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Convex OptimizationOptimizationTheoretical Computer Science·Captain: iris

A Fast Lewis-weight Interior Point Method for Linear Optimization over Product-Domain: Solving Linear Programs over Products of Convex Sets in Time O~(nd+d5/2)\tilde O(nd + d^{5/2})O~(nd+d5/2)Research Paper

Motivation

Many problems in statistics, control and data science minimize a linear objective over a product of small convex sets subject to a few linear equations: ℓp\ell_pℓp​ regression, entropy-regularized transport, and second-order cone programs with small cones. When the number of variables nnn is much larger than the number of equations ddd, the running time in terms of ddd decides what is practical.

For linear programs, the Lee–Sidford line of interior point methods replaced the n\sqrt nn​ iterations of the classical path-following method with O~(d)\widetilde O(\sqrt d)O(d​) iterations.

  • 1988. Renegar: O~(n)\widetilde O(\sqrt n)O(n​) iterations of path following.
  • 2014, 2019. Lee and Sidford (FOCS 2014, arXiv:1910.08033): O~(d)\widetilde O(\sqrt d)O(d​) iterations using Lewis weights, for scalar LPs with the logarithmic barrier.
  • 2021. van den Brand, Lee, Liu, Saranurak, Sidford, Song, Wang: scalar LPs in time O~(nd+d5/2)\widetilde O(nd+d^{5/2})O(nd+d5/2).
  • 2025. Liu, Peng, Tang, Weng, Yang: products of constant-dimensional convex sets with general barriers in time O~(nd+d6n)\widetilde O(nd+d^6\sqrt n)O(nd+d6n​), with n\sqrt nn​ iterations. They note that extending Lee–Sidford to such barriers is open.
  • 2026. Zhang and Wright (this manuscript): that extension, in time O~(nd+d5/2)\widetilde O(nd+d^{5/2})O(nd+d5/2).

Setting

The program is

min⁡x c⊤xsubject toA⊤x=b,x∈K=K1×⋯×Km,\min_{x}\ c^\top x\quad\text{subject to}\quad A^\top x=b,\quad x\in K=K_1\times\dots\times K_m,xmin​ c⊤xsubject toA⊤x=b,x∈K=K1​×⋯×Km​,

with A∈Rn×dA\in\mathbb R^{n\times d}A∈Rn×d, b∈Rdb\in\mathbb R^db∈Rd, c∈Rnc\in\mathbb R^nc∈Rn, compact convex Ki⊂RniK_i\subset\mathbb R^{n_i}Ki​⊂Rni​ and ∑ini=n\sum_in_i=n∑i​ni​=n.

Each KiK_iKi​ carries a 111-self-concordant barrier ϕi:int⁡Ki→R\phi_i:\operatorname{int}K_i\to\mathbb Rϕi​:intKi​→R: a convex C3C^3C3 function that tends to +∞+\infty+∞ at the boundary, with ∣∇3ϕi(x)[h,h,h]∣≤2∥h∥∇2ϕi(x)3|\nabla^3\phi_i(x)[h,h,h]|\le2\|h\|^3_{\nabla^2\phi_i(x)}∣∇3ϕi​(x)[h,h,h]∣≤2∥h∥∇2ϕi​(x)3​ and ∇ϕi⊤(∇2ϕi)−1∇ϕi≤1\nabla\phi_i^\top(\nabla^2\phi_i)^{-1}\nabla\phi_i\le1∇ϕi⊤​(∇2ϕi​)−1∇ϕi​≤1. Its Fenchel conjugate is ϕi∗(y)=sup⁡x∈int⁡Ki⟨x,y⟩−ϕi(x)\phi_i^*(y)=\sup_{x\in\operatorname{int}K_i}\langle x,y\rangle-\phi_i(x)ϕi∗​(y)=supx∈intKi​​⟨x,y⟩−ϕi​(x). The algorithm reaches ϕi\phi_iϕi​ and ϕi∗\phi_i^*ϕi∗​ only through constant-time oracles.

The regularized block Lewis weight of B∈Rn×dB\in\mathbb R^{n\times d}B∈Rn×d solves w=tr⁡G(P(W1/2−1/pB))+vw=\operatorname{tr}_G(P(W^{1/2-1/p}B))+vw=trG​(P(W1/2−1/pB))+v, where WWW is block diagonal with blocks wiIniw_iI_{n_i}wi​Ini​​, PPP is the orthogonal projection onto the column space, and tr⁡G\operatorname{tr}_GtrG​ is the vector of block traces. The method follows the central path weighted by τ(x)=w(C~(x,∇2Φ(x)))\tau(x)=w(\widetilde C(x,\nabla^2\Phi(x)))τ(x)=w(C(x,∇2Φ(x))), where C~\widetilde CC is the smoothed preconditioner, the root of Eu[∇2ϕi(xi+σMi−1/2u)−1]\mathbb E_u[\nabla^2\phi_i(x_i+\sigma M_i^{-1/2}u)^{-1}]Eu​[∇2ϕi​(xi​+σMi−1/2​u)−1] over the uniform law on the unit ball.

Formalization targets

Goal: Theorem 54, corrected

For every e>0e>0e>0 there are one program PPP of a real RAM with the two oracles, and constants C,kC,kC,k, such that for every instance with d≥1d\ge1d≥1, every κ\kappaκ bounding KiK_iKi​, cic_ici​ and ∥Ai∥op\|A_i\|_{\mathrm{op}}∥Ai​∥op​ and admitting a feasible zzz with B(zi,1/κ)⊆KiB(z_i,1/\kappa)\subseteq K_iB(zi​,1/κ)⊆Ki​, and every δ>0\delta>0δ>0: with probability at least 1−(n+2)−e1-(n+2)^{-e}1−(n+2)−e the run halts within

C nmax⁡k (nd+d5/2) (log⁡(n+d+κ+1/δ+2))kC\,n_{\max}^k\,(nd+d^{5/2})\,(\log(n+d+\kappa+1/\delta+2))^kCnmaxk​(nd+d5/2)(log(n+d+κ+1/δ+2))k

steps, with an output x∈Kx\in Kx∈K, A⊤x=bA^\top x=bA⊤x=b and c⊤x≤min⁡c⊤y+δc^\top x\le\min c^\top y+\deltac⊤x≤minc⊤y+δ. The manuscript's statement has no feasibility hypothesis and is false on infeasible instances; the corrections are declared on the item.

Milestones

In the order of the proof: the extended program with its start point and transfer (Lemma 49); stability of Lewis weights (Lemma 21); the smoothing estimates (Lemmas 23, 24); one-step stability of CCC, τ\tauτ, μ\muμ (Lemmas 28, 30, 31); potential change and contraction (Lemmas 34, 20); approximate feasibility and sampling (Lemmas 37, 38); finite-sum smoothing (the display in the proof of Lemma 42); the nearby sequence (Lemmas 51, 52); and exact feasibility with the final gap (Lemma 50). Matrix Bernstein and the bound ω<5/2\omega<5/2ω<5/2 are referenced from existing platform theorems.

Significance

The result gives the first O~(d)\widetilde O(\sqrt d)O(d​)-iteration path following for black-box self-concordant barriers on constant-dimensional blocks, and removes the n\sqrt nn​ of the earlier bound, moving the nearly linear time threshold from n≥d10n\ge d^{10}n≥d10 to n≥d3/2n\ge d^{3/2}n≥d3/2. The smoothed preconditioner replaces the higher-order self-concordance that earlier Lewis-weight analyses need.

The theorem is claimed in an unpublished manuscript; nothing in it is machine-checked. This mission adds block Lewis weights, the Bregman potential and a concrete model of computation with oracles to the platform, and states the main theorem and its key steps. Its corrected statements have counterexamples recorded on the items: Theorem 54, Lemma 37, Lemma 38, Lemma 49. The goal is open as a formal statement, and its proof must also handle points the manuscript leaves to adaptation, such as rank-deficient AAA.

Difficulty

The direct extension of scalar Lewis-weight arguments fails. A block carries one weight but a matrix-valued local geometry, and a small multiplicative change of a general positive definite preconditioner need not change the weights by a small relative amount. The analysis needs a Lipschitz derivative of ∇2ϕ−1/2\nabla^2\phi^{-1/2}∇2ϕ−1/2 along sampled sparse updates, and ordinary self-concordance controls only one derivative of the Hessian: the naive use of ∇2ϕ−1/2\nabla^2\phi^{-1/2}∇2ϕ−1/2 as preconditioner, as in the scalar proof, therefore has no second-order estimate.

A second obstacle is that the time bound rests on lazy data structures against adaptive updates by matrix-valued blocks. A count of iterations does not give the time.

Formalization scope

Coordinates are pairs (block, position). The model is a real RAM with a finite program, rational literals, +,−,×,÷,⋅,exp⁡,log⁡+,-,\times,\div,\sqrt{\cdot},\exp,\log+,−,×,÷,⋅​,exp,log, comparisons, integer pointers, a tape of Gaussian reals, and the two oracles, with charges (1+ni)2(1+n_i)^2(1+ni​)2 and 1+ni1+n_i1+ni​. A primal query outside int⁡Ki\operatorname{int}K_iintKi​ stops the run. There is no floor, sort, or matrix instruction, the program is chosen before the instance, and KiK_iKi​, κ\kappaκ and zzz are not in memory, which rules out a trivial solution by hard-coding or free computation. The minimum is written as ∀\forall∀ feasible yyy, so no junk infimum enters.

Milestones use one constant order: hidden constants for each bound on the block sizes, then CCC, then CVarC_{\mathrm{Var}}CVar​. They assume m≥2m\ge2m≥2 and full column rank where the page uses P(⋅)P(\cdot)P(⋅). Expectations in one-step lemmas are conditional on the good event of the sampling definition, since x(new)∈int⁡Kx^{(\mathrm{new})}\in\operatorname{int}Kx(new)∈intK is known only there.

The definitions of self-concordant barrier, real RAM and the uniform law on the ball are reused from the platform. Block Lewis weights, mixed norms and the machine are reusable beyond this mission. Contributions welcome: proofs of any milestone, the Lewis-weight existence and uniqueness of Lemma 57, Lemma 3-style Hessian comparisons for the barrier predicate, and data structures in the machine.

Selected references

  • P. Zhang, S. Wright, A Fast Lewis-weight Interior Point Method for Linear Optimization over Product-Domain, manuscript, November 2026, sha256 66072000….
  • J. Renegar, A polynomial-time algorithm, based on Newton's method, for linear programming, Math. Programming 40, 1988. https://doi.org/10.1007/BF01580724
  • Y. T. Lee, A. Sidford, Path finding methods for linear programming, FOCS 2014. https://arxiv.org/abs/1312.6677
  • Y. T. Lee, A. Sidford, Solving linear programs with Sqrt(rank) linear system solves, 2019. https://arxiv.org/abs/1910.08033
  • J. van den Brand, Y. T. Lee, Y. P. Liu, T. Saranurak, A. Sidford, Z. Song, D. Wang, Minimum cost flows, MDPs, and ℓ1\ell_1ℓ1​-regression in nearly linear time for dense instances, STOC 2021. https://arxiv.org/abs/2101.05719
  • Y. P. Liu, R. Peng, C. Tang, A. Weng, J. Yang, Adaptive matrix sparsification and applications to empirical risk minimization, 2025. https://arxiv.org/abs/2512.02003
27 thms5 active usersReviewed
Convex OptimizationOptimizationTheoretical Computer Science·Captain: iris

Adaptive Matrix Sparsification with Applications to Empirical Risk Minimization and Computational Geometry: ERM Solved to High Accuracy in Time O~(nd+d6n)\tilde O(nd + d^6\sqrt n)O~(nd+d6n​)Research Paper

Motivation

Empirical risk minimization (ERM) is a convex optimization problem that covers linear and ℓp\ell_pℓp​ regression, LASSO, logistic regression, support vector machines and quantile regression. Its dual form is

min⁡x∈K1×⋯×Km, A⊤x=bc⊤x,\min_{x\in K_1\times\cdots\times K_m,\ A^\top x=b} c^\top x,x∈K1​×⋯×Km​, A⊤x=bmin​c⊤x,

with A∈Rn×dA\in\mathbb R^{n\times d}A∈Rn×d and compact convex sets Ki⊆RniK_i\subseteq\mathbb R^{n_i}Ki​⊆Rni​ of constant dimension. The same form captures the minimum enclosing ball problem of computational geometry, a long-studied primitive in support vector machines and computer graphics (Liu et al., §1.1–§1.2). In statistics the interesting regime is tall: many more data points than dimensions, n≫dn\gg dn≫d, with AAA dense. There the input has size ndndnd, so a running time near ndndnd is what one can hope for.

Timeline, as cited by the source:

  • 1994: Nesterov and Nemirovskii, interior point methods from self-concordant barriers (NN94).
  • 2019: Lee, Song and Zhang solve the form above in time nmax⁡{ω,2+1/6}n^{\max\{\omega,2+1/6\}}nmax{ω,2+1/6}, transferring the square-regime linear programming bound to ERM with a robust central path of O~(n)\tilde O(\sqrt n)O~(n​) iterations (arXiv:1905.04447).
  • 2020: van den Brand, Lee, Sidford and Song solve tall dense linear programs in nearly linear time, on the Lee–Sidford O~(d)\tilde O(\sqrt d)O~(d​)-iteration method (arXiv:2002.02304).
  • 2021: van den Brand et al. reach O~(nd+d2.5)\tilde O(nd+d^{2.5})O~(nd+d2.5) for tall linear programs (arXiv:2101.05719). Neither the Lee–Sidford method nor Vaidya's volumetric barrier is known to extend to general ERM.
  • 2021–2022: for tall ERM with constant nin_ini​, Dong, Lee and Ye obtain O~(nd2)\tilde O(nd^2)O~(nd2) and Gu and Song O~(nd(ω+1)/2)\tilde O(nd^{(\omega+1)/2})O~(nd(ω+1)/2) (as cited on p.5 of the source).
  • 2026: Liu, Peng, Tang, Weng and Yang, this source, O~(nd+d6n)\tilde O(nd+d^6\sqrt n)O~(nd+d6n​): the first bound with leading term ndndnd for ERM, a question open since 2019 (p.5).

Setting

An ERM instance consists of mmm blocks with 1≤ni≤CK1\le n_i\le C_K1≤ni​≤CK​, n=∑inin=\sum_in_in=∑i​ni​, a matrix A∈Rn×dA\in\mathbb R^{n\times d}A∈Rn×d, vectors b∈Rdb\in\mathbb R^db∈Rd, c∈Rnc\in\mathbb R^nc∈Rn, and a bound κ\kappaκ. Each compact convex Ki⊆[−κ,κ]niK_i\subseteq[-\kappa,\kappa]^{n_i}Ki​⊆[−κ,κ]ni​ is accessed only through a self-concordant barrier ϕi:int⁡Ki→R\phi_i:\operatorname{int}K_i\to\mathbb Rϕi​:intKi​→R: a convex function that tends to +∞+\infty+∞ at the boundary and satisfies ∣ϕi′′′[h,h,h]∣≤2ϕi′′[h,h]3/2|\phi_i'''[h,h,h]|\le2\phi_i''[h,h]^{3/2}∣ϕi′′′​[h,h,h]∣≤2ϕi′′​[h,h]3/2 and ϕi′[h]2≤νiϕi′′[h,h]\phi_i'[h]^2\le\nu_i\phi_i''[h,h]ϕi′​[h]2≤νi​ϕi′′​[h,h]. An oracle returns ϕi\phi_iϕi​, ∇ϕi\nabla\phi_i∇ϕi​ and ∇2ϕi\nabla^2\phi_i∇2ϕi​ at a point of int⁡Ki\operatorname{int}K_iintKi​. The entries of A,b,cA,b,cA,b,c are at most κ\kappaκ and A⊤A⪰κ−1IA^\top A\succeq\kappa^{-1}IA⊤A⪰κ−1I.

The leverage score of a row aia_iai​ of AAA is τi=ai⊤(A⊤A)−1ai\tau_i=a_i^\top(A^\top A)^{-1}a_iτi​=ai⊤​(A⊤A)−1ai​. A family of overestimates τ~i≥τi\tilde\tau_i\ge\tau_iτ~i​≥τi​ with small sum tells one how to sample rows so that the sampled Gram matrix approximates A⊤AA^\top AA⊤A in the Loewner order. A batch is a set of row insertions and deletions given at once; the adversary is adaptive when it sees the published τ~\tilde\tauτ~ before choosing the next batch.

Formalization targets

Goal: Theorem 1, pp.6–7 (corrected)

For every CKC_KCK​ and c>0c>0c>0 there are one program PPP of a randomized real-arithmetic oracle machine and constants C,kC,kC,k such that for all admissible instances and all ε>0\varepsilon>0ε>0, with probability at least 1−(n+2)−c1-(n+2)^{-c}1−(n+2)−c, PPP halts within

C (nd+d6n) (log⁡(n+d+κ+1/ε+2))kC\,(nd+d^6\sqrt n)\,\big(\log(n+d+\kappa+1/\varepsilon+2)\big)^kC(nd+d6n​)(log(n+d+κ+1/ε+2))k

units of work with an xxx satisfying xi∈Kix_i\in K_ixi​∈Ki​ for all iii, A⊤x=bA^\top x=bA⊤x=b, and c⊤x≤ε+c⊤yc^\top x\le\varepsilon+c^\top yc⊤x≤ε+c⊤y for all feasible yyy.

Admissibility adds two hypotheses to the printed theorem: a feasible zzz with B(zi,1/κ)⊆KiB(z_i,1/\kappa)\subseteq K_iB(zi​,1/κ)⊆Ki​, and given start points wiw_iwi​ with B(wi,1/κ)⊆KiB(w_i,1/\kappa)\subseteq K_iB(wi​,1/κ)⊆Ki​. As printed, an infeasible instance meets every hypothesis.

Theorem 3, p.7

Leverage score overestimates under QQQ adaptive batches of row updates of total size O(n)O(n)O(n), with κ−1I⪯A⊤A⪯κI\kappa^{-1}I\preceq A^\top A\preceq\kappa Iκ−1I⪯A⊤A⪯κI throughout: τ~i≥τi\tilde\tau_i\ge\tau_iτ~i​≥τi​, ∑iτ~i≤O~(d)\sum_i\tilde\tau_i\le\tilde O(d)∑i​τ~i​≤O~(d), total work O~(nd+Qd6)\tilde O(nd+Qd^6)O~(nd+Qd6).

Milestones

The analysis of one interior point step (Lemmas 4.10, 4.11, 4.13, 4.7), the stability of the iterates (Lemma 4.15), the sampling of the step (Lemma 6.3), the matrix sampling lemma (Lemma 2.3, corrected), the decremental estimates (Lemmas 5.1, 5.3, 5.5, 5.6, the last two corrected), the Hessian comparisons (Lemmas C.2, C.3) and the final point (Lemma 6.4).

Significance

The result. The bound is nearly linear in the input size when AAA is dense and n≥d10n\ge d^{10}n≥d10. It extends nearly-linear tall linear programming to general ERM with blocks of constant dimension, and it yields the first nearly-linear algorithm for minimum enclosing ball with logarithmic dependence on ε\varepsilonε (Corollary 1.1). Theorem 3 is of independent interest: earlier dynamic leverage score structures handle graph Laplacians or matrices of the form A⊤DAA^\top DAA⊤DA for a fixed AAA.

Formalizing it. The source is an unpublished manuscript, and no part of this is machine-checked. The statement of Theorem 1 has been corrected, so a formal proof of the corrected form would also settle what the printed one should say. The mission adds to the platform a concrete machine model for interior point running times, a block ERM vocabulary, and the first formal statement of an adaptive sparsifier. Status: the source argues all of it, and [LSZ19, Lemmas D.2, D.3] and [Nes98] are cited rather than proved there.

Difficulty

An inserted row has no history, so it cannot be sketched in advance: the standard approach of maintaining a fixed matrix under a changing diagonal does not apply. A heavy-hitter data structure queried directly on this sequence fails, because the interior point method chooses its next updates after seeing the sparsifier sampled from the published estimates, so the structure's inputs depend on its own randomness. An obvious alternative, recomputing all leverage scores in each of the O~(n)\tilde O(\sqrt n)O~(n​) iterations, costs about n⋅nd\sqrt n\cdot ndn​⋅nd. A second obstacle is that the iterate xxx itself is not ℓ2\ell_2ℓ2​-stable under subsampling, so the number of updates to its approximation does not follow from a bound on the step size.

Formalization scope

Machine. One finite instruction list on the published real RAM core (SmaleNinth.RAMInstr), extended with integer pointers, ⋅\sqrt{\cdot}⋅​, exp⁡\expexp, a Gaussian tape and the barrier oracle; rational literals only; unit cost; no logarithm, floor, sort or matrix instruction. An oracle call outside int⁡Ki\operatorname{int}K_iintKi​ faults. The program and constants are chosen before the instance, so nothing can be hard-coded: a per-instance program, a function-valued instruction or a real literal would trivialize the claim.

Conventions. Blocks are consecutive coordinates. The barrier predicate is the published IsNuSelfConcordantBarrier, the line form of Definition 3.1, with νi≤CK\nu_i\le C_Kνi​≤CK​. The minimum is a bound against every feasible point. Failure probabilities are explicit, and bad events are bounded in outer measure. Adversaries and policies are measurable. Theorem 1's accuracy ε\varepsilonε, the small constant ε\varepsilonε of §4 and ϵchecker\epsilon_{\mathrm{checker}}ϵchecker​ of §5 are distinct. Item-level corrections and readings are listed in each statement.

Infrastructure and contributions. A complete development needs self-concordance calculus (Dikin ellipsoid, Hessian stability), matrix Bernstein, Johnson–Lindenstrauss (already on the platform), a dynamic heavy hitter, and a real-RAM implementation layer. All except the last are reusable beyond this mission. Proofs of any milestone are welcome, as are intermediate lemmas such as Lemmas 4.8, 4.9, 4.12, 5.7 and C.1, and sharper forms of the time bound.

Selected references

  • Y. P. Liu, R. Peng, C. Tang, A. Weng, J. Yang, Adaptive Matrix Sparsification with Applications to Empirical Risk Minimization and Computational Geometry, manuscript, 2026 (the source, sha256 7a66a27b…; no public link).
  • Y. T. Lee, Z. Song, Q. Zhang, Solving empirical risk minimization in the current matrix multiplication time, COLT 2019. https://arxiv.org/abs/1905.04447
  • J. van den Brand, Y. T. Lee, A. Sidford, Z. Song, Solving tall dense linear programs in nearly linear time, STOC 2020. https://arxiv.org/abs/2002.02304
  • J. van den Brand, Y. T. Lee, D. Nanongkai, R. Peng, T. Saranurak, A. Sidford, Z. Song, D. Wang, Bipartite matching in nearly-linear time on moderately dense graphs, FOCS 2020. https://arxiv.org/abs/2009.01802
  • J. van den Brand, Y. T. Lee, Y. P. Liu, T. Saranurak, A. Sidford, Z. Song, D. Wang, Minimum cost flows, MDPs, and ℓ1\ell_1ℓ1​-regression in nearly linear time for dense instances, STOC 2021. https://arxiv.org/abs/2101.05719
  • M. B. Cohen, Y. T. Lee, C. Musco, C. Musco, R. Peng, A. Sidford, Uniform sampling for matrix approximation, ITCS 2015. https://arxiv.org/abs/1408.5099
  • Y. Nesterov, A. Nemirovskii, Interior-Point Polynomial Algorithms in Convex Programming, SIAM, 1994. https://doi.org/10.1137/1.9781611970791
25 thms5 active usersReviewed
Control TheoryDynamical SystemsGraph Theory·Captain: mikedeng1

Synchronization via Pinning Control on General Complex Networks I: A Kronecker LMI Weighted by the Positive Left Null Vector of G Globally Synchronizes a Pinned Strongly Connected NetworkResearch Paper

Motivation

Many engineered and natural systems are networks of identical dynamical units coupled through a directed interaction graph: arrays of oscillators, power grids, sensor and multi-agent networks, gene regulatory circuits. A basic control question for such a network is how to force every unit onto a prescribed reference trajectory (an equilibrium, a periodic orbit or a chaotic solution of a single unit) by acting on only a few of them. Applying a feedback controller to a small fraction of the vertices and letting the coupling spread its effect is called pinning control. It was introduced for scale-free networks by Wang and Chen (2002), shown to work with a single controller on undirected networks by Chen, Liu and Lu (2007), and turned into checkable criteria for undirected networks by Yu, Chen and Lü (2009).

Directed networks are harder. Earlier criteria for directed networks (Zhou, Lu and Lü 2008; Song and Cao 2010) were stated through the symmetric part G+GTG+G^TG+GT of the coupling matrix, which may have eigenvalues with positive real part even when the network synchronizes, so they lose the structural information of the graph. Yu, Chen, Lü and Kurths (SIAM J. Control Optim., 2013) replaced the standard quadratic Lyapunov function by one weighted with the positive left null vector of the coupling matrix. This mission formalizes their main criterion for strongly connected networks (§3 of the paper) together with the matrix-theoretic lemmas it rests on (§2).

Setting

The network has NNN vertices with states xi(t)∈Rnx_i(t)\in\mathbb R^nxi​(t)∈Rn. A coupling matrix G=(Gij)∈RN×NG=(G_{ij})\in\mathbb R^{N\times N}G=(Gij​)∈RN×N has Gij≥0G_{ij}\ge 0Gij​≥0 for i≠ji\ne ji=j (Gij>0G_{ij}>0Gij​>0 means a connection from vertex jjj to vertex iii) and zero row sums, Gii=−∑j≠iGijG_{ii}=-\sum_{j\ne i}G_{ij}Gii​=−∑j=i​Gij​. The network is strongly connected if any vertex can be reached from any other by a directed path; GGG is irreducible if no simultaneous permutation of rows and columns brings it to block lower-triangular form (G~110G~21G~22)\begin{pmatrix}\tilde G_{11}&0\\\tilde G_{21}&\tilde G_{22}\end{pmatrix}(G~11​G~21​​0G~22​​) with square diagonal blocks of sizes mmm and N−mN-mN−m, 1≤m≤N−11\le m\le N-11≤m≤N−1. The in-degree of vertex iii is kiin=∑j≠iGijk_i^{\mathrm{in}}=\sum_{j\ne i}G_{ij}kiin​=∑j=i​Gij​.

Each vertex runs the dynamics x˙=f(x,t)\dot x=f(x,t)x˙=f(x,t) for a continuously differentiable f:Rn×R+→Rnf:\mathbb R^n\times\mathbb R_+\to\mathbb R^nf:Rn×R+​→Rn. A reference trajectory sss solves s˙=f(s,t)\dot s=f(s,t)s˙=f(s,t). With coupling strength ccc, inner coupling matrix Γ∈Rn×n\Gamma\in\mathbb R^{n\times n}Γ∈Rn×n and control gains di≥0d_i\ge0di​≥0 (vertex iii is pinned when di>0d_i>0di​>0), the controlled network is

x˙i=f(xi,t)+c∑j=1NGijΓxj−c diΓ(xi−s),i=1,…,N.\dot x_i=f(x_i,t)+c\sum_{j=1}^N G_{ij}\Gamma x_j-c\,d_i\Gamma(x_i-s),\qquad i=1,\dots,N.x˙i​=f(xi​,t)+cj=1∑N​Gij​Γxj​−cdi​Γ(xi​−s),i=1,…,N.

It is globally synchronized if xi(t)−s(t)→0x_i(t)-s(t)\to0xi​(t)−s(t)→0 for every iii, every reference trajectory and every solution. The vector field satisfies Assumption 1 if, for a constant matrix KKK,

(x−y)T(f(x,t)−f(y,t))≤(x−y)TKΓ(x−y)∀x,y∈Rn, t≥0.(x-y)^T\bigl(f(x,t)-f(y,t)\bigr)\le(x-y)^TK\Gamma(x-y)\qquad\forall x,y\in\mathbb R^n,\ t\ge0 .(x−y)T(f(x,t)−f(y,t))≤(x−y)TKΓ(x−y)∀x,y∈Rn, t≥0.

For positive weights ξ1,…,ξN\xi_1,\dots,\xi_Nξ1​,…,ξN​ put Ξ=diag⁡(ξ)\Xi=\operatorname{diag}(\xi)Ξ=diag(ξ), D=diag⁡(d)D=\operatorname{diag}(d)D=diag(d) and G^=12(ΞG+GTΞ)\widehat G=\tfrac12(\Xi G+G^T\Xi)G=21​(ΞG+GTΞ).

Formalization targets

Goal: Theorem 3.1 (p. 1402)

Let fff satisfy Assumption 1 with Γ\GammaΓ symmetric, let GGG be a strongly connected coupling matrix, and let ξ\xiξ be positive with G^\widehat GG having zero row sums (the weights of Lemma 2.12). If

Ξ⊗KΓ+ΓTKT2+c G^⊗Γ+ΓT2−c (ΞD)⊗Γ+ΓT2<0,\Xi\otimes\frac{K\Gamma+\Gamma^TK^T}{2}+c\,\widehat G\otimes\frac{\Gamma+\Gamma^T}{2}-c\,(\Xi D)\otimes\frac{\Gamma+\Gamma^T}{2}<0,Ξ⊗2KΓ+ΓTKT​+cG⊗2Γ+ΓT​−c(ΞD)⊗2Γ+ΓT​<0,

then the controlled network is globally synchronized.

Milestones

The path to the goal follows the paper: Lemma 2.5 (irreducible   ⟺  \iff⟺ strongly connected), Lemma 2.9 (ρ(A)=∥A∥∞\rho(A)=\|A\|_\inftyρ(A)=∥A∥∞​ for nonnegative AAA with constant row sums), Lemma 2.8 (Perron–Frobenius, already on the platform), Lemma 2.11 (a positive vector xxx with GTx=0G^Tx=0GTx=0), Lemma 2.12 (the weights Ξ\XiΞ), and the derivative estimate (3.4) for V=12∑iξieiTeiV=\tfrac12\sum_i\xi_ie_i^Te_iV=21​∑i​ξi​eiT​ei​, ei=xi−se_i=x_i-sei​=xi​−s:

V˙≤eT[Ξ⊗(KΓ)+c(G^−ΞD)⊗Γ]e.\dot V\le e^T\bigl[\Xi\otimes(K\Gamma)+c(\widehat G-\Xi D)\otimes\Gamma\bigr]e .V˙≤eT[Ξ⊗(KΓ)+c(G−ΞD)⊗Γ]e.

Companion results

Lemma 2.7, Lemma 2.10, and, under the paper's standing assumptions (KΓ=ΓKK\Gamma=\Gamma KKΓ=ΓK, θ=λmax⁡(K+KT2)≥0\theta=\lambda_{\max}(\tfrac{K+K^T}{2})\ge0θ=λmax​(2K+KT​)≥0) with Γ\GammaΓ positive definite: Corollary 3.2 (the N×NN\times NN×N condition θΞ+c(G^−ΞD)<0\theta\Xi+c(\widehat G-\Xi D)<0θΞ+c(G−ΞD)<0 suffices), Corollary 3.3 (i) (an explicit coupling threshold c>λmax⁡(θΞ)/∣λmax⁡(G^−ΞD)∣c>\lambda_{\max}(\theta\Xi)/|\lambda_{\max}(\widehat G-\Xi D)|c>λmax​(θΞ)/∣λmax​(G−ΞD)∣), and Corollary 3.4 (the necessary conditions di>θ/c−kiind_i>\theta/c-k_i^{\mathrm{in}}di​>θ/c−kiin​ at pinned and kiin>θ/ck_i^{\mathrm{in}}>\theta/ckiin​>θ/c at unpinned vertices).

Significance

The criterion reduces global synchronization of an nNnNnN-dimensional nonlinear system to one linear matrix inequality in the data (G,Γ,K,c,D)(G,\Gamma,K,c,D)(G,Γ,K,c,D), and the corollaries reduce it further to an N×NN\times NN×N inequality and to explicit bounds. Corollary 3.4 turns this into a pinning rule: vertices whose in-degree is below θ/c\theta/cθ/c must be controlled. Weighting by the left null vector of GGG is the device that later work on directed consensus and pinning reuses; Lemmas 2.11 and 2.12 isolate it as a statement about Metzler matrices.

The paper's results are proved on paper; none of them has a machine-checked proof that this mission is aware of. A formalization adds three things: a corrected statement of Theorem 3.1 (see the scope section), a Lean library of directed-network matrix facts (irreducibility in the permutation form, its equivalence with strong connectivity, positive left null vectors, the weighted symmetrization G^\widehat GG), and a reusable Lyapunov argument for linearly coupled networks with Kronecker-structured quadratic forms.

Difficulty

The obvious first idea, the unweighted Lyapunov function 12∑ieiTei\tfrac12\sum_ie_i^Te_i21​∑i​eiT​ei​, produces the symmetric part of GGG, which for a directed network need not be negative semidefinite; this is exactly the defect of earlier criteria. The weights must come from a positive left null vector of GGG, whose existence is a Perron–Frobenius statement that needs irreducibility, hence the graph–matrix equivalence of Lemma 2.5. The analytic part needs a derivative of VVV along solutions on [0,∞)[0,\infty)[0,∞), the conversion of a sum over vertices into a Kronecker quadratic form, and the passage from a negative definite form to convergence of every error component. On the Mathlib side, irreducibility in the paper's permutation sense, spectral radius through characteristic roots, and largest eigenvalues of symmetric matrices all have to be connected to existing API.

Formalization scope

States are Fin n → ℝ and matrices are indexed by Fin N, Fin n and, for Kronecker products, by pairs (i, a) with (A⊗B)(i,a),(j,b)=AijBab(A\otimes B)_{(i,a),(j,b)}=A_{ij}B_{ab}(A⊗B)(i,a),(j,b)​=Aij​Bab​; the stacked error uses the same order. Convergence (2.7) is stated with the neighbourhood filter of 000 in Rn\mathbb R^nRn, which does not depend on the norm. Derivatives are taken within [0,∞)[0,\infty)[0,∞). Pinning is encoded by di>0d_i>0di​>0 instead of the paper's reordering of the first lll vertices. "M<0M<0M<0" is positive definiteness of −M-M−M (Mathlib PosDef, which includes symmetry); every matrix compared with 000 is symmetric by construction. λmax⁡(A)\lambda_{\max}(A)λmax​(A) of a symmetric matrix is the least rrr with vTAv≤r vTvv^TAv\le r\,v^TvvTAv≤rvTv for all vvv; ρ(A)\rho(A)ρ(A) is the largest modulus of a complex characteristic root. Global synchronization quantifies over every reference solution and every network solution; existence of solutions is not asserted.

Added hypotheses, each disclosed in the item: ΓT=Γ\Gamma^T=\GammaΓT=Γ in Theorem 3.1 and (3.4), because the printed theorem allows any Γ\GammaΓ and is then false (a directed 3-cycle with Γ=(13−31)\Gamma=\begin{pmatrix}1&3\\-3&1\end{pmatrix}Γ=(1−3​31​) satisfies (3.2) but its error grows); c>0c>0c>0 in Corollary 3.4; at least one pinned vertex in Corollary 3.3 (i); N≥1N\ge1N≥1 in Lemma 2.10. The weights Ξ\XiΞ are not arbitrary: Theorem 3.1 and the corollaries require G^\widehat GG to have zero row sums, which for a coupling matrix is equivalent to GTξ=0G^T\xi=0GTξ=0. Assuming the derivative bound (3.4), negative definiteness of G^−ΞD\widehat G-\Xi DG−ΞD or decay of VVV in the goal would trivialize it and is excluded.

The mission needs: graph reachability for matrices with nonnegative off-diagonal entries; Perron–Frobenius for irreducible nonnegative matrices (referenced from the platform); Gershgorin-type bounds; Kronecker products and positive definiteness; and calculus of quadratic forms along solutions. The matrix lemmas (2.5, 2.7, 2.9–2.12) are reusable beyond this mission. Proofs of any item, and alternative proofs of the milestones, are welcome. Corollary 3.3 (ii) is not posed.

Selected references

  • W. Yu, G. Chen, J. Lü, J. Kurths, Synchronization via pinning control on general complex networks, SIAM J. Control Optim. 51(2) (2013), 1395–1416. https://doi.org/10.1137/100781699
  • X. F. Wang, G. Chen, Pinning control of scale-free dynamical networks, Physica A 310 (2002), 521–531. https://doi.org/10.1016/S0378-4371(02)00772-0
  • T. Chen, X. Liu, W. Lu, Pinning complex networks by a single controller, IEEE Trans. Circuits Syst. I 54 (2007), 1317–1326. https://doi.org/10.1109/TCSI.2007.895383
  • J. Zhou, J. Lu, J. Lü, Pinning adaptive synchronization of a general complex dynamical network, Automatica 44 (2008), 996–1003. https://doi.org/10.1016/j.automatica.2007.08.016
  • W. Yu, G. Chen, J. Lü, On pinning synchronization of complex dynamical networks, Automatica 45 (2009), 429–435. https://doi.org/10.1016/j.automatica.2008.07.016
  • Q. Song, J. Cao, On pinning synchronization of directed and undirected complex dynamical networks, IEEE Trans. Circuits Syst. I 57 (2010), 672–680. https://doi.org/10.1109/TCSI.2009.2024971
  • R. Olfati-Saber, R. M. Murray, Consensus problems in networks of agents with switching topology and time-delays, IEEE Trans. Automat. Control 49 (2004), 1520–1533. https://doi.org/10.1109/TAC.2004.834113
  • R. A. Horn, C. R. Johnson, Matrix Analysis, Cambridge University Press, 1985. https://doi.org/10.1017/CBO9780511810817
  • R. A. Brualdi, H. J. Ryser, Combinatorial Matrix Theory, Cambridge University Press, 1991. https://doi.org/10.1017/CBO9781107325708
10 thms5 active users
Complexity TheoryConvex OptimizationGraph Theory+1·Captain: iris

Asymptotic Rank of Weighted Graph Tensors via Completely Positive Covers: Over Every Field, MaxCut(W)≤log⁡2R~(WT(Q))≤UCPΔ(W)\mathrm{MaxCut}(W)\le\log_2\tilde R(\mathsf{WT}(Q))\le U^\Delta_{CP}(W)MaxCut(W)≤log2​R~(WT(Q))≤UCPΔ​(W) for Every Weighted Graph TensorResearch Paper

Motivation

The asymptotic rank of a tensor measures how cheaply many copies of it can be computed together. For the triangle graph tensor it is the matrix multiplication exponent: log⁡2R~F(GT2(K3))=ωF\log_2\tilde R_{\mathbb F}(\mathsf{GT}_2(K_3))=\omega_{\mathbb F}log2​R~F​(GT2​(K3​))=ωF​ over every field F\mathbb FF (Bürgisser–Clausen–Shokrollahi 1997, Prop. 15.1). Graph tensors extend this object from three parties to nnn: one tensor leg per vertex and an identity matrix on every edge. They model multilinear computation with several inputs and networks of pairwise entanglement, and their asymptotic rank and subrank were studied systematically by Christandl, Vrana and Zuiddam (2019). Allowing a different dimension on every edge gives weighted graph tensors (Christandl–Gesmundo–Michałek–Zuiddam 2021, §2.3), which include rectangular matrix multiplication.

