\infty}\frac1N\log L_N =\sup_{t\ge0}\inf_{s\ge0} \left[\sum_{j\in J}n_jM_j(s,t)-s(B+Ct)\right].N→∞lim​N1​logLN​=t≥0sup​s≥0inf​​j∈J∑​nj​Mj​(s,t)−s(B+Ct)​.

The supremum over duration remains outside the infimum over tilt. Both the continuous time domain and the infinite horizon are part of the target.

Three source milestones accompany the goal. Equation (6.1) asserts, for a measurable real random variable YYY and s≥0s\ge0s≥0,

P(Y>0)=E1{Y>0}≤EesY,P(Y>0)=\mathbb E\mathbf1_{\{Y>0\}}\le\mathbb E e^{sY},P(Y>0)=E1{Y>0}​≤EesY,

including infinite exponential expectations. Theorem 6.2 asserts the exact logarithmic rate for an iid sum exceeding ncncnc. Its assumptions include a mean below ccc, a positive probability of exceeding ccc, local MGF finiteness, and an optimizing tilt in the interior of the finite-MGF domain. Exercise 6.9 gives both the two-sequence and finite-sum largest-term principles, with finite real rates and positive sequences. It makes no assertion about a countable sum.

Significance

The goal relates the statistical characteristics of individual connections to the overload behavior of a large system. It retains duration as a variable, allowing temporal dependence within a connection to affect the rate. A fixed-time tail probability alone does not describe the workload accumulated from an unlimited past. This distinction is central to the buffered model in Chapter 6.

The formal deliverable specifies the source family, its scaling, the workload construction, and the variational expression in one consistent setting. It also separates extended expectations from finite real expectations, so the meaning of a rare event does not change when its probability is zero. These definitions can support later work on queueing large deviations without requiring a finite-state Markov model.

The local theorem files are declarations to be proved, not completed proofs. A published proved Chernoff bound is retained as a reference for the integrable exponential case. The separately published open Cramér theorem assumes finiteness at every real tilt and a closed tail event; it is not substituted for the chapter's local-MGF, strict-tail statement.

Difficulty

The source explicitly gives only a sketch for Theorem 6.10. Fixed-time exponential limits do not by themselves determine the exponential rate of a sum over infinitely many times. Exercise 6.9 establishes a finite-sum result, so it cannot close this gap. The continuous-time workload also raises a measurability and time-discretization issue. Finding F1 records the missing justification with an explicit array of exponentially small terms whose count grows exponentially.

Finding F4 gives an explicit counterexample to the printed goal, even with positive buffer and mean load below capacity. Independent sources have uniformly random phases of a periodic arrival rate taking values 0, 1, and 2. Each source contributes at most one unit of net input over any interval, so with B=C=1B=C=1B=C=1 the strict overflow probability is zero at every scale. At duration 2, however, the maximum input 3 has probability 1/51/51/5, giving a finite variational value −log⁡5-\log 5−log5. The faithful goal is retained as printed and is expected to be disproved; no corrected variant is proposed. This is a failure of the fixed-time application of Cramér’s theorem at a support endpoint, separate from F1’s infinite-time gap.

Finding F2 concerns a different finite-sample step in the proof of Cramér's theorem: convergence of a tilted-window probability to one half does not ensure it is at least one half for a given sample size. The limiting theorem is retained. Neither finding is converted into an extra hypothesis or a variant. The goal carries no uniform temporal decay estimate, mixing assumption, or fixed-time large-deviation conclusion as an assumption.

Formalization scope

The formalization uses Mathlib probability measures, independence and equality-in-distribution predicates, nonnegative Lebesgue integrals, and extended-real order topology. Whole source paths are independent; this is stronger information than independence of one chosen interval's workloads. Natural multiplicities provide exactly njNn_jNnj​N copies without rounding. Source indices begin at zero, and the asymptotic scale is represented as N+1N+1N+1 to avoid a zero denominator.

The queue supremum is over all nonnegative real times and takes values in EReal. Zero overflow probability has logarithm −∞-\infty−∞; infinite exponential expectation has logarithm +∞+\infty+∞. The rate subtracts only finite linear terms. Zero multiplicities contribute zero, including when an unused source has an infinite MGF. At zero time or zero tilt, the log MGF is zero under the source assumptions. No division by ststst is introduced.

Nonnegative additive increments use the usual half-open interval convention for endpoint arrivals. Measurability of the constructed workload is explicit, as required for the source's random-variable language. The model API also requires a probability measure and the relevant measurability when forming an overflow probability or exponential rate. Capacity and buffer are positive; F3 records a deterministic counterexample to extending the goal to zero buffer. Empty class sets and zero source counts remain permitted and give no overflow. For Exercise 6.9, positivity and a nonempty finite index set prevent default logarithms or maxima.

The goal must not be replaced by a finite-horizon queue, a deterministic drift inequality, or a hypothesis already asserting the desired asymptotic. No selected result uses an unspecified asymptotic constant, so there is no O(⋅)O(\cdot)O(⋅) constant to instantiate. No variant is posed. The model module supplies real definition bodies; theorem statements expand the relevant formulas so standalone blind read-backs can inspect their meaning without resolving unpublished imports.

Selected references

  • F. P. Kelly and E. Yudovina, Stochastic Networks, Cambridge University Press, 2014. DOI. The pinned supplied artifact is titled Lecture Notes on Stochastic Networks: Chapter 6, printed pages 133–148, PDF pages 141–156. Correspondence with a particular published printing is not asserted. PDF SHA-256: ec271d555059aee58613e5e9a98b8346214b16185c527314f5d94c1ac8b17b6a.
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Stochastic Networks X: Stationary Open Migration Processes Under Time ReversalTextbook

Motivation

A network of queues records both how many customers occupy each location and how they move between locations. These are different kinds of information. A simple distribution for the occupancies at one time need not make the arrival streams simple, or make the queues independent over time. Open migration processes provide a setting in which the distinction can be studied precisely: customers can move through a finite network, enter from outside, and eventually leave. Chapter 2 of Kelly and Yudovina, Stochastic Networks develops their equilibrium structure.

The target concerns what an observer sees when a stationary network is run backwards. It says that the reversed random process belongs to the same class of models, even when its rates differ from those of the original process. This structural result is the setting for the source's subsequent conclusion about Poisson exit streams. The mission treats the process statement itself, keeping the distinction between an equilibrium rate calculation and a statement about a random trajectory.

Setting

There are a finite positive number JJJ of colonies. The state is n=(n1,…,nJ)∈NJn=(n_1,\ldots,n_J)\in\mathbb N^Jn=(n1​,…,nJ​)∈NJ, where njn_jnj​ counts individuals at colony jjj. There is no upper bound on an occupancy or on the total population. A transition can transfer an individual from colony jjj to a different colony kkk, remove one from the system at colony jjj, or introduce one at colony kkk.

The corresponding rates are λjkφj(nj)\lambda_{jk}\varphi_j(n_j)λjk​φj​(nj​), μjφj(nj)\mu_j\varphi_j(n_j)μj​φj​(nj​), and νk\nu_kνk​. The coefficients are nonnegative, λjj=0\lambda_{jj}=0λjj​=0, and the service factors satisfy φj(0)=0\varphi_j(0)=0φj​(0)=0 and φj(r)>0\varphi_j(r)>0φj​(r)>0 when r≥1r\ge1r≥1. A departure requires an individual to be present. Immigration rates do not depend on the occupancy. These are the rates in Section 2.4 of the supplied source, printed pages 30–31.

A Markov process here consists of measurable random variables on one probability space, indexed by real time. Its conditional future distributions depend on the most recent state, through a time-homogeneous transition function. Transition rates are its right-hand infinitesimal transition probabilities. The standing assumptions from Section 1.1 are explicit: the process is irreducible, every state has a strictly positive finite exit rate, and sample paths have only finitely many jumps on each bounded interval. A stationary law is a positive normalized mass function π\piπ giving the distribution at every time.

Formalization targets

The goal is Theorem 2.9, printed page 32 of the supplied PDF:

(n(t))t∈R stationary open migration⟹(n(−t))t∈R stationary open migration.(n(t))_{t\in\mathbb R}\text{ stationary open migration} \quad\Longrightarrow\quad (n(-t))_{t\in\mathbb R}\text{ stationary open migration}.(n(t))t∈R​ stationary open migration⟹(n(−t))t∈R​ stationary open migration.

Three milestones support this target. The partial-balance equations (2.3) and (2.4) are grouped as one milestone because one published theorem supplies both identities. They express equilibrium flux balance for transitions associated with a colony and with the outside world. Theorem 2.8 gives the normalized product-form distribution. With positive traffic parameters αj\alpha_jαj​ satisfying

αj(μj+∑kλjk)=νj+∑kαkλkj,\alpha_j\left(\mu_j+\sum_k\lambda_{jk}\right) =\nu_j+\sum_k\alpha_k\lambda_{kj},αj​(μj​+k∑​λjk​)=νj​+k∑​αk​λkj​,

and finite normalizing sums gjg_jgj​, that distribution is

gj=∑m=0∞αjm∏r=1mφj(r),π(n)=∏jgj−1αjnj∏r=1njφj(r).g_j=\sum_{m=0}^{\infty}\frac{\alpha_j^m}{\prod_{r=1}^m\varphi_j(r)}, \qquad \pi(n)=\prod_j g_j^{-1}\frac{\alpha_j^{n_j}}{\prod_{r=1}^{n_j}\varphi_j(r)}.gj​=m=0∑∞​∏r=1m​φj​(r)αjm​​,π(n)=j∏​gj−1​∏r=1nj​​φj​(r)αjnj​​​.

The third milestone, Proposition 1.1, concerns a stationary process on a countable state space. Its reversed process has the same stationary law and rates

q′(i,j)=π(j)q(j,i)π(i).q'(i,j)=\frac{\pi(j)q(j,i)}{\pi(i)}.q′(i,j)=π(i)π(j)q(j,i)​.

All three source statements are in Kelly and Yudovina, printed pages 16–17 and 31. The goal does not assume the product form, a reverse-process Markov property, or any of the reverse-rate identities.

Significance

The result identifies a class of stochastic networks that remains closed under reversal of stationary time. It does not assert detailed balance or equality of the original and reversed rates. It also does not infer independence of colony trajectories from independence of occupancies at one time; the source expressly distinguishes these statements on printed page 32. This separation is needed when interpreting the Poisson exit-stream consequence on printed page 33 of the source.

Published formal results already supply partial balance, normalized full balance, and the algebraic reversed migration rates. They are included as references rather than repeated as new theorem statements. The remaining formal targets concern the actual countable-state random processes: the Markov property of the reversal and preservation of the open-migration class. The new definition layer also provides finite-cylinder and nonexplosive-path specifications that can be reused for other countable-state stationary models.

Difficulty

A formula for a reversed rate matrix alone does not establish a theorem about the reversed process. The latter has finite-dimensional distributions, measurable coordinates, and nonexplosive paths. These must all be connected to the rates. The occupancy space is countably infinite even though the number of colonies is finite, so finite-state reversal theorems do not directly cover the goal. Similarly, assuming the candidate product distribution as part of the meaning of a stationary migration process would omit part of the source's claim. The definition deliberately leaves the stationary law unspecified.

Formalization scope

Colonies are represented by Fin J\mathrm{Fin}\,JFinJ with J>0J>0J>0; states are unrestricted functions from this type to natural numbers. The zero-based colony labels differ only typographically from the source's labels 1,…,J1,\ldots,J1,…,J. The exact published migration operators and rate functions are reused. Their natural-number subtraction is protected by vanishing service factors at zero and a zero routing diagonal. Empty products equal one. Normalizing sums in the referenced product-form result use HasSum, so divergent real sums cannot acquire a default value and masquerade as finite normalizers.

