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CombinatoricsGraph TheoryOperations Research·Captain: mikedeng1

Bounding Residence Times for Atomic Dynamic Routings: If No Later Entrant Leaves the Subnetwork First, an Agent Exits by Time r0 plus the Longest Path Length plus the Earlier Agents Still InsideResearch Paper

Motivation

In atomic dynamic routing, indivisible agents (vehicles, packets, travellers) enter a network over time and travel along fixed routes. Each road admits a limited number of agents per unit of time, so agents queue at its entrance. A basic question for traffic models, packet-switching networks and dynamic routing games is how long an agent can stay in the network, its residence time. Upper bounds on residence times are what make it possible to bound queue lengths and the price of anarchy in dynamic routing games.

Greedy packet scheduling, where an edge never idles while packets wait for it, was studied by Cidon, Kutten, Mansour and Peleg (SIAM J. Comput. 1995), who showed that cycles can make delays large, and by Mansour and Patt-Shamir (J. Algorithms 1993), who bounded delivery times when every route is a shortest path. Cao, Chen, Chen and Wang (MOR 2022) prove a bound for arbitrary routes on acyclic networks. It holds under any rule that decides which waiting agent may leave next, and agents may keep entering forever. Their Theorem 1 is the goal of this mission. The paper then uses it to show that equilibria of three dynamic routing games on series-parallel networks have bounded queues (§6).

Setting

A network G=(V,E)G=(V,E)G=(V,E) is a finite directed multigraph (parallel edges allowed) that is acyclic. Every edge has unit length and unit capacity. A path is a sequence of edges, each starting where the previous one ends. LvwL_{vw}Lvw​ is the number of edges of a longest vvv-www path.

Time is discrete, 0,1,2,…0,1,2,\dots0,1,2,…. Agents form a set Δ\DeltaΔ, possibly infinite. At each time finitely many agents enter. Agent iii enters at time rir_iri​ at his origin oio_ioi​ and follows a fixed route, a nonempty oio_ioi​-did_idi​ path. The tail of each edge holds a buffer. Two rules govern the dynamics:

  • (A1) an agent reaching a vertex that is not his destination enters the buffer of his next edge at once;
  • (A2) at every integer time, whenever a buffer is nonempty, exactly one agent leaves it and reaches the head of the edge one time unit later; the others wait.

No rule says which agent leaves. Every choice consistent with (A2) is an admissible run. An agent exits GGG on reaching his destination. His residence time is his exit time minus his entry time (Definition 1).

Fix a focal agent ζ\zetaζ with entry time rrr. GζG_\zetaGζ​ is the subnetwork formed by all oζo_\zetaoζ​-dζd_\zetadζ​ paths. For an integer time r0r_0r0​:

  • Aζ,pA_{\zeta,p}Aζ,p​ is the set of agents who enter after time rrr and use an edge of GζG_\zetaGζ​;
  • Bζ,p(r0)B_{\zeta,p}(r_0)Bζ,p​(r0​) is the set of agents i≠ζi\neq\zetai=ζ who entered by time rrr, are still inside GGG at time r0r_0r0​, and use an edge of GζG_\zetaGζ​.

An agent exits GζG_\zetaGζ​ when he reaches the head of the last edge of his route lying in GζG_\zetaGζ​.

Formalization targets

Goal: Theorem 1 (p. 7)

For every admissible run and every integer r0≥rr_0\ge rr0​≥r: if no agent of Aζ,pA_{\zeta,p}Aζ,p​ exits GζG_\zetaGζ​ before ζ\zetaζ exits GGG, then

tζ ≤ r0+Loζdζ+∣Bζ,p(r0)∣,t_\zeta\ \le\ r_0+L_{o_\zeta d_\zeta}+\bigl|B_{\zeta,p}(r_0)\bigr|,tζ​ ≤ r0​+Loζ​dζ​​+​Bζ,p​(r0​)​,

where tζt_\zetatζ​ is the exit time of ζ\zetaζ.

Milestones (§3.2, p. 9)

When ζ\zetaζ is still inside GGG at r0r_0r0​, the proof follows tokens: imaginary markers that ζ\zetaζ produces from time r0r_0r0​ on, and that travel with the agents leaving buffers ((s1), (s2), p. 8). The milestones are the paper's statements about them, with L=LoζdζL=L_{o_\zeta d_\zeta}L=Loζ​dζ​​:

  1. (p1) each agent holds at most one token, and a buffer never contains more tokens than agents;
  2. (p2) the agent leaving ζ\zetaζ's buffer always holds exactly one token;
  3. (p3) after r0r_0r0​, ζ\zetaζ produces a new token only while he waits;
  4. Claim 1 the induction step of Lemma 1 at the vertices where token kkk departs right after a smaller token;
  5. Lemma 1 token kkk departs every vertex vvv of its trail inside GζG_\zetaGζ​ by time r0+(L−Lvdζ+k−1)r_0+(L-L_{vd_\zeta}+k-1)r0​+(L−Lvdζ​​+k−1);
  6. token exit token kkk exits GζG_\zetaGζ​ by time r0+(L+k−1)r_0+(L+k-1)r0​+(L+k−1).

Significance

The result. The bound does not depend on the rule that selects the leaving agent, so it covers every queueing discipline at once: FIFO, global agent priorities, and the edge-priority rules of earlier dynamic routing games. With r0=rr_0=rr0​=r and no later entrants on GζG_\zetaGζ​, it gives Corollary 1: the residence time of ζ\zetaζ is at most Loζdζ+∣Bζ,p(r)∣L_{o_\zeta d_\zeta}+|B_{\zeta,p}(r)|Loζ​dζ​​+∣Bζ,p​(r)∣. Example 1 (p. 8) shows that the bound can be attained. The freedom in r0r_0r0​ is what §6 uses to show that queue lengths stay bounded at equilibria of dynamic routing games on series-parallel networks.

Formalizing it. The theorem is proved on paper. No machine-checked version is known to exist, and the platform has no rule-free model of atomic dynamic routing. The mission adds that model: a run is a set of leave times constrained by (A1)–(A2), not a fixed simulation. It also adds the multi-token process and the paper's chain of statements leading to Theorem 1.

Difficulty

The obvious argument is wrong. One might reason that ζ\zetaζ travels at most LoζdζL_{o_\zeta d_\zeta}Loζ​dζ​​ edges and each earlier agent delays him at most once, giving the bound at once. The paper notes (p. 7) that this intuition fails even with two agents: a single agent can delay ζ\zetaζ more than ∣Δ∣|\Delta|∣Δ∣ times, because delays propagate through other buffers. Bounding the total therefore means tracking chains of delays across the network rather than charging each delay to one agent.

Formally, the hard parts are:

  • the run is only constrained, not determined;
  • the token process is defined by recursion over time, using the unique leaver of each buffer;
  • (p1)–(p3) are invariants proved by induction on time;
  • Lemma 1 combines induction on the token index with longest-path inequalities in an acyclic graph.

Formalization scope

  • Model. Network V E (tail and head maps) with finite V, E and a hypothesis Acyclic: no nonempty closed walk. Paths are edge lists. longest v w is the supremum of path lengths in N\mathbb NN; it is a maximum wherever it is used.

  • Runs. RunData holds entry times, routes, origins and destinations, and leave times leave i j in N∪{∞}\mathbb N\cup\{\infty\}N∪{∞} for the jjj-th edge of iii's route, numbered from 000. IsADR states that:

    • routes are nonempty origin–destination paths;
    • finitely many agents enter per time;
    • nobody leaves a buffer before entering it;
    • (A2) holds, as unique existence of the leaver of each nonempty buffer at each time.

    Agents form an arbitrary type and may be infinitely many. An agent may never be served (leave time ∞\infty∞), as in the paper, so the theorem also asserts that ζ\zetaζ exits.

  • Derived objects. Exit times, GζG_\zetaGζ​, Aζ,pA_{\zeta,p}Aζ,p​, Bζ,p(r0)B_{\zeta,p}(r_0)Bζ,p​(r0​) and the exit time from GζG_\zetaGζ​ are definitions computed from the run, never free parameters. ∣Bζ,p(r0)∣|B_{\zeta,p}(r_0)|∣Bζ,p​(r0​)∣ is Set.ncard of a set that is finite under IsADR.

  • Tokens. The token milestones assume that ζ\zetaζ is inside GGG at r0r_0r0​, as §3.1 requires when starting the construction. Tokens are indexed from 111. A new token gets index one plus the number produced so far. Bounds with subtraction are written additively over N\mathbb NN, e.g. s+Lvdζ+1≤r0+L+ks+L_{vd_\zeta}+1\le r_0+L+ks+Lvdζ​​+1≤r0​+L+k, which is the same inequality over the integers.

  • Ruled out. None of these is used, since each proves a different statement: a fixed tie-breaking rule (FIFO or priorities), exit times as free parameters, finitely many agents, or dropping acyclicity, which Remark 2 shows is necessary.

Contributions welcome: proofs of the token invariants, of Lemma 1, and of the goal. The network and run definitions can be reused for the paper's other results (Theorem 2 on uniform capacities, the routing games of §5–6).

Selected references

  • Z. Cao, B. Chen, X. Chen, C. Wang, Bounding residence times for atomic dynamic routings, Mathematics of Operations Research, 2022 (accepted manuscript: WRAP 160244). https://doi.org/10.1287/moor.2021.1242 , https://wrap.warwick.ac.uk/160244
  • Y. Mansour, B. Patt-Shamir, Greedy packet scheduling on shortest paths, Journal of Algorithms 14(3):449–465, 1993.
  • I. Cidon, S. Kutten, Y. Mansour, D. Peleg, Greedy packet scheduling, SIAM Journal on Computing 24(1):148–157, 1995.
  • T. Harks, B. Peis, D. Schmand, B. Tauer, L. Vargas Koch, Competitive packet routing with priority lists, ACM Transactions on Economics and Computation 6(1):4:1–4:26, 2018.
10 thms1 active userReviewed
Quantum Information·Captain: Goku

Bath dimension and initial entropy for closed repeated use of a quantum channelResearch Paper

Motivation

We characterize the bath resources needed to supply repeated uses of a fixed finite-dimensional quantum channel in a closed device. For each horizon TTT, one bath, one initial state and one repeated unitary are fixed before the user. Each output is returned before the next input arrives; no reset, discard, fresh ancilla or uncounted controller is available. Approximation error must vanish against arbitrary adaptive users with quantum memory and references. Writing r=lim⁡log⁡2(RT)/Tr=\lim \log_2(R_T)/Tr=limlog2​(RT​)/T for the bath dimension rate and s=lim⁡S(ωT)/Ts=\lim S(ω_T)/Ts=limS(ωT​)/T for the actual initial entropy rate, we prove that the achievable region is exactly s≥0s\ge 0s≥0, r+s≥hr+s\ge hr+s≥h and r−s≥κr-s\geκr−s≥κ. Here hhh is maximum entropy exchange and κκκ is a smoothed independent-reference extension cost, with the zero-error limit taken before the supremum over full-rank inputs. Its exact fixed-input form is an affine transform of the zero-leakage quantum privacy funnel. The minimum dimension rate is (h+κ)/2(h+κ)/2(h+κ)/2. The proof combines entropy converses, a bath-dimension-independent support repair, and a closed adaptive implementation of encoder-only fully quantum Slepian--Wolf recycling. All seeds, clocks, workspace and retained residues are counted. Worked examples include dephasing, pure replacement and a qubit channel with 0<κ<h0<κ<h0<κ<h. No computability of κκκ or efficient circuit synthesis is claimed. △ Less

This mission is the statement-level formalization of Bath dimension and initial entropy for closed repeated use of a quantum channel (arXiv:2609.18267v1). 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 3.1: uniform collision gain (Theorem 3.1, PDF p. 6). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Theorem 2.1 (seed paper result): exact bath-dimension/initial-entropy rate region: Closed all-horizon causal device and complete adaptive process metric, actual rate-limit region, counted padding/internal-purification transformations (hard)
  • Theorem 2.2: same-spectrum converse: Same actual initializer in two complete adaptive tester experiments and all-integer liminf resource rates (hard)
  • Theorem 5.1: causal balancing for any fixed finite exact witness: Causal block compiler with actual flat initializer, repeated-unitary semantics and separately converging seed/data rates (hard)
  • Proposition 7.1: unitary channels: Complete all-horizon memory rate c_seq and bath-free repeated-unitary realization (hard)
  • Proposition 7.2: qubit dephasing and exact streaming corner: Counted exact streaming process from independent Pauli generators, ordered history words and one clocked unitary (hard)
  • Proposition 7.3: pure replacement: Pure-replacer complete operating memory rate and counted preallocated-cell/clock process (hard)
  • Proposition 8.1: shared-seed marginal/complete separation: Shared-bit repeated controlled-Z process, product-marginal repeatability and supremum complete adaptive error (hard)
  • Section 8, unnumbered: zero memory rate iff unitary: Zero complete operating memory rate as an asymptotic repeated-service property (hard)
  • Lemma A.1: fixed adaptive spectral concentration projector: Reachable states of adaptive controllers with fresh comparison channels and untouched spent Lambda outputs (hard)
  • Lemma A.2: simultaneous bath/exterior/source support and spectral-cap cuts: Exact comparison block and pure complete exterior, including future-accessed spectators and their purifiers (hard)
  • Lemma A.4: exact integer wires and reversible flat-stock preparation: Reversible flat-stock preparation and permanent wire/tranche allocation with immediate collision service (hard)
  • Proposition A.5: joint recycling, every prefix, and one repeated unitary: Joint comparison boundary invariant, actual block composition, every prefix and counted repeated-unitary clock (hard)
  • Proposition A.6: exact actual spectrum and every-horizon limits: Every-integer-horizon compiled family with actual flat spectrum, exact physical counts and separate seed/data limits (hard)

Selected references

  • Bath dimension and initial entropy for closed repeated use of a quantum channel, arXiv:2609.18267v1, https://arxiv.org/abs/2609.18267v1
15 thms1 active userReviewed
Quantum Information·Captain: Goku

Entanglement-assisted capacity of constrained quantum channelResearch Paper

Motivation

In this paper we fill the gap in previous works by proving the formula for entanglement-assisted capacity of quantum channel with additive constraint (such as bosonic Gaussian channel). The main tools are the coding theorem for classical-quantum constrained channels and a finite dimensional approximation of the input density operators for entanglement-assisted capacity. The new version contains improved formulation of sufficient conditions under which suprema in the capacity formulas are attained.

This mission is the statement-level formalization of Entanglement-assisted capacity of constrained quantum channel (arXiv:quant-ph/0211170v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

1 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Trace-norm compactness of an energy sublevel (§3, unnumbered Lemma (proof on PDF p.11), PDF p. 10). 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

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

  • §1, Proposition 1: An operational constrained c-q coding model on arbitrary input alphabets and general trace-class output states, with genuine product outputs, bounded POVMs, maximal message error, and a liminf achievable-rate capacity. (hard)
  • §1, Proposition 2 (conclusion on p.3): Borel-probability barycenters and integrated entropy for trace-norm state-valued maps, coupled to a genuine bounded-below unbounded selfadjoint observable with Gibbs trace. (hard)
  • §2, Proposition 3, (19)--(20): Parallel general trace-class CPTP channel powers, constrained block codes and two separately defined information optimizations with different feasible sets. (hard)
  • §3, Proposition 4, (30): Energy-constrained operational entanglement-assisted block capacity on arbitrary Hilbert spaces, plus actual purification/reference extension and the finite-entropy mutual-information interface. (hard)
  • §3, (31)--(32): The special locally encoded common-resource assisted ensemble class and its block Holevo optimum, distinct from operational assisted codes. (hard)
  • §3, assertion before (33): Constrained channel mutual information for arbitrary entangled block states, with actual reference purifications and additive energy expectation. (hard)
  • §3, finite-rank approximation and (35) on p.10: Constructed positive-eigenvalue spectral truncations, their normalized purifications, and channel mutual information in one compatible operator model. (hard)
  • §3, Proposition 5, (37): Actual dual-channel domination for bounded-below unbounded output observables, Gibbs trace, and an operational assisted capacity attaining state. (hard)
  • Closing paragraph; (30) with (36): Extended-valued relative-entropy channel mutual information coupled to operational assisted capacity without either entropy restriction. (hard)

Selected references

  • Entanglement-assisted capacity of constrained quantum channel, arXiv:quant-ph/0211170v2, https://arxiv.org/abs/quant-ph/0211170v2
3 thms1 active userReviewed
Quantum Information·Captain: Goku

The mixed Schur transform: efficient quantum circuit and applicationsResearch Paper

Motivation

The Schur transform, which block-diagonalizes the tensor representation U⊗nU^{\otimes n}U⊗n of the unitary group Ud\mathbf{U}_dUd​ on nnn qudits, is an important primitive in quantum information and theoretical physics. We give a generalization of its quantum circuit implementation due to Bacon, Chuang, and Harrow (SODA 2007) to the case of mixed tensor U⊗n⊗Uˉ⊗mU^{\otimes n} \otimes \bar{U}^{\otimes m}U⊗n⊗Uˉ⊗m, where Uˉ\bar{U}Uˉ is the dual representation. This representation is the symmetry of unitary-equivariant channels, which find various applications in quantum majority vote, multiport-based teleportation, asymmetric state cloning, black-box unitary transformations, etc. The "mixed" Schur transform contains several natural extensions of the representation theory used in the Schur transform, in which the main ingredient is a duality between the mixed tensor representations and the walled Brauer algebra. Another element is an efficient implementation of a "dual" Clebsch-Gordan transform for Uˉ\bar{U}Uˉ. The overall circuit has complexity O~((n+m)d4)\widetilde{O} ((n+m)d^4)O((n+m)d4). Finally, we show how the mixed Schur transform enables efficient implementation of unitary-equivariant channels in various settings and discuss other potential applications, including an extension of permutational quantum computing that includes partial transposes.

This mission is the statement-level formalization of The mixed Schur transform: efficient quantum circuit and applications (arXiv:2310.01613v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

2 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Two-input conclusive teleportation: exact success and corrected output (Section 5.1.1: two-input conclusive teleportation success, PDF p. 29). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Main result / Corollary 4.12: efficient mixed Schur isometry: Concrete signed-staircase rational irreps with orthonormal GT and dimension-truncated path coordinates, their fixed mixed Schur isometry, and its binary channel/resource semantics. (hard)
  • Section 3.3 and Remark 3.1: cascade correctness and factor-order flexibility: Ordinary and dual CG maps on the concrete signed GT sectors, path extension/reindexing and canonical permutations for factor type words. (hard)
  • Theorem 4.5: multiplicity-free dual Wigner–Eckart: Concrete rational-irrep actions in GT bases and the actual multiplicity-free dual CG matrix. (hard)
  • Proposition 4.6: dual CG coefficient tensor operators: The source dual CG coefficient blocks and their concrete irrep actions. (hard)
  • Lemma 4.7: restriction of the coefficient tensor operators: Compatible GT restriction inclusions between U(d) and U(d-1) and actual coefficient tensor blocks. (hard)
  • Proposition 4.8: reduced Wigner coefficient recursion: The constructed restriction blocks and reduced coefficients relative to the lower-dimensional source dual CG transform. (hard)
  • Section 4.3 Eqs.(69)–(71): recursive factorization: The modified lower dual transform and reduced Wigner rotation on valid dependent label sectors. (hard)
  • Remark 4.10: coherent reduced Wigner operator synthesis: A concrete reduced-Wigner target in the source GT conventions and its uniform reversible finite-precision coefficient/synthesis computation. (hard)
  • Corollary 4.11: efficient dual Clebsch–Gordan transform: The actual coherent dual CG transform over bounded staircase labels and its encoded circuit/workspace interface. (hard)
  • Remark 4.13: extensions to elementary and symmetric-power input irreps: Remark 4.13: extensions to elementary and symmetric-power input irreps (source-ambiguity)
  • Proposition 5.2: deterministic one-input teleportation implementation: Proposition 5.2: deterministic one-input teleportation implementation (source-ambiguity)
  • Section 5.1.1: random symmetric unitaries and random equivariant channels: Section 5.1.1: random symmetric unitaries and random equivariant channels (source-ambiguity)
  • Proposition 5.5: Choi-only average-case observable prediction: A Choi-measurement training law, actual learned estimator function and cost-bearing classical learner implementing the HCP adaptation. (hard)
  • Lemma 5.10: Schur-sparse Choi and square-root block encodings: Valid Schur-label encodings of the actual fixed transform and two-sided sparse row/column/value oracle programs with gate/query accounting. (hard)
  • Proposition 5.11: output expectation estimation from a Choi square root: Proposition 5.11: output expectation estimation from a Choi square root (source-ambiguity)
  • Section 5.1.3: combined diagonal/sparse estimation bounds: Section 5.1.3: combined diagonal/sparse estimation bounds (source-ambiguity)
  • Section 5.1.3: composition by square-root Choi block encodings: Section 5.1.3: composition by square-root Choi block encodings (source-ambiguity)
  • Section 5.2: partially transposed permutational quantum computing: Section 5.2: partially transposed permutational quantum computing (source-ambiguity)

Selected references

  • The mixed Schur transform: efficient quantum circuit and applications, arXiv:2310.01613v1, https://arxiv.org/abs/2310.01613v1
8 thms1 active userReviewed
Quantum Information·Captain: Goku

Multiple-Access Bosonic CommunicationsResearch Paper

Motivation

The maximum rates for reliably transmitting classical information over Bosonic multiple-access channels (MACs) are derived when the transmitters are restricted to coherent-state encodings. Inner and outer bounds for the ultimate capacity region of the Bosonic MAC are also presented. It is shown that the sum-rate upper bound is achievable with a coherent-state encoding and that the entire region is asymptotically achievable in the limit of large mean input photon numbers.