Timeline of the results this mission builds on:

  • 1988: Strassen's spectral duality expresses asymptotic rank as a maximum over the asymptotic spectrum (Strassen 1988; see Wigderson–Zuiddam 2026).
  • 2017: Vrana and Christandl give the minimum-cut formula for the asymptotic subrank of weighted graph tensors (VC17).
  • 2019: Christandl, Vrana and Zuiddam bound the edge exponent of complete graphs by log⁡7(9/2)<0.773\log_7(9/2)<0.773log7​(9/2)<0.773 over C\mathbb CC for n≥4n\ge4n≥4 and ask whether log⁡2R~(GT2(K2m))\log_2\tilde R(\mathsf{GT}_2(K_{2m}))log2​R~(GT2​(K2m​)) equals the maximum cut (CVZ19, Questions 1.3.1–1.3.2).
  • 2026: OpenAI's polynomial-multiplication method gives ωC≤9/4\omega_{\mathbb C}\le 9/4ωC​≤9/4; Amanov, van den Berg and Zuiddam extend it to every field (ABZ26).
  • 2026: Zhou extends the method from three legs to nnn legs and to all weighted graph tensors over every field (arXiv:2610.34273), the source of this mission.

Setting

Fix a field F\mathbb FF and an integer n≥2n\ge2n≥2. A dimension matrix is a symmetric n×nn\times nn×n matrix QQQ of positive integers with Qi,i=1Q_{i,i}=1Qi,i​=1. The edge tensor Ei,j(q)E^{(q)}_{i,j}Ei,j(q)​ is the nnn-leg tensor ∑a<qea⊗ea\sum_{a<q}e_a\otimes e_a∑a<q​ea​⊗ea​ on legs i,ji,ji,j, with a one-dimensional factor on every other leg. The weighted graph tensor is the Kronecker product of the edge tensors,

WT(Q)=⨂1≤i<j≤nEi,j(Qi,j),\mathsf{WT}(Q)=\bigotimes_{1\le i<j\le n}E^{(Q_{i,j})}_{i,j},WT(Q)=1≤i<j≤n⨂​Ei,j(Qi,j​)​,

whose leg vvv has dimension Dv=∏jQv,jD_v=\prod_jQ_{v,j}Dv​=∏j​Qv,j​. For a graph GGG, GTq(G)=WT(Q)\mathsf{GT}_q(G)=\mathsf{WT}(Q)GTq​(G)=WT(Q) with Qi,j=qQ_{i,j}=qQi,j​=q on edges and 111 elsewhere. The rank RF(T)R_{\mathbb F}(T)RF​(T) is the least rrr with T⪯In(r)T\preceq I_n(r)T⪯In​(r) (restriction to the diagonal tensor), and R~F(T)=lim⁡NRF(T⊗N)1/N\tilde R_{\mathbb F}(T)=\lim_NR_{\mathbb F}(T^{\otimes N})^{1/N}R~F​(T)=limN​RF​(T⊗N)1/N.

The logarithmic edge-weight matrix is Wi,j=log⁡2Qi,jW_{i,j}=\log_2Q_{i,j}Wi,j​=log2​Qi,j​. For a nonempty proper vertex set SSS, cutW(S)=∑i<j, ∣{i,j}∩S∣=1Wi,j\mathrm{cut}_W(S)=\sum_{i<j,\ |\{i,j\}\cap S|=1}W_{i,j}cutW​(S)=∑i<j, ∣{i,j}∩S∣=1​Wi,j​, and MaxCut(W)\mathrm{MaxCut}(W)MaxCut(W) is the largest cut weight. With JJJ the all-one matrix and COPn\mathrm{COP}_nCOPn​ the cone of copositive matrices (aTXa≥0a^{\mathsf T}Xa\ge0aTXa≥0 for all a≥0a\ge0a≥0), the path-strengthened completely positive bound is

UCPΔ(W)=max⁡{∑i<jWi,jPi,j: P=PT, Pi,i=0, P≥0, J−2P∈COPn, Pi,j≤Pi,k+Pk,j},U^\Delta_{\mathrm{CP}}(W)=\max\Big\{\sum_{i<j}W_{i,j}P_{i,j}:\ P=P^{\mathsf T},\ P_{i,i}=0,\ P\ge0,\ J-2P\in\mathrm{COP}_n,\ P_{i,j}\le P_{i,k}+P_{k,j}\Big\},UCPΔ​(W)=max{i<j∑​Wi,j​Pi,j​: P=PT, Pi,i​=0, P≥0, J−2P∈COPn​, Pi,j​≤Pi,k​+Pk,j​},

the path inequalities ranging over all distinct i,j,ki,j,ki,j,k.

Formalization targets

Goal: Theorem 1.2

MaxCut(W) ≤ log⁡2R~F(WT(Q)) ≤ UCPΔ(W)\mathrm{MaxCut}(W)\ \le\ \log_2\tilde R_{\mathbb F}\big(\mathsf{WT}(Q)\big)\ \le\ U^\Delta_{\mathrm{CP}}(W)MaxCut(W) ≤ log2​R~F​(WT(Q)) ≤ UCPΔ​(W)

for every field F\mathbb FF, every n≥2n\ge2n≥2 and every dimension matrix QQQ. The statement fixes no characteristic, no nnn and no edge dimension.

Milestones

  1. Cut lower bound: the flattening rank across SSS is 2cutW(S)2^{\mathrm{cut}_W(S)}2cutW​(S) (Lemma A.3), hence MaxCut(W)≤log⁡2R~\mathrm{MaxCut}(W)\le\log_2\tilde RMaxCut(W)≤log2​R~, with equality for bipartite support (Proposition A.4).
  2. Spectral formula: Strassen duality (Theorem 2.20); a spectral point ϕ\phiϕ is determined on weighted graph tensors by its edge weights Pi,j(ϕ)∈[0,1]P^{(\phi)}_{i,j}\in[0,1]Pi,j(ϕ)​∈[0,1] (Lemma 2.25); and log⁡2R~(WT(Q))=ΓF(W)=max⁡ϕ∑i<jWi,jPi,j(ϕ)\log_2\tilde R(\mathsf{WT}(Q))=\Gamma_{\mathbb F}(W)=\max_\phi\sum_{i<j}W_{i,j}P^{(\phi)}_{i,j}log2​R~(WT(Q))=ΓF​(W)=maxϕ​∑i<j​Wi,j​Pi,j(ϕ)​ (Lemma 2.28).
  3. Complete graphs: polynomial multiplication has asymptotic rank 1+∑j(aj−1)1+\sum_j(a_j-1)1+∑j​(aj​−1) (Lemma 3.2); the entropy inequality (Corollary 3.5); the symmetric spectral profile is normalized, discretely concave and satisfies shifted tripling (Lemmas 4.2, 4.5, 4.8); diagonal growth (Lemma 4.9); and ⌊n2/4⌋≤log⁡2R~F(GT2(Kn))≤n2/4\lfloor n^2/4\rfloor\le\log_2\tilde R_{\mathbb F}(\mathsf{GT}_2(K_n))\le n^2/4⌊n2/4⌋≤log2​R~F​(GT2​(Kn​))≤n2/4 (Theorem 4.10 = Theorem 1.1).
  4. Conic constraints: J−2P(ϕ)J-2P^{(\phi)}J−2P(ϕ) is copositive (Lemma 5.1, eq. (8)) and P(ϕ)P^{(\phi)}P(ϕ) satisfies the path inequalities (Lemma 5.4).

Significance

For QQQ with entries 222 on the edges of a graph GGG, the goal bounds log⁡2R~(GT2(G))\log_2\tilde R(\mathsf{GT}_2(G))log2​R~(GT2​(G)) between the maximum cut and an explicit conic program, over every field. Theorem 4.10 settles the [CVZ19] maximum-cut question for even complete graphs, log⁡2R~(GT2(K2m))=m2\log_2\tilde R(\mathsf{GT}_2(K_{2m}))=m^2log2​R~(GT2​(K2m​))=m2, and gives edge exponents below 2/32/32/3 for n≥5n\ge5n≥5, against the previous 0.77230.77230.7723. For K3K_3K3​ it contains ω≤9/4\omega\le9/4ω≤9/4 over every field. Every feasible PPP for UCPΔU^\Delta_{\mathrm{CP}}UCPΔ​, and every completely positive cover, is a checkable certificate for an upper bound on asymptotic rank.

The results are proved on paper in the source, which cites Strassen's duality without proof. No statement about graph tensors, weighted graph tensors or asymptotic rank of tensors of order above three is on the platform; the abstract duality theorem is formalized inside the published mme_duality development, and ωC≤9/4\omega_{\mathbb C}\le9/4ωC​≤9/4 exists as a separate platform theorem. A formal proof would add the first machine-checked bound for higher-order graph tensors and a verified link between the asymptotic spectrum and copositive programming.

Difficulty

The lower bound is a flattening argument. The upper bound is not: a bound of the form ϕ(WT(Q))≤2U\phi(\mathsf{WT}(Q))\le2^{U}ϕ(WT(Q))≤2U must hold for every spectral point, and the spectrum is known only abstractly. The obvious route, bounding the rank of WT(Q)\mathsf{WT}(Q)WT(Q) or of its powers by an explicit decomposition, gives at best ∑i<jWi,j\sum_{i<j}W_{i,j}∑i<j​Wi,j​ and cannot reach n2/4n^2/4n2/4 for KnK_nKn​. The paper instead constrains P(ϕ)P^{(\phi)}P(ϕ) through the complete-graph estimate, whose proof needs a separation construction on n−2n-2n−2 shared legs at linear cost, an interpolation resource of asymptotic rank DDD over every field (including small finite fields, where Lagrange interpolation is unavailable), two polynomial degenerations, and a growth argument on a profile symmetrized over all n!n!n! leg permutations. The passage from KAK_AKA​ to arbitrary weights then needs vertex grouping and a continuity argument from integer to real vertex weights.

Formalization scope

Tensors are the published MME.TensorObj (finite-dimensional leg spaces and an element of their tensor product), with Kronecker sum and product, restriction, rank, asymptotic rank inf⁡N≥1R(T⊗N)1/N\inf_{N\ge1}R(T^{\otimes N})^{1/N}infN≥1​R(T⊗N)1/N (which the paper shows equals the limit), flattening rank, degeneration and leg permutations from the published MME library. Spectral points are the published monotone semiring homomorphisms on the tensor semiring modulo mutual restriction. WT(Q)\mathsf{WT}(Q)WT(Q) is defined in product coordinates: leg vvv is indexed by tuples (λv,j)j(\lambda_{v,j})_j(λv,j​)j​ instead of mixed-radix numbers, a relabeling within each leg. Vertices are Fin n\mathrm{Fin}\,nFinn, sums are over unordered pairs i<ji<ji<j, log⁡2\log_2log2​ is Real.logb 2, and the entropy in Corollary 3.5 is natural. MaxCut\mathrm{MaxCut}MaxCut, ΓF\Gamma_{\mathbb F}ΓF​ and UCPΔU^\Delta_{\mathrm{CP}}UCPΔ​ are real suprema of nonempty bounded families, equal to the paper's maxima.

Copositivity is not positive semidefiniteness: requiring J−2P⪰0J-2P\succeq0J−2P⪰0 gives a smaller program whose relation to ΓF\Gamma_{\mathbb F}ΓF​ the paper leaves open. The path inequalities range over all distinct triples, including non-edges, and the sums are not doubled over ordered pairs.

New definitions in the mission: dimension matrices, WT\mathsf{WT}WT, edge and graph tensors, cuts, UCPΔU^\Delta_{\mathrm{CP}}UCPΔ​, spectral edge weights, ΓF\Gamma_{\mathbb F}ΓF​, asymptotic restriction, polynomial multiplication tensors, the profile, and aligned partial direct sums (stated as a predicate). A complete proof needs, beyond the milestones, a concrete bridge between the platform's abstract Strassen duality and MME.tensorAsymptoticRank, Fekete-type limits for Kronecker powers, the separation theorem (Theorem 3.4), and the degenerations of Lemmas 4.4 and 4.7. The edge-tensor, flattening and polynomial-multiplication layers are reusable for other graph-tensor and matrix-multiplication missions. Proofs of any milestone, of intermediate lemmas posed by solvers, and of the duality bridge are welcome.

Selected references

  • H. Zhou, Asymptotic Rank of Weighted Graph Tensors via Completely Positive Covers, arXiv:2610.34273, 2026. https://arxiv.org/abs/2610.34273
  • V. Strassen, The asymptotic spectrum of tensors, J. reine angew. Math. 384 (1988) 102–152. https://doi.org/10.1515/crll.1988.384.102
  • M. Christandl, P. Vrana, J. Zuiddam, Asymptotic tensor rank of graph tensors: beyond matrix multiplication, Computational Complexity 28 (2019) 57–111. https://doi.org/10.1007/s00037-018-0172-8
  • M. Christandl, P. Vrana, J. Zuiddam, Universal points in the asymptotic spectrum of tensors, J. Amer. Math. Soc. 36 (2023) 31–79. https://doi.org/10.1090/jams/996
  • A. Wigderson, J. Zuiddam, Asymptotic spectra: theory, applications, and extensions, Bull. Amer. Math. Soc. 63 (2026) 199–331. https://doi.org/10.1090/bull/1880
  • P. Vrana, M. Christandl, Entanglement distillation from Greenberger–Horne–Zeilinger shares, Comm. Math. Phys. 352 (2017) 621–627. https://doi.org/10.1007/s00220-017-2861-6
  • M. Christandl, F. Gesmundo, M. Michałek, J. Zuiddam, Border rank nonadditivity for higher order tensors, SIAM J. Matrix Anal. Appl. 42 (2021) 503–527. https://doi.org/10.1137/20M1357366
  • A. Amanov, M. van den Berg, J. Zuiddam, Multiplying matrices via polynomials: exposition and barriers, arXiv:2610.30054, 2026. https://arxiv.org/abs/2610.30054
  • P. Bürgisser, M. Clausen, M. A. Shokrollahi, Algebraic Complexity Theory, Springer, 1997. https://doi.org/10.1007/978-3-662-03338-8
32 thms4 active usersReviewed
CombinatoricsGraph TheoryTheoretical Computer Science·Captain: iris

A Cheeger Inequality for Hypergraphs and Its Applications: Cheeger's Inequality ν₂(H)/Υ_H ≤ φ_h(H) ≤ √(2ν₂(H)) for Every Connected HypergraphResearch Paper

Why conductance of hypergraphs needs a spectral bound

The conductance of a graph measures its worst bottleneck: the smallest ratio of the weight crossing a cut to the volume of the smaller side. Cheeger's inequality for graphs, proved by Alon and Milman (JCTB 1985) and Alon (Combinatorica 1986), bounds conductance on both sides by an eigenvalue. Since an eigenvalue is computable and a minimum over cuts is not obviously so, this connection underlies spectral partitioning and the analysis of expanders and of random walks.

Many networks have interactions among more than two nodes, and hypergraphs model them. There the choice of operator matters. Banerjee (Linear Algebra Appl. 2021) introduced the matrix used here and obtained ϕh(H)≤(ΥH−1)(2−ν2(H))ν2(H)\phi_h(H)\le(\Upsilon_H-1)\sqrt{(2-\nu_2(H))\nu_2(H)}ϕh​(H)≤(ΥH​−1)(2−ν2​(H))ν2​(H)​ for connected HHH, whose upper bound grows with the rank. Chan, Louis, Tang and Zhang (JACM 2018) obtained γ2/2≤ϕh(H)≤2γ2\gamma_2/2\le\phi_h(H)\le\sqrt{2\gamma_2}γ2​/2≤ϕh​(H)≤2γ2​​, but for the eigenvalue γ2\gamma_2γ2​ of a nonlinear diffusion operator, not of a fixed matrix. Kamal and Bagchi's STOC 2027 submission states a bound for the fixed matrix with no rank in the upper side.

Setting: hypergraphs, conductance, and the normalized Laplacian

A hypergraph is H=(VH,EH,wH)H=(V_H,E_H,w_H)H=(VH​,EH​,wH​): a set VHV_HVH​ of nnn vertices, hyperedges EH⊆2VHE_H\subseteq 2^{V_H}EH​⊆2VH​, none of size one, and weights wH(e)∈[0,∞)w_H(e)\in[0,\infty)wH​(e)∈[0,∞). The degree of uuu is dH(u)=∑e∋uwH(e)d_H(u)=\sum_{e\ni u}w_H(e)dH​(u)=∑e∋u​wH​(e), the volume of SSS is volH(S)=∑v∈SdH(v)\mathrm{vol}_H(S)=\sum_{v\in S}d_H(v)volH​(S)=∑v∈S​dH​(v), and the rank ΥH\Upsilon_HΥH​ is the largest hyperedge size. HHH is connected if any two vertices are joined by a sequence of hyperedges whose consecutive members intersect. A 2-graph has all hyperedges of size two.

For ∅⊊S⊊VH\emptyset\subsetneq S\subsetneq V_H∅⊊S⊊VH​, the edge boundary ∂h(S)\partial_h(S)∂h​(S) is the set of hyperedges meeting both SSS and VH∖SV_H\setminus SVH​∖S, and

ϕh(S)=∑e∈∂h(S)wH(e)min⁡(volH(S),volH(VH∖S)),ϕ^h(S)=∑e∈∂h(S)wH(e)∣e∣−1∣e∩S∣∣e∩(VH∖S)∣min⁡(volH(S),volH(VH∖S)).\phi_h(S)=\frac{\sum_{e\in\partial_h(S)}w_H(e)}{\min(\mathrm{vol}_H(S),\mathrm{vol}_H(V_H\setminus S))},\qquad \hat\phi_h(S)=\frac{\sum_{e\in\partial_h(S)}\frac{w_H(e)}{|e|-1}|e\cap S||e\cap(V_H\setminus S)|}{\min(\mathrm{vol}_H(S),\mathrm{vol}_H(V_H\setminus S))}.ϕh​(S)=min(volH​(S),volH​(VH​∖S))∑e∈∂h​(S)​wH​(e)​,ϕ^​h​(S)=min(volH​(S),volH​(VH​∖S))∑e∈∂h​(S)​∣e∣−1wH​(e)​∣e∩S∣∣e∩(VH​∖S)∣​.

The conductance ϕh(H)\phi_h(H)ϕh​(H) and the diffusion conductance ϕ^h(H)\hat\phi_h(H)ϕ^​h​(H) are the minima of these over all such SSS. On a 2-graph the two agree and are written ϕg\phi_gϕg​.

The adjacency matrix has AH[u,v]=∑e⊇{u,v}wH(e)/(∣e∣−1)A_H[u,v]=\sum_{e\supseteq\{u,v\}}w_H(e)/(|e|-1)AH​[u,v]=∑e⊇{u,v}​wH​(e)/(∣e∣−1) for u≠vu\ne vu=v and zero diagonal. With DH=diag(dH)D_H=\mathrm{diag}(d_H)DH​=diag(dH​), the Laplacian is LH=DH−AHL_H=D_H-A_HLH​=DH​−AH​, the normalized Laplacian is LH=DH−1/2LHDH−1/2\mathcal L_H=D_H^{-1/2}L_HD_H^{-1/2}LH​=DH−1/2​LH​DH−1/2​, and ν1(H)≤ν2(H)≤⋯≤νn(H)\nu_1(H)\le\nu_2(H)\le\dots\le\nu_n(H)ν1​(H)≤ν2​(H)≤⋯≤νn​(H) are its eigenvalues.

The AE graph GHG_HGH​ replaces each hyperedge eee by a clique with edge weights wH(e)/(∣e∣−1)w_H(e)/(|e|-1)wH​(e)/(∣e∣−1), adding weights over repeated pairs.

Formalization targets

Goal: Theorem 4.1

For every connected hypergraph HHH,

ν2(H)ΥH≤ϕh(H)≤2ν2(H).\frac{\nu_2(H)}{\Upsilon_H}\le\phi_h(H)\le\sqrt{2\nu_2(H)}.ΥH​ν2​(H)​≤ϕh​(H)≤2ν2​(H)​.

Both sides are the goal, for every rank and all weights in [0,∞)[0,\infty)[0,∞).

Milestones

In proof order: the quadratic form (5) of LHL_HLH​; the Rayleigh characterization (7) of ν2\nu_2ν2​; the classical inequality for 2-graphs,

ν2(G)2≤ϕg(G)≤2ν2(G);\frac{\nu_2(G)}{2}\le\phi_g(G)\le\sqrt{2\nu_2(G)};2ν2​(G)​≤ϕg​(G)≤2ν2​(G)​;

Lemma 3.3 (HHH and GHG_HGH​ have identical AAA, LLL, L\mathcal LL); the bound (12) on ϕg(GH)\phi_g(G_H)ϕg​(GH​); Lemma 3.4 (ϕg(T)=ϕ^h(T)\phi_g(T)=\hat\phi_h(T)ϕg​(T)=ϕ^​h​(T) on GHG_HGH​); the bound

ν2(H)2≤ϕ^h(H)≤2ν2(H);(13)\frac{\nu_2(H)}{2}\le\hat\phi_h(H)\le\sqrt{2\nu_2(H)};\tag{13}2ν2​(H)​≤ϕ^​h​(H)≤2ν2​(H)​;(13)

and the comparisons (1) and (2),

ϕh(H)≤ϕ^h(H)≤ΥH2ϕh(H).\phi_h(H)\le\hat\phi_h(H)\le\frac{\Upsilon_H}{2}\phi_h(H).ϕh​(H)≤ϕ^​h​(H)≤2ΥH​​ϕh​(H).

What the result gives

The result. For a fixed symmetric matrix, the upper bound on conductance loses no factor depending on the rank, which improves Banerjee's bound for connected hypergraphs in that respect. The paper uses this bound for its applications: a family of hypergraph expanders, higher-order inequalities, and spectral partitioning. Those applications are outside this mission.

The formalization. This mission gives the platform a hypergraph Laplacian, a hypergraph conductance and a hypergraph Cheeger statement. None of the mission's statements has a machine-checked proof yet. The paper is a submission, and its Theorem 3.1 is cited rather than proved there. The platform has a proved Cheeger inequality for irreducible reversible Markov chains, MarkovMixing.cheeger_inequality, attached as a reference item. It is stated in other vocabulary and does not state Theorem 3.1. A proof must translate it, and must separately handle hypergraphs that are connected but not irreducible as chains.

Where the difficulty lies

The obvious first idea is to apply graph Cheeger to a clique expansion and read off ϕh\phi_hϕh​. That fails, because no clique expansion's cut weight equals the numerator of ϕh\phi_hϕh​: a crossing hyperedge counts once in ϕh\phi_hϕh​, but ∣e∩S∣∣e∖S∣/(∣e∣−1)|e\cap S||e\setminus S|/(|e|-1)∣e∩S∣∣e∖S∣/(∣e∣−1) times in ϕ^h\hat\phi_hϕ^​h​. The factor varies with the cut, between 111 and ∣e∣/2|e|/2∣e∣/2. So the spectral bound attaches to ϕ^h\hat\phi_hϕ^​h​, and any statement about ϕh\phi_hϕh​ must pay a comparison that is lossy on one side only. Equality in Lemma 3.3 is also not free of care: the degree identity ∑vAH[u,v]=dH(u)\sum_vA_H[u,v]=d_H(u)∑v​AH​[u,v]=dH​(u) depends on the excluded singleton hyperedges.

The main analytic content is the classical inequality for 2-graphs. Its weighted statement here also covers graphs with zero weights, where the chain is reducible and the Markov chain theorem above does not apply as stated.

Formalization scope

Vertices are a finite type VVV with 2≤∣V∣2\le|V|2≤∣V∣. Hyperedges form a Finset (Finset V), so there are no parallel hyperedges, and weights are a function read only on hyperedges. The empty hyperedge is allowed, as on the page, and enters no sum. All of ∣e∣−1|e|-1∣e∣−1 are real subtractions.

Weights may vanish, so a connected HHH can have a vertex of degree 000 or be disconnected in weight. No positivity is assumed. In those cases DH−1/2D_H^{-1/2}DH−1/2​ has entry 1/0=01/\sqrt0=01/0​=0 and a set's conductance is 0/0=00/0=00/0=0, both Lean conventions on inputs the page leaves undefined. Then ν2(H)=0=ϕh(H)\nu_2(H)=0=\phi_h(H)ν2​(H)=0=ϕh​(H). Connectedness ignores weights, and a zero-weight hyperedge counts for the rank.

ν2\nu_2ν2​ is the published AlonMilman.PropertyT.lambda1, the second-smallest eigenvalue with multiplicity of a real symmetric matrix. Minima over sets are real infima over the finite subtype of proper nonempty subsets, and the minima in (7) are stated with IsLeast over nonzero vectors. The AE graph is in merged form, so it is again a hypergraph with all hyperedges of size 2. A pair of total weight 000 stays an edge, which keeps it connected.

A trivializing reading is ruled out: ν2\nu_2ν2​ is not at a junk value, since it is the true second-smallest eigenvalue and is nonnegative, so the square root is meaningful.

A complete development needs Rayleigh–Ritz for LH\mathcal L_HLH​, the finite-sum identities behind Lemmas 3.3 and 3.4, the connectedness of GHG_HGH​, and the 2-graph inequality, whether through the Markov route or directly. The hypergraph layer is reusable for the paper's other results. Contributions on any milestone are welcome.

Selected references

  • N. Alon, V. D. Milman, λ₁, isoperimetric inequalities for graphs, and superconcentrators, Journal of Combinatorial Theory, Series B 38(1):73–88, 1985. https://doi.org/10.1016/0095-8956(85)90092-9
  • N. Alon, Eigenvalues and expanders, Combinatorica 6(2):83–96, 1986. https://doi.org/10.1007/BF02579166
  • A. Banerjee, On the spectrum of hypergraphs, Linear Algebra and its Applications 614:82–110, 2021. https://doi.org/10.1016/j.laa.2020.01.012
  • T-H. H. Chan, A. Louis, Z. G. Tang, C. Zhang, Spectral properties of hypergraph Laplacian and approximation algorithms, Journal of the ACM 65(3):1–48, 2018. https://doi.org/10.1145/3178123
  • R. Kamal, A. Bagchi, A Cheeger Inequality for Hypergraphs and Its Applications, STOC 2027 submission. https://arxiv.org/abs/2609.16286
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Quantum Information·Captain: iris

From Classical to Quantum Shannon Theory IV: Gentle Measurement for Ensembles: Σ pX(x)∥ρx − √Λρx√Λ∥₁ ≤ 2√εTextbook

Why measurement disturbance matters

Measuring a quantum system generally changes it. A qubit prepared in ∣0⟩|0\rangle∣0⟩ and measured along the XXX axis is left in ∣+⟩|+\rangle∣+⟩ or ∣−⟩|-\rangle∣−⟩, each with probability one half, and the original state is lost. The same qubit measured along the ZZZ axis returns its outcome with certainty and is left untouched. The gentle measurement lemma turns this intuition into an inequality: if one outcome of a measurement is very likely on a state, recording that outcome barely disturbs the state.

This bound is used throughout quantum Shannon theory. A decoder for classical communication over a quantum channel performs a sequence of measurements on the same received state, one test per candidate message, and it must know that the tests which pass leave the state almost intact for the tests that follow. The packing lemma, the covering lemma, the Holevo–Schumacher–Westmoreland theorem and the quantum union bound all rely on it. The ensemble version formalized here is the form that enters those coding arguments, where the disturbance must be controlled on average over a codebook rather than for one state.

The mission covers §§9.2–9.5 of M. M. Wilde, From Classical to Quantum Shannon Theory (arXiv:1106.1445v8), the fourth mission of a series that formalizes this textbook chapter by chapter.

Timeline. The lemma goes back to A. Winter's coding theorems (IEEE Trans. Inf. Theory 45, 1999), stated with the constant 8ε\sqrt{8\varepsilon}8ε​; the book proves it with the sharper constant 2ε2\sqrt\varepsilon2ε​ (Lemmas 9.4.1–9.4.3). Uhlmann's characterization of fidelity through purifications dates from 1976 (Rep. Math. Phys. 9); the relations between fidelity and trace distance are due to C. A. Fuchs and J. van de Graaf (IEEE Trans. Inf. Theory 45, 1999).

Setting

All Hilbert spaces are finite-dimensional, and all alphabets are finite. Operators on a space H\mathcal HH of dimension ddd are d×dd\times dd×d complex matrices.

  • A density operator ρ\rhoρ is a positive semi-definite operator of trace one; it describes the state of a quantum system.
  • The trace norm of an operator MMM is ∥M∥1=Tr⁡M†M\|M\|_1=\operatorname{Tr}\sqrt{M^\dagger M}∥M∥1​=TrM†M​, the sum of its singular values. The quantity ∥ρ−σ∥1\|\rho-\sigma\|_1∥ρ−σ∥1​ ranges over [0,2][0,2][0,2] for density operators.
  • A measurement operator is an operator Λ\LambdaΛ with 0≤Λ≤I0\le\Lambda\le I0≤Λ≤I; the probability that it detects the state ρ\rhoρ is Tr⁡{Λρ}\operatorname{Tr}\{\Lambda\rho\}Tr{Λρ}. Its positive square root is written Λ\sqrt\LambdaΛ​.
  • After the outcome Λ\LambdaΛ is detected, the state becomes the post-measurement state ρ′=ΛρΛ/Tr⁡{Λρ}\rho'=\sqrt\Lambda\rho\sqrt\Lambda/\operatorname{Tr}\{\Lambda\rho\}ρ′=Λ​ρΛ​/Tr{Λρ}.
  • An ensemble {pX(x),ρx}\{p_X(x),\rho_x\}{pX​(x),ρx​} is a probability distribution pXp_XpX​ on a finite alphabet X\mathcal XX together with density operators ρx\rho_xρx​; its average density operator is ρ=∑xpX(x)ρx\rho=\sum_x p_X(x)\rho_xρ=∑x​pX​(x)ρx​.
  • A purification of ρA\rho_AρA​ is a vector ∣ψ⟩RA|\psi\rangle_{RA}∣ψ⟩RA​ on a reference system RRR and the system AAA with Tr⁡R{∣ψ⟩⟨ψ∣RA}=ρA\operatorname{Tr}_R\{|\psi\rangle\langle\psi|_{RA}\}=\rho_ATrR​{∣ψ⟩⟨ψ∣RA​}=ρA​.
  • The fidelity of two density operators is F(ρ,σ)=∥ρσ∥12F(\rho,\sigma)=\|\sqrt\rho\sqrt\sigma\|_1^2F(ρ,σ)=∥ρ​σ​∥12​.
  • For a channel N\mathcal NN with Kraus operators {Km}\{K_m\}{Km​}, N(X)=∑mKmXKm†\mathcal N(X)=\sum_m K_mXK_m^\daggerN(X)=∑m​Km​XKm†​, the entanglement fidelity is Fe(ρ,N)=⟨ψ∣(idR⊗N)(ψRA)∣ψ⟩F_e(\rho,\mathcal N)=\langle\psi|(\mathrm{id}_R\otimes\mathcal N)(\psi_{RA})|\psi\rangleFe​(ρ,N)=⟨ψ∣(idR​⊗N)(ψRA​)∣ψ⟩ for a purification ∣ψ⟩RA|\psi\rangle_{RA}∣ψ⟩RA​ of ρ\rhoρ.

Formalization targets

Goal: gentle measurement for ensembles (Lemma 9.4.3, p. 279)

For an ensemble {pX(x),ρx}\{p_X(x),\rho_x\}{pX​(x),ρx​} with average ρ\rhoρ, a positive semi-definite Λ≤I\Lambda\le IΛ≤I and ε∈[0,1]\varepsilon\in[0,1]ε∈[0,1] with Tr⁡{ρΛ}≥1−ε\operatorname{Tr}\{\rho\Lambda\}\ge1-\varepsilonTr{ρΛ}≥1−ε,

∑xpX(x) ∥ρx−Λ ρx Λ∥1≤2ε.\sum_x p_X(x)\,\bigl\|\rho_x-\sqrt\Lambda\,\rho_x\,\sqrt\Lambda\bigr\|_1\le2\sqrt\varepsilon .x∑​pX​(x)​ρx​−Λ​ρx​Λ​​1​≤2ε​.

Milestones

  1. Theorem 9.2.1 (Uhlmann). For purifications ∣φρ⟩,∣φσ⟩|\varphi^\rho\rangle,|\varphi^\sigma\rangle∣φρ⟩,∣φσ⟩ on a common reference system, max⁡U∣⟨φρ∣UR⊗IA∣φσ⟩∣2=∥ρσ∥12\max_U|\langle\varphi^\rho|U_R\otimes I_A|\varphi^\sigma\rangle|^2=\|\sqrt\rho\sqrt\sigma\|_1^2maxU​∣⟨φρ∣UR​⊗IA​∣φσ⟩∣2=∥ρ​σ​∥12​.
  2. Lemma 9.2.1 (monotonicity). F(ρAB,σAB)≤F(ρA,σA)F(\rho_{AB},\sigma_{AB})\le F(\rho_A,\sigma_A)F(ρAB​,σAB​)≤F(ρA​,σA​); already proved on the platform in root-fidelity form.
  3. Lemma 9.4.1 (gentle measurement). If Tr⁡{Λρ}≥1−ε\operatorname{Tr}\{\Lambda\rho\}\ge1-\varepsilonTr{Λρ}≥1−ε, then ∥ρ−ρ′∥1≤2ε\|\rho-\rho'\|_1\le2\sqrt\varepsilon∥ρ−ρ′∥1​≤2ε​.
  4. Lemma 9.4.2 (gentle operator). Under the same hypothesis, ∥ρ−ΛρΛ∥1≤2ε\|\rho-\sqrt\Lambda\rho\sqrt\Lambda\|_1\le2\sqrt\varepsilon∥ρ−Λ​ρΛ​∥1​≤2ε​.
  5. Theorem 9.5.1. Fe(ρ,N)=∑m∣Tr⁡{ρKm}∣2F_e(\rho,\mathcal N)=\sum_m|\operatorname{Tr}\{\rho K_m\}|^2Fe​(ρ,N)=∑m​∣Tr{ρKm​}∣2.

Lemma 9.4.2 is the one-element case of the goal. Lemma 9.4.1 compares ρ\rhoρ with the normalized post-measurement state instead.

Significance

The result. The goal is the version of gentle measurement that coding theorems actually call: a decoder test Λ\LambdaΛ that accepts the average output state with high probability changes the individual codeword states by at most 2ε2\sqrt\varepsilon2ε​ on average. Without it, the analysis of sequential decoding and of the packing lemma (later in this series) has no control on how earlier tests damage the state seen by later ones. Uhlmann's theorem and the Kraus formula for the entanglement fidelity are the two standard tools for computing fidelities of states and channels, and they are reused across the remaining chapters.

Formalizing it. All results here are proved in the book, so the remaining work is to formalize the known proofs. The platform already has gentle measurement statements with the weaker constant 8ε\sqrt{8\varepsilon}8ε​ (one of them proved), and Uhlmann's theorem in root-fidelity form with a supremum (proved). The constant 2ε2\sqrt\varepsilon2ε​, the ensemble version, the attainment of the maximum in Uhlmann's theorem and the Kraus formula for FeF_eFe​ are not yet machine-checked anywhere on the platform. The relation 1−F≤12∥ρ−σ∥1≤1−F1-\sqrt F\le\frac12\|\rho-\sigma\|_1\le\sqrt{1-F}1−F​≤21​∥ρ−σ∥1​≤1−F​ (Theorem 9.3.1) and the fact that a measurement achieves the fidelity (Theorem 9.2.2) are open goals of other missions and are not posed again here.

Difficulty

The step that does not go through directly is the passage from one state to an ensemble. Applying Lemma 9.4.2 to each ρx\rho_xρx​ separately needs a lower bound on each Tr⁡{Λρx}\operatorname{Tr}\{\Lambda\rho_x\}Tr{Λρx​}, and the hypothesis bounds only the average. The individual bounds can be poor for some xxx, so the per-state lemma cannot be applied with a fixed ε\varepsilonε. What is needed is a bound on each ∥ρx−ΛρxΛ∥1\|\rho_x-\sqrt\Lambda\rho_x\sqrt\Lambda\|_1∥ρx​−Λ​ρx​Λ​∥1​ in terms of 1−Tr⁡{Λρx}1-\operatorname{Tr}\{\Lambda\rho_x\}1−Tr{Λρx​} that remains useful after averaging, which is a matter of the shape of the per-state inequality, not of its constant.

For the single-state lemmas, the obstacle is the constant: the triangle-inequality argument that gives 8ε\sqrt{8\varepsilon}8ε​ loses a factor 2\sqrt22​, and reaching 2ε2\sqrt\varepsilon2ε​ requires a sharper operator inequality. In Lean, the matrix square root, the trace norm and Hilbert–Schmidt Cauchy–Schwarz inequalities all have to be handled through the continuous functional calculus, where Mathlib's library for trace-class estimates is thin. Uhlmann's theorem needs the polar decomposition and the characterization of the trace norm as a maximum over unitaries.

