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arXiv:2610.41448

An Unbounded Separation of Almost-Quantum and Commuting-Operator Correlations in Zero-Error Communication

Rafiuddin Gazi, Biswadeep Chatterjee, Jayashree Karmakar, Ram Krishna Patra, Manik Banik, Anandamay Das Bhowmik

quant-phSubmitted Oct 30, 2026• Announced Nov 2, 2026
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Abstract

Almost-quantum correlations form the $\mathtt{1+AB}$ level of the Navascués--Pironio--Acín hierarchy. They strictly contain the quantum set, are characterized by a single semidefinite program, arise in Sorkin's quantum measure theory, and satisfy several principles proposed to single out quantum theory. We show that they are nevertheless unboundedly stronger than quantum correlations in a zero-error communication task. Alice and Bob receive labels $s,t\in[N]$, $N\ge3$; after one bit from Alice, Bob must decide whether $s=t$, never erring but allowed to abstain. For every model of quantum correlations, from finite-dimensional tensor products to commuting operators, the optimal worst-case probability of a conclusive answer is exactly $1/N$, the value attained with shared randomness, so the bound does not depend on the resolution of Tsirelson's problem. An explicit family of almost-quantum correlations attains $1/19$ for every $N$. For certificates of equality from binary-outcome boxes, we solve the underlying semidefinite programs in closed form. The almost-quantum optimum equals $N^2/(17N^2-80N+64)$ for $N\ge8$ and tends to $1/17$. The first level of the hierarchy, which coincides with the set singled out by macroscopic locality, attains $N/[8(N-2)]$, which tends to $1/8$; its optimal boxes lie outside the almost-quantum set for every $N\ge5$. For longer messages, entanglement saves at most one bit over shared randomness, whereas almost-quantum correlations reduce the one-way zero-error cost of deciding equality of $n$-bit strings from $n$ bits to at most $13$. The quantum bound also yields a linear witness of post-quantumness on a face of the nonsignalling polytope.

AI Summary

The paper asks how much almost-quantum (AQ, NPA level $1+AB$) correlations can outperform quantum correlations in zero-error communication. Alice and Bob receive labels $s,t\in[N]$; after one classical bit from Alice, Bob must decide whether $s=t$, allowing abstention but no errors. Performance is the worst-case probability of a conclusive answer. For every $N\ge3$, the optimal efficiency is exactly $1/N$ with shared randomness, entanglement, or commuting-operator correlations. Explicit binary-output AQ boxes instead achieve efficiency $1/19$ for every $N$, giving an unbounded ratio of at least $N/19$. For the restricted problem of certifying equality through a single joint outcome of a binary-output box, the AQ optimum is $1/N$ for $N\le8$ and $N^2/(17N^2-80N+64)$ for $N\ge8$, approaching $1/17$. The corresponding NPA level-1 optimum is $N/[8(N-2)]$ for $N\ge4$, approaching $1/8$. For equality of $n$-bit strings with abstention probability at most $1/2$, one-way classical communication costs exactly $n$ bits with quantum resources, versus at most $13$ with AQ resources. The quantum bounds use sequential-measurement packing and zero-error support constraints, extended to commuting operators. AQ membership is established through explicit Gram-vector constructions; symmetry-reduced semidefinite programs have matching analytic primal and dual certificates. The unrestricted AQ one-bit optimum remains open, as do possible improvements from larger outcome alphabets or message-dependent settings. The separation relies on exact zeros: its associated linear post-quantumness witness applies only on a specified nonsignalling face and establishes neither noise tolerance nor quantitative distance from quantum correlations.