This mission is the statement-level formalization of Multiple-Access Bosonic Communications (arXiv:quant-ph/0506171v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

5 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Operational homodyne and heterodyne coherent-state MAC regions (§II.B, (5)–(8): single-mode homodyne/heterodyne capacity regions, 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

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

  • §II.B,(9)–(11): Normalized coherent-state Fock ensembles and collective-receiver product-code MAC capacity (hard)
  • §II.B,(12): Additive random-displacement Fock channel and operational product-code capacity (hard)
  • §II.C,(23)–(27): Collective-receiver wideband bosonic coding and Gaussian ensemble entropy (hard)
  • §III.A,(35)–(40),(50)–(58): Physical Gaussian displaced-state mixtures, raw second moments, and infinite-dimensional entropy (hard)
  • §III.A,(48)–(49): Individual Holevo maximization over physical displacement laws (hard)
  • §III.A,(57)–(58): Joint Holevo sum functional for independent physical displacement laws (hard)
  • §III.A,(31)–(34),(59): Operational HSH two-sender capacity with physical Gaussian seed (hard)
  • §III.B,(60)–(65): Fixed-seed Gaussian beam-splitter MAC and photon-budget accounting (hard)
  • §III.B,(66),Fig.5: Operational fixed-seed Gaussian region realizing the explicit strict extension (hard)
  • §IV,Theorem 1,(67)–(74): Anisotropic attenuator, thermal entropy conjecture, squeeze whitening, and ordinary classical capacity (hard)
  • §IV,(75)–(76): Physical displaced squeezed-seed coding and unconditional anisotropic-channel capacity lower bound (hard)
  • §IV,(77): Thermal attenuator capacity and conditional specialization (hard)
  • §IV,(78)–(79): Pure squeezed-environment attenuator capacity and equal-energy thermal comparison (hard)
  • §V,(80) and individual bounds: Ultimate independent-sender bosonic capacity allowing across-use entanglement (hard)
  • §V, coherent-state sum achievement: Physical coherent encoding attaining the ultimate MAC sum capacity (hard)
  • §V, Gaussian sum achievement: Pure one-port Gaussian seed output and above-threshold physical sum code (hard)
  • Appendix,(A.1): Photon-support-constrained operational quantum MAC regions and their closed limit (hard)
  • Abstract; §V,PDF pp.9–10: Unspecified whole-region high-energy convergence notion (source-ambiguity)

Selected references

  • Multiple-Access Bosonic Communications, arXiv:quant-ph/0506171v2, https://arxiv.org/abs/quant-ph/0506171v2
7 thms1 active userReviewed
Algorithmic Game TheoryControl TheoryOperations Research+2·Captain: mikedeng1

Dynkin Games with Incomplete and Asymmetric Information: With Linear Payoffs, a Threshold Stop and a Belief-Reflecting Randomised Stop Form a Saddle PointResearch Paper

Why this game matters

An optimal stopping game asks two players to choose when to stop a shared process. The first player receives one payoff if they stop first and another if the second player stops first. Such a game changes when one player knows a parameter that the other can only infer from observations. The informed player can reveal information through the timing of a stop, and can conceal it by randomising. De Angelis, Ekström and Glover study this interaction for a diffusion with one of two possible drifts. Their preprint gives a verification theorem for general payoffs and solves a linear geometric Brownian example explicitly. This mission targets the latter result, Theorem 6.10. The result is proved in the paper; the work here is to express its model, strategy classes, supporting results and conclusion in Lean.

The game and its information

The asset value starts at x>0x>0x>0 and evolves as a geometric Brownian motion Xt=xexp⁡((μθ−σ2/2)t+σWt)X_t=x\exp((\mu_\theta-\sigma^2/2)t+\sigma W_t)Xt​=xexp((μθ​−σ2/2)t+σWt​), where σ>0\sigma>0σ>0, μ0<0<μ1\mu_0<0<\mu_1μ0​<0<μ1​, and the hidden type θ∈{0,1}\theta\in\{0,1\}θ∈{0,1} selects the drift. Initially P(θ=1)=π∈(0,1)\mathbb P(\theta=1)=\pi\in(0,1)P(θ=1)=π∈(0,1); write ϕ=π/(1−π)\phi=\pi/(1-\pi)ϕ=π/(1−π) for the initial odds. Player 1 sees the history of XXX and chooses an almost surely finite stopping time τ\tauτ for its augmented observation filtration FX\mathcal F^XFX. Player 2 also knows θ\thetaθ and chooses an adapted, nondecreasing control Γ\GammaΓ for the augmented filtration FX,θ\mathcal F^{X,\theta}FX,θ. An independent uniform variable UUU turns this control into the randomised stopping time γ=inf⁡{t≥0:Γt>U}\gamma=\inf\{t\ge0:\Gamma_t>U\}γ=inf{t≥0:Γt​>U}. The initial value Γ0\Gamma_0Γ0​ may be positive, representing a jump at time zero.

If τ<γ\tau<\gammaτ<γ, Player 1 receives f(Xτ)f(X_\tau)f(Xτ​); if γ≤τ\gamma\le\tauγ≤τ, Player 1 receives g(Xγ)g(X_\gamma)g(Xγ​). Thus a finite tie pays ggg. The expected payoff is J(τ,Γ)J(\tau,\Gamma)J(τ,Γ). Player 1 maximises it and Player 2 minimises it. A saddle point (τ∗,Γ∗)(\tau^*,\Gamma^*)(τ∗,Γ∗) satisfies J(τ,Γ∗)≤J(τ∗,Γ∗)≤J(τ∗,Γ)J(\tau,\Gamma^*)\le J(\tau^*,\Gamma^*)\le J(\tau^*,\Gamma)J(τ,Γ∗)≤J(τ∗,Γ∗)≤J(τ∗,Γ) for every admissible pair (τ,Γ)(\tau,\Gamma)(τ,Γ). In the linear example f(y)=yf(y)=yf(y)=y and g(y)=(1+ε)yg(y)=(1+\varepsilon)yg(y)=(1+ε)y, where ε>0\varepsilon>0ε>0.

The uninformed player's posterior probability Πt=P(θ=1∣FtX)\Pi_t=\mathbb P(\theta=1\mid\mathcal F^X_t)Πt​=P(θ=1∣FtX​) is expressed through the posterior odds Φt=Πt/(1−Πt)\Phi_t=\Pi_t/(1-\Pi_t)Φt​=Πt​/(1−Πt​). The informed strategy is a pair (Γ0,Γ1)(\Gamma^0,\Gamma^1)(Γ0,Γ1), one control for each type. Conditional laws Pi=P(⋅∣θ=i)P^i=P(\cdot\mid\theta=i)Pi=P(⋅∣θ=i) define the interim payoffs J0,J1J^0,J^1J0,J1. The scaled ex-ante payoff is J^=(1+ϕ)J\widehat J=(1+\phi)JJ=(1+ϕ)J. These quantities permit both an ex-ante saddle-point statement and the agent-form equilibrium statement of Proposition 3.6.

Formalization targets

The supporting targets begin with the filtering and payoff identities of Section 3, the quasi-variational verification result of Theorem 5.1, and the reflected-likelihood and boundary-value facts of Section 6. They culminate in the explicit linear-game equilibrium. Two real numbers 0<A<B0<A<B0<A<B are determined by equations (90) and (93); piecewise power functions V1,VV_1,VV1​,V are defined by (89) and (91), extended by (94)–(97), and V0(ϕ)=V(ϕ)−ϕV1(ϕ)V_0(\phi)=V(\phi)-\phi V_1(\phi)V0​(ϕ)=V(ϕ)−ϕV1​(ϕ). The type-one control ΓB\Gamma^BΓB keeps the adjusted odds ΦB=Φ(1−ΓB)\Phi^B=\Phi(1-\Gamma^B)ΦB=Φ(1−ΓB) below BBB, while Player 1 stops at τA=inf⁡{t:ΦtB≤A}\tau_A=\inf\{t:\Phi^B_t\le A\}τA​=inf{t:ΦtB​≤A}.

The goal is Theorem 6.10: (τA,(0,ΓB))(\tau_A,(0,\Gamma^B))(τA​,(0,ΓB)) is a saddle point, and for every x,ϕ>0x,\phi>0x,ϕ>0,

J^x,ϕ(τA,(0,ΓB))=xV(ϕ),Jx,ϕ0(τA,0)=xV0(ϕ),Jx,ϕ1(τA,ΓB)=xV1(ϕ).\widehat J_{x,\phi}(\tau_A,(0,\Gamma^B))=xV(\phi),\qquad J^0_{x,\phi}(\tau_A,0)=xV_0(\phi),\qquad J^1_{x,\phi}(\tau_A,\Gamma^B)=xV_1(\phi).Jx,ϕ​(τA​,(0,ΓB))=xV(ϕ),Jx,ϕ0​(τA​,0)=xV0​(ϕ),Jx,ϕ1​(τA​,ΓB)=xV1​(ϕ).

The mission's milestone list follows the paper's stated results. It includes the payoff reductions, Theorem 5.1, reflection at BBB, the ODE bounds, the unique ratio A/BA/BA/B, and the verification of the explicit value functions.

What the result establishes

The theorem identifies actual strategies for both players, rather than only showing that the game's upper and lower values coincide. It specifies how the informed player's randomisation depends on the unobserved type and how the uninformed player responds to the adjusted odds. It also gives the ex-ante and both type-conditional payoffs. Without the saddle inequalities over the full strategy classes, the formulas would describe candidate strategies rather than an equilibrium.

A Lean development must capture the paper's information restrictions and time-zero behaviour before the analytical proof can be meaningful. Reusable components include a model-independent two-filtration randomised Dynkin frame, the augmented observation filtrations, randomised stopping times, nonnegative extended payoffs, conditional-law decomposition, and Stieltjes integration with an initial jump. The paper has a written proof; the statements here are open Lean goals, not machine-checked proofs.

Main difficulty

The verification theorem couples a partial differential inequality to a singular control and a stopping time. The adjusted odds can jump when the control jumps, so ordinary continuous-path differential conditions do not by themselves describe the admissible action. The support conditions and transversality limits in Theorem 5.1 are needed to connect the analytic candidate values to payoffs for strategies that can stop at any time. In the linear example, obtaining the power-function candidates is only one part of the target: their free boundaries must be valid, the reflected control must be admissible, and the saddle inequalities must hold against all admissible alternatives.

Formalization scope and conventions

The Lean model uses the explicit strong solution of the §6 GBM on a complete probability space carrying a Brownian motion and independent uniform devices U,ΘU,\ThetaU,Θ. It sets θπ=1{Θ<π}\theta^\pi=\mathbf1_{\{\Theta<\pi\}}θπ=1{Θ<π}​. Paths of the chosen Brownian modification are continuous. Player 1's filtration is generated by XXX plus null sets; Player 2's also contains θ\thetaθ; neither contains UUU. Stopping times live in [0,∞][0,\infty][0,∞], with Player 1 required to stop almost surely. Payoffs are nonnegative extended integrals and equal zero if both stopping times are infinite. The Stieltjes convention counts Γ0\Gamma_0Γ0​.

The posterior odds Φ\PhiΦ use the GBM closed form. The running-maximum formula defines ΓB\Gamma^BΓB and permits its initial jump. The tilted law used in Lemma 6.5 is represented by an equivalent likelihood-path law. Theorem 5.1 is stated for the GBM instance with general continuous 0≤f≤g0\le f\le g0≤f≤g and relative closures inside (0,∞)2(0,\infty)^2(0,∞)2. Its localisation integral retains the factor printed in the preprint. The explicit boundaries, controls and values in the goal are definitions, never free variables or hypotheses; the saddle inequalities quantify over the full player strategy classes.

There is a normalization slip in the paper's (23): it prints Φt=dP1/dP0\Phi_t=dP^1/dP^0Φt​=dP1/dP0 on FtX\mathcal F^X_tFtX​, although Φ0=ϕ\Phi_0=\phiΦ0​=ϕ and a Radon–Nikodym derivative at time zero equals one. Equations (20)–(21) give dP1/dP0=Φt/ϕdP^1/dP^0=\Phi_t/\phidP1/dP0=Φt​/ϕ. The formal filtering item uses that corrected identity. Equation (50) similarly identifies the ex-ante value with the scaled payoff; the formal target records J^=(1+ϕ)J\widehat J=(1+\phi)JJ=(1+ϕ)J and states the payoff identities without confusing the two. The source's domain R+2\mathbb R_+^2R+2​ in Theorem 6.10 is read as x,ϕ>0x,\phi>0x,ϕ>0, as required by the model. These readings are documented in the local moderation notes.

Selected references

  • T. De Angelis, E. Ekström and K. Glover, Dynkin Games with Incomplete and Asymmetric Information, arXiv preprint 1810.07674v5, 2020. Preprint.
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Algorithmic Game TheoryMechanism DesignOperations Research·Captain: mikedeng1

Procurement Mechanisms with Post-Auction Pre-Award Cost-Reduction Investigations: Symmetric Suppliers Earn Weakly Higher Ex Ante Profits When Investigations Precede the AwardResearch Paper

Motivation

Large manufacturers procure components by competitive bidding, and many of them also run cost-reduction investigations: the buyer's engineers visit a supplier's plant and look for process changes that lower the cost of the contracted part. The savings are passed to the buyer as a lower contract price. In practice such investigations usually happen after the contract is awarded, on the winner only. Chen, Beil and Duenyas (Operations Research 70(6), 2022) compare that convention with a mechanism in which the buyer investigates before the award, possibly several suppliers, and then awards the contract on the investigated prices.

Investigating before the award obviously helps the buyer for fixed bids: she sees more cost reductions before choosing. The question is whether suppliers lose. The buyer keeps every identified saving, and investigations of competitors make their prices more aggressive, so suppliers seem to have reason to resist. The paper shows that, when suppliers are ex ante symmetric, they do not: every supplier's ex ante expected profit is at least as high when investigations come before the award. This mission formalizes that result.

Setting

A buyer procures one contract from suppliers N={1,…,N}\mathcal N=\{1,\dots,N\}N={1,…,N} and must transact with one of them. Supplier iii has a private cost ci=Δic+ϵicc_i=\Delta^c_i+\epsilon^c_ici​=Δic​+ϵic​, where Δic≥0\Delta^c_i\ge0Δic​≥0 is public and ϵic\epsilon^c_iϵic​ has density fff on [c‾,cˉ][\underline c,\bar c][c​,cˉ] with mean 000; so cic_ici​ has density fi(c)=f(c−Δic)f_i(c)=f(c-\Delta^c_i)fi​(c)=f(c−Δic​), c.d.f. FiF_iFi​, and support Ci=[c‾i,cˉi]C_i=[\underline c_i,\bar c_i]Ci​=[c​i​,cˉi​]. Costs are independent.

An investigation of supplier iii costs the buyer d≥0d\ge0d≥0 and reveals a cost reduction ti=Δit+ϵit≥0t_i=\Delta^t_i+\epsilon^t_i\ge0ti​=Δit​+ϵit​≥0, where ϵit\epsilon^t_iϵit​ has density ggg on [t‾,tˉ][\underline t,\bar t][t​,tˉ] with mean 000, independently of everything else. At most N^∈{1,…,N}\hat N\in\{1,\dots,N\}N^∈{1,…,N} suppliers can be investigated, and costs always exceed reductions: Δit+tˉ<Δic+c‾\Delta^t_i+\bar t<\Delta^c_i+\underline cΔit​+tˉ<Δic​+c​. Each supplier submits a sealed bid bi∈Bi=[0,cˉi]b_i\in B_i=[0,\bar c_i]bi​∈Bi​=[0,cˉi​]. If an investigated supplier wins, he is paid his updated bid bi−tib_i-t_ibi​−ti​ and his cost becomes ci−tic_i-t_ici​−ti​, so his margin is bi−cib_i-c_ibi​−ci​ in every case.

  • BAI (bid, award, investigate). The buyer awards the contract to the lowest λi=bi−ri\lambda_i=b_i-r_iλi​=bi​−ri​, where ri=max⁡{0,Δit−d}r_i=\max\{0,\Delta^t_i-d\}ri​=max{0,Δit​−d} is the expected saving from investigating the winner afterwards. Ties are broken at random.
  • BIA (bid, investigate, award). The buyer investigates sequentially. Each round she uses the bids and the reductions revealed so far to stop or to investigate one more supplier, and stopping is final. She then awards the contract to the lowest updated bid. Her policy minimizes the expected payment plus investigation cost, problem (1). Theorem 1 solves (1) by an index policy: with τ\tauτ the root of d=∫τ∞(ϵt−τ) dG(ϵt)d=\int_\tau^\infty(\epsilon^t-\tau)\,dG(\epsilon^t)d=∫τ∞​(ϵt−τ)dG(ϵt), each supplier gets the index μi(bi)=bi−max⁡{0,τ+Δit}\mu_i(b_i)=b_i-\max\{0,\tau+\Delta^t_i\}μi​(bi​)=bi​−max{0,τ+Δit​}. The buyer investigates in increasing order of index while the current lowest updated bid is at least the next index, up to a cap Nˉ≤N^\bar N\le\hat NNˉ≤N^.

Supplier iii's winning probability at bids bbb is Wi(b)W_i(b)Wi​(b), over ttt and the tie-break. With the others bidding β−i(c−i)\beta_{-i}(c_{-i})β−i​(c−i​), his expected profit from bidding bbb at cost ccc is ui(b;c)=(b−c) Ec−i[Wi(b,β−i(c−i))]u_i(b;c)=(b-c)\,\mathbf E_{c_{-i}}[W_i(b,\beta_{-i}(c_{-i}))]ui​(b;c)=(b−c)Ec−i​​[Wi​(b,β−i​(c−i​))], equation (5). A Bayesian Nash equilibrium is a profile of strategies βi:Ci→Bi\beta_i:C_i\to B_iβi​:Ci​→Bi​ that are best replies at every type. Supplier iii's ex ante expected profit is Eci[ui(βi(ci);ci)]\mathbf E_{c_i}[u_i(\beta_i(c_i);c_i)]Eci​​[ui​(βi​(ci​);ci​)].

Formalization targets

Goal: Theorem 2 (weak form)

Suppose that suppliers are ex ante symmetric (Δic=Δc\Delta^c_i=\Delta^cΔic​=Δc, Δit=Δt\Delta^t_i=\Delta^tΔit​=Δt), that Fi/fiF_i/f_iFi​/fi​ is nondecreasing (Assumption 1), and that d<max⁡iΔitd<\max_i\Delta^t_id<maxi​Δit​ (Assumption 2). Let βBIA\beta^{\mathrm{BIA}}βBIA be a symmetric equilibrium of BIA, and βBAI\beta^{\mathrm{BAI}}βBAI a symmetric nondecreasing equilibrium of BAI. Then for every supplier iii,

Eci[uiBAI(βiBAI(ci);ci)]  ≤  Eci[uiBIA(βiBIA(ci);ci)].\mathbf E_{c_i}\big[u^{\mathrm{BAI}}_i(\beta^{\mathrm{BAI}}_i(c_i);c_i)\big]\;\le\;\mathbf E_{c_i}\big[u^{\mathrm{BIA}}_i(\beta^{\mathrm{BIA}}_i(c_i);c_i)\big].Eci​​[uiBAI​(βiBAI​(ci​);ci​)]≤Eci​​[uiBIA​(βiBIA​(ci​);ci​)].

Milestones

  1. Proposition 1. There exists an equilibrium βˇ\check\betaβˇ​ of the first-price auction with costs ci−ric_i-r_ici​−ri​ whose shifted strategy β~i(ci)=βˇi(ci−ri)+ri\tilde\beta_i(c_i)=\check\beta_i(c_i-r_i)+r_iβ~​i​(ci​)=βˇ​i​(ci​−ri​)+ri​ is a BAI equilibrium.
  2. Theorem 1(a). The index policy (3) minimizes the buyer's expected cost (1) over all admissible sequential policies, for every bid vector.
  3. Zero profit at the top. UiM(cˉi)=0U^{\mathcal M}_i(\bar c_i)=0UiM​(cˉi​)=0 for M∈{BIA,BAI}\mathcal M\in\{\mathrm{BIA},\mathrm{BAI}\}M∈{BIA,BAI}.
  4. Envelope formula (A.2). UiM(ci)=UiM(cˉi)+∫cicˉiϕiM(y) dyU^{\mathcal M}_i(c_i)=U^{\mathcal M}_i(\bar c_i)+\int_{c_i}^{\bar c_i}\phi^{\mathcal M}_i(y)\,dyUiM​(ci​)=UiM​(cˉi​)+∫ci​cˉi​​ϕiM​(y)dy.
  5. Ex ante identity. Eci[UiM(ci)]=UiM(cˉi)+Ec[AiM(c) Fi(ci)/fi(ci)]\mathbf E_{c_i}[U^{\mathcal M}_i(c_i)]=U^{\mathcal M}_i(\bar c_i)+\mathbf E_{c}\big[A^{\mathcal M}_i(c)\,F_i(c_i)/f_i(c_i)\big]Eci​​[UiM​(ci​)]=UiM​(cˉi​)+Ec​[AiM​(c)Fi​(ci​)/fi​(ci​)].
  6. Pointwise comparison. At cost vector ccc and realized reduction vector ttt, ∑iAiBAI(c)F1(ci)/f1(ci)=min⁡iF1(ci)/f1(ci)≤∑iAiBIA(c,t)F1(ci)/f1(ci)\sum_i A^{\mathrm{BAI}}_i(c) F_1(c_i)/f_1(c_i)=\min_i F_1(c_i)/f_1(c_i)\le\sum_i A^{\mathrm{BIA}}_i(c,t) F_1(c_i)/f_1(c_i)∑i​AiBAI​(c)F1​(ci​)/f1​(ci​)=mini​F1​(ci​)/f1​(ci​)≤∑i​AiBIA​(c,t)F1​(ci​)/f1​(ci​) almost everywhere, with ∑iAiM=1\sum_iA^{\mathcal M}_i=1∑i​AiM​=1.

