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Algorithmic Game TheoryComplexity TheoryTheoretical Computer Science·Captain: mikedeng1

Anyone but Him: The Complexity of Precluding an Alternative: Control by Partition of Voters Is Vulnerable or NP-Complete for Plurality, Condorcet and Approval Voting, Depending on Tie-HandlingResearch Paper

Why election control is studied

An election is run by someone — a chair, a committee, an organiser — who can shape it without touching a single ballot: by deciding which candidates appear, which voters are registered, or how the electorate is split into bodies that pre-select nominees. Bartholdi, Tovey and Trick (1992) proposed to measure how well a voting rule protects itself against such manipulation by the computational difficulty of finding a successful manipulation: a rule for which the chair's problem is NP-complete is resistant, one for which it is solvable in polynomial time is vulnerable. They studied constructive control, where the chair wants a given candidate to become the unique winner.

Hemaspaandra, Hemaspaandra and Rothe (arXiv:cs/0507027, Artificial Intelligence 171, 2007) introduced destructive control: the chair wants a despised candidate not to be the unique winner ("anyone but him"). They classified plurality, Condorcet and approval voting under seven control types in both settings. This mission formalizes the last of their main results, Theorem 3.6, on control by partition of voters.

Timeline:

  • 1992: Bartholdi, Tovey and Trick define constructive control and its complexity for plurality and Condorcet; for partition of voters they use a model in which ties in subcommittees are forbidden.
  • 2005–2007: Hemaspaandra, Hemaspaandra and Rothe add destructive control, approval voting, and the two tie-handling models below.
  • 2026: version v5 of the paper adds Appendix A, a corrected proof of the TP case of Theorem 4.21.

Setting

An election has candidates C={0,…,m−1}C=\{0,\dots,m-1\}C={0,…,m−1} and voters V={0,…,n−1}V=\{0,\dots,n-1\}V={0,…,n−1}, each casting a ballot. For plurality and Condorcet voting a ballot is a strict ranking of CCC; for approval voting it is the set of candidates the voter approves of. The election (D,U)(D,U)(D,U), with candidates D⊆CD\subseteq CD⊆C and voters U⊆VU\subseteq VU⊆V, reads each ballot through the preferences it induces on DDD. Its winner set W(D,U)W(D,U)W(D,U) is:

  • plurality: the candidates of DDD ranked first among DDD by a maximum number of voters of UUU;
  • Condorcet: the x∈Dx\in Dx∈D that beat every other y∈Dy\in Dy∈D in the pairwise election, #{v∈U:x≻vy}>#{v∈U:y≻vx}\#\{v\in U: x\succ_v y\}>\#\{v\in U: y\succ_v x\}#{v∈U:x≻v​y}>#{v∈U:y≻v​x} (at most one candidate; possibly none);
  • approval: the candidates of DDD approved by a maximum number of voters of UUU.

In control by partition of voters the chair splits VVV into two subcommittees V1V_1V1​ and V2=V∖V1V_2=V\setminus V_1V2​=V∖V1​ (either may be empty). Each subcommittee holds the subelection (C,Vi)(C,V_i)(C,Vi​) and nominates candidates. Under Ties-Promote (TP) it nominates all its winners; under Ties-Eliminate (TE) it nominates its winner if there is exactly one and nobody otherwise. The two-stage election then is

twoStage(V1)=W(N(V1)∪N(V2), V),\mathrm{twoStage}(V_1)=W\bigl(N(V_1)\cup N(V_2),\,V\bigr),twoStage(V1​)=W(N(V1​)∪N(V2​),V),

the nominees running against each other before all voters. Given (C,c,V)(C,c,V)(C,c,V), the constructive problem asks whether some partition gives twoStage(V1)={c}\mathrm{twoStage}(V_1)=\{c\}twoStage(V1​)={c}, the destructive problem whether some partition gives twoStage(V1)≠{c}\mathrm{twoStage}(V_1)\neq\{c\}twoStage(V1​)={c}.

Definition 3.1 of the paper: a rule is susceptible to a control type if in some election the chair can change ccc from not being the unique winner to being it (constructive), or from being the unique winner to not being it (destructive). It is vulnerable if it is susceptible and the problem's language is in P; certifiably-vulnerable if it is susceptible and a successful partition can be computed in polynomial time; resistant if it is susceptible and the language is NP-complete.

Formalization targets

Goal: Theorem 3.6

With Hitting Set and Exact Cover by Three-Sets NP-complete (the two facts the paper takes from Garey and Johnson),

approval: resistant (CC, TE and TP); vulnerable and certifiably-vulnerable (DC, TE and TP);plurality: vulnerable and certifiably-vulnerable (CC and DC, TE); resistant (CC and DC, TP);Condorcet: vulnerable and certifiably-vulnerable (DC).\begin{aligned} &\text{approval: resistant (CC, TE and TP);\ vulnerable and certifiably-vulnerable (DC, TE and TP);}\\ &\text{plurality: vulnerable and certifiably-vulnerable (CC and DC, TE);\ resistant (CC and DC, TP);}\\ &\text{Condorcet: vulnerable and certifiably-vulnerable (DC).} \end{aligned}​approval: resistant (CC, TE and TP); vulnerable and certifiably-vulnerable (DC, TE and TP);plurality: vulnerable and certifiably-vulnerable (CC and DC, TE); resistant (CC and DC, TP);Condorcet: vulnerable and certifiably-vulnerable (DC).​

Nine clauses, each including its susceptibility part.

Milestones

  1. Susceptibility witnesses: Examples 4.9, 4.10, 4.11, 4.16, 4.17.
  2. Polynomial-time algorithms: Theorems 4.18 and 4.19 (plurality, TE), 4.20 (Condorcet), 4.21 (approval, destructive, TE and TP).
  3. Plurality TP hardness: Claims 4.29 and 4.30 on Construction 4.28; Theorem 4.39 (Restricted Hitting Set is NP-complete); Claims 4.40 and 4.41; Corollary 4.42.
  4. Approval constructive hardness: Theorems 4.45 (TP) and 4.46 (TE), by reduction from X3C.

Significance

Theorem 3.6 is where the tie-handling model changes the classification: plurality is vulnerable under TE and resistant under TP, for both constructive and destructive control. Under TE at most one candidate leaves each subcommittee; under TP any set of tied candidates may advance. The theorem also shows that approval and Condorcet, which resist constructive control by partition of voters, are vulnerable to its destructive form. Results of this kind underlie the comparison tables of the later control literature (Faliszewski, Hemaspaandra and Hemaspaandra, Control and bribery in voting, 2016).

The paper's proofs are combinatorial algorithms and many-one reductions, stated informally. No part of the paper has been machine-checked. A formal development produces:

  • the elections, winner sets on candidate subsets, and the two-stage election, in a form reusable for the other control types of the paper (adding, deleting and partitioning candidates or voters);
  • verified polynomial-time algorithms on Cook's Turing-machine model. Several of the printed algorithms have gaps, including the TP case of Theorem 4.21 that the authors corrected in v5, so a checked version settles their correctness;
  • verified reductions from Hitting Set and X3C.

Difficulty

The algorithmic clauses need more than correctness of a decision procedure: membership in P and polynomial-time computability are statements about a one-tape Turing machine reading binary codes. An algorithm described by "for each candidate d, check …" has to be compiled to that model, and its running time bounded, which no existing library on the platform does for elections.

The plurality TE algorithms are case analyses: who can be nominated by each part, and how many first-place votes each candidate must surrender. The cases where ccc has no first-place vote, or where a subcommittee is empty, are exactly where the printed algorithms slip. The approval TP destructive algorithm was wrong as first published.

For the hardness clauses the reductions must be shown correct for every instance. Claim 4.41 needs an arithmetic padding condition, which is why the paper first proves Restricted Hitting Set NP-complete (Theorem 4.39) and then reduces from it. NP membership, which the paper calls obvious, still has to be proved in the checking-relation form of NP.

Formalization scope

  • Candidates are Fin m and voters Fin n, both possibly empty. A profile is Fin n → Ballot m, so the multiset of ballots is a list (one ballot per voter, as the paper assumes on p. 4).
  • A ranking is Equiv.Perm (Fin m), read as the position of each candidate. An approval ballot is a Finset.
  • Winner sets are computed on a candidate subset with the induced preferences. Every election with an empty candidate set has no winner, and an empty subcommittee ties all candidates at score zero.
  • A partition is V₁ : Finset (Fin n) and its complement.
  • Unique winner means the winner set equals {c}; an empty winner set is a destructive success.
  • P, NP-completeness and polynomial-time computability are the published CookPvsNP notions. Instance codes are lists of binary numbers over the published alphabet BSym: m,n,cm, n, cm,n,c, then the ballots.
  • A certificate function must return the code of a partition that works on every yes-instance and the fixed token "control impossible" (encNats [0]) on every no-instance.
  • Construction 4.28 is a predicate satisfied by every profile of the stated shape, whatever the "arbitrary" orders.
  • The only hypotheses are NP-completeness of Hitting Set (p. 24) and of X3C (p. 28), exactly as the paper states them. Both are true (Garey–Johnson SP8, SP2).

None of these is a trivializing reading. "In P" is a Turing-machine statement, not a Decidable instance. Every vulnerable or resistant clause carries its susceptibility part. A certifiable-vulnerability witness must output a successful partition, which is more than deciding the language.

Welcome contributions: proofs of the examples (finite computations), of Claims 4.29–4.41 (counting arguments), of NP membership of the control languages, and Turing-machine implementations of election-scoring primitives, which later missions can reuse.

Selected references

  • E. Hemaspaandra, L. A. Hemaspaandra, J. Rothe, Anyone but Him: The Complexity of Precluding an Alternative, Artificial Intelligence 171(5–6):255–285, 2007; arXiv:cs/0507027v5, 2026. https://arxiv.org/abs/cs/0507027 — DOI https://doi.org/10.1016/j.artint.2007.01.005
  • J. Bartholdi III, C. Tovey, M. Trick, How hard is it to control an election?, Mathematical and Computer Modelling 16(8–9):27–40, 1992. https://doi.org/10.1016/0895-7177(92)90085-Y
  • M. Garey, D. Johnson, Computers and Intractability: A Guide to the Theory of NP-Completeness, W. H. Freeman, 1979.
  • S. Cook, The P versus NP problem, Clay Mathematics Institute problem description. https://www.claymath.org/wp-content/uploads/2022/06/pvsnp.pdf
  • P. Faliszewski, E. Hemaspaandra, L. A. Hemaspaandra, Control and bribery in voting, in Handbook of Computational Social Choice, Cambridge University Press, 2016. https://doi.org/10.1017/CBO9781107446984.008
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ProbabilityQuantum InformationRepresentation Theory·Captain: mikedeng1

Estimating the spectrum of a density operator: Normalized Young Frames Y/N Converge to the Spectrum of ρ, with Large-Deviation Rate the Relative Entropy Σ s_j ln(s_j/r_j)Research Paper

Motivation

A density operator ρ\rhoρ on Cd\mathbb C^dCd describes a quantum system completely, but it cannot be read off a single copy: it has to be estimated from many identically prepared copies. Its spectrum r1≥⋯≥rd≥0r_1 \ge \dots \ge r_d \ge 0r1​≥⋯≥rd​≥0, ∑αrα=1\sum_\alpha r_\alpha = 1∑α​rα​=1, is the part of ρ\rhoρ that does not depend on a basis. It determines the entropy and purity of the state and the amount of entanglement it carries when it is the reduced state of a pure state.

Keyl and Werner (arXiv:quant-ph/0102027, Phys. Rev. A 64, 052311, 2001) proposed measuring NNN copies with the projections of the Schur–Weyl decomposition of (Cd)⊗N(\mathbb C^d)^{\otimes N}(Cd)⊗N and reporting the normalized Young frame Y/NY/NY/N. They stated that this estimator is consistent and that its error probabilities decay exponentially, with rate the classical relative entropy of the estimate with respect to the true spectrum. The same measurement, now called weak Schur sampling, became the basic primitive of later spectrum, entropy and state tomography algorithms (Keyl, arXiv:quant-ph/0412053; O'Donnell and Wright, arXiv:1508.01907).

Timeline:

  • 1990. Duffield (Proc. Amer. Math. Soc. 109, 1990) proves large-deviation properties of tensor powers of group representations, which covers the maximally mixed state ρ=d−11\rho = d^{-1}\mathbb 1ρ=d−11.
  • 2001. Keyl and Werner state the theorem for every ρ\rhoρ, with a proof sketch that extends Duffield's computation.
  • 2006. Keyl (arXiv:quant-ph/0412053) gives a full large-deviation analysis of the full-state estimator built on this measurement.

Setting

Fix d≥1d \ge 1d≥1 and N≥1N \ge 1N≥1. A Young frame YYY with NNN boxes and at most ddd rows is a sequence of row lengths Y1≥Y2≥⋯≥Yd≥0Y_1 \ge Y_2 \ge \dots \ge Y_d \ge 0Y1​≥Y2​≥⋯≥Yd​≥0 with ∑αYα=N\sum_\alpha Y_\alpha = N∑α​Yα​=N.

The permutation ppp of NNN points acts on (Cd)⊗N(\mathbb C^d)^{\otimes N}(Cd)⊗N by permuting the tensor factors, Sp ψ1⊗⋯⊗ψN=ψp−11⊗⋯⊗ψp−1NS_p\,\psi_1\otimes\dots\otimes\psi_N = \psi_{p^{-1}1}\otimes\dots\otimes\psi_{p^{-1}N}Sp​ψ1​⊗⋯⊗ψN​=ψp−11​⊗⋯⊗ψp−1N​. Each d×dd\times dd×d matrix XXX acts by X⊗NX^{\otimes N}X⊗N. Grouping the irreducible components of the permutation action by type gives orthogonal projections PYP_YPY​, one for each Young frame, onto the summands RY⊗SY\mathcal R_Y \otimes \mathcal S_YRY​⊗SY​. Here SY\mathcal S_YSY​ is the Specht module of the symmetric group, and RY\mathcal R_YRY​ is the Schur module carrying an irreducible representation πY\pi_YπY​ of GL(d,C)GL(d,\mathbb C)GL(d,C). The character of πY\pi_YπY​ is χY(ρ)=tr⁡πY(ρ)\chi_Y(\rho) = \operatorname{tr}\pi_Y(\rho)χY​(ρ)=trπY​(ρ).

The set of possible spectra is the closed ordered simplex

Σ={s∈Rd:s1≥⋯≥sd≥0, ∑jsj=1}.\Sigma = \{ s \in \mathbb R^d : s_1 \ge \dots \ge s_d \ge 0,\ \textstyle\sum_j s_j = 1 \}.Σ={s∈Rd:s1​≥⋯≥sd​≥0, ∑j​sj​=1}.

The estimator reports Y/N∈ΣY/N \in \SigmaY/N∈Σ. Its outcome law on ρ⊗N\rho^{\otimes N}ρ⊗N is

KN(Δ)=tr⁡(EN(Δ) ρ⊗N),EN(Δ)=∑Y: Y/N∈ΔPY.K_N(\Delta) = \operatorname{tr}\big(E_N(\Delta)\,\rho^{\otimes N}\big), \qquad E_N(\Delta) = \sum_{Y:\ Y/N\in\Delta} P_Y .KN​(Δ)=tr(EN​(Δ)ρ⊗N),EN​(Δ)=Y: Y/N∈Δ∑​PY​.

The rate function is the relative entropy

I(s)=∑jsj(ln⁡sj−ln⁡rj)∈[0,∞],I(s) = \sum_j s_j(\ln s_j - \ln r_j) \in [0,\infty],I(s)=j∑​sj​(lnsj​−lnrj​)∈[0,∞],

with 0ln⁡0=00\ln 0 = 00ln0=0, and with I(s)=+∞I(s) = +\inftyI(s)=+∞ when sj>0=rjs_j > 0 = r_jsj​>0=rj​ for some jjj. A set Δ⊆Σ\Delta \subseteq \SigmaΔ⊆Σ has small boundary if its interior is dense in its closure, both taken in the topology of Σ\SigmaΣ.

Formalization targets

Goal: the Theorem of §II

For every density matrix ρ\rhoρ on Cd\mathbb C^dCd with spectrum r∈Σr \in \Sigmar∈Σ:

  1. Asymptotic exactness. For every fff continuous on Σ\SigmaΣ,
lim⁡N→∞∑Yf(Y/N)tr⁡(ρ⊗NPY)=f(r).\lim_{N\to\infty}\sum_Y f\big(Y/N\big)\operatorname{tr}(\rho^{\otimes N}P_Y) = f(r).N→∞lim​Y∑​f(Y/N)tr(ρ⊗NPY​)=f(r).
  1. Error estimate. If ρ\rhoρ is non-singular, then for every Δ⊆Σ\Delta\subseteq\SigmaΔ⊆Σ with small boundary,
lim⁡N→∞1Nln⁡KN(Δ)=−inf⁡s∈ΔI(s).\lim_{N\to\infty}\frac1N\ln K_N(\Delta) = -\inf_{s\in\Delta}I(s).N→∞lim​N1​lnKN​(Δ)=−s∈Δinf​I(s).
  1. Large-deviation bounds. For every ρ\rhoρ and every Δ⊆Σ\Delta\subseteq\SigmaΔ⊆Σ, with interior and closure relative to Σ\SigmaΣ,
−inf⁡int⁡ΔI≤lim inf⁡N1Nln⁡KN(Δ)≤lim sup⁡N1Nln⁡KN(Δ)≤−inf⁡cl⁡ΔI.-\inf_{\operatorname{int}\Delta} I \le \liminf_N \frac1N\ln K_N(\Delta) \le \limsup_N\frac1N\ln K_N(\Delta) \le -\inf_{\operatorname{cl}\Delta} I.−intΔinf​I≤Nliminf​N1​lnKN​(Δ)≤Nlimsup​N1​lnKN​(Δ)≤−clΔinf​I.