Little sign of AI-generated textAI use disclosed
A large language model (Claude, Anthropic) was used to assist with editing the text, simplifying the analytic certificates in Sections~\ref{sec:aq} and~\ref{sec:vec}.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

Comments
35 pages, single column, 2 figures; comments are welcome

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Almost-quantum correlations form the 1+AB\mathtt{1+AB}1+AB level of the Navascués--Pironio--Acín hierarchy. They strictly contain the quantum set, are characterized by a single semidefinite program, arise in Sorkin's quantum measure theory, and satisfy several principles proposed to single out quantum theory. We show that they are nevertheless unboundedly stronger than quantum correlations in a zero-error communication task. Alice and Bob receive labels s,t∈[N]s,t\in[N]s,t∈[N], N≥3N\ge3N≥3; after one bit from Alice, Bob must decide whether s=ts=ts=t, never erring but allowed to abstain. For every model of quantum correlations, from finite-dimensional tensor products to commuting operators, the optimal worst-case probability of a conclusive answer is exactly 1/N1/N1/N, the value attained with shared randomness, so the bound does not depend on the resolution of Tsirelson's problem. An explicit family of almost-quantum correlations attains 1/191/191/19 for every NNN. For certificates of equality from binary-outcome boxes, we solve the underlying semidefinite programs in closed form. The almost-quantum optimum equals N2/(17N2−80N+64)N^2/(17N^2-80N+64)N2/(17N2−80N+64) for N≥8N\ge8N≥8 and tends to 1/171/171/17. The first level of the hierarchy, which coincides with the set singled out by macroscopic locality, attains N/[8(N−2)]N/[8(N-2)]N/[8(N−2)], which tends to 1/81/81/8; its optimal boxes lie outside the almost-quantum set for every N≥5N\ge5N≥5. For longer messages, entanglement saves at most one bit over shared randomness, whereas almost-quantum correlations reduce the one-way zero-error cost of deciding equality of nnn-bit strings from nnn bits to at most 131313. The quantum bound also yields a linear witness of post-quantumness on a face of the nonsignalling polytope.
The paper asks how much almost-quantum (AQ, NPA level 1+AB1+AB1+AB) correlations can outperform quantum correlations in zero-error communication. Alice and Bob receive labels s,t∈[N]s,t\in[N]s,t∈[N]; after one classical bit from Alice, Bob must decide whether s=ts=ts=t, allowing abstention but no errors. Performance is the worst-case probability of a conclusive answer.
For every N≥3N\ge3N≥3, the optimal efficiency is exactly 1/N1/N1/N with shared randomness, entanglement, or commuting-operator correlations. Explicit binary-output AQ boxes instead achieve efficiency 1/191/191/19 for every NNN, giving an unbounded ratio of at least N/19N/19N/19. For the restricted problem of certifying equality through a single joint outcome of a binary-output box, the AQ optimum is 1/N1/N1/N for N≤8N\le8N≤8 and N2/(17N2−80N+64)N^2/(17N^2-80N+64)N2/(17N2−80N+64) for N≥8N\ge8N≥8, approaching 1/171/171/17. The corresponding NPA level-1 optimum is N/[8(N−2)]N/[8(N-2)]N/[8(N−2)] for N≥4N\ge4N≥4, approaching 1/81/81/8. For equality of nnn-bit strings with abstention probability at most 1/21/21/2, one-way classical communication costs exactly nnn bits with quantum resources, versus at most 131313 with AQ resources.
The quantum bounds use sequential-measurement packing and zero-error support constraints, extended to commuting operators. AQ membership is established through explicit Gram-vector constructions; symmetry-reduced semidefinite programs have matching analytic primal and dual certificates.
The unrestricted AQ one-bit optimum remains open, as do possible improvements from larger outcome alphabets or message-dependent settings. The separation relies on exact zeros: its associated linear post-quantumness witness applies only on a specified nonsignalling face and establishes neither noise tolerance nor quantitative distance from quantum correlations.