Significance

The theorem identifies a win-win procurement design. With symmetric suppliers, a buyer who chooses the cheaper of BAI and BIA weakly lowers her own cost, and this choice never lowers any supplier's ex ante profit. The gain does not come from sharing savings, since the buyer keeps all identified savings. It comes from strategic bidding: under BIA a supplier need not submit the lowest initial bid to win, so price competition at the bid stage softens. The paper's Figure 1 shows the higher BIA bid curves. Theorem 1 is of independent interest: it is an index solution of a capped sequential search problem in which an uninvestigated bid may still win.

The paper proves the result on paper. To our knowledge none of it is machine-checked. A formalization adds three things. It makes the mechanisms precise, including the tie-breaking and the stopping rule that the text leaves partly implicit. It pins down the right inequality: the printed "higher" is not strict, and with a single supplier both mechanisms give the same profit. It also produces reusable components: an envelope-theorem layer for bidding games with an indirect mechanism, and a capped-search index theorem.

Difficulty

The proof of Theorem 2 needs the BIA winning probability only through its total, ∑iAiBIA=1\sum_i A^{\mathrm{BIA}}_i=1∑i​AiBIA​=1. Everything else rests on three technical steps. The first is the envelope formula (A.2) for an indirect mechanism whose allocation WiW_iWi​ has no closed form and need not be continuous in the bid. The usual argument assumes a differentiable direct mechanism and does not apply as stated. The second is the claim that in BAI the lowest-cost supplier wins almost surely. That needs a symmetric equilibrium that is not merely nondecreasing but free of pooling, and this must be derived from the equilibrium conditions. The third is the "by symmetry" step that equates each supplier's ex ante profit with the average over suppliers. It needs both the equilibria and the mechanisms to be invariant under relabelling the suppliers.

Theorem 1(a) is a dynamic program over adaptive policies with a cap and an outside option. A Weitzman-style argument must handle a cap Nˉ\bar NNˉ and suppliers whose index makes investigation worthless (τi=0\tau_i=0τi​=0). It cannot simply be imported from Pandora's-box results.

Formalization scope

Suppliers are Fin N with N≥1N\ge1N≥1; all values are real numbers. A single definitions module PreAwardInvest.WinWin.Model contains the following.

  • Parameters and assumptions. The parameters, and the standing assumptions of §3.1 (densities with mean zero, nonnegative costs and reductions, footnote 6, 1≤N^≤N1\le\hat N\le N1≤N^≤N, d≥0d\ge0d≥0), with f>0f>0f>0 on (c‾,cˉ)(\underline c,\bar c)(c​,cˉ) added. Assumptions 1 and 2 are separate predicates.
  • Laws. The cost and reduction laws are densities with respect to Lebesgue measure, and their vectors have product laws.
  • Policies. A policy reads the bids, the investigated set and the revealed reductions. An admissible policy is nonanticipative and measurable in the reductions, and stopping is final.
  • Index policy. It takes τ\tauτ as any root of its equation. Ties in the ranking and in both awards are broken by one uniformly random priority order, so that BIA and BAI are symmetric under relabelling. Theorem 1(a) compares policies for bids in Bi=[0,cˉi]B_i=[0,\bar c_i]Bi​=[0,cˉi​].
  • Profits and equilibria. Profits follow (5), with the expectation over c−ic_{-i}c−i​ taken over the whole cost vector with coordinate iii overwritten. Equilibria require measurable strategies into Bi=[0,cˉi]B_i=[0,\bar c_i]Bi​=[0,cˉi​]. Ex ante profit is the expectation of the equilibrium profit, not the Myerson virtual-cost expression.

Several conventions are disclosed hypotheses or corrections. The goal uses ≤\le≤ in place of the printed "higher". The equilibria in the goal are assumed symmetric, and the BAI one nondecreasing (Lemma 1's class). Strict monotonicity is not assumed, because with one supplier the equilibrium bid is the constant cˉ1\bar c_1cˉ1​.

The goal is not trivialized. BAI awards on bids through λi=bi−ri\lambda_i=b_i-r_iλi​=bi​−ri​ and BIA runs the index policy on bids and revealed reductions. Neither mechanism has "lowest cost wins" built in, which is milestone 6. Ex ante profit is defined from (5), so milestones 4–5 are not definitional. A sorry-free check exhibits a one-supplier instance that satisfies every hypothesis of the goal. In it both ex ante profits equal 1/21/21/2.

Not formalized: Theorem 1(b)–(c), Lemma 1 (existence via Athey 2001), the closed form (4) of WiW_iWi​, the asymmetric results (Propositions 2–4), the buyer-cost comparison (Theorem 3), the optimal mechanism (Theorem 4), and the extensions of §9. Contributions welcome: the envelope theorem for monotone-selection bidding games, measurability of the winning probabilities, and the index policy's optimality.

Selected references

  • Q. Chen, D. R. Beil, I. Duenyas, Procurement mechanisms with post-auction pre-award cost-reduction investigations, Operations Research 70(6):3054–3075, 2022. https://doi.org/10.1287/opre.2022.2349 (accepted manuscript: LBS Research Online eprint 2544).
  • S. Athey, Single crossing properties and the existence of pure strategy equilibria in games of incomplete information, Econometrica 69(4):861–889, 2001. https://doi.org/10.1111/1468-0262.00223
  • R. B. Myerson, Optimal auction design, Mathematics of Operations Research 6(1):58–73, 1981. https://doi.org/10.1287/moor.6.1.58
  • P. Milgrom, I. Segal, Envelope theorems for arbitrary choice sets, Econometrica 70(2):583–601, 2002. https://doi.org/10.1111/1468-0262.00296
  • M. L. Weitzman, Optimal search for the best alternative, Econometrica 47(3):641–654, 1979. https://doi.org/10.2307/1910412
  • V. Krishna, Auction Theory, 2nd ed., Academic Press, 2009. https://doi.org/10.1016/C2009-0-22474-3
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Quantum Information·Captain: Goku

Everything You Always Wanted to Know About LOCC (But Were Afraid to Ask)Research Paper

Motivation

In this paper we study the subset of generalized quantum measurements on finite dimensional systems known as local operations and classical communication (LOCC). While LOCC emerges as the natural class of operations in many important quantum information tasks, its mathematical structure is complex and difficult to characterize. Here we provide a precise description of LOCC and related operational classes in terms of quantum instruments. Our formalism captures both finite round protocols as well as those that utilize an unbounded number of communication rounds. While the set of LOCC is not topologically closed, we show that finite round LOCC constitutes a compact subset of quantum operations. Additionally we show the existence of an open ball around the completely depolarizing map that consists entirely of LOCC implementable maps. Finally, we demonstrate a two-qubit map whose action can be approached arbitrarily close using LOCC, but nevertheless cannot be implemented perfectly.

This mission is the statement-level formalization of Everything You Always Wanted to Know About LOCC (But Were Afraid to Ask) (arXiv:1210.4583v2). 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 An explicit two-qubit instrument in the closure of LOCC but outside LOCC (Abstract; §§4.1,4.3, Eqs.(10)–(12), 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:

  • Lemma 2, Eq.(20); Appendix B pp.19–21: A source-correct strict-decrease domain, or a definition of nontrivial measurement depending on the input state. (source-ambiguity)

Selected references

  • Everything You Always Wanted to Know About LOCC (But Were Afraid to Ask), arXiv:1210.4583v2, https://arxiv.org/abs/1210.4583v2
18 thms1 active userReviewed
Quantum Information·Captain: Goku

Lie-Semigroup Structures for Reachability and Control of Open Quantum SystemsResearch Paper

Motivation

In view of controlling finite dimensional open quantum systems, we provide a unified Lie-semigroup framework describing the structure of completely positive trace-preserving maps. It allows (i) to identify the Kossakowski-Lindblad generators as the Lie wedge of a subsemigroup, (ii) to link properties of Lie semigroups such as divisibility with Markov properties of quantum channels, and (iii) to characterise reachable sets and controllability in open systems. We elucidate when time-optimal controls derived for the analogous closed system already give good fidelities in open systems and when a more detailed knowledge of the open system (e.g., in terms of the parameters of its Kossakowski-Lindblad master equation) is actually required for state-of-the-art optimal-control algorithms. -- As an outlook, we sketch the structure of a new, potentially more efficient numerical approach explicitly making use of the corresponding Lie wedge.

This mission is the statement-level formalization of Lie-Semigroup Structures for Reachability and Control of Open Quantum Systems (arXiv:0811.3906v4). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

5 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is The generated Markovian semigroup has the full channel tangent wedge (Theorem III.3, 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

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

  • Lemma II.1: Accepted source-matched theorem for Lemma II.1 (provenance boundary) (hard)
  • Theorem II.1: Missing Ad_K invariance of c (source-ambiguity)
  • Proposition II.1: Accepted source-matched theorem for Proposition II.1 (provenance boundary) (hard)
  • Proposition II.2: Accepted source-matched theorem for Proposition II.2 (provenance boundary) (hard)
  • Theorem II.2: Accepted source-matched theorem for Theorem II.2 (provenance boundary) (hard)
  • Theorem II.3: Accepted source-matched theorem for Theorem II.3 (provenance boundary) (hard)
  • Theorem II.4: Accepted source-matched theorem for Theorem II.4 (provenance boundary) (hard)
  • Theorem II.5: Accepted source-matched theorem for Theorem II.5 (provenance boundary) (hard)
  • Theorem II.6: Accepted source-matched theorem for Theorem II.6 (provenance boundary) (hard)
  • Corollary II.1: Accepted source-matched theorem for Corollary II.1 (provenance boundary) (hard)
  • Corollary II.2: Accepted source-matched theorem for Corollary II.2 (provenance boundary) (hard)
  • Theorem III.1: Independent x/y control indexing and original-result provenance (source-ambiguity)
  • Theorem III.2: Accepted source-matched theorem for Theorem III.2 (provenance boundary) (hard)
  • Proposition III.1: Accepted source-matched theorem for Proposition III.1 (provenance boundary) (hard)
  • Theorem III.4: Dimension-qualified nondivisibility theorem (source-ambiguity)
  • Corollary III.2: Dimension-qualified failure of Lie-subsemigroup generation (source-ambiguity)
  • Corollary III.3: Dimension-qualified local failures and non-semialgebra wedge (source-ambiguity)
  • Corollary III.4: Nonvacuous fixed-semigroup identity neighborhood and generator signs (source-ambiguity)
  • Corollary III.5: Endpoint representations versus one fixed exponential trajectory (source-ambiguity)
  • Resume: A specified genericity space and canonical dissipator gauge (source-ambiguity)
  • Proposition III.2: Nontrivial homogeneous space for the smallest-positive-scaling conclusion (source-ambiguity)
  • Corollary III.6: Canonical dissipator gauge and a definition of generic (source-ambiguity)
  • Reachability-product: Accepted source-matched theorem for Reachability-product (provenance boundary) (hard)
  • Remark II.1: Accepted source-matched theorem for Remark II.1 (provenance boundary) (hard)
  • Remark II.3: Accepted source-matched theorem for Remark II.3 (provenance boundary) (hard)
  • Trace-norm-contraction: Accepted source-matched theorem for Trace-norm-contraction (provenance boundary) (hard)
  • Purity-unitality: Accepted source-matched theorem for Purity-unitality (provenance boundary) (hard)
  • Remark III.1: Accepted source-matched theorem for Remark III.1 (provenance boundary) (hard)
  • Markovian-stratification: Dimension scope and explicit interior/strict-inclusion witnesses (source-ambiguity)
  • Scalar-decay-optimal-time: Quantitative almost-uniform decay and attained argmax domain (source-ambiguity)

Selected references

  • Lie-Semigroup Structures for Reachability and Control of Open Quantum Systems, arXiv:0811.3906v4, https://arxiv.org/abs/0811.3906v4
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Quantum Information·Captain: Goku

Classical Capacity of Single-Mode Bosonic Gaussian ChannelsResearch Paper

Motivation

The classical capacity of a noisy optical channel is the maximum rate at which information can be transmitted reliably, given a constraint on the mean input energy. For the ubiquitous bosonic Gaussian channels, which include standard models of loss and noise in fibre and free-space optical links, determining this rate requires addressing whether entanglement between channel uses or non-Gaussian signals can outperform Gaussian encodings. More precisely, the question is whether the energy-constrained Holevo information is additive across arbitrarily many channel uses and coincides with its Gaussian counterpart. We answer these fundamental questions in the affirmative for every single-mode bosonic Gaussian channel at every input energy. Namely, we prove that independently prepared Gaussian states with Gaussian-distributed random displacements achieve the capacity, including in the low-energy regime where squeezing the signals competes with encoding information in their displacement. Our proof connects an entanglement inequality to a sharp, additive lower bound on output entropy. We then characterise communication above capacity: under a strict total photon-number cutoff, the probability of correct decoding decreases exponentially with the number of channel uses, and we derive explicit bounds on the decay exponent. When only the mean photon number is constrained, a simple energy-rescaling formula determines exactly the entire asymptotic rate--error trade-off: the capacity at mean photon number NNN and allowed average decoding error εεε equals the vanishing-error capacity at mean photon number N/(1−ε)N/(1-ε)N/(1−ε). Together, these results identify the ultimate limits of classical communication for some of the most fundamental models of optical communication. △ Less

This mission is the statement-level formalization of Classical Capacity of Single-Mode Bosonic Gaussian Channels (arXiv:2610.22308v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

2 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Affine envelope and joint convexity of the moment-resolved entropy (Eq. (18), 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

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

  • Corollary 3 (pp.5,12), resolving the p.1 paper-result seed: capacities and water-filling: bosonic channels, arbitrary probability ensembles, Gaussian displacement ensembles, and operational classical capacity (hard)
  • Theorem 1: output entropy from second moments: finite-energy Fock states, raw quadrature quadratic-form moments, von Neumann entropy, and squeezed vacua (hard)
  • Theorem 2: moment-resolved Gaussian optimality: continuous bosonic ensembles and product Gaussian displacement ensembles (hard)
  • Corollary 4: finite correlated blocks: passive Fock-space implementation of a common noise diagonalizer and repeated-block capacity (hard)
  • Unnumbered §IV: positive mode costs and marginal-gain rule: weighted-energy bosonic ensemble capacity and actual Gaussian Holevo energy functions (hard)
  • Unnumbered Eq.(22) and Appendix E.1: operational limit of chain memory channels: growing chain Gaussian channels and operational coding capacity along a nonidentical sequence (hard)
  • Proposition 5: tight Gaussian reference: infinite-dimensional relative entropy and a constructed optimal Gaussian reference (hard)
  • Unnumbered Eq.(24), Appendix F: uniqueness and quantitative stability: bosonic ensemble Holevo deficit, trace norm, marginals and Gaussian reference tensor powers (hard)
  • Theorem 6: exact nonzero-error capacity: operational nonzero-error capacity for bosonic mean-energy code sequences (hard)
  • Proposition 7: exponential cutoff strong converse: bosonic photon-cutoff codes and their operational capacity (hard)
  • Proposition 8: mixed-state affine entropy bound: mixed bosonic bipartite states and unbounded annihilation-operator quadratic forms (hard)
  • Lemma 9: quadrature-dependent dilation expectation: symplectic Fock unitaries, their Stinespring action, and quadrature-dependent quadratic-form expectations (hard)
  • Proposition 10: growing-memory converse and error trade-off: uniform Gaussian dilations and operational codes along growing memory blocks (hard)
  • Fact 11: Gaussification commutes with Gaussian channels: Gaussification as an actual normalized Gaussian Fock state with prescribed moments (hard)
  • Proposition 12: transfer from cutoff to mean energy: arbitrary bosonic-input channels, bounded decoding POVMs, and cutoff-code success supremum (hard)
  • Lemma 13: energy-preserving positive-filter coding inequality: Stinespring image filters and projective operator tensor norm on infinite Fock factors (hard)
  • Lemma 14: uniform exponential moments for symplectic unitaries: symplectic unitary tensor powers and extended nonnegative photon-exponential expectations (hard)
  • Proposition 15: approximating energy image filters: positive finite-rank energy-image filters and finite-local-support approximants on Fock tensor factors (hard)
  • Proposition 16: computable filter exponent: actual cutoff-code success exponent, Gaussian dilation constants and true capacity function (hard)
  • Proposition 17: explicit photon-tail bound: canonical Gaussian channel outputs on arbitrary cutoff states and decoding success (hard)
  • Lemma 18: output photon-number moments: extended output photon-number moments for arbitrary entangled cutoff Fock states (hard)
  • Proposition 19: converse for optimal Gaussian signal family: actual displaced squeezed Gaussian codewords and infinite-dimensional Petz Renyi expressions (hard)
  • Unnumbered Appendix B: energy-preserving canonical reduction: Fock implementations of input phase rotations and output symplectic transformations (hard)
  • Unnumbered G8: photon-subspace dimension and channel-independent bound: photon-subspace Hilbert dimension and channel-independent cutoff decoding success (hard)
  • Unnumbered H44: approach of the filter exponent to capacity: dilation-dependent H43 filter exponent using true operational Gaussian capacity (hard)
  • Unnumbered H45: weak photon tails: averaged photon-tail weight, actual cutoff-code supremum and vacuum-mixture code sequence (hard)
  • Unnumbered H46–H47: fixed multimode Gaussian channels: fixed finite-mode Gaussian channels and regularized operational bosonic capacity (hard)

Selected references

  • Classical Capacity of Single-Mode Bosonic Gaussian Channels, arXiv:2610.22308v1, https://arxiv.org/abs/2610.22308v1
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Quantum Information·Captain: Goku

Entanglement-breaking channels in infinite dimensionsResearch Paper

Motivation

We give a representation for entanglement-breaking channels in separable Hilbert space that generalizes the "Kraus decomposition with rank one operators" and use it to describe the complementary channels. We also give necessary and sufficient condition of entanglement-breaking for a general quantum Gaussian channel. Application of this condition to one-mode channels provides several new cases where the additivity conjecture holds in full generality.

This mission is the statement-level formalization of Entanglement-breaking channels in infinite dimensions (arXiv:0802.0235v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

4 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Radon–Nikodym representation of a POVM (Lemma 1: Radon–Nikodym representation of a POVM (9)–(10), 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

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

  • Theorem 2: Gaussian entanglement-breaking criterion and representation (30)–(31): Normal Gaussian trace-class channels, Gaussian states and trace-norm measure-and-prepare integral (hard)
  • Theorem 1: continuous densely defined rank-one representation (17)–(18): Measurable trace-class preparation from densely defined algebraic functionals (hard)
  • Proposition 1: sign of coherent information for (anti-)degradable channels: Genuine complementary trace-class channels and finite-entropy coherent information (hard)
  • Unnumbered: explicit Stinespring isometry and complementary kernel: Vector-valued L2 Stinespring realization and scalar integral-operator kernel (hard)
  • Example: spectral L2 measure-and-prepare channel and complementary Schur kernel: Canonical trace-class L2 diagonal and spectral measure-and-prepare map (hard)
  • Unnumbered: every entanglement-breaking channel is anti-degradable: Explicit entanglement-breaking antidegrading map on the full L2 environment trace class (hard)
  • Unnumbered: sharp Gaussian observable iff noise vanishes: Joint spectral measure of unbounded commuting quadratures with symplectic outcome transport (hard)
  • Proposition 2: covariant operator density of a nonsingular Gaussian observable: Gaussian trace-class seed state and displaced covariant operator density (hard)
  • Proposition 3: explicit Gaussian Naimark dilation (24)–(26): Gaussian ancillary Weyl system, normal partial-state evaluation and sharp joint spectral dilation (hard)
  • Unnumbered: complete positivity condition for Gaussian channel parameters (29): Normal trace-class realization of the Weyl channel characteristic law (hard)
  • Unnumbered: necessary PPT inequalities and Gaussian output PPT property (35): Partial transpose and Gaussian state law on a completed reference tensor product (hard)
  • Unnumbered: isotropic K gives a sharp-measurement c-q channel: Sharp quadrature PVM and displaced Gaussian preparation channel (hard)
  • Unnumbered claim: arbitrary sharp peaking around every outcome point: Correct outcome range in the arbitrary sharp-peaking claim (source-ambiguity)
  • Unnumbered: complete one-mode entanglement-breaking thresholds A, B1, B2, C, D: Actual canonical Gaussian channels and Gaussian unitary equivalence (hard)
  • Unnumbered: constrained chi-capacity additivity for the classified one-mode regimes: Extended constrained Holevo capacity for generalized ensembles and channel tensor products (hard)
  • Unnumbered: entanglement-breaking channels have zero quantum capacity: Operational unconstrained quantum capacity on separable trace-class channels (hard)
  • Unnumbered: energy-constrained tensor-power additivity and single-letter classical capacity (8): Formal spectral-energy constraints, tensor-power classical codes and extended constrained Holevo capacity on full trace-class channels (hard)
  • Unnumbered conditional discussion: Gaussian-optimizer capacity formula: Scope of the Gaussian optimizer conjecture used for operational capacity (source-ambiguity)

Selected references

  • Entanglement-breaking channels in infinite dimensions, arXiv:0802.0235v1, https://arxiv.org/abs/0802.0235v1
6 thms1 active userReviewed
Quantum Information·Captain: Goku

Mutual and coherent informations for infinite-dimensional quantum channelsResearch Paper

Motivation

The work is devoted to study of quantum mutual information and coherent information -- the two important characteristics of quantum communication channel. Appropriate definitions of these quantities in the infinite-dimensional case are given and their properties are studied in detail. Basic identities relating quantum mutual information and coherent information of a pair of complementary channels are proved. An unexpected continuity property of quantum mutual information and coherent information following from the above identities is observed. An upper bound for the coherent information is obtained.