Three printed slips are corrected in this statement:

  • The printed (12) lacks the minus sign; the paper's own (11) has it.
  • The printed (5)–(6) define Σ\SigmaΣ with strict inequalities, which excludes Y/NY/NY/N for Y=(N,0,…,0)Y = (N,0,\dots,0)Y=(N,0,…,0).
  • (12) fails for some singular ρ\rhoρ: there 1Nln⁡KN(Δ)\frac1N\ln K_N(\Delta)N1​lnKN​(Δ) can oscillate between −∞-\infty−∞ and a finite value. Item 3 keeps the paper's "for every ρ\rhoρ".

Milestones (the steps of §III)

  • the properties of the PYP_YPY​ from (2)–(4), including the trace form tr⁡(SpPY)=dim⁡RY χ^Y(p)\operatorname{tr}(S_pP_Y) = \dim\mathcal R_Y\,\hat\chi_Y(p)tr(Sp​PY​)=dimRY​χ^​Y​(p) of (4) on the summand;
  • the trace formula tr⁡(ρ⊗NPY)=χY(ρ)dim⁡SY\operatorname{tr}(\rho^{\otimes N}P_Y) = \chi_Y(\rho)\dim\mathcal S_Ytr(ρ⊗NPY​)=χY​(ρ)dimSY​, (17);
  • the weight expansion of χY\chi_YχY​ as the Schur polynomial sY(r)s_Y(r)sY​(r), (20);
  • the highest-weight property of YYY;
  • the sandwich rY≤χY(ρ)≤dim⁡(RY) rYr^Y \le \chi_Y(\rho) \le \dim(\mathcal R_Y)\,r^YrY≤χY​(ρ)≤dim(RY​)rY, (21);
  • the bound dim⁡RY≤(N+1)d(d−1)/2\dim\mathcal R_Y \le (N+1)^{d(d-1)/2}dimRY​≤(N+1)d(d−1)/2;
  • the limit 1Nln⁡∑Ytr⁡(ρ⊗NPY)eη⋅Y→ln⁡∑αrαeηα\frac1N\ln\sum_Y \operatorname{tr}(\rho^{\otimes N}P_Y)e^{\eta\cdot Y} \to \ln\sum_\alpha r_\alpha e^{\eta_\alpha}N1​ln∑Y​tr(ρ⊗NPY​)eη⋅Y→ln∑α​rα​eηα​ for decreasing η\etaη, (22)–(25);
  • the Legendre identity I(s)=sup⁡η(η⋅s−ln⁡∑αrαeηα)I(s) = \sup_\eta(\eta\cdot s - \ln\sum_\alpha r_\alpha e^{\eta_\alpha})I(s)=supη​(η⋅s−ln∑α​rα​eηα​);
  • I≥0I \ge 0I≥0 on Σ\SigmaΣ, with I(s)=0I(s) = 0I(s)=0 only for s=rs = rs=r.

Significance

The theorem makes measuring the Young frame a consistent estimator of the spectrum, with an explicit exponential error rate. For a ball BBB around rrr, the probability that Y/NY/NY/N falls outside BBB is e−N(inf⁡Σ∖BI+o(1))e^{-N(\inf_{\Sigma\setminus B}I + o(1))}e−N(infΣ∖B​I+o(1)). This is the classical Cramér rate for the empirical distribution of NNN samples from rrr, even though no classical samples from rrr are ever produced. The same Schur–Weyl measurement underlies sample-optimal spectrum and state estimation, the quantum empirical-distribution analogues of Sanov's theorem, and universal entanglement concentration.

The paper gives a proof sketch. Its final step needs the scaled cumulant generating function outside the ordered cone and the regularity required by the Gärtner–Ellis theorem, and the authors leave this to an extension of Duffield's work. No machine-checked proof of the theorem or of any of its steps exists. Formalizing it also adds to the published Schur–Weyl layer (QAlgorithms.Schur.isotypicProjector, schurModule, schurPolynomial) its first theorems: projection identities, the trace formula, the Schur polynomial character formula and the Weyl dimension bound. Other missions built on weak Schur sampling can reuse these.

Difficulty

The obvious argument runs through a classical reduction: diagonalize ρ\rhoρ, observe that KNK_NKN​ depends only on rrr, and apply Sanov's theorem. This fails. tr⁡(ρ⊗NPY)=dim⁡SY sY(r)\operatorname{tr}(\rho^{\otimes N}P_Y) = \dim\mathcal S_Y\, s_Y(r)tr(ρ⊗NPY​)=dimSY​sY​(r) is not a multinomial law: the frame YYY is not the type of a sequence of independent samples from rrr. The authors remark that there seems to be no direct reduction to the i.i.d. setting.

The exponential rate has to be extracted from sY(r)s_Y(r)sY​(r) instead. This is a sum over exponentially many semistandard fillings, weighted by multiplicities, and it must be controlled uniformly over all frames. The paper's computation of the cumulant generating function covers only decreasing η\etaη, while the Gärtner–Ellis theorem needs it on all of Rd\mathbb R^dRd with regularity. For singular ρ\rhoρ, III is infinite on most of Σ\SigmaΣ and the limit (12) can genuinely fail to exist, so only the two-sided bounds survive.

Formalization scope

Lean conventions fixed by the statements:

  • States are Matrix (Fin d) (Fin d) ℂ satisfying QAlgorithms.IsDensityMatrix (positive semidefinite, trace one), and ρ⊗N\rho^{\otimes N}ρ⊗N is QAlgorithms.piKron N ρ.
  • Young frames are QAlgorithms.Schur.Partition d N.
  • PYP_YPY​ is the published isotypicProjector, defined from the permutation action alone. None of its properties is assumed; they are milestone 1.
  • Rows and coordinates are indexed by Fin d, and Lean's index 000 is the paper's index 111.
  • Σ\SigmaΣ is the closed ordered simplex.
  • rrr is tied to ρ\rhoρ by ρ=Udiag⁡(r)U∗\rho = U\operatorname{diag}(r)U^*ρ=Udiag(r)U∗ with UUU unitary and r∈Σr\in\Sigmar∈Σ.
  • 1Nln⁡KN(Δ)\frac1N\ln K_N(\Delta)N1​lnKN​(Δ) is computed in EReal with ln⁡0=−∞\ln 0 = -\inftyln0=−∞ (ENNReal.log), so an event of probability zero has rate −∞-\infty−∞, not 000.
  • III is EReal-valued, equal to +∞+\infty+∞ where sss charges a zero of rrr.
  • Interiors and closures are taken in the subspace topology of Σ\SigmaΣ. The interior of a subset of Σ\SigmaΣ taken in Rd\mathbb R^dRd is empty, and that reading would make item 2 vacuous; the relative topology rules it out.
  • Δ\DeltaΔ ranges over all subsets of Σ\SigmaΣ, since KNK_NKN​ is a finite sum.
  • Nothing in the goal is a free parameter pinned by hypotheses: KNK_NKN​ is the Born probability of the actual ρ⊗N\rho^{\otimes N}ρ⊗N, and rrr is the spectrum of ρ\rhoρ.

A complete development needs:

  • the basic representation theory of the published Schur–Weyl modules;
  • the character identity χY=sY\chi_Y = s_YχY​=sY​;
  • the Weyl dimension formula or a direct bound;
  • the Gärtner–Ellis theorem, or a direct Laplace-method argument on the finite set of frames;
  • the Gibbs variational formula for the relative entropy.

The Schur–Weyl facts and the Gärtner–Ellis theorem are reusable well beyond this mission. Contributions of any of these as separate theorems are welcome.

Selected references

  • M. Keyl and R. F. Werner, Estimating the spectrum of a density operator, Phys. Rev. A 64, 052311 (2001). arXiv:quant-ph/0102027
  • N. G. Duffield, A large deviation principle for the reduction of product representations, Proc. Amer. Math. Soc. 109, 503–515 (1990). https://www.ams.org/journals/proc/1990-109-02/
  • M. Keyl, Quantum state estimation and large deviations, Rev. Math. Phys. 18, 19–60 (2006). arXiv:quant-ph/0412053
  • R. O'Donnell and J. Wright, Efficient quantum tomography, STOC 2016. arXiv:1508.01907
  • R. S. Ellis, Entropy, Large Deviations, and Statistical Mechanics, Springer, Grundlehren 271 (1985).
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Bandit AlgorithmsMachine LearningOperations Research+1·Captain: mikedeng1

Learning Product Rankings Robust to Fake Users: With the Fakeness Budget F Unknown, FORC Has Regret O((n²F + log T) Σ_{j<i} log(nT)/Δ_{j,i})Research Paper

Motivation

Online platforms rank products, and the ranking is learned from clicks. Click farms and bots exploit this: fake users click on a product so that the platform promotes it. Golrezaei, Manshadi, Schneider and Sekar (arXiv:2009.05138, Operations Research 71(4), 2023) study how to learn a ranking when an unknown number of users are fake and cannot be told apart from real ones. They show that a standard optimistic learner (UCB) can be pushed to regret linear in TTT by O(log⁡2T)O(\log^2 T)O(log2T) fake users (their Theorem 1), and they give two robust algorithms: FAR, which needs the number FFF of fake users, and FORC (Fake-Oblivious Ranking with Cross-learning), which does not. The multi-level idea behind FORC comes from corruption-robust bandits (Lykouris, Mirrokni, Paes Leme, STOC 2018). The ranking setting makes it harder, because which products a customer examines is itself random.

Setting

A platform shows nnn products to TTT users in turn. Product iii has an unknown click probability μi∈[0,1]\mu_i\in[0,1]μi​∈[0,1], indexed so that

μ1>μ2>⋯>μn,\mu_1>\mu_2>\dots>\mu_n,μ1​>μ2​>⋯>μn​,

and Δj,i=μj−μi\Delta_{j,i}=\mu_j-\mu_iΔj,i​=μj​−μi​. A ranking π\piπ puts product π(j)\pi(j)π(j) at position jjj.

A real customer follows a cascade. She examines positions 1,2,…1,2,\dots1,2,… in turn and clicks the product at position jjj with probability μπ(j)\mu_{\pi(j)}μπ(j)​, which ends her visit. If she does not click, she leaves with an unknown exit probability qj∈[0,1]q_j\in[0,1]qj​∈[0,1], or moves on to position j+1j+1j+1. After position nnn she always leaves. The platform observes ctc_tct​: the last examined position and whether its product was clicked.

A fake entity controls the fake users. Its adaptive policy P\mathbf PP maps the history Ht−1={(πs,fs,cs)}s<t\mathcal H_{t-1}=\{(\pi_s,f_s,c_s)\}_{s<t}Ht−1​={(πs​,fs​,cs​)}s<t​ (past rankings, fake indicators and observations) to a probability distribution over this round's user. The user is either real, or fake and clicking any chosen product, or fake and clicking nothing and leaving at any chosen position. The fakeness budget FFF says that at most FFF rounds are fake on every realization. The platform never learns which users were fake. Only real clicks count:

RegT=sup⁡P{E[∑t=1TCr,t(π⋆)]−E[∑t=1TCr,t(πt)]},\mathrm{Reg}_T=\sup_{\mathbf P}\Big\{\mathbb E\Big[\sum_{t=1}^T\mathcal C_{r,t}(\pi^\star)\Big]-\mathbb E\Big[\sum_{t=1}^T\mathcal C_{r,t}(\pi_t)\Big]\Big\},RegT​=Psup​{E[t=1∑T​Cr,t​(π⋆)]−E[t=1∑T​Cr,t​(πt​)]},

where Cr,t=1\mathcal C_{r,t}=1Cr,t​=1 when the user of round ttt is real and clicks, and π⋆(i)=i\pi^\star(i)=iπ⋆(i)=i is the optimal ranking.

FORC runs L=⌈log⁡2T⌉L=\lceil\log_2T\rceilL=⌈log2​T⌉ levels. In each round it samples level ℓ\ellℓ with probability 2−ℓ2^{-\ell}2−ℓ (level 111 takes the remaining mass). Each level keeps feedback counts and a product-ordering graph G(ℓ)G^{(\ell)}G(ℓ), whose edge (i,j)(i,j)(i,j) records that product jjj is believed better than iii. The displayed ranking is GraphRankSelect(η(ℓt),G)\mathrm{GraphRankSelect}(\eta^{(\ell_t)},G)GraphRankSelect(η(ℓt​),G). It fills the positions in order, each time with a product that has no outgoing edge into the remaining set, preferring the one with the fewest observations. Samples propagate upward, with weight 2−ℓ2^{-\ell}2−ℓ at level ℓ\ellℓ (cross-learning). Edges propagate downward, and a graph that acquires a cycle is eliminated.

Formalization targets

Goal: Theorem 3

There is an absolute constant CCC such that, for all n≥1n\ge1n≥1, T≥2T\ge2T≥2, F≥0F\ge0F≥0, every instance, every policy within budget FFF, and every resolution of FORC's unspecified choices,

RegT(FORC)≤C (n2F+log⁡T)∑j=1n∑i=j+1nlog⁡(nT)Δj,i.\mathrm{Reg}_T(\mathrm{FORC})\le C\,\big(n^2F+\log T\big)\sum_{j=1}^n\sum_{i=j+1}^n\frac{\log(nT)}{\Delta_{j,i}}.RegT​(FORC)≤C(n2F+logT)j=1∑n​i=j+1∑n​Δj,i​log(nT)​.

This is the paper's O(⋅)O(\cdot)O(⋅) statement (16), with the constant made explicit and uniform.

Milestones, in the order the proof uses them

  1. Lemma 1 (regret decomposition): for any algorithm, regret ≤F+∑t∑j<iΔj,iPr⁡[Ar,t(πt(j)=i)]\le F+\sum_t\sum_{j<i}\Delta_{j,i}\Pr[\mathcal A_{r,t}(\pi_t(j)=i)]≤F+∑t​∑j<i​Δj,i​Pr[Ar,t​(πt​(j)=i)].
  2. Lemma 11: one level ℓ≥log⁡2F\ell\ge\log_2Fℓ≥log2​F is exposed to at most log⁡(2L/δ)+3\log(2L/\delta)+3log(2L/δ)+3 fake users with probability at least 1−δ/(2L)1-\delta/(2L)1−δ/(2L).
  3. Lemma 5: with probability at least 1−δ/21-\delta/21−δ/2, every level ℓ≥log⁡2F\ell\ge\log_2Fℓ≥log2​F is exposed to at most log⁡(2L/δ)+3\log(2L/\delta)+3log(2L/δ)+3 fake users, with δ=1/(n3T)\delta=1/(n^3T)δ=1/(n3T).
  4. Lemma 13: a Hoeffding bound 2e−2ε2η^2e^{-2\varepsilon^2\hat\eta}2e−2ε2η^​ for the cross-learned weighted mean.
  5. Lemma 6: the good event G\mathcal GG (accurate estimates at the high levels, few fake users there) has probability at least 1−δ1-\delta1−δ.
  6. Lemma 15: on G\mathcal GG, the graphs of levels ℓ≥⌈log⁡2F⌉\ell\ge\lceil\log_2F\rceilℓ≥⌈log2​F⌉ never hold an incorrect edge, and they hold the correct edge between iii and jjj once both products have γj,i=64log⁡(4nT/δ)/Δj,i2\gamma_{j,i}=64\log(4nT/\delta)/\Delta_{j,i}^2γj,i​=64log(4nT/δ)/Δj,i2​ cross-learned samples.
  7. Lemma 9: the loss off G\mathcal GG is at most 1/n21/n^21/n2.

Significance

Theorem 3 says that a platform that does not know how many of its users are fake loses only O((n2F+log⁡T)log⁡T)O((n^2F+\log T)\log T)O((n2F+logT)logT) real clicks against the best fixed ranking (for fixed nnn and gaps bounded below). The obvious algorithms lose Ω(T)\Omega(T)Ω(T). It extends multi-layer corruption robustness from multi-armed bandits to a combinatorial feedback model in which the observed coordinates are themselves random and depend on the ranking.

Formalizing it gives:

  • a machine-checked cascade click model with exit probabilities and an adaptive adversary;
  • a reusable regret decomposition for rankings (Lemma 1);
  • a per-level corruption bound for randomized level sampling (Lemmas 5 and 11);
  • a fully specified FORC.

None of these results is formalized anywhere, to our knowledge. The theorem is proved in the paper, so the remaining work is a formal proof of the known argument. The planning check of that argument found slips in constants of auxiliary lemmas (Lemmas 7, 8, 10) but nothing affecting the O(⋅)O(\cdot)O(⋅) statement.

Difficulty

The levels at or above ℓ⋆=⌈log⁡2F⌉\ell^\star=\lceil\log_2F\rceilℓ⋆=⌈log2​F⌉ are the easy part. They see O(log⁡log⁡T)O(\log\log T)O(loglogT) fake users, so their confidence windows absorb the corruption and their graphs stay correct (Lemmas 5, 6, 15).

The levels below ℓ⋆\ell^\starℓ⋆ are the hard part. They are sampled more often and can be corrupted arbitrarily. The obvious argument would bound the misplacements at each low level separately, and that fails: a corrupted low level can keep a bad product on top for as long as it is not eliminated. The paper's Lemma 10 controls these levels only through the interaction of the two cross-learning directions. It runs an induction over products with a change of measure between levels, and that step is where the factor n2Fn^2Fn2F comes from.

The adversary is adaptive and sees all past rankings. The bound fails if the adversary could see the current round's level.