The process definitions use probability measures, measurable coordinates, stochastic transition functions, finite-cylinder identities, and locally finite jump paths. Cylinder identities avoid conditioning by division at null events. The state space is countable with measurable singletons, and rate rows are explicitly summable. Positivity of the stationary mass function prevents a zero denominator in the reversal formula. Paths may take either adjacent value at a jump, accommodating the reversal of the right-continuous endpoint convention; isolated zero-duration spikes are excluded.

The goal must establish migration dynamics for the actual map t↦n(−t)t\mapsto n(-t)t↦n(−t); an algebraic rate identity or independence at a single time is not a substitute. No asymptotic constants or failure probabilities occur in these targets. The infinite-colony extension, Poisson departure processes, Little's law, Bartlett's theorem, and renewal-reward variants are outside this mission. The findings register preserves observations about out-of-scope source displays, but no variant theorem is proposed. Contributions to the countable-state stochastic foundations and proofs of the two draft theorem statements are within scope.

Selected references

  • F. P. Kelly and E. Yudovina, Stochastic Networks, Cambridge University Press, 2014. DOI. The pinned supplied artifact is titled Lecture Notes on Stochastic Networks: Section 1.1 and Proposition 1.1, printed pages 13–17 (PDF 21–25); Section 2.4, equations (2.2)–(2.4), Theorems 2.8–2.9, printed pages 30–33 (PDF 38–41). Equivalence to a particular published printing is unverified. PDF SHA-256: ec271d555059aee58613e5e9a98b8346214b16185c527314f5d94c1ac8b17b6a.
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Robust Optimization IX: Safe Matrix Chance ConstraintsTextbook

Matrix inequalities under random perturbations

A semidefinite constraint asks whether a symmetric matrix is positive semidefinite: every vector must have a nonnegative quadratic form under that matrix. In optimization, its entries can depend on a decision and on uncertain inputs. Requiring the constraint for every possible input can be restrictive, especially when rare inputs have very large magnitude. A chance constraint instead requires the matrix inequality to hold with a specified probability. Chapter 10 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization develops safe approximations for such constraints, including conic quadratic constraints represented through symmetric matrices.

The question here is how a known probability of a moderate matrix perturbation can imply a much higher probability at a larger threshold. The chapter gives explicit answers for bounded independent perturbations and for independent standard normal perturbations. The goal is its Corollary 10.1.3, including both distributional cases and the possibility that the reference matrix is singular.

Symmetric matrices, probability, and the variance certificate

Let A,B1,…,BLA,B_1,\ldots,B_LA,B1​,…,BL​ be deterministic symmetric real m×mm\times mm×m matrices, with m,L≥1m,L\ge1m,L≥1. The random perturbation is

S=∑ℓ=1LζℓBℓ.S=\sum_{\ell=1}^L\zeta_\ell B_\ell.S=ℓ=1∑L​ζℓ​Bℓ​.

The Loewner order C⪯DC\preceq DC⪯D means that D−CD-CD−C is positive semidefinite. Thus the event −tA⪯S⪯tA-tA\preceq S\preceq tA−tA⪯S⪯tA controls the perturbation simultaneously in every vector direction. For normalized matrices, ∥S∥\|S\|∥S∥ denotes the operator norm for Euclidean vectors, rather than a maximum entry or a row-sum norm.

The random coordinates are measurable and independent on a probability space. Under assumption A.I they have zero means and satisfy ∣ζℓ∣≤1|\zeta_\ell|\le1∣ζℓ​∣≤1 almost surely. Under A.II each has the standard normal law N(0,1)N(0,1)N(0,1). The deterministic variance certificate is

∃Y1,…,YL:(YℓBℓBℓA)⪰0(1≤ℓ≤L),∑ℓYℓ⪯A.\exists Y_1,\ldots,Y_L:\quad \begin{pmatrix}Y_\ell&B_\ell\\B_\ell&A\end{pmatrix}\succeq0 \quad(1\le\ell\le L),\qquad \sum_\ell Y_\ell\preceq A.∃Y1​,…,YL​:(Yℓ​Bℓ​​Bℓ​A​)⪰0(1≤ℓ≤L),ℓ∑​Yℓ​⪯A.

This is precisely system (10.1.13) in the source. A separate premise supplies the base probability

Pr⁡{−ΥA⪯S⪯ΥA}≥χ,\Pr\{-\Upsilon A\preceq S\preceq\Upsilon A\}\ge\chi,Pr{−ΥA⪯S⪯ΥA}≥χ,

where Υ>0\Upsilon>0Υ>0 and χ>0\chi>0χ>0. Neither this probability premise nor the certificate contains the amplified probability conclusion.

Write T(t)=Pr⁡{G>t}T(t)=\Pr\{G>t\}T(t)=Pr{G>t} for G∼N(0,1)G\sim N(0,1)G∼N(0,1), and qqq for its inverse upper-tail quantile. The book writes these functions as Erf and ErfInv. Its Erf is a one-sided upper Gaussian tail; substituting the common analytic error function would change every Gaussian bound.

Formalization targets

The goal, Corollary 10.1.3, asserts that under A.I, for every Ω>Υ\Omega>\UpsilonΩ>Υ,

Pr⁡{−ΩA⪯S⪯ΩA}≥1−1χexp⁡(−(Ω−Υ)216).\Pr\{-\Omega A\preceq S\preceq\Omega A\} \ge1-\frac1\chi\exp\left(-\frac{(\Omega-\Upsilon)^2}{16}\right).Pr{−ΩA⪯S⪯ΩA}≥1−χ1​exp(−16(Ω−Υ)2​).

Under A.II and the additional condition χ>1/2\chi>1/2χ>1/2, it asserts

Pr⁡{−ΩA⪯S⪯ΩA}≥1−T(q(1−χ)+(Ω−Υ)max⁡{1,q(1−χ)/Υ}).\Pr\{-\Omega A\preceq S\preceq\Omega A\} \ge1-T\left(q(1-\chi)+(\Omega-\Upsilon) \max\{1,q(1-\chi)/\Upsilon\}\right).Pr{−ΩA⪯S⪯ΩA}≥1−T(q(1−χ)+(Ω−Υ)max{1,q(1−χ)/Υ}).

Both conclusions retain the constants and strict threshold of equations (10.1.15)–(10.1.16).

Three source-numbered milestones support this goal. Theorem 10.1.1 concerns symmetric BℓB_\ellBℓ​ with ∑Bℓ2⪯I\sum B_\ell^2\preceq I∑Bℓ2​⪯I and defines χ=Pr⁡{∥S∥≤Υ}>0\chi=\Pr\{\|S\|\le\Upsilon\}>0χ=Pr{∥S∥≤Υ}>0. Its bounded-case conclusion is

Pr⁡{∥S∥>Ω}≤χ−1e−(Ω−Υ)2/16,Ω>Υ.\Pr\{\|S\|>\Omega\}\le\chi^{-1}e^{-(\Omega-\Upsilon)^2/16},\qquad \Omega>\Upsilon.Pr{∥S∥>Ω}≤χ−1e−(Ω−Υ)2/16,Ω>Υ.

Theorem B.5.1 concerns a closed convex set Q⊆RmQ\subseteq\mathbb R^mQ⊆Rm with standard Gaussian mass at least χ>1/2\chi>1/2χ>1/2. It asserts that QQQ contains the centered ball of radius q(1−χ)>0q(1-\chi)>0q(1−χ)>0. If it contains a centered ball of radius r≥q(1−χ)r\ge q(1-\chi)r≥q(1−χ), then for α≥1\alpha\ge1α≥1,

Pr⁡{G∉αQ}≤T(q(1−χ)+(α−1)r)≤T(αq(1−χ))≤12e−α2q(1−χ)2/2.\Pr\{G\notin\alpha Q\}\le T(q(1-\chi)+(\alpha-1)r) \le T(\alpha q(1-\chi))\le\tfrac12e^{-\alpha^2q(1-\chi)^2/2}.Pr{G∈/αQ}≤T(q(1−χ)+(α−1)r)≤T(αq(1−χ))≤21​e−α2q(1−χ)2/2.

Its further conclusion covers centered Gaussians with arbitrary positive semidefinite covariance: an outside probability at most δ<1/2\delta<1/2δ<1/2 becomes at most T(αq(δ))≤12e−α2q(δ)2/2T(\alpha q(\delta))\le\tfrac12e^{-\alpha^2q(\delta)^2/2}T(αq(δ))≤21​e−α2q(δ)2/2 after dilation. This clause includes degenerate covariance matrices.

Theorem 10.1.2 is the normalized Gaussian matrix milestone. With the same variance normalization and exact base mass χ>1/2\chi>1/2χ>1/2, it states, now for Ω≥Υ\Omega\ge\UpsilonΩ≥Υ,

Pr⁡{∥S∥>Ω}≤T(q(1−χ)+(Ω−Υ)max⁡{1,Υ−1q(1−χ)})≤e−Ω2Υ−2q(1−χ)2/2.\Pr\{\|S\|>\Omega\}\le T\left(q(1-\chi)+(\Omega-\Upsilon)\max\{1,\Upsilon^{-1}q(1-\chi)\}\right) \le e^{-\Omega^2\Upsilon^{-2}q(1-\chi)^2/2}.Pr{∥S∥>Ω}≤T(q(1−χ)+(Ω−Υ)max{1,Υ−1q(1−χ)})≤e−Ω2Υ−2q(1−χ)2/2.

What a formal development supplies

The chapter’s bounds connect a matrix certificate and a base confidence level to explicit larger-threshold confidence guarantees. They preserve information about the reference matrix, including its null directions. A statement requiring positive definiteness would exclude part of this conclusion.

These are established textbook results whose Lean proofs remain the targets of this mission. The draft supplies concrete definitions and open theorem statements, not completed proofs. Mathlib already provides probability measures, normal distributions, matrix positivity, and a semidefinite Schur-complement equivalence. The published theorem PinningSync.Tree.lemma_2_13 supplies the positive-definite Schur-complement branch as a reference; it is not presented as a substitute for the full semidefinite lemma.

Difficulty

The target combines probabilistic concentration with inequalities that must hold in every matrix direction. Entrywise bounds do not state the same event. Likewise, an invertible reference matrix is a restricted case of the goal. The Gaussian branch also requires exact control of inverse-tail conventions and dilation probabilities for general closed convex sets. The source’s proof of Theorem B.5.1(i) has inconsistent tail arguments in its separating-halfspace paragraph, recorded as a proof warning; the theorem statement retains the printed q(1−χ)q(1-\chi)q(1−χ).

Formalization scope

All matrices are real, finite, and explicitly symmetric in the theorems. Matrix and perturbation dimensions are positive; indexing by Fin changes only the origin of the indices. The setup uses Mathlib’s positive-semidefinite predicate directly. The two matrix inequalities are defined by their positive-semidefinite differences, and the variance certificate is an existential block-matrix condition. The Gaussian geometric theorem uses the concrete standard and multivariate Gaussian measures on Euclidean space, with a positive-semidefinite covariance premise.

Formalization Note. Equation (2.3.22) specifies the inverse tail on (0,1)(0,1)(0,1), while the later statements allow base mass one and failure probability zero. The draft retains those cases by using the extended-real inverse quantile, with q(0)=+∞q(0)=+\inftyq(0)=+∞, T(+∞)=0T(+\infty)=0T(+∞)=0, and the limiting exponential envelope zero at infinity. An infinite-radius centered ball is the whole space. All displayed formulas agree with the source on finite quantile arguments. This endpoint interpretation is recorded in the findings for review, rather than imposing an unprinted χ<1\chi<1χ<1 restriction.