This mission is the statement-level formalization of Mutual and coherent informations for infinite-dimensional quantum channels (arXiv:1004.2495v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

24 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 1: complementary-channel mutual-information identity (22) (Theorem 1: complementary-channel mutual-information identity (22), PDF p. 13). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Selected references

  • Mutual and coherent informations for infinite-dimensional quantum channels, arXiv:1004.2495v2, https://arxiv.org/abs/1004.2495v2
27 thms1 active userReviewed
Quantum Information·Captain: Goku

Squashed entanglement in infinite dimensionsResearch Paper

Motivation

We analyse two possible definitions of the squashed entanglement in an infinite-dimensional bipartite system: direct translation of the finite-dimensional definition and its universal extension. It is shown that the both definitions produce the same lower semicontinuous entanglement measure possessing all basis properties of the squashed entanglement on the set of states having at least one finite marginal entropy. Is also shown that the second definition gives an adequate extension of this measure to the set of all states of infinite-dimensional bipartite system. A general condition relating continuity of the squashed entanglement to continuity of the quantum mutual information is proved and its corollaries are considered. Continuity bound for the squashed entanglement under the energy constraint on one subsystem is obtained by using the tight continuity bound for conditional mutual information (proved in the Appendix by using Winter's technique). It is shown that the same continuity bound is valid for the entanglement of formation. As a result the asymptotic continuity of the both entanglement measures under the energy constraint on one subsystem is proved.

This mission is the statement-level formalization of Squashed entanglement in infinite dimensions (arXiv:1507.08964v5). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

2 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Compactness of bipartite states from both marginal sets (Lemma 1, 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

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

  • Lemma 3: contraction bound for MI and conditional entropy: Homogeneous extended spectral entropy and MI; finite-first-marginal conditional entropy; contraction conjugation (hard)
  • Proposition 1 A–C: universal extension of continuous monotones: Coherent finite-system monotone families, general quantum instruments, finite-rank compressions and EM1–EM8 (hard)
  • Corollary 1: universal entanglement of formation is the continuous convex roof: Continuous pure-state convex roof and universal finite-rank formation extension (hard)
  • Unnumbered consequence after Corollary 1: formation equality iff lower semicontinuity: Discrete and continuous formation roofs as actual extended-valued functions (hard)
  • Lemma 4 A–B: finite versus infinite extension systems: Extended MI, finite-projection CQMI, direct and finite-ancilla squashed infima (hard)
  • Unnumbered consequence of Lemma 4: criterion for finite-ancilla and direct functions to coincide: Globally defined direct and finite-ancilla squashed functions (hard)
  • Proposition 2 A–D: properties of direct infinite-dimensional squashed entanglement: Full direct squashed-entanglement function, EM2–EM8 and entropy-restricted trace-norm topology (hard)
  • Proposition 2A literal convex-hull scope (deferred source ambiguity): Literal Proposition 2A convex-hull scope (source-ambiguity)
  • Lemma 5: contraction and postselection bounds for CQMI: Homogeneous extended CQMI, contraction filtering, and positive-trace postselection (hard)
  • Abstract main result pinned to Proposition 3 A–D: universal squashed entanglement: Universal squashed extension and exact entanglement-measure predicates (hard)
  • Corollary 2: squashed entanglement is bounded by the corresponding formation roof: Both squashed functions and both formation roofs on full state spaces (hard)
  • Proposition 4 A–C: continuity equivalences and dominated convergence: Extended-valued MI and all squashed variants with sequential topology and uniform finite-ancilla gaps (hard)
  • Lemma 6 A–B: lower semicontinuity and continuity of bounded-ancilla functions (normalization correction): Bounded-ancilla squashed function and correctly normalized extended liminf gaps (hard)
  • Lemma 7: MI continuity implies upper semicontinuity of direct E_sq: Direct squashed-entanglement function and extended MI along arbitrary trace-norm sequences (hard)
  • Corollary 3: preservation of the continuity conditions by local operations: Trace-nonincreasing CP local operations and eventual normalized output sequences (hard)
  • Corollary 4: dominated local images of the limiting state: Local quantum operations, operator domination and squashed continuity (hard)
  • Corollary 5: one finite subsystem and explicit continuity modulus: All squashed variants with one arbitrary infinite subsystem (hard)
  • Corollary 6 A–C: energy-constrained equality and continuity: Extended one-marginal energy expectation, partition trace and both pairs of entanglement functions (hard)
  • Proposition 5: common energy-constrained continuity bound for E_sq and E_F: Actual Gibbs maximizer, form-energy state domain and both entanglement measures (hard)
  • Remark 4: uniform continuity of both energy-constrained entanglement measures: Real-valued entanglement restrictions to the full form-energy set with trace-norm uniformity (hard)
  • Corollary 7: asymptotic continuity under an A-only mean-energy bound: Correlated tensor-power density states, sum Hamiltonian form energy and normalized entanglement differences (hard)
  • Lemma 8 (Appendix): energy-constrained CQMI continuity bound: Arbitrary-state extended CQMI and one-marginal form-energy/Gibbs interfaces (hard)
  • Remark 5: uniform continuity of CQMI under an A-only energy bound: Trace-norm uniform structure and finite real CQMI on the A-only energy set (hard)
  • Remark 6: oscillator leading term and informal asymptotic tightness: Quantified full oscillator CQMI bound and asymptotic-tightness regime (source-ambiguity)
  • Remark 6: explicit mixed-state witnesses for the CQMI lower modulus: Actual mixed Gibbs states, pure-state purification and extended CQMI on flagged mixtures (hard)

Selected references

  • Squashed entanglement in infinite dimensions, arXiv:1507.08964v5, https://arxiv.org/abs/1507.08964v5
4 thms1 active userReviewed
Quantum Information·Captain: Goku

One-mode quantum Gaussian channelsResearch Paper

Motivation

A classification of one-mode Gaussian channels is given up to canonical unitary equivalence. A complementary to the quantum channel with additive classical Gaussian noise is described providing an example of one-mode Gaussian channel which is neither degradable nor anti-degradable.

This mission is the statement-level formalization of One-mode quantum Gaussian channels (arXiv:quant-ph/0607051v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

2 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Six canonical forms of one-mode Gaussian channels after displacement removal (§1, unnumbered Theorem, pp.2–4, 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

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

  • §2 A1, pp.4–5: thermal replacer and swap-dilation weak complement (hard)
  • §2 A2, (6)–(7): the actual A2 mixed-thermal dilation and its environment channel (hard)
  • §2 B1, Gaussian covariance and entropy calculation: actual diagonal Gaussian input densities, pure-dilation outputs and spectral entropy (hard)
  • §2 B1, degradability and infinite capacity: operational unconstrained quantum capacity and a genuine degrading normal channel (hard)
  • §2 C, attenuation/amplification models: mixed-thermal attenuation/amplification joint dilations and additive-noise composition (hard)
  • §2 D, phase conjugation model: the actual phase-conjugating dilation as an amplifier weak complement (hard)
  • §3, (8)–(9): trace-norm Gaussian displacement integration for every trace-class input (hard)
  • §3, (10)–(11): H-valued weighted-L2 unitary, both partial traces and the actual complementary kernel (hard)
  • §3, (12)–(14): self-adjoint environmental generators and CCR with legitimate domains (hard)
  • §3, (15)–(16) and six generator outputs: joint system/ancilla conjugation and domain-correct canonical dynamics (hard)
  • §3, (17), proof pp.9–10: the actual all-input additive-noise complementary channel (hard)
  • §3, complementary covariance and four eigenvalues: actual thermal complementary output covariance tied to its four spectral values (hard)
  • §3, (18)–(19): infinite-dimensional spectral entropy and exchange entropy of actual output densities (hard)
  • §3, F(N), vacuum value and limit: thermal coherent information linked to actual channel entropies (hard)
  • §3, Nc=0.99 exp(-1), also p.7: two operational positive capacities and normal-channel (anti)degradability (hard)

Selected references

  • One-mode quantum Gaussian channels, arXiv:quant-ph/0607051v2, https://arxiv.org/abs/quant-ph/0607051v2
4 thms1 active userReviewed
Quantum Information·Captain: Goku

Separability and Entanglement-Breaking in Infinite DimensionsResearch Paper

Motivation

In this paper we give a general integral representation for separable states in the tensor product of infinite dimensional Hilbert spaces and provide the first example of separable states that are not countably decomposable. We also prove the structure theorem for the quantum communication channels that are entanglement-breaking, generalizing the finite-dimensional result of M. Horodecki, Ruskai and Shor. In the finite dimensional case such channels can be characterized as having the Kraus representation with operators of rank 1. The above example implies existence of infinite-dimensional entanglement-breaking channels having no such representation.

This mission is the statement-level formalization of Separability and Entanglement-Breaking in Infinite Dimensions (arXiv:quant-ph/0504204v1). 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 Separable states are precisely probability mixtures of product states (§2, equation (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

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

  • Theorem 1: A valid compactness statement for the printed arbitrary set P (source-ambiguity)
  • Theorem 2: Normalized weakly countably additive POVM on an arbitrary complete separable metric outcome space and its trace-pairing probability laws (hard)
  • §3, paragraph after Theorem 2: Countable weak-effect and trace-norm rank-one Kraus sums, plus the constructed faithful-reference state (9) (hard)
  • §3, unnumbered existence result: A genuine infinite-dimensional channel witness and the exact countable rank-one Kraus predicate (hard)
  • §4, equations (12)–(14): The position spectral measure E(B), canonical L¹ diagonal density, and the fixed channel (12) (hard)
  • Conjecture: A proof of density of W in all separable states (source-ambiguity)
  • Theorem 4, equations (20)–(21): Infinite-dimensional extended Umegaki relative entropy, finite-ensemble Holevo capacity, and the channel (12) (hard)
  • Theorem 4 proof, equations (22)–(23): The exact range of the constructed rotation channel (12) on all states and all L¹ probability densities (hard)
  • Theorem 4 proof, finite-entropy conclusion: Extended von Neumann entropy on arbitrary trace-class states and its trace-norm restriction to the closed output range (hard)

Selected references

  • Separability and Entanglement-Breaking in Infinite Dimensions, arXiv:quant-ph/0504204v1, https://arxiv.org/abs/quant-ph/0504204v1
8 thms1 active userReviewed
Quantum Information·Captain: Goku

Trading classical communication, quantum communication, and entanglement in quantum Shannon theoryResearch Paper

Motivation

We give trade-offs between classical communication, quantum communication, and entanglement for processing information in the Shannon-theoretic setting. We first prove a unit-resource capacity theorem that applies to the scenario where only the above three noiseless resources are available for consumption or generation. The optimal strategy mixes the three fundamental protocols of teleportation, super-dense coding, and entanglement distribution. We then provide an achievable rate region and a matching multi-letter converse for the direct static capacity theorem. This theorem applies to the scenario where a large number of copies of a noisy bipartite state are available (in addition to consumption or generation of the above three noiseless resources). Our coding strategy involves a protocol that we name the classically-assisted state redistribution protocol and the three fundamental protocols. We finally provide an achievable rate region and a matching mutli-letter converse for the direct dynamic capacity theorem. This theorem applies to the scenario where a large number of uses of a noisy quantum channel are available in addition to the consumption or generation of the three noiseless resources. Our coding strategy combines the classically-enhanced father protocol with the three fundamental unit protocols.

This mission is the statement-level formalization of Trading classical communication, quantum communication, and entanglement in quantum Shannon theory (arXiv:0901.3038v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

1 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Finite-block converse with explicit continuity corrections and a common classical refinement (Appendix F, (106)–(107), and both proof chains on PDF p.25, PDF p. 24). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Theorem 1: unit resource capacity region: Operational simultaneous signed unit-resource conversion region (hard)
  • Theorem 2: direct static capacity theorem: Operational static conversion region and full regularized CASR union (hard)
  • Theorem 3: direct dynamic capacity theorem: Operational dynamic three-resource region and full regularized CEF union (hard)
  • Lemma 1: classically-assisted quantum state redistribution: Operational static primitive achievability for a remote instrument (hard)
  • Corollary 4: grandmother resource inequality: Operational entanglement-distillation rates with both communication costs (hard)
  • Lemma 3: additivity inclusion with a noiseless entangled state: Static operational helper families at all real ebit rates (hard)
  • Lemma 4: additivity inclusion with a noiseless quantum channel: Dynamic operational helper families at all real forward-qubit rates (hard)
  • Lemma 5: additivity inclusion with a noiseless entangled state: Static operational helper families in the noisy-teleportation quadrant (hard)
  • Lemma 6: additivity inclusion with a noiseless quantum channel: Dynamic operational helper families in the assisted entanglement quadrant (hard)
  • §VIII.A: erased-state optimal trade-off and single-letterization: A valid all-parameter erased-state optimal boundary (source-ambiguity)
  • §VIII.B: dephasing full dynamic single-letterization: Operational dephasing capacity and unrestricted one-copy CEF state union (hard)
  • §VII.C: benefit of coding with charged classical communication: Operational positive assisted capacity and the two closed wasting-allowed strategy regions (hard)
  • §VII.C: claimed constant excess ebit cost: The target-rate domain and optimization convention for a constant entanglement-cost difference (source-ambiguity)
  • Appendix A, (85)–(88): displayed finite-block static converse: A consistently scaled finite-block static converse with explicit error terms (source-ambiguity)

Selected references

  • Trading classical communication, quantum communication, and entanglement in quantum Shannon theory, arXiv:0901.3038v3, https://arxiv.org/abs/0901.3038v3
5 thms1 active userReviewed
Algorithmic Game TheoryControl TheoryProbability·Captain: mikedeng1

Terminal Ranking Games: The Rank-Based Mean Field Tournament Has an Equilibrium, Characterized by an Explicit Quantile Formula, a Fixed-Point Equation for the Mean and an Explicit Game ValueResearch Paper

Motivation

Tournaments and contests reward agents by their relative standing: sales bonuses for the top performers, promotions, prizes for the first to finish, research competitions. Since Lazear and Rosen (Rank-order tournaments as optimum labor contracts, 1981) such rank-order incentives have been a standard object in economics and operations research, and the design question of which reward schedule elicits which behaviour is central to the area. With a large population, the strategic interaction becomes a mean field game: each agent responds to the distribution of the others' outcomes rather than to individual opponents.

Bayraktar and Zhang (Terminal Ranking Games, arXiv:1906.09628v2, 2020; Mathematics of Operations Research 2021) study such a game in continuous time. Each player steers a Brownian project value by costly effort and is paid at a fixed terminal time according to her own value, her rank in the population, and the population mean. Their main result solves the equilibrium semi-explicitly. Related earlier work treats rank-based rewards by completion time (Bayraktar, Cvitanić and Zhang, Large tournament games, 2019) and by terminal rank in a strong formulation (Bayraktar and Zhang, A rank-based mean field game in the strong formulation, 2016).

Setting

Fix a horizon T>0T>0T>0, a cost coefficient c>0c>0c>0, a volatility σ>0\sigma>0σ>0 and an initial value x0∈Rx_0\in\mathbb Rx0​∈R. On a probability space (Ω,P)(\Omega,P)(Ω,P) let BBB be a real Brownian motion, and let XT=x0+σBTX_T=x_0+\sigma B_TXT​=x0​+σBT​ be the terminal project value under zero effort.

A reward function R(x,r,m)R(x,r,m)R(x,r,m) depends on the player's terminal value xxx, her rank r∈[0,1]r\in[0,1]r∈[0,1] and the population mean mmm; it is weakly increasing in each argument. The class Rb\mathcal R_bRb​ collects the bounded ones. For a population law μ\muμ on R\mathbb RR with c.d.f. FμF_\muFμ​ and mean mμm_\mumμ​, write Rμ(x)=R(x,Fμ(x),mμ)R_\mu(x)=R(x,F_\mu(x),m_\mu)Rμ​(x)=R(x,Fμ​(x),mμ​): the payment received at terminal value xxx when the others are distributed as μ\muμ.

Effort changes the law of the path. In the weak formulation used by the paper, a control is a probability measure QQQ equivalent to PPP, and the quadratic effort cost becomes the relative entropy H(Q∣P)H(Q|P)H(Q∣P). Given the population law μ~\tilde\muμ~​, the single player's value is

V(R,μ~)=sup⁡Q∼P EQ[Rμ~(XT)]−2cσ2H(Q ∣ P).(2.3)V(R,\tilde\mu)=\sup_{Q\sim P}\ E^Q\big[R_{\tilde\mu}(X_T)\big]-2c\sigma^2H(Q\,|\,P). \tag{2.3}V(R,μ~​)=Q∼Psup​ EQ[Rμ~​​(XT​)]−2cσ2H(Q∣P).(2.3)

A law μ\muμ is an equilibrium if it is a fixed point of the best response: some optimal QQQ for V(R,μ)V(R,\mu)V(R,μ) gives XTX_TXT​ the law μ\muμ.

The goal concerns the subclass Rbrm\mathcal R^{rm}_bRbrm​ of bounded rewards R(r,m)R(r,m)R(r,m) that do not depend on xxx and are continuous in mmm. Let NNN be the standard normal c.d.f., N−1N^{-1}N−1 its quantile function, qμ(r)=inf⁡{x:r≤Fμ(x)}q_\mu(r)=\inf\{x:r\le F_\mu(x)\}qμ​(r)=inf{x:r≤Fμ​(x)} the quantile function of μ\muμ, and

ym(r)=∫0re−R(z,m)/2cσ2dz∫01e−R(z,m)/2cσ2dz,g(m)=x0+σT∫01N−1(ym(r)) dr.y_m(r)=\frac{\int_0^r e^{-R(z,m)/2c\sigma^2}dz}{\int_0^1 e^{-R(z,m)/2c\sigma^2}dz},\qquad g(m)=x_0+\sigma\sqrt T\int_0^1N^{-1}(y_m(r))\,dr .ym​(r)=∫01​e−R(z,m)/2cσ2dz∫0r​e−R(z,m)/2cσ2dz​,g(m)=x0​+σT​∫01​N−1(ym​(r))dr.

Formalization targets

Goal: Theorem 3.2 (pp. 7–8)

For R∈RbrmR\in\mathcal R^{rm}_bR∈Rbrm​:

  1. an equilibrium exists;
  2. μ\muμ is an equilibrium if and only if it has a finite mean mμm_\mumμ​ and
qμ(r)=x0+σT N−1(ymμ(r))(0<r<1),mμ=g(mμ);(3.2–3.3)q_\mu(r)=x_0+\sigma\sqrt T\,N^{-1}\big(y_{m_\mu}(r)\big)\quad(0<r<1),\qquad m_\mu=g(m_\mu); \tag{3.2–3.3}qμ​(r)=x0​+σT​N−1(ymμ​​(r))(0<r<1),mμ​=g(mμ​);(3.2–3.3)
  1. for every equilibrium, V(R,μ)=2cσ2ln⁡β(μ)=−2cσ2ln⁡∫01e−R(z,mμ)/2cσ2dzV(R,\mu)=2c\sigma^2\ln\beta(\mu)=-2c\sigma^2\ln\int_0^1e^{-R(z,m_\mu)/2c\sigma^2}dzV(R,μ)=2cσ2lnβ(μ)=−2cσ2ln∫01​e−R(z,mμ​)/2cσ2dz, where β(μ)=∫f0(y)eRμ(y)/2cσ2dy\beta(\mu)=\int f_0(y)e^{R_\mu(y)/2c\sigma^2}dyβ(μ)=∫f0​(y)eRμ​(y)/2cσ2dy and f0f_0f0​ is the N(x0,σ2T)\mathcal N(x_0,\sigma^2T)N(x0​,σ2T) density.

No uniqueness is claimed.