Formalization scope

  • Model. Products, positions, levels and rounds are Fin n, Fin n, Fin L and Fin T, all 0-based. Lean level kkk is paper level ℓ=k+1\ell=k+1ℓ=k+1, so the condition ℓ≥⌈log⁡2F⌉\ell\ge\lceil\log_2F\rceilℓ≥⌈log2​F⌉ becomes F≤2k+1F\le2^{k+1}F≤2k+1.
  • Probabilities. Every space is finite, so expectations are finite sums over trajectories Fin T→Step\mathtt{Fin}\ T\to\mathtt{Step}Fin T→Step. Each trajectory is weighted by the level probabilities, the policy's PMF and the cascade law. No measure theory is used except in Lemma 13.
  • Adversary. The policy is a function of the past history only. It never sees the current ranking or level.
  • Algorithms. A general algorithm (Lemma 1) draws an internal label with history-dependent weights and ranks as a function of its own past. It never sees the fake indicators.
  • Committed conventions. L=⌈log⁡2T⌉L=\lceil\log_2T\rceilL=⌈log2​T⌉, δ=1/(n3T)\delta=1/(n^3T)δ=1/(n3T), natural logarithms. Rewards are averages of clicks, which reads Step 8's denominator η+1\eta+1η+1 as η\etaη. FORC's tie-breaking, its "arbitrary ranking" and its fallback when no level qualifies are arbitrary functions of its past, and every statement holds for all of them.
  • Added hypotheses. T≥2T\ge2T≥2 is added to the goal, because at T=1T=1T=1 the right-hand side is 000 while the regret can be positive. n≥1n\ge1n≥1 is added because δ\deltaδ is undefined at n=0n=0n=0.
  • Ruled out. FORC's definition takes no FFF, μ\muμ or qqq. The adversary is randomized and adaptive rather than oblivious. The customer law and the level weights are probability distributions (checked in a sorry-free sanity file). CCC is quantified before every other variable. Trivializing variants of the goal are therefore excluded.
  • Out of scope. Theorem 1 (UCB's linear regret), Theorem 2 (FAR, with FFF known), Lemmas 7, 8, 10, 16–18 (printed constants rest on non-integer counts), and the numerical study of §7.
  • Infrastructure. A complete development needs a Freedman/Bernstein inequality for bounded martingale differences (Lemma 12, cited from Beygelzimer et al. 2011). It also needs the conditional form of Hoeffding behind Lemma 6, and a coupling of the finite trajectory law with independent sample sequences. These pieces are reusable for any cascade or corruption-robust bandit formalization. Proofs of the milestones, and of Lemmas 7, 8 and 10 in any faithful form, are welcome.

Selected references

  • N. Golrezaei, V. Manshadi, J. Schneider, S. Sekar, Learning Product Rankings Robust to Fake Users, Operations Research 71(4), 2023; arXiv:2009.05138v1 (2020). https://arxiv.org/abs/2009.05138
  • T. Lykouris, V. Mirrokni, R. Paes Leme, Stochastic Bandits Robust to Adversarial Corruptions, STOC 2018. https://arxiv.org/abs/1803.09353
  • A. Beygelzimer, J. Langford, L. Li, L. Reyzin, R. Schapire, Contextual Bandit Algorithms with Supervised Learning Guarantees, AISTATS 2011. https://arxiv.org/abs/1002.4058
  • N. Craswell, O. Zoeter, M. Taylor, B. Ramsey, An Experimental Comparison of Click Position-Bias Models, WSDM 2008. https://doi.org/10.1145/1341531.1341545
  • B. Kveton, C. Szepesvári, Z. Wen, A. Ashkan, Cascading Bandits: Learning to Rank in the Cascade Model, ICML 2015. https://arxiv.org/abs/1502.02763
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CombinatoricsComplexity TheoryTheoretical Computer Science·Captain: mikedeng1

Complexity of n-Queens Completion: n-Queens Completion Is NP-Complete and #P-CompleteResearch Paper

Motivation

The n-Queens problem, placing nnn mutually non-attacking queens on an n×nn\times nn×n chessboard, is a standard benchmark in constraint programming and artificial intelligence. As a decision problem it is trivial: a solution exists for every nnn other than 222 and 333 and can be written down in closed form, and the input ⟨n⟩\langle n\rangle⟨n⟩ has only log⁡n\log nlogn bits. This has repeatedly led to criticism of its use as a benchmark.

The variant n-Queens Completion, posed in 1850, asks whether a board on which some queens are already placed can be completed to a full solution. Gent, Jefferson and Nightingale (JAIR 2017) show that this variant is genuinely hard: deciding it is NP-complete and counting its completions is #P-complete. This gives benchmark designers a version of the puzzle with a provable hardness guarantee, and it makes the n-Queens literature (Pólya's modular construction, Rivin–Zabih exchanges) a source of reduction gadgets.

Timeline:

  • Pólya: the product construction of n-Queens solutions from modular ones (as stated by Bell and Stevens 2009, Thm. 6).
  • 1992: Rivin and Zabih's exchange lemma for queens using the same lines (Thm. 2.4).
  • 1996: Creignou and Hermann classify the complexity of counting generalized satisfiability; #P-completeness of Monotone 1-in-3-SAT is a corollary.
  • 2014: Porschen, Schmidt, Speckenmeyer and Wotzlaw (Lemma 4): 1-in-3-SAT with positive literals, distinct variables per clause and at most three occurrences per variable is NP-complete.
  • 2017: Gent, Jefferson and Nightingale: n-Queens Completion is NP-complete and #P-complete (Theorem 37).

Setting

A queen is a pair q=(α,β)q=(\alpha,\beta)q=(α,β) of non-negative integers, its column and row. Its sum-diagonal is α+β\alpha+\betaα+β and its difference-diagonal is the integer α−β\alpha-\betaα−β. It fits on board size nnn if max⁡(α,β)<n\max(\alpha,\beta)<nmax(α,β)<n. Two distinct queens attack each other if they share a column, a row, a sum-diagonal or a difference-diagonal. A solution to the nnn-Queens problem (n≥1n\ge1n≥1) is a set of nnn queens that fit on board size nnn, no two attacking.

An instance of n-Queens Completion (Problem 2) is a pair ⟨n,P⟩\langle n,P\rangle⟨n,P⟩: a board size n≥1n\ge1n≥1 and a set PPP of queens that fit on board size nnn, no two in the same row or column. PPP may contain two queens on a common diagonal; such an instance simply has no solution. A completion is an nnn-Queens solution SSS with P⊆SP\subseteq SP⊆S.

The proof passes through four intermediate problems. In Problem 3 the extra queens must use prescribed columns CCC and rows RRR. In Problem 4 (Excluded Diagonals) sets D−D^-D−, D+D^+D+ of difference- and sum-diagonals are forbidden. Problem 5 is a family of Problem 4 instances that interact only through their sum-diagonals. Problem 6 is Restricted 1-in-3-SAT: clauses of three distinct positive variables, every variable in at most three clauses, and an assignment must make exactly one variable of every clause true.

Complexity is measured on the published CookLevin machine model: a language is a set of binary strings, CookLevin.NPComplete is NP-completeness under polynomial-time many-one reductions, and a function fff from strings to N\mathbb NN is in #P if it counts the accepted certificates of an NP verifier. Every instance is coded with its board size in unary, as the paper assumes (p. 820). NQC\mathrm{NQC}NQC is the language of codes of instances that have a completion, and #NQC(x)\#\mathrm{NQC}(x)#NQC(x) is the number of completions of the instance coded by xxx.

Formalization targets

Goal: Theorem 37

NQC is NP-completeand#NQC is #P-complete.\mathrm{NQC}\ \text{is NP-complete}\qquad\text{and}\qquad \#\mathrm{NQC}\ \text{is \#P-complete}.NQC is NP-completeand#NQC is #P-complete.

Here #P-completeness means membership in #P together with hardness under parsimonious reductions: polynomial-time maps RRR with f(x)=#NQC(R(x))f(x)=\#\mathrm{NQC}(R(x))f(x)=#NQC(R(x)) for every string xxx. The statement is unconditional.

Milestones

  • Theorem 4: Restricted 1-in-3-SAT is NP-complete and #P-complete.
  • Theorem 36, with Lemmas 33–35: variable and clause gadgets give a parsimonious reduction from Restricted 1-in-3-SAT to Problem 5.
  • Theorem 23, with Lemmas 9, 21, 22: laying the gadgets out along one long diagonal reduces Problem 5 to Problem 4.
  • Theorem 19, with Lemmas 17, 18: blocker queens outside the board reduce Problem 4 to Problem 3.
  • Theorem 13, with Lemmas 11, 12: a 19-queens frame filled with modular solutions reduces Problem 3 to n-Queens Completion.
  • Supporting results: Pólya's Theorem 2, Observation 6 on Q19Q_{19}Q19​, Lemma 7 on AnA_nAn​, BnB_nBn​, the Rivin–Zabih Lemma 8, Lemma 25 and Observation 29, and Lemma 30.

Each reduction theorem states both halves of "parsimonious": the paper's construction preserves the number of solutions instance by instance, and a polynomial-time map on codes implements it.

Significance

The result. Theorem 37 shows that the hardness of n-Queens Completion is not an artefact of a particular solver. The same chain shows that Excluded Diagonals and Blocked n-Queens are NP- and #P-complete (Corollary 38), and Corollary 15 (from Lemma 12) shows that every non-attacking set of queens occurs inside some full solution of a larger board. Because the reductions are parsimonious, they also transfer counting hardness: counting completions exactly is as hard as #SAT.

Formalizing it. The result is proved on paper; no part of it is machine-checked. The mission adds the platform's first #P layer (#P, parsimonious reductions, #P-completeness) on top of the published CookLevin NP framework, and the first chessboard objects. Four printed slips are corrected, each with a counterexample: Lemma 8 needs ∣P1∣=∣P∣|P_1|=|P|∣P1​∣=∣P∣; Problem 3 needs C,R⊆{0,…,n−1}C,R\subseteq\{0,\dots,n-1\}C,R⊆{0,…,n−1} (Theorem 13 fails otherwise); Definition 20's D+D^+D+ overshoots 2n−22n-22n−2; Definition 20 is undefined for the empty family.

Difficulty

The obvious argument fails in two places.

First, each reduction is a bijection between solution sets whose correctness depends on exhaustive diagonal bookkeeping: that the 19-queens frame and the embedded modular solutions leave exactly the intended squares free, that the blockers of Definition 16 rule out exactly the chosen diagonals, and that gadgets on a long diagonal interact only through sum-diagonals. Each is a case analysis over many families of squares, with integer arithmetic on both diagonals.

Second, Theorem 4 is cited, not proved, for its hard part. A proof from scratch needs #P-hardness of a 1-in-3-SAT variant, i.e. a parsimonious version of the Cook–Levin theorem. The published CookLevin.sat_npComplete gives the decision half only, and many standard reductions from SAT are not parsimonious. In addition, every map must be shown polynomial-time on the CookLevin machine model, which the paper asserts "by inspection".

Formalization scope

Lean conventions:

  • a queen is ℕ × ℕ (column, row), the difference-diagonal is computed in ℤ, and sets of queens are Finset (ℕ × ℕ);
  • board sizes are n≥1n\ge1n≥1, and an instance of Problem 3 (hence of Problems 4 and 5) has C,R⊆{0,…,n−1}C,R\subseteq\{0,\dots,n-1\}C,R⊆{0,…,n−1};
  • a Problem 5 instance is a List of Problem 4 instances, and its sum-diagonal condition applies to distinct indices;
  • a Problem 6 instance is a duplicate-free list of three-element clauses over natural-number variables, the list order being the clause order and variables ordered increasingly, and a solution is the set of true variables;
  • codes write every number in unary and list a set without repetition; strings that code no valid instance are no-instances with count 000;
  • counts are Set.ncard of solution sets, which are finite.

The constructions (Definitions 10, 16, 20, 24, 26–28, 31) are transcribed as defs, never chosen by Classical.choice. Each reduction theorem fixes its output to the code of the paper's construction.

Trivializing formalizations are ruled out explicitly:

  • the problems are List Bool languages, not Prop-valued predicates;
  • #P membership requires the verifier's polynomial length bound, without which ncard of an infinite set is 000;
  • parsimonious reductions must be CookLevin.IsPolyTimeComputable;
  • counts are of solutions, not of codes;
  • the board size is unary;
  • the goal assumes no hardness hypothesis.

Infrastructure that is reusable beyond this mission: the #P definitions and their closure under composition of parsimonious reductions, and polynomial-time computability of list and arithmetic manipulations on unary codes, for which the published WordRAM simulation (CookLevin.ramPolyTime_to_tm_poly, CookLevin.polyTimeComputable_comp) is the intended route. A parsimonious Cook–Levin theorem would serve every future #P-completeness result. Contributions are welcome on any milestone; the gadget lemmas (33–35) and the arithmetic facts (Lemma 9, Observations 6 and 29, Lemma 30) are self-contained and decidable on finite data.

Selected references

  • I. P. Gent, C. Jefferson, P. Nightingale, Complexity of n-Queens Completion, Journal of Artificial Intelligence Research 59 (2017) 815–848. https://doi.org/10.1613/jair.5512
  • J. Bell, B. Stevens, A survey of known results and research areas for n-queens, Discrete Mathematics 309(1) (2009) 1–31.
  • I. Rivin, R. Zabih, A dynamic programming solution to the n-queens problem, Information Processing Letters 41(5) (1992) 253–256.
  • N. Creignou, M. Hermann, Complexity of generalized satisfiability counting problems, Information and Computation 125(1) (1996) 1–12.
  • S. Porschen, T. Schmidt, E. Speckenmeyer, A. Wotzlaw, XSAT and NAE-SAT of linear CNF classes, Discrete Applied Mathematics 167 (2014) 1–14.
  • C. H. Papadimitriou, Computational Complexity, Addison-Wesley, 1994, Chapter 18.
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Functional AnalysisQuantum InformationQuantum Mechanics·Captain: mikedeng1

Additivity properties of a Gaussian channel: the maximal output k-norm of m uses of the classical-noise channel N_n is [(n+1)^k − n^k]^(−m/k), attained by coherent product statesResearch Paper

Why maximal output norms matter

A quantum channel can carry classical information at a rate given by its Holevo capacity C1C_1C1​ for one use. If a sender may encode messages in states that are entangled across mmm uses, the capacity per use could in principle exceed C1C_1C1​, and the ultimate classical capacity then requires a limit m→∞m\to\inftym→∞ (Holevo; Schumacher–Westmoreland). Whether this regularization is ever needed is the additivity question of quantum Shannon theory. It is equivalent to the additivity of the minimum output entropy of the channel (Shor 2004).

Amosov, Holevo and Werner proposed a stronger property (AHW 2000): the maximal output zzz-norm of a channel is multiplicative,

νz(M⊗m)=[νz(M)]m.\nu_z(\mathcal M^{\otimes m})=[\nu_z(\mathcal M)]^m .νz​(M⊗m)=[νz​(M)]m.

Through the Rényi entropies Sz(ρ)=−ln⁡Tr⁡[ρz]/(z−1)S_z(\rho)=-\ln\operatorname{Tr}[\rho^z]/(z-1)Sz​(ρ)=−lnTr[ρz]/(z−1) this is the same as additivity of the minimum output Rényi entropy of order zzz, and multiplicativity for zzz arbitrarily close to 111 would give the additivity of the Holevo capacity.

Timeline. In 2004 Giovannetti, Lloyd, Maccone, Shapiro and Yen computed νk\nu_kνk​ for one use of the classical-noise channel at integer kkk (arXiv:quant-ph/0404037). In the same year Giovannetti and Lloyd proved multiplicativity for mmm uses of that channel at every integer kkk (arXiv:quant-ph/0403075), the result of this mission. In 2009 Hayden and Winter disproved multiplicativity for general channels at z>1z>1z>1 (arXiv:0807.4753), and Hastings disproved additivity of the minimum output entropy in general (arXiv:0809.3972). For bosonic Gaussian channels the question was settled positively by Giovannetti, Holevo and García-Patrón (arXiv:1312.2251) and Mari, Giovannetti and Holevo (arXiv:1312.3545). The integer-order case for the classical-noise channel predates these and has a self-contained Gaussian-integral proof.

The channel and the norms

One use of the channel is a single bosonic mode with annihilation operator aaa and Fock basis ∣0⟩,∣1⟩,…|0\rangle,|1\rangle,\dots∣0⟩,∣1⟩,…. The displacement operator is D(μ)=exp⁡(μa†−μ∗a)D(\mu)=\exp(\mu a^\dagger-\mu^*a)D(μ)=exp(μa†−μ∗a) for μ∈C\mu\in\mathbb Cμ∈C. For a noise parameter n≥0n\ge0n≥0, the classical-noise channel displaces the input by a random amount:

Nn(ρ)=∫d2μ  Pn(μ) D(μ)ρD†(μ),Pn(μ)=e−∣μ∣2/nπn,\mathcal N_n(\rho)=\int d^2\mu\;P_n(\mu)\,D(\mu)\rho D^\dagger(\mu),\qquad P_n(\mu)=\frac{e^{-|\mu|^2/n}}{\pi n},Nn​(ρ)=∫d2μPn​(μ)D(μ)ρD†(μ),Pn​(μ)=πne−∣μ∣2/n​,

with d2μ=d Re μ d Im μd^2\mu=d\,\mathrm{Re}\,\mu\,d\,\mathrm{Im}\,\mud2μ=dReμdImμ; at n=0n=0n=0 the law is the point mass at 000 and the channel is the identity.

For mmm uses the Hilbert space is H⊗m=ℓ2(Nm)\mathcal H^{\otimes m}=\ell^2(\mathbb N^m)H⊗m=ℓ2(Nm), with basis ∣u⟩|u\rangle∣u⟩, u∈Nmu\in\mathbb N^mu∈Nm. With μ⃗∈Cm\vec\mu\in\mathbb C^mμ​∈Cm and D(μ⃗)=D1(μ1)⋯Dm(μm)D(\vec\mu)=D_1(\mu_1)\cdots D_m(\mu_m)D(μ​)=D1​(μ1​)⋯Dm​(μm​),

Nn⊗m(ρ)=∫d2μ⃗  Pn(μ⃗) D(μ⃗) ρ D†(μ⃗),Pn(μ⃗)=e−∣μ⃗∣2/n(πn)m,\mathcal N_n^{\otimes m}(\rho)=\int d^2\vec\mu\;P_n(\vec\mu)\,D(\vec\mu)\,\rho\,D^\dagger(\vec\mu),\qquad P_n(\vec\mu)=\frac{e^{-|\vec\mu|^2/n}}{(\pi n)^m},Nn⊗m​(ρ)=∫d2μ​Pn​(μ​)D(μ​)ρD†(μ​),Pn​(μ​)=(πn)me−∣μ​∣2/n​,

for every density operator ρ\rhoρ of the mmm modes, including states entangled across uses.