The reusable components are the matrix perturbation, the two-sided order event, the block certificate, and the Gaussian tail conventions. Proof contributions must establish the full statements with their constants and endpoints. No variants are posed in this mission.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI. Chapter 10, printed pp. 237–241; Appendix B.5, printed p. 508; equation (2.3.22), printed p. 39.
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AlgebraQuantum InformationRepresentation Theory·Captain: mikedeng1

Structure and Properties of the Algebra of Partially Transposed Permutation Operators: A = M ⊕ S, M = ⊕ U(α) with U(α) ≅ M(rank Q(α), ℂ), and S ≅ ⊕_{h(ν)<d} M(dim ψ^ν, ℂ)Research Paper

Motivation

Permutation operators encode the symmetries of many identical quantum systems. When one tensor factor is transposed, the resulting operators occur in questions about the commutant of mixed tensor representations and about partially transposed quantum states. The usual symmetric-group algebra no longer describes their multiplication: a product can acquire a factor equal to the local dimension ddd. Mozrzymas, Horodecki, and Studziński determined the full algebraic structure of their span in their 2014 paper. Their description identifies its simple components even when a small local dimension makes the natural spanning family linearly dependent.

Setting

Let d≥1d\ge1d≥1 and n=m+2≥2n=m+2\ge2n=m+2≥2. On nnn tensor factors of Cd\mathbb C^dCd, the permutation operator V(σ)V(\sigma)V(σ) moves the computational-basis tensor indexed by (i1,…,in)(i_1,\ldots,i_n)(i1​,…,in​) to the tensor indexed by (iσ−1(1),…,iσ−1(n))(i_{\sigma^{-1}(1)},\ldots,i_{\sigma^{-1}(n)})(iσ−1(1)​,…,iσ−1(n)​). Write tnt_ntn​ for matrix transposition on the last tensor factor only. The object of this mission is the complex operator algebra

A=Antn(d)=span⁡C{V(σ)tn:σ∈S(n)}.A=A_n^{t_n}(d)=\operatorname{span}_{\mathbb C}\{V(\sigma)^{t_n}:\sigma\in S(n)\}.A=Antn​​(d)=spanC​{V(σ)tn​:σ∈S(n)}.

The subspace MMM is spanned by those V(σ)tnV(\sigma)^{t_n}V(σ)tn​ for which σ(n)≠n\sigma(n)\ne nσ(n)=n. Its complement SSS in the result is an ideal that annihilates MMM on both sides. The permutations of the first n−2n-2n−2 positions act on (Cd)⊗(n−2)(\mathbb C^d)^{\otimes(n-2)}(Cd)⊗(n−2). For each irreducible representation φα\varphi^\alphaφα of S(n−2)S(n-2)S(n−2) that occurs in this action, write wα=dim⁡φαw^\alpha=\dim\varphi^\alphawα=dimφα. Definition 40 constructs operators uijab(α)u^{ab}_{ij}(\alpha)uijab​(α) from their matrix coefficients, the permutation operators, and partial transposition. Their span is U(α)U(\alpha)U(α).

Definition 29 assigns to α\alphaα a block matrix Q(α)Q(\alpha)Q(α) indexed by (a,i)(a,i)(a,i) and (b,j)(b,j)(b,j), where 1≤a,b≤n−11\le a,b\le n-11≤a,b≤n−1 and 1≤i,j≤wα1\le i,j\le w^\alpha1≤i,j≤wα. Its (a,b)(a,b)(a,b) block is dδabφα((a n−1)(ab)(b n−1))d^{\delta_{ab}}\varphi^\alpha((a\ n-1)(ab)(b\ n-1))dδab​φα((a n−1)(ab)(b n−1)), so every diagonal block is ddd times the identity. Finally, a partition ν\nuν of n−1n-1n−1 labels an irreducible representation ψν\psi^\nuψν of S(n−1)S(n-1)S(n−1); h(ν)h(\nu)h(ν) counts the rows of its Young diagram.

Formalization targets

Structure theorem

Theorem 30 asserts that AAA splits into mutually annihilating ideals, and that those ideals split further into full matrix algebras:

A=M⊕S,M=⨁φα⊆Vd[S(n−2)]U(α),U(α)≅Mrank⁡Q(α)(C),S≅⨁ν⊢n−1h(ν)<dMdim⁡ψν(C).A=M\oplus S,\qquad M=\bigoplus_{\varphi^\alpha\subseteq V_d[S(n-2)]}U(\alpha),\qquad U(\alpha)\cong M_{\operatorname{rank}Q(\alpha)}(\mathbb C),\qquad S\cong\bigoplus_{\substack{\nu\vdash n-1\\h(\nu)<d}}M_{\dim\psi^\nu}(\mathbb C).A=M⊕S,M=φα⊆Vd​[S(n−2)]⨁​U(α),U(α)≅MrankQ(α)​(C),S≅ν⊢n−1h(ν)<d​⨁​Mdimψν​(C).

When det⁡Q(α)≠0\det Q(\alpha)\ne0detQ(α)=0, the U(α)U(\alpha)U(α) summand has order (n−1)wα(n-1)w^\alpha(n−1)wα. The goal also includes the multiplication law for the uuu operators, with coefficient Qjkbp(α)Q^{bp}_{jk}(\alpha)Qjkbp​(α) as in equation (6) of Proposition 44. This identity specifies how their natural generators multiply even when Q(α)Q(\alpha)Q(α) is singular. The two cases for SSS printed in Theorem 30, d≥nd\ge nd≥n and d<nd<nd<n, give the same uniform restriction h(ν)<dh(\nu)<dh(ν)<d because every partition of n−1n-1n−1 has at most n−1n-1n−1 rows.

Significance

The theorem identifies the simple ideals and their sizes from representation data of two smaller symmetric groups. It separates the dimension-dependent part MMM, where the rank of Q(α)Q(\alpha)Q(α) may drop, from the part SSS controlled by partitions with fewer than ddd rows. Consequently, it determines the irreducible representations of this concrete operator algebra and explains why its decomposition changes with ddd.

The result is proved in the cited paper; this mission asks for a machine-checked proof of its precise statement. The published operator model and tensor-permutation definition already fix the underlying matrices. A completed development would add reusable facts about partial transposition, ideals of represented group algebras, matrix units arising from singular coefficient matrices, and occurrence of symmetric-group representations. The read side of this mission is an open theorem, not a claim that Theorem 30 has already been formalized.

Difficulty

The natural spanning elements V(σ)tnV(\sigma)^{t_n}V(σ)tn​ are not a basis when d<nd<nd<n, and the uijab(α)u^{ab}_{ij}(\alpha)uijab​(α) can also be dependent. Counting generators therefore cannot establish the orders of the matrix ideals. The matrix Q(α)Q(\alpha)Q(α) records those dependencies; its rank, not its number of rows, governs the U(α)U(\alpha)U(α) summand. The complementary ideal SSS requires tracking which representations of S(n−1)S(n-1)S(n−1) survive after the MMM component is removed. A dimension count alone would identify neither the actual ideals nor their matrix-unit multiplication laws.

Formalization scope

Operators are matrices indexed by functions Fin n → Fin d, a coordinate model of (Cd)⊗n(\mathbb C^d)^{\otimes n}(Cd)⊗n. The last-factor transpose is the published ptLast; AAA and MMM are the published complex spans algA and algM. The paper's labels 1,…,n−11,\ldots,n-11,…,n−1 become Fin (m+1), and its last label becomes Fin.last (m+1). Permutations multiply right to left. The irreducible family is represented by real orthogonal matrices, hence by unitary complex matrices after casting; the explicit completeness condition ∑α(wα)2=(n−2)!\sum_\alpha(w^\alpha)^2=(n-2)!∑α​(wα)2=(n−2)! ensures that every irreducible of S(n−2)S(n-2)S(n−2) is present in the family.

Occurrence means that a nonzero intertwiner embeds an irreducible into the action on exactly (Cd)⊗(n−2)(\mathbb C^d)^{\otimes(n-2)}(Cd)⊗(n−2). An ideal is a complex subspace of AAA closed under multiplication on both sides. An assertion I≅Mr(C)I\cong M_r(\mathbb C)I≅Mr​(C) requires r2r^2r2 linearly independent matrix units spanning III and obeying the matrix-unit law; it cannot be discharged by a dimension count. For r=0r=0r=0 this requires I=0I=0I=0. The order dim⁡ψν\dim\psi^\nudimψν is represented by the number of standard Young tableaux of shape ν\nuν, using the classical symmetric-group dimension formula. The goal permits n=2n=2n=2 and requires d≥1d\ge1d≥1.

Theorem 30's displayed coefficient QikbpQ^{bp}_{ik}Qikbp​ conflicts with Proposition 44's equation (6), QjkbpQ^{bp}_{jk}Qjkbp​; the latter agrees with the matrix-index contraction and is used here. Contributions toward the listed source results, the partition occurrence criterion, and the singular-matrix algebra reduction are useful. An arbitrary family of subspaces with the right dimensions does not meet the target: the statements fix AAA, MMM, U(α)U(\alpha)U(α), Q(α)Q(\alpha)Q(α), and the matrix-unit structure of each component.

Selected references

  • M. Mozrzymas, M. Horodecki, M. Studziński, Structure and properties of the algebra of partially transposed permutation operators, Journal of Mathematical Physics 55, 032202 (2014), arXiv:1308.2653v3. The cited version supplies the page and result numbers used in this mission.
  • M. Studziński, M. Horodecki, M. Mozrzymas, Commutant structure of U⊗(n−1)⊗U transformations*, arXiv:1305.6183v2. Its published operator model supplies the shared Lean definitions.
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ProbabilityQuantum InformationTheoretical Computer Science·Captain: mikedeng1

Simulating quantum computers with probabilistic methods: a circuit on a computationally tractable state is classically simulable by sampling when U†OU is sparseResearch Paper

Why this problem arose

A quantum circuit may create a state whose full list of amplitudes is far too large for a classical computer to store. That fact alone does not show that every observable feature of its output is hard to estimate. In Simulating quantum computers with probabilistic methods, Van den Nest asks when classical sampling can reproduce the accuracy of a quantum experiment that estimates an observable's expectation. The paper's Theorem 1 identifies a condition on the input state and on the observable after it is pulled back through the circuit, rather than requiring the circuit itself to have a sparse matrix. This separates the cost of describing a whole output state from the cost of estimating the particular quantity measured at the end. Van den Nest, §§1–3

The paper distinguishes weak simulation, which achieves the accuracy available from polynomially many experimental runs, from strong simulation, which asks for much finer numerical precision. This mission addresses the sampling estimate behind the former. The source's 2010 preprint proves an efficient classical algorithm under computational assumptions; the formal target below states its finite probability guarantee for the particular estimator in that proof. Van den Nest, pp. 2, 6–7

States, sparse operators, and samples

An nnn-qubit computational basis has labels x∈{0,1}nx\in\{0,1\}^nx∈{0,1}n. A state ∣ψ⟩|\psi\rangle∣ψ⟩ has complex coefficient ψx=⟨x∣ψ⟩\psi_x=\langle x|\psi\rangleψx​=⟨x∣ψ⟩ at each label, with ∑x∣ψx∣2=1\sum_x|\psi_x|^2=1∑x​∣ψx​∣2=1. Measurement in this basis yields xxx with Born probability px=∣ψx∣2p_x=|\psi_x|^2px​=∣ψx​∣2. A state is computationally tractable (CT) in the paper when these probabilities can be sampled, and individual coefficients can be evaluated, in polynomial time. The finite development below represents the resulting sample and coefficient access directly. Van den Nest, Definition 1, p. 8