Formalization scope

Operators are complex matrices Matrix n n ℂ over a finite index type; a vector on R⊗AR\otimes AR⊗A is a function on r × a (reference first, Mathlib's Kronecker convention). The trace norm is the published WildeQIT.traceNorm, unhalved; square roots are CFC.sqrt. The condition 0≤Λ≤I0\le\Lambda\le I0≤Λ≤I is positive semidefiniteness of Λ\LambdaΛ and of I−ΛI-\LambdaI−Λ. Traces that are real for positive operators, such as Tr⁡{Λρ}\operatorname{Tr}\{\Lambda\rho\}Tr{Λρ}, are taken as real parts of complex traces. Distributions are the published WildeQIT.FinDist, and channels the published Kraus-form WildeQIT.QChannel. The maximum in Uhlmann's theorem is stated as IsGreatest: it is attained, not only a supremum. Lemma 9.4.1 assumes Tr⁡{Λρ}≠0\operatorname{Tr}\{\Lambda\rho\}\ne0Tr{Λρ}=0, which excludes only the case where the book's ρ′\rho'ρ′ is undefined.

No statement is trivialized by a degenerate case: every hypothesis is satisfied by ρ=Λ=I\rho=\Lambda=Iρ=Λ=I on a one-dimensional space with ε=0\varepsilon=0ε=0, and the constant 2ε2\sqrt\varepsilon2ε​ is that of the book, not the weaker 8ε\sqrt{8\varepsilon}8ε​.

A complete development needs the operator inequality Λ≥Λ\sqrt\Lambda\ge\LambdaΛ​≥Λ for 0≤Λ≤I0\le\Lambda\le I0≤Λ≤I, the Hilbert–Schmidt Cauchy–Schwarz inequality, the triangle inequality and convexity of the trace norm, and concavity of the square root. These lemmas are reusable well beyond this mission. Contributions of any of them, or of the polar-decomposition and trace-norm duality results behind Uhlmann's theorem, are welcome.

Selected references

  • M. M. Wilde, From Classical to Quantum Shannon Theory, arXiv:1106.1445v8, 2019, §§9.2–9.5. https://arxiv.org/abs/1106.1445v8
  • A. Winter, Coding theorem and strong converse for quantum channels, IEEE Trans. Inf. Theory 45(7), 1999. https://doi.org/10.1109/18.796385
  • A. Uhlmann, The "transition probability" in the state space of a ∗-algebra, Rep. Math. Phys. 9(2), 1976. https://doi.org/10.1016/0034-4877(76)90060-4
  • C. A. Fuchs, J. van de Graaf, Cryptographic distinguishability measures for quantum-mechanical states, IEEE Trans. Inf. Theory 45(4), 1999. https://doi.org/10.1109/18.761271
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AnalysisConvex OptimizationOptimization·Captain: iris

Parabolic Regularity of Spectral Functions: Parabolic Regularity Passes Between a Convex Spectral Function θ∘λ and Its Symmetric Function θ, with a Second Subderivative FormulaResearch Paper

Motivation

A spectral function is an extended-real-valued function ggg on the space Sn\mathbf S^nSn of real symmetric n×nn\times nn×n matrices that is orthogonally invariant: g(U⊤XU)=g(X)g(U^\top XU)=g(X)g(U⊤XU)=g(X) for every orthogonal UUU. Eigenvalue optimization, semidefinite programming, matrix completion and low-rank regularization all lead to such functions: the largest eigenvalue, the nuclear norm of a symmetric matrix, the indicator of the positive semidefinite cone, −log⁡det⁡-\log\det−logdet. Every spectral function factors as g=θ∘λg=\theta\circ\lambdag=θ∘λ, where λ(X)\lambda(X)λ(X) is the vector of eigenvalues in nonincreasing order and θ:Rn→[−∞,∞]\theta:\mathbb R^n\to[-\infty,\infty]θ:Rn→[−∞,∞] is symmetric, i.e. invariant under permutations of coordinates (Lewis, Convex analysis on the Hermitian matrices).

A long line of work shows that properties of θ\thetaθ transfer to ggg: convexity and the subdifferential (Lewis 1996), differentiability (Lewis 1996), twice differentiability (Lewis–Sendov 2001), and second-order expansions of eigenvalues (Torki 2001). Second-order optimality conditions for nonsmooth problems need more: the second subderivative of ggg and the regularity property, parabolic regularity, that makes it computable and makes ggg twice epi-differentiable (Mohammadi–Mordukhovich–Sarabi, Parabolic regularity in geometric variational analysis, Trans. Amer. Math. Soc. 374, 2021). A. Mohammadi and E. Sarabi, Parabolic Regularity of Spectral Functions (arXiv:2301.04240v3, 2024; Mathematics of Operations Research, 2025) prove that parabolic regularity also passes between θ\thetaθ and ggg.

Setting

Sn\mathbf S^nSn carries ⟨X,Y⟩=tr⁡(XY)\langle X,Y\rangle=\operatorname{tr}(XY)⟨X,Y⟩=tr(XY). λ(X)=(λ1(X)≥⋯≥λn(X))\lambda(X)=(\lambda_1(X)\ge\dots\ge\lambda_n(X))λ(X)=(λ1​(X)≥⋯≥λn​(X)); On(X)O^n(X)On(X) is the set of orthogonal UUU with X=UDiag⁡(λ(X))U⊤X=U\operatorname{Diag}(\lambda(X))U^\topX=UDiag(λ(X))U⊤. If μ1>⋯>μr\mu_1>\dots>\mu_rμ1​>⋯>μr​ are the distinct eigenvalues of XXX, the blocks are αm={i∣λi(X)=μm}\alpha_m=\{i\mid\lambda_i(X)=\mu_m\}αm​={i∣λi​(X)=μm​}, and UαmU_{\alpha_m}Uαm​​ is the matrix of the columns of UUU indexed by αm\alpha_mαm​. The eigenvalue map has one-sided derivatives λ′(X;H)\lambda'(X;H)λ′(X;H) and λ′′(X;H,W)\lambda''(X;H,W)λ′′(X;H,W) along parabolic curves X+tH+12t2WX+tH+\tfrac12t^2WX+tH+21​t2W.

For f:X→[−∞,∞]f:\mathbf X\to[-\infty,\infty]f:X→[−∞,∞] on a finite-dimensional Hilbert space, finite at xˉ\bar xxˉ:

  • the subderivative df(xˉ)(w)=lim inf⁡t↓0,w′→w(f(xˉ+tw′)−f(xˉ))/t\mathrm df(\bar x)(w)=\liminf_{t\downarrow0,w'\to w}(f(\bar x+tw')-f(\bar x))/tdf(xˉ)(w)=liminft↓0,w′→w​(f(xˉ+tw′)−f(xˉ))/t;
  • the second subderivative d2f(xˉ,vˉ)(w)=lim inf⁡t↓0,w′→wΔt2f(xˉ,vˉ)(w′)\mathrm d^2f(\bar x,\bar v)(w)=\liminf_{t\downarrow0,w'\to w}\Delta^2_tf(\bar x,\bar v)(w')d2f(xˉ,vˉ)(w)=liminft↓0,w′→w​Δt2​f(xˉ,vˉ)(w′), with Δt2f(xˉ,vˉ)(w)=(f(xˉ+tw)−f(xˉ)−t⟨vˉ,w⟩)/12t2\Delta^2_tf(\bar x,\bar v)(w)=(f(\bar x+tw)-f(\bar x)-t\langle\bar v,w\rangle)/\tfrac12t^2Δt2​f(xˉ,vˉ)(w)=(f(xˉ+tw)−f(xˉ)−t⟨vˉ,w⟩)/21​t2;
  • the parabolic subderivative d2f(xˉ)(w ∣ z)\mathrm d^2f(\bar x)(w\,|\,z)d2f(xˉ)(w∣z), the same kind of liminf along xˉ+tw+12t2z′\bar x+tw+\tfrac12t^2z'xˉ+tw+21​t2z′;
  • the critical cone Kf(xˉ,vˉ)={w∣df(xˉ)(w)=⟨vˉ,w⟩}K_f(\bar x,\bar v)=\{w\mid\mathrm df(\bar x)(w)=\langle\bar v,w\rangle\}Kf​(xˉ,vˉ)={w∣df(xˉ)(w)=⟨vˉ,w⟩}.

A convex fff is parabolically regular at xˉ\bar xxˉ for vˉ∈∂f(xˉ)\bar v\in\partial f(\bar x)vˉ∈∂f(xˉ) if every finite value d2f(xˉ,vˉ)(w)\mathrm d^2f(\bar x,\bar v)(w)d2f(xˉ,vˉ)(w) is attained along some tk↓0t_k\downarrow0tk​↓0, wk→ww_k\to wwk​→w with ∥wk−w∥=O(tk)\|w_k-w\|=O(t_k)∥wk​−w∥=O(tk​) (Definition 5.1). Parabolic epi-differentiability asks that the parabolic subderivative be a full limit along every tk↓0t_k\downarrow0tk​↓0.

Formalization targets

Goal: Theorem 5.8

Let g=θ∘λg=\theta\circ\lambdag=θ∘λ be locally Lipschitz continuous relative to its domain, lower semicontinuous and convex. (a) If Y∈∂g(X)Y\in\partial g(X)Y∈∂g(X) and θ\thetaθ is parabolically regular at λ(X)\lambda(X)λ(X) for λ(Y)\lambda(Y)λ(Y) and parabolically epi-differentiable at λ(X)\lambda(X)λ(X), then ggg is parabolically regular at XXX for YYY, and for every H∈Kg(X,Y)H\in K_g(X,Y)H∈Kg​(X,Y) and U∈On(X)∩On(Y)U\in O^n(X)\cap O^n(Y)U∈On(X)∩On(Y)

d2g(X,Y)(H)=d2θ(λ(X),λ(Y))(λ′(X;H))+2∑m=1r⟨Λ(Y)αmαm,Uαm⊤H(μmI−X)†HUαm⟩.\mathrm d^2g(X,Y)(H)=\mathrm d^2\theta(\lambda(X),\lambda(Y))(\lambda'(X;H))+2\sum_{m=1}^r\big\langle\Lambda(Y)_{\alpha_m\alpha_m},U_{\alpha_m}^\top H(\mu_mI-X)^\dagger HU_{\alpha_m}\big\rangle .d2g(X,Y)(H)=d2θ(λ(X),λ(Y))(λ′(X;H))+2m=1∑r​⟨Λ(Y)αm​αm​​,Uαm​⊤​H(μm​I−X)†HUαm​​⟩.

(b) If ggg is parabolically epi-differentiable and parabolically regular at XXX, then θ\thetaθ is parabolically regular at λ(X)\lambda(X)λ(X).

Milestones

  • Fan's inequality (2.3) (already proved on the platform) and the distance identities (1.3), (3.5).
  • Eigenvalue expansions: Propositions 2.1, 2.2 with (2.13), and Corollary 2.3.
  • First order: the subdifferential (Proposition 3.4), the subderivative chain rule (Theorem 3.5), and tangent cones of spectral sets (Corollary 3.6).
  • Parabolic: second-order tangent sets (Theorem 4.3), domains of parabolic subderivatives (Proposition 4.6), the parabolic chain rule (Theorem 4.7), and PX,Hn\mathbf P^n_{X,H}PX,Hn​-symmetry (Proposition 4.8).
  • §5: the characterization of parabolic regularity (Proposition 5.2, corrected), the lower estimate (5.1) (Proposition 5.3), the critical cone (Proposition 5.4), the attaining matrix W^\widehat WW (Proposition 5.6), and the domain of d2g(X,Y)\mathrm d^2g(X,Y)d2g(X,Y) (Proposition 5.7).

Significance

Theorem 5.8(a) gives an explicit second subderivative for every convex spectral function whose symmetric part is parabolically regular, for example every polyhedral θ\thetaθ (Corollary 5.9 of the paper). This yields second-order necessary and sufficient optimality conditions for min⁡φ(X)+g(X)\min\varphi(X)+g(X)minφ(X)+g(X) and, through the results of Mohammadi–Sarabi (SIAM J. Optim. 30, 2020), twice epi-differentiability of ggg and proto-differentiability of ∂g\partial g∂g. The curvature term 2∑m⟨⋅,⋅⟩2\sum_m\langle\cdot,\cdot\rangle2∑m​⟨⋅,⋅⟩ recovers the known formula −2⟨Y,HX†H⟩-2\langle Y,HX^\dagger H\rangle−2⟨Y,HX†H⟩ for the positive semidefinite cone as a special case.

The theorem is proved in the paper; none of it is formalized. Formalizing it adds a library of second-order variational analysis on a general space (parabolic subderivatives, second subderivatives, parabolic regularity) and second-order perturbation theory of eigenvalues, both absent from Mathlib. Proposition 5.2 as printed is false (see Difficulty), so the mission also records the corrected statement.

Difficulty

The eigenvalue map is not twice differentiable where eigenvalues coalesce, so the standard composite chain rules of Mohammadi–Sarabi (2020), which need a twice differentiable inner map, do not apply. The paper replaces differentiability with Torki's parabolic expansion (Proposition 2.2), whose second-order term depends on a choice of eigenvector bases QmQ_mQm​ inside each eigenvalue block. The upper bound of Theorem 5.8(a) needs a direction W^\widehat WW attaining the infimum of the parabolic subderivative. Building it (Proposition 5.6) requires a minimizer sorted inside each block βjm\beta^m_jβjm​ and a choice of QmQ_mQm​ adapted to YYY (5.22).

A natural first idea is to prove (5.20), d2g(X,Y)(H)=inf⁡W{d2g(X)(H∣W)−⟨Y,W⟩}\mathrm d^2g(X,Y)(H)=\inf_W\{\mathrm d^2g(X)(H|W)-\langle Y,W\rangle\}d2g(X,Y)(H)=infW​{d2g(X)(H∣W)−⟨Y,W⟩}, and conclude by Proposition 5.2. This does not work: the implication "(b) ⇒ (a)" of Proposition 5.2 is false. The convex function f(x,y)=x2+x4/yf(x,y)=x^2+x^4/yf(x,y)=x2+x4/y (y>0y>0y>0), f(0,0)=0f(0,0)=0f(0,0)=0 satisfies (b) at xˉ=0\bar x=0xˉ=0, vˉ=0\bar v=0vˉ=0, but at w=(1,0)w=(1,0)w=(1,0) the infimum is not attained and fff is not parabolically regular. Attainment at W^\widehat WW is what is needed.

Formalization scope

  • Sn\mathbf S^nSn is the published SunNLSDP.Equiv.SymMat (Fin n), with entrywise inner product equal to tr⁡(XY)\operatorname{tr}(XY)tr(XY); λ\lambdaλ is the published ModernConvex.Spectral.eigVec; Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n). Indices are 0-based.
  • Functions take values in EReal. Wherever the paper assumes f(xˉ)f(\bar x)f(xˉ) finite, the definitions subtract the real f(xˉ)f(\bar x)f(xˉ), and ∂f(xˉ)=∅\partial f(\bar x)=\emptyset∂f(xˉ)=∅ when f(xˉ)f(\bar x)f(xˉ) is infinite.
  • Convexity is that of the epigraph, with no properness bundled.
  • λ′\lambda'λ′ and λ′′\lambda''λ′′ are one-sided limits, whose existence is a milestone (Corollary 2.3).
  • Z†Z^\daggerZ† is the Moore–Penrose inverse (functional calculus).
  • The curvature sum is written per index, ∑iλi(Y)(U⊤H(λi(X)I−X)†HU)ii\sum_i\lambda_i(Y)(U^\top H(\lambda_i(X)I-X)^\dagger HU)_{ii}∑i​λi​(Y)(U⊤H(λi​(X)I−X)†HU)ii​, a regrouping of the block sum.
  • The formula holds for every U∈On(X)∩On(Y)U\in O^n(X)\cap O^n(Y)U∈On(X)∩On(Y).

Two trivializations are ruled out by the definitions. Parabolic regularity keeps both the recovery-sequence requirement and the bound ∥wk−w∥=O(tk)\|w_k-w\|=O(t_k)∥wk​−w∥=O(tk​). All liminfs range over Sn\mathbf S^nSn, not over all matrices.

The development needs variational analysis on a general inner-product space (reusable for any composite or matrix problem) and second-order eigenvalue perturbation theory. Proofs of any milestone, of the cited results (Propositions 2.1, 2.2, 3.4, 4.6), and of the corrected Proposition 5.2 are welcome.

Selected references

  • A. Mohammadi, E. Sarabi, Parabolic Regularity of Spectral Functions, arXiv:2301.04240v3, 2024; Mathematics of Operations Research, 2025. https://arxiv.org/abs/2301.04240
  • A. S. Lewis, Convex analysis on the Hermitian matrices, SIAM J. Optim. 6:164–177 (1996). https://doi.org/10.1137/0806009
  • A. Mohammadi, B. S. Mordukhovich, M. E. Sarabi, Parabolic regularity in geometric variational analysis, Trans. Amer. Math. Soc. 374:1711–1763 (2021).
  • A. S. Lewis, H. S. Sendov, Twice differentiable spectral functions, SIAM J. Matrix Anal. Appl. 23:368–386 (2001). https://doi.org/10.1137/S089547980036838X
  • M. Torki, Second-order directional derivatives of all eigenvalues of a symmetric matrix, Nonlinear Anal. 46:1133–1150 (2001).
  • A. Mohammadi, E. Sarabi, Twice epi-differentiability of extended-real-valued functions with applications in composite optimization, SIAM J. Optim. 30:2379–2409 (2020).
  • R. T. Rockafellar, R. J-B. Wets, Variational Analysis, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
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Quantum Information·Captain: iris

An application of a matrix inequality in quantum information theory: the maximal output p-norm is multiplicative for a diagonal CP map and any CP map, for all p ≥ 1Research Paper

Motivation

A quantum channel is a completely positive, trace-preserving linear map between finite-dimensional matrix algebras. One central question in quantum Shannon theory was whether the minimal output entropy Smin⁡(Φ)=inf⁡ρS(Φ(ρ))S_{\min}(\Phi) = \inf_\rho S(\Phi(\rho))Smin​(Φ)=infρ​S(Φ(ρ)) is additive under tensor products, Smin⁡(Φ⊗Ψ)=Smin⁡(Φ)+Smin⁡(Ψ)S_{\min}(\Phi\otimes\Psi) = S_{\min}(\Phi) + S_{\min}(\Psi)Smin​(Φ⊗Ψ)=Smin​(Φ)+Smin​(Ψ). Shor showed in 2004 (Commun. Math. Phys. 246, 453–472) that this conjecture is equivalent to the additivity of the Holevo capacity and of the entanglement of formation. A standard approach goes through the maximal output ppp-norm νp\nu_pνp​ (Amosov–Holevo–Werner 2000). Its derivative at p=1p = 1p=1 is the negative minimal output entropy, so multiplicativity of νp\nu_pνp​ for ppp near 111 implies additivity.

Timeline:

  • 2000. Amosov, Holevo and Werner introduce νp\nu_pνp​ and conjecture multiplicativity for all p≥1p \ge 1p≥1.
  • 2002. Werner and Holevo give a counterexample for p>4.79p > 4.79p>4.79, so multiplicativity fails in general for large ppp (J. Math. Phys. 43, 4353).
  • 2002–2003. King proves multiplicativity for all p≥1p \ge 1p≥1 for unital qubit channels and for entanglement-breaking channels (arXiv:quant-ph/0103156, arXiv:quant-ph/0212057). The second proof uses the Lieb–Thirring inequality, following an argument of Lieb and Ruskai.
  • 2004. In the paper formalized here, King uses the same inequality to prove multiplicativity for all p≥1p \ge 1p≥1 when one factor is a diagonal map, the class described by Landau and Streater (arXiv:quant-ph/0412046).
  • 2009. Hastings shows that minimal output entropy is not additive in general (Nature Physics 5, 255).

Setting

Matrices are complex and indexed by finite sets. MnM_nMn​ is the algebra of n×nn\times nn×n matrices. A state is a positive semidefinite matrix of trace 111. The Hadamard product of two n×nn\times nn×n matrices is (A∗B)ij=AijBij(A*B)_{ij} = A_{ij}B_{ij}(A∗B)ij​=Aij​Bij​.

A linear map Ψ:Mk→Mm\Psi : M_k \to M_mΨ:Mk​→Mm​ is completely positive (CP) if I⊗ΨI\otimes\PsiI⊗Ψ maps positive semidefinite matrices to positive semidefinite matrices for every identity III. In finite dimension this holds exactly when Ψ(X)=∑jEjXEj∗\Psi(X) = \sum_j E_j X E_j^*Ψ(X)=∑j​Ej​XEj∗​ for finitely many m×km\times km×k matrices EjE_jEj​ (a Kraus form). Trace preservation is not assumed anywhere.

A map Φ:Mn→Mn\Phi : M_n\to M_nΦ:Mn​→Mn​ is diagonal (Definition 3) if there is a positive semidefinite C∈MnC\in M_nC∈Mn​ with

Φ(ρ)=C∗ρfor all ρ.\Phi(\rho) = C * \rho \qquad\text{for all } \rho .Φ(ρ)=C∗ρfor all ρ.

The tensor product Φ⊗Ψ:Mnk→Mnm\Phi\otimes\Psi : M_{nk}\to M_{nm}Φ⊗Ψ:Mnk​→Mnm​ is the linear map with (Φ⊗Ψ)(X⊗Y)=Φ(X)⊗Ψ(Y)(\Phi\otimes\Psi)(X\otimes Y) = \Phi(X)\otimes\Psi(Y)(Φ⊗Ψ)(X⊗Y)=Φ(X)⊗Ψ(Y). A matrix on Cn⊗Ck\mathbb C^n\otimes\mathbb C^kCn⊗Ck is read as an n×nn\times nn×n block matrix with k×kk\times kk×k blocks.

For p≥1p\ge1p≥1, the Schatten ppp-norm of XXX is ∥X∥p=(Tr⁡(X∗X)p/2)1/p\|X\|_p = (\operatorname{Tr}(X^*X)^{p/2})^{1/p}∥X∥p​=(Tr(X∗X)p/2)1/p. The maximal output ppp-norm of a map Θ\ThetaΘ is

νp(Θ)=sup⁡ρ state∥Θ(ρ)∥p,\nu_p(\Theta) = \sup_{\rho\ \text{state}} \|\Theta(\rho)\|_p ,νp​(Θ)=ρ statesup​∥Θ(ρ)∥p​,

with the supremum over states in the domain of Θ\ThetaΘ.

Formalization targets

Goal: Theorem 4

For a diagonal map Φ\PhiΦ on MnM_nMn​, any CP map Ψ:Mk→Mm\Psi : M_k\to M_mΨ:Mk​→Mm​, and every real p≥1p\ge1p≥1,

νp(Φ⊗Ψ)=νp(Φ) νp(Ψ).\nu_p(\Phi\otimes\Psi) = \nu_p(\Phi)\,\nu_p(\Psi).νp​(Φ⊗Ψ)=νp​(Φ)νp​(Ψ).

The goal fixes no dimension and no value of ppp. It includes p=1p = 1p=1, partners whose output dimension differs from their input dimension, and maps that are not trace preserving.

Milestones

The milestones follow the order of the proof:

  1. the Lieb–Thirring inequality (9), Tr⁡(VKV∗)p≤Tr⁡(V∗V)p/2Kp(V∗V)p/2=Tr⁡(V∗V)pKp\operatorname{Tr}(VKV^*)^p \le \operatorname{Tr}(V^*V)^{p/2}K^p(V^*V)^{p/2} = \operatorname{Tr}(V^*V)^pK^pTr(VKV∗)p≤Tr(V∗V)p/2Kp(V∗V)p/2=Tr(V∗V)pKp;
  2. the Hadamard decomposition ρ=(A⊗Jk)∗τ\rho = (A\otimes J_k)*\tauρ=(A⊗Jk​)∗τ of a state (12), where Aij=(αiαj)1/2A_{ij} = (\alpha_i\alpha_j)^{1/2}Aij​=(αi​αj​)1/2, αi=Tr⁡(ρ)ii\alpha_i = \operatorname{Tr}(\rho)_{ii}αi​=Tr(ρ)ii​, and JkJ_kJk​ is the all-ones matrix;
  3. compatibility of the decomposition with I⊗ΨI\otimes\PsiI⊗Ψ (14), and the product map (Φ⊗Ψ)(ρ)=(Φ(A)⊗J)∗((I⊗Ψ)(τ))(\Phi\otimes\Psi)(\rho) = (\Phi(A)\otimes J)*((I\otimes\Psi)(\tau))(Φ⊗Ψ)(ρ)=(Φ(A)⊗J)∗((I⊗Ψ)(τ)) (15);
  4. the block rows ViV_iVi​ of ((I⊗Ψ)(τ))1/2((I\otimes\Psi)(\tau))^{1/2}((I⊗Ψ)(τ))1/2 satisfy Ψ((τ)ii)=ViVi∗\Psi((\tau)_{ii}) = V_iV_i^*Ψ((τ)ii​)=Vi​Vi∗​ and ∥ViVi∗∥p≤νp(Ψ)\|V_iV_i^*\|_p\le\nu_p(\Psi)∥Vi​Vi∗​∥p​≤νp​(Ψ) (16)–(18);
  5. the factorization (Φ⊗Ψ)(ρ)=VKV∗(\Phi\otimes\Psi)(\rho) = VKV^*(Φ⊗Ψ)(ρ)=VKV∗ with V=diag⁡(V1,…,Vn)V = \operatorname{diag}(V_1,\dots,V_n)V=diag(V1​,…,Vn​) and K=Φ(A)⊗I′K = \Phi(A)\otimes I'K=Φ(A)⊗I′ (21)–(24);
  6. the trace formula Tr⁡(V∗V)pKp=∑iTr⁡(Vi∗Vi)p((Φ(A))p)ii\operatorname{Tr}(V^*V)^pK^p = \sum_i\operatorname{Tr}(V_i^*V_i)^p((\Phi(A))^p)_{ii}Tr(V∗V)pKp=∑i​Tr(Vi∗​Vi​)p((Φ(A))p)ii​ (25)–(26), and the fact that Vi∗ViV_i^*V_iVi∗​Vi​ and ViVi∗V_iV_i^*Vi​Vi∗​ have the same nonzero spectrum;
  7. the bounds (27)–(29), ending in Tr⁡((Φ⊗Ψ)(ρ))p≤νp(Ψ)pνp(Φ)p\operatorname{Tr}((\Phi\otimes\Psi)(\rho))^p\le\nu_p(\Psi)^p\nu_p(\Phi)^pTr((Φ⊗Ψ)(ρ))p≤νp​(Ψ)pνp​(Φ)p;
  8. the upper bound νp(Φ⊗Ψ)≤νp(Φ)νp(Ψ)\nu_p(\Phi\otimes\Psi)\le\nu_p(\Phi)\nu_p(\Psi)νp​(Φ⊗Ψ)≤νp​(Φ)νp​(Ψ) (30), and the product-state lower bound νp(Φ)νp(Ψ)≤νp(Φ⊗Ψ)\nu_p(\Phi)\nu_p(\Psi)\le\nu_p(\Phi\otimes\Psi)νp​(Φ)νp​(Ψ)≤νp​(Φ⊗Ψ), which together give the goal.

Significance

The result. Theorem 4 places the diagonal maps among the classes for which νp\nu_pνp​ is multiplicative for every p≥1p\ge1p≥1 and every CP partner. At p↓1p\downarrow 1p↓1 it gives additivity of the minimal output entropy, and through Shor's equivalences the additivity of the Holevo capacity, whenever one channel is diagonal. Diagonal maps include the completely dephasing channel and, more generally, the Hadamard channels, which are complementary to entanglement-breaking channels. The paper also shows that Lieb–Thirring arguments are not tied to the entanglement-breaking class.

Formalizing it. The result is proved on paper, and no machine-checked proof is known to exist. A formalization supplies a checked proof of Theorem 4 and of its steps. It also supplies a statement of the Lieb–Thirring trace inequality for rectangular VVV and all p≥1p\ge1p≥1, and lemmas on block-diagonal matrices, Hadamard products and Kronecker products under the functional calculus. These are reusable elsewhere in matrix analysis.

Difficulty

The inequality νp(Φ⊗Ψ)≥νp(Φ)νp(Ψ)\nu_p(\Phi\otimes\Psi)\ge\nu_p(\Phi)\nu_p(\Psi)νp​(Φ⊗Ψ)≥νp​(Φ)νp​(Ψ) is the easy direction: restrict the supremum to product states. The other direction is the content of the theorem. The obvious approach, bounding ∥(Φ⊗Ψ)(ρ)∥p\|(\Phi\otimes\Psi)(\rho)\|_p∥(Φ⊗Ψ)(ρ)∥p​ directly for an entangled ρ\rhoρ, does not work. The ppp-norm of a matrix is not controlled by the norms of its blocks, and for general channels the inequality is false (Werner–Holevo). The diagonal structure has to be used through the Hadamard product, and the resulting expression has to be bounded by a trace inequality that moves the power ppp inside a product, which is the Lieb–Thirring inequality. The inequality itself rests on operator interpolation or Epstein's concavity theorem, and Mathlib does not have it. Smaller obstacles in Lean are real powers of positive semidefinite matrices, block-diagonal and Kronecker structure under the functional calculus, and the attainment and boundedness of the real suprema defining νp\nu_pνp​.

Formalization scope

Maps are plain functions on matrices, Superop ι κ := Matrix ι ι ℂ → Matrix κ κ ℂ, over arbitrary finite index types, which may be empty. Complete positivity is the finite Kraus form FiniteKrausCP. The tensor product of maps is superopTensor, defined on every matrix through matrix units, with the first factor's index first, so the block (ρ)ij(\rho)_{ij}(ρ)ij​ of ρ\rhoρ is fun a b => ρ (i, a) (j, b). The maximal output norm is nu (ENNReal.ofReal p): a real sSup, over density matrices (positive semidefinite, trace one), of the Schatten norm (Re⁡Tr⁡(X∗X)p/2)1/p(\operatorname{Re}\operatorname{Tr}(X^*X)^{p/2})^{1/p}(ReTr(X∗X)p/2)1/p. These three objects are reused from a published definition layer. Matrix powers are cfc (fun x : ℝ => x ^ p), applied only to positive semidefinite matrices. Traces in inequalities are compared through their real parts.

The goal is not trivial. IsDiagonalMap requires C⪰0C\succeq0C⪰0, and the identity map (with CCC the all-ones matrix) satisfies it. The supremum in νp\nu_pνp​ ranges over a nonempty set whenever the input index type is nonempty. For an empty input type both sides of the goal are 000, which matches the convention that there are no states. The quantities τ\tauτ, AAA, ViV_iVi​ and VVV are computed from ρ\rhoρ and Ψ\PsiΨ, never chosen existentially. Where the paper divides by (αiαj)1/2(\alpha_i\alpha_j)^{1/2}(αi​αj​)1/2, Lean reads 0−10^{-1}0−1 as 000, and the milestones are stated for all states.

Contributions in three areas are welcome. The first is a general Lieb–Thirring inequality in Mathlib style. The second is lemmas on the continuous functional calculus of Kronecker and block-diagonal matrices. The third is the compactness and attainment facts for νp\nu_pνp​, which serve any multiplicativity statement built on the same layer.

Selected references

  • C. King, An application of a matrix inequality in quantum information theory, arXiv:quant-ph/0412046v1, 2004. https://arxiv.org/abs/quant-ph/0412046
  • G. G. Amosov, A. S. Holevo, R. F. Werner, On some additivity problems in quantum information theory, Problems of Information Transmission 36, 305–313, 2000. https://arxiv.org/abs/math-ph/0003002
  • E. H. Lieb, W. Thirring, Inequalities for the moments of the eigenvalues of the Schrödinger Hamiltonian and their relation to Sobolev inequalities, in Studies in Mathematical Physics, Princeton University Press, 1976. https://doi.org/10.1007/3-540-27056-6_16
  • H. Araki, On an inequality of Lieb and Thirring, Letters in Mathematical Physics 19, 167–170, 1990. https://doi.org/10.1007/BF01045887
  • R. F. Werner, A. S. Holevo, Counterexample to an additivity conjecture for output purity of quantum channels, Journal of Mathematical Physics 43, 4353–4357, 2002. https://arxiv.org/abs/quant-ph/0203003
  • P. W. Shor, Equivalence of additivity questions in quantum information theory, Communications in Mathematical Physics 246, 453–472, 2004. https://doi.org/10.1007/s00220-003-0981-7
  • C. King, Maximal p-norms of entanglement breaking channels, Quantum Information and Computation 3, 186–190, 2003. https://arxiv.org/abs/quant-ph/0212057
  • M. B. Hastings, Superadditivity of communication capacity using entangled inputs, Nature Physics 5, 255–257, 2009. https://arxiv.org/abs/0809.3972
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AlgebraOptimization·Captain: mikedeng1

Invariant Semidefinite Programs: Every Matrix ∗-Algebra Is ∗-Isomorphic to a Direct Sum of Full Matrix AlgebrasResearch Paper

Motivation

Semidefinite programs that arise in coding theory, extremal geometry, crossing-number bounds and polynomial optimization are often too large to solve directly, but they are invariant under a large symmetry group. Restricting the matrix variable to the invariant matrices loses nothing, and the invariant matrices form a matrix ∗-algebra. The survey of Bachoc, Gijswijt, Schrijver and Vallentin (arXiv:1007.2905, published in the Handbook on Semidefinite, Conic and Polynomial Optimization, Springer, 2012) organizes this symmetry reduction into steps. Its Step 2 (§1.2, pp. 5–7) replaces an SDP over such an algebra by an SDP over a few small blocks, and the justification of that step is a single structure theorem: every matrix ∗-algebra is ∗-isomorphic to a direct sum of full matrix algebras (Theorem 1.2, restated as Theorem 2.7 on p. 13).

The theorem is classical. It is the finite-dimensional case of the structure theory of C∗-algebras (Davidson, C∗-Algebras by Example, Chapter I.10), and in the unital, non-star form it is the Wedderburn–Artin theorem for semisimple algebras over ℂ. Its use in SDP symmetry reduction goes back to Gatermann and Parrilo (2004) and de Klerk, Pasechnik and Schrijver (2007). Section 2.5 of the survey gives a short, elementary, self-contained proof using only linear algebra; this mission follows that proof.

Setting

A matrix ∗-algebra (Definition 2.1, p. 10) is a complex linear subspace A⊆Cn×n\mathcal A \subseteq \mathbb C^{n\times n}A⊆Cn×n that is closed under matrix multiplication and under the conjugate transpose X↦X∗X \mapsto X^*X↦X∗. It need not contain the identity matrix, and it may be {0}\{0\}{0}.

A map φ:A→B\varphi : \mathcal A \to \mathcal Bφ:A→B between matrix ∗-algebras is a ∗-homomorphism (Definition 2.6, p. 13) if it is linear, satisfies φ(XY)=φ(X)φ(Y)\varphi(XY) = \varphi(X)\varphi(Y)φ(XY)=φ(X)φ(Y) and φ(X∗)=φ(X)∗\varphi(X^*) = \varphi(X)^*φ(X∗)=φ(X)∗; a bijective ∗-homomorphism is a ∗-isomorphism. The direct sum ⨁k=1dCmk×mk\bigoplus_{k=1}^d \mathbb C^{m_k\times m_k}⨁k=1d​Cmk​×mk​ is the algebra of block-diagonal matrices with diagonal blocks of sizes m1,…,mdm_1, \dots, m_dm1​,…,md​ (p. 10).

The proof uses the following vocabulary (p. 13). The center of A\mathcal AA is CA={Z∈A:ZX=XZ for all X∈A}\mathcal C_{\mathcal A} = \{Z \in \mathcal A : ZX = XZ \text{ for all } X \in \mathcal A\}CA​={Z∈A:ZX=XZ for all X∈A}. The unit of A\mathcal AA is the unique E∈AE \in \mathcal AE∈A with EX=XE=XEX = XE = XEX=XE=X for all X∈AX \in \mathcal AX∈A. A\mathcal AA is simple if it is non-zero and CA=CE\mathcal C_{\mathcal A} = \mathbb C ECA​=CE. For a partition [n]=S0∪S1∪⋯∪Sk[n] = S_0 \cup S_1 \cup \dots \cup S_k[n]=S0​∪S1​∪⋯∪Sk​, IiI_iIi​ is the zero-one diagonal matrix with ones in the positions of SiS_iSi​.

Formalization targets

Goal: Theorem 2.7 (= Theorem 1.2), p. 13

For every matrix ∗-algebra A⊆Cn×n\mathcal A \subseteq \mathbb C^{n\times n}A⊆Cn×n there are ddd and m1,…,mdm_1, \dots, m_dm1​,…,md​ and a ∗-isomorphism

φ:A⟶⨁k=1dCmk×mk.\varphi : \mathcal A \longrightarrow \bigoplus_{k=1}^d \mathbb C^{m_k\times m_k}.φ:A⟶k=1⨁d​Cmk​×mk​.

The goal fixes no sizes: it asserts only the existence of the block structure, which is the form Step 2 uses.

Milestones, in the order of the paper's proof

  1. Theorem 2.2 (p. 11): a commutative matrix ∗-algebra is unitarily similar to {λ1I1+⋯+λkIk:λi∈C}\{\lambda_1 I_1 + \dots + \lambda_k I_k : \lambda_i \in \mathbb C\}{λ1​I1​+⋯+λk​Ik​:λi​∈C} for a partition with S1,…,SkS_1, \dots, S_kS1​,…,Sk​ nonempty and S0S_0S0​ possibly empty.
  2. A maximal commutative ∗-subalgebra B\mathcal BB of A\mathcal AA contains every element of A\mathcal AA that commutes with B\mathcal BB (p. 14).
  3. Observations (i)–(ii) (p. 14): with B\mathcal BB in diagonal form, for X∈AX \in \mathcal AX∈A each IiXIiI_iXI_iIi​XIi​ is a multiple of IiI_iIi​, and I0X=XI0=0I_0X = XI_0 = 0I0​X=XI0​=0.
  4. Observation (iii) (p. 14): each block IiXIjI_iXI_jIi​XIj​ is zero or a nonzero multiple of a square unitary matrix.
  5. The unit of A\mathcal AA exists and is unique (p. 13).
  6. The relation i∼j  ⟺  IiAIj≠{0}i \sim j \iff I_i\mathcal A I_j \neq \{0\}i∼j⟺Ii​AIj​={0} is an equivalence relation (p. 14).
  7. A=⨁i=1dEiA\mathcal A = \bigoplus_{i=1}^d E_i\mathcal AA=⨁i=1d​Ei​A, where E1,…,EdE_1, \dots, E_dE1​,…,Ed​ are the minimal idempotents of CA\mathcal C_{\mathcal A}CA​ and each EiAE_i\mathcal AEi​A is simple (p. 14).
  8. Every simple matrix ∗-algebra is ∗-isomorphic to a full matrix algebra Ck×k\mathbb C^{k\times k}Ck×k (p. 14, proved pp. 14–15).