Information causality (IC) posits that communicating m classical bits cannot give the receiver access to more than m bits of information about the sender's independent data. Although IC holds in quantum theory and excludes a broad class of supra-quantum correlations, its validity for the almost-quantum set has remained open. This semidefinite relaxation of the quantum set satisfies nontrivial communication complexity, no advantage for non-local computation, macroscopic locality, local orthogonality, and numerical evidence has suggested that it may also satisfy IC. Here we show that almost-quantum correlations violate IC, and do so without bound. Unlike earlier violations of IC, which rely on biased guesses, ours is driven by zero-error certificates: each is rare but never wrong, carries information linear in its probability, and vouches for many of the sender's bits at once. This establishes a sharp dichotomy: either IC is a valid physical principle that excludes these correlations, or any nonsignalling theory realizing them admits no mutual information obeying consistency, data processing and the chain rule. In the latter case, we discuss why the chain rule is the natural property to relinquish, and how this possibility relates to histories-based formulations and to locality defined relative to the state rather than presupposed in a fixed spacetime.
We give exact rational certificates for two results in the bipartite Bell scenario with three two-outcome measurements per party. First, the maximum of the I3322I_{3322}I3322​ (Froissart) functional over the almost-quantum set -- the 1+AB1{+}AB1+AB level of the Navascues-Pironio-Acin (NPA) hierarchy -- is certified to lie between 0.25147088380.25147088380.2514708838 and 0.25147090160.25147090160.2514709016 (width <2×10−8<2\times10^{-8}<2×10−8), in the normalization with classical bound 000 and quantum maximum ≈0.2508754\approx0.2508754≈0.2508754; to our knowledge no value for this landmark had been published. Second, we exhibit a single exact rational behavior T∗T^{*}T∗ carrying certificates in both directions: a rational moment matrix proving T∗T^{*}T∗ almost-quantum, and a rational dual object proving that every NPA level-2 completion of T∗T^{*}T∗ requires slack at least q=4.5934×10−4q=4.5934\times10^{-4}q=4.5934×10−4, so that T∗T^{*}T∗ is not quantum. The strict inclusion Q⊊Q~Q\subsetneq\tilde{Q}Q⊊Q~​ in the minimal three-setting scenario is thereby established end-to-end with no reliance on floating-point computation. Anatomically, the witness is locally quantum: all nine of its 2×22\times22×2 correlator subtables pass the Tsirelson-Landau-Masanes criterion, so its non-quantumness is irreducibly a three-setting phenomenon, concentrated in ordering-dependent pseudo-moments coupling each party's third setting to the other's first two; the level-2 certificate is equivalently an exact sum-of-squares identity that any quantum state values nonnegatively and the witness is forced to value at −q-q−q. The certificates follow the rational rounding-projection-lifting programme recently developed for noncommutative optimization; for NPA moment matrices in canonical form the required projection reduces to a per-moment uniform shift, making certification essentially free at these sizes, and we work the programme in both the feasibility and infeasibility directions on one witness. Machine-checkable certificates and verifiers requiring only the Python standard library accompany the paper. Files in this record: the paper (PDF); exact rational certificates for both theorems (i3322_1AB_certificate.json, i3322_level2_infeasibility_certificate.json); standalone verifiers requiring only the Python 3 standard library (verify_i3322_certificate.py, verify_level2_certificate.py); and the generating scripts (certify_landmark.py, certify_level2.py). See README_ancillary.txt for which artifact proves which theorem and how to run the verifiers. v2: corrects the mechanism attribution in Sec. 5 (anatomy) and adds the archive reference to Data Availability; theorems, certificates, and verifiers unchanged.