For z≥1z\ge1z≥1 the zzz-norm is ∥A∥z=(Tr⁡∣A∣z)1/z\|A\|_z=(\operatorname{Tr}|A|^z)^{1/z}∥A∥z​=(Tr∣A∣z)1/z and the maximal output zzz-norm is

νz(Nn⊗m)=sup⁡ρ∥Nn⊗m(ρ)∥z,\nu_z(\mathcal N_n^{\otimes m})=\sup_\rho\big\|\mathcal N_n^{\otimes m}(\rho)\big\|_z ,νz​(Nn⊗m​)=ρsup​​Nn⊗m​(ρ)​z​,

the supremum over all density operators of the mmm uses. A coherent product is ∣α1⟩⊗⋯⊗∣αm⟩|\alpha_1\rangle\otimes\cdots\otimes|\alpha_m\rangle∣α1​⟩⊗⋯⊗∣αm​⟩, with ⟨p∣α⟩=e−∣α∣2/2αp/p!\langle p|\alpha\rangle=e^{-|\alpha|^2/2}\alpha^p/\sqrt{p!}⟨p∣α⟩=e−∣α∣2/2αp/p!​.

Formalization targets

Goal: Eq. (11)

For all n≥0n\ge0n≥0, all mmm and every integer k≥1k\ge1k≥1,

νk(Nn⊗m)=[1(n+1)k−nk]m/k,\nu_k(\mathcal N_n^{\otimes m})=\left[\frac{1}{(n+1)^k-n^k}\right]^{m/k},νk​(Nn⊗m​)=[(n+1)k−nk1​]m/k,

and every coherent product attains this value. Since the single-use value is [(n+1)k−nk]−1/k[(n+1)^k-n^k]^{-1/k}[(n+1)k−nk]−1/k, this is multiplicativity at every integer order.

Milestones

  1. Eq. (10), for mmm-fold coherent products and every real z≥1z\ge1z≥1: ∥Nn⊗m(ρα⃗)∥z=[(n+1)z−nz]−m/z\|\mathcal N_n^{\otimes m}(\rho_{\vec\alpha})\|_z=[(n+1)^z-n^z]^{-m/z}∥Nn⊗m​(ρα​)∥z​=[(n+1)z−nz]−m/z.
  2. Part one (Sec. I A): every input is dominated by a pure input, so νz\nu_zνz​ is a supremum over pure states.
  3. Eqs. (16)–(17): for ρ=∣ψ⟩⟨ψ∣\rho=|\psi\rangle\langle\psi|ρ=∣ψ⟩⟨ψ∣, Tr⁡{[Nn⊗m(ρ)]k}\operatorname{Tr}\{[\mathcal N_n^{\otimes m}(\rho)]^k\}Tr{[Nn⊗m​(ρ)]k} is the Gaussian average of ∏s⟨ψ∣D†(μ⃗s)D(μ⃗s+1)∣ψ⟩\prod_s\langle\psi|D^\dagger(\vec\mu_s)D(\vec\mu_{s+1})|\psi\rangle∏s​⟨ψ∣D†(μ​s​)D(μ​s+1​)∣ψ⟩.
  4. Eq. (A1): the Weyl relation D†(μ⃗)D(ν⃗)=D(ν⃗−μ⃗) e(ν⃗⋅μ⃗†−μ⃗⋅ν⃗†)/2D^\dagger(\vec\mu)D(\vec\nu)=D(\vec\nu-\vec\mu)\,e^{(\vec\nu\cdot\vec\mu^\dagger-\vec\mu\cdot\vec\nu^\dagger)/2}D†(μ​)D(ν)=D(ν−μ​)e(ν⋅μ​†−μ​⋅ν†)/2.
  5. Eq. (A12) (= (33)): ∫d2ν e−d∣ν∣2/∣e∣2πn∣e∣2⟨p∣D(−ν)∣q⟩=2/n2d+∣e∣2(2d−∣e∣22d+∣e∣2)pδpq\int d^2\nu\,\frac{e^{-d|\nu|^2/|e|^2}}{\pi n|e|^2}\langle p|D(-\nu)|q\rangle=\frac{2/n}{2d+|e|^2}\big(\frac{2d-|e|^2}{2d+|e|^2}\big)^p\delta_{pq}∫d2νπn∣e∣2e−d∣ν∣2/∣e∣2​⟨p∣D(−ν)∣q⟩=2d+∣e∣22/n​(2d+∣e∣22d−∣e∣2​)pδpq​ for Re d>0\mathrm{Re}\,d>0Red>0, e≠0e\ne0e=0.
  6. Eq. (34), last identity: (1/nk)/det⁡[C+G†G/2]=1/((n+1)k−nk)(1/n^k)/\det[C+G^\dagger G/2]=1/((n+1)^k-n^k)(1/nk)/det[C+G†G/2]=1/((n+1)k−nk) for the circulant matrices of (26)–(28).
  7. Eq. (22) with λ0\lambda_0λ0​ of (34): ∣⟨ϕ∣Θ∣ϕ⟩∣≤[(n+1)k−nk]−m∥ϕ∥2|\langle\phi|\Theta|\phi\rangle|\le[(n+1)^k-n^k]^{-m}\|\phi\|^2∣⟨ϕ∣Θ∣ϕ⟩∣≤[(n+1)k−nk]−m∥ϕ∥2 on the kkk-copy space.
  8. Eq. (12): Tr⁡{[Nn⊗m(ρ)]k}≤[(n+1)k−nk]−m\operatorname{Tr}\{[\mathcal N_n^{\otimes m}(\rho)]^k\}\le[(n+1)^k-n^k]^{-m}Tr{[Nn⊗m​(ρ)]k}≤[(n+1)k−nk]−m for every input ρ\rhoρ.

Significance

The identity shows that, for the classical-noise channel, entangled inputs never increase the maximal output kkk-norm: the optimum over mmm uses is attained by unentangled coherent products. Equivalently, the minimum output Rényi entropy of every integer order k≥2k\ge2k≥2 is additive for Nn\mathcal N_nNn​. It was one of the first proofs of the Amosov–Holevo–Werner property for an infinite-dimensional channel, and through the decomposition of Sec. II of the paper it extends to the non-circular classical channels and to the attenuator and amplifier channels with thermal noise.

The paper result is proved; no machine-checked proof exists. A formalization produces Fock-coefficient models of multi-mode displacements and of a Gaussian channel acting on entangled inputs, a Schatten-norm interface on ℓ2\ell^2ℓ2, the multi-mode Weyl relation, and the Gaussian-average identity (A12), all reusable for other bosonic channels.

Difficulty

The lower bound is a computation on coherent inputs. The upper bound must hold for every input of mmm modes, entangled across uses, without any energy constraint, in an infinite-dimensional space. Bounding each use separately does not work: the kkk-th moment of the output is not a product over uses when the input is entangled. The obstruction is removed only after rewriting the moment as an expectation value of an operator on kkk copies of the mmm-mode space and controlling its spectrum, which needs exact Gaussian integrals of displacement matrix elements and an explicit circulant determinant. On the formal side, the traces, functional-calculus powers and series of infinite-dimensional trace-class operators each need their own convergence arguments.

Formalization scope

  • Fock coordinates are occupation strings Fin m → ℕ; operators are coefficient arrays Matrix (Fin m → ℕ) (Fin m → ℕ) ℂ with Xuv=⟨u∣X∣v⟩X_{uv}=\langle u|X|v\rangleXuv​=⟨u∣X∣v⟩; the Hilbert space is lp (fun _ => ℂ) 2. ℓ2(N)⊗m=ℓ2(Nm)\ell^2(\mathbb N)^{\otimes m}=\ell^2(\mathbb N^m)ℓ2(N)⊗m=ℓ2(Nm) replaces the Hilbert tensor product, which Mathlib lacks.
  • Density operators, rank-one arrays and the single-mode displacement and coherent coefficients come from two published platform definition modules (Dependency50.P33, Dependency50.P39).
  • Nn⊗m\mathcal N_n^{\otimes m}Nn⊗m​ is the integral (14) acting on every coefficient array; it is never defined through its values on product or coherent inputs. It is the multi-mode, coefficient-level counterpart of the platform's single-mode operator Claimed50.P39.displacementNoiseChannel, which cannot act on entangled inputs.
  • The noise law is N(0,n/2)⊗N(0,n/2)\mathcal N(0,n/2)\otimes\mathcal N(0,n/2)N(0,n/2)⊗N(0,n/2) in (Re μ,Im μ)(\mathrm{Re}\,\mu,\mathrm{Im}\,\mu)(Reμ,Imμ); at n=0n=0n=0 it is the Dirac mass, so all statements hold for every n≥0n\ge0n≥0. Only (A12) and (34), whose formulas divide by nnn, assume n>0n>0n>0.
  • ∥A∥z=(∑u⟨u∣(A†A)z/2∣u⟩)1/z\|A\|_z=(\sum_u\langle u|(A^\dagger A)^{z/2}|u\rangle)^{1/z}∥A∥z​=(∑u​⟨u∣(A†A)z/2∣u⟩)1/z through the continuous functional calculus; traces, norms and νz\nu_zνz​ take values in [0,∞][0,\infty][0,∞], so no supremum has a junk real value.
  • kkk ranges over all integers k≥1k\ge1k≥1 and zzz over all reals z≥1z\ge1z≥1; the abstract's "greater than two" is not a hypothesis.

A supremum over product, Gaussian or finite-photon inputs, or a channel defined only on coherent states, would make the goal a different and much weaker theorem; νk\nu_kνk​ here ranges over all density operators of the mmm modes.

Contributions welcome: the multi-mode Weyl relation and Gaussian integrals of displacement matrix elements, a trace-class and Schatten-norm library on ℓ2\ell^2ℓ2 of a countable index, and the spectral argument for the operator Θ\ThetaΘ.

Selected references

  • V. Giovannetti, S. Lloyd, Additivity properties of a Gaussian channel, Phys. Rev. A 69, 062307 (2004); arXiv:quant-ph/0403075v3. https://arxiv.org/abs/quant-ph/0403075
  • V. Giovannetti, S. Lloyd, L. Maccone, J. H. Shapiro, B. J. Yen, Minimum Rényi and Wehrl entropies at the output of bosonic channels, Phys. Rev. A 70, 022328 (2004); arXiv:quant-ph/0404037. https://arxiv.org/abs/quant-ph/0404037
  • P. W. Shor, Equivalence of additivity questions in quantum information theory, Commun. Math. Phys. 246, 453 (2004); arXiv:quant-ph/0305035. https://arxiv.org/abs/quant-ph/0305035
  • G. G. Amosov, A. S. Holevo, R. F. Werner, On some additivity problems in quantum information theory, Problems of Information Transmission 36, 305 (2000); arXiv:math-ph/0003002. https://arxiv.org/abs/math-ph/0003002
  • P. Hayden, A. Winter, Counterexamples to the maximal p-norm multiplicativity conjecture for all p > 1, Commun. Math. Phys. 284, 263 (2008); arXiv:0807.4753. https://arxiv.org/abs/0807.4753
  • M. B. Hastings, Superadditivity of communication capacity using entangled inputs, Nature Physics 5, 255 (2009); arXiv:0809.3972. https://arxiv.org/abs/0809.3972
  • V. Giovannetti, A. S. Holevo, R. García-Patrón, A solution of Gaussian optimizer conjecture, Commun. Math. Phys. 334, 1553 (2015); arXiv:1312.2251. https://arxiv.org/abs/1312.2251
  • A. Mari, V. Giovannetti, A. S. Holevo, Quantum state majorization at the output of bosonic Gaussian channels, Nature Communications 5, 3826 (2014); arXiv:1312.3545. https://arxiv.org/abs/1312.3545
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Complexity TheoryInformation TheoryTheoretical Computer Science·Captain: mikedeng1

On the Inherent Intractability of Certain Coding Problems: COSET WEIGHTS (Decoding a Binary Linear Code) and SUBSPACE WEIGHTS (a Codeword of Given Weight) Are NP-CompleteResearch Paper

Motivation

A binary linear code is used on a noisy channel by transmitting codewords and correcting the errors at the receiver. If HHH is a parity-check matrix of the code and yyy is the received word, the receiver computes the syndrome s=yHs = yHs=yH and must find a minimum-weight error pattern zzz with zH=szH = szH=s. A second basic question is whether a code has a codeword of a given weight, which governs its error-correcting ability. For a general code the best known algorithms for both tasks search an exponentially large set.

Berlekamp, McEliece and van Tilborg (IEEE Trans. Inform. Theory 24(3), 1978) showed that both tasks, in their decision form, are NP-complete. The result is the standard explanation of why no efficient general decoder is expected, and it is the hardness assumption behind code-based public-key cryptography (the McEliece cryptosystem, proposed by McEliece in the same year, and its descendants).

Timeline. Karp (1972) listed THREE-DIMENSIONAL MATCHING among 21 NP-complete problems. Berlekamp, McEliece and van Tilborg (1978) reduced it to COSET WEIGHTS and to SUBSPACE WEIGHTS. They left open whether the minimum-distance version ("weight ≤w\le w≤w" in SUBSPACE WEIGHTS) is NP-complete; Vardy proved it in 1997 (IEEE Trans. Inform. Theory 43(6)).

Setting

All vectors and matrices have entries in GF(2)\mathrm{GF}(2)GF(2), and xxx is a row vector: xAxAxA is computed modulo 2, with xxx indexed by the rows of AAA. The Hamming weight ∣x∣|x|∣x∣ is the number of nonzero entries of xxx.

  • COSET WEIGHTS. Input: a binary m×nm \times nm×n matrix AAA, a binary vector yyy of length nnn and a nonnegative integer www. Property: there is xxx with ∣x∣≤w|x| \le w∣x∣≤w and xA=yxA = yxA=y.
  • SUBSPACE WEIGHTS. Input: a binary m×nm \times nm×n matrix AAA and a nonnegative integer www. Property: there is xxx with ∣x∣=w|x| = w∣x∣=w and xA=0xA = 0xA=0.
  • THREE-DIMENSIONAL MATCHING (3DM). Input: a finite set TTT and a set U⊆T×T×TU \subseteq T \times T \times TU⊆T×T×T of triples. Property: there is W⊆UW \subseteq UW⊆U with ∣W∣=∣T∣|W| = |T|∣W∣=∣T∣ in which no two triples agree in any coordinate.

A decision problem is presented to a machine through a fixed binary encoding of its instances. It is in NP if the encodings of its yes-instances form a language with a polynomial-time verifier and polynomially long certificates. It is NP-hard if every language in NP reduces to it by a polynomial-time computable many-one reduction, a map from strings to instances that preserves the answer. It is NP-complete if both hold.

The triple incidence matrix BBB of UUU has one row per triple. With ∣T∣=n|T| = n∣T∣=n and T={0,…,n−1}T = \{0, \dots, n-1\}T={0,…,n−1}, the row of (a,b,c)(a, b, c)(a,b,c) has a 111 in columns aaa, n+bn + bn+b and 2n+c2n + c2n+c and zeros elsewhere. For SUBSPACE WEIGHTS the paper builds, with t=∣U∣t = |U|t=∣U∣, the (3nt+3n+t)×(3nt+3n)(3nt + 3n + t) \times (3nt + 3n)(3nt+3n+t)×(3nt+3n) matrix AAA. Its top ttt rows are BBB followed by 3n3n3n copies of the t×tt \times tt×t identity matrix ItI_tIt​, and its lower 3nt+3n3nt + 3n3nt+3n rows form the identity matrix I3n(t+1)I_{3n(t+1)}I3n(t+1)​.

Formalization targets

Goal

COSET WEIGHTS and SUBSPACE WEIGHTS are both in NP and both NP-hard.\text{COSET WEIGHTS and SUBSPACE WEIGHTS are both in NP and both NP-hard.}COSET WEIGHTS and SUBSPACE WEIGHTS are both in NP and both NP-hard.

Formally: NPCompleteFor encodeCoset CosetWeightsYes ∧ NPCompleteFor encodeSubspace SubspaceWeightsYes, with no hypotheses. This is the paper's abstract and the two conclusions of Section III.

Milestones

  1. 3DM is NP-hard (Karp's problem 17), referenced from the published PricingWithTips.threeDM_np_hard.
  2. A polynomial-time many-one reduction from 3DM makes any encoded problem NP-hard.
  3. COSET WEIGHTS is in NP. SUBSPACE WEIGHTS is in NP.
  4. UUU has a matching iff some ∣T∣|T|∣T∣ rows of BBB have mod 2 sum 11⋯111\cdots111⋯1.
  5. UUU has a matching iff (B, 11⋯1, ∣T∣)(B,\ 11\cdots1,\ |T|)(B, 11⋯1, ∣T∣) is a yes-instance of COSET WEIGHTS, and this instance is computed in polynomial time.
  6. Every xxx with xA=0xA = 0xA=0 satisfies ∣x1∣=∣y∣+3n∣x0∣|x_1| = |y| + 3n|x_0|∣x1​∣=∣y∣+3n∣x0​∣ and ∣x∣=∣y∣+(3n+1)∣x0∣|x| = |y| + (3n+1)|x_0|∣x∣=∣y∣+(3n+1)∣x0​∣, where x0x_0x0​ is the first ttt coordinates of xxx, x1x_1x1​ the remaining 3n(t+1)3n(t + 1)3n(t+1), and y=x0By = x_0 By=x0​B.
  7. ∣x0∣|x_0|∣x0​∣ is the quotient and ∣y∣|y|∣y∣ the remainder of ∣x∣|x|∣x∣ divided by 3n+13n + 13n+1. In particular, ∣x∣=3n2+4n|x| = 3n^2 + 4n∣x∣=3n2+4n forces ∣x0∣=n|x_0| = n∣x0​∣=n and ∣y∣=3n|y| = 3n∣y∣=3n.
  8. UUU has a matching iff (A, 3n2+4n)(A,\ 3n^2 + 4n)(A, 3n2+4n) is a yes-instance of SUBSPACE WEIGHTS, and this instance is computed in polynomial time.