Milestones 7 and 8 together give the goal.

Significance

The result. A ∗-isomorphism preserves positive semidefiniteness, so Theorem 2.7 turns the constraint "X∈AX \in \mathcal AX∈A, X⪰0X \succeq 0X⪰0" into ddd independent constraints on blocks of sizes m1,…,mdm_1, \dots, m_dm1​,…,md​, with ∑kmk2=dim⁡A\sum_k m_k^2 = \dim \mathcal A∑k​mk2​=dimA. This is what makes the Lovász ϑ-number of symmetric graphs, the Delsarte and Schrijver bounds for codes, and the crossing-number bound of de Klerk et al. computable at scale (§§4–6 of the survey). Without it, an invariant SDP still has a variable of the original size nnn.

Formalizing it. The theorem is proved and textbook material; it is not open. As far as a search of the platform shows, it is not formalized in this form: Mathlib has Wedderburn–Artin for semisimple unital algebras over an algebraically closed field, which yields an algebra isomorphism but neither the star structure nor the non-unital case, and the platform holds a proved matrix-units statement for unital ∗-subalgebras (HarlowTASI.fdStarAlgebra_exists_matrixUnits, attached to this mission as a reference). The mission adds the non-unital ∗-isomorphism, the simultaneous unitary diagonalization of a commutative matrix ∗-algebra, and the intermediate facts of the elementary proof, each stated in a reusable form.

Difficulty

Two points make the obvious routes insufficient. First, a matrix ∗-algebra need not contain the identity: its unit is a projection onto a subspace, and the coordinates in S0S_0S0​ carry no part of the algebra. Statements and arguments that start from a unital subalgebra do not apply without first cutting the algebra down to the range of its unit. Second, an algebra isomorphism onto a product of matrix algebras is not enough: the isomorphism must commute with the conjugate transpose, since positive semidefiniteness is defined through it. Abstract Wedderburn–Artin provides the first kind of isomorphism, and turning it into a ∗-isomorphism requires choosing the matrix units compatibly with the adjoint, which is where the content of the theorem lies. The elementary proof avoids ring theory entirely but has to control every off-diagonal block IiXIjI_iXI_jIi​XIj​, which is the role of observations (i)–(iii).

Formalization scope

  • A matrix ∗-algebra is NonUnitalStarSubalgebra ℂ (Matrix (Fin n) (Fin n) ℂ); Mathlib's star on matrices is the conjugate transpose. The index set [n][n][n] is Fin n (0-based).
  • A ∗-isomorphism is StarAlgEquiv ℂ (≃⋆ₐ[ℂ]) on the subtype of A\mathcal AA: additive, multiplicative, ℂ-linear, star-preserving and bijective, exactly Definition 2.6.
  • ⨁k=1dCmk×mk\bigoplus_{k=1}^d \mathbb C^{m_k\times m_k}⨁k=1d​Cmk​×mk​ is the product type (k : Fin d) → Matrix (Fin (m k)) (Fin (m k)) ℂ with pointwise operations and star; it is ∗-isomorphic to the block-diagonal algebra (Matrix.blockDiagonal'). d=0d = 0d=0 is allowed and is needed for A={0}\mathcal A = \{0\}A={0}.
  • A partition [n]=S0∪S1∪⋯∪Sk[n] = S_0 \cup S_1 \cup \dots \cup S_k[n]=S0​∪S1​∪⋯∪Sk​ is a map S : Fin n → Option (Fin k), with none for S0S_0S0​ and some i for Si+1S_{i+1}Si+1​; the paper's block AijA_{ij}Aij​ is represented by the full-size product IiXIjI_iXI_jIi​XIj​.
  • The center is the set of elements of A\mathcal AA commuting with A\mathcal AA, not the commutant in Cn×n\mathbb C^{n\times n}Cn×n. "Simple" is the paper's definition: non-zero, with center CE\mathbb C ECE for the unit EEE.
  • Milestones 3, 4 and 6 are stated in the proof's normalized setting: B\mathcal BB is a maximal commutative ∗-subalgebra of A\mathcal AA that is already in diagonal form; the unitary change of basis is milestone 1.

The goal is not to be read with a unital StarSubalgebra (that adds the hypothesis I∈AI \in \mathcal AI∈A and is the case already covered by the reference item), with an AlgEquiv that ignores the star, or with a mere linear equivalence (which exists for dimensional reasons and has no content). Each of these would trivialize or weaken the statement.

Useful infrastructure, reusable beyond this mission: simultaneous unitary diagonalization of commuting normal matrices, the unit and the central decomposition of a non-unital finite-dimensional ∗-algebra, and an explicit ∗-isomorphism from a corner algebra onto Ck×k\mathbb C^{k\times k}Ck×k. Proofs of any milestone, and alternative routes to the goal (for example through Mathlib's Wedderburn–Artin plus a star-compatibility argument), are welcome.

Selected references

  • C. Bachoc, D. C. Gijswijt, A. Schrijver, F. Vallentin, Invariant semidefinite programs, in: Handbook on Semidefinite, Conic and Polynomial Optimization, Springer, 2012. arXiv:1007.2905v2. https://arxiv.org/abs/1007.2905
  • K. R. Davidson, C∗-Algebras by Example, Fields Institute Monographs 6, American Mathematical Society, 1996. https://doi.org/10.1090/fim/006
  • K. Gatermann, P. A. Parrilo, Symmetry groups, semidefinite programs, and sums of squares, Journal of Pure and Applied Algebra 192 (2004) 95–128. https://doi.org/10.1016/j.jpaa.2003.12.011
  • E. de Klerk, D. V. Pasechnik, A. Schrijver, Reduction of symmetric semidefinite programs using the regular ∗-representation, Mathematical Programming 109 (2007) 613–624. https://doi.org/10.1007/s10107-006-0039-7
  • R. A. Horn, C. R. Johnson, Matrix Analysis, Cambridge University Press, 1985. https://doi.org/10.1017/CBO9780511810817
11 thms4 active usersReviewed
Quantum Information·Captain: mikedeng1

Improvements in Quantum SDP-Solving with Applications 2: A Two-Outcome Measurement Implemented With Bias ε Gives a (1, a+1, ε)-Block-Encoding of Its POVM Element MResearch Paper

Motivation

Many recent quantum algorithms for linear algebra and optimization take their input as a block-encoding: a unitary circuit whose top-left block, after projecting a set of ancilla qubits onto ∣0⟩|0\rangle∣0⟩, approximates the matrix of interest. The quantum semidefinite-programming solver of van Apeldoorn and Gilyén (arXiv:1804.05058) introduces the quantum operator model, in which every constraint matrix of the SDP is given this way (Definition 2, p. 4). Block-encodings are also the input format of quantum singular value transformation and of Hamiltonian simulation by qubitization (Low and Chuang, arXiv:1610.06546).

A natural question is where block-encodings come from in applications. In §4.1, on shadow tomography, the constraint matrices are the elements EjE_jEj​ of two-outcome measurements, and what a user can do is perform those measurements, not write down their matrices. The closing remark of §4.1 (pp. 24–25) answers the question for that setting: if a two-outcome measurement can be implemented on a quantum computer with small bias, then a block-encoding of its measurement operator can be built from the same circuit with one extra qubit and one CNOT gate. The remark is credited to the same observation by Low and Chuang (arXiv:1707.05391).

Setting

A two-outcome POVM on a finite-dimensional system is a pair {M,I−M}\{M, I - M\}{M,I−M} of operators with MMM and I−MI - MI−M positive semidefinite. A mixed state (density matrix) is a positive semidefinite operator ρ\rhoρ with Tr⁡ρ=1\operatorname{Tr}\rho = 1Trρ=1; outcome MMM occurs with probability Tr⁡(Mρ)\operatorname{Tr}(M\rho)Tr(Mρ).

An implementation of the measurement on a quantum computer, as the paper fixes it, takes the input ρ\rhoρ, attaches aaa ancilla qubits in the state ∣0⟩⊗a|0\rangle^{\otimes a}∣0⟩⊗a, applies a unitary UUU to system and ancillas, measures in the computational basis, and accepts when the last qubit reads ∣0⟩|0\rangle∣0⟩:

ρ→ρ⊗∣0⟩⟨0∣⊗a→U(ρ⊗∣0⟩⟨0∣⊗a)U†→Tr⁡((I⊗∣0⟩⟨0∣) U(ρ⊗∣0⟩⟨0∣⊗a)U†).\rho \to \rho\otimes|0\rangle\langle 0|^{\otimes a} \to U\big(\rho\otimes|0\rangle\langle 0|^{\otimes a}\big)U^\dagger \to \operatorname{Tr}\Big((I\otimes|0\rangle\langle 0|)\,U\big(\rho\otimes|0\rangle\langle 0|^{\otimes a}\big)U^\dagger\Big).ρ→ρ⊗∣0⟩⟨0∣⊗a→U(ρ⊗∣0⟩⟨0∣⊗a)U†→Tr((I⊗∣0⟩⟨0∣)U(ρ⊗∣0⟩⟨0∣⊗a)U†).

The implementation has bias at most ε\varepsilonε if, for every state ρ\rhoρ,

∣Tr⁡((I⊗∣0⟩⟨0∣) U(ρ⊗∣0⟩⟨0∣⊗a)U†)−Tr⁡(Mρ)∣≤ε.(14)\Big|\operatorname{Tr}\Big((I\otimes|0\rangle\langle 0|)\,U\big(\rho\otimes|0\rangle\langle 0|^{\otimes a}\big)U^\dagger\Big) - \operatorname{Tr}(M\rho)\Big| \le \varepsilon. \qquad (14)​Tr((I⊗∣0⟩⟨0∣)U(ρ⊗∣0⟩⟨0∣⊗a)U†)−Tr(Mρ)​≤ε.(14)

Write K=(I⊗⟨0∣⊗a) U†(I⊗∣0⟩⟨0∣)U (I⊗∣0⟩⊗a)K = (I\otimes\langle 0|^{\otimes a})\,U^\dagger(I\otimes|0\rangle\langle 0|)U\,(I\otimes|0\rangle^{\otimes a})K=(I⊗⟨0∣⊗a)U†(I⊗∣0⟩⟨0∣)U(I⊗∣0⟩⊗a), an operator on the system. A unitary VVV on a′a'a′ ancilla qubits and the system is an (α,a′,ε)(\alpha, a', \varepsilon)(α,a′,ε)-block-encoding of AAA (Definition 2) if ∥A−α(⟨0∣⊗a′⊗I)V(∣0⟩⊗a′⊗I)∥≤ε\|A - \alpha(\langle 0|^{\otimes a'}\otimes I)V(|0\rangle^{\otimes a'}\otimes I)\| \le \varepsilon∥A−α(⟨0∣⊗a′⊗I)V(∣0⟩⊗a′⊗I)∥≤ε in the operator norm. Finally U′=U⊗I2U' = U\otimes I_2U′=U⊗I2​ adds one fresh qubit, and I⊗CNOTI\otimes\mathrm{CNOT}I⊗CNOT is a CNOT gate whose control is the measured qubit and whose target is the fresh qubit.

Formalization targets

Goal (§4.1, p. 25)

(14)  ⟹  U′†(I⊗CNOT)U′ is a (1, a+1, ε)-block-encoding of M.\text{(14)} \;\Longrightarrow\; U'^\dagger(I\otimes\mathrm{CNOT})U' \text{ is a } (1,\ a+1,\ \varepsilon)\text{-block-encoding of } M .(14)⟹U′†(I⊗CNOT)U′ is a (1, a+1, ε)-block-encoding of M.

The subnormalization is 111, the ancilla count is a′=a+1a' = a + 1a′=a+1 and the error is the same ε\varepsilonε as the bias; none of these is weakened.

Milestones (all p. 25, in the order of the derivation)

  1. The trace identity: ρ⊗∣0⟩⟨0∣⊗a=(I⊗∣0⟩⊗a)ρ(I⊗⟨0∣⊗a)\rho\otimes|0\rangle\langle 0|^{\otimes a} = (I\otimes|0\rangle^{\otimes a})\rho(I\otimes\langle 0|^{\otimes a})ρ⊗∣0⟩⟨0∣⊗a=(I⊗∣0⟩⊗a)ρ(I⊗⟨0∣⊗a), hence the acceptance probability equals Tr⁡(Kρ)\operatorname{Tr}(K\rho)Tr(Kρ).
  2. The equivalence ∀ρ: ∣Tr⁡([K−M]ρ)∣≤ε  ⟺  ∥K−M∥≤ε\forall\rho:\ |\operatorname{Tr}([K - M]\rho)| \le \varepsilon \iff \|K - M\| \le \varepsilon∀ρ: ∣Tr([K−M]ρ)∣≤ε⟺∥K−M∥≤ε, with ρ\rhoρ over density matrices.
  3. The CNOT identity K=(I⊗⟨0∣⊗a′) U′†(I⊗CNOT)U′ (I⊗∣0⟩⊗a′)K = (I\otimes\langle 0|^{\otimes a'})\,U'^\dagger(I\otimes\mathrm{CNOT})U'\,(I\otimes|0\rangle^{\otimes a'})K=(I⊗⟨0∣⊗a′)U′†(I⊗CNOT)U′(I⊗∣0⟩⊗a′).

Significance

The result. It converts an operational primitive, performing a measurement, into the input format that block-encoding algorithms consume, with an additive error equal to the measurement's bias and at the cost of one qubit and one CNOT. In the paper it is what makes the shadow-tomography application of §4.1 meaningful: the cost of the SDP solver is stated in terms of block-encodings of the EjE_jEj​, and this remark lets one replace that by the cost of controlled implementations of the measurements. More generally it shows that the quantum operator model is no stronger than the ability to measure.

Formalizing it. The paper proves the remark in a few displayed lines, one of which ("it is easy to see") is left to the reader and whose CNOT direction is not printed. No machine-checked version exists. A formal proof fixes the register conventions, makes the direction of the CNOT explicit, and contributes a reusable fact about matrices: for a Hermitian XXX, sup⁡ρ∣Tr⁡(Xρ)∣=∥X∥\sup_\rho |\operatorname{Tr}(X\rho)| = \|X\|supρ​∣Tr(Xρ)∣=∥X∥ over density matrices. The block-encoding predicate itself is already published on the platform and is reused.

Difficulty

The algebra of milestones 1 and 3 is bookkeeping over tensor-product index sets, and the main cost there is choosing representations that make the registers line up.

The one step with mathematical content is the direction "⇒\Rightarrow⇒" of milestone 2. The bias condition controls ∣Tr⁡(Xρ)∣|\operatorname{Tr}(X\rho)|∣Tr(Xρ)∣ only for density matrices ρ\rhoρ, that is, it bounds the numerical radius of X=K−MX = K - MX=K−M, while a block-encoding needs the operator norm. For a general matrix these differ by up to a factor of two, so the step needs XXX to be Hermitian: MMM is Hermitian as a POVM element, and KKK is Hermitian because it is a compression of the projector I⊗∣0⟩⟨0∣I\otimes|0\rangle\langle 0|I⊗∣0⟩⟨0∣. A formal proof must use both facts and exhibit a state that attains the norm.

Formalization scope

The Lean development lives in the namespace QuantumSDP18.MeasureBE. Its conventions are:

  • The system register is an arbitrary finite type ι\iotaι (a www-qubit system is ι={0,1}w\iota = \{0,1\}^wι={0,1}w). Operators are complex matrices; †\dagger† is the conjugate transpose; the operator norm is the platform's QAlgorithms.specNorm.
  • The ancilla register is Qubits c × Bool, so a=c+1≥1a = c + 1 \ge 1a=c+1≥1 and the Bool factor is the last, measured qubit. The basis state ∣0⟩|0\rangle∣0⟩ of any register is its all-false index.
  • (14) ranges over all density matrices (PosSemidef with trace 111), and its absolute value is the modulus of a complex trace.
  • The CNOT is the platform's QAlgorithms.cnot (control first), placed on the measured qubit (control) and the fresh qubit (target). With the opposite direction the block is U†UU^\dagger UU†U and the goal is false; the chosen direction is the only reading under which the page's identity holds.
  • The block-encoding predicate is the platform's QAlgorithms.IsBlockEncoding, which puts the ancilla register first, as Definition 2 does; the circuit, written system-first as on p. 25, is reindexed to match.
  • Added hypothesis: ε≥0\varepsilon \ge 0ε≥0 (a bias is nonnegative). It matters only for a zero-dimensional system, where (14) holds vacuously.

The goal keeps both POVM hypotheses (M⪰0M \succeq 0M⪰0 and I−M⪰0I - M \succeq 0I−M⪰0), and the bias condition quantifies over all states rather than one fixed state, under which the conclusion would be false. A formalization in which (14) ranges over arbitrary matrices, or which drops the CNOT and states only ∥K−M∥≤ε\|K - M\| \le \varepsilon∥K−M∥≤ε, is a different theorem.

Needed infrastructure: Kronecker products and reindexing of matrices, the unitarity of permutation matrices and of Kronecker products, and the variational characterization of the operator norm of a Hermitian matrix through its eigenvectors. The last is reusable beyond this mission. Proofs of the three milestones are welcome independently.

Selected references

  • J. van Apeldoorn, A. Gilyén, Improvements in quantum SDP-solving with applications, arXiv preprint, 2018 (ICALP 2019). https://arxiv.org/abs/1804.05058
  • G. H. Low, I. L. Chuang, Hamiltonian simulation by qubitization, arXiv preprint, 2016 (Quantum 3, 163, 2019). https://arxiv.org/abs/1610.06546
  • G. H. Low, I. L. Chuang, Hamiltonian simulation by uniform spectral amplification, arXiv preprint, 2017. https://arxiv.org/abs/1707.05391
  • S. Aaronson, Shadow tomography of quantum states, STOC 2018. https://arxiv.org/abs/1711.01053
8 thms4 active usersReviewed
Complexity TheoryGraph TheoryTheoretical Computer Science·Captain: mikedeng1

Most Tensor Problems Are NP-Hard 2: Graph 3-Colorability Reduces to Tensor Bilinear Feasibility over the Reals and over the Complex NumbersResearch Paper

Motivation

A matrix A∈Cn×nA \in \mathbb C^{n\times n}A∈Cn×n is singular exactly when the pair of linear systems x⊤A=0\mathbf x^\top A = 0x⊤A=0, Ay=0A\mathbf y = 0Ay=0 has a solution with both x\mathbf xx and y\mathbf yy nonzero, and this is decided in polynomial time by Gaussian elimination. The natural analogue for a 3-tensor replaces the two linear systems by three families of bilinear equations, one for each way of contracting the tensor against two vectors. For tensors whose dimensions satisfy the Gelfand–Kapranov–Zelevinsky condition, solvability of that system is equivalent to the vanishing of the hyperdeterminant, and for any tensor it is equivalent to 000 being a singular value in the sense of Lim (2005). The same system appears in multiview geometry (Cohen and Tomasi 1997).

C. J. Hillar and L.-H. Lim, Most Tensor Problems Are NP-Hard (J. ACM 60(6), 2013; arXiv:0911.1393), show that, unlike the matrix case, this feasibility question is NP-hard over R\mathbb RR and over C\mathbb CC (their Theorem 3.7). The proof is a reduction from graph 3-colorability through the polynomial color encoding of a graph, an idea the authors trace to Bayer's thesis (1982) and to Lovász (1994) and De Loera (1995). This mission formalizes that reduction and its consequence for tensor singular values (Theorem 6.2).

Setting

A 3-tensor over a field FFF is an array A=[ ⁣[aijk] ⁣]∈Fl×m×n\mathcal A = [\![a_{ijk}]\!] \in F^{l\times m\times n}A=[[aijk​]]∈Fl×m×n. Its slices are the matrices Ai(j,k)=Bj(i,k)=Ck(i,j)=aijkA_i(j,k) = B_j(i,k) = C_k(i,j) = a_{ijk}Ai​(j,k)=Bj​(i,k)=Ck​(i,j)=aijk​, all read off the same array.

Tensor bilinear feasibility (Problem 3.1) asks, for a rational tensor A∈Ql×m×n\mathcal A \in \mathbb Q^{l\times m\times n}A∈Ql×m×n and F=RF = \mathbb RF=R or C\mathbb CC, whether the system (9)

v⊤Aiw=0 (i≤l),u⊤Bjw=0 (j≤m),u⊤Ckv=0 (k≤n)\mathbf v^\top A_i\mathbf w = 0\ (i \le l),\qquad \mathbf u^\top B_j \mathbf w = 0\ (j \le m),\qquad \mathbf u^\top C_k \mathbf v = 0\ (k \le n)v⊤Ai​w=0 (i≤l),u⊤Bj​w=0 (j≤m),u⊤Ck​v=0 (k≤n)

has a solution u∈Fl\mathbf u \in F^lu∈Fl, v∈Fm\mathbf v\in F^mv∈Fm, w∈Fn\mathbf w \in F^nw∈Fn with each of the three vectors nonzero. In Lean this is TBF A.

The color encoding CGC_GCG​ of a graph G=(V,E)G = (V,E)G=(V,E) on vvv vertices (Definition 2.9) is the set of 4v4v4v quadratics in x1,…,xv,y1,…,yv,zx_1,\dots,x_v,y_1,\dots,y_v,zx1​,…,xv​,y1​,…,yv​,z:

xiyi−z2,yiz−xi2,xiz−yi2,∑j:{i,j}∈E(xi2+xixj+xj2),i=1,…,v.x_iy_i - z^2,\quad y_iz - x_i^2,\quad x_iz - y_i^2,\quad \sum_{j:\{i,j\}\in E}(x_i^2 + x_ix_j + x_j^2),\qquad i = 1,\dots,v .xi​yi​−z2,yi​z−xi2​,xi​z−yi2​,j:{i,j}∈E∑​(xi2​+xi​xj​+xj2​),i=1,…,v.

The tensor AG∈Zl×m×n\mathcal A_G \in \mathbb Z^{l\times m\times n}AG​∈Zl×m×n of the proof of Theorem 3.7 has m=n=2v+1m = n = 2v+1m=n=2v+1 and l=v(2v+5)l = v(2v+5)l=v(2v+5) slices: v(2v+1)v(2v+1)v(2v+1) slices whose bilinear forms are the 2×22\times 22×2 minors of the matrix [v w][\mathbf v\ \mathbf w][v w], then 3v+v3v + v3v+v slices whose bilinear forms restrict, on w=v\mathbf w = \mathbf vw=v, to the polynomials of CGC_GCG​ (Lean: AG G).

The tensor B\mathcal BB of Lemma 3.6 doubles a real tensor A\mathcal AA into R2l×2m×2n\mathbb R^{2l\times 2m\times 2n}R2l×2m×2n through the slices Bi=[Ai00−Ai]B_i = \left[\begin{smallmatrix} A_i & 0 \\ 0 & -A_i\end{smallmatrix}\right]Bi​=[Ai​0​0−Ai​​], Bl+i=[0AiAi0]B_{l+i} = \left[\begin{smallmatrix} 0 & A_i \\ A_i & 0\end{smallmatrix}\right]Bl+i​=[0Ai​​Ai​0​] (Lean: doubling A).

An ℓ2\ell^2ℓ2-singular value σ\sigmaσ of A\mathcal AA (Definition 6.1) admits nonzero u,v,w\mathbf u,\mathbf v,\mathbf wu,v,w with ∑j,kaijkvjwk=σui\sum_{j,k}a_{ijk}v_jw_k = \sigma u_i∑j,k​aijk​vj​wk​=σui​ and the two analogous equations; an ℓ3\ell^3ℓ3-singular value has σui2\sigma u_i^2σui2​, σvj2\sigma v_j^2σvj2​, σwk2\sigma w_k^2σwk2​ on the right. At σ=0\sigma = 0σ=0 both reduce to (9).

Formalization targets

Goal: Theorem 3.7

3-COLORABILITY≤pTBFRand3-COLORABILITY≤pTBFC,\textsf{3-COLORABILITY} \le_p \textsf{TBF}_{\mathbb R} \quad\text{and}\quad \textsf{3-COLORABILITY} \le_p \textsf{TBF}_{\mathbb C},3-COLORABILITY≤p​TBFR​and3-COLORABILITY≤p​TBFC​,

polynomial-time many-one reductions between languages of binary codes. NP-hardness of tensor bilinear feasibility then follows from the NP-completeness of 3-colorability (Karp 1972), which is cited and not part of the statement.

Milestones, in the order the proof uses them

  1. Lemma 2.10. CGC_GCG​ has a nonzero complex zero iff GGG is 3-colorable.
  2. The minors (proof of Theorem 3.7). For nonzero v,w∈CN\mathbf v, \mathbf w \in \mathbb C^Nv,w∈CN, all 2×22\times22×2 minors of [v w][\mathbf v\ \mathbf w][v w] vanish iff v=cw\mathbf v = c\mathbf wv=cw for some c∈Cc \in \mathbb Cc∈C.
  3. Correctness over C\mathbb CC (proof of Theorem 3.7). For v≥1v \ge 1v≥1, TBFC(AG)  ⟺  G\mathrm{TBF}_{\mathbb C}(\mathcal A_G) \iff GTBFC​(AG​)⟺G is 3-colorable.
  4. Lemma 3.6. TBFR(B)  ⟺  TBFC(A)\mathrm{TBF}_{\mathbb R}(\mathcal B) \iff \mathrm{TBF}_{\mathbb C}(\mathcal A)TBFR​(B)⟺TBFC​(A) for real A\mathcal AA.
  5. Theorem 6.2 (further result). 3-colorability reduces to deciding whether 000 is an ℓ2\ell^2ℓ2-singular value, and whether it is an ℓ3\ell^3ℓ3-singular value, over R\mathbb RR and over C\mathbb CC.

Significance

Theorem 3.7 is the hub of the paper's bilinear results: Section 6 derives from it the NP-hardness of deciding whether 000 is a tensor singular value (Theorem 6.2), and the triple bilinear problem (Theorem 3.8) is handled by the same techniques. It separates tensors from matrices in a precise sense: the matrix analogue of (9) is decided by a determinant, while the tensor version encodes a classical NP-complete problem. It does not settle the hardness of the hyperdeterminant, since the dimensions l=v(2v+5)l = v(2v+5)l=v(2v+5), m=n=2v+1m = n = 2v+1m=n=2v+1 of AG\mathcal A_GAG​ violate the GKZ condition; the paper leaves that as a conjecture.

The result is proved in the paper; none of it is formalized on Prove2Me or, to our knowledge, elsewhere. A complete development produces a machine-checked polynomial-time reduction in Cook's Turing-machine model between two concrete algebraic problems, the color-encoding lemma for 3-colorability (reusable by any reduction that goes through polynomial systems, including Theorems 1.3 and 2.6 of the same paper), and the realification of bilinear systems.

Difficulty

The algebra of the reduction is short; two places need care. First, the bilinear system does not see CGC_GCG​ directly: (9) involves two independent vectors v,w\mathbf v, \mathbf wv,w, and the reduction recovers the quadratic system only because the minors force v=cw\mathbf v = c\mathbf wv=cw, which requires both vectors to be nonzero. Second, the converse direction must produce a nonzero u\mathbf uu satisfying the second and third families, a homogeneous linear system of 4v+24v+24v+2 equations in l=v(2v+5)l = v(2v+5)l=v(2v+5) unknowns; this works only when l>4v+2l > 4v+2l>4v+2, which fails for the empty graph, so the reduction has to treat v=0v = 0v=0 separately.

The goal also asks for polynomial-time computability in a Turing-machine model: decoding a graph code, rejecting malformed words, and writing the binary code of AG\mathcal A_GAG​ (or of its doubling over R\mathbb RR). This bookkeeping, not the algebra, is the bulk of a complete proof.

Formalization scope

  • Tensors are functions I → J → K → F over finite index types, 0-based: the paper's aijka_{ijk}aijk​ is A (i-1) (j-1) (k-1). Problem 3.1 requires u\mathbf uu, v\mathbf vv, w\mathbf ww each nonzero, not merely (u,v,w)≠0(\mathbf u, \mathbf v, \mathbf w) \neq 0(u,v,w)=0, and the three equation families come from one tensor.
  • The doubled tensor of Lemma 3.6 is indexed by I ⊕ I, J ⊕ J, K ⊕ K, with Sum.inr i standing for the paper's index l+il+il+i. Lemma 3.6 is stated for this explicit B\mathcal BB; a bare existential would be witnessed by any tensor with the right truth value. Only the equivalence of existence is stated, not the paper's "one-to-one" correspondence (which pairs u′=(p,q)\mathbf u' = (\mathbf p,\mathbf q)u′=(p,q) with the conjugate-type vector p−iq\mathbf p - i\mathbf qp−iq).
  • The paper does not print the matrices of the last 4v4v4v slices of AG\mathcal A_GAG​. The mission fixes the bilinearizations xiy^i−zz^x_i\hat y_i - z\hat zxi​y^​i​−zz^, yiz^−xix^iy_i\hat z - x_i\hat x_iyi​z^−xi​x^i​, xiz^−yiy^ix_i\hat z - y_i\hat y_ixi​z^−yi​y^​i​ and ∑j∼i(xix^i+xix^j+xjx^j)\sum_{j\sim i}(x_i\hat x_i + x_i\hat x_j + x_j\hat x_j)∑j∼i​(xi​x^i​+xi​x^j​+xj​x^j​); each restricts to the printed polynomial on w=v\mathbf w = \mathbf vw=v.
  • "Nontrivial zero" in the minors claim is read as both v\mathbf vv and w\mathbf ww nonzero; the correctness milestone over C\mathbb CC assumes v≥1v \geq 1v≥1, since for v=0v = 0v=0 the printed tensor has no slices and its system (9) is infeasible.
  • "Polynomially reducible" is formalized as Cook–Karp many-one reducibility (CookPvsNP.PolyReducible), which the paper's proof constructs and which implies the paper's oracle notion of §1.4. "NP-hard" in Theorem 6.2 is rendered the same way, and "(ℓ2\ell^2ℓ2 or ℓ3\ell^3ℓ3)" as the claim for each notion. Rational inputs are coded as numerator and denominator in binary; tensors as l,m,nl, m, nl,m,n and then their entries in lexicographic order.
  • The singular-value equations (20)–(21) are taken literally over C\mathbb CC, without conjugates and without normalization; only σ=0\sigma = 0σ=0 is used, where they are scale-free.
  • NP-completeness of 3-colorability is cited, not formalized; no statement mentions P, NP-membership, or hyperdeterminants.
  • A trivializing formalization is ruled out: the goal is the polynomial-time reduction, not the bare equivalence of yes-instances, and the reduction must handle every input word.

The mission reuses the published definitions CookPvsNP_defs (Turing machines, polynomial-time computability, many-one reducibility) and ProjSchedTW.Complexity.Encoding (the binary alphabet and number codes), and Mathlib's SimpleGraph.Colorable. Contributions welcome: the algebraic milestones (Lemma 2.10, the minors, Lemma 3.6) are independent and self-contained; a library of polynomial-time computable list and arithmetic operations on BSym codes would serve both this goal and Theorem 6.2.

Selected references

  • C. J. Hillar, L.-H. Lim, Most Tensor Problems Are NP-Hard, J. ACM 60(6), Art. 45, 2013. https://doi.org/10.1145/2512329 (arXiv:0911.1393v5, https://arxiv.org/abs/0911.1393)
  • R. M. Karp, Reducibility among combinatorial problems, in Complexity of Computer Computations, Plenum, 1972. https://doi.org/10.1007/978-1-4684-2001-2_9
  • L.-H. Lim, Singular values and eigenvalues of tensors: a variational approach, Proc. IEEE CAMSAP, 2005. https://arxiv.org/abs/math/0607648
  • I. M. Gelfand, M. M. Kapranov, A. V. Zelevinsky, Discriminants, Resultants, and Multidimensional Determinants, Birkhäuser, 1994. https://doi.org/10.1007/978-0-8176-4771-1
  • S. A. Cook, The P versus NP problem, Clay Mathematics Institute problem description, 2000. https://www.claymath.org/wp-content/uploads/2022/06/pvsnp.pdf
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Complexity TheoryGraph TheoryTheoretical Computer Science·Captain: mikedeng1

Most Tensor Problems Are NP-Hard 1: Graph 3-Colorability Reduces to Deciding Whether 0 Is an Eigenvalue of a Rational 3-Tensor over the RealsResearch Paper

Motivation

Eigenvalues of matrices are computable in polynomial time to any accuracy, and numerical linear algebra rests on that fact. Higher-order tensors appear in statistics (moment and cumulant tensors), signal processing, quantum information and polynomial optimization, and several notions of tensor eigenvalue were proposed for them, independently by Lim and by Qi in 2005 (Lim 2005; Qi 2005). Hillar and Lim (J. ACM 60(6), 2013, Art. 45; arXiv:0911.1393) showed that most of the natural tensor analogues of tractable matrix problems are NP-hard. Their first example, Theorem 1.3, concerns the simplest one: deciding whether a given number is an eigenvalue of a 3-tensor.

This mission formalizes that theorem together with the lemmas its proof uses. The reduction starts from graph 3-colorability, and its intermediate step, quadratic feasibility (Theorem 2.6), is reused throughout the paper: the bilinear, singular value and triple-bilinear results all go through the same color encoding.

Setting

A 3-tensor over a field FFF is an array A=[ ⁣[aijk] ⁣]∈Fn×n×n\mathcal A=[\![a_{ijk}]\!]\in F^{n\times n\times n}A=[[aijk​]]∈Fn×n×n. A scalar λ∈F\lambda\in Fλ∈F is an eigenvalue of A\mathcal AA (eq. (3) of the paper) if there is a nonzero x∈Fn\mathbf x\in F^nx∈Fn with

∑i,j=1naijk xixj=λxk,k=1,…,n.\sum_{i,j=1}^{n}a_{ijk}\,x_ix_j=\lambda x_k,\qquad k=1,\dots,n.i,j=1∑n​aijk​xi​xj​=λxk​,k=1,…,n.

The sum is over the first two indices. For λ=0\lambda=0λ=0 the condition is invariant under scaling of x\mathbf xx, so no normalization enters.

Problem 1.2 (tensor λ\lambdaλ-eigenvalue) fixes F∈{R,C}F\in\{\mathbb R,\mathbb C\}F∈{R,C} and λ∈Q\lambda\in\mathbb Qλ∈Q, and asks, for a rational tensor A∈Qn×n×n\mathcal A\in\mathbb Q^{n\times n\times n}A∈Qn×n×n, whether λ\lambdaλ is an eigenvalue of A\mathcal AA with an eigenvector in FnF^nFn.

Problem 2.2 (quadratic feasibility) asks, for rational matrices A1,…,Am∈Qn×nA_1,\dots,A_m\in\mathbb Q^{n\times n}A1​,…,Am​∈Qn×n, whether the system x⊤Aix=0\mathbf x^\top A_i\mathbf x=0x⊤Ai​x=0 (i=1,…,mi=1,\dots,mi=1,…,m) has a nonzero solution x∈Fn\mathbf x\in F^nx∈Fn.

A proper 3-coloring of a simple graph G=(V,E)G=(V,E)G=(V,E) assigns one of three colors to each vertex so that adjacent vertices receive different colors.

The color encoding CGC_GCG​ of a graph on vertices 1,…,v1,\dots,v1,…,v (Definition 2.9) is the family of 4v4v4v quadratics in x1,…,xv,y1,…,yv,zx_1,\dots,x_v,y_1,\dots,y_v,zx1​,…,xv​,y1​,…,yv​,z:

xiyi−z2,yiz−xi2,xiz−yi2,∑j:{i,j}∈E(xi2+xixj+xj2),i=1,…,v.x_iy_i-z^2,\quad y_iz-x_i^2,\quad x_iz-y_i^2,\quad \sum_{j:\{i,j\}\in E}(x_i^2+x_ix_j+x_j^2),\qquad i=1,\dots,v.xi​yi​−z2,yi​z−xi2​,xi​z−yi2​,j:{i,j}∈E∑​(xi2​+xi​xj​+xj2​),i=1,…,v.

Lemma 2.7 replaces a complex quadratic system by a real one of twice the size, and Lemma 2.8 pads a real system to a square one. Applied to CGC_GCG​, they give NNN real quadratics x⊤Bkx\mathbf x^\top B_k\mathbf xx⊤Bk​x in NNN unknowns. The tensor TGT_GTG​ with aijk=(Bk)ija_{ijk}=(B_k)_{ij}aijk​=(Bk​)ij​ is the output of the reduction.

Formalization targets

Goal: Theorem 1.3

3-COL ≤p TENSOR-0-EIGR.\textsf{3-COL}\ \le_p\ \textsf{TENSOR-0-EIG}_{\mathbb R}.3-COL ≤p​ TENSOR-0-EIGR​.

Graph 3-colorability is polynomial-time many-one reducible to the language of binary codes of rational tensors having 000 as a real eigenvalue.