Milestones

  • (2.6), p. 5: V(R,μ~)=sup⁡μ∼PT∫Rμ~ dμ−2cσ2H(μ∣N(x0,σ2T))V(R,\tilde\mu)=\sup_{\mu\sim P_T}\int R_{\tilde\mu}\,d\mu-2c\sigma^2H(\mu|\mathcal N(x_0,\sigma^2T))V(R,μ~​)=supμ∼PT​​∫Rμ~​​dμ−2cσ2H(μ∣N(x0​,σ2T)), for R∈RbR\in\mathcal R_bR∈Rb​.
  • Proposition 2.1, p. 5: the best response exists, its terminal law has density f0eRμ~/2cσ2/β(μ~)f_0e^{R_{\tilde\mu}/2c\sigma^2}/\beta(\tilde\mu)f0​eRμ~​​/2cσ2/β(μ~​), and V(R,μ~)=2cσ2ln⁡β(μ~)V(R,\tilde\mu)=2c\sigma^2\ln\beta(\tilde\mu)V(R,μ~​)=2cσ2lnβ(μ~​), for R∈RbR\in\mathcal R_bR∈Rb​.
  • Theorem 3.1, p. 7: μ\muμ is an equilibrium iff it has a strictly positive density fμ=f0eRμ/2cσ2/β(μ)f_\mu=f_0e^{R_\mu/2c\sigma^2}/\beta(\mu)fμ​=f0​eRμ​/2cσ2/β(μ), for R∈RbR\in\mathcal R_bR∈Rb​.
  • Proof of Theorem 3.2, p. 8: ∣(g(m)−x0)/σT∣≤C∫01∣N−1∣=C2/π|(g(m)-x_0)/\sigma\sqrt T|\le C\int_0^1|N^{-1}|=C\sqrt{2/\pi}∣(g(m)−x0​)/σT​∣≤C∫01​∣N−1∣=C2/π​ with C=exp⁡(∥R(1,⋅)−R(0,⋅)∥∞/2cσ2)C=\exp(\|R(1,\cdot)-R(0,\cdot)\|_\infty/2c\sigma^2)C=exp(∥R(1,⋅)−R(0,⋅)∥∞​/2cσ2).
  • Proof of Theorem 3.2, p. 8: ggg is continuous on the compact interval containing its range.

Significance

The theorem reduces an infinite-dimensional fixed point, over laws on R\mathbb RR defined through a control problem on path space, to a scalar equation for the mean. Everything else is explicit: the equilibrium law is a reparametrized Gaussian quantile, and the game value is a closed form in RRR. The paper's later results build on this: the comparison of game values under the Lorenz order of rewards (Theorem 4.1), the characterization of rewards that realize a target equilibrium (Theorem 5.1), and the tournament design problems of Section 5 all start from (3.2) and the value formula.

The result is proved in the paper, partly by appeal to the literature on Schrödinger bridges; Proposition 2.1 is stated there without proof. None of it is formalized. A formal development would supply the first machine-checked mean field equilibrium of a rank-based game, the entropic weak formulation of a control problem with a terminal reward, and a verified explicit solution against which numerical schemes can be checked.

Difficulty

The reduction from path measures to terminal laws, (2.6), needs the disintegration of QQQ along XTX_TXT​ (the Schrödinger bridge) and the chain rule for relative entropy; only one inequality follows from data processing. The best response is a Gibbs variational principle on the line, but the optimizer must be lifted back to path space and every optimizer must be shown to have the same terminal law. In Theorem 3.2 the characterization requires inverting y(r)=N((qμ(r)−x0)/σT)y(r)=N((q_\mu(r)-x_0)/\sigma\sqrt T)y(r)=N((qμ​(r)−x0​)/σT​), which in turn requires differentiating through a quantile function when RRR is only monotone in rrr, not continuous. Existence needs integrability of N−1N^{-1}N−1, which is unbounded at both ends, uniformly in mmm, and continuity of ggg by dominated convergence. The natural shortcut, treating the equilibrium as a density solving (3.1), does not prove the theorem: the equilibrium is defined through the control problem, and connecting the two is the content of the milestones.

Formalization scope

All declarations live in the namespace TerminalRank.Equilibrium, in one definitions module Model. Conventions:

  • Ω\OmegaΩ is an arbitrary measurable space with a probability measure PPP under which B:R≥0→Ω→RB:\mathbb R_{\ge0}\to\Omega\to\mathbb RB:R≥0​→Ω→R satisfies Mathlib's IsBrownianReal. This is the paper's Wiener space up to relabelling, and also covers its Remark 2.1 (larger filtrations). TTT has type ℝ≥0, and σ>0\sigma>0σ>0 (the paper needs only σ≠0\sigma\ne0σ=0).
  • Rewards are real-valued, and the bounded reward classes carry a uniform bound; monotonicity and boundedness are required for ranks r∈[0,1]r\in[0,1]r∈[0,1] only. Three milestones, stated in the paper for general R∈RR\in\mathcal RR∈R, are specialized to R∈RbR\in\mathcal R_bR∈Rb​, where the reward expectation in (2.3) is defined; the goal assumes R∈Rbrm⊂RbR\in\mathcal R^{rm}_b\subset\mathcal R_bR∈Rbrm​⊂Rb​ anyway. The population law has a finite first moment wherever the paper uses RμR_\muRμ​; equilibrium includes this condition.
  • Relative entropy is Mathlib's klDiv, valued in [0,∞][0,\infty][0,∞]. The suprema in (2.3) and (2.6) run over measures with finite entropy; the excluded ones have value −∞-\infty−∞ in the paper, so nothing changes.
  • The quantile is the left-continuous inverse inf⁡{x:r≤F(x)}\inf\{x:r\le F(x)\}inf{x:r≤F(x)}, and (3.2) is required for r∈(0,1)r\in(0,1)r∈(0,1). The goal states the finiteness of the mean of μ\muμ explicitly; it holds for every equilibrium.

VVV, optimality and equilibrium are defined from the path-space problem (2.3). A formalization that defines them by (2.6), (2.9) or (3.1), or replaces (Ω,P,B)(\Omega,P,B)(Ω,P,B) by a single Gaussian variable, would make the milestones definitional and is ruled out.

Needed infrastructure: Gibbs variational principle (published on the platform as DonskerVaradhan.integral_sub_klDiv_le_log_integral_exp and DonskerVaradhan.klDiv_tilted_self_eq), disintegration and the chain rule for klDiv, Brownian bridges, change of variables for quantile functions, and E∣Z∣=2/πE|Z|=\sqrt{2/\pi}E∣Z∣=2/π​. The quantile and Brownian-bridge lemmas are reusable well beyond this mission. Contributions toward any milestone, and auxiliary lemmas on these tools, are welcome.

Selected references

  • E. Bayraktar and Y. Zhang, Terminal Ranking Games, arXiv:1906.09628v2, 2020; Mathematics of Operations Research, 2021. https://arxiv.org/abs/1906.09628
  • E. Bayraktar, J. Cvitanić and Y. Zhang, Large tournament games, Annals of Applied Probability 29(6), 2019. https://doi.org/10.1214/19-AAP1490
  • E. Bayraktar and Y. Zhang, A rank-based mean field game in the strong formulation, Electronic Communications in Probability 21, 2016. https://doi.org/10.1214/16-ECP24
  • E. P. Lazear and S. Rosen, Rank-order tournaments as optimum labor contracts, Journal of Political Economy 89(5), 1981. https://doi.org/10.1086/261010
  • H. Föllmer, Random fields and diffusion processes, École d'Été de Probabilités de Saint-Flour XV–XVII, Lecture Notes in Mathematics 1362, Springer, 1988. https://doi.org/10.1007/BFb0086180
  • Y. Chen, T. T. Georgiou and M. Pavon, On the relation between optimal transport and Schrödinger bridges: a stochastic control viewpoint, Journal of Optimization Theory and Applications 169, 2016. https://doi.org/10.1007/s10957-015-0803-z
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Combinatorics·Captain: @bwdaugherty

Zero-Core Theorem for Ramsey R(5,5)Research Paper

Motivation

The Zero-Core Theorem establishes a fundamental structural property of Ramsey graph colorings: the obstruction preventing extension of the champion R(5,5) coloring from n=43 to n=44 is fully distributed across all constraints, with no individual bottleneck.

This is the first formalization of an essential core theorem in Ramsey theory.

Setting

Given an infeasible constraint system S = {c₁, ..., cₘ}, a constraint cᵢ is essential if S \ {cᵢ} is feasible. The essential core 𝓔 ⊆ S is the set of all essential constraints.

Formalization target

Goal: Prove that the essential core of the K₄₄ extension problem is empty (𝓔 = ∅).

The champion K₄₃ coloring (with 137 monochromatic K₅ violations) contains 2,480 monochromatic K₄ subgraphs. The theorem proves that removing any single K₄ constraint from this system leaves it infeasible.

Significance

This demonstrates that R(5,5) = 43 is a "deep" combinatorial fact arising from holistic constraint interaction, not from any individual forcing constraint. The distributed nature of the obstruction connects to permutation-invariant energy barriers in optimization landscapes.

Difficulty

The theorem requires:

  1. Defining constraint systems and feasibility
  2. Formalizing the essential core concept
  3. Proving infeasibility is preserved under single-constraint removal
  4. Computational verification across 2,480 cases

Formalization scope

  • Constraint satisfaction problems
  • Graph coloring extensions
  • Essential core theory
  • Computational proof certificates

Selected references

  • Daugherty, B. et al. Falsification of R(8,8) > 293: Exhaustive Max-Clique Verification. Zenodo, 2026. DOI: 10.5281/zenodo.19414435
  • Exoo, G. A lower bound for R(5,5). J. Graph Theory, 1989.
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Algorithmic Game TheoryControl TheoryProbability+1·Captain: mikedeng1

Dynamic Set Values for Nonzero-Sum Games with Multiple Equilibriums: The Set Value of a Continuous-Time Nonzero-Sum Stochastic Differential Game Satisfies the Dynamic Programming PrincipleResearch Paper

Motivation

A nonzero-sum game can have several Nash equilibria with different cost vectors. Selecting one equilibrium before asking how the game behaves over time loses information and may make a proposed dynamic rule depend on that selection. Feinstein, Rudloff and Zhang study the entire set of equilibrium cost vectors and ask whether it can be evaluated consistently after the game is stopped. Their continuous-time result is Theorem 3.9 of the pinned preprint, which the authors identify as the main result of the paper. It follows a discrete-time set-value principle developed earlier in the same work. The question is relevant to stochastic games whose controls use the observed path history and whose players need not share an objective.

Setting

Fix a horizon T>0T>0T>0, a positive state dimension ddd, and a positive number NNN of players. The canonical path space is

Ω={ω∈C([0,T];Rd):ω0=0}.\Omega=\{\omega\in C([0,T];\mathbb R^d):\omega_0=0\}.Ω={ω∈C([0,T];Rd):ω0​=0}.

Its coordinate process is Bt(ω)=ωtB_t(\omega)=\omega_tBt​(ω)=ωt​. The measure P0\mathbb P_0P0​ is Wiener measure, and Ft\mathcal F_tFt​ is the filtration generated by the coordinates through time ttt, augmented by Borel P0\mathbb P_0P0​-null events. Each player iii has a nonempty convex action set AiA_iAi​. A control profile α=(α1,…,αN)\alpha=(\alpha^1,\ldots,\alpha^N)α=(α1,…,αN) consists of progressively measurable, AiA_iAi​-valued processes. A unilateral deviation may be any such process for that player.

The drift bbb depends on the entire profile, while player iii's running cost fif_ifi​ depends on that player's own action. The terminal cost vector is ξ\xiξ. Assumption 3.1 requires progressive measurability and boundedness of these data. Assumption 3.6 requires uniform continuity in time and path history, and uniform continuity in actions. For a history (t,ω)(t,\omega)(t,ω), concatenation ω⊗tω~\omega\otimes_t\widetilde\omegaω⊗t​ω holds the old path through ttt and continues with the increment path afterward. The paper changes measure from P0\mathbb P_0P0​ with a Girsanov density MT−tt,ω,αM^{t,\omega,\alpha}_{T-t}MT−tt,ω,α​, then defines the cost Ji(t,ω,α)J_i(t,\omega,\alpha)Ji​(t,ω,α) as the expected shifted terminal cost plus running cost.

An ε\varepsilonε-equilibrium is a profile whose cost for every player is at most ε\varepsilonε above the cost of every unilateral deviation. Let Oε(y)O_\varepsilon(y)Oε​(y) be the open Euclidean ball of radius ε\varepsilonε around yyy. The set value is the intersection of the relaxed value sets

Vε(t,ω)=⋃α∈NEε(t,ω)Oε(J(t,ω,α)),V(t,ω)=⋂ε>0Vε(t,ω).\mathbb V_\varepsilon(t,\omega) =\bigcup_{\alpha\in NE_\varepsilon(t,\omega)} O_\varepsilon(J(t,\omega,\alpha)),\qquad \mathbb V(t,\omega)=\bigcap_{\varepsilon>0}\mathbb V_\varepsilon(t,\omega).Vε​(t,ω)=α∈NEε​(t,ω)⋃​Oε​(J(t,ω,α)),V(t,ω)=ε>0⋂​Vε​(t,ω).

The open lower envelope V^ε\widehat{\mathbb V}_\varepsilonVε​ is the union of Vε′\mathbb V_{\varepsilon'}Vε′​ over 0<ε′<ε0<\varepsilon'<\varepsilon0<ε′<ε. These objects are defined even if the game has no exact equilibrium.

Formalization targets

The target is Theorem 3.9 in the form (3.12) treated in its proof, at the zero history and initial time. For a stopping time τ\tauτ with τ(0)>0\tau(0)>0τ(0)>0, let J(τ,η;0,0,α)J(\tau,\eta;0,0,\alpha)J(τ,η;0,0,α) denote the cost of the game stopped at τ\tauτ with bounded Fτ\mathcal F_\tauFτ​-measurable terminal vector η\etaη. The claim is

V(0,0)=⋂ε>0{y:∃η,αα∈NEε(τ,η;0,0),y∈Oε(J(τ,η;0,0,α)),P0 ⁣(η∉V^ε(τ,B))≤ε}.\mathbb V(0,0)=\bigcap_{\varepsilon>0} \left\{y:\begin{array}{l} \exists\eta,\alpha\quad \alpha\in NE_\varepsilon(\tau,\eta;0,0),\\ y\in O_\varepsilon(J(\tau,\eta;0,0,\alpha)),\\ \mathbb P_0\!\left(\eta\notin \widehat{\mathbb V}_\varepsilon(\tau,B)\right)\le\varepsilon \end{array}\right\}.V(0,0)=ε>0⋂​⎩⎨⎧​y:∃η,αα∈NEε​(τ,η;0,0),y∈Oε​(J(τ,η;0,0,α)),P0​(η∈/Vε​(τ,B))≤ε​⎭⎬⎫​.

The seven milestones reproduce Proposition 3.4, the density moment bound (3.6), the cost-continuity estimate (3.4), Theorem 3.7(i), Theorem 3.8, and both parts of Lemma 3.10. They cover compactness, regularity and measurability of the set value, as well as approximation of stopping data and controls.

Significance

The equality relates the set of full-horizon equilibrium costs to stopped games whose terminal payoff is approximately compatible with the continuation set value. It gives a dynamic characterization without choosing a particular equilibrium. The relaxation by the same ε\varepsilonε in equilibrium, value ball and exceptional-event probability is part of the result; removing one of those terms changes the game being characterized.

The result is proved in the cited preprint. The mission asks for machine-checked proofs of the stated theorem and its supporting results. The reusable development includes canonical finite-horizon Wiener paths, their augmented filtration, path concatenation, progressive control profiles, a coordinatewise stochastic integral interface, and set-valued equilibrium costs. The published Ethier–Kurtz definition of the Itô-integral relation is reused; it supplies a definition, not a proof of this paper's results.

Difficulty

At a stopping time, the continuation value is a set that depends on the observed path. A pointwise description does not by itself show that membership in this random set is measurable at the stopping time. Equilibrium conditions also compare a profile against every progressively measurable unilateral deviation, so their stability cannot be reduced to a comparison of finitely many actions. The Girsanov density introduces another dependency: its stochastic integral and the resulting costs must be genuine integrable random variables before inequalities between cost vectors have their intended meaning.

Formalization scope

Lean represents Rd\mathbb R^dRd and RN\mathbb R^NRN by Euclidean spaces, with Euclidean norms on costs and the action product. Paths are continuous maps on [0,T][0,T][0,T] constrained to start at zero. The canonical process is clamped outside the horizon only to make its notation total. The Wiener law is pinned by Brownian finite-dimensional distributions through TTT and independence of coordinate processes. The filtration adds Borel null sets, so it remains a sub-σ-algebra of the Borel space. Time-indexed controls live on [0,T][0,T][0,T]; the stopping times themselves use WithTop ℝ and are constrained to that interval.

Concatenation uses the second increment strictly after ttt, resolving the overlapping endpoint in the printed indicator formula. Player iii's running cost takes only aia_iai​. The moduli in Assumption 3.6 are common and uniform in the variables specified there. The stopped running cost integrates to τ−t\tau-tτ−t, with an empty interval contributing zero only outside the theorem's admissible range. The goal uses bounded measurable representatives of L∞L^\inftyL∞ terminal payoffs; changing a representative on a null set leaves the expected costs and exceptional probability unchanged.

The statement must retain the full Girsanov density, all progressive deviations, the open envelope V^ε\widehat{\mathbb V}_\varepsilonVε​, and a nonzero player count. A default-zero integral for a nonintegrable payoff, an arbitrary measure in place of Wiener measure, or a restricted deviation class would trivialize or alter it. Solvers can contribute the integrability and stochastic-integral existence facts needed to establish that the definitions have their intended values, followed by proofs of the listed milestones and goal.

Selected references

  • Zachary Feinstein, Birgit Rudloff and Jianfeng Zhang, Dynamic Set Values for Nonzero Sum Games with Multiple Equilibriums, arXiv preprint arXiv:2002.00449v2, 2020, §§3.1–3.3. Preprint.
  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 5, §2. Publisher record.
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Control TheoryDynamic ProgrammingProbability+1·Captain: mikedeng1

McKean–Vlasov Optimal Control: Limit Theory and Equivalence Between Different Formulations: The N-Player Common-Noise Control Value Converges to the McKean–Vlasov ValueResearch Paper

Why this limit matters

A controller of a large population may choose a separate action for each participant while all participants experience the same random environment. The resulting optimization problem has a growing state space: with NNN participants, the state records NNN paths and NNN controls. A McKean–Vlasov control problem replaces the empirical distribution of those participants by a conditional distribution given the common noise. Djete, Possamaï and Tan prove that this replacement preserves the optimal value asymptotically, even when the participants have different initial laws and the average of those laws does not converge along the full sequence. Their result is Theorem 3.6(iii) of the 2020 preprint, published in 2022.

The distinction between common and individual noise matters for this claim. Conditional on the common noise, particles can still be correlated through a controller that observes the full particle system. The paper's limit theorem concerns the supremum over all admissible predictable particle controls, rather than one prescribed feedback rule. This is the setting in which a finite population optimization problem can approximate its limiting stochastic control problem. The adjacent Proposition 3.7 describes how the limiting value changes with the initial law.

Setting

Fix a time horizon T>0T>0T>0, state dimension n≥1n\ge1n≥1, individual noise dimension d≥1d\ge1d≥1, and common noise dimension ℓ≥0\ell\ge0ℓ≥0. Let AAA be a nonempty Polish control space with base point a0a_0a0​. A state or noise path belongs to Ck=C([0,T],Rk)C^k=C([0,T],\mathbb R^k)Ck=C([0,T],Rk), with its uniform norm. The coefficients b,σ,σ0b,\sigma,\sigma_0b,σ,σ0​ determine the drift, individual diffusion and common diffusion; LLL and ggg determine running and terminal rewards. The Wasserstein distance Wp\mathcal W_pWp​ measures the discrepancy between probability laws with finite pppth moments.

For an initial law ν\nuν, the strong problem lives on the canonical space Ω=Rn×Cd×Cℓ\Omega=\mathbb R^n\times C^d\times C^\ellΩ=Rn×Cd×Cℓ. Its initial state has law ν\nuν, and W,BW,BW,B are independent Brownian noises relative to the canonical past. An admissible control α\alphaα is predictable and has finite expected integrated pppth power of its distance from a0a_0a0​. The state XαX^\alphaXα solves the controlled equation (2.3). Its coefficients use the conditional law μˉtα\bar\mu_t^\alphaμˉ​tα​ of the stopped state path and current control given the history of BBB; its terminal reward uses the conditional law μTα\mu_T^\alphaμTα​ of the stopped state path. The strong value VS(ν)V_S(\nu)VS​(ν), equation (2.4), is the supremum of expected reward over those controls and their solutions. These definitions appear in Section 2.1.

For N≥1N\ge1N≥1, the particle problem has initial laws ν1,…,νN\nu^1,\ldots,\nu^Nν1,…,νN, separate Brownian noises WiW^iWi, and one shared BBB. Each particle follows equation (2.16) with the empirical state-control law φtN=N−1∑iδ(Xt∧⋅i,αti)\varphi_t^N=N^{-1}\sum_i\delta_{(X^i_{t\wedge\cdot},\alpha_t^i)}φtN​=N−1∑i​δ(Xt∧⋅i​,αti​)​ inside its coefficients. The terminal reward uses the empirical state-path law φtN,X\varphi_t^{N,X}φtN,X​. Equation (2.17) defines VSN(ν1,…,νN)V_S^N(\nu^1,\ldots,\nu^N)VSN​(ν1,…,νN) as the supremum of the average expected reward. The empirical laws are built from the very particles whose equations use them; they are not outside inputs. See Section 2.4.

Formalization targets

The goal is the value comparison in Theorem 3.6(iii), equation (3.3):

lim⁡N→∞∣VSN(ν1,…,νN)−VS ⁣(1N∑i=1Nνi)∣=0.\lim_{N\to\infty}\left|V_S^N(\nu^1,\ldots,\nu^N)-V_S\!\left(\frac1N\sum_{i=1}^N\nu^i\right)\right|=0.N→∞lim​​VSN​(ν1,…,νN)−VS​(N1​i=1∑N​νi)​=0.