Milestone 7 corrects the paper's wording. Read in order, "they are the remainder and quotient" makes ∣x0∣|x_0|∣x0​∣ the remainder, which is false: n=1n = 1n=1, U={(1,1,1)}U = \{(1,1,1)\}U={(1,1,1)} and xxx the all-ones vector give ∣x∣=7=1⋅4+3|x| = 7 = 1 \cdot 4 + 3∣x∣=7=1⋅4+3 with ∣x0∣=1|x_0| = 1∣x0​∣=1 and ∣y∣=3|y| = 3∣y∣=3. The paper's next sentence uses the correct order.

Significance

The result. NP-completeness of COSET WEIGHTS means that maximum-likelihood decoding of a general binary linear code on the binary symmetric channel is as hard as any problem in NP. Efficient decoders must therefore use structure: algebraic codes, low-density parity checks, list or iterative decoding. NP-completeness of SUBSPACE WEIGHTS shows the same for deciding whether a code has a word of a given weight, and so for computing weight distributions. Code-based cryptography cites these results to support its security assumptions. Later hardness results in coding theory (minimum distance, approximate decoding, decoding with preprocessing) build on the same reduction pattern.

Formalizing it. The result has been proved since 1978, but no machine-checked proof of it exists on this platform. What is published nearby is the NP-hardness of 3DM, in the TM2 framework this mission uses, and the NP-hardness of a gap promise version of binary syndrome decoding (the GapCVP development). The gap result is in a different machine framework, does not include NP membership, and does not cover SUBSPACE WEIGHTS. This mission adds:

  • the two problems with honest encodings;
  • their membership in NP, which needs polynomial-time verifiers built as Mathlib TM2 machines;
  • both reductions, including the weight-counting argument behind the SUBSPACE reduction;
  • a general transfer lemma for NP-hardness along polynomial-time reductions from 3DM, reusable for any further reduction from 3DM in this framework.

Difficulty

The combinatorics is short. The work lies elsewhere.

  • Machine-level complexity. Mathlib states composition of polynomial-time TM2 computations only as proof_wanted. Transferring NP-hardness along a reduction therefore requires composing two TM2 machines with a polynomial time bound. The NP verifiers and the two reduction maps (building BBB and the large matrix AAA from the 3DM table, writing www in binary) must be built as concrete multi-stack machines with step counts. A proof that only shows the maps are computable, or computable by some unspecified algorithm, does not prove these statements.
  • The SUBSPACE direction "weight 3n2+4n3n^2+4n3n2+4n ⇒ matching". A codeword of the right weight need not visibly come from a set of triples. The weight identity and the quotient–remainder argument force ∣x0∣=n|x_0| = n∣x0​∣=n and x0B=11⋯1x_0 B = 11\cdots1x0​B=11⋯1. Since every row of BBB has weight 3, nnn rows summing to a vector of weight 3n3n3n must have disjoint supports, and disjoint supports mean a matching.
  • ≤\le≤ against ===. COSET WEIGHTS asks for weight at most ∣T∣|T|∣T∣, while a matching uses exactly ∣T∣|T|∣T∣ rows. Closing the gap uses the same row-weight count.

Formalization scope

  • Instances. COSET instances are CosetInstance ⟨m,n,A,y,w⟩\langle m, n, A, y, w \rangle⟨m,n,A,y,w⟩ and SUBSPACE instances are SubspaceInstance ⟨m,n,A,w⟩\langle m, n, A, w \rangle⟨m,n,A,w⟩, with A : Matrix (Fin m) (Fin n) (ZMod 2). xAxAxA is Matrix.vecMul x A, and the Hamming weight is hammingNorm.
  • Encodings. encodeCoset and encodeSubspace write mmm and nnn in unary, then the entries bit by bit, then www in binary with a self-delimiting marker code. Unary dimensions keep the certificate length mmm polynomial in the input length. Binary www is the stricter choice for membership and changes nothing for hardness, since the reductions output w=nw = nw=n and w=3n2+4nw = 3n^2 + 4nw=3n2+4n.
  • 3DM. 3DM is the published PricingWithTips.ThreeDMInstance ⟨n,edge⟩\langle n, \mathrm{edge} \rangle⟨n,edge⟩, with TTT = Fin n and UUU = the true entries of the table. Its yes-predicate ThreeDMYes assigns each first coordinate a pair of second and third coordinates, using no second and no third coordinate twice and only triples of UUU. The definition is imported from a market model (PricingWithTips_Model), but only its matching part, the structure Allocation, is used; nothing about markets enters. The triples are listed lexicographically, which fixes the row order of BBB.
  • NP. Membership in NP is the published PricingWithTips.PolynomiallyVerifiable. NP-hardness, NPHardFor, is the published NPHardMarketPredicate generalized from 3DM instances to any encoded instance type. Reductions are many-one maps computed by Turing.TM2ComputableInPolyTime from the input string to the encoding of the produced instance.
  • Ruled out. A reduction given only as a function with an "iff" is not a reduction; any problem reduces to any nontrivial problem that way. Every reduction here carries a polynomial-time TM2 machine.
  • Degenerate instances are kept. With T=∅T = \emptysetT=∅ all three problems answer yes (SUBSPACE with w=0w = 0w=0). With U=∅U = \emptysetU=∅ and n>0n > 0n>0 all answer no. Both cases, and the paper's Example 1, were checked by decide on the definitions.
  • Not formalized. Concluding Remarks 1)–3): full column rank, generator-matrix versions, and the minimum-distance conjecture. Also not formalized is the Section III remark relating the decision problem to finding a minimum-weight solution.
  • Contributions welcome. A general composition lemma for TM2ComputableInPolyTime, and TM2 machines for matrix arithmetic over GF(2)\mathrm{GF}(2)GF(2), are reusable well beyond this mission.

Selected references

  • E. R. Berlekamp, R. J. McEliece, H. C. A. van Tilborg, On the inherent intractability of certain coding problems, IEEE Trans. Inform. Theory 24(3):384–386, 1978. https://doi.org/10.1109/TIT.1978.1055873
  • R. M. Karp, Reducibility among combinatorial problems, in Complexity of Computer Computations, Plenum, 1972, pp. 85–103. https://doi.org/10.1007/978-1-4684-2001-2_9
  • M. R. Garey, D. S. Johnson, Computers and Intractability: A Guide to the Theory of NP-Completeness, Freeman, 1979.
  • A. Vardy, The intractability of computing the minimum distance of a code, IEEE Trans. Inform. Theory 43(6):1757–1766, 1997. https://doi.org/10.1109/18.641542
  • R. J. McEliece, A public-key cryptosystem based on algebraic coding theory, DSN Progress Report 42-44, 1978.
18 thms2 active usersReviewed
Information TheoryQuantum Information·Captain: mikedeng1

Inequalities and Separations among Assisted Capacities of Quantum Channels: The Retrocorrectable Channel R₂,₂ Has Two-Way-Assisted Quantum Capacity Q₂ Exceeding Its One-Shot Holevo Capacity C_HResearch Paper

Motivation

A quantum channel has many capacities, one for each kind of information sent and each auxiliary resource allowed: classical bits or qubits, with or without shared entanglement, with or without a free classical side channel. Comparing these capacities is how quantum Shannon theory locates the value of each resource. Some comparisons look as if they should be trivially ordered. A qubit can carry a classical bit, so one might expect the capacity for quantum information never to exceed the capacity for classical information.

Bennett, Devetak, Shor and Smolin (arXiv:quant-ph/0406086, 2004) show that this expectation fails once classical communication is free. They construct retrocorrectable channels, whose noise can be undone after the fact by combining a classical output of the channel with a reference system entangled with one of its inputs, and they show that for these channels the quantum capacity assisted by two-way classical communication, Q2Q_2Q2​, exceeds the unassisted one-shot Holevo capacity, CHC_HCH​. The one-shot Holevo capacity was the standard single-letter quantity for classical communication at the time (Holevo 1998; Schumacher and Westmoreland 1997). This mission formalizes that headline for the paper's smallest example, the qubit channel R2,2R_{2,2}R2,2​.

Setting

The standard retrocorrectable channel Rc,dR_{c,d}Rc,d​ (Fig. 1, p. 2) has a control input in Cc\mathbb C^cCc, a data input in Cd\mathbb C^dCd, a data output in Cd\mathbb C^dCd, and a classical control output. At each use the channel draws, independently,

  1. a basis B={w1,…,wc}B=\{w_1,\dots,w_c\}B={w1​,…,wc​} of Cc\mathbb C^cCc, the columns of a Haar-random unitary W∈U(c)W\in U(c)W∈U(c), and
  2. unitaries U1,…,Uc∈U(d)U_1,\dots,U_c\in U(d)U1​,…,Uc​∈U(d), each Haar-random.

It measures the control input in the basis BBB, obtaining jjj; applies UjU_jUj​ to the data; emits the data and the classical flag k=(B,U1,…,Uc)k=(B,U_1,\dots,U_c)k=(B,U1​,…,Uc​); and keeps jjj hidden. For a fixed flag, an input operator XXX on Cc⊗Cd\mathbb C^c\otimes\mathbb C^dCc⊗Cd is mapped to

Nk(X)=∑j=1cUj Tr⁡c ⁣[(∣wj⟩⟨wj∣⊗I)X] Uj†.\mathcal N_k(X)=\sum_{j=1}^{c}U_j\,\operatorname{Tr}_c\!\big[(|w_j\rangle\langle w_j|\otimes I)X\big]\,U_j^\dagger .Nk​(X)=j=1∑c​Uj​Trc​[(∣wj​⟩⟨wj​∣⊗I)X]Uj†​.

The paper's example is S=R2,2S=R_{2,2}S=R2,2​.

The one-shot Holevo capacity CHC_HCH​ is the supremum, over finite input ensembles {px,ρx}\{p_x,\rho_x\}{px​,ρx​} of density matrices on the full input, of the entropy of the average output minus the average output entropy, in bits. The flag is part of the output, but it is independent of the input, so this equals the flag average

χ({px,ρx})=Ek[S(∑xpxNk(ρx))−∑xpxS(Nk(ρx))].\chi(\{p_x,\rho_x\})=\mathbb E_k\Big[S\Big(\sum_xp_x\mathcal N_k(\rho_x)\Big)-\sum_xp_xS(\mathcal N_k(\rho_x))\Big].χ({px​,ρx​})=Ek​[S(x∑​px​Nk​(ρx​))−x∑​px​S(Nk​(ρx​))].

The two-way assisted quantum capacity Q2Q_2Q2​ is the supremum of rates RRR such that, for every η>0\eta>0η>0 and all large nnn, Alice can send m≥Rnm\ge Rnm≥Rn qubits to Bob with fidelity at least 1−η1-\eta1−η on every pure message, using the channel exactly nnn times interleaved with unlimited local operations and free classical communication in both directions, and no prior entanglement. Each use's flag becomes known after that use.

Formalization targets

Goal: the separation

CH(R2,2) < Q2(R2,2).C_H(R_{2,2})\ <\ Q_2(R_{2,2}).CH​(R2,2​) < Q2​(R2,2​).

This is the abstract's claim for the paper's witness. It fixes no constant, so it is the most stable form of the result.

Milestones

  1. Echo effect (§3, p. 3). On the maximally entangled state of a reference and the control, measuring the reference in the basis BTB^TBT and the control in BBB yields equal outcomes, with probability δij/c\delta_{ij}/cδij​/c for the pair (i,j)(i,j)(i,j).
  2. Fig. 2 (p. 3). One use of SSS with two-way classical communication implements a noiseless qubit channel: the output equals the input on every one-qubit state.
  3. First bullet of §3 (p. 3): Q2(R2,2)≥1Q_2(R_{2,2})\ge 1Q2​(R2,2​)≥1.
  4. Eq. (1) (p. 2):
CH(R2,2)=1+π2/18−5/6ln⁡2=0.5888.C_H(R_{2,2})=1+\frac{\pi^2/18-5/6}{\ln 2}=0.5888 .CH​(R2,2​)=1+ln2π2/18−5/6​=0.5888.

Significance

The result. The separation shows that free two-way classical communication can raise a channel's quantum capacity above its unassisted one-shot classical capacity. No ordering of the form "quantum ≤ classical" can therefore hold across assistance models without qualification. The paper uses the same family of channels to separate feedback-assisted classical capacity from CHC_HCH​, and it places these examples in a ladder of inequalities among the assisted capacities (§5, Fig. 5). The retrocorrectable channel is a reusable counterexample: its noise is invisible to either party alone and removable by both together.

Formalizing it. The result has a complete informal argument in the paper: eq. (1) is stated with its reduction by symmetry, and the protocol of Fig. 2 is explicit. To our knowledge it has no machine-checked proof. The formal development adds three things: a definition of an operational two-way assisted capacity for channels with a continuous classical output; an exact evaluation of a one-shot Holevo capacity that requires an optimization over all input ensembles, entangled and mixed ones included; and a verified echo-effect identity that is reusable for transpose-trick protocols.

Difficulty

The two sides of the inequality are hard for different reasons.

On the Q2Q_2Q2​ side, Fig. 2 makes the lower bound look immediate, but it must be carried out inside an operational model. Such a model has adaptive instruments, public outcomes, a fresh Haar-distributed flag at each use, and a protocol output that is a measure-theoretic average over the flags. Achievability then requires codes for every large block length.

On the CHC_HCH​ side, the paper's evaluation rests on a symmetry claim: the optimum is attained by a uniform data ensemble with a fixed control input. Proving this means showing that no ensemble does better, including ensembles that entangle control and data. The obvious bound fixes one flag and maximizes, but this fails, because for a fixed flag the channel can be nearly noiseless. The bound must use the average over the Haar flag of the minimum output entropy, and that average is a two-dimensional integral over the overlaps ∣⟨w1∣ψ⟩∣2|\langle w_1|\psi\rangle|^2∣⟨w1​∣ψ⟩∣2 and ∣⟨ϕ∣U1†U2∣ϕ⟩∣2|\langle\phi|U_1^\dagger U_2|\phi\rangle|^2∣⟨ϕ∣U1†​U2​∣ϕ⟩∣2. Its closed form, 5/6−π2/185/6-\pi^2/185/6−π2/18 nats, has to be computed exactly.

Formalization scope

Lean conventions:

  • The flag is a pair (W, U) with W : Matrix.unitaryGroup (Fin c) ℂ (the basis BBB is its columns, whose phases are also revealed; they are independent of the input and change no capacity) and U : Fin c → Matrix.unitaryGroup (Fin d) ℂ.
  • The flag law is the product of the published normalized Haar measures QAlgorithms.Schur.unitaryHaar. The paper's "random" is read as independent Haar, the reading under which eq. (1) holds.
  • Inputs are indexed (control, data), 0-based.
  • Entropies are in bits (QAlgorithms.vnEntropy).
  • CHC_HCH​ is an iSup in ℝ≥0∞ of a lower Lebesgue integral over the flag. Q2Q_2Q2​ is an sSup in ℝ≥0∞ of achievable rates, defined through an inductive predicate of adaptive protocols with an exact count of channel uses.
  • BTB^TBT is the basis of transposed projectors (∣wj⟩⟨wj∣)T(|w_j\rangle\langle w_j|)^T(∣wj​⟩⟨wj​∣)T.

Trivializing formalizations are ruled out:

  • The flag-averaged channel ρ↦EkNk(ρ)\rho\mapsto\mathbb E_k\mathcal N_k(\rho)ρ↦Ek​Nk​(ρ), or any model that discards the flag, has CH=0C_H=0CH​=0 and Q2=0Q_2=0Q2​=0.
  • A non-Haar flag law, a point mass for instance, makes the data channel noiseless and the goal false.
  • Restricting CHC_HCH​ to product, pure or fixed-control inputs would assume the paper's symmetry claim instead of proving it.

None of these is used: the flag is conditioned on in both capacities, the law is Haar, and ensembles range over all density matrices on C2⊗C2\mathbb C^2\otimes\mathbb C^2C2⊗C2.

Needed infrastructure: Haar integration of polynomial and entropy functionals over U(2)U(2)U(2); continuity and concavity of von Neumann entropy; Bochner integration of matrix-valued maps; and the composition and repetition of adaptive protocols. Contributions toward any of these, and toward the general-c,dc,dc,d statements of the paper, are welcome.

Selected references

  • C. H. Bennett, I. Devetak, P. W. Shor, J. A. Smolin, Inequalities and separations among assisted capacities of quantum channels, arXiv:quant-ph/0406086v1, 2004. https://arxiv.org/abs/quant-ph/0406086
  • A. S. Holevo, The capacity of the quantum channel with general signal states, IEEE Trans. Inf. Theory 44(1), 269–273, 1998. https://doi.org/10.1109/18.651037
  • B. Schumacher, M. D. Westmoreland, Sending classical information via noisy quantum channels, Phys. Rev. A 56, 131, 1997. https://doi.org/10.1103/PhysRevA.56.131
  • C. H. Bennett, D. P. DiVincenzo, J. A. Smolin, Capacities of quantum erasure channels, Phys. Rev. Lett. 78, 3217, 1997. https://arxiv.org/abs/quant-ph/9701015
13 thms2 active usersReviewed
Markov ChainOperations ResearchOptimization+1·Captain: mikedeng1

Pricing and Optimization in Shared Vehicle Systems: An Approximation Framework: Elevated-Flow-Relaxation Prices Earn an m/(m+n−1) Fraction of the Optimal State-Dependent ObjectiveResearch Paper

Motivation

Bike-sharing and car-sharing systems, and ride-hailing platforms, all move a fixed fleet of units between stations. Every ride takes a unit away from its origin and leaves it at its destination, so demand that is unbalanced across stations drains some stations and floods others. Pricing is the main lever an operator has: raising the price of rides out of a depleted station throttles the outflow. Choosing such prices optimally is hard, because the optimal policy may react to the full system state, a placement of mmm units over nnn stations, of which there are (m+n−1n−1)\binom{m+n-1}{n-1}(n−1m+n−1​).