Milestones, in the order the proof uses them

  1. Lemma 2.10. CGC_GCG​ has a nonzero complex solution if and only if GGG is 3-colorable.
  2. Lemma 2.7. The 2m2m2m real equations with matrices [Ai00−Ai]\begin{bmatrix}A_i&0\\0&-A_i\end{bmatrix}[Ai​0​0−Ai​​] and [0AiAi0]\begin{bmatrix}0&A_i\\A_i&0\end{bmatrix}[0Ai​​Ai​0​] have a nonzero real solution iff {z⊤Aiz=0}\{\mathbf z^\top A_i\mathbf z=0\}{z⊤Ai​z=0} has a nonzero complex solution.
  3. Lemma 2.8. Padding to r≥m+1r\ge m+1r≥m+1 equations in s≥ns\ge ns≥n unknowns preserves real feasibility.
  4. Theorem 2.6. 3-COL≤p\textsf{3-COL}\le_p3-COL≤p​ quadratic feasibility over R\mathbb RR and over C\mathbb CC.
  5. Proof of Theorem 1.3, first step. 000 is a real eigenvalue of A\mathcal AA iff the square system x⊤Akx=0\mathbf x^\top A_k\mathbf x=0x⊤Ak​x=0, Ak(i,j)=aijkA_k(i,j)=a_{ijk}Ak​(i,j)=aijk​, has a nonzero real solution.
  6. Proof of Theorem 1.3, the construction. GGG is 3-colorable iff 000 is a real eigenvalue of TGT_GTG​.

Significance

The result. Theorem 1.3 shows that deciding whether 000 is an eigenvalue of a rational 3-tensor over R\mathbb RR is NP-hard, in contrast to the matrix case. Because the instance is a single rational tensor with small integer entries, the hardness does not come from numerical precision: it is a property of the exact problem. The same encoding underlies the paper's hardness of approximating an eigenvector (Theorem 1.5) and its remarks on counting eigenvectors (Corollary 1.16).

Formalizing it. The result is proved in the paper, but no part of it is machine-checked. The mission adds three things. It gives a precise language-level statement of what "polynomially reducible" means for this problem. It gives a checked equivalence between 3-colorability and the eigenvalue condition for the explicit tensor TGT_GTG​. And it gives reusable statements about homogeneous quadratic systems (realification and padding), which the bilinear and singular value missions of this series also need.

Difficulty

The algebraic core is Lemma 2.10, and its reverse direction is where a first attempt fails. The fourth family of CGC_GCG​ does not say that each term xi2+xixj+xj2x_i^2+x_ix_j+x_j^2xi2​+xi​xj​+xj2​ vanishes; it says only that their sum over the neighbours of iii vanishes, over C\mathbb CC, where nonzero terms can cancel. A common zero yields a coloring only after the first three families have pinned down each coordinate, and the case z=0z=0z=0 must be excluded separately.

Lemma 2.7 needs care because the matrices AiA_iAi​ are not assumed symmetric: the imaginary part of z⊤Az\mathbf z^\top A\mathbf zz⊤Az is u⊤Av+v⊤Au\mathbf u^\top A\mathbf v+\mathbf v^\top A\mathbf uu⊤Av+v⊤Au, not 2u⊤Av2\mathbf u^\top A\mathbf v2u⊤Av. Lemma 2.8 uses that R\mathbb RR is formally real; it fails over C\mathbb CC.

At the language level, the reduction must be exhibited as a Turing machine computation on binary codes in polynomial time. That is bookkeeping, but it is the part the paper does not write down.

Formalization scope

  • Tensors and vectors. Tensors are arrays Fin n → Fin n → Fin n → F, vectors Fin n → F, and indices are 0-based. The eigenvalue condition is eq. (3) verbatim, without normalization; for λ=0\lambda=0λ=0 none is needed. Rational data are cast into R\mathbb RR or C\mathbb CC.
  • Quadratic polynomials. A homogeneous quadratic is a (not necessarily symmetric) rational matrix MMM, read as x⊤Mx\mathbf x^\top M\mathbf xx⊤Mx, and the monomial xaxbx_ax_bxa​xb​ is the matrix unit EabE_{ab}Eab​. A vertex without neighbours contributes the zero polynomial to CGC_GCG​.
  • Choices in the construction. The square size is N=8v+2N=8v+2N=8v+2. It meets Lemma 2.8's bounds r≥8v+1r\ge 8v+1r≥8v+1 and s≥4v+2s\ge 4v+2s≥4v+2 for every v≥0v\ge 0v≥0; Example 1.4's count differs and is not used.
  • Reducibility. "Polynomially reducible" is Cook's polynomial-time many-one reducibility (CookPvsNP.PolyReducible, published definition CookPvsNP_defs). The paper's reduction maps one graph to one tensor, and a many-one reduction implies the oracle notion of its §1.4.
  • Binary codes. Instances are coded over the alphabet BSym with the binary codes of the published definition ProjSchedTW.Complexity.Encoding. A graph is ν\nuν followed by its adjacency matrix. A rational is its numerator then its denominator. A tensor is nnn followed by its entries in lexicographic order. The target language contains all rational tensors, not only integral ones.
  • Not formalized. NP-completeness of 3-colorability (Karp 1972) is cited, not formalized, and the goal states only the reduction. Approximation (Theorem 1.5), counting (Corollary 1.16) and the solution count of Example 1.4 are out of scope.
  • Trivializations ruled out. Every feasibility statement requires a nonzero solution, since the zero vector solves every homogeneous system. The goal includes polynomial-time computability of the reduction, not just the existence of an equivalence-preserving map, which would be trivial. The milestones concern the paper's explicit CGC_GCG​ and TGT_GTG​, not an arbitrary tensor.

Contributions are welcome in four places:

  • proofs of the milestones;
  • a polynomial-time Turing machine computing G↦TGG\mapsto T_GG↦TG​ on codes;
  • general lemmas on homogeneous quadratic systems over formally real fields;
  • a composition (transitivity) lemma for CookPvsNP.PolyReducible.

Selected references

  • C. J. Hillar and L.-H. Lim, Most Tensor Problems Are NP-Hard, Journal of the ACM 60(6), Article 45, 2013. https://doi.org/10.1145/2512329 (arXiv:0911.1393v5, https://arxiv.org/abs/0911.1393)
  • L.-H. Lim, Singular values and eigenvalues of tensors: a variational approach, Proc. IEEE CAMSAP 2005, pp. 129–132. https://doi.org/10.1109/CAMAP.2005.1574201
  • L. Qi, Eigenvalues of a real supersymmetric tensor, Journal of Symbolic Computation 40(6), 2005, pp. 1302–1324. https://doi.org/10.1016/j.jsc.2005.05.007
  • 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
  • S. Cook, The P versus NP problem, Clay Mathematics Institute Millennium Problem description, 2000. https://www.claymath.org/millennium/p-vs-np/
14 thms4 active usersReviewed
Graph TheoryProbabilityTheoretical Computer Science·Captain: iris

Incremental All-Pairs Effective Resistance in Almost-Linear Time: (1±ε)(1\pm\varepsilon)(1±ε)-Approximate Sparse-Demand Energies in Total Time m(1/ε)O(log⁡nlog⁡log⁡n)m(1/\varepsilon)^{O(\sqrt{\log n\log\log n})}m(1/ε)O(lognloglogn​)Research Paper

Why incremental effective resistances

The effective resistance between two vertices of a graph with edge conductances is the energy of the electrical flow that sends one unit of current between them. More generally, a demand d∈RVd\in\mathbb R^Vd∈RV with zero sum has energy d⊤LG†dd^\top L_G^\dagger dd⊤LG†​d, where LGL_GLG​ is the graph Laplacian. These quantities drive spectral sparsification (Spielman–Srivastava, SIAM J. Comput. 2011), electrical-flow and interior-point methods for maximum flow, and graph analysis based on commute times and leverage scores.

When the graph changes, recomputing energies from scratch costs a Laplacian solve per query. A line of work maintains Schur complements onto small terminal sets instead:

  • Durfee, Gao, Goranci and Peng (STOC 2019) gave the first dynamic Laplacian solvers with sublinear update and query times on general graphs.
  • Chen, Goranci, Henzinger, Peng and Saranurak (FOCS 2020) maintained a hierarchy of Schur complements and obtained n2/3+o(1)ε−O(1)n^{2/3+o(1)}\varepsilon^{-O(1)}n2/3+o(1)ε−O(1) amortized time per operation for all-pairs effective resistances.
  • Goranci, Kyng, Probst Gutenberg, Zhao and Zöcklein (STOC 2027 submission, manuscript of November 3, 2026) obtain subpolynomial time per operation under edge insertions. This mission formalizes their main theorem.

Setting

A graph G=(V,E,c)G=(V,E,c)G=(V,E,c) has nnn vertices and positive edge capacities cec_ece​; parallel edges are allowed. Its Laplacian is LG=∑e=(u,v)ce(1u−1v)(1u−1v)⊤L_G=\sum_{e=(u,v)}c_e(\mathbf 1_u-\mathbf 1_v)(\mathbf 1_u-\mathbf 1_v)^\topLG​=∑e=(u,v)​ce​(1u​−1v​)(1u​−1v​)⊤, and LG†L_G^\daggerLG†​ is its Moore–Penrose pseudoinverse. A demand ddd is componentwise feasible if it sums to zero on every connected component of GGG.

The data structure starts from the empty graph on nnn vertices and an accuracy 0<ε<1/20<\varepsilon<1/20<ε<1/2. It processes a sequence of operations, fixed in advance (an oblivious adversary), one at a time:

  1. InsertEdge(u,v,c)\mathrm{InsertEdge}(u,v,c)InsertEdge(u,v,c) adds an edge of capacity ccc; the ratio of any two capacities is at most nbn^bnb;
  2. Query(d)\mathrm{Query}(d)Query(d) gives a componentwise feasible demand with at most (1+log⁡n)a(1+\log n)^a(1+logn)a nonzero entries and must return a number in [(1−ε) d⊤LG†d, (1+ε) d⊤LG†d][(1-\varepsilon)\,d^\top L_G^\dagger d,\,(1+\varepsilon)\,d^\top L_G^\dagger d][(1−ε)d⊤LG†​d,(1+ε)d⊤LG†​d] for the current graph GGG.

The algorithm is one program of a randomized real RAM: unit-cost exact arithmetic, square roots and powers, integer pointers, fair coins, and no floor. It reads each operation from its memory and keeps its own state between operations.

The proof works with leverage degrees ℓG(v)=∑wc(v,w)Reff(v,w)\ell^G(v)=\sum_{w}c(v,w)R_{\mathrm{eff}}(v,w)ℓG(v)=∑w​c(v,w)Reff​(v,w), the sum of the leverage scores of the edges at vvv, and with the Schur complement SC(G,T)SC(G,T)SC(G,T) onto a terminal set TTT. The excess is qG(v)=ℓG(v)−2q^G(v)=\ell^G(v)-2qG(v)=ℓG(v)−2. Inserting vvv into TTT costs fT(v)=ℓT∪{v}G(v)f_T(v)=\ell^G_{T\cup\{v\}}(v)fT​(v)=ℓT∪{v}G​(v), the leverage degree of vvv in SC(G,T∪{v})SC(G,T\cup\{v\})SC(G,T∪{v}). The standard random walk moves from uuu to www with probability cuw/duc_{uw}/d_ucuw​/du​, where dud_udu​ is the capacitated degree.

Formalization targets

Goal: Theorem 1.1

For all exponents a,b∈Na,b\in\mathbb Na,b∈N, c>1c>1c>1 and κ>0\kappa>0κ>0 there are C>0C>0C>0 and one program PPP such that for every n≥1n\ge1n≥1, ε∈(0,1/2)\varepsilon\in(0,1/2)ε∈(0,1/2) and valid sequence of MMM operations:

total work≤C M (1/ε)Clog⁡n log⁡log⁡non every coin outcome,\text{total work}\le C\,M\,(1/\varepsilon)^{C\sqrt{\log n\,\log\log n}}\quad\text{on every coin outcome},total work≤CM(1/ε)Clognloglogn​on every coin outcome, M≤nκ ⟹ Pr⁡[some answer is outside its (1±ε) interval]≤n−c.M\le n^\kappa\ \Longrightarrow\ \Pr[\text{some answer is outside its }(1\pm\varepsilon)\text{ interval}]\le n^{-c}.M≤nκ ⟹ Pr[some answer is outside its (1±ε) interval]≤n−c.

The goal fixes no constant, so it survives any improvement of the exponent.

Milestones

The milestones are the mathematical statements the proof rests on, in the order the proof uses them:

  1. Schur complements: Fact 3.4, which says they preserve energies and resistances, raise conductances and compose.
  2. Leverage degrees: Fact 3.6, with Foster's identity ∑vℓG(v)=2(∣V∣−1)\sum_v\ell^G(v)=2(|V|-1)∑v​ℓG(v)=2(∣V∣−1).
  3. Excess under elimination and its walk form: Lemmas 3.7 and 3.8.
  4. Leverage degrees above a random-walk hitting set: Lemma 3.10.
  5. Multiplicative weights: deterministic (Lemma 4.3) and with stochastic feedback (Lemma 4.11).
  6. Averaging bounds ≤4\le4≤4 for random terminal sets: Lemmas 4.4 and 4.9, built on Lemma 4.8.
  7. Subadditivity over terminal sets: Lemma 4.13.
  8. The grounded inverse LSˉ,Sˉ−1L^{-1}_{\bar S,\bar S}LSˉ,Sˉ−1​ as random-walk quantities: Lemma 5.2.
  9. The Doob-transformed sampling chain: Lemma 5.6.
  10. Connectivity augmentation (23) and the composition of the hierarchy's levels, from the proof of Theorem 1.1 (pp.38–39).

Significance

Theorem 1.1 is the first data structure with subpolynomial update and query time for all-pairs effective resistances on general graphs, even when only insertions are allowed. With d=1s−1td=\mathbf 1_s-\mathbf 1_td=1s​−1t​ it gives (1±ε)(1\pm\varepsilon)(1±ε)-approximate resistances in no(1)n^{o(1)}no(1) amortized time per operation when ε≥1/log⁡O(1)n\varepsilon\ge1/\log^{O(1)}nε≥1/logO(1)n. Its central tool is a terminal-robust Schur complement: a terminal set enlarged so that inserting any further terminal changes the Schur complement by only O~(1)\tilde O(1)O~(1) leverage-score mass in expectation.

The result is new and unpublished; no part of it is formalized. A formalization produces the first dynamic-data-structure statement about graph Laplacians on the platform. It also yields a reusable library of Schur complements, leverage degrees, hitting probabilities from path weights, grounded Laplacian inverses and multiplicative-weights bounds. Several milestones (Facts 3.4, 3.6, Lemmas 3.7, 4.3, 5.2) are classical results that have no formal proof on the platform.

Difficulty

The obvious approach maintains a Schur complement onto a small terminal set and adds a query's support as terminals. It fails because inserting one terminal can change polynomially many edges of the Schur complement. In a hierarchy of Schur complements these changes compound from level to level. Bounding the change requires controlling leverage-score mass in expectation over a randomized terminal set. That set must be computed by multiplicative weights from feedback that can only be estimated by sampling random walks, and a solver must close the gap between expectation bounds and a worst-case, online time bound. The goal also asks for a time bound on every coin outcome. An expected-time argument does not suffice; the paper caps each copy's work with a budget.

Formalization scope

  • Graphs. The goal uses edge lists on {0,…,n−1}\{0,\dots,n-1\}{0,…,n−1}, with Laplacians as sums over the list; loops are allowed and contribute nothing. The milestones use graphs as symmetric conductance functions on a finite type with zero diagonal, so parallel edges are merged. Merging changes no Laplacian, resistance, leverage degree or walk. The combinatorial degree becomes the number of distinct neighbours.
  • Pseudoinverse and Schur complements. L†L^\daggerL† is the published Moore–Penrose pseudoinverse. Schur complements use Mathlib's matrix inverse of the eliminated block. Milestones assume the graph connected, which is the paper's standing assumption (p.10).
  • Walks. Every probability is a sum of path weights of the published MarkovMixing network walk. No probability is defined by a linear-algebra formula, so Lemmas 3.8, 5.2 and 5.6 are not tautologies.
  • The machine and the protocol. The program is the published exact real RAM PNormReg.Machine. Operations are written into its memory one at a time, together with nnn and ε\varepsilonε, so no initialization is free and zero operations cost zero time. Registers are reset between operations, while memory, the coin position and the work counter are kept. Logarithms are natural, and ⋅\sqrt{\cdot}⋅​ of a negative number is 000.
  • Trivializations ruled out. One finite program serves all nnn. The constants CCC and PPP come after a,b,c,κa,b,c,\kappaa,b,c,κ and before n,εn,\varepsilonn,ε and the sequence. Without floor the machine cannot pack words, and the time bound depends only on n,ε,Mn,\varepsilon,Mn,ε,M.
  • Contributions welcome: proofs of the milestones, especially Facts 3.4 and 3.6, which unlock the rest. Also welcome: a formal treatment of spectral sparsification ([SS11]) and of the dynamic vertex sparsifier ([DGGP19]) on this machine, both of which the proof of the goal imports.

Selected references

  • G. Goranci, R. Kyng, M. Probst Gutenberg, Y. Zhao, G. Zöcklein, Incremental All-Pairs Effective Resistance in Almost-Linear Time, STOC 2027 submission, manuscript dated November 3, 2026 (no public version).
  • D. Durfee, Y. Gao, G. Goranci, R. Peng, Fully dynamic spectral vertex sparsifiers and applications, STOC 2019. https://doi.org/10.1145/3313276.3316379
  • L. Chen, G. Goranci, M. Henzinger, R. Peng, T. Saranurak, Fast Dynamic Cuts, Distances and Effective Resistances via Vertex Sparsifiers, FOCS 2020. https://doi.org/10.1109/FOCS46700.2020.00109
  • D. Spielman, N. Srivastava, Graph Sparsification by Effective Resistances, SIAM J. Comput. 40(6), 2011. https://doi.org/10.1137/080734029
  • S. Arora, E. Hazan, S. Kale, The multiplicative weights update method: a meta-algorithm and applications, Theory of Computing 8, 2012. https://doi.org/10.4086/toc.2012.v008a006
  • D. Spielman, S.-H. Teng, Nearly linear time algorithms for preconditioning and solving symmetric, diagonally dominant linear systems, SIAM J. Matrix Anal. Appl. 35(3), 2014. https://doi.org/10.1137/090771430
29 thms3 active usersReviewed
AlgebraComplexity TheoryRandom Matrix Theory+1·Captain: iris

On the average-case complexity landscape for Tensor-Isomorphism-complete problems over finite fields: Algebra Isomorphism in Randomized poly(n, log q) Time on a 1/Θ(q) Fraction of AlgebrasResearch Paper

Motivation

Tensor Isomorphism (TI) asks whether two 3-way arrays over a field are related by invertible changes of basis along their three directions. A family of problems is polynomial-time equivalent to it: isomorphism of algebras given by structure constants, conjugacy of matrix codes, isomorphism of ppp-groups of class 2 and exponent ppp, and others (Grochow–Qiao, SIAM J. Comput. 2023). These TI-complete problems are the hardness assumptions of several post-quantum signature schemes (MEDS, ALTEQ), and cryptanalysis has shown that their practical difficulty differs from problem to problem despite the worst-case equivalence.

Over a finite field Fq\mathbb F_qFq​, every earlier rigorous average-case algorithm for these problems runs in time qO(n)q^{O(n)}qO(n) and succeeds on a 1−1/qΩ(n)1-1/q^{\Omega(n)}1−1/qΩ(n) fraction of inputs (Li–Qiao, FOCS 2017; Brooksbank–Li–Qiao–Wilson, ESA 2020; Grochow–Qiao–Tang, J. Groups Complex. Cryptol. 2022). Li, Li, Qiao, Tao and Wang (arXiv:2604.00591) trade success fraction for running time: algebra isomorphism becomes solvable in randomized time polynomial in nnn and log⁡q\log qlogq on a 1/Θ(q)1/\Theta(q)1/Θ(q) fraction of inputs. The analysis rests on new estimates for random matrices over finite fields, which the authors call their main technical contribution.

Setting

Fix a finite field Fq\mathbb F_qFq​ and let U=FqnU=\mathbb F_q^nU=Fqn​. An algebra on UUU is a bilinear multiplication gA:U×U→Ug_A:U\times U\to UgA​:U×U→U, given by its structure constants: a 3-way array A=(ai,j,k)∈T(n×n×n,q)A=(a_{i,j,k})\in T(n\times n\times n,q)A=(ai,j,k​)∈T(n×n×n,q) with gA(ei,ej)=∑kai,j,kekg_A(e_i,e_j)=\sum_k a_{i,j,k}e_kgA​(ei​,ej​)=∑k​ai,j,k​ek​. No associativity, commutativity or unit is assumed. Two algebras A,BA,BA,B are isomorphic when some invertible linear map φ\varphiφ of UUU satisfies φ(gA(x,y))=gB(φx,φy)\varphi(g_A(x,y))=g_B(\varphi x,\varphi y)φ(gA​(x,y))=gB​(φx,φy); equivalently B=(T⊗T⊗T−t)⋅AB=(T\otimes T\otimes T^{-t})\cdot AB=(T⊗T⊗T−t)⋅A for some T∈GL(n,q)T\in\mathrm{GL}(n,q)T∈GL(n,q).

A random algebra has independent uniform structure constants. The horizontal slices Ai=(ai,j,k)j,kA_i=(a_{i,j,k})_{j,k}Ai​=(ai,j,k​)j,k​ span a matrix code A≤M(n,q)\mathcal A\le\mathrm M(n,q)A≤M(n,q). With the trace form f(X,Y)=Tr(XY)f(X,Y)=\mathrm{Tr}(XY)f(X,Y)=Tr(XY), the orthogonal space is A⊥\mathcal A^\perpA⊥, the hull is H(A)=A∩A⊥H(\mathcal A)=\mathcal A\cap\mathcal A^\perpH(A)=A∩A⊥, a matrix is self-dual if Tr(X2)=0\mathrm{Tr}(X^2)=0Tr(X2)=0, and a self-dual line is a one-dimensional subspace L⊆L⊥L\subseteq L^\perpL⊆L⊥. With cn(q)=∏i=1n(1−q−i)c_n(q)=\prod_{i=1}^n(1-q^{-i})cn​(q)=∏i=1n​(1−q−i) and c(q)=lim⁡ncn(q)c(q)=\lim_n c_n(q)c(q)=limn​cn​(q), the limiting probabilities below are explicit functions of c(q)c(q)c(q).

Formalization targets

Goal: Theorem 1.1

There are a machine MMM, a degree kkk and an absolute c>0c>0c>0 such that MMM halts within (L+2)k(L+2)^k(L+2)k steps on every instance and every coin string (LLL the input length), and for every qqq, every presentation of Fq\mathbb F_qFq​ and every n≥N0(q)n\ge N_0(q)n≥N0​(q),

#{A∈T(n×n×n,q): ∀B, Pr⁡coins[M(A,B)=[A≅B]]≥2/3} ≥ cq qn3.\#\{A\in T(n\times n\times n,q):\ \forall B,\ \Pr_{\text{coins}}[M(A,B)=[A\cong B]]\ge 2/3\}\ \ge\ \frac{c}{q}\,q^{n^3}.#{A∈T(n×n×n,q): ∀B, coinsPr​[M(A,B)=[A≅B]]≥2/3} ≥ qc​qn3.

Milestones

The proof passes through, in order: the constants cn(q)c_n(q)cn​(q), c(q)c(q)c(q) (Propositions 2.1, 2.2); the Neumann–Praeger generating functions (Proposition 6.1); the self-dual probability σ(n,q)→1/q\sigma(n,q)\to1/qσ(n,q)→1/q (Theorem 6.5); eigenvalue-free matrices with prescribed Tr(A2)\mathrm{Tr}(A^2)Tr(A2) (Theorem 6.12); a unique simple eigenvalue for a self-dual matrix,

lim⁡n→∞Pr⁡[unique simple Fq-eigenvalue∣Tr(A2)=0]=q c(q)qq−1>e−23/9\lim_{n\to\infty}\Pr\bigl[\text{unique simple }\mathbb F_q\text{-eigenvalue}\mid\mathrm{Tr}(A^2)=0\bigr]=\frac{q\,c(q)^q}{q-1}>e^{-23/9}n→∞lim​Pr[unique simple Fq​-eigenvalue∣Tr(A2)=0]=q−1qc(q)q​>e−23/9

(Theorem 6.11) and its consequence for the hull (Theorem 3.5); hulls and conjugation (Lemma 3.2); the hull-one probability π1(q)+o(1)=Θ(1/q)\pi_1(q)+o(1)=\Theta(1/q)π1​(q)+o(1)=Θ(1/q) (Proposition 3.3) and the uniformity of the hull line (Proposition 3.4); generation of M(n,q)\mathrm M(n,q)M(n,q) by two random matrices (Theorem 2.3, Corollary 2.4); and the contraction step (Proposition 3.6), whose joint success probability is at least 1/31/31/3.

Significance

The result. Theorem 1.1 is the first average-case algorithm for a TI-complete problem whose running time is polynomial in log⁡q\log qlogq rather than in qnq^{n}qn, at the price of a success fraction 1/Θ(q)1/\Theta(q)1/Θ(q) instead of 1−q−Ω(n)1-q^{-\Omega(n)}1−q−Ω(n). For constant qqq it decides a constant fraction of instances in polynomial time. It separates the average-case behaviour of algebra isomorphism and matrix code conjugacy from that of 3-tensor isomorphism, for which no such algorithm is known, and it bears on the choice of parameters in TI-based cryptography. The random-matrix results of §6 (Theorems 6.5, 6.11, 6.12) are statements about matrices over finite fields with a trace condition and an eigenvalue condition, of independent use.

Formalizing it. The paper is a 2026 preprint; none of its results has a machine-checked proof. Mathlib has the order of GL(n,q)\mathrm{GL}(n,q)GL(n,q) (Matrix.card_GL_field), characteristic polynomials and root multiplicities, but nothing on hulls of matrix codes, on the Neumann–Praeger counts, or on generation of matrix algebras by random elements. Theorems 2.3 and 6.1 are cited results ([NP95], [NP98]); formalizing them is part of the mission.

Difficulty

An algorithm in time poly(n,log⁡q)\mathrm{poly}(n,\log q)poly(n,logq) cannot enumerate GL(n,q)\mathrm{GL}(n,q)GL(n,q) or even a field-sized set of candidates, so it needs canonical objects attached to the algebra that every isomorphism must respect. The slice code itself is not canonical enough: a random nnn-dimensional code in M(n,q)\mathrm M(n,q)M(n,q) has no structure that a polynomial-time procedure can normalise. The hull is canonical, but it is a single line only with probability Θ(1/q)\Theta(1/q)Θ(1/q), which is where the success fraction comes from.

The analytic difficulty is conditioning. The hull generator is a uniform self-dual matrix, not a uniform matrix, so the classical counts of matrices by eigenvalue multiplicities (Neumann–Praeger) do not apply directly: one needs the joint law of the spectrum over Fq\mathbb F_qFq​ and of Tr(A2)\mathrm{Tr}(A^2)Tr(A2), with explicit error terms (Theorems 6.11, 6.12). Proposition 3.6 has a second dependence problem: the contraction XXX is built from the same random slices that determine the hull, so it is not independent of the first canonical matrix.

Formalization scope

The goal is stated for Mathlib multi-stack Turing machines (Turing.TM2ComputableAux Bool Bool, run through HMBinPacking.OutputsWithin), with the field given as Fp[x]/(f)\mathbb F_p[x]/(f)Fp​[x]/(f) and all numbers in a self-delimiting binary code. Randomness is a coin string of length (L+2)k(L+2)^k(L+2)k appended to the input; the time bound holds for every coin string and every instance, and correctness is required against every second tensor BBB. The constant ccc is absolute and chosen before qqq; N0N_0N0​ depends on qqq. A statement that bounds the time only on good inputs, fixes qqq, or quantifies a single BBB would trivialize or weaken the theorem and is excluded.

Milestones are stated for every finite field KKK with q=∣K∣q=|K|q=∣K∣. Probabilities are ratios of counts (Nat.card), conditional probabilities ratios of counts over the conditioning set. c(q)c(q)c(q) and π1(q)\pi_1(q)π1​(q) are infima of their decreasing partial products, so no infinite product carries a junk value. "Eigenvalue in Fq\mathbb F_qFq​" means a root of the characteristic polynomial in KKK, with algebraic multiplicity. "Generate M(n,q)\mathrm M(n,q)M(n,q)" means the unital subalgebra. Every Θ\ThetaΘ and Ω\OmegaΩ has absolute constants.

Reusable infrastructure: hulls of matrix codes under the trace form, eigenvalue-free and unipotent proportions in GL(n,q)\mathrm{GL}(n,q)GL(n,q), the self-dual count, and the generation of M(n,q)\mathrm M(n,q)M(n,q) by two random matrices. Contributions are welcome on any milestone, and on the machine-level argument for the goal (polynomial-time linear algebra, polynomial factorization and matrix-tuple conjugacy over Fq\mathbb F_qFq​).

Selected references

  • T. Li, Y. Li, Y. Qiao, D. Tao, Y. Wang, On the average-case complexity landscape for Tensor-Isomorphism-complete problems over finite fields, preprint, 2026. https://arxiv.org/abs/2604.00591
  • P. M. Neumann, C. E. Praeger, Cyclic matrices over finite fields, J. London Math. Soc. 52(2), 1995. https://doi.org/10.1112/jlms/52.2.263
  • P. M. Neumann, C. E. Praeger, Derangements and eigenvalue-free elements in finite classical groups, J. London Math. Soc., 1998. https://doi.org/10.1112/S0024610798006772
  • O. Gorodetsky, B. Rodgers, Traces of powers of matrices over finite fields, Trans. Amer. Math. Soc. 374(7), 2021. https://doi.org/10.1090/tran/8337
  • J. A. Grochow, Y. Qiao, On the complexity of isomorphism problems for tensors, groups, and polynomials I: Tensor Isomorphism-completeness, SIAM J. Comput. 52, 2023. https://arxiv.org/abs/1907.00309
33 thms3 active usersReviewed
Quantum Information·Captain: iris

From Classical to Quantum Shannon Theory I: A Channel Is Entanglement-Breaking If and Only If It Has Unit-Rank Kraus OperatorsTextbook

Motivation

A quantum channel models every physical process a quantum system can undergo: noise in a fibre, a gate in a circuit, a measurement, a preparation. Some channels destroy every correlation of the input with the outside world that is not classical. These entanglement-breaking channels are the channels that can be simulated by measuring the input and preparing a fresh state from the outcome, so no quantum information survives them. They are central in quantum Shannon theory: the classical capacity of an entanglement-breaking channel is additive (Shor 2002), so its Holevo quantity is its capacity, and their quantum capacity is zero.

This mission is the first of a series formalizing Mark M. Wilde's textbook From Classical to Quantum Shannon Theory (arXiv:1106.1445v8). It covers the axiomatic description of quantum channels in §4.4 and the structure theorem for entanglement-breaking channels in §4.6.7.

Timeline. Kraus (1971, 1983) and Choi (1975) showed that completely positive maps between matrix algebras are exactly the maps X↦∑lVlXVl†X\mapsto\sum_l V_lXV_l^\daggerX↦∑l​Vl​XVl†​. Horodecki, Shor and Ruskai (2003) introduced entanglement-breaking channels in this generality and proved that they are exactly the channels with a Kraus representation by rank-one operators, equivalently the measure-and-prepare channels of Holevo's form (Holevo 1998).

Setting

All Hilbert spaces are finite dimensional. An operator on HA\mathcal H_AHA​ is a complex dA×dAd_A\times d_AdA​×dA​ matrix, and L(HA,HB)\mathcal L(\mathcal H_A,\mathcal H_B)L(HA​,HB​) is the space of dB×dAd_B\times d_AdB​×dA​ matrices. A density operator is a positive semidefinite matrix of trace one.

For a linear map N:L(HA)→L(HB)\mathcal N:\mathcal L(\mathcal H_A)\to\mathcal L(\mathcal H_B)N:L(HA​)→L(HB​) and a reference system RRR, the map idR⊗N\mathrm{id}_R\otimes\mathcal NidR​⊗N acts blockwise:

(idR⊗N)(∑i,j∣i⟩⟨j∣R⊗XAi,j)=∑i,j∣i⟩⟨j∣R⊗N(XAi,j).(\mathrm{id}_R\otimes\mathcal N)\Big(\sum_{i,j}|i\rangle\langle j|_R\otimes X^{i,j}_A\Big)=\sum_{i,j}|i\rangle\langle j|_R\otimes\mathcal N(X^{i,j}_A).(idR​⊗N)(i,j∑​∣i⟩⟨j∣R​⊗XAi,j​)=i,j∑​∣i⟩⟨j∣R​⊗N(XAi,j​).

The map N\mathcal NN is completely positive when idR⊗N\mathrm{id}_R\otimes\mathcal NidR​⊗N sends positive semidefinite operators to positive semidefinite operators for references RRR of every size, and trace preserving when Tr⁡{N(X)}=Tr⁡{X}\operatorname{Tr}\{\mathcal N(X)\}=\operatorname{Tr}\{X\}Tr{N(X)}=Tr{X} for every XXX. A quantum channel is a linear, completely positive, trace-preserving map. A Choi–Kraus decomposition of N\mathcal NN is a finite family {Vl}\{V_l\}{Vl​} in L(HA,HB)\mathcal L(\mathcal H_A,\mathcal H_B)L(HA​,HB​) with

N(X)=∑lVlXVl†,∑lVl†Vl=IA.\mathcal N(X)=\sum_l V_lXV_l^\dagger,\qquad \sum_l V_l^\dagger V_l=I_A .N(X)=l∑​Vl​XVl†​,l∑​Vl†​Vl​=IA​.

A state of RBRBRB is separable when it is a convex combination ∑xp(x) ∣ψx⟩⟨ψx∣R⊗∣ϕx⟩⟨ϕx∣B\sum_xp(x)\,|\psi_x\rangle\langle\psi_x|_R\otimes|\phi_x\rangle\langle\phi_x|_B∑x​p(x)∣ψx​⟩⟨ψx​∣R​⊗∣ϕx​⟩⟨ϕx​∣B​ of products of pure states. A channel N\mathcal NN is entanglement breaking when (idR⊗N)(ρRA)(\mathrm{id}_R\otimes\mathcal N)(\rho_{RA})(idR​⊗N)(ρRA​) is separable for every reference RRR and every state ρRA\rho_{RA}ρRA​. A POVM is a family {Λz}\{\Lambda^z\}{Λz} with Λz≥0\Lambda^z\ge0Λz≥0 and ∑zΛz=I\sum_z\Lambda^z=I∑z​Λz=I. The quantum–classical channel of a POVM is M(X)=∑zTr⁡{ΛzX}∣z⟩⟨z∣Z\mathcal M(X)=\sum_z\operatorname{Tr}\{\Lambda^zX\}|z\rangle\langle z|_ZM(X)=∑z​Tr{ΛzX}∣z⟩⟨z∣Z​, and the classical–quantum channel of states {σz}\{\sigma^z\}{σz} is P(Y)=∑z⟨z∣Y∣z⟩σz\mathcal P(Y)=\sum_z\langle z|Y|z\rangle\sigma^zP(Y)=∑z​⟨z∣Y∣z⟩σz.

Formalization targets

Goal: Theorem 4.6.1

For a quantum channel N\mathcal NN,

N is entanglement breaking  ⟺  N(X)=∑lVlXVl†,  ∑lVl†Vl=IA,  rank⁡Vl=1 for all l.\mathcal N\text{ is entanglement breaking}\iff \mathcal N(X)=\sum_lV_lXV_l^\dagger,\ \ \sum_lV_l^\dagger V_l=I_A,\ \ \operatorname{rank}V_l=1\ \text{for all }l .N is entanglement breaking⟺N(X)=l∑​Vl​XVl†​,  l∑​Vl†​Vl​=IA​,  rankVl​=1 for all l.

Theorem 4.4.1 (Choi–Kraus)

A linear map is completely positive and trace preserving if and only if it has a Choi–Kraus decomposition, and every channel has one with at most dAdBd_Ad_BdA​dB​ Kraus operators.

Proposition 4.4.1

The adjoint N†\mathcal N^\daggerN† of a channel, defined by Tr⁡{Y†N(X)}=Tr⁡{N†(Y)†X}\operatorname{Tr}\{Y^\dagger\mathcal N(X)\}=\operatorname{Tr}\{\mathcal N^\dagger(Y)^\dagger X\}Tr{Y†N(X)}=Tr{N†(Y)†X}, is completely positive and unital: N†(IB)=IA\mathcal N^\dagger(I_B)=I_AN†(IB​)=IA​.

Corollary 4.6.1

Every entanglement-breaking channel factors as

N=PZ→B∘MA→Z\mathcal N=\mathcal P_{Z\to B}\circ\mathcal M_{A\to Z}N=PZ→B​∘MA→Z​

for some finite classical system ZZZ, a POVM defining M\mathcal MM and density operators defining P\mathcal PP.

Significance

The Choi–Kraus theorem is the bridge between the axioms of quantum evolution and the formula used in every computation; later chapters of the book use the Kraus form of a channel on almost every page, and a formal version of it lets statements be posed on the axiomatic definition and proved with Kraus operators. Proposition 4.4.1 is the passage from the Schrödinger to the Heisenberg picture. Theorem 4.6.1 replaces a condition over all reference systems and all input states by a condition on one Kraus representation; Corollary 4.6.1 is the measure-and-prepare form on which the additivity of the Holevo capacity of entanglement-breaking channels rests (Theorem 13.3.1 of the book).

All four results are classical in the literature. The platform already has the direction "completely positive implies a Kraus form" for maps given as functions (PeresTerno.completelyPositive_exists_kraus, OCB2012.exists_kraus_of_cj_posSemidef), and an Open item for the Horodecki–Shor–Ruskai equivalences on maps from MdM_dMd​ to MdM_dMd​ (QAlgorithms.Papers.Independent.Independent1.P02.entanglementBreaking_equivalences). None of these has the iff with trace preservation and the bound d≤dAdBd\le d_Ad_Bd≤dA​dB​, or the unit-rank characterization for channels between spaces of different dimension. The mission produces these in the book's own definitions.

