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Prepare-and-broadcast scenarios activate nonclassicality in resources that remain classical under standard prepare-and-measure or Bell tests.

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2026-06-30 00:29 UTC pith:V4LVFPDO

load-bearing objection The paper sets up a prepare-and-broadcast scenario that activates nonclassicality with multiple measurements per party while collapsing under shared randomness for single measurements.

arxiv 2606.28632 v1 pith:V4LVFPDO submitted 2026-06-26 quant-ph

The Prepare and Broadcast Scenario

classification quant-ph
keywords prepare-and-broadcast scenariononclassicality activationBell inequalitiesquantum correlationsdimension restrictionprepare-and-measurebroadcasting transformationnonsignaling models
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper defines a dimension-restricted prepare-and-broadcast scenario in which a sender prepares a system that undergoes a broadcasting transformation before multiple receivers perform local measurements. It constructs hierarchies of classical, quantum, and nonsignaling correlation sets for this setup and develops methods to certify them via new Bell-like inequalities together with linear and semidefinite programming. When each receiver has only one measurement choice the three hierarchies coincide, but when multiple measurement choices are allowed the sets separate and nonclassical correlations appear that are invisible in ordinary prepare-and-measure or Bell scenarios. This matters because it supplies a concrete way to certify quantum resources that would otherwise be dismissed as classical.

Core claim

The prepare-and-broadcast scenario generalizes prepare-and-measure frameworks by inserting a broadcasting step before local measurements. Hierarchies of correlation sets are characterized, and the classical, quantum, and nonsignaling sets are shown to collapse when each party performs only one measurement. With multiple measurements the sets separate, so that resources admitting classical descriptions in standard settings can produce genuinely nonclassical correlations once the broadcast step is included.

What carries the argument

The dimension-restricted prepare-and-broadcast scenario, in which a prepared system is broadcast before local measurements by multiple receivers.

Load-bearing premise

The broadcasting transformation preserves the dimension restriction and the correlation sets are correctly captured by the defined classical, quantum, and nonsignalling hierarchies without additional hidden assumptions on the broadcast channel.

What would settle it

An explicit quantum state, broadcast map, and set of measurements that produce correlations outside the classical set in the PAB scenario but inside the classical set for the corresponding prepare-and-measure scenario would confirm activation; the absence of any such example after complete enumeration of low-dimensional cases would falsify it.

Watch this falsifier — get emailed when new claim-graph text bears on it.

If this is right

  • New families of Bell-like inequalities become available for certifying nonclassicality in broadcast settings.
  • Linear and semidefinite programming methods can decide membership in the classical, quantum, and nonsignaling sets for concrete correlations.
  • Resources that are classical in prepare-and-measure or Bell scenarios can exhibit nonclassical behavior once a broadcast step is added.
  • The hierarchy of models collapses to a single set whenever each receiver is restricted to one measurement choice.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The activation effect may appear in other network scenarios that combine preparation with shared channels to multiple parties.
  • The same hierarchy techniques could be used to bound the power of broadcast-assisted communication protocols.
  • Experimental tests could focus on low-dimensional states already known to be classical in simpler scenarios but suspected to violate PAB inequalities.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit.

Referee Report

0 major / 3 minor

Summary. The paper introduces the dimension-restricted prepare-and-broadcast (PAB) scenario, in which a sender prepares a system that undergoes a broadcasting transformation before being measured locally by multiple receivers. It constructs explicit hierarchies of classical, quantum, and nonsignalling correlation sets, derives associated Bell-like inequalities together with LP and SDP relaxations for their certification, proves that the hierarchies collapse to a single set under shared randomness when each party performs only one measurement, and demonstrates activation of nonclassicality when multiple measurements per party are allowed, such that resources classical in standard prepare-and-measure or Bell scenarios become nonclassical in the PAB setting.

Significance. If the stated proofs and characterizations hold, the work supplies a new, operationally motivated scenario for studying nonclassicality activation together with concrete computational tools (LP/SDP hierarchies) and explicit collapse/activation theorems. The activation result is a clear strength, as it identifies genuinely nonclassical features invisible in the usual Bell or prepare-and-measure settings; the provision of both analytic proofs and numerical methods is also a positive feature.

minor comments (3)
  1. [Abstract / §4] The abstract states that new families of Bell-like inequalities are derived, yet the main text does not appear to include an explicit example inequality together with its quantum violation and classical bound; adding one concrete inequality (with the corresponding SDP value) in §4 or §5 would strengthen the presentation of the certification methods.
  2. [§3] The definition of the broadcasting map in the dimension-restricted setting (likely around Eq. (3) or the start of §3) should explicitly state whether the output dimension is strictly preserved or allowed to increase; the current wording leaves open whether the restriction is on the input or on each output leg.
  3. [Figure 1 / §2] Figure 1 (or the equivalent diagram of the PAB scenario) would benefit from an explicit label indicating the shared-randomness variable λ and the local measurement choices x_i, to match the notation used in the correlation definitions later in the text.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their positive assessment of the manuscript, the recognition of the activation result as a strength, and the recommendation for minor revision. No major comments were raised in the report.