For a matrix AAA, the entry AyxA_{yx}Ayx​ is its transition from basis label xxx to label yyy. The operator is sss-sparse if each row and each column has at most sss nonzero entries. Its column data consist of coefficients αi(x)\alpha_i(x)αi​(x) and row labels ri(x)r_i(x)ri​(x) for i=1,…,si=1,\ldots,si=1,…,s, with A∣x⟩=∑iαi(x)∣ri(x)⟩A|x\rangle=\sum_i\alpha_i(x)|r_i(x)\rangleA∣x⟩=∑i​αi​(x)∣ri​(x)⟩. Nonzero coefficients in a column occupy distinct rows. The paper calls such an operator efficiently computable sparse (ECS) when the nonzero entries can also be found efficiently. Van den Nest, §4.3, pp. 10–11

For two normalized states ψ,ϕ\psi,\phiψ,ϕ, write qy=∣ϕy∣2q_y=|\phi_y|^2qy​=∣ϕy​∣2. The paper defines bounded complex functions FiF_iFi​ and GiG_iGi​ from the column data, separating each contribution according to whether px≥qri(x)p_x\ge q_{r_i(x)}px​≥qri​(x)​. The estimator is the sum over iii of a sample mean of FiF_iFi​ under ppp and a sample mean of GiG_iGi​ under qqq. The same KKK independent draws from each law are used for every iii in this formalization. Its target is the matrix element ⟨ϕ∣A∣ψ⟩\langle\phi|A|\psi\rangle⟨ϕ∣A∣ψ⟩. Van den Nest, Eqs. (5)–(8), pp. 12–13

Formalization targets

The main result concerns a unitary UUU, a Hermitian observable OOO with spectral norm at most one, and the pulled-back operator B=U†OUB=U^\dagger O UB=U†OU. When BBB is sss-sparse and has the stated column data, the estimator o^\widehat oo targets the output expectation ⟨Uψ∣O∣Uψ⟩\langle U\psi|O|U\psi\rangle⟨Uψ∣O∣Uψ⟩. For K≥1K\ge1K≥1 samples of each kind and ε>0\varepsilon>0ε>0, the target is

Pr⁡{∣o^−⟨Uψ∣O∣Uψ⟩∣>ε}≤8sexp⁡(−Kε232s4).\Pr\bigl\{|\widehat o-\langle U\psi|O|U\psi\rangle|>\varepsilon\bigr\} \le 8s\exp\left(-\frac{K\varepsilon^2}{32s^4}\right).Pr{∣o−⟨Uψ∣O∣Uψ⟩∣>ε}≤8sexp(−32s4Kε2​).

The paper states Theorem 1 as an efficient simulation claim. The displayed explicit tail is obtained from its Theorem 3, the pointwise bounds on FiF_iFi​ and GiG_iGi​, and Appendix A's Chernoff–Hoeffding estimate. Its exact constants are a commitment of this finite accuracy target, not a constant printed in Theorem 1. Van den Nest, Theorem 1, p. 2; Theorem 3, p. 11; Eq. (18), p. 23

The milestones follow the paper's supporting statements: the real and complex sampling bounds, the sparse matrix-element decomposition, the two expectation identities, the bound on FiF_iFi​, the row-preimage count, the bound on GiG_iGi​, and the general matrix-element estimate of Theorem 3. Theorem 3 permits two different normalized states and a sparse operator that need not be unitary. Its specialization with ϕ=ψ\phi=\psiϕ=ψ and A=U†OUA=U^\dagger O UA=U†OU gives the target above. Van den Nest, pp. 11–13, 23

What the result provides

The theorem gives a concrete error probability for recovering an output observable's expectation from classical samples of the input state. The condition concerns U†OUU^\dagger O UU†OU; it allows the circuit matrix UUU itself to be dense. Thus it applies to circuit and observable pairs for which output-state enumeration is a poor guide to the cost of this particular expectation estimate. The paper develops consequences for local observables and other circuit families after Theorem 3. Van den Nest, Theorem 1 and §5

A formal development would make the finite probability claim, the sample-access model, and the spectral-norm assumptions independently checkable. The paper's theorem is proved mathematically, but this mission's Lean theorems are open statements awaiting proofs. In particular, machine-checking the explicit estimator's accuracy is separate from representing a polynomial-time classical machine, which this mission does not undertake.

Where the difficulty lies

Sparse columns make ⟨ϕ∣A∣ψ⟩\langle\phi|A|\psi\rangle⟨ϕ∣A∣ψ⟩ a sum of terms indexed by iii, but they do not by themselves give a bounded random variable when a term is sampled from pxp_xpx​. Dividing by a small pxp_xpx​ may create a large weight. Sampling from qyq_yqy​ has the analogous problem in the opposite direction, and the row labels ri(x)r_i(x)ri​(x) need not be injective as functions of xxx. The paper's two functions split those regimes; its row-sparsity condition controls the number of terms that can contribute to one Gi(y)G_i(y)Gi​(y). The proof must also keep the complex modulus, the strict failure event, and the shared sample sets consistent with the finite probability law. Van den Nest, proof of Theorem 3, pp. 12–13

Formalization scope

Lean represents basis labels as functions Fin n → Bool, states as finite complex coefficient vectors, and operators as complex matrices. The operator bound uses the published spectral norm QAlgorithms.specNorm. Theorem 1 assumes a unit vector, a unitary matrix, and a Hermitian observable of norm at most one. The general Theorem 3 uses any finite basis and two normalized coefficient vectors. Column data can enumerate nonzero entries in any order; the proof needs their values and distinctness, while the paper fixes top-to-bottom order. All expectations and event probabilities are finite sums. No measurable-space conventions or Bochner-integral defaults enter.

The estimator is fixed by the definitions of FiF_iFi​, GiG_iGi​, and their two sample means. It reads sampled labels, state coefficients, and sparse column data. It cannot read the target matrix element, enumerate all basis labels to output the answer, or inspect UUU and OOO outside the supplied column data. The model asserts the accuracy that these accesses support; it does not certify that sampling, coefficient evaluation, column enumeration, or the circuit family run in polynomial time. This is the precise part of the paper's classical simulation statement represented here.

Positive KKK avoids the undefined statistical meaning of an empty sample mean. The split assigns equality px=qri(x)p_x=q_{r_i(x)}px​=qri​(x)​ to FiF_iFi​. A zero Born probability has zero sampling mass; the corresponding totalized quotient is set to zero. For s=0s=0s=0, the sparse matrix and estimator are zero, and the theorem's failure bound is zero. The displayed 8s8s8s bound is the one derived from the paper's inequalities; the complex-valued intermediate constant is likewise derived from Eq. (18). Reusable contributions include the finite product-sampling concentration theorem, the column-data representation, and the matrix-element decomposition. Van den Nest, pp. 10–13, 23

Selected references

  • M. Van den Nest, Simulating quantum computers with probabilistic methods, arXiv:0911.1624v3, 2010. arXiv
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CombinatoricsQuantum InformationRepresentation Theory·Captain: mikedeng1

Optimal Quantum Purity Amplification: Removing the Bottom Box of the Last Column of Each Schur-Sampled Young Diagram Gives the Optimal Choi Matrix for Purifying n Depolarized QuditsResearch Paper

Motivation

Quantum devices rarely prepare the state they are asked for. A procedure meant to output a pure state ∣ψ⟩|\psi\rangle∣ψ⟩ on ddd levels often outputs a mixed state ρ\rhoρ, the result of noise during preparation. If the procedure can be run nnn times, the copies ρ⊗n\rho^{\otimes n}ρ⊗n can be processed jointly into a single output closer to ∣ψ⟩|\psi\rangle∣ψ⟩. This task is quantum purity amplification (QPA), also called purification. It appears as a primitive in error mitigation, in state preparation on near-term hardware, and in the theory of quantum state estimation and cloning.

For qubits and depolarizing noise, Cirac, Ekert and Macchiavello found the optimal protocol in 1999 (Phys. Rev. Lett. 82, 4344), and Keyl and Werner determined the rate of optimal purification procedures (Ann. Henri Poincaré 2, 2001), with the minimum fidelity as figure of merit. For qudits (d>2d>2d>2) the optimal protocol remained open. Childs, Fu, Leung, Li, Ozols and Vyas gave a streaming protocol (arXiv:2309.16387), and Grinko and Ozols reduced unitary-equivariant SDPs of this type to linear programs (arXiv:2207.05713) without solving this one in closed form. Li, Fu, Isogawa, Silva and Chuang (arXiv:2409.18167, version 4 of 25 Dec 2025) solve the qudit case exactly: they give the Choi matrix of the optimal channel in closed form (Theorem II.1).

Setting

Let W=CdW=\mathbb C^dW=Cd. An unknown pure state σ=∣ψ⟩⟨ψ∣\sigma=|\psi\rangle\langle\psi|σ=∣ψ⟩⟨ψ∣ is corrupted by the depolarizing channel of strength λ∈(0,1)\lambda\in(0,1)λ∈(0,1):

ρ=Dλ(σ)=(1−λ) σ+λ Idd.\rho=\mathcal D_\lambda(\sigma)=(1-\lambda)\,\sigma+\lambda\,\frac{\mathbb I_d}{d}.ρ=Dλ​(σ)=(1−λ)σ+λdId​​.

A QPA protocol is a quantum channel Φ\PhiΦ from W⊗nW^{\otimes n}W⊗n (the input registers) to WWW (the output register). Its quality at ψ\psiψ is the fidelity FΦ(ψ)=⟨ψ∣Φ(ρ⊗n)∣ψ⟩F_\Phi(\psi)=\langle\psi|\Phi(\rho^{\otimes n})|\psi\rangleFΦ​(ψ)=⟨ψ∣Φ(ρ⊗n)∣ψ⟩, and the figure of merit is the minimum fidelity min⁡∥ψ∥=1FΦ(ψ)\min_{\|\psi\|=1}F_\Phi(\psi)min∥ψ∥=1​FΦ​(ψ).

A channel is described by its Choi matrix TTT, an operator on out⊗in\mathrm{out}\otimes\mathrm{in}out⊗in with T⪰0T\succeq0T⪰0 and troutT=Iin\mathrm{tr}_{\mathrm{out}}T=\mathbb I_{\mathrm{in}}trout​T=Iin​; the channel is ΦT(X)=trin(T(I⊗X⊤))\Phi_T(X)=\mathrm{tr}_{\mathrm{in}}(T(\mathbb I\otimes X^\top))ΦT​(X)=trin​(T(I⊗X⊤)). Averaging the fidelity over a Haar-random ψ\psiψ gives the semidefinite program (SDP)

max⁡ tr(C⊤T)s.t.troutT=Iin, T⪰0,C=∫σU⊤⊗ρU⊗n dU,\max\ \mathrm{tr}(C^\top T)\quad\text{s.t.}\quad \mathrm{tr}_{\mathrm{out}}T=\mathbb I_{\mathrm{in}},\ T\succeq0,\qquad C=\int\sigma_U^\top\otimes\rho_U^{\otimes n}\,dU,max tr(C⊤T)s.t.trout​T=Iin​, T⪰0,C=∫σU⊤​⊗ρU⊗n​dU,

with σU=U∣0⟩⟨0∣U†\sigma_U=U|0\rangle\langle0|U^\daggerσU​=U∣0⟩⟨0∣U†, ρU=Dλ(σU)\rho_U=\mathcal D_\lambda(\sigma_U)ρU​=Dλ​(σU​), and dUdUdU the Haar probability measure on U(d)U(d)U(d).