Banerjee, Freund and Lykouris (arXiv:1608.06819v4, Operations Research 2022) give an approximation framework for this control problem. Their first result, Theorem 15, shows that one convex program yields state-independent prices whose steady-state performance is within a factor m/(m+n−1)m/(m+n-1)m/(m+n−1) of the best state-dependent policy. The guarantee holds simultaneously for throughput, social welfare and revenue under regular demand.

Timeline. Gordon and Newell (1967) gave the product-form stationary law of closed queueing networks. Whitt (1984) observed that balanced closed networks give every node availability m/(m+n−1)m/(m+n-1)m/(m+n−1). George and Xia (2011) studied availability in vehicle-rental networks via closed queueing networks. Waserhole and Jost (2014) proved the m/(m+n−1)m/(m+n-1)m/(m+n−1) guarantee for throughput. Banerjee, Freund and Lykouris extended it to concave reward curves, and to travel times and other controls.

Setting

There are nnn nodes and mmm units. A state is x∈Sn,m={x∈N0n:∑ixi=m}x\in S_{n,m}=\{x\in\mathbb N_0^n:\sum_ix_i=m\}x∈Sn,m​={x∈N0n​:∑i​xi​=m}. Customers wishing to travel from iii to jjj arrive at node iii at rate φij≥0\varphi_{ij}\ge0φij​≥0. A quantile qij∈[0,1]q_{ij}\in[0,1]qij​∈[0,1] is the fraction of them willing to pay the quoted price. A customer who accepts engages a unit at iii if one is present, moving the system from xxx to x−ei+ejx-e_i+e_jx−ei​+ej​.

A state-dependent policy chooses quantiles qij(x)∈[0,1]q_{ij}(x)\in[0,1]qij​(x)∈[0,1] at every state, with qij(x)=0q_{ij}(x)=0qij​(x)=0 when xi=0x_i=0xi​=0. A stationary law π\piπ is a probability vector on Sn,mS_{n,m}Sn,m​ satisfying the balance equation (1):

π(x)∑i,jφijqij(x)=∑i,jπ(x+ei−ej)φijqij(x+ei−ej).\pi(x)\sum_{i,j}\varphi_{ij}q_{ij}(x)=\sum_{i,j}\pi(x+e_i-e_j)\varphi_{ij}q_{ij}(x+e_i-e_j).π(x)i,j∑​φij​qij​(x)=i,j∑​π(x+ei​−ej​)φij​qij​(x+ei​−ej​).

Rewards are given by per-ride rewards IijI_{ij}Iij​, functions of the quantile, with reward curves Rij(q)=q Iij(q)R_{ij}(q)=q\,I_{ij}(q)Rij​(q)=qIij​(q). The steady-state objective (2) is

Objm(q)=∑x∈Sn,mπ(x)∑i,jφijRij(qij(x)),\mathrm{Obj}_m(q)=\sum_{x\in S_{n,m}}\pi(x)\sum_{i,j}\varphi_{ij}R_{ij}(q_{ij}(x)),Objm​(q)=x∈Sn,m​∑​π(x)i,j∑​φij​Rij​(qij​(x)),

and Optm\mathrm{Opt}_mOptm​ is its best value over all state-dependent policies and their stationary laws.

The elevated flow relaxation (Algorithm 1) drops availability from the objective and adds a flow-conservation constraint:

max⁡q Obj^(q)=∑i,jφijRij(qij)s.t.∑kφkiqki=∑jφijqij ∀i,q∈[0,1]n×n.\max_q\ \widehat{\mathrm{Obj}}(q)=\sum_{i,j}\varphi_{ij}R_{ij}(q_{ij})\quad\text{s.t.}\quad\sum_k\varphi_{ki}q_{ki}=\sum_j\varphi_{ij}q_{ij}\ \forall i,\qquad q\in[0,1]^{n\times n}.qmax​ Obj​(q)=i,j∑​φij​Rij​(qij​)s.t.k∑​φki​qki​=j∑​φij​qij​ ∀i,q∈[0,1]n×n.

A feasible qqq has balanced demand. Its optimum q~\tilde qq~​ is then quoted as a fixed price at every non-empty station.

Formalization targets

Goal: Theorem 15

If every RijR_{ij}Rij​ is concave on [0,1][0,1][0,1], q~\tilde qq~​ is an optimal solution of Algorithm 1 whose support graph {(a,b):a≠b, φabq~ab>0}\{(a,b):a\ne b,\ \varphi_{ab}\tilde q_{ab}>0\}{(a,b):a=b, φab​q~​ab​>0} is strongly connected, and π~\tilde\piπ~ is a stationary law of q~\tilde qq~​, then for every state-dependent policy qqq and every stationary law π\piπ of it,

Objm(q~) ≥ mm+n−1 Objm(q),i.e.Objm(q~)≥mm+n−1Optm.\mathrm{Obj}_m(\tilde q)\ \ge\ \frac{m}{m+n-1}\,\mathrm{Obj}_m(q),\qquad\text{i.e.}\qquad \mathrm{Obj}_m(\tilde q)\ge\frac{m}{m+n-1}\mathrm{Opt}_m.Objm​(q~​) ≥ m+n−1m​Objm​(q),i.e.Objm​(q~​)≥m+n−1m​Optm​.

The connectivity hypothesis is the paper's standing irreducibility assumption, and the printed statement is false without it.

Milestones

These follow the paper's own sequence:

  • Propositions 7 and 8 (demand bounding, supply circulation);
  • Lemma 9, Obj^(q~)≥Optm\widehat{\mathrm{Obj}}(\tilde q)\ge\mathrm{Opt}_mObj​(q~​)≥Optm​;
  • the reduction of a state-independent policy to a Gordon–Newell network (§2.3) and the Gordon–Newell theorem (Theorem 2, an already proved platform theorem);
  • Lemma 3, availability in product-form networks;
  • Lemma 13, a weighted bipartite graph between Sn,mS_{n,m}Sn,m​ and Sn,m−1S_{n,m-1}Sn,m−1​;
  • Lemma 14, Am=rmax⁡Gm−1/Gm≥m/(m+n−1)A_m=r_{\max}G_{m-1}/G_m\ge m/(m+n-1)Am​=rmax​Gm−1​/Gm​≥m/(m+n−1);
  • Proposition 6, infinite-unit availabilities ri/max⁡jrjr_i/\max_jr_jri​/maxj​rj​;
  • Lemma 10, equal availabilities under balanced demand;
  • Lemma 11, Obj∞=Obj^\mathrm{Obj}_\infty=\widehat{\mathrm{Obj}}Obj∞​=Obj​;
  • Lemma 12, Objm=Am Obj∞\mathrm{Obj}_m=A_m\,\mathrm{Obj}_\inftyObjm​=Am​Obj∞​.

Significance

The result. Theorem 15 turns an exponentially large control problem into a convex program with n2n^2n2 variables and a guarantee that does not depend on the arrival rates. The factor m/(m+n−1)m/(m+n-1)m/(m+n−1) tends to 111 as the fleet grows relative to the number of stations. The same framework gives the paper's later results on travel times, rebalancing and constrained pricing. In those settings the balanced-demand shortcut is unavailable and the infinite-unit comparison (Lemmas 12 and 14) carries the argument.

Formalizing it. The theorem is proved in the paper; nothing here is open. The mission produces a machine-checked version and a reusable layer: stationarity of finite-state rate-based chains via balance equations, the identification of state-independent pricing with Gordon–Newell networks, and availability identities for product-form laws. The Gordon–Newell product form itself is already proved on the platform and is referenced, not restated. No result of this paper had a machine-checked proof on the platform when the mission was drafted.

Difficulty

The comparison is against state-dependent policies, which can be reducible and have many stationary laws. Lemma 9 must hold for every one of them, so no product form is available on that side: only the balance equations are.

On the other side, the availability of a state-independent policy depends on the traffic intensities in a way that has no closed form for finite mmm, and the bound m/(m+n−1)m/(m+n-1)m/(m+n−1) must hold uniformly over all of them.

A natural first idea is to compare q~\tilde qq~​ directly with the averaged quantiles of the optimal policy. That idea fails: averaging ignores availability, which is exactly the loss being bounded.

Finally, identifying the stationary law of q~\tilde qq~​ with the uniform law uses irreducibility, which must be derived from the connectivity hypothesis.

Formalization scope

Nodes are Fin n, so the paper's node iii is index i−1i-1i−1. States reuse the closed-network vocabulary of the platform (states, moveState, productForm, normConst, tailMarginal). Laws are real functions on Nn\mathbb N^nNn that vanish off Sn,mS_{n,m}Sn,m​.

Decisions and rewards.

  • Decision variables are quantiles. Value distributions and prices do not appear, and IijI_{ij}Iij​ is any real function of the quantile.
  • Rij(q):=q Iij(q)R_{ij}(q):=q\,I_{ij}(q)Rij​(q):=qIij​(q), so Rij(0)=0R_{ij}(0)=0Rij​(0)=0. Concavity is required on [0,1][0,1][0,1] only.
  • A state-independent qqq enters the mmm-unit system as the policy x↦qij1{xi>0}x\mapsto q_{ij}\mathbf 1\{x_i>0\}x↦qij​1{xi​>0}.

Stationarity and the optimum.

  • Stationarity is the balance equation (1) plus nonnegativity, vanishing off Sn,mS_{n,m}Sn,m​ and total mass 111. Without the total mass, the zero function would satisfy (1).
  • Optm\mathrm{Opt}_mOptm​ is never a supremum: the goal quantifies over every policy and every stationary law, so no junk value of sSup can enter.
  • Policies must vanish at empty stations, so no ride is counted from a station without units.

Ratios and traffic.

  • Ratios are stated as products, e.g. Objm=Am Obj∞\mathrm{Obj}_m=A_m\,\mathrm{Obj}_\inftyObjm​=Am​Obj∞​, so there is no division by an objective.
  • Traffic intensities are solutions of ∑jrjφjiqji=ri∑kφikqik\sum_jr_j\varphi_{ji}q_{ji}=r_i\sum_k\varphi_{ik}q_{ik}∑j​rj​φji​qji​=ri​∑k​φik​qik​.

The milestones that depend on connectivity (Proposition 6, Lemmas 10 and 11) state it as a hypothesis, as the goal does.

The needed infrastructure is finite sums over Sn,mS_{n,m}Sn,m​, Jensen's inequality for concave functions on [0,1][0,1][0,1], and the bridge from the balance equation to the closed-network steady state. Proofs of any milestone, and alternative proofs of the bridge, are welcome.

Selected references

  • S. Banerjee, D. Freund, T. Lykouris, Pricing and Optimization in Shared Vehicle Systems: An Approximation Framework, Operations Research 70(3), 2022; arXiv:1608.06819v4. https://arxiv.org/abs/1608.06819
  • W. J. Gordon, G. F. Newell, Closed Queuing Systems with Exponential Servers, Operations Research 15(2), 1967. https://doi.org/10.1287/opre.15.2.254
  • D. K. George, C. H. Xia, Fleet-sizing and service availability for a vehicle rental system via closed queueing networks, European Journal of Operational Research 211(1), 2011. https://doi.org/10.1016/j.ejor.2010.12.015
  • A. Waserhole, V. Jost, Pricing in vehicle sharing systems: optimization in queuing networks with product forms, EURO Journal on Transportation and Logistics 5(3), 2016. https://doi.org/10.1007/s13676-014-0054-4
  • R. Serfozo, Introduction to Stochastic Networks, Springer, 1999. https://doi.org/10.1007/978-1-4612-1482-3
15 thms2 active usersReviewed
Functional AnalysisLinear algebraQuantum Information·Captain: mikedeng1

The Quantum Chernoff Bound: Tr[A^s B^{1−s}] ≥ Tr[A + B − |A − B|]/2 for All Positive Trace-Class Operators A, B and All 0 ≤ s ≤ 1Research Paper

Motivation

Suppose a quantum system has been prepared nnn times, either always in the state ρ0\rho_0ρ0​ (with prior probability π0\pi_0π0​) or always in the state ρ1\rho_1ρ1​ (with prior π1\pi_1π1​), and the task is to guess which. Helstrom's formula gives the smallest error probability over all measurements,

Pe,min⁡,n=12(1−∥π1ρ1⊗n−π0ρ0⊗n∥1),P_{e,\min,n}=\tfrac12\big(1-\|\pi_1\rho_1^{\otimes n}-\pi_0\rho_0^{\otimes n}\|_1\big),Pe,min,n​=21​(1−∥π1​ρ1⊗n​−π0​ρ0⊗n​∥1​),

and the question is how fast it decays in nnn. Classically, for two probability distributions, the answer is the Chernoff bound ξCB=−log⁡min⁡0≤s≤1∑ip0(i)sp1(i)1−s\xi_{CB}=-\log\min_{0\le s\le1}\sum_i p_0(i)^s p_1(i)^{1-s}ξCB​=−logmin0≤s≤1​∑i​p0​(i)sp1​(i)1−s. The quantum analogue was an open question (Ogawa and Hayashi raised the conjecture). In 2006 two papers settled it together: Nussbaum and Szkoła proved that the exponent is at least −log⁡min⁡sTr⁡[ρ0sρ11−s]-\log\min_s\operatorname{Tr}[\rho_0^s\rho_1^{1-s}]−logmins​Tr[ρ0s​ρ11−s​], and Audenaert, Calsamiglia, Masanes, Muñoz-Tapia, Acín, Bagan and Verstraete (arXiv:quant-ph/0610027) proved the matching upper bound. The upper bound follows at once from a single operator inequality, Theorem 1 of the latter paper, which is the subject of this mission.

Timeline:

  • 1976: Helstrom identifies the optimal one-shot error probability for two quantum states.
  • 2006: Nussbaum and Szkoła prove the lower bound on the exponent, in finite dimension (arXiv:quant-ph/0607216).
  • 2006: Audenaert et al. prove Theorem 1, which gives the upper bound and with it the exact quantum Chernoff exponent; the proof is stated to work in infinite dimensions.

Setting

Let HHH be a complex Hilbert space of any dimension. An operator means a bounded linear map H→HH\to HH→H. A self-adjoint operator AAA is positive, written A≥0A\ge0A≥0, when ⟨v,Av⟩≥0\langle v,Av\rangle\ge0⟨v,Av⟩≥0 for all vvv (positive semidefinite, not necessarily invertible). For self-adjoint XXX the absolute value is ∣X∣=(X∗X)1/2|X|=(X^*X)^{1/2}∣X∣=(X∗X)1/2 and the positive part is X+=(∣X∣+X)/2X_+=(|X|+X)/2X+​=(∣X∣+X)/2.

An operator TTT is trace class when ∑i⟨ei,∣T∣ei⟩<∞\sum_i\langle e_i,|T|e_i\rangle<\infty∑i​⟨ei​,∣T∣ei​⟩<∞ for an orthonormal basis (ei)(e_i)(ei​); its trace is Tr⁡T=∑i⟨ei,Tei⟩\operatorname{Tr}T=\sum_i\langle e_i,Te_i\rangleTrT=∑i​⟨ei​,Tei​⟩. In finite dimension every operator is trace class and Tr⁡\operatorname{Tr}Tr is the matrix trace.

For a positive operator AAA, the support projection ΠA\Pi_AΠA​ is the orthogonal projection onto the closure of the range of AAA. The power AsA^sAs is defined by the functional calculus, x↦xsx\mapsto x^sx↦xs, for s>0s>0s>0, and by A0:=ΠAA^0:=\Pi_AA0:=ΠA​. Writing qPow A s for AsA^sAs and supportProj A for ΠA\Pi_AΠA​, the Lean development uses the same notation as this text.

Formalization targets

Goal: Theorem 1 (p. 2, eq. (4))

For all positive trace-class operators A,BA,BA,B on HHH and all 0≤s≤10\le s\le10≤s≤1,

Tr⁡[AsB1−s] ≥ Tr⁡[A+B−∣A−B∣]2.\operatorname{Tr}\big[A^sB^{1-s}\big]\ \ge\ \frac{\operatorname{Tr}\big[A+B-|A-B|\big]}{2}.Tr[AsB1−s] ≥ 2Tr[A+B−∣A−B∣]​.

Both endpoints are included, with the support-projection convention; the inequality holds in the order of C\mathbb CC, so it asserts that the left side is real.

Milestones

  1. Eq. (9), p. 4, operator form, corrected to 0<t<10<t<10<t<1: At=sin⁡(tπ)π∫0∞xt−1A(A+x)−1dxA^t=\frac{\sin(t\pi)}{\pi}\int_0^\infty x^{t-1}A(A+x)^{-1}dxAt=πsin(tπ)​∫0∞​xt−1A(A+x)−1dx for A≥0A\ge0A≥0.
  2. Resolvent identity, p. 4: A(A+x)−1−B(B+x)−1=∫01ddt(B+tΔ)(B+tΔ+x)−1dt=∫01x(B+tΔ+x)−1Δ(B+tΔ+x)−1dtA(A+x)^{-1}-B(B+x)^{-1}=\int_0^1\frac{d}{dt}(B+t\Delta)(B+t\Delta+x)^{-1}dt=\int_0^1x(B+t\Delta+x)^{-1}\Delta(B+t\Delta+x)^{-1}dtA(A+x)−1−B(B+x)−1=∫01​dtd​(B+tΔ)(B+tΔ+x)−1dt=∫01​x(B+tΔ+x)−1Δ(B+tΔ+x)−1dt, Δ=A−B\Delta=A-BΔ=A−B, x>0x>0x>0.
  3. Eq. (10), p. 5, corrected to C+xC+xC+x invertible: Tr⁡[PB(C+x)−1Δ(C+x)−1]≥0\operatorname{Tr}[PB(C+x)^{-1}\Delta(C+x)^{-1}]\ge0Tr[PB(C+x)−1Δ(C+x)−1]≥0, Δ=C−B\Delta=C-BΔ=C−B, P=Π(C−B)+P=\Pi_{(C-B)_+}P=Π(C−B)+​​.
  4. Lemma 1, p. 3, eq. (5): Tr⁡[PB(At−Bt)]≥0\operatorname{Tr}[PB(A^t-B^t)]\ge0Tr[PB(At−Bt)]≥0 for 0≤t≤10\le t\le10≤t≤1, P=Π(A−B)+P=\Pi_{(A-B)_+}P=Π(A−B)+​​.
  5. Maximum principle, p. 3: Tr⁡[K+]=max⁡QTr⁡[QK]\operatorname{Tr}[K_+]=\max_Q\operatorname{Tr}[QK]Tr[K+​]=maxQ​Tr[QK] over orthogonal projections QQQ, for self-adjoint trace-class KKK.
  6. Half-range inequality, p. 3: Tr⁡[a−asb1−s]≤Tr⁡[(a−b)+]=Tr⁡[(a−b)+∣a−b∣]/2\operatorname{Tr}[a-a^sb^{1-s}]\le\operatorname{Tr}[(a-b)_+]=\operatorname{Tr}[(a-b)+|a-b|]/2Tr[a−asb1−s]≤Tr[(a−b)+​]=Tr[(a−b)+∣a−b∣]/2 for 0≤s≤120\le s\le\frac120≤s≤21​.