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The paper introduces the dimension-restricted PAB scenario as a generalization, explicitly defines classical/quantum/nonsignalling correlation sets via standard hierarchies, and derives collapse (under shared randomness, single measurement) and activation results as theorems with SDP/LP certification methods. No self-definitional reductions, fitted inputs renamed as predictions, or load-bearing self-citations appear in the provided abstract or described construction; the activation claim rests on the new scenario's explicit models rather than prior author results or ansatze.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only the abstract is available; no explicit free parameters, axioms, or invented entities can be extracted or audited.

pith-pipeline@v0.9.1-grok · 5669 in / 1068 out tokens · 28843 ms · 2026-06-30T00:29:38.711049+00:00 · methodology

0 comments
read the original abstract

We introduce the dimension-restricted prepare and broadcast (PAB) scenario, which generalizes standard prepare-and-measure frameworks. Here, the system prepared by a sender undergoes a broadcasting transformation before being locally measured by multiple receivers. We develop a hierarchy of classical, quantum, and nonsignalling models describing this scenario, characterize their corresponding correlation sets, and derive new families of Bell-like inequalities together with linear and semidefinite programming methods for their certification. First, assuming shared randomness, we prove that the hierarchy collapses into a single set whenever we consider only one measurement per party. Then, considering multiple possible measurements, we show that PAB scenarios allow the activation of nonclassicality, revealing genuinely nonclassical features in resources that admit classical descriptions in standard prepare-and-measure or Bell settings.

Figures

Figures reproduced from arXiv: 2606.28632 by A. de Oliveira Junior, Mois\'es Alves, Rafael Chaves, Santiago Zamora, Tailan S. Sarubi, Vin\'icius F. Alves.

Figure 1
Figure 1. Figure 1: FIG. 1 [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2 [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3 [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4 [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Critical PAM visibility as a function of the number [PITH_FULL_IMAGE:figures/full_fig_p013_5.png] view at source ↗

discussion (0)

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Reference graph

Works this paper leans on

58 extracted references · 4 canonical work pages · 1 internal anchor

  1. [1]

    ForW (2) CC in Eq. (27), the optimal encoding instead groupsx=0,1 together and isolatesx=2, giving A(0) = 2 2 −2 2 ! ,A (1) = −1−1 1−1 ! ,(51) whose quantum correlator values are 4 √ 2 and 2 √ 2, so that βCQ(W(2) CC)=6 √ 2. E. An SDP approximation for the quantum-quantum broadcasting model We now introduce an SDP relaxation to upper bound lin- ear witness...

  2. [2]

    For the maximally entangled stateρ=|Φ +⟩⟨Φ+|, with|Φ +⟩=2 −1/2(|00⟩+|11⟩), the CHSH threshold isv= 1√ 2 ≃ 0.7071. More generally, for correlation Bell tests with pro- jective measurements, the Werner state does not violate any Bell inequality wheneverv≤ 1 G3 , where 1 G3 ≃0.697 where G3 is Grothendieck’s constant of order three. It is also known that this...

  3. [3]

    J. B. Brask, N. Brunner, J. Pauwels, D. Rusca, and A. Tavakoli, Quantum correlations in prepare-and-measure sce- narios and their semi-device-independent applications (2026), arXiv:2603.23604 [quant-ph]

  4. [4]

    Ambainis, A

    A. Ambainis, A. Nayak, A. Ta-Shma, and U. Vazirani, Dense quantum coding and quantum finite automata, J. ACM49, 496–511 (2002)

  5. [5]

    Nayak, Optimal lower bounds for quantum automata and random access codes, inProc

    A. Nayak, Optimal lower bounds for quantum automata and random access codes, inProc. - Annu. IEEE Symp. Found. Com- put. Sci, FOCS ’99 (IEEE Computer Society, USA, 1999) p. 369

  6. [6]

    Quantum Random Access Codes with Shared Randomness

    A. Ambainis, D. Leung, L. Mancinska, and M. Ozols, Quan- tum random access codes with shared randomness (2009), arXiv:0810.2937 [quant-ph]