The answer is phrased with Young diagrams. A Young diagram ς\varsigmaς with nnn boxes and at most ddd rows labels an irreducible representation W[ς]W^{[\varsigma]}W[ς] of U(d)U(d)U(d) of dimension d[ς]d^{[\varsigma]}d[ς], and Πς\Pi_\varsigmaΠς​ denotes the projector onto the ς\varsigmaς-isotypic part of W⊗nW^{\otimes n}W⊗n (weak Schur sampling). The protocol must be covariant under the mixed representation R(U)=Uˉ⊗U⊗nR(U)=\bar U\otimes U^{\otimes n}R(U)=Uˉ⊗U⊗n. Inside the ς\varsigmaς-sector this representation splits as ⨁iW[μi]\bigoplus_i W^{[\mu_i]}⨁i​W[μi​], where [μi]=ς−ei[\mu_i]=\varsigma-e_i[μi​]=ς−ei​ removes the last box of row iii of ς\varsigmaς (padded with zeros to ddd rows). Row iii is feasible if it is the last row or ςi>ςi+1\varsigma_i>\varsigma_{i+1}ςi​>ςi+1​. Let i∗i^*i∗ be the smallest feasible row; [μi∗][\mu_{i^*}][μi∗​] is ς\varsigmaς with the bottom box of its last column removed. PμP_\muPμ​ is the projector onto the [μ][\mu][μ]-isotypic component of RRR.

Formalization targets

Goal: Theorem II.1

T∗=∑ςd[ς]d[μi∗]  Pμi∗(Iout⊗Πς)T^*=\sum_{\varsigma}\frac{d^{[\varsigma]}}{d^{[\mu_{i^*}]}}\;P_{\mu_{i^*}}\big(\mathbb I_{\mathrm{out}}\otimes\Pi_\varsigma\big)T∗=ς∑​d[μi∗​]d[ς]​Pμi∗​​(Iout​⊗Πς​)

is feasible and optimal for the SDP. Its channel ΦT∗\Phi_{T^*}ΦT∗​ is a quantum channel. For every channel Φ\PhiΦ, min⁡ψFΦ(ψ)≤min⁡ψ′FΦT∗(ψ′)\min_\psi F_\Phi(\psi)\le\min_{\psi'}F_{\Phi_{T^*}}(\psi')minψ​FΦ​(ψ)≤minψ′​FΦT∗​​(ψ′). The statement asserts optimality, not uniqueness, and holds for every d≥1d\ge1d≥1, n≥0n\ge0n≥0, 0<λ<10<\lambda<10<λ<1.

Milestones (in the order the proof uses them)

  • Proposition S2.1. An operator commuting with Uˉ⊗U⊗n\bar U\otimes U^{\otimes n}Uˉ⊗U⊗n (U∈SU(d)U\in SU(d)U∈SU(d)) and with input permutations is a scalar mim_imi​ on each block [μi][\mu_i][μi​] of every sector.
  • Eq. (S23). ∣ψ⟩⟨ψ∣=A(−ρ−1)+B Id/d|\psi\rangle\langle\psi|=A(-\rho^{-1})+B\,\mathbb I_d/d∣ψ⟩⟨ψ∣=A(−ρ−1)+BId​/d with A=λ(d(1−λ)+λ)d2(1−λ)A=\frac{\lambda(d(1-\lambda)+\lambda)}{d^2(1-\lambda)}A=d2(1−λ)λ(d(1−λ)+λ)​, B=d+λ1−λB=d+\frac{\lambda}{1-\lambda}B=d+1−λλ​.
  • Lemma S2.3. P=Id−Id⊗troutP=\mathrm{Id}-\frac{\mathbb I}{d}\otimes\mathrm{tr}_{\mathrm{out}}P=Id−dI​⊗trout​ is an orthogonal projector.
  • Lemma S2.4. If P(C1)=AP(C2)P(C_1)=AP(C_2)P(C1​)=AP(C2​) with A>0A>0A>0, the two SDPs have the same optimal solutions.
  • Eq. (S25). P(C)=AP(C′)P(C)=AP(C')P(C)=AP(C′) with C′=−∫(ρU⊤)−1⊗ρU⊗n dUC'=-\int(\rho_U^\top)^{-1}\otimes\rho_U^{\otimes n}\,dUC′=−∫(ρU⊤​)−1⊗ρU⊗n​dU.
  • Eq. (S26). C′C'C′ acts on the block [μi][\mu_i][μi​] as ci′=−S[μi](a,…,a,b)c'_i=-S^{[\mu_i]}(a,\dots,a,b)ci′​=−S[μi​](a,…,a,b), a=λ/da=\lambda/da=λ/d, b=1−d−1dλb=1-\frac{d-1}{d}\lambdab=1−dd−1​λ, where S[μ]=s[μ]/d[μ]S^{[\mu]}=s^{[\mu]}/d^{[\mu]}S[μ]=s[μ]/d[μ] is the normalized Schur polynomial.
  • Eqs. (S27)–(S28). S[μ]≤S[λ]S^{[\mu]}\le S^{[\lambda]}S[μ]≤S[λ] on (0,∞)d(0,\infty)^d(0,∞)d iff [μ]⪯[λ][\mu]\preceq[\lambda][μ]⪯[λ] in dominance order.
  • p. 21. [μi]⪯[μj][\mu_i]\preceq[\mu_j][μi​]⪯[μj​] whenever i≤ji\le ji≤j.

Significance

The theorem gives the exact optimal purification channel for every ddd, nnn and depolarizing strength, and the channel does not depend on λ\lambdaλ. It has an operational form, worked out in the paper's Sec. II C: Schur sampling, a correction inside each sector, and a partial trace. From it the paper derives the optimal sample complexity n≈1δ(1−1d)λ(1−λ)2n\approx\frac1\delta(1-\frac1d)\frac{\lambda}{(1-\lambda)^2}n≈δ1​(1−d1​)(1−λ)2λ​ for output infidelity δ\deltaδ (Theorem II.2) and an efficient circuit implementation (Algorithm 1). Both rest on Theorem II.1.

The result is proved on paper but not formalized anywhere. A formal proof would check a chain that mixes semidefinite programming, Haar integration, the Schur–Weyl duality of the mixed representation Uˉ⊗U⊗n\bar U\otimes U^{\otimes n}Uˉ⊗U⊗n, and a combinatorial inequality for normalized Schur polynomials (Sra's theorem, European J. Combin. 51, 2016), which is cited and not proved in the paper. Several of these components are general results: the block decomposition of covariant operators, the cost-matrix projection argument for SDPs with a partial-trace constraint, and the dominance ordering of normalized Schur polynomials.

Difficulty

Symmetry reduces the SDP to a linear program in one coefficient tit_iti​ per block, but the coefficients cic_ici​ of the original cost matrix CCC are hard to evaluate directly. The proof replaces CCC by C′C'C′, whose block coefficients are characters of rational representations evaluated at the spectrum of ρ\rhoρ, and shows that the replacement leaves the optimizer unchanged. The remaining step compares these characters across blocks. That comparison is the Cuttler–Greene–Skandera inequality for normalized Schur polynomials, a nontrivial combinatorial theorem. One natural guess fails: keeping the block of the largest feasible row instead of the smallest gives a channel that is not optimal in general. The optimal block removes the bottom box of the last column, which is generally a different row.

Formalization scope

Operators are complex matrices indexed by Fin d×(Fin n→Fin d)\mathrm{Fin}\,d\times(\mathrm{Fin}\,n\to\mathrm{Fin}\,d)Find×(Finn→Find), output register first. Partial traces are the published WildeQIT.partialTraceLeft/Right. The Haar measure is the published probability Haar measure QAlgorithms.Schur.unitaryHaar d on U(d)U(d)U(d), and Haar integrals of matrices are taken entrywise. Young diagrams, Schur polynomials, dimensions d[ν]d^{[\nu]}d[ν] (semistandard tableau counts), Schur modules with their polynomial representations, and the weak Schur sampling projector Πς\Pi_\varsigmaΠς​ come from the published QAlgorithms.Schur layer; channels are QAlgorithms.IsChannel (finite Kraus families). Rows are 0-based in Lean.

The irreps [μi][\mu_i][μi​] of the mixed representation (Nguyen, arXiv:2310.01613) are rational: when ς\varsigmaς has fewer than ddd rows, μd\mu_dμd​ has last row −1-1−1. They are encoded by the determinant shift νi=ς+(1d)−ei\nu_i=\varsigma+(1^d)-e_iνi​=ς+(1d)−ei​, a Young diagram with n+d−1n+d-1n+d−1 boxes, with [μi]=[νi]⊗det⁡−1[\mu_i]=[\nu_i]\otimes\det^{-1}[μi​]=[νi​]⊗det−1. The isotypic projector is the character integral Pμ=d[ν]∫χν(U)‾det⁡U R(U) dUP_\mu=d^{[\nu]}\int\overline{\chi_\nu(U)}\det U\,R(U)\,dUPμ​=d[ν]∫χν​(U)​detUR(U)dU.

Disclosed choices:

  • Proposition S2.1 is stated on the full space with an added permutation-invariance hypothesis, which replaces the paper's restriction to one irrep block. Without it the full-space statement is false.
  • Lemma S2.4 uses Re tr(CT)\mathrm{Re}\,\mathrm{tr}(CT)Retr(CT) without the transpose, as printed, and the constraint troutT=I\mathrm{tr}_{\mathrm{out}}T=\mathbb Itrout​T=I.
  • Eq. (S28) makes the quantifier over positive arguments explicit.
  • The goal's minimum-fidelity clause is stated without infima: there is a ψ\psiψ whose fidelity under Φ\PhiΦ is at most the fidelity of ΦT∗\Phi_{T^*}ΦT∗​ at every ψ′\psi'ψ′.

Trivializing formalizations are ruled out. T∗T^*T∗ is the explicit operator above, computed from ddd and nnn alone, never an argmax or a hypothesis. The cost matrix is the actual Haar integral, not a closed form. The competitors are all feasible TTT and all channels Φ\PhiΦ, with no symmetry assumed.

Welcome contributions: the tracing and Pieri-type decomposition of Uˉ⊗U⊗n\bar U\otimes U^{\otimes n}Uˉ⊗U⊗n; Haar orthogonality of characters on U(d)U(d)U(d); the equivalence of Choi feasibility and Kraus channels; Sra's inequality. Each is reusable beyond this mission.

Selected references

  • Z. Li, H. Fu, T. Isogawa, C. Silva, I. Chuang, Optimal Quantum Purity Amplification, arXiv:2409.18167v4, 2025. https://arxiv.org/abs/2409.18167
  • J. I. Cirac, A. K. Ekert, C. Macchiavello, Optimal purification of single qubits, Phys. Rev. Lett. 82, 4344, 1999. https://doi.org/10.1103/PhysRevLett.82.4344
  • M. Keyl, R. F. Werner, The rate of optimal purification procedures, Annales Henri Poincaré 2, 1–26, 2001.
  • A. M. Childs, H. Fu, D. Leung, Z. Li, M. Ozols, V. Vyas, Streaming quantum state purification, arXiv:2309.16387, 2023. https://arxiv.org/abs/2309.16387
  • D. Grinko, M. Ozols, Linear programming with unitary-equivariant constraints, arXiv:2207.05713, 2023. https://arxiv.org/abs/2207.05713
  • Q. T. Nguyen, The mixed Schur transform: efficient quantum circuit and applications, arXiv:2310.01613, 2023. https://arxiv.org/abs/2310.01613
  • S. Sra, On inequalities for normalized Schur functions, European Journal of Combinatorics 51, 492, 2016.
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Information TheoryMathematical PhysicsQuantum Information·Captain: mikedeng1

The Entropy Photon-Number Inequality and its Consequences: It Implies Both Minimum Output Entropy Conjectures, So Vacuum and Thermal Inputs Minimize the Beam-Splitter Output EntropyResearch Paper

Motivation

Light carries information in electromagnetic field modes. At optical frequencies, photon statistics affect the capacities of thermal-noise and broadcast communication channels. Bounds on these capacities depend on identifying the smallest entropy that a beam splitter can produce under specified input conditions. Guha, Erkmen, and Shapiro explain why two such minimum output entropy claims matter: their first supports the proposed thermal-noise channel capacity, and their second supports the proposed bosonic broadcast capacity region. The paper states both as conjectures and shows that they follow from its Entropy Photon-Number Inequality (EPnI).