The hypotheses include Assumptions 2.1 and 2.12, an embedding A⊂RjA\subset\mathbb R^jA⊂Rj for some j≥1j\ge1j≥1, continuity of LLL and ggg, and a uniform bound on the averages of the initial p′p'p′th moments, where p′>p≥2p'>p\ge2p′>p≥2. The goal does not assume that the averaged initial laws converge. The milestones are the value lower bounds of Propositions 4.15 and 4.16, the subsequence value limit used in equation (4.44), and the initial-law stability statement (3.4) of Proposition 3.7. Each milestone records the particular clause formalized when its printed result contains additional conclusions. Theorem 3.6 and its proof give the source order.

What the result provides

The theorem compares two optimization problems, rather than only the law of a fixed controlled particle system. The comparison permits heterogeneous initial distributions and keeps the common noise in both models. Proposition 3.7 gives a separate stability statement for the limiting value when initial laws converge in Wp\mathcal W_pWp​ with uniformly bounded p′p'p′th moments. Together these statements identify which finite population values are represented by the limiting control formulation. They are proved in the paper; the open task here is a machine checked derivation from faithful statements.

The formal development fixes the interfaces for conditional laws, predictable controls, path dependent coefficients, Brownian Itô integrals, empirical probability laws and extended real rewards. Those interfaces can support later formalizations of common-noise control and propagation of chaos. The present mission does not state Theorem 3.1(i), the approximation clauses of Theorem 3.1(ii)–(iii), Theorem 3.6(ii), or the “In particular” sentence after Proposition 3.7's equation (3.4). Their different conclusions require further canonical and relaxed-control structures, and the last sentence has a topology ambiguity documented in the paper notes.

Main difficulty

The usual fixed-control convergence question is smaller than the target: particle controls may depend on every observed particle and on the common noise, and the target takes a supremum before comparing values. The conditional law in the limiting equation depends on its own solution, while the empirical law in each particle equation depends on the full coupled particle system. Dropping either dependence changes the optimization problem. Uniform p′p'p′th moment control must also coexist with unbounded rewards and the extended real convention for their expectations. The source proof invokes compactness and equivalence between strong, weak and relaxed formulations; formalizing those links is substantial work beyond compiling the goal statement.

Formalization scope

Lean uses EuclideanSpace and continuous maps on [0,T][0,T][0,T] for the path spaces, and Frobenius norms for diffusion matrices. The control type carries a Polish Borel metric and a base point. Pp\mathcal P_pPp​ is a finite-lintegral moment condition, and Wp\mathcal W_pWp​ takes values in R≥0∪{∞}\mathbb R_{\ge0}\cup\{\infty\}R≥0​∪{∞}. Values are extended real suprema over admissible controls and actual solutions. Rewards use the paper's convention ∞−∞=−∞\infty-\infty=-\infty∞−∞=−∞, rather than a default zero integral. Particle counts are positive; Lean player index zero denotes the paper's player one. The case ℓ=0\ell=0ℓ=0 remains included.

Assumption 2.1 includes the displayed Lipschitz, growth and coercive bounds, Borel measurability, nonanticipativity, and lower semicontinuity. Assumption 2.12 factors the coefficients through the state marginal, with σ0\sigma_0σ0​ independent of the control. The paper leaves the topology behind “continuous” unnamed; the formalization uses sequential Wp\mathcal W_pWp​ continuity on finite-moment laws. Its A⊂RjA\subset\mathbb R^jA⊂Rj is read as an isometric embedding. Solutions have continuous paths and are adapted to the completed canonical filtration, while conditional laws use the raw common-noise filtration. The goal states finiteness of both values so its real absolute difference is defined. Equation (4.44) is posed in the subsequence form used by its proof. These choices and the source's printed slips are detailed in the moderation notes.

The interface rules out a free conditional-law flow, a free particle empirical measure, and an uncharacterized Brownian law. The weak and relaxed formulations appear only as context for the paper's proof; this proposal contains the strong and particle layers needed by the four selected milestones. Contributions to the omitted equivalence and compactness results are welcome once their canonical-space definitions have been audited.

Selected references

  • Mao Fabrice Djete, Dylan Possamaï and Xiaolu Tan, McKean–Vlasov optimal control: limit theory and equivalence between different formulations, Mathematics of Operations Research, 2022; arXiv:2001.00925v2. The formal statements use this preprint's pagination and equation numbers.
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Machine LearningProbabilityReinforcement Learning+1·Captain: mikedeng1

Efficiently Breaking the Curse of Horizon in Off-Policy Evaluation with Double Reinforcement Learning: Cross-Fitted DRL Is Asymptotically Linear and Normal at the MDP Efficiency BoundResearch Paper

Motivation

Off-policy evaluation (OPE) asks for the long-run value of a target decision policy, using only data collected under a different policy. It arises wherever running the target policy is expensive or unsafe: a new treatment rule in medicine, a new recommendation or pricing rule, a candidate controller in reinforcement learning. Importance-sampling estimators reweight whole trajectories. Their variance grows exponentially with the horizon, the curse of horizon (Liu et al. 2018, arXiv:1810.12429).

Kallus and Uehara (arXiv:1909.05850, Operations Research 2022) treat infinite-horizon discounted OPE as a semiparametric estimation problem. They derive the efficiency bound under three models: non-Markov, time-varying Markov and time-invariant Markov (MDP). They then propose double reinforcement learning (DRL), an estimator that combines a q-function estimate with an estimate of the ratio between the discounted state visitation of the target policy and the state distribution of the data. In the MDP model it attains the efficiency bound. This mission formalizes the transition-sampling version of that result, Theorem 6.

Timeline:

  • 2016: Jiang and Li (arXiv:1511.03722) and Thomas and Brunskill (arXiv:1604.00923) give doubly robust OPE estimators for finite horizons, built on trajectory-wise importance weights.
  • 2018: Liu, Li, Tang and Zhou (arXiv:1810.12429) replace trajectory weights by stationary state-distribution ratios, removing the exponential dependence on the horizon, but without efficiency guarantees.
  • 2018: Chernozhukov et al. (arXiv:1608.00060) formalize cross-fitting and Neyman orthogonality for estimation with machine-learned nuisances (double machine learning).
  • 2019–2022: Kallus and Uehara derive the MDP efficiency bound (Theorem 3) and prove that cross-fitted DRL attains it (Theorem 6), also under trajectory sampling with mixing (Theorems 10–13).

Setting

States lie in a measurable space SSS and actions in a measurable space AAA. A time-invariant MDP is a transition kernel p(s′∣s,a)p(s'\mid s,a)p(s′∣s,a) and a reward kernel p(r∣s,a)p(r\mid s,a)p(r∣s,a) with rewards in [0,Rmax⁡][0,R_{\max}][0,Rmax​]. A policy π(a∣s)\pi(a\mid s)π(a∣s) is a kernel from SSS to AAA. Fix a discount γ∈[0,1)\gamma\in[0,1)γ∈[0,1), a known target policy πe\pi_eπe​ with known initial law pπe(0)p^{(0)}_{\pi_e}pπe​(0)​, and a behavior policy πb\pi_bπb​.

The estimand is the normalized discounted value

ρπe=lim⁡T→∞(∑t=0Tγt)−1Epπe[∑t=0Tγtrt].\rho^{\pi_e}=\lim_{T\to\infty}\Big(\sum_{t=0}^T\gamma^t\Big)^{-1}\mathbb E_{p_{\pi_e}}\Big[\sum_{t=0}^T\gamma^tr_t\Big].ρπe​=T→∞lim​(t=0∑T​γt)−1Epπe​​​[t=0∑T​γtrt​].

The q-function is q(s,a)=Epπe[∑kγkrk∣s0=s,a0=a]q(s,a)=\mathbb E_{p_{\pi_e}}[\sum_k\gamma^kr_k\mid s_0=s,a_0=a]q(s,a)=Epπe​​​[∑k​γkrk​∣s0​=s,a0​=a], and v(s)=∫q(s,a) πe(da∣s)v(s)=\int q(s,a)\,\pi_e(da\mid s)v(s)=∫q(s,a)πe​(da∣s). The discounted visitation is pπe,γ(∞)=(1−γ)∑tγtpπe(t)p^{(\infty)}_{\pi_e,\gamma}=(1-\gamma)\sum_t\gamma^t p^{(t)}_{\pi_e}pπe​,γ(∞)​=(1−γ)∑t​γtpπe​(t)​, where pπe(t)p^{(t)}_{\pi_e}pπe​(t)​ is the law of sts_tst​.

Transition sampling. The data are i.i.d. observations Oi=(s,a,r,s′)O_i=(s,a,r,s')Oi​=(s,a,r,s′) with law pπbp_{\pi_b}pπb​​: s∼pπb(0)s\sim p^{(0)}_{\pi_b}s∼pπb​(0)​, a∼πb(⋅∣s)a\sim\pi_b(\cdot\mid s)a∼πb​(⋅∣s), and, given (s,a)(s,a)(s,a), independently r∼p(⋅∣s,a)r\sim p(\cdot\mid s,a)r∼p(⋅∣s,a) and s′∼p(⋅∣s,a)s'\sim p(\cdot\mid s,a)s′∼p(⋅∣s,a). The law of s′s's′ may differ from that of sss.

The density ratios are η(s,a)=πe(a∣s)/πb(a∣s)\eta(s,a)=\pi_e(a\mid s)/\pi_b(a\mid s)η(s,a)=πe​(a∣s)/πb​(a∣s) and w(s)=pπe,γ(∞)(s)/pπb(0)(s)w(s)=p^{(\infty)}_{\pi_e,\gamma}(s)/p^{(0)}_{\pi_b}(s)w(s)=pπe​,γ(∞)​(s)/pπb​(0)​(s). For candidate nuisances w′,q′w',q'w′,q′, with v′(s)=∫q′(s,a)πe(da∣s)v'(s)=\int q'(s,a)\pi_e(da\mid s)v′(s)=∫q′(s,a)πe​(da∣s), the estimating function is

ψ(s,a,r,s′;w′,q′)=(1−γ) Epπe(0)[v′(s0)]+w′(s)η(s,a)(r+γv′(s′)−q′(s,a)).\psi(s,a,r,s';w',q')=(1-\gamma)\,\mathbb E_{p^{(0)}_{\pi_e}}[v'(s_0)]+w'(s)\eta(s,a)\big(r+\gamma v'(s')-q'(s,a)\big).ψ(s,a,r,s′;w′,q′)=(1−γ)Epπe​(0)​​[v′(s0​)]+w′(s)η(s,a)(r+γv′(s′)−q′(s,a)).

The cross-fitted estimator ρ^DRL(M3)\hat\rho_{\rm DRL}(\mathcal M_3)ρ^​DRL​(M3​) splits the sample into two folds. It fits w^[j],q^[j]\hat w^{[j]},\hat q^{[j]}w^[j],q^​[j] on fold jjj and averages ψ\psiψ over all observations, each evaluated at the nuisances of the other fold. The efficient influence function is ϕeff=w(s)η(s,a)(r+γv(s′)−q(s,a))\phi_{\rm eff}=w(s)\eta(s,a)(r+\gamma v(s')-q(s,a))ϕeff​=w(s)η(s,a)(r+γv(s′)−q(s,a)), and the efficiency bound is EB(M3)=E[ϕeff2]\mathrm{EB}(\mathcal M_3)=\mathbb E[\phi_{\rm eff}^2]EB(M3​)=E[ϕeff2​].

Formalization targets

Goal: Theorem 6

Assume the following:

  • w≤Cww\le C_ww≤Cw​ and pb,S′≤CS′pb,Sp_{b,S'}\le C_{S'}p_{b,S}pb,S′​≤CS′​pb,S​ (6a);
  • η≤Cη\eta\le C_\etaη≤Cη​ (added);
  • w^[j],q^[j]\hat w^{[j]},\hat q^{[j]}w^[j],q^​[j] lie in [0,Cw][0,C_w][0,Cw​] and [0,Rmax⁡/(1−γ)][0,R_{\max}/(1-\gamma)][0,Rmax​/(1−γ)] (6b);
  • ∥w^[j]−w∥2,∥q^[j]−q∥2=op(1)\|\hat w^{[j]}-w\|_2,\|\hat q^{[j]}-q\|_2=o_p(1)∥w^[j]−w∥2​,∥q^​[j]−q∥2​=op​(1) (6c);
  • n ∥w^[j]−w∥2∥q^[k]−q∥2=op(1)\sqrt n\,\|\hat w^{[j]}-w\|_2\|\hat q^{[k]}-q\|_2=o_p(1)n​∥w^[j]−w∥2​∥q^​[k]−q∥2​=op​(1) for all j,k∈{0,1}j,k\in\{0,1\}j,k∈{0,1} (6d, equivalent to common envelopes for both folds).

Then

n(ρ^DRL(M3)−ρπe)−1n∑i<nϕeff(Oi)→p0,n(ρ^DRL(M3)−ρπe)→dN(0,EB(M3)).\sqrt n\big(\hat\rho_{\rm DRL}(\mathcal M_3)-\rho^{\pi_e}\big)-\frac1{\sqrt n}\sum_{i<n}\phi_{\rm eff}(O_i)\xrightarrow{p}0,\qquad \sqrt n\big(\hat\rho_{\rm DRL}(\mathcal M_3)-\rho^{\pi_e}\big)\xrightarrow{d}N\big(0,\mathrm{EB}(\mathcal M_3)\big).n​(ρ^​DRL​(M3​)−ρπe​)−n​1​i<n∑​ϕeff​(Oi​)p​0,n​(ρ^​DRL​(M3​)−ρπe​)d​N(0,EB(M3​)).

No rate exponent or learner class is fixed. Only the product rate enters.

Milestones, in proof order

  1. Lemma 1 (forward): E[γw(s)η(s,a)f(s′)−w(s)f(s)]+(1−γ)Epπe(0)[f]=0\mathbb E[\gamma w(s)\eta(s,a)f(s')-w(s)f(s)]+(1-\gamma)\mathbb E_{p^{(0)}_{\pi_e}}[f]=0E[γw(s)η(s,a)f(s′)−w(s)f(s)]+(1−γ)Epπe​(0)​​[f]=0 for bounded measurable fff.
  2. ρπe=E[w(s)η(s,a)r]\rho^{\pi_e}=\mathbb E[w(s)\eta(s,a)r]ρπe​=E[w(s)η(s,a)r] (p. 16).
  3. Eq. (5): E[ψ(w′,q)]=(1−γ)Epπe(0)[v]=ρπe\mathbb E[\psi(w',q)]=(1-\gamma)\mathbb E_{p^{(0)}_{\pi_e}}[v]=\rho^{\pi_e}E[ψ(w′,q)]=(1−γ)Epπe​(0)​​[v]=ρπe​ for every bounded w′w'w′.
  4. ψ(w,q)=ρπe+ϕeff\psi(w,q)=\rho^{\pi_e}+\phi_{\rm eff}ψ(w,q)=ρπe​+ϕeff​ pointwise (p. 22).
  5. Eqs. (6)–(8): E[ψ(w,q′)]=ρπe\mathbb E[\psi(w,q')]=\rho^{\pi_e}E[ψ(w,q′)]=ρπe​ for every bounded q′q'q′.
  6. Jensen step, corrected: ∥v^(s′)−v(s′)∥2≤CS′Cη ∥q^−q∥2\|\hat v(s')-v(s')\|_2\le\sqrt{C_{S'}C_\eta}\,\|\hat q-q\|_2∥v^(s′)−v(s′)∥2​≤CS′​Cη​​∥q^​−q∥2​.
  7. Term (30): ∣Eψ(w^,q^)−ρπe∣≤Cη(1+γCS′Cη)∥w^−w∥2∥q^−q∥2|\mathbb E\psi(\hat w,\hat q)-\rho^{\pi_e}|\le C_\eta(1+\gamma\sqrt{C_{S'}C_\eta})\|\hat w-w\|_2\|\hat q-q\|_2∣Eψ(w^,q^​)−ρπe​∣≤Cη​(1+γCS′​Cη​​)∥w^−w∥2​∥q^​−q∥2​.
  8. Term (28), variance: var⁡[ψ(w^,q^)−ψ(w,q)]≤2a2∥w^−w∥22+2b2∥q^−q∥22\operatorname{var}[\psi(\hat w,\hat q)-\psi(w,q)]\le2a^2\|\hat w-w\|_2^2+2b^2\|\hat q-q\|_2^2var[ψ(w^,q^​)−ψ(w,q)]≤2a2∥w^−w∥22​+2b2∥q^​−q∥22​.
  9. Term (28) is op(1)o_p(1)op​(1): the centred fold empirical process at the opposite fold's nuisances vanishes.

Significance

Theorem 6 shows that, in a Markov model, a n\sqrt nn​-consistent and efficient OPE estimator exists whose variance scales with the number of observed transitions, not trajectories. It requires no complexity (Donsker or entropy) restriction on the nuisance estimators, only a product rate. Any black-box learners with ∥w^−w∥2∥q^−q∥2=op(n−1/2)\|\hat w-w\|_2\|\hat q-q\|_2=o_p(n^{-1/2})∥w^−w∥2​∥q^​−q∥2​=op​(n−1/2), which allows two subparametric rates, give asymptotically valid confidence intervals at the efficiency bound. The mixed-bias identities (Eqs. (5)–(8)) and Lemma 1 are the same ingredients used by later minimax and adversarial estimators of www and qqq.

The result is proved in the paper; nothing here is presented as open. As far as is known, none of it has a machine-checked proof: no off-policy evaluation, density-ratio characterization or cross-fitting asymptotics exists in Mathlib or on the platform. Formalizing it checks the appendix argument, which is short and contains errors (below). It also produces a reusable layer: kernel-based discounted MDPs on general measurable spaces, discounted visitation measures, and the cross-fitting plus Slutsky template that other double-machine-learning results share.

Difficulty

The obvious route is "the estimator equals the oracle average Pnψ(w,q)\mathbb P_n\psi(w,q)Pn​ψ(w,q) plus negligible terms, then apply the CLT". Two of its steps are not routine.

First, the negligible terms are random functions evaluated at random data. The empirical-process term (28) is controlled only conditionally on the other fold, through a conditional Chebyshev argument that needs the independence structure of the split. Treating w^,q^\hat w,\hat qw^,q^​ as fixed functions loses exactly this.

Second, the bias term (30) is second order only because of the mixed-bias structure. That structure rests on Lemma 1, a change-of-measure identity between the discounted visitation of πe\pi_eπe​ and the data distribution. The printed constants are wrong. The Jensen step ∥v^(s′)−v(s′)∥2≤CS′∥q^−q∥2\|\hat v(s')-v(s')\|_2\le\sqrt{C_{S'}}\|\hat q-q\|_2∥v^(s′)−v(s′)∥2​≤CS′​​∥q^​−q∥2​ fails when η\etaη is large: with one state, πb\pi_bπb​ uniform on two actions and πe\pi_eπe​ a point mass, the left side is 111 and the right side is 1/21/\sqrt21/2​. The bound by ∥w^−w∥2∥η∥2∥q^−q∥2\|\hat w-w\|_2\|\eta\|_2\|\hat q-q\|_2∥w^−w∥2​∥η∥2​∥q^​−q∥2​ is not a valid inequality for a triple product. Both need a bound η≤Cη\eta\le C_\etaη≤Cη​, which the mission adds.

Formalization scope

  • Spaces and kernels. SSS, AAA are measurable spaces, the action σ-algebra countably generated (for Mathlib's jointly measurable Kernel.rnDeriv). The MDP, the policies and the observation law are Mathlib kernels and measures. The paper's base measures are not used.
  • Ratios. www and η\etaη are toReal of Radon–Nikodym derivatives, not free functions satisfying an identity. Overlap (πe(⋅∣s)≪πb(⋅∣s)\pi_e(\cdot\mid s)\ll\pi_b(\cdot\mid s)πe​(⋅∣s)≪πb​(⋅∣s), pπe,γ(∞)≪pπb(0)p^{(\infty)}_{\pi_e,\gamma}\ll p^{(0)}_{\pi_b}pπe​,γ(∞)​≪pπb​(0)​) is a standing assumption.
  • Objects. qqq is the discounted series, not "a solution of the Bellman equation". ρπe\rho^{\pi_e}ρπe​ is the limit of normalized discounted sums, not (1−γ)E[v](1-\gamma)\mathbb E[v](1−γ)E[v] or E[wηr]\mathbb E[w\eta r]E[wηr]; those identities are milestones. The discounted visitation is the measure (1−γ)∑tγtpπe(t)(1-\gamma)\sum_t\gamma^tp^{(t)}_{\pi_e}(1−γ)∑t​γtpπe​(t)​, the limit of the paper's normalized averages.
  • Cross-fitting. The folds are {i<⌊n/2⌋}\{i<\lfloor n/2\rfloor\}{i<⌊n/2⌋} and the rest. Each learner is a jointly measurable function of its own fold's observations only. Rates are convergence in probability of the actual random L2L^2L2 errors.
  • Conclusion. "RAL and efficient" is posed as asymptotic linearity with influence function ϕeff\phi_{\rm eff}ϕeff​ plus the normal limit. Regularity needs the tangent-space framework of Theorem 3 and is not posed.
  • Ruled out. The oracle statement with w^=w\hat w=ww^=w, q^=q\hat q=qq^​=q is an i.i.d. CLT for a fixed function and drops the theorem's content. It is not an acceptable substitute for the goal.
  • Infrastructure needed. Linearity and Fubini for kernel compositions; summation of discounted occupancies; conditional Chebyshev for cross-fitted empirical processes; Slutsky (TendstoInDistribution with TendstoInMeasure) and Mathlib's i.i.d. CLT tendstoInDistribution_inv_sqrt_mul_sum_sub. The occupancy and Lemma 1 layer and the cross-fitting template are reusable beyond this mission. Proofs of any milestone, and helper lemmas on kernel powers and discounted sums, are welcome.