  7. [7]

    Pawłowski and M

    M. Pawłowski and M. ˙Zukowski, Entanglement-assisted ran- dom access codes, Phys. Rev. A81, 042326 (2010)

  8. [8]

    Tavakoli, A

    A. Tavakoli, A. Hameedi, B. Marques, and M. Bourennane, Quantum random access codes using singled-level systems, Phys. Rev. Lett.114, 170502 (2015)

  9. [9]

    Moreno, R

    G. Moreno, R. Nery, C. de Gois, R. Rabelo, and R. Chaves, Semi-device-independent certification of entanglement in su- perdense coding, Phys. Rev. A103, 022426 (2021)

  10. [10]

    Tavakoli, J

    A. Tavakoli, J. Pauwels, E. Woodhead, and S. Pironio, Correla- tions in entanglement-assisted prepare-and-measure scenarios, PRX Quantum2, 040357 (2021)

  11. [11]

    Gallego, N

    R. Gallego, N. Brunner, C. Hadley, and A. Ac ´ın, Device- independent tests of classical and quantum dimensions, Phys. Rev. Lett.105, 230501 (2010)

  12. [12]

    Tavakoli, A

    A. Tavakoli, A. A. Abbott, M.-O. Renou, N. Gisin, and N. Brun- ner, Semi-device-independent characterization of multipartite entanglement of states and measurements, Phys. Rev. A98, 052333 (2018)

  13. [13]

    Pauwels, A

    J. Pauwels, A. Tavakoli, E. Woodhead, and S. Pironio, Entan- glement in prepare-and-measure scenarios: many questions, a few answers, New J. Phys24, 063015 (2022)

  14. [14]

    Vieira, C

    C. Vieira, C. de Gois, L. Pollyceno, and R. Rabelo, Interplays between classical and quantum entanglement-assisted commu- nication scenarios, New J. Phys25, 113004 (2023)

  15. [15]

    Zamora, R

    S. Zamora, R. A. Mac ˆedo, T. S. Sarubi, M. Alves, D. Poderini, and R. Chaves, Semi-device-independent nonstabilizerness cer- tification in the prepare-and-measure scenario, Phys. Rev. A 112, 042410 (2025)

  16. [16]

    H.-W. Li, M. Pawłowski, Z.-Q. Yin, G.-C. Guo, and Z.-F. Han, Semi-device-independent randomness certification usingn→1 quantum random access codes, Phys. Rev. A85, 052308 (2012)

  17. [17]

    Lunghi, J

    T. Lunghi, J. B. Brask, C. C. W. Lim, Q. Lavigne, J. Bowles, A. Martin, H. Zbinden, and N. Brunner, Self-testing quantum random number generator, Phys. Rev. Lett.114, 150501 (2015)

  18. [18]

    Passaro, D

    E. Passaro, D. Cavalcanti, P. Skrzypczyk, and A. Ac´ın, Optimal randomness certification in the quantum steering and prepare- and-measure scenarios, New J. Phys17, 113010 (2015)

  19. [19]

    Alves, V

    M. Alves, V . L. Sena, S. Zamora, T. S. Sarubi, A. de Oliveira Ju- nior, A. B. Tacla, and R. Chaves, Semi-device-independent ran- domness certification on discretized continuous-variable plat- forms, Phys. Rev. A113, 042418 (2026)

  20. [20]

    Pawłowski and N

    M. Pawłowski and N. Brunner, Semi-device-independent se- curity of one-way quantum key distribution, Phys. Rev. A84, 010302(R) (2011)

  21. [21]

    E. Woodhead,Imperfections and self testing in prepare-and- measure quantum key distribution, Phd thesis, Universit ´e li- bre de Bruxelles, Facult ´e des Sciences – Physique, Bruxelles (2014)

  22. [22]

    Pawłowski, T

    M. Pawłowski, T. Paterek, D. Kaszlikowski, V . Scarani, A. Win- ter, and M. ˙Zukowski, Information causality as a physical prin- ciple, Nature461, 1101 (2009)

  23. [23]

    T. S. Sarubi, S. Zamora, M. Alves, V . F. Alves, G. M. Viswanathan, and R. Chaves, Detection efficiency bounds in (semi-)device-independent scenarios, Braz. J. Phys56, 136 (2026)

  24. [24]

    Chaves, C

    R. Chaves, C. Majenz, and D. Gross, Information-theoretic im- plications of quantum causal structures, Nat. Commun6, 5766 (2015)

  25. [25]

    Chaves, G

    R. Chaves, G. B. Lemos, and J. Pienaar, Causal modeling the delayed-choice experiment, Phys. Rev. Lett.120, 190401 (2018)