Difficulty

The direction "unit-rank Kraus operators imply entanglement breaking" is a computation. The converse is the substance: from the separability of a single output, the Choi state (id⊗N)(ΦRA)(\mathrm{id}\otimes\mathcal N)(\Phi_{RA})(id⊗N)(ΦRA​), one must build Kraus operators. This needs the Choi correspondence between a linear map and its Choi operator (which determines the map), a decomposition of a separable state into pure product states, the identification of the reference marginal with the maximally mixed state, and the transpose trick that turns a reference vector ∣φ⟩R|\varphi\rangle_R∣φ⟩R​ into an input functional ⟨φ∗∣A\langle\varphi^*|_A⟨φ∗∣A​. The Choi–Kraus theorem itself needs the spectral decomposition of the Choi operator and a dimension count. The naive approach of decomposing (idR⊗N)(ρRA)(\mathrm{id}_R\otimes\mathcal N)(\rho_{RA})(idR​⊗N)(ρRA​) for each input separately gives no single Kraus family; the whole point is that one input, the maximally entangled state, suffices.

Formalization scope

Operators are complex matrices indexed by finite types; a map is a C\mathbb CC-linear map Matrix a a ℂ →ₗ[ℂ] Matrix b b ℂ. The reference system is the first tensor factor and ranges over Cr\mathbb C^rCr for every rrr; idR⊗N\mathrm{id}_R\otimes\mathcal NidR​⊗N is the published QAlgorithms.idTensorSuperop and complete positivity the published QAlgorithms.Entanglement.IsCompletelyPositive. Separable states and density operators are the published WildeQIT.IsSeparable and WildeQIT.IsDensityOperator. Entanglement breaking is the operational Definition 4.6.8, never the Kraus condition, so Theorem 4.6.1 is not true by definition; likewise a channel is defined by complete positivity and trace preservation, not by a Kraus form, so Theorem 4.4.1 has two real directions. Unit rank means rank exactly one: a zero Kraus operator does not count. The adjoint is any linear map satisfying the defining equations, which determine it uniquely.

Useful infrastructure, reusable beyond this mission: the Choi operator and the fact that it determines a linear map, Choi's criterion for complete positivity, and the pure-state decomposition of separable states. Contributions of these lemmas, of the transpose identity ∑i,j∣i⟩⟨j∣X∣i⟩⟨j∣=XT\sum_{i,j}|i\rangle\langle j|X|i\rangle\langle j|=X^T∑i,j​∣i⟩⟨j∣X∣i⟩⟨j∣=XT, and of proofs of the milestones are welcome.

Selected references

  • M. M. Wilde, From Classical to Quantum Shannon Theory, arXiv:1106.1445v8, 2019 (§4.4, §4.6.7). https://arxiv.org/abs/1106.1445
  • M.-D. Choi, Completely positive linear maps on complex matrices, Linear Algebra Appl. 10 (1975) 285–290. https://doi.org/10.1016/0024-3795(75)90075-0
  • M. Horodecki, P. W. Shor, M. B. Ruskai, Entanglement breaking channels, Rev. Math. Phys. 15 (2003) 629–641. https://arxiv.org/abs/quant-ph/0302031
  • P. W. Shor, Additivity of the classical capacity of entanglement-breaking quantum channels, J. Math. Phys. 43 (2002) 4334–4340. https://arxiv.org/abs/quant-ph/0201149
  • A. S. Holevo, Coding theorems for quantum channels, Tamagawa Univ. Research Review 4 (1998). https://arxiv.org/abs/quant-ph/9809023
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Information TheoryQuantum Information·Captain: iris

A Condition for the Nullity of Quantum Discord: Discord Vanishes If and Only If the State Is Block-Diagonal in an Eigenbasis of the Marginal of BResearch Paper

Why zero discord matters

Quantum discord was introduced by Ollivier and Zurek (quant-ph/0105072) and by Henderson and Vedral (quant-ph/0105028) as the part of the correlations of a bipartite quantum state that no local measurement can reveal. It is nonzero for some unentangled states, and it has been proposed as a resource behind mixed-state quantum computation with little entanglement. The states of zero discord are the ones whose correlations are entirely accessible to a measurement on one side; Ollivier and Zurek identified them with the pointer states of decoherence theory.

A. Datta (arXiv:1003.5256v2) gives a short proof that discord is nonnegative from strong subadditivity of the von Neumann entropy, and uses the equality case of strong subadditivity, characterized by Hayden, Jozsa, Petz and Winter (quant-ph/0304007), to characterize the states of zero discord. This mission formalizes that paper.

Setting

Let AAA and BBB be finite-dimensional quantum systems with Hilbert spaces HA\mathcal H_AHA​, HB\mathcal H_BHB​, and let ρAB\rho_{AB}ρAB​ be a density matrix on HA⊗HB\mathcal H_A\otimes\mathcal H_BHA​⊗HB​: positive semidefinite with trace one. Its marginals are ρA=TrBρAB\rho_A=\mathrm{Tr}_B\rho_{AB}ρA​=TrB​ρAB​ and ρB=TrAρAB\rho_B=\mathrm{Tr}_A\rho_{AB}ρB​=TrA​ρAB​. The von Neumann entropy is H(σ)=−Tr(σlog⁡2σ)H(\sigma)=-\mathrm{Tr}(\sigma\log_2\sigma)H(σ)=−Tr(σlog2​σ), in bits.

A POVM on BBB is a finite family of positive semidefinite operators {Πi}\{\Pi_i\}{Πi​} with ∑iΠi=I\sum_i\Pi_i=I∑i​Πi​=I; it is rank one if every Πi\Pi_iΠi​ has rank one. Measuring BBB with {Πi}\{\Pi_i\}{Πi​} gives outcome iii with probability pi=Tr((IA⊗Πi)ρAB)p_i=\mathrm{Tr}\big((I_A\otimes\Pi_i)\rho_{AB}\big)pi​=Tr((IA​⊗Πi​)ρAB​) and leaves AAA in the state ρA∣i=TrB((IA⊗Πi)ρAB)/pi\rho_{A|i}=\mathrm{Tr}_B\big((I_A\otimes\Pi_i)\rho_{AB}\big)/p_iρA∣i​=TrB​((IA​⊗Πi​)ρAB​)/pi​ (Eq. (1)). The measured conditional entropy is H~{Πi}(A∣B)=∑ipiH(ρA∣i)\tilde H_{\{\Pi_i\}}(A|B)=\sum_i p_iH(\rho_{A|i})H~{Πi​}​(A∣B)=∑i​pi​H(ρA∣i​).

With the mutual information I(A:B)=H(ρA)+H(ρB)−H(ρAB)I(A:B)=H(\rho_A)+H(\rho_B)-H(\rho_{AB})I(A:B)=H(ρA​)+H(ρB​)−H(ρAB​) and the classical correlation J(A:B)=H(ρA)−min⁡{Πi}H~{Πi}(A∣B)\mathcal J(A:B)=H(\rho_A)-\min_{\{\Pi_i\}}\tilde H_{\{\Pi_i\}}(A|B)J(A:B)=H(ρA​)−min{Πi​}​H~{Πi​}​(A∣B), the minimum over rank-one POVMs on BBB, the discord is (Eq. (2))

D(A:B)=I(A:B)−J(A:B)=H(ρB)−H(ρAB)+min⁡{Πi}H~{Πi}(A∣B).\mathcal D(A:B)=I(A:B)-\mathcal J(A:B)=H(\rho_B)-H(\rho_{AB})+\min_{\{\Pi_i\}}\tilde H_{\{\Pi_i\}}(A|B).D(A:B)=I(A:B)−J(A:B)=H(ρB​)−H(ρAB​)+{Πi​}min​H~{Πi​}​(A∣B).

In Lean these are DattaDiscord.measuredCondEntropy, minCondEntropy, mutualInfo, classicalCorr and discord, built on the published QAlgorithms.IsDensityMatrix, vnEntropy, IsPOVM, pureDensity, traceLeft (TrA\mathrm{Tr}_ATrA​) and traceRight (TrB\mathrm{Tr}_BTrB​).

Formalization targets

Goal: Theorem 2

For every density matrix ρAB\rho_{AB}ρAB​,

D(A:B)=0  ⟺  ∃ orthonormal basis {∣ej⟩} of HB, probability vector {τj}:ρB=∑jτj∣ej⟩⟨ej∣,ρAB=∑jPjρABPj,\mathcal D(A:B)=0\iff\exists\ \text{orthonormal basis }\{|e_j\rangle\}\text{ of }\mathcal H_B,\ \text{probability vector }\{\tau_j\}:\quad \rho_B=\sum_j\tau_j|e_j\rangle\langle e_j|,\quad \rho_{AB}=\sum_jP_j\rho_{AB}P_j,D(A:B)=0⟺∃ orthonormal basis {∣ej​⟩} of HB​, probability vector {τj​}:ρB​=j∑​τj​∣ej​⟩⟨ej​∣,ρAB​=j∑​Pj​ρAB​Pj​,

with Pj=IA⊗∣ej⟩⟨ej∣P_j=I_A\otimes|e_j\rangle\langle e_j|Pj​=IA​⊗∣ej​⟩⟨ej​∣: zero discord is block-diagonality in an eigenbasis of ρB\rho_BρB​.

Milestones

  1. Attainment (p.1): the minimum in Eq. (2) exists and is attained at an extreme point of the set of POVMs that is rank one, even against all finite POVMs.
  2. Eqs. (3)–(4c): the dilated state ρABC′=∑j,k⟨ej∣ρAB∣ek⟩⊗∣ej⟩⟨ek∣⊗∣fj⟩⟨fk∣\rho'_{ABC}=\sum_{j,k}\langle e_j|\rho_{AB}|e_k\rangle\otimes|e_j\rangle\langle e_k|\otimes|f_j\rangle\langle f_k|ρABC′​=∑j,k​⟨ej​∣ρAB​∣ek​⟩⊗∣ej​⟩⟨ek​∣⊗∣fj​⟩⟨fk​∣ and its marginals, including ρAB′=∑jpjρA∣j⊗∣ej⟩⟨ej∣=∑jPjρABPj\rho'_{AB}=\sum_jp_j\rho_{A|j}\otimes|e_j\rangle\langle e_j|=\sum_jP_j\rho_{AB}P_jρAB′​=∑j​pj​ρA∣j​⊗∣ej​⟩⟨ej​∣=∑j​Pj​ρAB​Pj​.
  3. Entropy identities: H(ρABC′)=H(ρAB)H(\rho'_{ABC})=H(\rho_{AB})H(ρABC′​)=H(ρAB​), H(ρAB′)=H(p)+∑jpjH(ρA∣j)H(\rho'_{AB})=H(\mathbf p)+\sum_jp_jH(\rho_{A|j})H(ρAB′​)=H(p)+∑j​pj​H(ρA∣j​), H(ρBC′)=H(ρB)H(\rho'_{BC})=H(\rho_B)H(ρBC′​)=H(ρB​), H(ρB′)=H(p)H(\rho'_B)=H(\mathbf p)H(ρB′​)=H(p).
  4. Eq. (5), strong subadditivity: the proved platform theorem QAlgorithms.Papers.Independent.Gap48.P20.strongSubadditivity.
  5. Eq. (6): H~{Πi}(A∣B)≥H(ρAB)−H(ρB)\tilde H_{\{\Pi_i\}}(A|B)\ge H(\rho_{AB})-H(\rho_B)H~{Πi​}​(A∣B)≥H(ρAB​)−H(ρB​) for every rank-one POVM.
  6. Theorem 1: D(A:B)≥0\mathcal D(A:B)\ge0D(A:B)≥0.
  7. Eq. (8): D(A:B)=0\mathcal D(A:B)=0D(A:B)=0 iff ρAB=∑jpjσj⊗∣λj⟩⟨λj∣\rho_{AB}=\sum_jp_j\sigma_j\otimes|\lambda_j\rangle\langle\lambda_j|ρAB​=∑j​pj​σj​⊗∣λj​⟩⟨λj​∣ for states σj\sigma_jσj​ and an orthonormal eigenbasis {∣λj⟩}\{|\lambda_j\rangle\}{∣λj​⟩} of ρB\rho_BρB​.

The paper's Lemma 1, the Hayden–Jozsa–Petz–Winter structure of states saturating strong subadditivity, is already posed on the platform as the open goal QAlgorithms.Papers.Independent.Renew46.P35.ssaEquality_iff_blocks; it is not posed again here.

Significance

Theorem 2 gives a checkable criterion for zero discord: diagonalize ρB\rho_BρB​ and test block-diagonality, instead of optimizing over all measurements. It identifies the zero-discord states with the classical–quantum states, the states that a measurement of BBB leaves undisturbed, which is the form in which zero discord enters later work on completely positive dynamics, quantum-to-classical transitions and discord-based resource theories. Theorem 1, the nonnegativity of discord, is the basic sanity property of the quantity.

Both results are proved in the literature: Theorem 1 is due to Ollivier and Zurek, and the characterization of zero discord appears in Ollivier–Zurek and, in the form used here, in Datta's paper. Neither, to the knowledge of this mission, has a machine-checked proof. On the platform, strong subadditivity in finite dimensions is proved; a Rényi discord, an infinite-dimensional one-directional variant of the zero-discord condition, and the strong-subadditivity equality structure are posed as open goals in other missions, with different definitions. This mission adds the standard (von Neumann, rank-one POVM, measured system BBB) discord and its two main theorems.

Difficulty

The obvious route to the forward direction is to take a minimizing measurement and read off the structure of ρAB\rho_{AB}ρAB​ from the equality H~{Πi}(A∣B)=H(ρAB)−H(ρB)\tilde H_{\{\Pi_i\}}(A|B)=H(\rho_{AB})-H(\rho_B)H~{Πi​}​(A∣B)=H(ρAB​)−H(ρB​). For a basis measurement this equality is equality in strong subadditivity for the dilated state, and the conclusion needs the full equality case of strong subadditivity, a substantial structure theorem in its own right. Two further points block a direct argument. First, the minimizer must exist, which requires a compactness argument over POVMs with a bounded number of outcomes and a reduction from general to rank-one POVMs. Second, a rank-one POVM need not be a basis measurement, so Eq. (6) for general rank-one POVMs needs a Naimark dilation, and the equality case must be transported through it. The reverse direction is a computation with the entropy identities but still requires the entropy of block-diagonal and isometrically embedded states.

Formalization scope

Systems are finite index types A, B (with Fintype and DecidableEq), operators are Matrix (A × B) (A × B) ℂ with A the first factor, and PjP_jPj​ is Matrix.kronecker 1 (pureDensity (e j)) for e : OrthonormalBasis B ℂ (EuclideanSpace ℂ B). Entropies are in bits. POVMs have outcome set Fin n for arbitrary n. The minimum in the discord is written as the infimum sInf of the explicit set of values over rank-one POVMs; that set is nonempty and bounded below by 000, so the infimum is not a junk value, and nested ⨅ with a POVM-condition binder, which would collapse to 000 in ℝ, is not used. Outcomes of probability zero contribute 000 to H~\tilde HH~. The discord follows the first line of Eq. (2); the printed second line has a sign slip. The block-diagonal condition alone does not suffice (the Bell state is block-diagonal for the single spectral projector of ρB=I/2\rho_B=I/2ρB​=I/2 yet has discord one), so the goal keeps the rank-one eigenbasis clause, and the basis is existential (not every eigenbasis works when ρB\rho_BρB​ is degenerate).

A complete development needs: the spectral calculus of vnEntropy (unitary invariance, entropy of block-diagonal and isometrically embedded states), strong subadditivity in this vocabulary, its equality case, compactness of bounded POVMs, and Naimark dilation. The equality case of strong subadditivity and Naimark dilation are reusable beyond this mission; contributions to either are welcome, as are proofs of the converse direction alone.

Selected references

  • A. Datta, A Condition for the Nullity of Quantum Discord, arXiv:1003.5256v2, 2011. https://arxiv.org/abs/1003.5256
  • H. Ollivier, W. H. Zurek, Quantum Discord: A Measure of the Quantumness of Correlations, Phys. Rev. Lett. 88, 017901, 2001. https://arxiv.org/abs/quant-ph/0105072
  • L. Henderson, V. Vedral, Classical, quantum and total correlations, J. Phys. A 34, 6899, 2001. https://arxiv.org/abs/quant-ph/0105028
  • P. Hayden, R. Jozsa, D. Petz, A. Winter, Structure of states which satisfy strong subadditivity of quantum entropy with equality, Commun. Math. Phys. 246, 359–374, 2004. https://arxiv.org/abs/quant-ph/0304007
  • E. H. Lieb, M. B. Ruskai, Proof of the strong subadditivity of quantum-mechanical entropy, J. Math. Phys. 14, 1938, 1973. https://doi.org/10.1063/1.1666274
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Operations ResearchOptimization·Captain: iris

Best Principal Submatrix Selection for the Maximum Entropy Sampling Problem: relaxation-based sampling is within slog⁡s+log⁡(ns)−slog⁡n+αs\log s+\log\binom{n}{s}-s\log n+\alphaslogs+log(sn​)−slogn+α of the optimumResearch Paper

Motivation

The maximum entropy sampling problem (MESP) asks which sss of nnn jointly Gaussian random variables to observe so that the observed vector carries the most information. For a Gaussian vector the differential entropy of a sub-vector is, up to constants, the logarithm of the determinant of its covariance matrix, so the question is to choose the size-sss principal submatrix of the covariance matrix with the largest log-determinant. The problem was introduced by Shewry and Wynn (1987) for the design of monitoring networks and has since been used for sensor placement, environmental monitoring, and feature selection. It is NP-hard (Ko, Lee and Queyranne 1995), so practical methods rely on relaxations that give upper bounds, and on rounding schemes that turn a relaxed solution into a subset with a provable guarantee.

Timeline of the guarantees relevant here:

  • Nikolov (2015) introduced the concave function Γs\Gamma_sΓs​ and a relaxation based on it, and showed that randomized rounding of an optimal solution loses at most log⁡(ss/s!)≈s\log(s^s/s!)\approx slog(ss/s!)≈s in the log-determinant objective (STOC 2015, pp. 861–870).
  • Li and Xie (2020–2024) derived the same objective as the primal characterization of a Lagrangian dual of MESP, and proved for a different sampling law the bound slog⁡s+log⁡(ns)−slog⁡ns\log s+\log\binom ns-s\log nslogs+log(sn​)−slogn, plus the accuracy α\alphaα of an approximately optimal relaxed solution (arXiv:2001.08537; Operations Research, 2024). Their bound is never worse than Nikolov's and is much smaller when sss is close to nnn.

Setting

Let C∈Rn×nC\in\mathbb R^{n\times n}C∈Rn×n be positive semidefinite of rank ddd, written as C=V⊤VC=V^\top VC=V⊤V with V∈Rd×nV\in\mathbb R^{d\times n}V∈Rd×n, and let vi∈Rdv_i\in\mathbb R^dvi​∈Rd be the iii-th column of VVV. Fix an integer sss with 1≤s≤d≤n1\le s\le d\le n1≤s≤d≤n. Logarithms are natural, with log⁡0=−∞\log 0=-\inftylog0=−∞.

  • For a symmetric X⪰0X\succeq0X⪰0 with eigenvalues λ1≥⋯≥λd≥0\lambda_1\ge\cdots\ge\lambda_d\ge0λ1​≥⋯≥λd​≥0, det⁡s(X)=∏i≤sλi\det^s(X)=\prod_{i\le s}\lambda_idets(X)=∏i≤s​λi​ is the product of the sss largest eigenvalues and det⁡s(X)\det_s(X)dets​(X) the product of the sss smallest (Definition 1).
  • The MESP value is z∗=max⁡{log⁡det⁡(CS,S):S⊆[n], ∣S∣=s}z^*=\max\{\log\det(C_{S,S}) : S\subseteq[n],\ |S|=s\}z∗=max{logdet(CS,S​):S⊆[n], ∣S∣=s}. Since det⁡(CS,S)=det⁡s(∑i∈Svivi⊤)\det(C_{S,S})=\det^s(\sum_{i\in S}v_iv_i^\top)det(CS,S​)=dets(∑i∈S​vi​vi⊤​) (Observation 1), MESP selects sss columns of VVV.
  • For X⪰0X\succeq0X⪰0 let kkk be the unique integer 0≤k<s0\le k<s0≤k<s with λk>1s−k∑i>kλi≥λk+1\lambda_k>\frac1{s-k}\sum_{i>k}\lambda_i\ge\lambda_{k+1}λk​>s−k1​∑i>k​λi​≥λk+1​ (Lemma 2, λ0=∞\lambda_0=\inftyλ0​=∞), and set
Γs(X)=log⁡∏i≤kλi+(s−k)log⁡(1s−k∑i>kλi).\Gamma_s(X)=\log\prod_{i\le k}\lambda_i+(s-k)\log\Bigl(\frac1{s-k}\sum_{i>k}\lambda_i\Bigr).Γs​(X)=logi≤k∏​λi​+(s−k)log(s−k1​i>k∑​λi​).
  • The relaxation PC (9) maximizes Γs(∑ixivivi⊤)\Gamma_s(\sum_ix_iv_iv_i^\top)Γs​(∑i​xi​vi​vi⊤​) over D={x∈[0,1]n:∑ixi=s}D=\{x\in[0,1]^n:\sum_ix_i=s\}D={x∈[0,1]n:∑i​xi​=s}; its value zLDz^{LD}zLD equals the value of the Lagrangian dual LD (5) (Theorems 1 and 2), and zLD≥z∗z^{LD}\ge z^*zLD≥z∗.
  • A point x^∈D\hat x\in Dx^∈D is α-optimal if Γs(∑ix^ivivi⊤)≥zLD−α\Gamma_s(\sum_i\hat x_iv_iv_i^\top)\ge z^{LD}-\alphaΓs​(∑i​x^i​vi​vi⊤​)≥zLD−α.
  • The sampling law (13) draws a size-sss subset S~\tilde SS~ with probability proportional to ∏i∈S~x^i\prod_{i\in\tilde S}\hat x_i∏i∈S~​x^i​; the normalizer is the elementary symmetric polynomial Es(x^)E_s(\hat x)Es​(x^).

Formalization targets

Goal: Theorem 5

For every α>0\alpha>0α>0 and every α-optimal x^\hat xx^,

log⁡E[det⁡s(∑i∈S~vivi⊤)] ≥ z∗−slog⁡s−log⁡(ns)+slog⁡n−α.\log\mathbb E\Bigl[{\det}^s\Bigl(\sum_{i\in\tilde S}v_iv_i^\top\Bigr)\Bigr]\ \ge\ z^*-s\log s-\log\binom ns+s\log n-\alpha .logE[dets(i∈S~∑​vi​vi⊤​)] ≥ z∗−slogs−log(sn​)+slogn−α.

The statement is uniform in VVV of rank ddd, in s∈[d]s\in[d]s∈[d], in α>0\alpha>0α>0, and in the α-optimal point.

Milestones

  1. Observation 1: det⁡(CS,S)=det⁡s(∑i∈Svivi⊤)\det(C_{S,S})=\det^s(\sum_{i\in S}v_iv_i^\top)det(CS,S​)=dets(∑i∈S​vi​vi⊤​) for ∣S∣=s|S|=s∣S∣=s.
  2. Lemma 11: sorted vectors solve two majorization-constrained linear programs.
  3. Lemma 1: max⁡X⪰0{log⁡det⁡s(X)−tr⁡(XΛ)}=−log⁡det⁡s(Λ)−s\max_{X\succeq0}\{\log\det^s(X)-\operatorname{tr}(X\Lambda)\}=-\log\det_s(\Lambda)-smaxX⪰0​{logdets(X)−tr(XΛ)}=−logdets​(Λ)−s for Λ≻0\Lambda\succ0Λ≻0.
  4. Theorem 1: LD (5) is the Lagrangian dual of MESP, and zLD≥z∗z^{LD}\ge z^*zLD≥z∗.
  5. Lemma 2 (with nonnegative λ\lambdaλ): the index kkk exists and is unique.
  6. Lemma 3: the conjugate identities (7) and (8), ending in Γs(X)+s\Gamma_s(X)+sΓs​(X)+s.
  7. Theorem 2: LD (5) equals PC (9), and (9) is attained.
  8. Lemma 5: ∑∣S∣=s∏i∈Sx^idet⁡s(VSVS⊤)≥exp⁡Γs(∑ix^ivivi⊤)\sum_{|S|=s}\prod_{i\in S}\hat x_i\det^s(V_SV_S^\top)\ge\exp\Gamma_s(\sum_i\hat x_iv_iv_i^\top)∑∣S∣=s​∏i∈S​x^i​dets(VS​VS⊤​)≥expΓs​(∑i​x^i​vi​vi⊤​).
  9. Maclaurin step: Es(x^)≤(s/n)s(ns)E_s(\hat x)\le(s/n)^s\binom nsEs​(x^)≤(s/n)s(sn​) on DDD.

Significance

The bound is additive in the log-determinant, so it says that the expected determinant of the sampled submatrix is within the multiplicative factor (s/n)s(ns) eα(s/n)^s\binom ns\,e^{\alpha}(s/n)s(sn​)eα of the optimal determinant. Because (s/n)s(ns)≤ss/s!(s/n)^s\binom ns\le s^s/s!(s/n)s(sn​)≤ss/s!, it improves Nikolov's guarantee, and the factor (s/n)s(ns)(s/n)^s\binom ns(s/n)s(sn​) equals 111 at s=ns=ns=n. The same proof gives the relaxation gap zLD≤z∗+slog⁡s+log⁡(ns)−slog⁡nz^{LD}\le z^*+s\log s+\log\binom ns-s\log nzLD≤z∗+slogs+log(sn​)−slogn (Corollary 1), and the paper derandomizes the sampler with the same guarantee (Theorem 6).

The result is proved in the paper; no machine-checked proof of it, of Nikolov's relaxation, or of the Lagrangian duality for MESP exists on the platform or in Mathlib. The mission produces a formal statement of the whole chain from the dual to the sampling bound. Formalizing it requires a library for spectral functions of symmetric matrices (products of extreme eigenvalues, their conjugates), Maclaurin's inequality for elementary symmetric polynomials, and Nikolov's inequality behind Lemma 5, which the paper cites without proof.

Difficulty

Lemma 5 is the hard step. The paper does not prove it and defers to theorem 18 of Nikolov (2015). The obvious attempt, comparing det⁡s\det^sdets of the weighted sum with the weighted sum of det⁡s\det^sdets term by term, fails: det⁡s\det^sdets is neither linear nor multiplicative in the summands, and Γs\Gamma_sΓs​ is a different function of the spectrum from log⁡det⁡s\log\det^slogdets whenever the rank exceeds sss. The duality results (Lemmas 1 and 3, Theorems 1 and 2) are convex analysis over symmetric matrices, but they hinge on eigenvalue–diagonal majorization (Schur–Horn type inequalities, Lemma 11) and on an explicit KKT analysis that pins down the index kkk; a naive argument that treats Λ\LambdaΛ as diagonal does not justify the reduction. Theorem 2 also needs a strong-duality theorem with attainment for a non-smooth concave objective.

Formalization scope

  • Matrices are Matrix (Fin d) (Fin n) ℝ; the hypothesis C⪰0C\succeq0C⪰0 of rank ddd is V.rank = d (which implies d≤nd\le nd≤n), and 1≤s≤d1\le s\le d1≤s≤d.
  • Eigenvalues are Mathlib's IsHermitian.eigenvalues₀, sorted decreasingly and reindexed by Fin d (0-based).
  • All logarithmic quantities (log⁡det⁡\log\detlogdet, log⁡det⁡s\log\det^slogdets, Γs\Gamma_sΓs​, z∗z^*z∗, zLDz^{LD}zLD, the left side of the goal) are EReal via ENNReal.log ∘ ENNReal.ofReal, so log⁡0=−∞\log 0=-\inftylog0=−∞ as in the paper. A Real.log encoding would make Lemma 1 false and would let a rank-deficient point pass as α-optimal through a junk value.
  • LD (5) is an infimum over Λ≻0\Lambda\succ0Λ≻0, ν≥0\nu\ge0ν≥0, μ≥0\mu\ge0μ≥0; PC (9) is a supremum over DDD, and α-optimality is measured against PC (9), as on p.11.
  • The random set of Algorithm 2 is the random set with law (13); its expectation is the finite sum over size-sss subsets.
  • The index kkk is defined by both inequalities of Lemma 2, not by a maximization. Lemma 2 is stated for nonnegative vectors, which corrects the printed version (false for λ=(−1,−2)\lambda=(-1,-2)λ=(−1,−2), s=1s=1s=1).
  • Reused: gram, weightedGram, xPow from the published PropVolSampling.Reduction definitions.

Contributions welcome: proofs of the milestones, a general Maclaurin inequality, spectral majorization lemmas, and a formal proof of Nikolov's inequality (Lemma 5).

Selected references

  • Y. Li, W. Xie, Best Principal Submatrix Selection for the Maximum Entropy Sampling Problem: Scalable Algorithms and Performance Guarantees, arXiv:2001.08537v3, 2023; Operations Research, 2024. https://arxiv.org/abs/2001.08537
  • A. Nikolov, Randomized Rounding for the Largest Simplex Problem, Proceedings of the 47th Annual ACM Symposium on Theory of Computing (STOC), 2015, pp. 861–870.
  • M. C. Shewry, H. P. Wynn, Maximum entropy sampling, Journal of Applied Statistics 14(2):165–170, 1987. https://doi.org/10.1080/02664768700000020
  • C.-W. Ko, J. Lee, M. Queyranne, An exact algorithm for maximum entropy sampling, Operations Research 43(4), 1995. https://doi.org/10.1287/opre.43.4.684
  • M. Lin, N. S. Trudinger, On some inequalities for elementary symmetric functions, Bulletin of the Australian Mathematical Society 50(2):317–326, 1994.
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Quantum Information·Captain: iris

Oblivious remote state preparation: a faithful forward-only RSP protocol for a generic ensemble that is oblivious to Bob can be made oblivious to Alice with the same message distributionResearch Paper

Motivation

Teleportation (Bennett et al. 1993) sends an unknown state of a ddd-dimensional system using one maximally entangled pair and 2log⁡d2\log d2logd bits of classical communication, and both resources are necessary. Remote state preparation (RSP) is the same task when the sender, Alice, knows the state she wants the receiver, Bob, to hold. Lo (PRA 62, 012313, 2000) asked whether this knowledge can save classical communication and conjectured that, in general, 2log⁡d2\log d2logd bits are still needed. Holevo's bound only gives log⁡d\log dlogd bits, and Bennett et al. (2001) found probabilistic RSP protocols whose expected cost approaches log⁡d\log dlogd, so the conjecture can only hold under extra conditions.

Leung and Shor (arXiv:quant-ph/0201008) identify such conditions. Timeline:

  • 1993: teleportation, 2log⁡d2\log d2logd cbits and one ebit, necessary and sufficient.
  • 2000: Lo introduces RSP and conjectures that 2log⁡d2\log d2logd cbits are necessary.
  • 2001: Bennett, DiVincenzo, Shor, Smolin, Terhal and Wootters give RSP protocols with expected cost near log⁡d\log dlogd and suggest the conjecture may hold for protocols that leak nothing extra to Bob.
  • 2002: Leung and Shor prove that a faithful RSP protocol for a generic ensemble that is oblivious to Bob can be converted into one that needs only a specimen of the state, at the same classical cost, which gives Lo's conjecture under these conditions.

Setting

The input space is Cd\mathbb C^dCd, with basis indexed by a finite set ι\iotaι. A pure state is φ=∣ψ⟩⟨ψ∣\varphi = |\psi\rangle\langle\psi|φ=∣ψ⟩⟨ψ∣ for a unit vector ψ\psiψ. A set SSS of unit vectors is a generic ensemble when the projectors ∣ψ⟩⟨ψ∣|\psi\rangle\langle\psi|∣ψ⟩⟨ψ∣, ψ∈S\psi\in Sψ∈S, span all d×dd\times dd×d complex matrices (the paper asks for a basis).

Alice and Bob share the maximally entangled state ∣Φd′⟩=d′−1/2∑j∣j⟩∣j⟩|\Phi_{d'}\rangle = d'^{-1/2}\sum_j |j\rangle|j\rangle∣Φd′​⟩=d′−1/2∑j​∣j⟩∣j⟩ on Cd′⊗Cd′\mathbb C^{d'}\otimes\mathbb C^{d'}Cd′⊗Cd′ (index set σ\sigmaσ; d′d'd′ need not equal ddd). Knowing ψ\psiψ, Alice applies a POVM {Eψ,m}m∈M\{E_{\psi,m}\}_{m\in M}{Eψ,m​}m∈M​ to her half and sends the outcome mmm to Bob. Bob's half is then left in the unnormalized state

pmρφm=Tr⁡1[(Eψ,m⊗I) ∣Φd′⟩⟨Φd′∣]p_m\rho_{\varphi m} = \operatorname{Tr}_1\big[(E_{\psi,m}\otimes I)\,|\Phi_{d'}\rangle\langle\Phi_{d'}|\big]pm​ρφm​=Tr1​[(Eψ,m​⊗I)∣Φd′​⟩⟨Φd′​∣]

(bobState). Bob applies an isometry VmV_mVm​ that depends on mmm only. The protocol is faithful (exact and deterministic) and oblivious to Bob when, for every ψ∈S\psi\in Sψ∈S and every mmm,

Vm (pmρφm) Vm†=pm (φ⊗bm),V_m\,(p_m\rho_{\varphi m})\,V_m^\dagger = p_m\,(\varphi\otimes b_m),Vm​(pm​ρφm​)Vm†​=pm​(φ⊗bm​),

with probabilities pmp_mpm​ and extra output states bmb_mbm​ that do not depend on φ\varphiφ (IsObliviousRSP). A protocol is oblivious to Alice if her measurement uses only one specimen of φ\varphiφ and not her knowledge of it.

Formalization targets

Goal: oblivious to Bob implies oblivious to Alice

For a generic ensemble SSS and a protocol as above, there is one POVM {Mm}m∈M\{M_m\}_{m\in M}{Mm​}m∈M​ on Cd⊗Cd′\mathbb C^d\otimes\mathbb C^{d'}Cd⊗Cd′ (specimen and Alice's half), chosen before ψ\psiψ, such that for every ψ∈S\psi\in Sψ∈S and every mmm

Tr⁡12[(φ1⊗∣Φd′⟩⟨Φd′∣23)(Mm,12⊗I3)]=pm ρφm.\operatorname{Tr}_{12}\big[(\varphi_1\otimes|\Phi_{d'}\rangle\langle\Phi_{d'}|_{23})(M_{m,12}\otimes I_3)\big] = p_m\,\rho_{\varphi m}.Tr12​[(φ1​⊗∣Φd′​⟩⟨Φd′​∣23​)(Mm,12​⊗I3​)]=pm​ρφm​.

Same messages, same probabilities, same states for Bob: the classical cost is unchanged in every cost measure.

Milestones (in the order of the paper's proof)

  1. Eq. (1): pmρφm=pmVm†(φ⊗bm)Vmp_m\rho_{\varphi m} = p_m V_m^\dagger(\varphi\otimes b_m)V_mpm​ρφm​=pm​Vm†​(φ⊗bm​)Vm​.
  2. Eq. (2): ∑mpmρφm=I/d′\sum_m p_m\rho_{\varphi m} = I/d'∑m​pm​ρφm​=I/d′ for any POVM of Alice.
  3. Eq. (3): F(X)=∑mpmVm†(X⊗bm)Vm=Tr⁡(X) I/d′\mathcal F(X) = \sum_m p_m V_m^\dagger(X\otimes b_m)V_m = \operatorname{Tr}(X)\, I/d'F(X)=∑m​pm​Vm†​(X⊗bm​)Vm​=Tr(X)I/d′ for every XXX.
  4. Eqs. (4)–(5): Mm=d d′ pm(I⊗VmT)(∣Φd⟩⟨Φd∣⊗bmT)(I⊗Vm‾)M_m = d\,d'\,p_m(I\otimes V_m^T)(|\Phi_d\rangle\langle\Phi_d|\otimes b_m^T)(I\otimes\overline{V_m})Mm​=dd′pm​(I⊗VmT​)(∣Φd​⟩⟨Φd​∣⊗bmT​)(I⊗Vm​​) is a POVM.
  5. Tr⁡(A Tr⁡2B)=Tr⁡((A⊗I)B)\operatorname{Tr}(A\,\operatorname{Tr}_2 B) = \operatorname{Tr}((A\otimes I)B)Tr(ATr2​B)=Tr((A⊗I)B).
  6. d Tr⁡1[(φT⊗I)∣Φd⟩⟨Φd∣]=φd\,\operatorname{Tr}_1[(\varphi^T\otimes I)|\Phi_d\rangle\langle\Phi_d|] = \varphidTr1​[(φT⊗I)∣Φd​⟩⟨Φd​∣]=φ.
  7. Eqs. (6)–(8): b=∑j1,j2Tr⁡[1d′(φ⊗∣j1⟩⟨j2∣)Mm] ∣j1⟩⟨j2∣\mathbf b = \sum_{j_1,j_2}\operatorname{Tr}[\tfrac1{d'}(\varphi\otimes|j_1\rangle\langle j_2|)M_m]\,|j_1\rangle\langle j_2|b=∑j1​,j2​​Tr[d′1​(φ⊗∣j1​⟩⟨j2​∣)Mm​]∣j1​⟩⟨j2​∣.
  8. Eqs. (9)–(13): b=pmρφm\mathbf b = p_m\rho_{\varphi m}b=pm​ρφm​ for the MmM_mMm​ of (4).

Significance

The paper draws from the goal its corollary: the modified protocol preserves entanglement with other systems and can be used for superdense coding, so it, and hence the original protocol, needs at least 2log⁡d2\log d2logd cbits. This proves Lo's conjecture for faithful, forward-only RSP protocols for generic ensembles that are oblivious to Bob, and it shows which conditions cheaper protocols must drop: the latitude ensemble at the end of the paper shows that genericity cannot be dropped.

The result is proved on paper; no machine-checked version is known to exist. This mission produces a checked conversion from Bob-oblivious to Alice-oblivious protocols, together with reusable finite-dimensional identities about the maximally entangled state (steering, the transpose trick, the partial-trace pairing) and a POVM notion over arbitrary outcome sets. The corollary on communication cost is not part of the mission, since the paper only sketches it.