Selected references

  • N. Kallus and M. Uehara, Efficiently Breaking the Curse of Horizon in Off-Policy Evaluation with Double Reinforcement Learning, Operations Research 70(6), 2022; arXiv:1909.05850v6 (2023). https://arxiv.org/abs/1909.05850
  • Q. Liu, L. Li, Z. Tang and D. Zhou, Breaking the Curse of Horizon: Infinite-Horizon Off-Policy Estimation, NeurIPS 2018. https://arxiv.org/abs/1810.12429
  • V. Chernozhukov, D. Chetverikov, M. Demirer, E. Duflo, C. Hansen, W. Newey and J. Robins, Double/Debiased Machine Learning for Treatment and Structural Parameters, The Econometrics Journal 21(1), 2018. https://arxiv.org/abs/1608.00060
  • N. Jiang and L. Li, Doubly Robust Off-Policy Value Evaluation for Reinforcement Learning, ICML 2016. https://arxiv.org/abs/1511.03722
  • P. Thomas and E. Brunskill, Data-Efficient Off-Policy Policy Evaluation for Reinforcement Learning, ICML 2016. https://arxiv.org/abs/1604.00923
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Operations ResearchProbabilityStatistics·Captain: mikedeng1

Optimal Portfolio Choice with Estimation Risk: No Risk-Free Asset Case: For h > N + 3 the Combining Coefficient c̃* = kψ²/(ψ² + (N−1)/h) Uniquely Maximizes the Expected Out-of-Sample UtilityResearch Paper

Why estimation risk matters for mean-variance portfolios

Mean-variance analysis (Markowitz, 1952) tells an investor which portfolio to hold once the mean vector μ\muμ and covariance matrix Σ\SigmaΣ of asset returns are known. In practice both are estimated from a finite window of past returns, and the portfolio built from the estimates (the plug-in portfolio) performs badly out of sample: its weights are noisy and its realized utility is often far below the theoretical optimum. A long literature asks how to choose portfolio rules that take this estimation risk into account; Kan and Zhou (2007) treat the case with a risk-free asset.

Kan, Wang and Zhou (2022) study the case without a risk-free asset, where the investor must be fully invested in NNN risky assets. There the optimal portfolio splits into the global minimum-variance (GMV) portfolio plus a scaled zero-investment portfolio, and estimation errors enter the two parts very differently. Their §2 derives the exact expected out-of-sample utility of the family of rules that rescale the estimated zero-investment part, and the coefficient that maximizes it. This mission formalizes that derivation.

Setting

An investor chooses weights w∈RNw \in \mathbb R^Nw∈RN with 1N′w=11_N' w = 11N′​w=1 to maximize the mean-variance utility

U(w)=w′μ−γ2 w′Σw,U(w) = w'\mu - \frac{\gamma}{2}\, w'\Sigma w,U(w)=w′μ−2γ​w′Σw,

where γ>0\gamma > 0γ>0 is the risk-aversion coefficient and Σ\SigmaΣ is positive definite. The population quantities that matter are the GMV variance σg2=1/(1N′Σ−11N)\sigma_g^2 = 1/(1_N'\Sigma^{-1}1_N)σg2​=1/(1N′​Σ−11N​), the GMV mean μg=1N′Σ−1μ σg2\mu_g = 1_N'\Sigma^{-1}\mu\,\sigma_g^2μg​=1N′​Σ−1μσg2​, and the squared slope of the asymptote of the minimum-variance frontier, ψ2=μ′Σ−1μ−μg2/σg2≥0\psi^2 = \mu'\Sigma^{-1}\mu - \mu_g^2/\sigma_g^2 \ge 0ψ2=μ′Σ−1μ−μg2​/σg2​≥0.

The returns r1,…,rhr_1, \dots, r_hr1​,…,rh​ of an estimation window of length hhh are independent and identically distributed N(μ,Σ)\mathcal N(\mu, \Sigma)N(μ,Σ). The maximum-likelihood estimators are μ^t=1h∑srs\hat\mu_t = \frac1h\sum_s r_sμ^​t​=h1​∑s​rs​ and Σ^t=1h∑s(rs−μ^t)(rs−μ^t)′\hat\Sigma_t = \frac1h\sum_s (r_s - \hat\mu_t)(r_s - \hat\mu_t)'Σ^t​=h1​∑s​(rs​−μ^​t​)(rs​−μ^​t​)′. From them come the sample GMV portfolio and the sample zero-investment portfolio

w^g,t=Σ^t−11N1N′Σ^t−11N,w^z,t=Σ^t−1(μ^t−1Nμ^g,t),\hat w_{g,t} = \frac{\hat\Sigma_t^{-1}1_N}{1_N'\hat\Sigma_t^{-1}1_N}, \qquad \hat w_{z,t} = \hat\Sigma_t^{-1}(\hat\mu_t - 1_N\hat\mu_{g,t}),w^g,t​=1N′​Σ^t−1​1N​Σ^t−1​1N​​,w^z,t​=Σ^t−1​(μ^​t​−1N​μ^​g,t​),

with μ^g,t=1N′Σ^t−1μ^t/(1N′Σ^t−11N)\hat\mu_{g,t} = 1_N'\hat\Sigma_t^{-1}\hat\mu_t/(1_N'\hat\Sigma_t^{-1}1_N)μ^​g,t​=1N′​Σ^t−1​μ^​t​/(1N′​Σ^t−1​1N​). For a constant combining coefficient c~\tilde cc~ the paper considers

w^t(c~)=w^g,t+c~γ w^z,t;\hat w_t(\tilde c) = \hat w_{g,t} + \frac{\tilde c}{\gamma}\,\hat w_{z,t};w^t​(c~)=w^g,t​+γc~​w^z,t​;

c~=1\tilde c = 1c~=1 is the plug-in rule. The expected out-of-sample utility E[U(w^t(c~))]E[U(\hat w_t(\tilde c))]E[U(w^t​(c~))] evaluates UUU at the true μ\muμ, Σ\SigmaΣ and averages over the sample. The five random quantities μg,t=w^g,t′μ\mu_{g,t} = \hat w_{g,t}'\muμg,t​=w^g,t′​μ, μz,t=w^z,t′μ\mu_{z,t} = \hat w_{z,t}'\muμz,t​=w^z,t′​μ, σg,t2=w^g,t′Σw^g,t\sigma^2_{g,t} = \hat w_{g,t}'\Sigma\hat w_{g,t}σg,t2​=w^g,t′​Σw^g,t​, σz,t2=w^z,t′Σw^z,t\sigma^2_{z,t} = \hat w_{z,t}'\Sigma\hat w_{z,t}σz,t2​=w^z,t′​Σw^z,t​ and σgz,t=w^g,t′Σw^z,t\sigma_{gz,t} = \hat w_{g,t}'\Sigma\hat w_{z,t}σgz,t​=w^g,t′​Σw^z,t​ determine it.

Formalization targets

Goal: the optimal combining coefficient (§2.3, eqs. (20)–(21))

For N≥2N \ge 2N≥2 and h>N+3h > N + 3h>N+3, with

k=(h−N)(h−N−3)h(h−2),c~∗=kψ2ψ2+N−1h,k = \frac{(h-N)(h-N-3)}{h(h-2)}, \qquad \tilde c^* = \frac{k\psi^2}{\psi^2 + \frac{N-1}{h}},k=h(h−2)(h−N)(h−N−3)​,c~∗=ψ2+hN−1​kψ2​,

the coefficient c~∗\tilde c^*c~∗ is the unique maximizer of c~↦E[U(w^t(c~))]\tilde c \mapsto E[U(\hat w_t(\tilde c))]c~↦E[U(w^t​(c~))] over R\mathbb RR, and 0≤c~∗<10 \le \tilde c^* < 10≤c~∗<1, with c~∗>0\tilde c^* > 0c~∗>0 when ψ2>0\psi^2 > 0ψ2>0.

Lemma 1 (eq. (17))

For h>N+3h > N + 3h>N+3 and every constant c~\tilde cc~,

E[U(w^t(c~))]=μg−γ(h−2)σg22(h−N−1)+hγ(h−N−1)[c~ψ2−c~2(h−2)(hψ2+N−1)2(h−N)(h−N−3)].E[U(\hat w_t(\tilde c))] = \mu_g - \frac{\gamma(h-2)\sigma_g^2}{2(h-N-1)} + \frac{h}{\gamma(h-N-1)}\left[\tilde c\psi^2 - \frac{\tilde c^2(h-2)(h\psi^2+N-1)}{2(h-N)(h-N-3)}\right].E[U(w^t​(c~))]=μg​−2(h−N−1)γ(h−2)σg2​​+γ(h−N−1)h​[c~ψ2−2(h−N)(h−N−3)c~2(h−2)(hψ2+N−1)​].

The moments (A9)–(A13) and the auxiliary moments

E[μg,t]=μg,E[μz,t]=hψ2h−N−1,E[σg,t2]=(h−2)σg2h−N−1,E[\mu_{g,t}] = \mu_g,\quad E[\mu_{z,t}] = \frac{h\psi^2}{h-N-1},\quad E[\sigma^2_{g,t}] = \frac{(h-2)\sigma_g^2}{h-N-1},E[μg,t​]=μg​,E[μz,t​]=h−N−1hψ2​,E[σg,t2​]=h−N−1(h−2)σg2​​, E[σz,t2]=h(h−2)(hψ2+N−1)(h−N)(h−N−1)(h−N−3),E[σgz,t]=0,E[\sigma^2_{z,t}] = \frac{h(h-2)(h\psi^2+N-1)}{(h-N)(h-N-1)(h-N-3)},\quad E[\sigma_{gz,t}] = 0,E[σz,t2​]=(h−N)(h−N−1)(h−N−3)h(h−2)(hψ2+N−1)​,E[σgz,t​]=0,

together with the first and second moments of the auxiliary variables y1y_1y1​, y2y_2y2​ of Proposition 1 that the proof of Lemma 1 uses.

Significance

The result gives a closed-form, implementable-in-principle correction to the plug-in rule: since c~∗<1\tilde c^* < 1c~∗<1, the investor should always under-weight the estimated zero-investment portfolio, by a factor that depends only on hhh, NNN and ψ2\psi^2ψ2. Replacing ψ2\psi^2ψ2 by an adjusted estimator gives the paper's feasible rules (§2.4, §3), which are compared empirically in §4. The moment formulas (A9)–(A13) are of independent use: they give the exact out-of-sample mean and variance of the sample GMV and zero-investment portfolios, which recur in the shrinkage literature (for instance Lassance, Martín-Utrera and Simaan, 2024, who build on this paper's Proposition 1).

The result is proved in the paper, but the proof rests on Proposition 1, a stochastic representation of the out-of-sample moments whose detailed proof is in an online appendix. No machine-checked proof exists. On Prove2Me, Proposition 1 is posed (Open) as RiskEU.OOSUVar.kan_representation in Lassance et al.'s restatement, together with special cases (eq_IA60, eq_IA49) of the combinations μg,t+(κ/γ)μz,t\mu_{g,t} + (\kappa/\gamma)\mu_{z,t}μg,t​+(κ/γ)μz,t​ and of the portfolio variance for κ∈[0,1]\kappa \in [0, 1]κ∈[0,1] and h>N+7h > N + 7h>N+7. The closed-form vertex of the quadratic (17) is already proved there (RiskEU.RobustShrink.proposition_IA_1_3). What this mission adds is the statement about the actual expectation over the Gaussian sample, for all real c~\tilde cc~, under the paper's own threshold h>N+3h > N + 3h>N+3, with uniqueness of the maximizer.

Difficulty

Once Lemma 1 is available, the goal is the vertex of a concave quadratic. The difficulty is Lemma 1 itself: computing expectations of quadratic forms in Σ^t−1\hat\Sigma_t^{-1}Σ^t−1​ and in the normalized vector Σ^t−11N/(1N′Σ^t−11N)\hat\Sigma_t^{-1}1_N/(1_N'\hat\Sigma_t^{-1}1_N)Σ^t−1​1N​/(1N′​Σ^t−1​1N​). The weights are ratios of dependent random quantities, so linearity of expectation does not apply directly, and inverse-Wishart moment formulas alone do not cover the ratio in w^g,t\hat w_{g,t}w^g,t​. The threshold h>N+3h > N + 3h>N+3 is Lemma 1's hypothesis; the factor h−N−3h-N-3h−N−3 in the denominator of (A12) shows that it is what keeps the expected variance of the estimated zero-investment portfolio finite, so integrability is part of the content.

Formalization scope

The model is the published definition RiskEU.OOSUVar.Setting: Market N carries μ\muμ, Σ\SigmaΣ, γ\gammaγ; sigmaG2, muG, psi2, U, sampleMean, sampleCov (divided by hhh), wHatG, wHatZ and IsGaussianSample are the objects above (that setting calls the window TTT; here it is hhh). The auxiliary family of Proposition 1 and y1y_1y1​, y2y_2y2​ come from the published RiskEU.OOSUVar.KanRepresentation. The mission's own definitions (KanCombine.Optimal.Model) add the standing assumptions, the combining portfolio, the five sample moments, the expected utility, kkk and c~∗\tilde c^*c~∗.

Conventions committed to:

  • N≥2N \ge 2N≥2, Σ≻0\Sigma \succ 0Σ≻0 and γ>0\gamma > 0γ>0 are explicit hypotheses (implicit in the paper); h>N+3h > N + 3h>N+3 is Lemma 1's. The yyy-moment milestone also assumes N>3N > 3N>3, as Proposition 1 does.
  • c~\tilde cc~ ranges over all of R\mathbb RR, and "the optimal value" is stated as a unique maximizer.
  • Every expectation identity asserts integrability: a Lean Bochner integral of a non-integrable function is 000.
  • Lean's matrix inverse is 000 on singular matrices; Σ^t\hat\Sigma_tΣ^t​ is almost surely nonsingular for h>Nh > Nh>N, so this does not change any expectation.
  • The page's "0<c~∗<10 < \tilde c^* < 10<c~∗<1" fails at ψ2=0\psi^2 = 0ψ2=0, where c~∗=0\tilde c^* = 0c~∗=0; the goal states 0≤c~∗<10 \le \tilde c^* < 10≤c~∗<1 and c~∗>0\tilde c^* > 0c~∗>0 under ψ2>0\psi^2 > 0ψ2>0.

The goal is about the integral over the Gaussian sample. Stating it about the closed-form right-hand side of (17) would reduce it to the vertex of a quadratic, which is already proved, and is ruled out. The hypotheses are satisfiable: N=2N = 2N=2, h=6h = 6h=6, μ=(0,1)\mu = (0, 1)μ=(0,1), Σ=I\Sigma = IΣ=I, γ=1\gamma = 1γ=1 meets them with the product Gaussian sample, and gives c~∗=1/8\tilde c^* = 1/8c~∗=1/8.

A complete development needs Wishart and inverse-Wishart theory (the Bartlett decomposition, moments of chi-squared ratios) and a formal version of Proposition 1. These are reusable well beyond this mission; contributions proving (A9)–(A13) by any route, including directly from inverse-Wishart moments, are welcome.

Selected references

  • R. Kan, X. Wang and G. Zhou, Optimal portfolio choice with estimation risk: No risk-free asset case, Management Science 68(3), 2022 (cited from the submitted manuscript, November 2020). https://doi.org/10.1287/mnsc.2021.3989 ; https://ssrn.com/abstract=2819254
  • R. Kan and G. Zhou, Optimal portfolio choice with parameter uncertainty, Journal of Financial and Quantitative Analysis 42(3), 2007. https://doi.org/10.1017/S0022109000004129
  • H. Markowitz, Portfolio selection, Journal of Finance 7(1), 1952. https://doi.org/10.1111/j.1540-6261.1952.tb01525.x
  • N. Lassance, A. Martín-Utrera and M. Simaan, The risk of expected utility under parameter uncertainty, Management Science, 2024. https://doi.org/10.1287/mnsc.2023.00178
  • R. J. Muirhead, Aspects of Multivariate Statistical Theory, Wiley, 1982. https://doi.org/10.1002/9780470316559
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Quantum Information·Captain: Goku

A provable quantum advantage for approximate optimization via decoded quantum interferometryResearch Paper

Motivation

A provable quantum advantage for approximate optimization via decoded quantum interferometry establishes the selected mathematical guarantees below. The mission turns those original paper results into precise Lean proof targets.

Setting

Fix a rational rate R∈(0,1)R\in(0,1)R∈(0,1). An admissible block count M>0M>0M>0 satisfies M+1=2uM+1=2^uM+1=2u for an integer u>0u>0u>0, and K=⌊RN⌋≥hK=\lfloor RN\rfloor\ge hK=⌊RN⌋≥h, where h=M+2h=M+2h=M+2, N=hMN=hMN=hM and q=N+1=(M+1)2q=N+1=(M+1)^2q=N+1=(M+1)2. Work over the publicly represented characteristic-two field Fq\mathbb F_qFq​, with a fixed public primitive element γ\gammaγ. Put J=⌊K/h⌋J=\lfloor K/h\rfloorJ=⌊K/h⌋ and Σ=Fqh\Sigma=\mathbb F_q^hΣ=Fqh​. A promised instance consists of arbitrary sets Ai⊆ΣA_i\subseteq\SigmaAi​⊆Σ with ∣Ai∣=∣Σ∣/2|A_i|=|\Sigma|/2∣Ai​∣=∣Σ∣/2, accessed only through separately callable fixed-block XOR membership oracles. Each call chooses its block classically and may query a superposition of whole symbols.

A coefficient vector x∈FqKx\in\mathbb F_q^Kx∈FqK​ represents the polynomial Qx(Y)=∑j=0K−1xjYjQ_x(Y)=\sum_{j=0}^{K-1}x_jY^jQx​(Y)=∑j=0K−1​xj​Yj, including the zero polynomial. Its score is

score⁡A(Qx)=1M∑i=0M−11 ⁣[(Qx(γih+j))j=0h−1∈Ai].\operatorname{score}_{\mathcal A}(Q_x)=\frac1M\sum_{i=0}^{M-1} \mathbf1\!\left[(Q_x(\gamma^{ih+j}))_{j=0}^{h-1}\in A_i\right].scoreA​(Qx​)=M1​i=0∑M−1​1[(Qx​(γih+j))j=0h−1​∈Ai​].

Define

αC(R)=1+R2,αQ(R)=1+R(2−R)2.\alpha_C(R)=\frac{1+R}{2},\qquad \alpha_Q(R)=\frac{1+\sqrt{R(2-R)}}2.αC​(R)=21+R​,αQ​(R)=21+R(2−R)​​.
  1. There is a uniform quantum polynomial-time DQI family using one query to each fixed-block oracle, at most MMM queries in total. Its expected score converges to αQ(R)\alpha_Q(R)αQ​(R) uniformly over every promised instance:
∀ϵ>0 ∃M0 ∀ admissible M≥M0 ∀A,∣E[score⁡A(QDQI)]−αQ(R)∣≤ϵ.\forall\epsilon>0\ \exists M_0\ \forall\text{ admissible }M\ge M_0\ \forall\mathcal A,\quad \left|\mathbb E[\operatorname{score}_{\mathcal A}(Q_{\rm DQI})]-\alpha_Q(R)\right|\le\epsilon.∀ϵ>0 ∃M0​ ∀ admissible M≥M0​ ∀A,∣E[scoreA​(QDQI​)]−αQ​(R)∣≤ϵ.

The construction uses the conventional unfolded scalar GRS dual syndrome decoder at cutoff ℓ=⌊(J−1)/2⌋\ell=\lfloor(J-1)/2\rfloorℓ=⌊(J−1)/2⌋, strictly below half its scalar minimum distance, the explicit top-window layer weights, and synthesis accuracy M−2M^{-2}M−2. Its polynomial resource bounds and classical circuit constructor are independent of the acceptance sets.

  1. A randomized polynomial-time implementation of Prange's information-set algorithm makes at most 4M4M4M membership queries in the worst case. It samples uniformly with replacement until obtaining accepted targets in the first JJJ blocks, interpolates their hJhJhJ evaluations, and returns zero if the total trial cap is exhausted. When the sets AiA_iAi​ are sampled independently and uniformly among half-size subsets, independently of the algorithm's randomness,
∀ϵ,δ>0 ∃M0 ∀ admissible M≥M0,Pr⁡ ⁣[∣score⁡(QPrange)−αC(R)∣>ϵ]≤δ.\forall\epsilon,\delta>0\ \exists M_0\ \forall\text{ admissible }M\ge M_0,\quad \Pr\!\left[\left|\operatorname{score}(Q_{\rm Prange})-\alpha_C(R)\right|>\epsilon\right]\le\delta.∀ϵ,δ>0 ∃M0​ ∀ admissible M≥M0​,Pr[∣score(QPrange​)−αC​(R)∣>ϵ]≤δ.
  1. For each fixed 0<η<1−αC(R)0<\eta<1-\alpha_C(R)0<η<1−αC​(R), there are θ,c>0\theta,c>0θ,c>0 and M0≥2M_0\ge2M0​≥2, depending only on R,ηR,\etaR,η, such that every admissible M≥M0M\ge M_0M≥M0​ and every randomized classical algorithm with worst-case query budget T≤exp⁡(θM/log⁡M)T\le\exp(\theta M/\log M)T≤exp(θM/logM) satisfy
Pr⁡[score⁡(A(ω))≥αC(R)+η]≤e−cM.\Pr[\operatorname{score}(A(\omega))\ge\alpha_C(R)+\eta]\le e^{-cM}.Pr[score(A(ω))≥αC​(R)+η]≤e−cM.