  26. [26]

    Bowles, N

    J. Bowles, N. Brunner, and M. Pawłowski, Testing dimension and nonclassicality in communication networks, Phys. Rev. A 92, 022351 (2015)

  27. [27]

    Mohan, A

    K. Mohan, A. Tavakoli, and N. Brunner, Sequential random access codes and self-testing of quantum measurement instru- ments, New J. Phys21, 083034 (2019)

  28. [28]

    Miklin, J

    N. Miklin, J. J. Borkała, and M. Pawłowski, Semi-device- independent self-testing of unsharp measurements, Phys. Rev. Res.2, 033014 (2020)

  29. [29]

    Munroe, xkcd - a webcomic of romance, sarcasm, math, and language (2025), accessed: 2025-03-06

    R. Munroe, xkcd - a webcomic of romance, sarcasm, math, and language (2025), accessed: 2025-03-06

  30. [30]

    Bowles, F

    J. Bowles, F. Hirsch, and D. Cavalcanti, Single-copy activation of Bell nonlocality via broadcasting of quantum states, Quan- tum5, 499 (2021)

  31. [31]

    Villegas-Aguilar, E

    L. Villegas-Aguilar, E. Polino, F. Ghafari, M. T. Quintino, K. T. Laverick, I. R. Berkman, S. Rogge, L. K. Shalm, N. Tischler, E. G. Cavalcanti, S. Slussarenko, and G. J. Pryde, Nonlocality activation in a photonic quantum network, Nat. Commun15, 3112 (2024)

  32. [32]

    Boghiu, F

    E.-C. Boghiu, F. Hirsch, P.-S. Lin, M. T. Quintino, and J. Bowles, Device-independent and semi-device-independent entanglement certification in broadcast Bell scenarios, SciPost Phys. Core6, 028 (2023)

  33. [33]

    Polino, L

    E. Polino, L. Villegas-Aguilar, D. Poderini, N. Walk, F. Ghafari, M. T. Quintino, A. Lyasota, S. Rogge, R. Chaves, G. J. Pryde, E. G. Cavalcanti, N. Tischler, and S. Slussarenko, Experimental quantum randomness enhanced by a quantum network (2024), 16 arXiv:2412.16973 [quant-ph]

  34. [34]

    Y . Wang, I. W. Primaatmaja, E. Lavie, A. Varvitsiotis, and C. C. W. Lim, Characterising the correlations of prepare-and- measure quantum networks, npj Quantum Information5, 17 (2019)

  35. [35]

    Ioannou, P

    M. Ioannou, P. Sekatski, A. A. Abbott, D. Rosset, J.-D. Ban- cal, and N. Brunner, Receiver-device-independent quantum key distribution protocols, New J. Phys24, 063006 (2022)

  36. [36]

    Y . Jia, F. Guo, Y . Wang, H. Dong, and F. Gao, Characterizing the set of quantum correlations in prepare-and-measure quan- tum multichain-shaped networks, Phys. Rev. A111, 022439 (2025)

  37. [37]

    Navascu ´es, S

    M. Navascu ´es, S. Pironio, and A. Ac ´ın, Bounding the set of quantum correlations, Phys. Rev. Lett.98, 010401 (2007)

  38. [38]

    Pauwels, S

    J. Pauwels, S. Pironio, E. Woodhead, and A. Tavakoli, Almost qudits in the prepare-and-measure scenario, Phys. Rev. Lett. 129, 250504 (2022)

  39. [39]

    Van Himbeeck, E

    T. Van Himbeeck, E. Woodhead, N. J. Cerf, R. Garc ´ıa-Patr´on, and S. Pironio, Semi-device-independent framework based on natural physical assumptions, Quantum1, 33 (2017)

  40. [40]

    Chaves, J

    R. Chaves, J. B. Brask, and N. Brunner, Device-independent tests of entropy, Phys. Rev. Lett.115, 110501 (2015)

  41. [41]

    Tavakoli, E

    A. Tavakoli, E. Zambrini Cruzeiro, J. Bohr Brask, N. Gisin, and N. Brunner, Informationally restricted quantum correla- tions, Quantum4, 332 (2020)

  42. [42]

    Tavakoli, Semi-device-independent framework based on restricted distrust in prepare-and-measure experiments, Phys

    A. Tavakoli, Semi-device-independent framework based on restricted distrust in prepare-and-measure experiments, Phys. Rev. Lett.126, 210503 (2021)

  43. [43]