The authors model the EPnI on the classical entropy power inequality, but its quantum version concerns density operators rather than probability densities. Their 2007 paper does not prove the EPnI. A later platform theorem, sourced from an OpenAI mathematics preprint codebase, is marked Proved for finite-energy inputs. It supplies this mission's referenced first milestone. The statements here express the paper's two consequences in that same model; their Lean proofs are still open in this proposal.

Setting

A bosonic mode has number states ∣m⟩|m\rangle∣m⟩ indexed by m∈Nm\in\mathbb Nm∈N. An nnn-mode state ρ\rhoρ is a positive density operator on the full Fock space indexed by Nn\mathbb N^nNn, with trace one. Its von Neumann entropy is S(ρ)=−tr⁡(ρlog⁡ρ)S(\rho)=-\operatorname{tr}(\rho\log\rho)S(ρ)=−tr(ρlogρ). All logarithms are natural. A thermal state with average photon number N≥0N\ge0N≥0 per mode has weights Nm/(N+1)m+1N^m/(N+1)^{m+1}Nm/(N+1)m+1 in the number basis; for nnn modes the state is the product of these single-mode distributions. At N=0N=0N=0 this is the vacuum, with zero photons in every mode. A pure state is a projector onto a unit Fock vector. A state has zero mean field when the expectation of the annihilation operator is zero for each mode.

Two independent input states ρa\rho_aρa​ and ρb\rho_bρb​ enter a lossless beam splitter with transmissivity η∈[0,1]\eta\in[0,1]η∈[0,1]. For each mode its retained output has annihilation operator c^=η a^+1−η b^\hat c=\sqrt{\eta}\,\hat a+\sqrt{1-\eta}\,\hat bc^=η​a^+1−η​b^; the other output is discarded. The retained density operator is ρc\rho_cρc​. Independence means that the joint input is ρa⊗ρb\rho_a\otimes\rho_bρa​⊗ρb​; correlations among modes inside either input are allowed. The thermal entropy per mode is

g(N)=(N+1)log⁡(N+1)−Nlog⁡N,g(N)=(N+1)\log(N+1)-N\log N,g(N)=(N+1)log(N+1)−NlogN,

with the continuous convention at N=0N=0N=0. The entropy photon-number of an nnn-mode state is g−1(S(ρ)/n)g^{-1}(S(\rho)/n)g−1(S(ρ)/n). Eq. (13) of the paper asserts that the output entropy photon-number is at least η\etaη times that of the first input plus 1−η1-\eta1−η times that of the second. The source paper gives the definitions in §II.B, p. 2.

Formalization targets

The first target fixes the second input to a thermal product state of mean K≥0K\ge0K≥0, while the first ranges over zero-mean-field pure states. The second fixes the first input to the vacuum, while the second ranges over states with entropy ng(K)n g(K)ng(K). For each class, the claimed lower bound and attained minimum are

S(ρc)≥n g((1−η)K),min⁡S(ρc)=n g((1−η)K).S(\rho_c)\ge n\,g((1-\eta)K),\qquad \min S(\rho_c)=n\,g((1-\eta)K).S(ρc​)≥ng((1−η)K),minS(ρc​)=ng((1−η)K).

For the first class the vacuum first input attains equality. For the second, the product thermal second input attains equality. The goal states both claims together, including the existence of an attaining input and output. The shared attack path contains the EPnI, Eq. (13), the scalar properties of ggg and its inverse, thermal state existence and entropy, zero entropy of pure states, the beam splitter's thermal output for vacuum and thermal inputs, and the inequalities of Eqs. (16)–(17). Each milestone uses the statement on pp. 2–3 of the paper.

Significance

An attained minimum gives the precise noise floor for the two input classes. In the paper's capacity arguments, the first class concerns the thermal-noise channel and the second the bosonic broadcast channel. The mission records the exact optimizer and the output entropy, including the endpoints η=0,1\eta=0,1η=0,1 and K=0K=0K=0. Without the optimizer's output value, a lower bound alone would not identify the minimum.

The referenced EPnI is marked Proved on Prove2Me under finite-energy assumptions. This mission's thermal-state, pure-state, and beam-splitter statements are draft targets and have no machine-checked proofs here. Closing them would connect the platform's general inequality to the two applications explicitly worked through by Guha, Erkmen, and Shapiro. The thermal-state and entropy facts can also serve other bosonic-channel formalizations using the same Fock-space interface.

Difficulty

The EPnI supplies an entropy photon-number bound, but converting it into an attained output-entropy minimum requires more than substituting a pure input. One must justify that the inverse thermal entropy behaves as expected on nonnegative entropies, that thermal product states really exist in the chosen infinite-dimensional state space, and that vacuum mixed with thermal noise produces the specified thermal output. The last claim is a statement about the full beam-splitter matrix and its partial trace, not just a scalar entropy comparison. Infinite sums also demand care: a formal expression that defaults to zero when it diverges would give a spurious entropy value.

Formalization scope

The development reuses OAI.EntropyPhotonNumber.State n, its number-basis matrix entries, real-valued entropy, ggg, the infimum definition of g−1g^{-1}g−1, and the beam-splitter output relation. The new definitions express thermal, vacuum, pure, and zero-mean-field states on that same carrier. The thermal state uses Eq. (10)'s number-basis formula; Eq. (9)'s coherent-state integral is outside this mission. The beam splitter uses the sign convention in the published definition, which yields the paper's retained output c^\hat cc^. The zero-mean-field condition includes convergence of each annihilation expectation.

There is at least one mode, n≥1n\ge1n≥1, since Eq. (11) divides entropy by nnn. Inputs to which the EPnI is applied have finite energy. This assumption is additional to the paper's phrasing: it is required by the referenced platform theorem and prevents the real-valued infinite-series entropy from taking a default zero on a divergent input. The first optimized input is therefore a finite-energy pure state; the second is a finite-energy state of entropy ng(K)n g(K)ng(K). The thermal and vacuum witnesses themselves have finite energy. These conditions are disclosed in the theorem statements and are not assertions that the unrestricted conjectures have been settled here.

The goal quantifies over every feasible input and corresponding output, states equality for every output from the named optimizer, and asserts that the optimizer and an output exist. This rules out a vacuous result from an empty thermal-state class or a bound that omits attainment. Contributions to the scalar ggg lemmas, thermal-state construction, pure-state entropy, and the beam-splitter output calculation are all within scope. Infrastructure for summable Fock-space matrix entries and operator entropy should remain reusable beyond this mission.

Selected references

  • S. Guha, B. I. Erkmen, and J. H. Shapiro, The Entropy Photon-Number Inequality and its Consequences, arXiv:0710.5666v2, 2007. arXiv
  • OpenAI, EntropyPhotonNumber Lean development, September 2026, unreviewed preprint code. Source; Prove2Me theorem.
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AlgebraRepresentation Theory·Captain: mikedeng1

Cyclotomic Birman–Wenzl–Murakami Algebras, II: Admissibility Relations and Freeness: Over an Admissible Integral Domain S, W_{n,S,r} Is a Free S-Module of Rank r^n(2n−1)!!Research Paper

Motivation

The cyclotomic Birman–Wenzl–Murakami algebra is an algebra of braids and contractions equipped with an additional cyclotomic relation. It connects diagram algebras, representation theory, and knot theoretic constructions. For calculations over a coefficient ring, one needs to know whether the diagrammatic spanning elements remain independent after parameters are specialized. The freeness theorem of Goodman and Hauschild Mosley answers that question for admissible integral ground rings: the algebra has a basis of the size predicted by labeled Brauer diagrams. The paper also identifies the algebra with a cyclotomic Kauffman tangle algebra. This mission targets the algebra's freeness and rank assertion.

The cited paper builds on admissibility relations developed with Wilcox and Yu. Its earlier definitions and preliminary statements already appear in Prove2Me mission 92e1197e-907f-4ab8-92be-01ea44f6cfef. The present mission reuses that published layer and poses the deferred freeness theorem and the intermediate results that support it. The distinction matters because two algebras with similar names but different generators or parameter conventions need not have the same rank statement.

Setting

A ground ring SSS is a commutative unital ring with a positive integer rrr and parameters ρ,q,δ0,δ1,…,u1,…,ur\rho,q,\delta_0,\delta_1,\ldots,u_1,\ldots,u_rρ,q,δ0​,δ1​,…,u1​,…,ur​. The parameters ρ,q,δ0,u1,…,ur\rho,q,\delta_0,u_1,\ldots,u_rρ,q,δ0​,u1​,…,ur​ are units, and they satisfy

ρ−1−ρ=(q−1−q)(δ0−1).\rho^{-1}-\rho=(q^{-1}-q)(\delta_0-1).ρ−1−ρ=(q−1−q)(δ0​−1).

The algebra Wn,S,rW_{n,S,r}Wn,S,r​ is generated over SSS by invertible braids gig_igi​, contractions eie_iei​, and an invertible affine generator y1y_1y1​. It obeys the affine BMW relations of Definition 2.1 and the cyclotomic relation ∏j=1r(y1−uj)=0\prod_{j=1}^r(y_1-u_j)=0∏j=1r​(y1​−uj​)=0 of Definition 2.8. The shared published presentation uses indices i=0,…,n−2i=0,\ldots,n-2i=0,…,n−2 for gig_igi​ and eie_iei​, corresponding to the paper's gi+1g_{i+1}gi+1​ and ei+1e_{i+1}ei+1​. At n=0n=0n=0 there are no generators.

The parameters are admissible when q−q−1q-q^{-1}q−q−1 is nonzero and not a zero divisor, weak admissibility holds for every integer shift of the δ\deltaδ relations, and e1,y1e1,…,y1r−1e1e_1,y_1e_1,\ldots,y_1^{r-1}e_1e1​,y1​e1​,…,y1r−1​e1​ are SSS-linearly independent in W2,S,rW_{2,S,r}W2,S,r​. These are the conditions of Definition 3.3, expressed using condition (1) of Theorem 3.2. A morphism of ground rings preserves all δj\delta_jδj​ and uiu_iui​ and permits exactly the four paired sign actions on ρ\rhoρ and qqq in Definition 2.13. Consequently, base change includes the sign twists allowed by the paper.

For the generic case, F=Q(q,u1,…,ur)F=\mathbb Q(q,u_1,\ldots,u_r)F=Q(q,u1​,…,ur​) is the rational function field in algebraically independent variables. Put p=∏jujp=\prod_j u_jp=∏j​uj​, set ρ=p\rho=pρ=p for odd rrr and ρ=q−1p\rho=q^{-1}pρ=q−1p for even rrr, and define δa=∑jγjuja\delta_a=\sum_j\gamma_j u_j^aδa​=∑j​γj​uja​, where γj\gamma_jγj​ is the rational expression in equation (3.6). A shape in Γn\Gamma_nΓn​ is an rrr-tuple of Young diagrams whose total number of boxes is at most nnn and congruent to nnn modulo two. An up–down tableau of shape λ\lambdaλ is a path from the empty tuple to λ\lambdaλ, adding or removing one box at each step. Its set is T(n,λ)T(n,\lambda)T(n,λ).

Formalization targets

The central target is the freeness half of Theorem 6.1. For every admissible integral ground ring SSS and every n≥0n\ge0n≥0,

Wn,S,r≅SS rn(2n−1)!!.W_{n,S,r}\cong_S S^{\,r^n(2n-1)!!}.Wn,S,r​≅S​Srn(2n−1)!!.

Here (−1)!!=1(-1)!!=1(−1)!!=1, so the asserted rank at n=0n=0n=0 is one. A basis indexed by a finite type of that cardinality states both freeness and rank.