Bounding the correlations predicted by quantum theory is an important challenge in quantum information science. Today's leading approach is semidefinite programming relaxations, but existing methods still cannot account for many relevant types of constraints. Here, we propose a semidefinite relaxation methodology that can incorporate a breadth of constraints needed in various quantum correlation problems, thereby generalising the seminal Navascués-Pironio-Acín hierarchy. It yields useful results at reasonable computational cost. We showcase the methodology and its features by using it to address five different quantum information problems. These are (i) entanglement witnessing from imperfect measurement devices, (ii) certifying measurements from fidelity-constrained sources, (iii) computing dimensionality in genuine multi-particle entangled states, (iv) benchmarking dimensionality for state preparation devices, and (v) finding uncertainty relations for nearly anti-commuting observables. These applications reflect both the usefulness and versatility of the methodology, as well as its potential for broader relevance in the field.
The Navascués--Pironio--Acín (NPA) hierarchy gives the standard semidefinite outer approximations to quantum behaviors. Whether \emph{any} finite level can already equal the quantum set has remained open even in the bipartite scenario with two binary measurements per party. We demonstrate that \emph{no finite level} is exact. For the symmetric doubly tilted CHSH functional hα=A0B0+A0B1+A1B0−A1B1+α(A0+B0)h_α=A_0B_0+A_0B_1+A_1B_0-A_1B_1+α(A_0+B_0)hα​=A0​B0​+A0​B1​+A1​B0​−A1​B1​+α(A0​+B0​), set T=1−αT=1-αT=1−α. Its quantum maximum satisfies [ωQ(1−T)−(4−2T)]/T3→4/3[ω_{\rm Q}(1-T)-(4-2T)]/T^3\to4/3[ωQ​(1−T)−(4−2T)]/T3→4/3, whereas every fixed NPA level satisfies [ωL(1−T)−ωQ(1−T)]/T3→+∞[ω_L(1-T)-ω_{\rm Q}(1-T)]/T^3\to+\infty[ωL​(1−T)−ωQ​(1−T)]/T3→+∞. Under the corresponding boundary rescaling, an explicit expectation of the positive operator ωQ(1−t2)I−Htω_{\rm Q}(1-t^2)I-H_tωQ​(1−t2)I−Ht​ converges to the Motzkin polynomial. A bounded fixed-level error would therefore make the Motzkin polynomial plus a nonnegative constant a sum of squares, which is impossible. Consequently, every standard NPA relaxation based on a fixed finite list of words in the measurement projectors strictly contains the complete quantum set, and its nonquantum behaviors accumulate at a local deterministic behavior. Thus, the finite-level exactness of CHSH and all one-sided tilted CHSH maxima does not extend to an exact finite-level description of the complete quantum set in the minimal scenario.
The conditional probabilities achievable by local measurements on a shared quantum state in a Bell scenario form the set of quantum behaviors, whose structure was studied by Tsirelson. In 1993, Tsirelson asked whether this set is semialgebraic, that is, describable by finite Boolean combinations of polynomial equations and inequalities. This question has remained open. We answer it in the negative: with four binary measurements per party, the set of finite-dimensional quantum behaviors, its closure, and the commuting-operator set are all nonsemialgebraic. More strongly, none admits a finite real-analytic description even locally near a particular classical behavior. These results rule out exact finite semidefinite representations and show that no finite level of the Navascués-Pironio-Acín hierarchy characterizes these sets exactly.
We establish optimal quantum-classical separations in communication complexity for search problems. We introduce a total search problem called Pelagic Fourier Fishing and show that it admits an nnn-qubit quantum one-way protocol, whereas every randomized two-way protocol requires Ω(2n)Ω(2^n)Ω(2n) bits of communication. We then introduce a variant of this problem whose solutions can be verified in polynomial time. This variant also admits an nnn-qubit quantum one-way protocol, while every randomized one-way protocol requires Ω(2n)Ω(2^n)Ω(2n) bits of communication. We also construct a family of efficiently verifiable total search problems achieving an nnn versus Ωd(nd)Ω_d(n^d)Ωd​(nd) separation between quantum one-way and randomized one-way communication for every fixed d≥2d \ge 2d≥2. In the quantum protocol, Alice prepares her message using a single unitary from the dddth level of the Clifford hierarchy, and Bob performs a Clifford measurement. This separation is asymptotically optimal under this restriction on Alice's message. For d=2d = 2d=2, Alice's message is a stabilizer state and Bob's measurement is Clifford, so the protocol uses no magic, yet achieves an optimal quadratic quantum advantage. Finally, we discuss how these separations can be adapted to near-term quantum advantage experiments in which the demonstrated advantage is both unconditional and efficiently verifiable.