Significance

With A=π1ρ1⊗nA=\pi_1\rho_1^{\otimes n}A=π1​ρ1⊗n​ and B=π0ρ0⊗nB=\pi_0\rho_0^{\otimes n}B=π0​ρ0⊗n​ the right side of (4) is Pe,min⁡,nP_{e,\min,n}Pe,min,n​ and the left side factorizes as π1sπ01−s(Tr⁡[ρ1sρ01−s])n\pi_1^s\pi_0^{1-s}(\operatorname{Tr}[\rho_1^s\rho_0^{1-s}])^nπ1s​π01−s​(Tr[ρ1s​ρ01−s​])n, so Theorem 1 gives the upper bound on the quantum Chernoff exponent independently of the priors. Beyond hypothesis testing, the inequality lower-bounds the trace norm ∥A−B∥1\|A-B\|_1∥A−B∥1​ by a multiplicative quantity; it underlies the bounds 1−Q≤T≤1−Q21-Q\le T\le\sqrt{1-Q^2}1−Q≤T≤1−Q2​ between the trace distance and the non-logarithmic Chernoff quantity QQQ (eq. (6) of the paper), and later work on error exponents and Rényi divergences builds on it.

The result is proved. What this mission adds is a machine-checked proof at the generality the paper claims: trace-class operators on an arbitrary Hilbert space, both endpoints, and reality of the trace. The platform already holds a proved special case (Claimed50.P15.proposition_1_1): positive-definite matrices, with A0=1A^0=1A0=1 and a comparison of real parts only. That case does not reach singular states, which are the interesting ones (pure states have rank one), nor infinite dimension.

Difficulty

The matrices AsA^sAs and B1−sB^{1-s}B1−s do not commute, so the scalar inequality asb1−s≥min⁡(a,b)a^sb^{1-s}\ge\min(a,b)asb1−s≥min(a,b) cannot be applied eigenvalue by eigenvalue; diagonalizing AAA and BBB separately and comparing spectra fails, because Tr⁡[AsB1−s]\operatorname{Tr}[A^sB^{1-s}]Tr[AsB1−s] depends on the relative position of the eigenbases. Operator monotonicity of x↦xtx\mapsto x^tx↦xt alone gives nothing either, since A≥BA\ge BA≥B fails in general. The paper's route goes through a trace inequality with a projection fixed by A−BA-BA−B, and every step must be carried out for operators that need not be invertible, with the endpoint cases s∈{0,1}s\in\{0,1\}s∈{0,1} handled separately because the integral representation (9) degenerates there.

In infinite dimension there is a further gap: the proof applies Lemma 1 to a1−sa^{1-s}a1−s and b1−sb^{1-s}b1−s, which are in the Schatten class S1/(1−s)S_{1/(1-s)}S1/(1−s)​ but not trace class when a,ba,ba,b have infinite rank. A complete proof must bridge it, for example by finite-rank compression or by a Schatten-class form of Lemma 1.

Formalization scope

Operators are H →L[ℂ] H for [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]; no finite dimension or separability is assumed. Positivity is Mathlib's Loewner order 0 ≤ A. Powers for s>0s>0s>0 are CFC.rpow; ∣X∣|X|∣X∣ is CFC.abs X =X∗X=\sqrt{X^*X}=X∗X​ and X+X_+X+​ is X⁺ from the continuous functional calculus. The zeroth power is the support projection supportProj A, the orthogonal projection onto the closure of the range (Mathlib's A ^ (0:ℝ) = 1 is not used). Trace class and trace are the published platform definitions IsModulusTraceClass and basisOperatorTrace (module QAlgorithms_Papers_Independent_Next46_P02, scalar field C\mathbb CC). Every operator whose trace is taken is trace class under the stated hypotheses, so no trace is a junk value of a divergent sum. Inequalities between traces are in ComplexOrder. Inverses are Ring.inverse, used only where the operator is invertible (for x>0x>0x>0, or under the explicit invertibility hypothesis of (10)).

Two encodings would trivialize the goal and are excluded: dropping the trace-class hypotheses (a divergent trace is 000 in Lean, so the inequality could hold by junk), and the zeroth power A0=1A^0=1A0=1 (which makes the endpoints weaker than the paper's). The statements of (9) and (10) are corrected where the printed ranges are false: (9) fails at t∈{0,1}t\in\{0,1\}t∈{0,1}, and (10) is undefined at x=0x=0x=0 for singular CCC.

Infrastructure a complete development needs: basis independence and cyclicity of the trace on trace-class operators, Hölder's inequality for Schatten classes, operator integrals of resolvents, and strong convergence At→ΠAA^t\to\Pi_AAt→ΠA​ as t→0+t\to0^+t→0+. These are reusable well beyond this mission. Contributions are welcome on any milestone, on that trace-class infrastructure, and on the finite-dimensional case of each milestone as a stepping stone.

Selected references

  • K. M. R. Audenaert, J. Calsamiglia, Ll. Masanes, R. Muñoz-Tapia, A. Acín, E. Bagan, F. Verstraete, The Quantum Chernoff Bound, arXiv:quant-ph/0610027v1, 2006; Phys. Rev. Lett. 98, 160501 (2007). https://arxiv.org/abs/quant-ph/0610027
  • M. Nussbaum, A. Szkoła, The Chernoff lower bound for symmetric quantum hypothesis testing, Ann. Statist. 37 (2009), 1040–1057. https://arxiv.org/abs/quant-ph/0607216
  • C. W. Helstrom, Quantum Detection and Estimation Theory, Academic Press, 1976.
  • T. Ogawa, M. Hayashi, On error exponents in quantum hypothesis testing, IEEE Trans. Inf. Theory 50 (2004), 1368–1372. https://arxiv.org/abs/quant-ph/0206151
  • R. Bhatia, Matrix Analysis, Springer GTM 169, 1997. https://doi.org/10.1007/978-1-4612-0653-8
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Universal recovery map for approximate Markov chainsResearch Paper

Motivation

A central question in quantum information theory is to determine how well lost information can be reconstructed. Crucially, the corresponding recovery operation should perform well without knowing the information to be reconstructed. In this work, we show that the quantum conditional mutual information measures the performance of such recovery operations. More precisely, we prove that the conditional mutual information I(A:C∣B)I(A:C|B)I(A:C∣B) of a tripartite quantum state ρABCρ_{ABC}ρABC​ can be bounded from below by its distance to the closest recovered state RB→BC(ρAB)\mathcal{R}_{B \to BC}(ρ_{AB})RB→BC​(ρAB​), where the CCC-part is reconstructed from the BBB-part only and the recovery map RB→BC\mathcal{R}_{B \to BC}RB→BC​ merely depends on ρBCρ_{BC}ρBC​. One particular application of this result implies the equivalence between two different approaches to define topological order in quantum systems.

This mission is the statement-level formalization of Universal recovery map for approximate Markov chains (arXiv:1504.07251v3). 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 Commuting rotations give a state-dependent linear recovery bound (Lemma 6.1, PDF p. 19). 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

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

  • Theorem 2.1: universal recovery for separable systems: Extended CMI and a coordinate-to-bounded-operator realization compatible with recovery, tensor action and marginals (hard)
  • Remark 2.2: measured-relative-entropy strengthening: Extended CMI and realized finite-channel amplification on arbitrary separable ancillas (hard)
  • Remark 2.3: the universal map recovers its prescribed marginal: Universal-validity predicate built from realized coordinate recovery and extended CMI (hard)
  • Corollary 2.4: linear bound and unital recovery structure: Realized separable recovery, extended CMI and the supported finite unital structure (hard)
  • Remark 2.5: commuting-unitary mixture for the linear bound: Realized universal recovery and an integrable probability mixture of supported rotated transpose maps (hard)
  • Remark 2.5: semidefinite optimization and efficiency claim: Remark 2.5: semidefinite optimization and efficiency claim (source-ambiguity)
  • Remark 2.5: generic replacement by imaginary powers: Remark 2.5: generic replacement by imaginary powers (source-ambiguity)
  • Example 2.6: product marginal and unique transpose recovery: Realization-compatible product recovery, extended CMI and universal supported uniqueness (hard)
  • §3, eq.(15): topological-order application: §3, eq.(15): topological-order application (source-ambiguity)
  • Proposition 4.1: pointwise-to-universal minimax principle: Proposition 4.1: pointwise-to-universal minimax principle (source-ambiguity)
  • Lemma 4.2: measured-entropy slack properties: Realization-compatible CMI, measured entropy, flagged mixtures and slack topology (hard)
  • Lemma 5.1: uniform comparison under normalized BC compression: Realized local tensor projections, positive-trace joint compression and extended-CMI slack (hard)
  • Lemma 5.2: compression of approximately marginal-preserving channels: Realized input/output channel compression and fixed-marginal slack infima (hard)
  • Lemma 5.3: trace retained by a compressed channel: Realized channel action compatible with arbitrary local projections and marginals (hard)
  • Lemma 6.2: linear fidelity slack properties: Realized flagged tensor action, CMI and trace-norm topology for arbitrary separable ancillas (hard)
  • §7: conditional universal relative-entropy improvement: Realization-compatible global extension family and relative-entropy recovery slack (hard)
  • Lemma C.4: fidelity continuous in a finite-dimensional recovery map: Operator realization of coordinate amplification and its root fidelity on arbitrary separable ancillas (hard)
  • Lemma C.5: continuity of a channel tensored with identity: Cross-system operator realization of coordinate amplification and compatible trace-norm topology (hard)
  • Lemma E.1: fidelity with a projected positive operator: Realized tensor-local projections and normalization compatible with local root fidelity (hard)
  • Lemma E.3: fixed-marginal finite-support approximations: Arbitrary bounded local projections acting on coordinate states with exact-marginal support slices (hard)
  • Appendix F: additional fourth-root counterexample claim: Full-scope separable-system transpose recovery and fidelity comparison, compatible with the accepted coordinate tensor model (hard)

Selected references

  • Universal recovery map for approximate Markov chains, arXiv:1504.07251v3, https://arxiv.org/abs/1504.07251v3
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Unconstrained distillation capacities of a pure-loss bosonic broadcast channelResearch Paper

Motivation

Bosonic channels are important in practice as they form a simple model for free-space or fiber-optic communication. Here we consider a single-sender two-receiver pure-loss bosonic broadcast channel and determine the unconstrained capacity region for the distillation of bipartite entanglement and secret key between the sender and each receiver, whenever they are allowed arbitrary public classical communication. We show how the state merging protocol leads to achievable rates in this setting, giving an inner bound on the capacity region. We also evaluate an outer bound on the region by using the relative entropy of entanglement and a `reduction by teleportation' technique. The outer bounds match the inner bounds in the infinite-energy limit, thereby establishing the unconstrained capacity region for such channels. Our result could provide a useful benchmark for implementing a broadcasting of entanglement and secret key through such channels. An important open question relevant to practice is to determine the capacity region in both this setting and the single-sender single-receiver case when there is an energy constraint on the transmitter.

This mission is the statement-level formalization of Unconstrained distillation capacities of a pure-loss bosonic broadcast channel (arXiv:1601.05563v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

3 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Actual TMSV broadcast conditional entropies and their unconstrained limits (Appendix after (29); Section III.A, (12)-(13), p.3, 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

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

  • Theorem 1, (4)-(6): Unrestricted bosonic joint entanglement/private-state operational capacity region (hard)
  • Theorem 2, (27): Arbitrary-m unrestricted joint Bell/private distillation region and its cut theorem (hard)
  • Section III.A, (8)-(10); Appendix (28)-(29): Bosonic reverse state-merging distillation protocols for finite-energy TMSV resources (hard)
  • Remark 3: Sequential reverse-merging execution and absence of entanglement borrowing at every stage (hard)
  • Section III.B displacement covariance and teleportation reduction: Normalized continuous-variable teleportation instruments and actual adaptive broadcast-output reduction (hard)
  • Section III.B, (17)-(20); Appendix (31): Energy limit and ordered operational interpretation in (17)-(20)/(31) (source-ambiguity)

Selected references

  • Unconstrained distillation capacities of a pure-loss bosonic broadcast channel, arXiv:1601.05563v3, https://arxiv.org/abs/1601.05563v3
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Multiparty Quantum Mutual Information: An alternative definitionResearch Paper

Motivation

Mutual information is the reciprocal information that is common to or shared by two or more parties. Quantum mutual information for bipartite quantum systems is non-negative, and bears the interpretation of total correlation between the two subsystems. This may, however, no longer be true for three or more party quantum systems. In this paper, we propose an alternative definition of multipartite information taking into account the shared information between two and more parties. It is non-negative, observes monotonicity under partial trace as well as completely positive maps, and equals multipartite information measure in literature for pure states. We then define multiparty quantum discord, and give some examples. Interestingly, we observe that quantum discord increases when measurement is performed on a large number of subsystems. Consequently, the symmetric quantum discord, which involves measurement on all parties, reveals the maximal quantumness. This raises question on the interpretation of measured mutual information as classical correlation.

This mission is the statement-level formalization of Multiparty Quantum Mutual Information: An alternative definition (arXiv:1504.07176v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

8 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Alternative multipartite information is nonnegative (Theorem 1, 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

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

  • Theorem 3: Locality and trace normalization of the claimed operation (source-ambiguity)
  • Equation (11), final equality: Replica-space identification and valid support containment for equation (11) (source-ambiguity)
  • Equation (12), final equality: Replica-space identification and matching marginals in equation (12) (source-ambiguity)
  • Equation (13), last line: General tensor-power representation of complementary marginal entropy sum (source-ambiguity)
  • Equation (14), numerical n=3,4 claim and saturation: A valid domain and a specified pair-index set for the numerical bound (source-ambiguity)
  • Figure 2(c) caption: Normalized noisy three-qutrit family in Figure 2(c) (source-ambiguity)

Selected references

  • Multiparty Quantum Mutual Information: An alternative definition, arXiv:1504.07176v2, https://arxiv.org/abs/1504.07176v2
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Concentrating Partial Entanglement by Local OperationsResearch Paper

Motivation

If two separated observers are supplied with entanglement, in the form of nnn pairs of particles in identical partly-entangled pure states, one member of each pair being given to each observer; they can, by local actions of each observer, concentrate this entanglement into a smaller number of maximally-entangled pairs of particles, for example Einstein-Podolsky-Rosen singlets, similarly shared between the two observers. The concentration process asymptotically conserves {\em entropy of entanglement}---the von Neumann entropy of the partial density matrix seen by either observer---with the yield of singlets approaching, for large nnn, the base-2 entropy of entanglement of the initial partly-entangled pure state. Conversely, any pure or mixed entangled state of two systems can be produced by two classically-communicating separated observers, drawing on a supply of singlets as their sole source of entanglement.

This mission is the statement-level formalization of Concentrating Partial Entanglement by Local Operations (arXiv:quant-ph/9511030v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

18 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Entropy-efficient exact singlet concentration (Abstract, §I: asymptotically efficient concentration of pure entanglement, 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

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

  • §III, Eqs.(7),(9): batching reaches near powers of two: An IID binomial type-history process, positive-time near-power hitting/stopping events, and its physically counted stopped-batch singlet-efficiency functional. (hard)
  • §IV: two-sided QDC is not entanglement concentration: A complete largest-eigenvalue compressed two-sided state with rounded/capped dimension, fixed spectral tie order, positive-success normalization, and same-dimension Bell/Haar teleportation fidelity. (hard)
  • §IV: growth of Schmidt-coefficient variance: The probability distribution and scaling underlying the asserted Schmidt-coefficient variance. (source-ambiguity)
  • §IV footnote 1: majority-up encoding and marginal spectra: The input ensemble determining the majority-up marginal density matrices. (source-ambiguity)
  • §IV: quantum compression followed by concentration and teleportation: A typed source-averaged compression/concentration/teleportation composition with a deterministic compressed-qubit requirement, heralded concentration supply, and separated classical-message accounting. (hard)

Selected references

  • Concentrating Partial Entanglement by Local Operations, arXiv:quant-ph/9511030v1, https://arxiv.org/abs/quant-ph/9511030v1
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Compression of sources of probability distributions and density operatorsResearch Paper

Motivation

We study the problem of efficient compression of a stochastic source of probability distributions. It can be viewed as a generalization of Shannon's source coding problem. It has relation to the theory of common randomness, as well as to channel coding and rate--distortion theory: in the first two subjects ``inverses'' to established coding theorems can be derived, yielding a new approach to proving converse theorems, in the third we find a new proof of Shannon's rate--distortion theorem. After reviewing the known lower bound for the optimal compression rate, we present a number of approaches to achieve it by code constructions. Our main results are: a better understanding of the known lower bounds on the compression rate by means of a strong version of this statement, a review of a construction achieving the lower bound by using common randomness which we complement by showing the optimal use of the latter within a class of protocols. Then we review another approach, not dependent on common randomness, to minimizing the compression rate, providing some insight into its combinatorial structure, and suggesting an algorithm to optimize it. The second part of the paper is concerned with the generalization of the problem to quantum information theory: the compression of mixed quantum states. Here, after reviewing the known lower bound we contribute a strong version of it, and discuss the relation of the problem to other issues in quantum information theory.