    Navascu ´es and T

    M. Navascu ´es and T. V ´ertesi, Bounding the set of finite di- mensional quantum correlations, Phys. Rev. Lett.115, 020501 (2015)

  44. [44]

    Navascu ´es, A

    M. Navascu ´es, A. Feix, M. Ara ´ujo, and T. V ´ertesi, Character- izing finite-dimensional quantum behavior, Phys. Rev. A92, 042117 (2015)

  45. [45]

    P. E. Frenkel and M. Weiner, Classical information storage in ann-level quantum system, Commun. Math. Phys340, 563 (2015)

  46. [46]

    D. Avis, K. Fukuda, and S. Picozzi, On canonical representa- tions of convex polyhedra, inMathematical software(World Scientific, 2002) pp. 350–360

  47. [47]

    Sarubi, The prepare-and-broadcast scenario – numerical codes (2025)

    T. Sarubi, The prepare-and-broadcast scenario – numerical codes (2025)

  48. [48]

    Navascu ´es, S

    M. Navascu ´es, S. Pironio, and A. Ac ´ın, A convergent hierar- chy of semidefinite programs characterizing the set of quantum correlations, New J. Phys10, 073013 (2008)

  49. [49]

    W. F. Stinespring, Positive functions on C*-algebras, Proc. Amer. Math. Soc6, 211 (1955)

  50. [50]

    M. A. Naimark, Spectral functions of a symmetric operator, Izvestiya Akademii Nauk SSSR, Seriya Matematicheskaya4, 277 (1940)

  51. [51]

    Svegborn and A

    E. Svegborn and A. Tavakoli, Entanglement in prepare- and-measure scenarios without receiver inputs (2026), arXiv:2603.29625 [quant-ph]

  52. [52]

    Palazuelos, Superactivation of quantum nonlocality, Phys

    C. Palazuelos, Superactivation of quantum nonlocality, Phys. Rev. Lett.109, 190401 (2012)

  53. [53]

    Cavalcanti, M

    D. Cavalcanti, M. L. Almeida, V . Scarani, and A. Ac´ın, Quan- tum networks reveal quantum nonlocality, Nat. Commun2, 184 (2011)

  54. [54]

    de Gois, G

    C. de Gois, G. Moreno, R. Nery, S. Brito, R. Chaves, and R. Ra- belo, General method for classicality certification in the prepare and measure scenario, PRX Quantum2, 030311 (2021)

  55. [55]

    M. J. Renner, A. Tavakoli, and M. T. Quintino, Classical cost of transmitting a qubit, Phys. Rev. Lett.130, 120801 (2023). Appendix A: Optimal configurations The configurations below specify explicit quantum strate- gies attaining the values reported in Table II. In all cases, the optimization is performed over pure qubit preparations, di- chotomic projec...

  56. [56]

    (26), we obtain (W (1) CC)Q = 12.944

    Configuration forW (1) CC For the inequalityW (1) CC in Eq. (26), we obtain (W (1) CC)Q = 12.944. One strategy attaining this value is ⃗r0 =(−0.478199,−0.107883,−0.871600), ⃗r1 =(+0.250024,+0.932540,+0.260494), ⃗r2 =(+0.254570,−0.726206,+0.638607), ⃗b0 =(−0.082521,+0.038075,+0.995862), ⃗b1 =(−0.173429,−0.984571,+0.023272), ⃗c0 =(−0.548986,−0.011222,−0.835...

  57. [57]

    (27), the optimized value is (W(2) CC)Q =10.828

    Configuration forW (2) CC For the inequalityW (2) CC in Eq. (27), the optimized value is (W(2) CC)Q =10.828. A corresponding numerical strategy is ⃗r0 =(+0.346743,−0.937953,−0.003529), ⃗r1 =(−0.002956,+0.002670,−0.999992), ⃗r2 =(−0.243094,+0.661345,+0.709597), ⃗b0 =(−0.617353,−0.151021,−0.772054), ⃗b1 =(+0.562743,+0.601009,−0.567546), ⃗c0 =(+0.628887,+0.4...

  58. [58]

    (36), we find (W (3) CNS)Q = 5.196

    Configuration forW (3) CNS For the inequalityW (3) CNS in Eq. (36), we find (W (3) CNS)Q = 5.196. One configuration realizing this value is ⃗r0 =(+0.866026,+0.000000,−0.500000), ⃗r1 =(+0.000000,+0.000000,+1.000000), ⃗r2 =(−0.866025,+0.000000,−0.500000), ⃗b0 =(−0.206988,+0.940398,+0.269828), ⃗b1 =(−0.702801,−0.707550,+0.073780), ⃗c0 =(−0.439119,−0.242599,+...