The milestone path includes the paper's admissibility equivalences, generic parameter construction, universal admissible integral domain, base change, the spanning family of rn(2n−1)!!r^n(2n-1)!!rn(2n−1)!! elements, the relevant Jones ideal and Hecke quotient results, and the generic structure results. At the generic field, Theorem 4.8 supplies split matrix blocks indexed by Γn\Gamma_nΓn​, with block size ∣T(n,λ)∣|T(n,\lambda)|∣T(n,λ)∣. The count in the proof of Theorem 5.2 is

∑λ∈Γn∣T(n,λ)∣2=rn(2n−1)!!,\sum_{\lambda\in\Gamma_n}|T(n,\lambda)|^2=r^n(2n-1)!!,λ∈Γn​∑​∣T(n,λ)∣2=rn(2n−1)!!,

which agrees with the generic dimension asserted by Theorem 5.2. The final theorem applies over an admissible integral domain, rather than only over FFF.

Significance

The result supplies an exact finite basis for Wn,S,rW_{n,S,r}Wn,S,r​ throughout the admissible integral-domain regime. It fixes the module rank independently of a choice of specialization and gives a numerical benchmark for presentations and representations of these algebras. The generic matrix decomposition also records the simple-block labels and their sizes; the tableau identity explains how those dimensions total the same rank.

Goodman and Hauschild Mosley proved these results. This mission asks for machine-checked proofs of the statements already known in the paper. Its reusable output includes ground-ring morphisms with sign twists, the generic parameter model, and finite tableau types. The published preliminary layer in mission 92e1197e-907f-4ab8-92be-01ea44f6cfef contains two proved and four open results among the six referenced milestones; none of the eight new theorem statements is presented here as already machine proved.

Difficulty

A spanning family alone does not show a basis: specializations can introduce linear dependence, and an equality of dimensions over one field does not itself establish independence over every integral ground ring. The argument also has to maintain the exact admissibility conditions when moving between coefficient rings. Over the generic field, identifying the right semisimple blocks requires the branching shapes and tableau sizes, while the final statement concerns arbitrary admissible integral domains. These are distinct algebraic regimes, and the same presentation and parameter conventions must be kept through each one.

Formalization scope

Lean uses the published GroundParameters, BMW, BMWAdmissible, UAdmissible, and equation (3.6) gamma expression from QAlgorithms.Papers.Independent.Support21.P14. The algebra is the quotient of a free algebra by the source's relations, with zero-based generator indices. The new definition layer records all four sign cases of Definition 2.13, the generic field as a fraction ring of a multivariate polynomial ring over Q\mathbb QQ, and shapes and tableaux as finite-indexed Young diagrams. A generic ground-parameter value is asserted to exist as a theorem because the required unit and compatibility proofs are substantive.

The universal-ring milestone states all five parts of Theorem 3.19 for R‾0\overline R_0R0​ and R‾+\overline R_+R+​; part (5) is read inside FFF, where the universal uuu-admissible ring is the subring generated by q±1q^{\pm1}q±1, (q−1−q)−1(q^{-1}-q)^{-1}(q−1−q)−1, δ0−1\delta_0^{-1}δ0−1​ and ui±1u_i^{\pm1}ui±1​. The base-change statement uses S′⊗SWS'\otimes_S WS′⊗S​W for the source's W⊗SS′W\otimes_S S'W⊗S​S′. Theorem 4.8 is expressed as a product of full matrix algebras with tableau-sized blocks, combining its split and labeling clauses with the block dimensions stated elsewhere in §4. Theorem 6.1's Kauffman-tangle isomorphism is not posed because a corresponding tangle algebra has not been provided here. The cited spanning set is expressed as an indexed family, which remains meaningful when a degenerate coefficient ring identifies elements.

The goal requires an actual basis of cardinality rn(2n−1)!!r^n(2n-1)!!rn(2n−1)!! over an admissible integral domain. A mere dimension equality or spanning claim does not satisfy it. Contributions toward the missing generic decomposition, tableau count, base-change isomorphism, and passage to arbitrary admissible domains are all within scope. The ground-parameter and quotient-presentation definitions are reusable independently of this mission.

Selected references

  • F. M. Goodman and H. Hauschild Mosley, Cyclotomic Birman–Wenzl–Murakami algebras, II: Admissibility Relations and Freeness, 2008, arXiv:math/0612065v5.
16 thms3 active usersReviewed
Quantum Information·Captain: Goku

Entanglement-Assisted Classical Capacity of Noisy Quantum ChannelsResearch Paper

Motivation

Prior entanglement between sender and receiver, which exactly doubles the classical capacity of a noiseless quantum channel, can increase the classical capacity of some noisy quantum channels by an arbitrarily large constant factor depending on the channel, relative to the best known classical capacity achievable without entanglement. The enhancement factor is greatest for very noisy channels, with positive classical capacity but zero quantum capacity. Although such quantum channels can be simulated classically, no violation of causality is implied, because the simulation requires at least as much forward classical communication as the entanglement-assisted classical capacity of the channel being simulated. We obtain exact expressions for the entanglement-assisted capacity of depolarizing and erasure channels in d dimensions.

This mission is the statement-level formalization of Entanglement-Assisted Classical Capacity of Noisy Quantum Channels (arXiv:quant-ph/9904023v5). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

14 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Abstract main result / equation (3): depolarizing assisted capacity (Abstract main result / equation (3): depolarizing assisted capacity, PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Unnumbered C <= CE <= FCCC: A resource-counted finite adaptive bipartite channel-simulation model with arbitrary local ancillas, message-independent prior pure entanglement, free backward classical communication, an actual forward classical arm, and asymptotically faithful reference-preserving simulation. (hard)
  • Erasure flags simulate depolarization and all corresponding capacity inequalities: Source-compatible Q2 from counted noisy-channel calls interleaved with adaptive finite LOCC, initially with no shared entanglement. (hard)
  • Again the difference between the bounds approaches H2(x): A source-pinned noise regime for the asserted limit of the signed quantum-bound gap. (source-ambiguity)
  • Author note [9]: A transpose/label convention or restriction making the three induced classical transition matrices literally identical. (source-ambiguity)

Selected references

  • Entanglement-Assisted Classical Capacity of Noisy Quantum Channels, arXiv:quant-ph/9904023v5, https://arxiv.org/abs/quant-ph/9904023v5
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Quantum Information·Captain: Goku

The operational meaning of quantum conditional informationResearch Paper

Motivation

How correlated are two quantum systems from the perspective of a third? We answer this by providing an optimal quantum state redistribution protocol for multipartite product sources. Specifically, given an arbitrary quantum state of three systems, where Alice holds two and Bob holds one, we identify the cost, in terms of quantum communication and entanglement, for Alice to give one of her parts to Bob. The communication cost gives the first known operational interpretation to quantum conditional mutual information. The optimal procedure is self-dual under time reversal and is perfectly composable. This generalizes known protocols such as the state merging and fully quantum Slepian-Wolf protocols, from which almost every known protocol in quantum Shannon theory can be derived.

This mission is the statement-level formalization of The operational meaning of quantum conditional information (arXiv:quant-ph/0612050v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

8 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Exact state-redistribution rate region and optimal corner (Main result: exact state-redistribution rate region and corner, Eqs. (1)–(2), PDF p. 2). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • w-state: Independently moderated correction of the printed W-state numerical communication cost (source-ambiguity)
  • zero-communication-entanglement: Independently moderated correction of the printed flagged-state entanglement-cost sign (source-ambiguity)

Selected references

  • The operational meaning of quantum conditional information, arXiv:quant-ph/0612050v2, https://arxiv.org/abs/quant-ph/0612050v2
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Quantum Information·Captain: Goku

The capacity of the quantum depolarizing channelResearch Paper

Motivation

The information carrying capacity of the d-dimensional depolarizing channel is computed. It is shown that this capacity can be achieved by encoding messages as products of pure states belonging to an orthonormal basis of the state space, and using measurements which are products of projections onto this same orthonormal basis. In other words, neither entangled signal states nor entangled measurements give any advantage for information capacity. The result follows from an additivity theorem for the capacity of the product of the depolarizing channel with an arbitrary channel. We establish the Amosov-Holevo-Werner p-norm conjecture for this product channel for all p >= 1, and deduce from this the additivity of the minimal entropy and of the Holevo quantity.

This mission is the statement-level formalization of The capacity of the quantum depolarizing channel (arXiv:quant-ph/0204172v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

14 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Depolarizing channel: exact unassisted classical capacity (Theorem 1 / abstract: exact unassisted classical capacity and basis strategy, 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.

Selected references

  • The capacity of the quantum depolarizing channel, arXiv:quant-ph/0204172v2, https://arxiv.org/abs/quant-ph/0204172v2
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Quantum Information·Captain: Goku

Capacities of Quantum Erasure ChannelsResearch Paper

Motivation

The quantum analog of the classical erasure channel provides a simple example of a channel whose asymptotic capacity for faithful transmission of intact quantum states, with and without the assistance of a two-way classical side channel, can be computed exactly. We derive the quantum and classical capacities for the quantum erasure channel and related channels, and compare them to the depolarizing channel, for which only upper and lower bounds on the capacities are known.

This mission is the statement-level formalization of Capacities of Quantum Erasure Channels (arXiv:quant-ph/9701015v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

8 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Exact capacities of the qubit quantum erasure channel (Eq. (2), PDF p. 2). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Selected references

  • Capacities of Quantum Erasure Channels, arXiv:quant-ph/9701015v2, https://arxiv.org/abs/quant-ph/9701015v2
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Quantum Information·Captain: Goku

An additive and operational entanglement measure: conditional entanglement of mutual informationResearch Paper

Motivation

Based on the monogamy of entanglement, we develop the technique of quantum conditioning to build an {\it additive} entanglement measure: the conditional entanglement of mutual information. Its {\it operational} meaning is elaborated to be the minimal net "flow of qubits" in the process of partial state merging. The result and conclusion can also be generalized to multipartite entanglement cases.

This mission is the statement-level formalization of An additive and operational entanglement measure: conditional entanglement of mutual information (arXiv:0804.3683v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

12 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Proposition 1: bipartite additivity (Proposition 1: bipartite additivity (the page-1 seed pinned to its numbered theorem), PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Unnumbered: fixed-extension partial state merging cost and route independence: Admissible resource/protocol class and ancillary-work accounting for the signed net-qubit PSM/PSD minimum (source-ambiguity)
  • Proposition 2: CEMI as optimized partial state merging cost: Admissible resource/protocol class and ancillary-work accounting for the signed net-qubit PSM/PSD minimum (source-ambiguity)
  • Proposition 4: multipartite CEMI as optimized partial state merging cost: Admissible resource/protocol class and ancillary-work accounting for the signed net-qubit PSM/PSD minimum (source-ambiguity)
  • Unnumbered: reversed process partial state distribution: Admissible resource/protocol class and ancillary-work accounting for the signed net-qubit PSM/PSD minimum (source-ambiguity)

Selected references

  • An additive and operational entanglement measure: conditional entanglement of mutual information, arXiv:0804.3683v2, https://arxiv.org/abs/0804.3683v2
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Operations ResearchOptimizationQuantum Information·Captain: mikedeng1

An Optimal Product-State Approximation for 2-Local Quantum Hamiltonians with Positive Terms: Rounding Level 2 of the Quantum Lasserre Hierarchy Gives a 1/2-Approximation for Quantum Max CutResearch Paper

Motivation

Quantum Max Cut assigns a qubit to each vertex of a weighted graph and a two-qubit energy term to each edge. It asks for a quantum state with high total energy. The problem is a quantum analogue of graph Max Cut, but states can be entangled and edge terms act on a Hilbert space whose dimension grows exponentially with the number of vertices. Approximation algorithms therefore need a compact way to reason about the best quantum state without describing that state explicitly. Gharibian and Parekh's 2019 algorithm used product-state rounding for a quantum Max Cut relaxation; Parekh and Thompson's level-2 work showed why stronger quantum relaxations matter. The present paper combines a level-2 relaxation with a different treatment of highly valued edges to obtain a one-half guarantee.