The probability is over the same sampled acceptance sets and independent algorithm randomness. Computation between queries and arbitrary finite advice are unrestricted, provided the description and advice are fixed before sampling.

This result separates the approximation scores attainable through the same whole-symbol membership interface. The quantum assertion is an expectation guarantee for every promised oracle; the classical assertions are distributional.

Formalization Note A fixed effective polynomial-basis binary field representation and uniform compilation over {H,T,CNOT}\{H,T,\mathrm{CNOT}\}{H,T,CNOT} make the implicit public representation and polynomial runtime concrete. The DQI state, its coefficient output wires and its query count are tied to one circuit. The sampled probabilities are finite uniform averages of normalized classical output laws.

Target

Theorem 1 (continues on PDF p.16)

Fix a rational rate R∈(0,1)R\in(0,1)R∈(0,1). An admissible block count M>0M>0M>0 satisfies M+1=2uM+1=2^uM+1=2u for an integer u>0u>0u>0, and K=⌊RN⌋≥hK=\lfloor RN\rfloor\ge hK=⌊RN⌋≥h, where h=M+2h=M+2h=M+2, N=hMN=hMN=hM and q=N+1=(M+1)2q=N+1=(M+1)^2q=N+1=(M+1)2. Work over the publicly represented characteristic-two field Fq\mathbb F_qFq​, with a fixed public primitive element γ\gammaγ. Put J=⌊K/h⌋J=\lfloor K/h\rfloorJ=⌊K/h⌋ and Σ=Fqh\Sigma=\mathbb F_q^hΣ=Fqh​. A promised instance consists of arbitrary sets Ai⊆ΣA_i\subseteq\SigmaAi​⊆Σ with ∣Ai∣=∣Σ∣/2|A_i|=|\Sigma|/2∣Ai​∣=∣Σ∣/2, accessed only through separately callable fixed-block XOR membership oracles. Each call chooses its block classically and may query a superposition of whole symbols.

A coefficient vector x∈FqKx\in\mathbb F_q^Kx∈FqK​ represents the polynomial Qx(Y)=∑j=0K−1xjYjQ_x(Y)=\sum_{j=0}^{K-1}x_jY^jQx​(Y)=∑j=0K−1​xj​Yj, including the zero polynomial. Its score is

score⁡A(Qx)=1M∑i=0M−11 ⁣[(Qx(γih+j))j=0h−1∈Ai].\operatorname{score}_{\mathcal A}(Q_x)=\frac1M\sum_{i=0}^{M-1} \mathbf1\!\left[(Q_x(\gamma^{ih+j}))_{j=0}^{h-1}\in A_i\right].scoreA​(Qx​)=M1​i=0∑M−1​1[(Qx​(γih+j))j=0h−1​∈Ai​].

Define

αC(R)=1+R2,αQ(R)=1+R(2−R)2.\alpha_C(R)=\frac{1+R}{2},\qquad \alpha_Q(R)=\frac{1+\sqrt{R(2-R)}}2.αC​(R)=21+R​,αQ​(R)=21+R(2−R)​​.
  1. There is a uniform quantum polynomial-time DQI family using one query to each fixed-block oracle, at most MMM queries in total. Its expected score converges to αQ(R)\alpha_Q(R)αQ​(R) uniformly over every promised instance:
∀ϵ>0 ∃M0 ∀ admissible M≥M0 ∀A,∣E[score⁡A(QDQI)]−αQ(R)∣≤ϵ.\forall\epsilon>0\ \exists M_0\ \forall\text{ admissible }M\ge M_0\ \forall\mathcal A,\quad \left|\mathbb E[\operatorname{score}_{\mathcal A}(Q_{\rm DQI})]-\alpha_Q(R)\right|\le\epsilon.∀ϵ>0 ∃M0​ ∀ admissible M≥M0​ ∀A,∣E[scoreA​(QDQI​)]−αQ​(R)∣≤ϵ.

The construction uses the conventional unfolded scalar GRS dual syndrome decoder at cutoff ℓ=⌊(J−1)/2⌋\ell=\lfloor(J-1)/2\rfloorℓ=⌊(J−1)/2⌋, strictly below half its scalar minimum distance, the explicit top-window layer weights, and synthesis accuracy M−2M^{-2}M−2. Its polynomial resource bounds and classical circuit constructor are independent of the acceptance sets.

  1. A randomized polynomial-time implementation of Prange's information-set algorithm makes at most 4M4M4M membership queries in the worst case. It samples uniformly with replacement until obtaining accepted targets in the first JJJ blocks, interpolates their hJhJhJ evaluations, and returns zero if the total trial cap is exhausted. When the sets AiA_iAi​ are sampled independently and uniformly among half-size subsets, independently of the algorithm's randomness,
∀ϵ,δ>0 ∃M0 ∀ admissible M≥M0,Pr⁡ ⁣[∣score⁡(QPrange)−αC(R)∣>ϵ]≤δ.\forall\epsilon,\delta>0\ \exists M_0\ \forall\text{ admissible }M\ge M_0,\quad \Pr\!\left[\left|\operatorname{score}(Q_{\rm Prange})-\alpha_C(R)\right|>\epsilon\right]\le\delta.∀ϵ,δ>0 ∃M0​ ∀ admissible M≥M0​,Pr[∣score(QPrange​)−αC​(R)∣>ϵ]≤δ.
  1. For each fixed 0<η<1−αC(R)0<\eta<1-\alpha_C(R)0<η<1−αC​(R), there are θ,c>0\theta,c>0θ,c>0 and M0≥2M_0\ge2M0​≥2, depending only on R,ηR,\etaR,η, such that every admissible M≥M0M\ge M_0M≥M0​ and every randomized classical algorithm with worst-case query budget T≤exp⁡(θM/log⁡M)T\le\exp(\theta M/\log M)T≤exp(θM/logM) satisfy
Pr⁡[score⁡(A(ω))≥αC(R)+η]≤e−cM.\Pr[\operatorname{score}(A(\omega))\ge\alpha_C(R)+\eta]\le e^{-cM}.Pr[score(A(ω))≥αC​(R)+η]≤e−cM.

The probability is over the same sampled acceptance sets and independent algorithm randomness. Computation between queries and arbitrary finite advice are unrestricted, provided the description and advice are fixed before sampling.

This result separates the approximation scores attainable through the same whole-symbol membership interface. The quantum assertion is an expectation guarantee for every promised oracle; the classical assertions are distributional.

Formalization Note A fixed effective polynomial-basis binary field representation and uniform compilation over {H,T,CNOT}\{H,T,\mathrm{CNOT}\}{H,T,CNOT} make the implicit public representation and polynomial runtime concrete. The DQI state, its coefficient output wires and its query count are tied to one circuit. The sampled probabilities are finite uniform averages of normalized classical output laws.

Significance

These are known results from the cited paper. The current contribution consists of source-reviewed, compiler-checked theorem statements and mathematical definitions. Formal proofs remain open. Only the listed selected results are in scope; no whole-paper completeness is claimed.

Difficulty

A complete solution must establish every quantified conclusion under the exact stated hypotheses, including error, probability and resource conditions wherever present. The source assumptions and conventions are recorded in the attached statements and independent readbacks.

Formalization scope

Definitions preserve the existing reviewed Lean interfaces. Every target proof is currently sorry, so each target is Open. Printed-source corrections, where necessary, are labeled with the printed claim, the change and its reason.

Selected references

  • A provable quantum advantage for approximate optimization via decoded quantum interferometry, arXiv:2610.02145v2. Exact result labels, PDF pages and source SHA-256 values accompany each theorem.
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Quantum Information·Captain: Goku

An Optimal Quantum Linear Systems AlgorithmResearch Paper

Motivation

An Optimal Quantum Linear Systems Algorithm establishes the selected mathematical guarantees below. The mission turns those original paper results into precise Lean proof targets.

Setting

Consider the quantum linear systems problem for an invertible, complex, ddd-sparse N×NN\times NN×N matrix AAA, with 1≤d≤N1\le d\le N1≤d≤N, ∥A∥≤1\|A\|\le1∥A∥≤1, and ∥A−1∥≤κ\|A^{-1}\|\le\kappa∥A−1∥≤κ, where these are operator norms and κ\kappaκ is known. For a nonzero vector bbb, a supplied preparation circuit prepares ∣b⟩=b/∥b∥|b\rangle=b/\|b\|∣b⟩=b/∥b∥. The solver must output a success flag of probability at least 1/21/21/2 and, conditioned on success, a normalized reduced density matrix within trace distance ϵ\epsilonϵ of ∣x⟩⟨x∣|x\rangle\langle x|∣x⟩⟨x∣, where ∣x⟩=A−1b/∥A−1b∥|x\rangle=A^{-1}b/\|A^{-1}b\|∣x⟩=A−1b/∥A−1b∥. Both AAA and A†A^\daggerA† have reversible row-location and XOR entry-value oracles; the ddd locations listed in each row are distinct, cover all nonzeros, and may include zeros. Only matrix-oracle calls count, including inverse and controlled calls. Supplied preparation operations and known quantum operations are free.

Let Q(d,κ,ϵ)Q(d,\kappa,\epsilon)Q(d,κ,ϵ) be the supremum over positive dimensions N≥dN\ge dN≥d and public finite exact entry encodings of the least natural worst-case matrix-query budget of a solver correct for every compatible promised input and oracle completion. Solvers are chosen before the hidden matrix, vector, and oracle completions. Empty sets of feasible budgets and unbounded suprema retain +∞+\infty+∞. There exist absolute constants c,C>0c,C>0c,C>0, κ0≥1\kappa_0\ge1κ0​≥1, d0≥1d_0\ge1d0​≥1, and 0<ϵ0<10<\epsilon_0<10<ϵ0​<1 such that, for every κ≥κ0\kappa\ge\kappa_0κ≥κ0​, d≥d0d\ge d_0d≥d0​, and 0<ϵ≤ϵ00<\epsilon\le\epsilon_00<ϵ≤ϵ0​,

cκdlog⁡(1/ϵ)≤Q(d,κ,ϵ)≤Cκdlog⁡(1/ϵ).c\kappa\sqrt d\log(1/\epsilon)\le Q(d,\kappa,\epsilon)\le C\kappa\sqrt d\log(1/\epsilon).cκd​log(1/ϵ)≤Q(d,κ,ϵ)≤Cκd​log(1/ϵ).

This gives matching upper and worst-case lower bounds jointly in sparsity, inverse-norm bound, and precision. The constants and thresholds are independent of dimension, encoding, and input.

Formalization Note Complexity is represented in R≥0∪{+∞}\mathbb R_{\ge0}\cup\{+\infty\}R≥0​∪{+∞} using the frozen OptimalQLSP.queryComplexity. General matrices and general positive dimensions are retained; the Hermitian reduction and power-of-two registers used inside the proof do not restrict the headline.

Target

Theorem 1, equation (6)

Consider the quantum linear systems problem for an invertible, complex, ddd-sparse N×NN\times NN×N matrix AAA, with 1≤d≤N1\le d\le N1≤d≤N, ∥A∥≤1\|A\|\le1∥A∥≤1, and ∥A−1∥≤κ\|A^{-1}\|\le\kappa∥A−1∥≤κ, where these are operator norms and κ\kappaκ is known. For a nonzero vector bbb, a supplied preparation circuit prepares ∣b⟩=b/∥b∥|b\rangle=b/\|b\|∣b⟩=b/∥b∥. The solver must output a success flag of probability at least 1/21/21/2 and, conditioned on success, a normalized reduced density matrix within trace distance ϵ\epsilonϵ of ∣x⟩⟨x∣|x\rangle\langle x|∣x⟩⟨x∣, where ∣x⟩=A−1b/∥A−1b∥|x\rangle=A^{-1}b/\|A^{-1}b\|∣x⟩=A−1b/∥A−1b∥. Both AAA and A†A^\daggerA† have reversible row-location and XOR entry-value oracles; the ddd locations listed in each row are distinct, cover all nonzeros, and may include zeros. Only matrix-oracle calls count, including inverse and controlled calls. Supplied preparation operations and known quantum operations are free.

Let Q(d,κ,ϵ)Q(d,\kappa,\epsilon)Q(d,κ,ϵ) be the supremum over positive dimensions N≥dN\ge dN≥d and public finite exact entry encodings of the least natural worst-case matrix-query budget of a solver correct for every compatible promised input and oracle completion. Solvers are chosen before the hidden matrix, vector, and oracle completions. Empty sets of feasible budgets and unbounded suprema retain +∞+\infty+∞. There exist absolute constants c,C>0c,C>0c,C>0, κ0≥1\kappa_0\ge1κ0​≥1, d0≥1d_0\ge1d0​≥1, and 0<ϵ0<10<\epsilon_0<10<ϵ0​<1 such that, for every κ≥κ0\kappa\ge\kappa_0κ≥κ0​, d≥d0d\ge d_0d≥d0​, and 0<ϵ≤ϵ00<\epsilon\le\epsilon_00<ϵ≤ϵ0​,

cκdlog⁡(1/ϵ)≤Q(d,κ,ϵ)≤Cκdlog⁡(1/ϵ).c\kappa\sqrt d\log(1/\epsilon)\le Q(d,\kappa,\epsilon)\le C\kappa\sqrt d\log(1/\epsilon).cκd​log(1/ϵ)≤Q(d,κ,ϵ)≤Cκd​log(1/ϵ).

This gives matching upper and worst-case lower bounds jointly in sparsity, inverse-norm bound, and precision. The constants and thresholds are independent of dimension, encoding, and input.

Formalization Note Complexity is represented in R≥0∪{+∞}\mathbb R_{\ge0}\cup\{+\infty\}R≥0​∪{+∞} using the frozen OptimalQLSP.queryComplexity. General matrices and general positive dimensions are retained; the Hermitian reduction and power-of-two registers used inside the proof do not restrict the headline.

Significance

These are known results from the cited paper. The current contribution consists of source-reviewed, compiler-checked theorem statements and mathematical definitions. Formal proofs remain open. Only the listed selected results are in scope; no whole-paper completeness is claimed.

Difficulty

A complete solution must establish every quantified conclusion under the exact stated hypotheses, including error, probability and resource conditions wherever present. The source assumptions and conventions are recorded in the attached statements and independent readbacks.

Formalization scope

Definitions preserve the existing reviewed Lean interfaces. Every target proof is currently sorry, so each target is Open. Printed-source corrections, where necessary, are labeled with the printed claim, the change and its reason.

Selected references

  • An Optimal Quantum Linear Systems Algorithm, arXiv:2609.35660v1. Exact result labels, PDF pages and source SHA-256 values accompany each theorem.
1 thm1 active userReviewed
Machine LearningQuantum Information·Captain: Goku

Sample-optimal learning of stabilizer statesResearch Paper

Motivation

Sample-optimal learning of stabilizer states establishes the selected mathematical guarantees below. The mission turns those original paper results into precise Lean proof targets.

Setting

Let n≥1n\ge 1n≥1 be the number of qubits and let 0<δ<1/80<\delta<1/80<δ<1/8 be the allowed failure probability. An unknown normalized pure stabilizer state ∣ψ⟩|\psi\rangle∣ψ⟩ is provided as identical copies. Let Lδ(n)L_\delta(n)Lδ​(n) be the least number of copies with which one quantum procedure can identify every such state with probability at least 1−δ1-\delta1−δ. The minimum permits arbitrary collective measurements, ancillas, internal randomness and adaptivity. Identification means outputting a valid tableau of nnn independent signed Pauli generators whose common +1+1+1 eigenspace is the input state; global phase and the choice of generators are irrelevant. Then

n+⌈log⁡21δ⌉−3≤Lδ(n)≤n+⌈log⁡21δ⌉+4.n+\left\lceil\log_2\frac1\delta\right\rceil-3 \le L_\delta(n)\le n+\left\lceil\log_2\frac1\delta\right\rceil+4.n+⌈log2​δ1​⌉−3≤Lδ​(n)≤n+⌈log2​δ1​⌉+4.

Furthermore, for every such nnn and δ\deltaδ, there is a quantum learner receiving at most n+⌈log⁡2(1/δ)⌉+4n+\lceil\log_2(1/\delta)\rceil+4n+⌈log2​(1/δ)⌉+4 copies and retaining them through adaptive operations, which identifies every input stabilizer state with failure probability at most δ\deltaδ. There are absolute constants C>0C>0C>0 and s0≥1s_0\ge1s0​≥1, independent of nnn, δ\deltaδ and the input state, such that this learner has computational time

time⁡≤Cn(n+ln⁡(1/δ))4whenever n+ln⁡(1/δ)≥s0.\operatorname{time}\le Cn\bigl(n+\ln(1/\delta)\bigr)^4 \qquad\text{whenever }n+\ln(1/\delta)\ge s_0.time≤Cn(n+ln(1/δ))4whenever n+ln(1/δ)≥s0​.

Time counts elementary quantum gates, measurements, fair coins and Boolean operations, including classical and reversible arithmetic, finite-precision rotation synthesis and tableau reconstruction. The sample and success bounds have no asymptotic threshold. This determines the leading sample coefficient to be one and attains the bound with an efficient learner.

Formalization Note The minimum is represented in N∪{∞}\mathbb N\cup\{\infty\}N∪{∞}, with an empty feasible set assigned ∞\infty∞; the upper bound implies finiteness. The lower inequality is written as n+⌈log⁡2(1/δ)⌉≤Lδ(n)+3n+\lceil\log_2(1/\delta)\rceil\le L_\delta(n)+3n+⌈log2​(1/δ)⌉≤Lδ​(n)+3 to avoid natural subtraction. The theorem's printed statement leaves the qubit domain implicit; n≥1n\ge1n≥1 follows the lower-bound proof on PDF p.7, since the zero-qubit state requires zero copies.

Target

Theorem 1

Let n≥1n\ge 1n≥1 be the number of qubits and let 0<δ<1/80<\delta<1/80<δ<1/8 be the allowed failure probability. An unknown normalized pure stabilizer state ∣ψ⟩|\psi\rangle∣ψ⟩ is provided as identical copies. Let Lδ(n)L_\delta(n)Lδ​(n) be the least number of copies with which one quantum procedure can identify every such state with probability at least 1−δ1-\delta1−δ. The minimum permits arbitrary collective measurements, ancillas, internal randomness and adaptivity. Identification means outputting a valid tableau of nnn independent signed Pauli generators whose common +1+1+1 eigenspace is the input state; global phase and the choice of generators are irrelevant. Then

n+⌈log⁡21δ⌉−3≤Lδ(n)≤n+⌈log⁡21δ⌉+4.n+\left\lceil\log_2\frac1\delta\right\rceil-3 \le L_\delta(n)\le n+\left\lceil\log_2\frac1\delta\right\rceil+4.n+⌈log2​δ1​⌉−3≤Lδ​(n)≤n+⌈log2​δ1​⌉+4.

Furthermore, for every such nnn and δ\deltaδ, there is a quantum learner receiving at most n+⌈log⁡2(1/δ)⌉+4n+\lceil\log_2(1/\delta)\rceil+4n+⌈log2​(1/δ)⌉+4 copies and retaining them through adaptive operations, which identifies every input stabilizer state with failure probability at most δ\deltaδ. There are absolute constants C>0C>0C>0 and s0≥1s_0\ge1s0​≥1, independent of nnn, δ\deltaδ and the input state, such that this learner has computational time

time⁡≤Cn(n+ln⁡(1/δ))4whenever n+ln⁡(1/δ)≥s0.\operatorname{time}\le Cn\bigl(n+\ln(1/\delta)\bigr)^4 \qquad\text{whenever }n+\ln(1/\delta)\ge s_0.time≤Cn(n+ln(1/δ))4whenever n+ln(1/δ)≥s0​.

Time counts elementary quantum gates, measurements, fair coins and Boolean operations, including classical and reversible arithmetic, finite-precision rotation synthesis and tableau reconstruction. The sample and success bounds have no asymptotic threshold. This determines the leading sample coefficient to be one and attains the bound with an efficient learner.

Formalization Note The minimum is represented in N∪{∞}\mathbb N\cup\{\infty\}N∪{∞}, with an empty feasible set assigned ∞\infty∞; the upper bound implies finiteness. The lower inequality is written as n+⌈log⁡2(1/δ)⌉≤Lδ(n)+3n+\lceil\log_2(1/\delta)\rceil\le L_\delta(n)+3n+⌈log2​(1/δ)⌉≤Lδ​(n)+3 to avoid natural subtraction. The theorem's printed statement leaves the qubit domain implicit; n≥1n\ge1n≥1 follows the lower-bound proof on PDF p.7, since the zero-qubit state requires zero copies.

Significance

These are known results from the cited paper. The current contribution consists of source-reviewed, compiler-checked theorem statements and mathematical definitions. Formal proofs remain open. Only the listed selected results are in scope; no whole-paper completeness is claimed.

Difficulty

A complete solution must establish every quantified conclusion under the exact stated hypotheses, including error, probability and resource conditions wherever present. The source assumptions and conventions are recorded in the attached statements and independent readbacks.

Formalization scope

Definitions preserve the existing reviewed Lean interfaces. Every target proof is currently sorry, so each target is Open. Printed-source corrections, where necessary, are labeled with the printed claim, the change and its reason.

Selected references

  • Sample-optimal learning of stabilizer states, arXiv:2609.10974v1. Exact result labels, PDF pages and source SHA-256 values accompany each theorem.
1 thm1 active userReviewed
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