Difficulty

The construction of MmM_mMm​ is explicit, so the work is in the identities. Two points are easy to get wrong. First, genericity enters exactly once, in (3): the identity F(φ)=I/d′\mathcal F(\varphi) = I/d'F(φ)=I/d′ is known only for the states of SSS and must be extended to every operator by linearity, with an infinite message set summed unconditionally. Without this extension, ∑mMm=I⊗I\sum_m M_m = I\otimes I∑m​Mm​=I⊗I fails. Second, (4) uses transposes and entrywise conjugates, not adjoints, and its registers must be regrouped consistently; replacing VmTV_m^TVmT​ by Vm†V_m^\daggerVm†​ gives operators that do not sum to the identity. The step from (8) to (13) also needs the transpose trick on the maximally entangled state of the input space, which is a different system from the shared state.

Formalization scope

Operators are complex matrices indexed by arbitrary finite types with decidable equality: ι\iotaι (input), σ\sigmaσ (each half of the shared state), KmK_mKm​ (Bob's extra output after message mmm). None is assumed nonempty. The message set MMM is an arbitrary type, and every sum over messages is a HasSum (never a tsum). Tensor products are Mathlib's Kronecker product with the paper's first register first, and three-register operators are regrouped with Equiv.prodAssoc. Partial traces are the published WildeQIT.partialTraceLeft and WildeQIT.partialTraceRight, and density matrices are the published WildeQIT.IsDensityOperator. Conditional states are unnormalized (pmρφmp_m\rho_{\varphi m}pm​ρφm​), so nothing is divided by a possibly zero probability. Bob's unitary with ancilla is replaced by an isometry, so the Tr⁡3\operatorname{Tr}_3Tr3​ of (4) and the Tr⁡2\operatorname{Tr}_2Tr2​ of (1) disappear.

Obliviousness to Alice is the quantifier order of the goal: the POVM is chosen before ψ\psiψ, and it may depend only on VVV, ppp, bbb. A version with the existential after ψ\psiψ would be trivial and is ruled out. The hypotheses are satisfiable with genuine content: the qubit teleportation protocol on the generic ensemble {∣0⟩,∣1⟩,(3∣0⟩+4∣1⟩)/5,(3∣0⟩+4i∣1⟩)/5}\{|0\rangle,|1\rangle,(3|0\rangle+4|1\rangle)/5,(3|0\rangle+4i|1\rangle)/5\}{∣0⟩,∣1⟩,(3∣0⟩+4∣1⟩)/5,(3∣0⟩+4i∣1⟩)/5} satisfies them.

Proofs of the milestones, alternative arguments for the goal, and general lemmas about HasSum of matrix-valued series and about the maximally entangled state are all welcome.

Selected references

  • D. W. Leung and P. W. Shor, Oblivious remote state preparation, arXiv:quant-ph/0201008v1, 2002. https://arxiv.org/abs/quant-ph/0201008
  • H.-K. Lo, Classical-communication cost in distributed quantum-information processing: a generalization of quantum-communication complexity, Phys. Rev. A 62, 012313, 2000. https://doi.org/10.1103/PhysRevA.62.012313
  • C. H. Bennett, D. P. DiVincenzo, P. W. Shor, J. A. Smolin, B. M. Terhal and W. K. Wootters, Remote state preparation, Phys. Rev. Lett. 87, 077902, 2001 (arXiv:quant-ph/0006044). https://arxiv.org/abs/quant-ph/0006044
  • C. H. Bennett, G. Brassard, C. Crépeau, R. Jozsa, A. Peres and W. K. Wootters, Teleporting an unknown quantum state via dual classical and Einstein–Podolsky–Rosen channels, Phys. Rev. Lett. 70, 1895, 1993. https://doi.org/10.1103/PhysRevLett.70.1895
19 thms3 active usersReviewed
Functional AnalysisQuantum 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
9 thms3 active usersReviewed
Quantum Error CorrectionQuantum Information·Captain: mikedeng1

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

Motivation

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

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

Setting

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

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

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

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

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

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

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

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

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

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

Formalization targets

Goal: Corollary 3

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

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

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

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

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

Theorem 2

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

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

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

Milestones

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

Significance

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

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

Difficulty

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

Formalization scope

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

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

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

Selected references

  • P. Mandayam and H. K. Ng, Towards a unified framework for approximate quantum error correction, Phys. Rev. A 86, 012335 (2012). arXiv:1202.5139 (version v2 is the one formalized).
  • H. K. Ng and P. Mandayam, Simple approach to approximate quantum error correction based on the transpose channel, Phys. Rev. A 81, 062342 (2010). arXiv:0909.0931
  • D. Kribs, R. Laflamme and D. Poulin, Unified and generalized approach to quantum error correction, Phys. Rev. Lett. 94, 180501 (2005). arXiv:quant-ph/0412076
  • E. Knill and R. Laflamme, Theory of quantum error-correcting codes, Phys. Rev. A 55, 900 (1997). arXiv:quant-ph/9604034
  • H. Barnum and E. Knill, Reversing quantum dynamics with near-optimal quantum and classical fidelity, J. Math. Phys. 43, 2097 (2002). arXiv:quant-ph/0004088
14 thms3 active usersReviewed
AnalysisFunctional Analysis·Captain: mikedeng1

Noncommutative Lp modules: Every Lp Module over a Finite-Dimensional von Neumann Algebra Is Isometrically Isomorphic, as a Module, to a Principal Column Sum of Projected Lp SpacesResearch Paper

Motivation

A Hilbert space has an orthonormal basis, so every Hilbert space is isometric to some ℓ2(I)\ell^2(I)ℓ2(I). Hilbert C∗^*∗-modules, the analogue of Hilbert spaces in which the inner product takes values in an operator algebra, have no such basis in general. Over a von Neumann algebra M\mathcal MM, Paschke showed that the self-dual Hilbert C∗^*∗-modules are exactly the "ultraweak direct sums" of corners qαMq_\alpha\mathcal Mqα​M cut by projections qα∈Mq_\alpha\in\mathcal Mqα​∈M (Paschke, Trans. AMS 182, 1973).

Junge and Sherman (arXiv:math/0301044v2, 2003, revised 2004) carried this picture to the noncommutative LpL^pLp spaces Lp(M)L^p(\mathcal M)Lp(M), 0<p≤∞0<p\le\infty0<p≤∞. They introduced LpL^pLp modules, whose inner product takes values in Lp/2(M)L^{p/2}(\mathcal M)Lp/2(M), and proved that every LpL^pLp module is a column sum of corners qαLp(M)q_\alpha L^p(\mathcal M)qα​Lp(M). The result organizes the study of module maps between noncommutative LpL^pLp spaces (the paper's §5–§6 on commutants and LpL^pLp bimodules build on it), and it is the LpL^pLp form of the orthonormal-basis theorem. Earlier, Junge had proved a version for a special class of LpL^pLp modules ([J1, Prop. 2.8]).

Setting

Let n∈Nn\in\mathbb Nn∈N and let M\mathcal MM be a unital ∗*∗-subalgebra of the matrix algebra Mn(C)M_n(\mathbb C)Mn​(C); these are exactly the finite-dimensional von Neumann algebras. For real 0<p<∞0<p<\infty0<p<∞, Lp(M)L^p(\mathcal M)Lp(M) is M\mathcal MM with the tracial (quasi)norm

∥a∥p=(Tr (a∗a)p/2)1/p.\|a\|_p=\big(\mathrm{Tr}\,(a^*a)^{p/2}\big)^{1/p}.∥a∥p​=(Tr(a∗a)p/2)1/p.

In the Lean files this is lpNorm p a, the published Schatten norm schattenNorm.

Let X\mathfrak XX be a complex vector space with a right action (ξ,x)↦ξx(\xi,x)\mapsto\xi x(ξ,x)↦ξx of M\mathcal MM (act). An Lp/2L^{p/2}Lp/2-valued inner product (Definition 2.1) is a map ⟨⋅,⋅⟩:X×X→M\langle\cdot,\cdot\rangle:\mathfrak X\times\mathfrak X\to\mathcal M⟨⋅,⋅⟩:X×X→M (ip). It is conjugate linear in the first variable and linear in the second, and satisfies

⟨ξ,ηx⟩=⟨ξ,η⟩x,⟨ξ,η⟩=⟨η,ξ⟩∗,⟨ξ,ξ⟩≥0,⟨ξ,ξ⟩=0  ⟺  ξ=0.\langle\xi,\eta x\rangle=\langle\xi,\eta\rangle x,\qquad\langle\xi,\eta\rangle=\langle\eta,\xi\rangle^*,\qquad\langle\xi,\xi\rangle\ge0,\quad\langle\xi,\xi\rangle=0\iff\xi=0.⟨ξ,ηx⟩=⟨ξ,η⟩x,⟨ξ,η⟩=⟨η,ξ⟩∗,⟨ξ,ξ⟩≥0,⟨ξ,ξ⟩=0⟺ξ=0.

It induces

∥ξ∥=∥⟨ξ,ξ⟩1/2∥p=(Tr ⟨ξ,ξ⟩p/2)1/p\|\xi\|=\big\|\langle\xi,\xi\rangle^{1/2}\big\|_p=\big(\mathrm{Tr}\,\langle\xi,\xi\rangle^{p/2}\big)^{1/p}∥ξ∥=​⟨ξ,ξ⟩1/2​p​=(Tr⟨ξ,ξ⟩p/2)1/p

(gauge p ip ξ). By Proposition 2.2 this is a norm for p≥2p\ge2p≥2 and a p/2p/2p/2-norm for p≤2p\le2p≤2. A right LpL^pLp M\mathcal MM-module (Definition 2.3) is such an X\mathfrak XX that is complete in ∥⋅∥\|\cdot\|∥⋅∥.

Given projections (qα)α∈I(q_\alpha)_{\alpha\in I}(qα​)α∈I​ of M\mathcal MM, the column sum (2.4) is

⨁cqαLp={(ξα)α∈I: ξα∈qαLp, ∑αξα∗ξα converges},⟨(ξα),(ηα)⟩=∑αξα∗ηα.\textstyle\bigoplus_c q_\alpha L^p=\Big\{(\xi_\alpha)_{\alpha\in I}:\ \xi_\alpha\in q_\alpha L^p,\ \sum_\alpha\xi_\alpha^*\xi_\alpha\ \text{converges}\Big\},\qquad\langle(\xi_\alpha),(\eta_\alpha)\rangle=\sum_\alpha\xi_\alpha^*\eta_\alpha.⨁c​qα​Lp={(ξα​)α∈I​: ξα​∈qα​Lp, ∑α​ξα∗​ξα​ converges},⟨(ξα​),(ηα​)⟩=∑α​ξα∗​ηα​.

In Lean this is columnSumSet M q with colIp. The paper calls these modules principal.

Formalization targets

Goal: Theorem 2.5

For every right LpL^pLp M\mathcal MM-module X\mathfrak XX there are an index set III, projections (qα)(q_\alpha)(qα​) of M\mathcal MM and a map T:X→⨁cqαLpT:\mathfrak X\to\bigoplus_c q_\alpha L^pT:X→⨁c​qα​Lp with the following properties: TTT is bijective, complex linear and a module map, and

∥(∑αT(ξ)α∗T(ξ)α)1/2∥p=∥⟨ξ,ξ⟩1/2∥p(ξ∈X).\Big\|\Big(\sum_\alpha T(\xi)_\alpha^*T(\xi)_\alpha\Big)^{1/2}\Big\|_p=\big\|\langle\xi,\xi\rangle^{1/2}\big\|_p\qquad(\xi\in\mathfrak X).​(α∑​T(ξ)α∗​T(ξ)α​)1/2​p​=​⟨ξ,ξ⟩1/2​p​(ξ∈X).

This is the paper's statement as printed: "isometrically isomorphic, as a module". The index set and the projections are not fixed; they are part of the conclusion.

Milestones

  1. Lemma 1.2: Mφ1/p‾=Lps(φ)\overline{\mathcal M\varphi^{1/p}}=L^ps(\varphi)Mφ1/p​=Lps(φ) and φ1/pM‾=s(φ)Lp\overline{\varphi^{1/p}\mathcal M}=s(\varphi)L^pφ1/pM​=s(φ)Lp.
  2. Lemma 1.4: a bounded compatible net ξα=ξαpα\xi_\alpha=\xi_\alpha p_\alphaξα​=ξα​pα​, ξβpα=ξα\xi_\beta p_\alpha=\xi_\alphaξβ​pα​=ξα​ (α<β)(\alpha<\beta)(α<β) in LrL^rLr, r<∞r<\inftyr<∞, converges in norm.
  3. Proposition 2.2: ⟨ξ,η⟩=⟨ξ,ξ⟩1/2T⟨η,η⟩1/2\langle\xi,\eta\rangle=\langle\xi,\xi\rangle^{1/2}T\langle\eta,\eta\rangle^{1/2}⟨ξ,η⟩=⟨ξ,ξ⟩1/2T⟨η,η⟩1/2 with ∥T∥≤1\|T\|\le1∥T∥≤1; ∥⟨ξ,η⟩∥p/2≤∥ξ∥∥η∥\|\langle\xi,\eta\rangle\|_{p/2}\le\|\xi\|\|\eta\|∥⟨ξ,η⟩∥p/2​≤∥ξ∥∥η∥; and ∥⋅∥\|\cdot\|∥⋅∥ is a norm (p≥2p\ge2p≥2) or a p/2p/2p/2-norm (p≤2p\le2p≤2).
  4. (2.4): the column sum is a right LpL^pLp module.
  5. The cyclic case: ξM‾≅s(⟨ξ,ξ⟩1/2)Lp\overline{\xi\mathcal M}\cong s(\langle\xi,\xi\rangle^{1/2})L^pξM​≅s(⟨ξ,ξ⟩1/2)Lp.
  6. Case 2 (p>2p>2p>2): the closed span of an orthogonal family is isomorphic to a column sum, and a vector with 000 as best approximant from that span is orthogonal to the family.

Significance

Theorem 2.5 reduces questions about arbitrary LpL^pLp modules to columns of corners of Lp(M)L^p(\mathcal M)Lp(M). Two consequences follow. Module maps between LpL^pLp modules become matrices of maps between corners, and the paper identifies the commutant of the right action and describes LpL^pLp bimodules in this way. For p=2p=2p=2 the theorem is the orthonormal-basis theorem with M\mathcal MM-valued inner products; for p=∞p=\inftyp=∞ it is Paschke's theorem. In between, there is no Hilbert-space structure to fall back on.

The result is proved in the paper for every von Neumann algebra and every 0<p≤∞0<p\le\infty0<p≤∞. No part of it has been formalized. Mathlib has Hilbert C∗^*∗-modules with the C∗^*∗-norm and the Hermitian functional calculus for matrices, but no noncommutative LpL^pLp spaces, no LpL^pLp modules and no column sums. This mission produces the finite-dimensional theory: the definitions, the Cauchy–Schwarz inequality (2.1)–(2.2) for Lp/2L^{p/2}Lp/2-valued inner products, the column-sum construction and the structure theorem.

Difficulty

Even when M\mathcal MM is finite-dimensional, X\mathfrak XX need not be. An LpL^pLp module may be an infinite column of corners, and the theorem must produce the decomposition without any basis to start from. The obvious idea is to copy Gram–Schmidt and Zorn: take a maximal orthogonal family {ξα}\{\xi_\alpha\}{ξα​} and show that its closed span X0\mathfrak X_0X0​ is everything. For p≠2p\ne2p=2 this step fails as stated. Without an inner product on X\mathfrak XX there is no orthogonal projection onto X0\mathfrak X_0X0​. A best approximation from X0\mathfrak X_0X0​ exists only for p>2p>2p>2 (where X\mathfrak XX is a Banach space and X0\mathfrak X_0X0​ is reflexive), and turning "000 is a best approximant of ζ\zetaζ" into the algebraic identity ⟨ζ,ξλ⟩=0\langle\zeta,\xi_\lambda\rangle=0⟨ζ,ξλ​⟩=0 needs smoothness of the LpL^pLp norm together with the factorization (2.1). The case p<2p<2p<2 is reached by a different route through tensor products with Lq(M)L^q(\mathcal M)Lq(M). A second difficulty is that ∥⋅∥\|\cdot\|∥⋅∥ is the trace norm of ⟨ξ,ξ⟩1/2\langle\xi,\xi\rangle^{1/2}⟨ξ,ξ⟩1/2: it depends on ppp and is not the C∗^*∗-module norm, so Mathlib's C∗^*∗-module results do not apply.

Formalization scope

  • Finite-dimensional algebra. M\mathcal MM is a StarSubalgebra ℂ (Matrix (Fin n) (Fin n) ℂ). Lp(M)L^p(\mathcal M)Lp(M) is M\mathcal MM with the Schatten (quasi)norm of the trace, which is isometric to Haagerup's Lp(M)L^p(\mathcal M)Lp(M). This restriction is forced: Haagerup LpL^pLp spaces of a general von Neumann algebra exist neither in Mathlib nor on the platform. Because Lp/2(M)=ML^{p/2}(\mathcal M)=\mathcal MLp/2(M)=M as a set, the inner-product axioms do not depend on ppp; the norm does.
  • Exponents. Every item assumes 0<p<∞0<p<\infty0<p<∞, and Case 2 items assume p>2p>2p>2 as in the paper. p=∞p=\inftyp=∞ is out of scope.
  • The module. X\mathfrak XX is any complex vector space, of any dimension. The action is a function act with the right-module axioms for elements of M\mathcal MM, and the inner product is the structure LpInnerProduct. Completeness is sequential completeness for ∥⋅∥\|\cdot\|∥⋅∥ (GaugeComplete), since ∥⋅∥\|\cdot\|∥⋅∥ is only a quasi-norm for p<2p<2p<2.
  • Column sums. A column sum is a set of families I→Mn(C)I\to M_n(\mathbb C)I→Mn​(C). Convergence of ∑αξα∗ξα\sum_\alpha\xi_\alpha^*\xi_\alpha∑α​ξα∗​ξα​ is unconditional summability. In the goal, III lives in the universe of X\mathfrak XX.
  • Closures. In Lemma 1.2 and in the cyclic case the closures on the page are of finite-dimensional subspaces and are dropped. The closed span X0\mathfrak X_0X0​ of Case 2 keeps its closure.
  • No trivialization. Several formalizations would make the theorem empty or a different theorem, and none is admissible: measuring X\mathfrak XX in the C∗^*∗-norm ∥⟨ξ,ξ⟩∥1/2\|\langle\xi,\xi\rangle\|^{1/2}∥⟨ξ,ξ⟩∥1/2 (which makes the statement the p=∞p=\inftyp=∞ theorem), assuming X\mathfrak XX finite-dimensional or given with a basis, or asking only for a non-bijective or non-linear TTT.
  • Infrastructure. The development needs the Hermitian functional calculus on matrices (square roots, powers, support projections), Hölder's inequality and the p/2p/2p/2-triangle inequality for Schatten quasinorms, and summability of positive matrix families. These pieces are reusable beyond this mission. Proofs of any milestone are welcome, as are proofs of Theorem 2.5 by routes other than the paper's.

Selected references

  • M. Junge and D. Sherman, Noncommutative LpL^pLp modules, preprint arXiv:math/0301044v2, 2003, revised 14 Sep 2004. arXiv:math/0301044v2
  • W. L. Paschke, Inner product modules over B∗^*∗-algebras, Trans. Amer. Math. Soc. 182 (1973), 443–468 (reference [Pa] of the paper; cited as [P] on p. 10).
  • H. Kosaki, Applications of the complex interpolation method to a von Neumann algebra: noncommutative LpL^pLp-spaces, J. Funct. Anal. 56 (1984), 29–78 (reference [K1] of the paper).
  • U. Haagerup, LpL^pLp-spaces associated with an arbitrary von Neumann algebra, Algèbres d’opérateurs et leurs applications en physique mathématique, CNRS 15 (1979), 175–184 (reference [H] of the paper).
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Quantum InformationRepresentation Theory·Captain: mikedeng1

Commutant Structure of U⊗(n−1) ⊗ U* Transformations: The Operator Basis v^{ab}_{ij}(α) Is a Linear Combination of Partially Transposed Permutation Operators, and ConverselyResearch Paper

Motivation

Operators on nnn copies of Cd\mathbb C^dCd that commute with every U⊗nU^{\otimes n}U⊗n, UUU unitary, are exactly the linear combinations of permutation operators V(σ)V(\sigma)V(σ), σ∈S(n)\sigma\in S(n)σ∈S(n) (Schur–Weyl duality). Many protocols in quantum information carry a different symmetry: the first n−1n-1n−1 systems transform by UUU and the last by the complex conjugate Uˉ\bar UUˉ. It is the symmetry of port-based teleportation (Ishizaka–Hiroshima 2008), whose optimal performance is computed from the representation theory of exactly this commutant (Studziński et al. 2017). The commutant of U⊗(n−1)⊗UˉU^{\otimes(n-1)}\otimes\bar UU⊗(n−1)⊗Uˉ is the algebra A\mathcal AA spanned by the partially transposed permutation operators V′(σ)V'(\sigma)V′(σ): the permutation operators with the transpose taken on the last system.

Studziński, Horodecki and Mozrzymas give an explicit operator basis of an ideal of A\mathcal AA adapted to the irreducible representations of S(n−2)S(n-2)S(n−2). Their main structural result, Theorem 9, states that this basis and the partially transposed permutation operators are linear combinations of each other, with coefficients that are irrep matrix elements.

Setting

Let H=Cd\mathcal H=\mathbb C^dH=Cd and n≥2n\ge2n≥2. For σ∈S(n)\sigma\in S(n)σ∈S(n), the permutation operator V(σ)V(\sigma)V(σ) on H⊗n\mathcal H^{\otimes n}H⊗n is V(σ)∣i1…in⟩=∣iσ−1(1)…iσ−1(n)⟩V(\sigma)|i_1\dots i_n\rangle=|i_{\sigma^{-1}(1)}\dots i_{\sigma^{-1}(n)}\rangleV(σ)∣i1​…in​⟩=∣iσ−1(1)​…iσ−1(n)​⟩. The partial transposition X↦X′X\mapsto X'X↦X′ transposes the last system: (∣x1…xn⟩⟨y1…yn∣)′=∣x1…xn−1yn⟩⟨y1…yn−1xn∣(|x_1\dots x_n\rangle\langle y_1\dots y_n|)'=|x_1\dots x_{n-1}y_n\rangle\langle y_1\dots y_{n-1}x_n|(∣x1​…xn​⟩⟨y1​…yn​∣)′=∣x1​…xn−1​yn​⟩⟨y1​…yn−1​xn​∣. The algebra A\mathcal AA is the span of all V′(τ)V'(\tau)V′(τ), τ∈S(n)\tau\in S(n)τ∈S(n). S(k)S(k)S(k) is regarded inside S(n)S(n)S(n) as the permutations fixing the systems after kkk.

Fix π1,…,πn−1∈S(n−1)\pi_1,\dots,\pi_{n-1}\in S(n-1)π1​,…,πn−1​∈S(n−1) with πk(n−1)=k\pi_k(n-1)=kπk​(n−1)=k, and write Πk=V(πk)\Pi_k=V(\pi_k)Πk​=V(πk​). For labels a,b∈{1,…,n−1}a,b\in\{1,\dots,n-1\}a,b∈{1,…,n−1}, the maps fab:S(n−2)→S(n)f_{ab}:S(n-2)\to S(n)fab​:S(n−2)→S(n) are

fab(σ)=πb∘σ∘(n n−1)∘πa−1.f_{ab}(\sigma)=\pi_b\circ\sigma\circ(n\ n-1)\circ\pi_a^{-1}.fab​(σ)=πb​∘σ∘(n n−1)∘πa−1​.

The standing data are a family of real orthogonal, irreducible, pairwise inequivalent matrix representations φα\varphi^\alphaφα of S(n−2)S(n-2)S(n−2), of dimensions dαd_\alphadα​, and a Schur basis: an orthonormal basis ∣ϕi(α,r)⟩|\phi_i(\alpha,r)\rangle∣ϕi​(α,r)⟩ of H⊗(n−2)\mathcal H^{\otimes(n-2)}H⊗(n−2), where rrr ranges over the multiplicity of α\alphaα, such that V(σ)∣ϕj(α,r)⟩=∑iφijα(σ)∣ϕi(α,r)⟩V(\sigma)|\phi_j(\alpha,r)\rangle=\sum_i\varphi^\alpha_{ij}(\sigma)|\phi_i(\alpha,r)\rangleV(σ)∣ϕj​(α,r)⟩=∑i​φijα​(σ)∣ϕi​(α,r)⟩. With ∣Φ+⟩=1d∑l∣ll⟩|\Phi^+\rangle=\frac1{\sqrt d}\sum_l|ll\rangle∣Φ+⟩=d​1​∑l​∣ll⟩ on the last two systems, the paper defines

∣ψik(α,r)⟩=d Πk∣ϕi(α,r)⟩∣Φ+⟩,vijab(α)=∑r∣ψia(α,r)⟩⟨ψjb(α,r)∣,|\psi^k_i(\alpha,r)\rangle=\sqrt d\,\Pi_k|\phi_i(\alpha,r)\rangle|\Phi^+\rangle,\qquad v^{ab}_{ij}(\alpha)=\sum_r|\psi^a_i(\alpha,r)\rangle\langle\psi^b_j(\alpha,r)|,∣ψik​(α,r)⟩=d​Πk​∣ϕi​(α,r)⟩∣Φ+⟩,vijab​(α)=r∑​∣ψia​(α,r)⟩⟨ψjb​(α,r)∣,

and Eijα=∑r∣ϕi(α,r)⟩⟨ϕj(α,r)∣E^\alpha_{ij}=\sum_r|\phi_i(\alpha,r)\rangle\langle\phi_j(\alpha,r)|Eijα​=∑r​∣ϕi​(α,r)⟩⟨ϕj​(α,r)∣. In Lean these are IrrepFamily, SchurBasis, psi, vOp, EOp, with ptLast for ′'′, fPerm for fabf_{ab}fab​ and algA for A\mathcal AA.

Formalization targets

Goal: Theorem 9

For all a,ba,ba,b, α\alphaα, i,ji,ji,j:

vijab(α)=dα(n−2)!∑σ∈S(n−2)φijα(σ) V′(fba(σ))∈A,v^{ab}_{ij}(\alpha)=\frac{d_\alpha}{(n-2)!}\sum_{\sigma\in S(n-2)}\varphi^\alpha_{ij}(\sigma)\,V'\big(f_{ba}(\sigma)\big)\in\mathcal A,vijab​(α)=(n−2)!dα​​σ∈S(n−2)∑​φijα​(σ)V′(fba​(σ))∈A,

and for every σ∈S(n−2)\sigma\in S(n-2)σ∈S(n−2), with σab=fab(σ)\sigma_{ab}=f_{ab}(\sigma)σab​=fab​(σ),

V′(σab)=⨁α∑i,jφijα(fab−1(σab)) vijba(α).V'(\sigma_{ab})=\bigoplus_\alpha\sum_{i,j}\varphi^\alpha_{ij}\big(f_{ab}^{-1}(\sigma_{ab})\big)\,v^{ba}_{ij}(\alpha).V′(σab​)=α⨁​i,j∑​φijα​(fab−1​(σab​))vijba​(α).

The goal is the whole theorem, both directions and the membership in A\mathcal AA.

Milestones

  1. Permutations of S(n−1)S(n-1)S(n−1) are invariant under ′'′ and pass through it: V(ρ)V′(τ)V(ρ′)=V′(ρτρ′)V(\rho)V'(\tau)V(\rho')=V'(\rho\tau\rho')V(ρ)V′(τ)V(ρ′)=V′(ρτρ′) (proof of Lemma 26).
  2. Lemma 26: V′(σab)=ΠbV(fab−1(σab))V′(n n−1)Πa−1V'(\sigma_{ab})=\Pi_bV(f^{-1}_{ab}(\sigma_{ab}))V'(n\ n-1)\Pi_a^{-1}V′(σab​)=Πb​V(fab−1​(σab​))V′(n n−1)Πa−1​ with fab−1(σab)∈S(n−2)f^{-1}_{ab}(\sigma_{ab})\in S(n-2)fab−1​(σab​)∈S(n−2).
  3. Eq. (9): the Sab=fab(S(n−2))S_{ab}=f_{ab}(S(n-2))Sab​=fab​(S(n−2)) and S(n−1)S(n-1)S(n−1) partition S(n)S(n)S(n), and each fabf_{ab}fab​ is injective.
  4. V′(n−1,n)=1⊗∑l,l′∣ll⟩⟨l′l′∣V'(n-1,n)=\mathbb 1\otimes\sum_{l,l'}|ll\rangle\langle l'l'|V′(n−1,n)=1⊗∑l,l′​∣ll⟩⟨l′l′∣.
  5. Eq. (21): Eijα∈C[S(n−2)]E^\alpha_{ij}\in\mathbb C[S(n-2)]Eijα​∈C[S(n−2)] maps to vijab(α)=Πa(Eijα⊗1)V′(n n−1)Πb−1∈Mv^{ab}_{ij}(\alpha)=\Pi_a(E^\alpha_{ij}\otimes\mathbb 1)V'(n\ n-1)\Pi_b^{-1}\in\mathcal Mvijab​(α)=Πa​(Eijα​⊗1)V′(n n−1)Πb−1​∈M.
  6. Eq. (139): the orthogonality relation 1∣G∣∑gφijα(g)φkpβ(g−1)=1dαδαβδipδjk\frac1{|G|}\sum_g\varphi^\alpha_{ij}(g)\varphi^\beta_{kp}(g^{-1})=\frac1{d_\alpha}\delta^{\alpha\beta}\delta_{ip}\delta_{jk}∣G∣1​∑g​φijα​(g)φkpβ​(g−1)=dα​1​δαβδip​δjk​ for G=S(n−2)G=S(n-2)G=S(n−2).
  7. Eq. (86): Eijα=dα(n−2)!∑σφijα(σ)V(σ)E^\alpha_{ij}=\frac{d_\alpha}{(n-2)!}\sum_\sigma\varphi^\alpha_{ij}(\sigma)V(\sigma)Eijα​=(n−2)!dα​​∑σ​φijα​(σ)V(σ).
  8. Eq. (86): V(σ)=⨁α∑ijφijα(σ)EijαV(\sigma)=\bigoplus_\alpha\sum_{ij}\varphi^\alpha_{ij}(\sigma)E^\alpha_{ij}V(σ)=⨁α​∑ij​φijα​(σ)Eijα​.

Significance

Theorem 9 shows that the vijab(α)v^{ab}_{ij}(\alpha)vijab​(α) span the same space as the operators V′(σ)V'(\sigma)V′(σ) with σ(n)≠n\sigma(n)\neq nσ(n)=n. That space is the ideal of A\mathcal AA on which the partial transposition acts non-trivially. Because the vijab(α)v^{ab}_{ij}(\alpha)vijab​(α) multiply like block matrices (Lemma 8 of the paper), the theorem converts questions about A\mathcal AA into finite matrix computations indexed by irreps of S(n−2)S(n-2)S(n−2). The later constructions of the paper rest on this: the Gram matrices Q(α)Q(\alpha)Q(α), the biorthogonal basis and the explicit irreps of A\mathcal AA. The same formalism underlies the eigenvalue analysis of port-based teleportation (Mozrzymas–Studziński–Horodecki 2018).

The result has a published proof but no machine-checked one. This mission adds that check, together with a reusable Lean vocabulary: the partial transpose on one site of (Cd)⊗n(\mathbb C^d)^{\otimes n}(Cd)⊗n, the embeddings S(k)↪S(n)S(k)\hookrightarrow S(n)S(k)↪S(n), and Schur-basis data for permutation operators. It also pins down the conventions that the printed text leaves inconsistent (see Formalization scope).

Difficulty

The algebraic manipulations are short on paper; the work lies in the bookkeeping they hide. Lemma 26 requires checking that πb−1∘σab∘πa∘(n n−1)\pi_b^{-1}\circ\sigma_{ab}\circ\pi_a\circ(n\ n-1)πb−1​∘σab​∘πa​∘(n n−1) fixes both of the last two systems, which uses πk(n−1)=k\pi_k(n-1)=kπk​(n−1)=k in an essential way. The partial transposition is not multiplicative, so every step that moves an operator through ′'′ needs the specific invariance of milestone 1. Eq. (86) is the identification of the Schur-basis matrix units with group-algebra elements; it needs completeness of the basis together with Schur's orthogonality relations for real irreps, and it is false without irreducibility and inequivalence. Mathlib has Schur's lemma but no coordinate form of the orthogonality relations for matrix representations, and nothing on partial transposes of tensor-power permutation operators.

Formalization scope

  • Indexing. The paper's nnn is m+2m+2m+2. S(n−2)S(n-2)S(n−2), S(n−1)S(n-1)S(n−1), S(n)S(n)S(n) are Equiv.Perm (Fin m), Equiv.Perm (Fin (m+1)), Equiv.Perm (Fin (m+2)). Systems are 0-based, so systems n−1,nn-1,nn−1,n are indices m,m+1m,m+1m,m+1, and labels a,ba,ba,b are Fin (m+1). Permutation products compose right to left.
  • Operators are complex matrices indexed by {1..d}k\{1..d\}^k{1..d}k. V(σ)V(\sigma)V(σ) is the published QAlgorithms.Schur.tensorPermutation. ′'′ is on the last system only. groupAlg is the represented C[S(n−2)]\mathbb C[S(n-2)]C[S(n−2)]; algM spans the V′(τ)V'(\tau)V′(τ) with τ(n)≠n\tau(n)\ne nτ(n)=n.
  • Standing data. IrrepFamily m contains real orthogonal matrix representations of S(m)S(m)S(m) of positive dimension, irreducible over C\mathbb CC and pairwise inequivalent over C\mathbb CC (p. 7 and Notation 32 of the paper). SchurBasis F d is an orthonormal, spanning family of vectors on which V(σ)V(\sigma)V(σ) acts by the φα\varphi^\alphaφα. Multiplicities may be zero. The family is not required to list every irrep of S(m)S(m)S(m). Every πk\pi_kπk​ satisfies πk(n−1)=k\pi_k(n-1)=kπk​(n−1)=k (Definition 24).
  • Constants are literal: dα/(n−2)!d_\alpha/(n-2)!dα​/(n−2)!, the factor d\sqrt dd​ of ψ\psiψ and the 1/d1/\sqrt d1/d​ of ∣Φ+⟩|\Phi^+\rangle∣Φ+⟩. ⨁α\bigoplus_\alpha⨁α​ is a sum over all labels.
  • Ruled out. vijab(α)v^{ab}_{ij}(\alpha)vijab​(α) is defined from the vectors ψ\psiψ (Definition 5) and EijαE^\alpha_{ij}Eijα​ from the Schur basis (footnote 4). Neither is defined as a group sum or through Fabt\mathcal F^t_{ab}Fabt​, and the Schur basis carries no orthogonality relation. A formalization that builds (86) or (21) into the definitions makes Theorem 9 a tautology and is not this mission.
  • Source slips. Eq. (11) prints σab(n)=a\sigma_{ab}(n)=aσab​(n)=a, σab−1[n]=b\sigma^{-1}_{ab}[n]=bσab−1​[n]=b, contrary to Notation 1 and eq. (7); the Lean statements follow Notation 1 (σab(a)=n\sigma_{ab}(a)=nσab​(a)=n, σab(n)=b\sigma_{ab}(n)=bσab​(n)=b). Eq. (139) is stated with 1/∣G∣1/|G|1/∣G∣ and a sum over ggg, correcting the printed 1/n!1/n!1/n! and ∑h\sum_h∑h​.
  • Welcome contributions: the coordinate Schur orthogonality relations for matrix representations of finite groups, and lemmas on ptLast and on liftPerm. Both are reusable beyond this paper.

Selected references

  • M. Studziński, M. Horodecki, M. Mozrzymas, Commutant structuture of U⊗(n−1)⊗U∗U^{\otimes(n-1)}\otimes U^*U⊗(n−1)⊗U∗ transformations, arXiv:1305.6183v2, 2013. https://arxiv.org/abs/1305.6183
  • S. Ishizaka, T. Hiroshima, Asymptotic teleportation scheme as a universal programmable quantum processor, Phys. Rev. Lett. 101, 240501, 2008. https://arxiv.org/abs/0807.4568
  • M. Studziński, S. Strelchuk, M. Mozrzymas, M. Horodecki, Port-based teleportation in arbitrary dimension, Sci. Rep. 7, 10871, 2017. https://arxiv.org/abs/1612.09260
  • M. Mozrzymas, M. Studziński, M. Horodecki, A simplified formalism of the algebra of partially transposed permutation operators with applications, J. Phys. A 51, 125202, 2018. https://arxiv.org/abs/1708.02434
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Quantum Information·Captain: mikedeng1

On a Family of a Linear Maps from Mₙ(ℂ) to Mₙ²(ℂ): Φ[α, β] on M₃(ℂ) Is 2-Positive and Not Completely Positive Exactly When β ≤ −0.2 and α Lies in an Explicit IntervalResearch Paper

Motivation

Positive linear maps on complex matrix algebras provide tests for quantum entanglement: applying such a map to one part of a bipartite state can expose a state that cannot be written as a mixture of product states. The distinction between ordinary positivity, positivity with an auxiliary matrix system, and complete positivity is therefore substantive. Collins, Osaka, and Sapra study an explicit two-parameter family that makes these distinctions visible through inequalities in the parameters. Their paper identifies the exact region where a map from three-by-three matrices to nine-by-nine matrices is 2-positive but fails to be completely positive. This is the stated main result of their 2018 paper, rather than an open conjecture.

Setting

Write Mn(C)M_n(\mathbb C)Mn​(C) for the algebra of n×nn\times nn×n complex matrices. A matrix XXX is positive semidefinite, written X≥0X\geq0X≥0, when it is Hermitian and has no negative eigenvalues. A complex-linear map Ψ:Md1(C)→Md2(C)\Psi:M_{d_1}(\mathbb C)\to M_{d_2}(\mathbb C)Ψ:Md1​​(C)→Md2​​(C) is positive when X≥0X\geq0X≥0 implies Ψ(X)≥0\Psi(X)\geq0Ψ(X)≥0. It is kkk-positive when the same condition holds after the identity map on Mk(C)M_k(\mathbb C)Mk​(C) is tensored with Ψ\PsiΨ. It is completely positive when it is kkk-positive for every kkk. A map is completely copositive when its composition with transpose on the source is completely positive. These are the paper's definitions on page 2.