The target is a known result from the pinned version arXiv:2206.08342v2, not an open conjecture. This mission isolates its Quantum Max Cut theorem. The paper also treats other positive 2-local Hamiltonians and a separate guarantee for graphs of prescribed minimum degree; neither is part of this target.

Setting

Let G=(V,E)G=(V,E)G=(V,E) be a finite undirected graph with a nonnegative weight wijw_{ij}wij​ on each edge, and put one qubit at each vertex. Write Xi,Yi,ZiX_i,Y_i,Z_iXi​,Yi​,Zi​ for the three Pauli operators acting on qubit iii. The edge Hamiltonian and total Quantum Max Cut Hamiltonian are

Hij=I−XiXj−YiYj−ZiZj4,H=∑{i,j}∈EwijHij.H_{ij}=\frac{I-X_iX_j-Y_iY_j-Z_iZ_j}{4},\qquad H=\sum_{\{i,j\}\in E}w_{ij}H_{ij}.Hij​=4I−Xi​Xj​−Yi​Yj​−Zi​Zj​​,H={i,j}∈E∑​wij​Hij​.

Every undirected edge appears once. A density matrix σ\sigmaσ is positive semidefinite with trace one. Its energy is Tr⁡(Hσ)\operatorname{Tr}(H\sigma)Tr(Hσ), and λmax⁡(H)\lambda_{\max}(H)λmax​(H) is the largest energy attainable by any density matrix, including an entangled one.

A Pauli polynomial is a real linear combination of tensor products of I,X,Y,ZI,X,Y,ZI,X,Y,Z. A monomial's degree counts its nonidentity factors. A kkk-positive pseudo-density ρ~\widetilde\rhoρ​ is Hermitian, has trace one, and satisfies Tr⁡(ρ~P2)≥0\operatorname{Tr}(\widetilde\rho P^2)\ge0Tr(ρ​P2)≥0 for every Pauli polynomial PPP of degree at most kkk. The level-2 quantum Lasserre relaxation maximizes Tr⁡(Hρ~)\operatorname{Tr}(H\widetilde\rho)Tr(Hρ​) over all such pseudo-densities. It is an upper bound on the unrestricted quantum optimum, even though ρ~\widetilde\rhoρ​ itself need not be positive semidefinite. These definitions are from pp. 6–8 of the paper.

For an edge, its relaxed value is μij=Tr⁡(Hijρ~)\mu_{ij}=\operatorname{Tr}(H_{ij}\widetilde\rho)μij​=Tr(Hij​ρ​). The rescaled value vijv_{ij}vij​ is defined by μij=(1+3vij)/4\mu_{ij}=(1+3v_{ij})/4μij​=(1+3vij​)/4. Algorithm 4 chooses a threshold γ\gammaγ, puts every edge with vij>γv_{ij}>\gammavij​>γ in LLL, and calls vertices incident to no edge in LLL the set BBB. It assigns the two-qubit mixed state (I−ZiZj)/4(I-Z_iZ_j)/4(I−Zi​Zj​)/4 to each edge in LLL. Vertices in BBB receive single-qubit states obtained by normalizing three independent Gaussian projections of the relaxation's rounding vectors. The output ρ\rhoρ is the product of those factors, as in equation (5), p. 14. The large edges form a matching at the selected threshold, so those factors occupy disjoint qubits. The Gaussian draw is the algorithm's only randomness.

Formalization targets

Theorem 3: a one-half approximation

The goal is the paper's Theorem 3, p. 17. A single threshold must work for every graph and every nonnegative edge weighting:

∃γ∈(−1/3,1]∀H of the form above,ETr⁡(HρAlg4)≥12λmax⁡(H).\exists\gamma\in(-1/3,1]\quad \forall H\text{ of the form above},\qquad \mathbb E\operatorname{Tr}(H\rho_{\mathrm{Alg4}}) \ge \frac12\lambda_{\max}(H).∃γ∈(−1/3,1]∀H of the form above,ETr(HρAlg4​)≥21​λmax​(H).

The level-2 solution used by Algorithm 4 is optimal for the given HHH. The goal also says that the matrix output is a density matrix for every Gaussian outcome. Its threshold is existential because the theorem does not fix a decimal constant; the paper subsequently selects 0.9110.9110.911 for its analysis.

Supporting results

The fourteen milestones follow the order in which the proof of Theorem 3 uses them.

  1. Relaxation and assembly. Lemma 9 (p. 28): the level-kkk value νk(H)\nu_k(H)νk​(H) is at least λmax⁡(H)\lambda_{\max}(H)λmax​(H). Proposition 1 (p. 9), for strictly quadratic 2-local Hamiltonians (Definition 3): if Tr⁡(Hijρ)≥αμij\operatorname{Tr}(H_{ij}\rho)\ge\alpha\mu_{ij}Tr(Hij​ρ)≥αμij​ on every edge, then Tr⁡(Hρ)≥αλmax⁡(H)\operatorname{Tr}(H\rho)\ge\alpha\lambda_{\max}(H)Tr(Hρ)≥αλmax​(H). Lemma 5 (p. 17): μij∈[0,1]\mu_{ij}\in[0,1]μij​∈[0,1], vij∈[−1/3,1]v_{ij}\in[-1/3,1]vij​∈[−1/3,1], sij∈[−1,1]s_{ij}\in[-1,1]sij​∈[−1,1] for k≥2k\ge2k≥2.
  2. Edges inside BBB. Lemma 4 (p. 12): for a k×dk\times dk×d standard Gaussian matrix ZZZ and unit u,vu,vu,v,
E[Zu∥Zu∥⋅Zv∥Zv∥]=F(k,u⋅v),F(k,t)=2k(Γ(k+12)Γ(k2))2t 2F1(12,12;k2+1;t2).\mathbb E\Big[\tfrac{Zu}{\|Zu\|}\cdot\tfrac{Zv}{\|Zv\|}\Big]=F(k,u\cdot v),\qquad F(k,t)=\frac2k\Big(\frac{\Gamma(\frac{k+1}2)}{\Gamma(\frac k2)}\Big)^2t\,{}_2F_1\big(\tfrac12,\tfrac12;\tfrac k2+1;t^2\big).E[∥Zu∥Zu​⋅∥Zv∥Zv​]=F(k,u⋅v),F(k,t)=k2​(Γ(2k​)Γ(2k+1​)​)2t2​F1​(21​,21​;2k​+1;t2).

Equation (7) (p. 17): Gaussian product-state rounding earns (1+F(3,vij))/4(1+F(3,v_{ij}))/4(1+F(3,vij​))/4 in expectation on edge ijijij. Lemma 6 (p. 18) reduces min⁡v∈(−1/3,γ](1+F(3,v))/(1+3v)≥1/2\min_{v\in(-1/3,\gamma]}(1+F(3,v))/(1+3v)\ge1/2minv∈(−1/3,γ]​(1+F(3,v))/(1+3v)≥1/2 to two checks at γ\gammaγ; Definition 13 (p. 19) asserts that γ=0.911\gamma=0.911γ=0.911 passes them; Fact 1 (p. 16) is the resulting factor 1/21/21/2 on edges with both ends in BBB. 3. Monogamy. The 4×44\times44×4 SWAP Gram matrix M(p,q,r)M(p,q,r)M(p,q,r) of three qubits is positive semidefinite (p. 20). Lemma 8 (p. 22): M⪰0M\succeq0M⪰0 and q≤0q\le0q≤0 imply p≥−3/2p\ge-\sqrt3/2p≥−3​/2. Fact 2 (p. 16): if vij>0.911v_{ij}>0.911vij​>0.911 then vik<1/3v_{ik}<1/3vik​<1/3. Remark 3 (p. 19): the large edges form a matching. 4. Edges touching LLL. Equation (12) (p. 19): (I−Z⊗Z)/4(I-Z\otimes Z)/4(I−Z⊗Z)/4 earns 1/2≥μij/21/2\ge\mu_{ij}/21/2≥μij​/2 on a large edge. The last display of the proof of Theorem 3 (p. 19): an edge adjacent to LLL earns exactly 1/4>μij/21/4>\mu_{ij}/21/4>μij​/2.

Significance

The theorem guarantees half of the optimum over all quantum states while returning a state built from one- and two-qubit product factors. This is stronger than a guarantee relative only to the best product state: the benchmark permits entanglement. It also explains why a level-2 relaxation has algorithmic value for this problem. The comparison and the claimed approximation factor are established in the paper; formalizing them would leave a reusable verified interface for finite-qubit Pauli polynomials, pseudo-densities, and Gaussian product-state rounding.

The formal work still needed is a machine-checked proof of the known theorem and its milestones. The published register, Pauli, density-matrix and standard-Gaussian-vector definitions can be reused. The source's separate results for other positive 2-local Hamiltonians would need additional models and theorems, beyond this mission.

Difficulty

Level-1 Gaussian product-state rounding alone does not reach one half uniformly: the paper identifies an edge range where its ratio falls below 0.50.50.5. Large edge values cannot be handled by the same rounding estimate. A level-2 pseudo-density supplies stronger constraints between adjacent edges, but it is not itself a physical state, so ordinary positivity of ρ~\widetilde\rhoρ​ is unavailable. The source's SWAP matrix and threshold analysis express the needed restrictions. The paper's printed dual certificate for Lemma 8 has a coordinate-order erratum; the lemma's statement remains the target.

Formalization scope

Qubits are indexed by Fin n (the paper uses 1,…,n1,\ldots,n1,…,n), with basis Fin n → Bool. Operators are complex matrices. The real part of a trace represents the expectation of a Hermitian expression. The maximum eigenvalue is stated through comparison with every density matrix; for Hermitian HHH, this is equivalent to comparing with its largest eigenvalue. Expected energy is a Bochner integral over a probability measure carrying independent standard Gaussian coordinates. A zero Gaussian projection is assigned Bloch vector zero, giving the maximally mixed one-qubit state at that outcome.

The rounding vectors are given with unit norms and exactly the Gram matrix obtained from the level-2 solution. The output state is computed as the matrix product in equation (5); energy is traced against that matrix. Positivity is required for every real degree-2 Pauli polynomial, and the pseudo-density is required to be optimal. These choices exclude vacuous variants based on degree-1 positivity, free Bloch vectors, or edge energies supplied as assumptions. The finite operator model also covers an empty graph; the approximation inequality there is 0≥00\ge00≥0.

The statement formalizes the approximation guarantee and state validity. The polynomial running-time clause of the paper's general approximation definition is outside this Lean statement. Reusable contributions include the Pauli-polynomial interface, matrix and moment identities for pseudo-densities, integrability and measurability facts for the Gaussian rounding, and the SWAP semidefinite bound.

Selected references

  • Ojas Parekh and Kevin Thompson, An Optimal Product-State Approximation for 2-Local Quantum Hamiltonians with Positive Terms, arXiv preprint, 2022, version 2 dated 2026. arXiv:2206.08342.
  • Sevag Gharibian and Ojas Parekh, Almost Optimal Classical Approximation Algorithms for a Quantum Generalization of Max-Cut, APPROX/RANDOM, 2019. DOI:10.4230/LIPIcs.APPROX-RANDOM.2019.31.
  • Ojas Parekh and Kevin Thompson, Application of the Level-2 Quantum Lasserre Hierarchy in Quantum Approximation Algorithms, ICALP, 2021. arXiv:2105.05698.
  • Jop Briët, Fernando Mário de Oliveira Filho and Frank Vallentin, Grothendieck Inequalities for Semidefinite Programs with Rank Constraint, Theory of Computing 10, 2014, 77–105. Journal article.
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