This mission is the statement-level formalization of Compression of sources of probability distributions and density operators (arXiv:quant-ph/0208131v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

17 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Common-randomness compression with typical-word guarantees (Theorem 9, 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

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

  • Question 4: Unconditional no-shared-randomness block-error achievability at mutual information. (source-ambiguity)
  • Question 4': Ordinary block-error compression with simultaneous typical-word fidelity at mutual information. (source-ambiguity)
  • Section VI.C: A source-pinned multi-constraint rate-distortion formula with precise feasible set and boundary approximation convention. (source-ambiguity)
  • Conjecture 23: Proved quantum visible compression with the stated communication and randomness rates. (source-ambiguity)
  • Question 24: Unconditional quantum fixed-error compression equality at Holevo information. (source-ambiguity)

Selected references

  • Compression of sources of probability distributions and density operators, arXiv:quant-ph/0208131v1, https://arxiv.org/abs/quant-ph/0208131v1
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Quantum Channel Capacity of Very Noisy ChannelsResearch Paper

Motivation

We present a family of additive quantum error-correcting codes whose capacities exceeds that of quantum random coding (hashing) for very noisy channels. These codes provide non-zero capacity in a depolarizing channel for fidelity parameters fff when f>.80944f> .80944f>.80944. Random coding has non-zero capacity only for f>.81071f>.81071f>.81071; by analogy to the classical Shannon coding limit, this value had previously been conjectured to be a lower bound. We use the method introduced by Shor and Smolin of concatenating a non-random (cat) code within a random code to obtain good codes. The cat code with block size five is shown to be optimal for single concatenation. The best known multiple-concatenated code we found has a block size of 25. We derive a general relation between the capacity attainable by these concatenation schemes and the coherent information of the inner code states.

This mission is the statement-level formalization of Quantum Channel Capacity of Very Noisy Channels (arXiv:quant-ph/9706061v3). 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 Five-in-five cat concatenation strictly improves hashing (Abstract and Section V.B: five-in-five concatenation improves the hashing threshold, PDF p. 19). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Section V.A, Eqs. (40)-(41): two claimed asymptotic contributions: The central-syndrome partial contribution, its index window, the constant c, and the intended asymptotic equivalence including polynomial prefactors. (source-ambiguity)
  • Numerical reports: Table I, five-in-five, and note [36]: Certified precision or a rounding convention for Table I, the five-in-five threshold, and reference note [36]. (source-ambiguity)
  • Section VI: limited Monte-Carlo search observation: A specified Monte-Carlo search experiment: sampled code set, fidelity range, sampling distribution, transcript, and stopping rule. (source-ambiguity)
  • Section VI: proposed extension to generalized depolarizing channels: A precise generalized-channel or k>1 extension, with modified weight polynomials and operational statement. (source-ambiguity)
  • Reference note [20]: typical hashing distance heuristic: A probability model and limit quantifiers for “typical,” an asymptotic error statement, and an exact meaning of coefficient .8. (source-ambiguity)

Selected references

  • Quantum Channel Capacity of Very Noisy Channels, arXiv:quant-ph/9706061v3, https://arxiv.org/abs/quant-ph/9706061v3
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Classical capacity of a noiseless quantum channel assisted by noisy entanglementResearch Paper

Motivation

We derive the general formula for the capacity of a noiseless quantum channel assisted by an arbitrary amount of noisy entanglement. In this capacity formula, the ratio of the quantum mutual information and the von Neumann entropy of the sender's share of the noisy entanglement plays the role of mutual information in the completely classical case. A consequence of our results is that bound entangled states cannot increase the capacity of a noiseless quantum channel.

This mission is the statement-level formalization of Classical capacity of a noiseless quantum channel assisted by noisy entanglement (arXiv:quant-ph/0106080v3). 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 Full noisy-entanglement-assisted capacity with the unassisted baseline (Eqs. (3),(4),(6),(15); abstract, 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

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

  • Eqs. (7),(9); compare Eq. (6) on p.3: A source-consistent identification of the unrestricted fixed-(d,n) operational capacity from Eq. (6) with a regularized finite Holevo objective, or an explicitly justified restriction to independent-letter encoders. (source-ambiguity)

Selected references

  • Classical capacity of a noiseless quantum channel assisted by noisy entanglement, arXiv:quant-ph/0106080v3, https://arxiv.org/abs/quant-ph/0106080v3
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Bidirectional coherent classical communicationResearch Paper

Motivation

A unitary interaction coupling two parties enables quantum communication in both the forward and backward directions. Each communication capacity can be thought of as a tradeoff between the achievable rates of specific types of forward and backward communication. Our first result shows that for any bipartite unitary gate, coherent classical communication is no more difficult than classical communication -- they have the same achievable rate regions. Previously this result was known only for the unidirectional capacities (i.e., the boundaries of the tradeoff). We then relate the tradeoff curve for two-way coherent communication to the tradeoff for two-way quantum communication and the tradeoff for coherent communiation in one direction and quantum communication in the other.

This mission is the statement-level formalization of Bidirectional coherent classical communication (arXiv:quant-ph/0412126v3). 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 Bidirectional coherification with arbitrary signed entanglement (Theorem 1, Eqs. (2)–(3), 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

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

  • §IV: RRE = CCE: A source-pinned signed independent bidirectional RSP task: state-family/block convention, description uniformity, consumed remote-preparation call semantics, and counted catalytic startup. (source-ambiguity)

Selected references

  • Bidirectional coherent classical communication, arXiv:quant-ph/0412126v3, https://arxiv.org/abs/quant-ph/0412126v3
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Quantum Information·Captain: Goku

Characterization of convex μμμ-compact setsResearch Paper

Motivation

The class of μμμ-compact sets can be considered as a natural extension of the class of compact metrizable subsets of locally convex spaces, to which the particular results well known for compact sets can be generalized. This class contains all compact sets as well as many noncompact sets widely used in applications. In this paper we give a characterization of a convex μμμ-compact set in terms of properties of functions defined on this set. Namely, we prove that the class of convex μμμ-compact sets can be characterized by continuity of the operation of convex closure of a function (= the double Fenchel transform) with respect to monotonic pointwise converging sequences of continuous bounded and of lower semicontinuous lower bounded functions.

This mission is the statement-level formalization of Characterization of convex μμμ-compact sets (arXiv:1004.3792v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

7 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Monotone continuity characterizes convex µ-compact sets (Theorem, PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Selected references

  • Characterization of convex μμμ-compact sets, arXiv:1004.3792v1, https://arxiv.org/abs/1004.3792v1
11 thms2 active usersReviewed
Quantum Information·Captain: Goku

On some additivity problems in quantum information theoryResearch Paper

Motivation

A class of problems in quantum information theory, having an elementary formulation but still resisting solution, concerns the additivity properties of various quantities characterizing quantum channels, notably the "classical capacity", and the "maximal output purity". All known results, including extensive numerical work, are consistent with the conjecture that these quantities are indeed additive (resp. multiplicative) with respect to tensor products of channels. A proof of this conjecture would have important consequences in quantum information theory. In particular, according to this conjecture, the classical capacity or the maximal purity of outputs cannot be increased by using entangled inputs of the channel. In this paper we state the additivity/multiplicativity problems, give some relations between them, and prove some new partial results, which also support the conjecture.

This mission is the statement-level formalization of On some additivity problems in quantum information theory (arXiv:math-ph/0003002v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

14 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Depolarizing products: multiplicativity and explicit purities (§5, Theorem (i)-(iii): multiplicativity and explicit depolarizing purities, PDF p. 11). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Lemma (9), minus-infinity branch: A valid identity-ancilla equality for the source minimum least output eigenvalue including singular outputs. (source-ambiguity)
  • Quantitative remainder sentence after (15)-(16): An exact spectral-deficit premise or quantitative rate and sign condition on the arbitrary initial little-o term. (source-ambiguity)

Selected references

  • On some additivity problems in quantum information theory, arXiv:math-ph/0003002v2, https://arxiv.org/abs/math-ph/0003002v2
21 thms2 active usersReviewed
Quantum Information·Captain: Goku

Theoretical Guarantees for Permutation-Equivariant Quantum Neural NetworksResearch Paper

Motivation

Despite the great promise of quantum machine learning models, there are several challenges one must overcome before unlocking their full potential. For instance, models based on quantum neural networks (QNNs) can suffer from excessive local minima and barren plateaus in their training landscapes. Recently, the nascent field of geometric quantum machine learning (GQML) has emerged as a potential solution to some of those issues. The key insight of GQML is that one should design architectures, such as equivariant QNNs, encoding the symmetries of the problem at hand. Here, we focus on problems with permutation symmetry (i.e., the group of symmetry SnS_nSn​), and show how to build SnS_nSn​-equivariant QNNs. We provide an analytical study of their performance, proving that they do not suffer from barren plateaus, quickly reach overparametrization, and generalize well from small amounts of data. To verify our results, we perform numerical simulations for a graph state classification task. Our work provides the first theoretical guarantees for equivariant QNNs, thus indicating the extreme power and potential of GQML.

This mission is the statement-level formalization of Theoretical Guarantees for Permutation-Equivariant Quantum Neural Networks (arXiv:2210.09974v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

17 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 1 (Variance of partial derivatives) (Theorem 1 (Variance of partial derivatives); seed paper result, 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

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

  • Corollary 1 (Dataset condition claimed to prevent barren plateaus): A nonzero lower bound on generator-times-observable Delta in a data-bearing sector (source-ambiguity)
  • Unnumbered architecture-wide absence of barren plateaus; Eq.(18): Valid uniform sectorwise scaling including normalization and scalar sectors (source-ambiguity)
  • Unnumbered extension of Eq.(16) to general compact groups: Independent cross-sector conjugation moments for general compact-group representations (hard)
  • Example 1 (Dataset cancellation versus individual trainability): Consistent coefficients and exact Delta in the mixed-sign symmetric-basis example (source-ambiguity)
  • Unnumbered fixed Hamming-weight encoding guarantees, Eqs.(72)–(75): Correct orbit-stabilizer projector and distinct overlap versus Delta expectation (source-ambiguity)
  • Theorem 8 (Claimed VC bound for general equivariant channels): A fixed parameter-independent input feature map for the asserted output-dimension VC bound (source-ambiguity)
  • Unnumbered strong anti-concentration estimate, Eq.(100): A valid anti-concentration hypothesis or inequality replacing reversed Chebyshev (source-ambiguity)
  • Unnumbered extension claimed for equivariant data re-uploading: Specified data-dependent class, upload schedule and parameter moment law (hard)
  • Unnumbered run-time scaling in the Supplementary Note: A specified cost and accuracy model for the source QNN runtime claim (source-ambiguity)

Selected references

  • Theoretical Guarantees for Permutation-Equivariant Quantum Neural Networks, arXiv:2210.09974v3, https://arxiv.org/abs/2210.09974v3
22 thms2 active usersReviewed
Quantum Information·Captain: Goku

Multiplicativity of maximal output purities of Gaussian channels under Gaussian inputsResearch Paper

Motivation

We address the question of the multiplicativity of the maximal p-norm output purities of bosonic Gaussian channels under Gaussian inputs. We focus on general Gaussian channels resulting from the reduction of unitary dynamics in larger Hilbert spaces. It is shown that the maximal output purity of tensor products of single-mode channels under Gaussian inputs is multiplicative for any p>1 for products of arbitrary identical channels as well as for a large class of products of different channels. In the case of p=2 multiplicativity is shown to be true for arbitrary products of generic channels acting on any number of modes.

This mission is the statement-level formalization of Multiplicativity of maximal output purities of Gaussian channels under Gaussian inputs (arXiv:quant-ph/0406065v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

11 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Abstract/main result: Gaussian maximal-output-purity multiplicativity (Abstract/main result: Gaussian maximal-output-purity multiplicativity, 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

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

  • Proposition 1, unrestricted second sentence; reiterated PDF p.8: A valid unrestricted actual Gaussian optimizer and output-majorization statement for singular channels. (source-ambiguity)
  • Appendix B, (B6): A correct first-variation formula including normalization and repeated symplectic eigenvalues. (source-ambiguity)

Selected references

  • Multiplicativity of maximal output purities of Gaussian channels under Gaussian inputs, arXiv:quant-ph/0406065v1, https://arxiv.org/abs/quant-ph/0406065v1
15 thms2 active usersReviewed
Quantum Information·Captain: Goku

Sending Quantum Information with Gaussian StatesResearch Paper

Motivation

Quantum information characteristics, such as quantum mutual information, loss, noise and coherent information are explicitly calculated for Bosonic attenuation/amplification channel with input Gaussian state. The coherent information is shown to be negative for the values of the attenuation coefficient k<1/2k<1/\sqrt{2}k<1/2​.

This mission is the statement-level formalization of Sending Quantum Information with Gaussian States (arXiv:quant-ph/9809022v1). 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 Thermal output and the three entropies (§4, unnumbered main result: thermal output and all three entropies, PDF p. 9). 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:

  • §4, qualitative information-triangle dominance: A mathematical definition of information-triangle dominance and the printed regime k ÷ 1 (source-ambiguity)

Selected references

  • Sending Quantum Information with Gaussian States, arXiv:quant-ph/9809022v1, https://arxiv.org/abs/quant-ph/9809022v1
10 thms2 active usersReviewed
Quantum Information·Captain: Goku

A Fully Quantum Asymptotic Equipartition PropertyResearch Paper

Motivation

The classical asymptotic equipartition property is the statement that, in the limit of a large number of identical repetitions of a random experiment, the output sequence is virtually certain to come from the typical set, each member of which is almost equally likely. In this paper, we prove a fully quantum generalization of this property, where both the output of the experiment and side information are quantum. We give an explicit bound on the convergence, which is independent of the dimensionality of the side information. This naturally leads to a family of Renyi-like quantum conditional entropies, for which the von Neumann entropy emerges as a special case.

This mission is the statement-level formalization of A Fully Quantum Asymptotic Equipartition Property (arXiv:0811.1221v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

18 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Fully quantum asymptotic equipartition property (Theorem 1 (AEP), equations (6)-(7); original paper-level seed, 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

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

  • Appendix A, (A1) and Lemma 13: A well-defined singular-reference quasi-entropy S_f for every continuous f:[0,infinity)->R with f(0)=0 (source-ambiguity)

Selected references

  • A Fully Quantum Asymptotic Equipartition Property, arXiv:0811.1221v3, https://arxiv.org/abs/0811.1221v3
28 thms2 active usersReviewed
Quantum Information·Captain: Goku

Classical codes for quantum broadcast channelsResearch Paper

Motivation

We present two approaches for transmitting classical information over quantum broadcast channels. The first technique is a quantum generalization of the superposition coding scheme for the classical broadcast channel. We use a quantum simultaneous nonunique decoder and obtain a proof of the rate region stated in [Yard et al., IEEE Trans. Inf. Theory 57 (10), 2011]. Our second result is a quantum generalization of the Marton coding scheme. The error analysis for the quantum Marton region makes use of ideas in our earlier work and an idea recently presented by Radhakrishnan et al. in arXiv:1410.3248. Both results exploit recent advances in quantum simultaneous decoding developed in the context of quantum interference channels.

This mission is the statement-level formalization of Classical codes for quantum broadcast channels (arXiv:1111.3645v4). 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 Theorem 1: superposition coding inner bound (Theorem 1: superposition coding inner bound (paper seed), PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Selected references

  • Classical codes for quantum broadcast channels, arXiv:1111.3645v4, https://arxiv.org/abs/1111.3645v4
12 thms2 active usersReviewed
Quantum Information·Captain: Goku

Reversing Unknown Qubit-Unitary Operation, Deterministically and ExactlyResearch Paper

Motivation

We report a deterministic and exact protocol to reverse any unknown qubit-unitary operation, which simulates the time inversion of a closed qubit system. To avoid known no-go results on universal deterministic exact unitary inversion, we consider the most general class of protocols transforming unknown unitary operations within the quantum circuit model, where the input unitary operation is called multiple times in sequence and fixed quantum circuits are inserted between the calls. In the proposed protocol, the input qubit-unitary operation is called 4 times to achieve the inverse operation, and the output state in an auxiliary system can be reused as a catalyst state in another run of the unitary inversion. We also present the simplification of the semidefinite programming for searching the optimal deterministic unitary inversion protocol for an arbitrary dimension presented by M. T. Quintino and D. Ebler [Quantum 6\textbf{6}6, 679 (2022)]. We show a method to reduce the large search space representing all possible protocols, which provides a useful tool for analyzing higher-order quantum transformations for unitary operations.

This mission is the statement-level formalization of Reversing Unknown Qubit-Unitary Operation, Deterministically and Exactly (arXiv:2209.02907v5). 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 1: deterministic exact four-call inversion (Theorem 1: deterministic exact four-call qubit-unitary inversion, 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

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

  • Unnumbered assertion following S70: Continuity of the target channel, or an almost-everywhere conclusion, in the general-f average-fidelity criterion. (source-ambiguity)
  • Lemma S4, S83-S86: Constructed real Young-Yamanouchi physical matrix units E_ij^mu in every d-truncated tensor-power sector. (hard)
  • Lemma S5, S87: Compatible last-symbol tableau extension and physical E_ij^mu at consecutive tensor levels. (hard)
  • Theorem S7, S122-S125: Concrete Young-coordinate sequential SDP: computed physical block extraction, cycle representation and branching matrices. (hard)
  • Theorem S8, S126-S127: Concrete Young-coordinate parallel SDP with computed D^alpha and the physical/block objective transport. (hard)

Selected references

  • Reversing Unknown Qubit-Unitary Operation, Deterministically and Exactly, arXiv:2209.02907v5, https://arxiv.org/abs/2209.02907v5
13 thms2 active usersReviewed
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