Let Bn=∑i=1nei⊗eiB_n=\sum_{i=1}^n e_i\otimes e_iBn​=∑i=1n​ei​⊗ei​ be the unnormalized Bell vector, and let Bn2=BnBn∗B_{n^2}=B_nB_n^*Bn2​=Bn​Bn∗​ denote its rank-one projector. For real α,β\alpha,\betaα,β and n≥3n\geq3n≥3, the family on page 3 is

Φα,β,n(A)=AT⊗In+In⊗A+Tr⁡(A)(αIn2+βBn2).\Phi_{\alpha,\beta,n}(A) =A^{\mathsf T}\otimes I_n+I_n\otimes A +\operatorname{Tr}(A)\bigl(\alpha I_{n^2}+\beta B_{n^2}\bigr).Φα,β,n​(A)=AT⊗In​+In​⊗A+Tr(A)(αIn2​+βBn2​).

The transpose belongs to the first tensor factor. The mission concentrates on Φ[α,β]=Φα,β,3\Phi[\alpha,\beta]=\Phi_{\alpha,\beta,3}Φ[α,β]=Φα,β,3​. Its Choi matrix is CΨ=∑i,jeij⊗Ψ(eij)C_\Psi=\sum_{i,j}e_{ij}\otimes\Psi(e_{ij})CΨ​=∑i,j​eij​⊗Ψ(eij​). For this finite-dimensional setting, the Choi criterion relates complete positivity to CΨ≥0C_\Psi\geq0CΨ​≥0; it does not define complete positivity. The paper also identifies an equivariance property: unitary conjugation of the input corresponds to conjugation of the output by a matrix associated with the same unitary.

Formalization targets

For β∈R\beta\in\mathbb Rβ∈R, define two boundary curves and a cubic root:

ℓP(β)=−(2+3β)+9β2−4β+42,ℓCP(β)=−(3+3β)+9β2−10β+172,\ell_P(\beta)=\frac{-(2+3\beta)+\sqrt{9\beta^2-4\beta+4}}2, \qquad \ell_{CP}(\beta)=\frac{-(3+3\beta)+\sqrt{9\beta^2-10\beta+17}}2,ℓP​(β)=2−(2+3β)+9β2−4β+4​​,ℓCP​(β)=2−(3+3β)+9β2−10β+17​​, Sβ=min⁡{x∈R:x3+(−2−3β)x2+(−2+4β)x+2β=0}.S_\beta=\min\{x\in\mathbb R:x^3+(-2-3\beta)x^2+(-2+4\beta)x+2\beta=0\}.Sβ​=min{x∈R:x3+(−2−3β)x2+(−2+4β)x+2β=0}.

The goal is Theorem 3.9, page 10:

Φ[α,β] is 2-positive and not completely positive⟺β≤−15,α∈[ℓP(β),ℓCP(β))∩[1,∞)∩[−Sβ,∞).\Phi[\alpha,\beta]\text{ is 2-positive and not completely positive} \quad\Longleftrightarrow\quad \beta\leq-\tfrac15, \quad\alpha\in[\ell_P(\beta),\ell_{CP}(\beta)) \cap[1,\infty)\cap[-S_\beta,\infty).Φ[α,β] is 2-positive and not completely positive⟺β≤−51​,α∈[ℓP​(β),ℓCP​(β))∩[1,∞)∩[−Sβ​,∞).

The left endpoint of the first interval is included and the right endpoint is excluded. The milestones record the paper's earlier criteria for positivity, complete positivity, and 2-positivity, together with its general equivariance criterion and the computation for this family. Their inequalities are separate targets; none is built into the definitions of these map properties.

Significance

The goal gives an exact, parameter-level example of 2-positivity without complete positivity. It identifies all such members of this family on M3(C)M_3(\mathbb C)M3​(C), including the boundary cases, rather than only exhibiting one map. The surrounding results locate the positive and completely positive regions and give a criterion for testing kkk-positivity of equivariant maps. Together, they provide a compact source of concrete maps with different strengths of positivity, as described in Sections 2 and 3 of the paper.

The mathematical result was proved in 2018. This mission seeks a machine-checked account of the stated criteria, with the family, Choi matrix, Bell projector, and positivity predicates exposed as reusable declarations. A finished proof would connect elementary matrix positivity and tensor products to explicit real-algebraic parameter bounds. It would also make each boundary independently inspectable. The Lean theorem statements here are draft targets with sorry; they are not existing machine-checked proofs of the paper.

Difficulty

Testing only Φ[α,β](e11)≥0\Phi[\alpha,\beta](e_{11})\geq0Φ[α,β](e11​)≥0 yields ordinary positivity, not 2-positivity. Testing only the Choi matrix addresses complete positivity, which is stronger than the desired property. The 2-positive condition quantifies over every positive semidefinite matrix in M2(C)⊗M3(C)M_2(\mathbb C)\otimes M_3(\mathbb C)M2​(C)⊗M3​(C); the paper's criterion reduces that universal condition under equivariance to positivity of a specific block matrix. The block matrix has parameter-dependent eigenvalues, including roots of a cubic. This makes a simple comparison of the two square-root boundary curves insufficient: the smallest cubic root supplies an additional lower bound on α\alphaα. The endpoint β=−1/5\beta=-1/5β=−1/5 also needs attention because the case descriptions for complete positivity meet there.

Formalization scope

The Lean model uses Matrix (Fin n) (Fin n) ℂ for Mn(C)M_n(\mathbb C)Mn​(C) and Fin n × Fin n for the output tensor indices, with the first coordinate corresponding to the transposed factor. The paper's one-based e11e_{11}e11​ is Matrix.single 0 0 1. Positive semidefiniteness is Mathlib's Matrix.PosSemidef. The shared QAlgorithms.idTensorSuperop applies a map blockwise with the auxiliary index first, and the published QAlgorithms.Entanglement.IsCompletelyPositive quantifies over all auxiliary sizes. Size zero is harmless for that quantifier because the corresponding matrix type is empty. The paper's n≥3n\geq3n≥3 appears on the general-family results; the main goal fixes n=3n=3n=3.

The Bell projector is unnormalized, matching the paper's BnBn∗B_nB_n^*Bn​Bn∗​. The two square roots have positive radicands on the real parameter range. The cubic root SβS_\betaSβ​ is defined as the infimum of its real root set; the odd-degree cubic has a nonempty, finite set of real roots, so this is its least root. The proof development needs reusable facts about unitary conjugation of positive matrices, Kronecker products, Choi matrices, and positivity of the parameterized block matrix. Direct calculations of the boundary inequalities are also welcome. Defining kkk-positivity by the block criterion, complete positivity by Choi positivity, omitting the transpose in Φ\PhiΦ, or treating SβS_\betaSβ​ as an arbitrary parameter would make the targets lose their intended content.

Selected references

  • Benoît Collins, Hiroyuki Osaka, and Gunjan Sapra, On a family of a linear maps from Mn(C) to Mn2(C), Linear Algebra and its Applications, 2018; cited here from arXiv:1802.07553v1, pp. 2–10.
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OptimizationQuantum InformationTheoretical Computer Science·Captain: mikedeng1

Optimization by Decoded Quantum Interferometry 1: The Semicircle Law — the Optimal Degree-ℓ DQI State Satisfies ⟨s⟩/m → (√(μ(1−ρ)) + √(ρ(1−μ)))² When 2ℓ + 1 < d⊥Research Paper

Motivation

Decoded quantum interferometry (DQI) is a quantum algorithm, introduced by Jordan, Shutty, Wootters, Zalcman, Schmidhuber, King, Isakov, Khattar and Babbush (arXiv:2408.08292), that turns an approximate optimization problem over a finite field into a decoding problem for a linear code. It applies to max-LINSAT: given linear constraints over Fp\mathbb F_pFp​, satisfy as many of them as possible. For structured instances such as optimal polynomial intersection the authors find DQI reaching approximation ratios that no known polynomial-time classical algorithm reaches, which makes it one of the few concrete candidates for a quantum advantage in optimization.

Whether DQI is useful on an instance depends on one number: the expected fraction of constraints satisfied by the string it outputs. Theorem 4.1 of the paper computes this number, in the limit of many constraints, for the best DQI state of a given degree. Every comparison of DQI with classical algorithms in the paper (simulated annealing, Prange's algorithm, the OPI and max-XORSAT benchmarks) is a comparison against this formula, and the follow-up analysis of imperfect decoders (Theorem 10.1) is a perturbation of it.

Setting

Fix a prime ppp. A max-LINSAT instance is a matrix B∈Fpm×nB\in\mathbb F_p^{m\times n}B∈Fpm×n​ with rows b1,…,bm\mathbf b_1,\dots,\mathbf b_mb1​,…,bm​ and subsets F1,…,Fm⊆FpF_1,\dots,F_m\subseteq\mathbb F_pF1​,…,Fm​⊆Fp​; constraint iii asks that bi⋅x∈Fi\mathbf b_i\cdot\mathbf x\in F_ibi​⋅x∈Fi​ (Definition 2.1). Throughout, m>nm>nm>n and every FiF_iFi​ has the same size r∈{1,…,p−1}r\in\{1,\dots,p-1\}r∈{1,…,p−1}. Put fi(a)=+1f_i(a)=+1fi​(a)=+1 if a∈Fia\in F_ia∈Fi​ and −1-1−1 otherwise, and

f(x)=∑i=1mfi(bi⋅x),s(x)=#{i:bi⋅x∈Fi}.f(\mathbf x)=\sum_{i=1}^m f_i(\mathbf b_i\cdot\mathbf x),\qquad s(\mathbf x)=\#\{i:\mathbf b_i\cdot\mathbf x\in F_i\}.f(x)=i=1∑m​fi​(bi​⋅x),s(x)=#{i:bi​⋅x∈Fi​}.

For a real polynomial PPP of degree at most ℓ\ellℓ, the DQI state is ∣P(f)⟩=∑x∈FpnP(f(x))∣x⟩|P(f)\rangle=\sum_{\mathbf x\in\mathbb F_p^n}P(f(\mathbf x))|\mathbf x\rangle∣P(f)⟩=∑x∈Fpn​​P(f(x))∣x⟩, normalized so that ∑xP(f(x))2=1\sum_{\mathbf x}P(f(\mathbf x))^2=1∑x​P(f(x))2=1. Measuring it in the computational basis returns x\mathbf xx with probability P(f(x))2P(f(\mathbf x))^2P(f(x))2, so the expected number of satisfied constraints is

⟨s⟩=∑xP(f(x))2 s(x),\langle s\rangle=\sum_{\mathbf x}P(f(\mathbf x))^2\,s(\mathbf x),⟨s⟩=x∑​P(f(x))2s(x),

and ⟨s(m,ℓ)⟩opt\langle s^{(m,\ell)}\rangle_{\rm opt}⟨s(m,ℓ)⟩opt​ is its supremum over all such PPP.

The dual code is C⊥={d∈Fpm:BTd=0}C^\perp=\{\mathbf d\in\mathbb F_p^m:B^T\mathbf d=0\}C⊥={d∈Fpm​:BTd=0} and d⊥d^\perpd⊥ is the least Hamming weight of a nonzero codeword. The condition 2ℓ+1<d⊥2\ell+1<d^\perp2ℓ+1<d⊥ says that syndromes of errors of weight up to ℓ\ellℓ (and a little more) determine the error.

The analysis passes through rescaled constraint functions gi=(fi−fˉ)/φg_i=(f_i-\bar f)/\varphigi​=(fi​−fˉ​)/φ with Fourier transforms g~i\tilde g_ig~​i​, the elementary symmetric polynomials P(k)P^{(k)}P(k) evaluated at the gi(bi⋅x)g_i(\mathbf b_i\cdot\mathbf x)gi​(bi​⋅x), and the (ℓ+1)×(ℓ+1)(\ell+1)\times(\ell+1)(ℓ+1)×(ℓ+1) symmetric tridiagonal matrix A(m,ℓ,d)A^{(m,\ell,d)}A(m,ℓ,d) with diagonal 0,d,2d,…,ℓd0,d,2d,\dots,\ell d0,d,2d,…,ℓd and off-diagonal entries ak=k(m−k+1)a_k=\sqrt{k(m-k+1)}ak​=k(m−k+1)​, at d=(p−2r)/r(p−r)d=(p-2r)/\sqrt{r(p-r)}d=(p−2r)/r(p−r)​.

Formalization targets

Goal: Theorem 4.1 (the semicircle law)

Fix ppp, rrr and μ≥0\mu\ge0μ≥0. For any sequence of instances with m→∞m\to\inftym→∞, ℓ/m→μ\ell/m\to\muℓ/m→μ and 2ℓ+1<d⊥2\ell+1<d^\perp2ℓ+1<d⊥, writing ρ=r/p\rho=r/pρ=r/p,

lim⁡⟨s(m,ℓ)⟩optm={(μ(1−ρ)+ρ(1−μ))2,ρ≤1−μ,1,otherwise.\lim\frac{\langle s^{(m,\ell)}\rangle_{\rm opt}}{m}=\begin{cases}\big(\sqrt{\mu(1-\rho)}+\sqrt{\rho(1-\mu)}\big)^2,&\rho\le1-\mu,\\ 1,&\text{otherwise.}\end{cases}limm⟨s(m,ℓ)⟩opt​​={(μ(1−ρ)​+ρ(1−μ)​)2,1,​ρ≤1−μ,otherwise.​

For ρ=12\rho=\tfrac12ρ=21​ the curve is 12+μ(1−μ)\tfrac12+\sqrt{\mu(1-\mu)}21​+μ(1−μ)​, a semicircle, which gives the theorem its name.

Milestones

  1. The normalization of the rescaled gig_igi​, (37)–(40).
  2. Lemma A.1: under a common quadratic identity, P(x1+⋯+xm)P(x_1+\dots+x_m)P(x1​+⋯+xm​) is a fixed linear combination of elementary symmetric polynomials.
  3. The counting identity (68), ∑∣y∣=k∣g~(y)∣2=(mk)\sum_{|\mathbf y|=k}|\tilde g(\mathbf y)|^2=\binom mk∑∣y∣=k​∣g~​(y)∣2=(km​), and the Fourier picture (65) of the DQI state.
  4. Lemma 9.1 (norm =∥w∥2=\|\mathbf w\|^2=∥w∥2 when 2ℓ<d⊥2\ell<d^\perp2ℓ<d⊥) and Lemma 9.2 (the expected count is mrp+r(p−r)pwTA(m,ℓ,d)w\frac{mr}p+\frac{\sqrt{r(p-r)}}p\mathbf w^TA^{(m,\ell,d)}\mathbf wpmr​+pr(p−r)​​wTA(m,ℓ,d)w when 2ℓ+1<d⊥2\ell+1<d^\perp2ℓ+1<d⊥).
  5. The finite-size identity (131): ⟨s(m,ℓ)⟩opt/m=ρ+ρ(1−ρ) λmax⁡(m,ℓ,d)/m\langle s^{(m,\ell)}\rangle_{\rm opt}/m=\rho+\sqrt{\rho(1-\rho)}\,\lambda_{\max}^{(m,\ell,d)}/m⟨s(m,ℓ)⟩opt​/m=ρ+ρ(1−ρ)​λmax(m,ℓ,d)​/m.
  6. Lemma 9.3, λmax⁡(m,ℓ,d)/m→μd+2μ(1−μ)\lambda_{\max}^{(m,\ell,d)}/m\to\mu d+2\sqrt{\mu(1-\mu)}λmax(m,ℓ,d)​/m→μd+2μ(1−μ)​, with its lower half (114) and the Gershgorin bound (129).
  7. The algebra (132) and (136)–(137) that produce the closed form.

Significance

The result. Theorem 4.1 makes DQI's performance a closed-form function of two numbers, r/pr/pr/p and ℓ/m\ell/mℓ/m, and moves every question about an instance into coding theory: how large a d⊥d^\perpd⊥ the instance's dual code has, and whether it can be decoded efficiently up to ℓ\ellℓ errors. The OPI advantage claim of the paper, the comparison with Prange's algorithm on max-XORSAT, and the imperfect-decoding bound of Theorem 10.1 all start from this formula. The finite-size identity (131) is also useful on its own: it gives the exact optimum for any instance, not only in the limit.

Formalizing it. The theorem is proved in the paper; to our knowledge no part of it has been machine-checked. A formalization would check the Fourier bookkeeping of §8.2.1 and §9 (normalizations pn−k(mk)\sqrt{p^{n-k}\binom mk}pn−k(km​)​, character sums over Fp\mathbb F_pFp​), the claim that every degree-ℓ\ellℓ DQI state is a combination of the ∣P(k)⟩|P^{(k)}\rangle∣P(k)⟩ and conversely, and the eigenvalue asymptotics of the tridiagonal matrix. Two points of the printed text need care and are stated correctly here: Lemma 9.2 writes its decomposition in the fif_ifi​ where the normalization requires the rescaled gig_igi​, and the "otherwise =1=1=1" branch of Theorem 4.1 is argued only briefly on p. 34.

Difficulty

The algebraic steps are finite but long, and every one carries a normalization that a careless formalization gets wrong. The asymptotic step is the main obstacle. Lemma 9.3 needs a lower bound on λmax⁡\lambda_{\max}λmax​ from a test vector of growing width and a matching upper bound from Gershgorin's theorem, and the upper bound holds only under d≥−(m−2ℓ)/ℓ(m−ℓ)d\ge-(m-2\ell)/\sqrt{\ell(m-\ell)}d≥−(m−2ℓ)/ℓ(m−ℓ)​, which is exactly the regime ρ≤1−μ\rho\le1-\muρ≤1−μ. In the other regime that hypothesis fails and the Gershgorin bound overshoots, so the limit 111 needs a separate argument; the observation that ⟨s⟩opt\langle s\rangle_{\rm opt}⟨s⟩opt​ "increases in rrr", printed on p. 34, does not give it at fixed ppp and rrr. A second difficulty is that ⟨s⟩opt\langle s\rangle_{\rm opt}⟨s⟩opt​ is a supremum over polynomials, while Lemma 9.2 is a statement about weight vectors w\mathbf ww; identifying the two needs both directions of Lemma A.1's correspondence and the normalization of Lemma 9.1.

Formalization scope

All objects live in the namespace DQI.Semicircle and one definitions file. Fp\mathbb F_pFp​ is ZMod p with [Fact p.Prime]; vectors are Fin n → ZMod p; constraints are indexed by Fin m from 000. ωpa=exp⁡(2πi a/p)\omega_p^a=\exp(2\pi i\,a/p)ωpa​=exp(2πia/p) is computed from the representative of aaa in {0,…,p−1}\{0,\dots,p-1\}{0,…,p−1}. Polynomials are real with natDegree ≤ ℓ; weight vectors are real. The optimum ⟨s⟩opt\langle s\rangle_{\rm opt}⟨s⟩opt​ is the real supremum over exactly the normalized polynomials of degree at most ℓ\ellℓ evaluated at f(x)f(\mathbf x)f(x); its set is nonempty (constant polynomials) and bounded by mmm. The dual-distance condition is "every nonzero d\mathbf dd with BTd=0B^T\mathbf d=0BTd=0 has weight >t>t>t"; d⊥d^\perpd⊥ is never an infimum, and m>nm>nm>n (the paper's standing assumption) guarantees a nonzero codeword, so the condition forces 2ℓ<m2\ell<m2ℓ<m. λmax⁡\lambda_{\max}λmax​ is the supremum of the real spectrum. The limit "m→∞m\to\inftym→∞ with ℓ/m\ell/mℓ/m fixed" is any sequence of instances with mj→∞m_j\to\inftymj​→∞ and ℓj/mj→μ\ell_j/m_j\to\muℓj​/mj​→μ, with ppp and rrr fixed along it. Convergence of the ratio includes irrational μ\muμ with integer sizes.

Added hypotheses, all disclosed in the items: Lemma 9.2 decomposes in the gig_igi​ rather than the printed fif_ifi​; (129) assumes ℓ≥1\ell\ge1ℓ≥1 to avoid dividing by 0\sqrt00​; Lemma 9.3 imposes its hypothesis on ddd only when ℓj≥1\ell_j\ge1ℓj​≥1; (114) is stated as a lim inf⁡\liminfliminf with an explicit ε\varepsilonε.

A formalization that replaces ⟨s⟩opt\langle s\rangle_{\rm opt}⟨s⟩opt​ by a supremum over all states (which gives 111), drops "nonzero" from the distance condition (which makes it unsatisfiable), or states the goal at a single mmm is not this theorem and is ruled out by the definitions above.

Needed infrastructure: Fourier analysis on Fpn\mathbb F_p^nFpn​ (character orthogonality, Parseval), elementary symmetric polynomials and their reduction modulo a quadratic, Rayleigh quotients and Gershgorin discs for real symmetric matrices, and elementary limits. The tridiagonal-matrix bounds and the quadratic-reduction lemma are reusable beyond DQI. Proofs of any milestone, alternative arguments for the "otherwise" branch, and sharper finite-mmm bounds on λmax⁡\lambda_{\max}λmax​ are welcome.

Selected references

  • S. P. Jordan, N. Shutty, M. Wootters, A. Zalcman, A. Schmidhuber, R. King, S. V. Isakov, T. Khattar, R. Babbush, Optimization by Decoded Quantum Interferometry, arXiv:2408.08292v5, 2025. https://arxiv.org/abs/2408.08292
  • S. Gershgorin, Über die Abgrenzung der Eigenwerte einer Matrix, Izv. Akad. Nauk SSSR, Ser. Fiz.-Mat. 6, 749–754, 1931.
  • R. G. Gallager, Low-Density Parity-Check Codes, IRE Trans. Inform. Theory 8(1), 21–28, 1962. https://doi.org/10.1109/TIT.1962.1057683
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OptimizationQuantum Information·Captain: mikedeng1

The Sum-of-Squares Hierarchy on the Sphere, and Applications in Quantum Information Theory II: The Dual of the ℓ-th DPS Cone Is the Set of M for Which ‖y‖^{2(ℓ−1)}·p_M Is a Real Sum of SquaresResearch Paper

Motivation

Deciding whether a bipartite quantum state is entangled is a basic computational problem of quantum information theory, and it is NP-hard in general (Gurvits 2003). The most widely used family of tests is the DPS hierarchy of Doherty, Parrilo and Spedalieri (DPS 2002, DPS 2004): a sequence of semidefinite programs, indexed by an integer level ℓ≥1\ell\ge1ℓ≥1, whose feasible sets shrink to the set of separable states. On the dual side, a matrix MMM that is nonnegative on separable states is an entanglement witness, and certifying such witnesses is the problem of certifying nonnegativity of a biquadratic Hermitian form, a classical question in real algebraic geometry.

That the DPS hierarchy is, dually, a sum-of-squares hierarchy for these forms has been used repeatedly in the literature, but, as Fang and Fawzi note (arXiv:1908.05155v1, p. 4), without a formal and complete proof. Their Theorem 12 gives one. They then combine it with their sum-of-squares convergence rate on the sphere (Theorem 2 of the same paper) to recover the O(dB2/ℓ2)O(d_B^2/\ell^2)O(dB2​/ℓ2) convergence rate of Navascués, Owari and Plenio 2009 for the DPS hierarchy.

Timeline:

  • 2002–2004: Doherty, Parrilo, Spedalieri introduce the hierarchy and prove completeness.
  • 2009: Navascués, Owari, Plenio prove hDPSℓ≤(1+O(dB2/ℓ2))hSeph_{\mathrm{DPS}_\ell}\le(1+O(d_B^2/\ell^2))h_{\mathrm{Sep}}hDPSℓ​​≤(1+O(dB2​/ℓ2))hSep​ by a quantum argument.
  • 2019: Fang and Fawzi prove the duality (Theorem 12) and recover the 2009 rate from sums of squares (Theorem 15).

Setting

Let HA=CdA\mathcal H_A=\mathbb C^{d_A}HA​=CdA​ and HB=CdB\mathcal H_B=\mathbb C^{d_B}HB​=CdB​. A matrix MMM on HA⊗HB\mathcal H_A\otimes\mathcal H_BHA​⊗HB​ has entries Mij,klM_{ij,kl}Mij,kl​ (row (i,j)(i,j)(i,j), column (k,l)(k,l)(k,l)); Herm(dAdB)\mathrm{Herm}(d_Ad_B)Herm(dA​dB​) is the space of Hermitian ones.

  • The separable cone SEP\mathcal{SEP}SEP is the set of finite conic combinations ∑ipi(xixi†)⊗(yiyi†)\sum_ip_i(x_ix_i^\dagger)\otimes(y_iy_i^\dagger)∑i​pi​(xi​xi†​)⊗(yi​yi†​), pi≥0p_i\ge0pi​≥0.
  • Fix ℓ≥1\ell\ge1ℓ≥1 and ℓ\ellℓ copies B1,…,BℓB_1,\dots,B_\ellB1​,…,Bℓ​ of HB\mathcal H_BHB​. The DPS cone DPSℓ\mathcal{DPS}_\ellDPSℓ​ is the set of positive semidefinite ρ\rhoρ on HA⊗HB\mathcal H_A\otimes\mathcal H_BHA​⊗HB​ that have a positive semidefinite extension ρAB[ℓ]\rho_{AB[\ell]}ρAB[ℓ]​ on HA⊗HB⊗ℓ\mathcal H_A\otimes\mathcal H_B^{\otimes\ell}HA​⊗HB⊗ℓ​ with three properties: tracing out B2,…,BℓB_2,\dots,B_\ellB2​,…,Bℓ​ returns ρ\rhoρ; (I⊗Πℓ)ρAB[ℓ](I⊗Πℓ)=ρAB[ℓ](I\otimes\Pi_\ell)\rho_{AB[\ell]}(I\otimes\Pi_\ell)=\rho_{AB[\ell]}(I⊗Πℓ​)ρAB[ℓ]​(I⊗Πℓ​)=ρAB[ℓ]​, where Πℓ=1ℓ!∑σ∈SℓPσ\Pi_\ell=\frac1{\ell!}\sum_{\sigma\in\mathfrak S_\ell}P_\sigmaΠℓ​=ℓ!1​∑σ∈Sℓ​​Pσ​ projects onto the symmetric subspace of HB⊗ℓ\mathcal H_B^{\otimes\ell}HB⊗ℓ​; and every partial transpose ρAB[ℓ]TB[s]\rho_{AB[\ell]}^{\mathsf T_{B[s]}}ρAB[ℓ]TB[s]​​ on B1,…,BsB_1,\dots,B_sB1​,…,Bs​, s=1,…,ℓs=1,\dots,\ells=1,…,ℓ, is positive semidefinite.
  • The EXT cone EXTℓ\mathcal{EXT}_\ellEXTℓ​ is the same without the partial-transpose conditions.
  • For a set KKK, the dual cone is K∗={M∈Herm(dAdB):Tr[Mρ]≥0 ∀ρ∈K}K^*=\{M\in\mathrm{Herm}(d_Ad_B):\mathrm{Tr}[M\rho]\ge0\ \forall\rho\in K\}K∗={M∈Herm(dA​dB​):Tr[Mρ]≥0 ∀ρ∈K}.
  • To MMM is attached the Hermitian polynomial pM(x,xˉ,y,yˉ)=∑ijklMij,klxixˉkyjyˉlp_M(x,\bar x,y,\bar y)=\sum_{ijkl}M_{ij,kl}x_i\bar x_ky_j\bar y_lpM​(x,xˉ,y,yˉ​)=∑ijkl​Mij,kl​xi​xˉk​yj​yˉ​l​.
  • A real-valued polynomial in (x,xˉ,y,yˉ)(x,\bar x,y,\bar y)(x,xˉ,y,yˉ​) is rsos if it is a finite sum of squares of Hermitian polynomials, equivalently of real polynomials in the real and imaginary parts of x,yx,yx,y; it is csos if it is a finite sum ∑i∣qi(x,y)∣2\sum_i|q_i(x,y)|^2∑i​∣qi​(x,y)∣2 with qiq_iqi​ holomorphic polynomials.

Formalization targets

Goal: Theorem 12

SEP∗={M:pM≥0},DPSℓ∗={M:∥y∥2(ℓ−1)pM is rsos},EXTℓ∗={M:∥y∥2(ℓ−1)pM is csos},\mathcal{SEP}^*=\{M: p_M\ge0\},\qquad \mathcal{DPS}_\ell^*=\{M:\|y\|^{2(\ell-1)}p_M\ \text{is rsos}\},\qquad \mathcal{EXT}_\ell^*=\{M:\|y\|^{2(\ell-1)}p_M\ \text{is csos}\},SEP∗={M:pM​≥0},DPSℓ∗​={M:∥y∥2(ℓ−1)pM​ is rsos},EXTℓ∗​={M:∥y∥2(ℓ−1)pM​ is csos},

for all dA,dBd_A,d_BdA​,dB​ and all ℓ≥1\ell\ge1ℓ≥1, with MMM ranging over Herm(dAdB)\mathrm{Herm}(d_Ad_B)Herm(dA​dB​).

Milestones

  1. Theorem 12 (i), the first equality.
  2. The identity (37): (x⊗yˉ⊗s⊗y⊗ℓ−s)†W(⋅)=(x⊗y⊗ℓ)†WTB[s](x⊗y⊗ℓ)(x\otimes\bar y^{\otimes s}\otimes y^{\otimes\ell-s})^\dagger W(\cdot)=(x\otimes y^{\otimes\ell})^\dagger W^{\mathsf T_{B[s]}}(x\otimes y^{\otimes\ell})(x⊗yˉ​⊗s⊗y⊗ℓ−s)†W(⋅)=(x⊗y⊗ℓ)†WTB[s]​(x⊗y⊗ℓ).
  3. Lemma 19: ∥y∥2(ℓ−1)pM\|y\|^{2(\ell-1)}p_M∥y∥2(ℓ−1)pM​ is rsos iff it is ∑s=0ℓ(x⊗yˉ⊗s⊗y⊗ℓ−s)†Ws(x⊗yˉ⊗s⊗y⊗ℓ−s)\sum_{s=0}^\ell(x\otimes\bar y^{\otimes s}\otimes y^{\otimes\ell-s})^\dagger W_s(x\otimes\bar y^{\otimes s}\otimes y^{\otimes\ell-s})∑s=0ℓ​(x⊗yˉ​⊗s⊗y⊗ℓ−s)†Ws​(x⊗yˉ​⊗s⊗y⊗ℓ−s) with Ws⪰0W_s\succeq0Ws​⪰0.
  4. (39): (x⊗y⊗ℓ)†(Y−ΠℓYΠℓ)(x⊗y⊗ℓ)=0(x\otimes y^{\otimes\ell})^\dagger(Y-\Pi_\ell Y\Pi_\ell)(x\otimes y^{\otimes\ell})=0(x⊗y⊗ℓ)†(Y−Πℓ​YΠℓ​)(x⊗y⊗ℓ)=0.
  5. The dual SDP description: DPSℓ∗={M:M⊗IB[2:ℓ]=(Y−ΠℓYΠℓ)+∑s=0ℓWsTB[s], Y∈Herm, Ws⪰0}\mathcal{DPS}_\ell^*=\{M: M\otimes I_{B[2:\ell]}=(Y-\Pi_\ell Y\Pi_\ell)+\sum_{s=0}^\ell W_s^{\mathsf T_{B[s]}},\ Y\in\mathrm{Herm},\ W_s\succeq0\}DPSℓ∗​={M:M⊗IB[2:ℓ]​=(Y−Πℓ​YΠℓ​)+∑s=0ℓ​WsTB[s]​​, Y∈Herm, Ws​⪰0}.
  6. Lemma 20: ∥y∥2(ℓ−1)pM\|y\|^{2(\ell-1)}p_M∥y∥2(ℓ−1)pM​ is csos iff it is (x⊗y⊗ℓ)†W(x⊗y⊗ℓ)(x\otimes y^{\otimes\ell})^\dagger W(x\otimes y^{\otimes\ell})(x⊗y⊗ℓ)†W(x⊗y⊗ℓ) with W⪰0W\succeq0W⪰0.
  7. Theorem 15: there are absolute C,C′>0C,C'>0C,C′>0 with hSep(M)≤hDPSℓ(M)≤(1+CdB2/ℓ2)hSep(M)h_{\mathrm{Sep}}(M)\le h_{\mathrm{DPS}_\ell}(M)\le(1+Cd_B^2/\ell^2)h_{\mathrm{Sep}}(M)hSep​(M)≤hDPSℓ​​(M)≤(1+CdB2​/ℓ2)hSep​(M) for ℓ≥C′dB\ell\ge C'd_Bℓ≥C′dB​, whenever (x⊗y)†M(x⊗y)≥0(x\otimes y)^\dagger M(x\otimes y)\ge0(x⊗y)†M(x⊗y)≥0.

Significance

Theorem 12 makes the DPS hierarchy and the sum-of-squares hierarchy for biquadratic forms interchangeable. A convergence bound for one is a convergence bound for the other: the paper uses this to derive the DPS rate (Theorem 15) from a rate for sums of squares on the sphere, and conversely quantum de Finetti arguments give sum-of-squares bounds. Part (iii) separates the two notions of Hermitian sum of squares: dropping the partial transposes corresponds exactly to passing from real to complex sums of squares. This explains, for example, why (z+zˉ)2(z+\bar z)^2(z+zˉ)2 (rsos but not csos) behaves differently in the two hierarchies.

The results are proved on paper; none is formalized. The mission produces a machine-checked statement and proof of the duality, together with the matrix-analytic infrastructure behind it: partial traces and partial transposes on HA⊗HB⊗ℓ\mathcal H_A\otimes\mathcal H_B^{\otimes\ell}HA​⊗HB⊗ℓ​, the symmetric projector, conic duality for semidefinite cones, and the passage between Gram matrices and sums of squares. Theorem 15 additionally depends on the sphere rate of the companion mission (Theorem 6 there) and on the unproved Lemma 13 and display (26) of the paper.

Difficulty

The inclusion of each sum-of-squares cone in the corresponding dual cone is a direct computation. The reverse inclusions are harder: a certificate involving arbitrary Hermitian polynomials must yield positive semidefinite matrices indexed by the prescribed tensor products, even though its square terms can mix different patterns of complex conjugation. Likewise, weak semidefinite duality alone does not show that every element of DPSℓ∗\mathcal{DPS}_\ell^*DPSℓ∗​ has the displayed finite certificate; limits of certificates may require a separate closedness argument. The symmetric-subspace condition adds another constraint because an extension must be supported on that subspace, not merely invariant under permutations.

Formalization scope

  • Indices: HA⊗HB\mathcal H_A\otimes\mathcal H_BHA​⊗HB​ is Fin dA × Fin dB (Mathlib's Kronecker convention); HA⊗HB⊗ℓ\mathcal H_A\otimes\mathcal H_B^{\otimes\ell}HA​⊗HB⊗ℓ​ is Fin dA × (Fin ℓ → Fin dB).
  • The level is written ℓ=m+1\ell=m+1ℓ=m+1 with m∈Nm\in\mathbb Nm∈N, so ℓ≥1\ell\ge1ℓ≥1 is built in and ∥y∥2(ℓ−1)=∥y∥2m\|y\|^{2(\ell-1)}=\|y\|^{2m}∥y∥2(ℓ−1)=∥y∥2m; B1,…,BℓB_1,\dots,B_\ellB1​,…,Bℓ​ are coordinates 0,…,m0,\dots,m0,…,m.
  • Matrices are complex; positive semidefiniteness is Mathlib's Matrix.PosSemidef (which includes Hermitian). Dual cones are subsets of Herm(dAdB)\mathrm{Herm}(d_Ad_B)Herm(dA​dB​) with the pairing Re⁡Tr[Mρ]\operatorname{Re}\mathrm{Tr}[M\rho]ReTr[Mρ].
  • pMp_MpM​ is (25) literally; "pM≥0p_M\ge0pM​≥0" is Re⁡pM≥0\operatorname{Re}p_M\ge0RepM​≥0.
  • rsos is a finite sum of squares of real polynomials (MvPolynomial over R\mathbb RR) in the real and imaginary parts of (x,y)(x,y)(x,y); csos is a finite sum of ∣qi∣2|q_i|^2∣qi​∣2 with qiq_iqi​ complex polynomials in (x,y)(x,y)(x,y) only. Swapping the two, or allowing complex gig_igi​ in rsos, would change parts (ii) and (iii).
  • Condition (21) is stated literally with the explicit projector; "commutes with all permutations" would be weaker and is not used.
  • In Theorem 15, hSeph_{\mathrm{Sep}}hSep​ and hDPSℓh_{\mathrm{DPS}_\ell}hDPSℓ​​ are real suprema over trace-one elements, dA,dB≥1d_A,d_B\ge1dA​,dB​≥1 is assumed so the sets are nonempty, and C,C′C,C'C,C′ are quantified before all dimensions.

No trivializing reading is available: the cones are defined by their page conditions, the dual cones keep the Hermitian constraint, and no degree bound or extra hypothesis is placed on the sums of squares. Welcome contributions include a general library for partial traces and transposes of multipartite matrices, the spanning property of {y⊗ℓ}\{y^{\otimes\ell}\}{y⊗ℓ} in the symmetric subspace, and Gram-matrix characterizations of sums of squares of polynomials; all are reusable well beyond this mission.

Selected references

  • K. Fang, H. Fawzi, The sum-of-squares hierarchy on the sphere, and applications in quantum information theory, arXiv preprint, 2019. https://arxiv.org/abs/1908.05155v1
  • A. C. Doherty, P. A. Parrilo, F. M. Spedalieri, Distinguishing separable and entangled states, Physical Review Letters 88, 187904, 2002. https://arxiv.org/abs/quant-ph/0112007
  • A. C. Doherty, P. A. Parrilo, F. M. Spedalieri, Complete family of separability criteria, Physical Review A 69, 022308, 2004. https://arxiv.org/abs/quant-ph/0308032
  • M. Navascués, M. Owari, M. B. Plenio, Power of symmetric extensions for entanglement detection, Physical Review A 80, 052306, 2009. https://arxiv.org/abs/0906.2731
  • L. Gurvits, Classical deterministic complexity of Edmonds' problem and quantum entanglement, STOC 2003. https://doi.org/10.1145/780542.780545
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