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arxiv: 2606.31097 · v1 · pith:KWLI6KA5new · submitted 2026-06-30 · 🪐 quant-ph

Generalised Probabilistic Theories

Pith reviewed 2026-07-01 05:51 UTC · model grok-4.3

classification 🪐 quant-ph
keywords generalised probabilistic theoriesconvex frameworkquantum foundationsBell non-localitybox worldgeneralised Hamiltonian mechanicsphase space negativity
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The pith

States in physical theories are represented as real vectors of probabilities, transformations as matrices, and measurements as linear functionals.

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

The paper presents the generalised probabilistic theories framework as an operational description that applies to classical probability theory, quantum theory and theories beyond quantum mechanics. States appear as real vectors whose entries are the probabilities of different measurement outcomes. Transformations act as real matrices that map one state vector to another while preserving the probabilistic structure. Measurement outcomes correspond to real vectors that extract probabilities via inner products with the state vectors. This representation lets the same mathematical language describe local hidden variable models, quantum systems and hypothetical super-quantum correlations such as those in box world.

Core claim

Any physical theory of interest is modelled by a convex set of states given as real vectors, transformations given by real matrices that map the set to itself, and measurement outcomes given by real vectors whose inner product with a state vector equals the probability of that outcome.

What carries the argument

The convex framework in which states form a convex cone inside a real vector space, transformations are linear maps on that space, and effects are dual vectors that yield probabilities.

If this is right

  • Classical probability theory is recovered by taking states to be probability distributions over deterministic outcomes.
  • Quantum theory is recovered by embedding density operators into a real vector space with the Hilbert-Schmidt inner product.
  • Bell non-locality appears as a constraint on the joint probability vectors obtainable from composite systems.
  • Box world realises correlations stronger than quantum theory while remaining inside the same convex framework.
  • Generalised Hamiltonian dynamics can be defined on the discrete state space or on continuous phase space, with negativity of the phase-space function signalling contextuality.

Where Pith is reading between the lines

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

  • The framework supplies a uniform language in which to search for theories that lie between quantum mechanics and box world.
  • Phase-space negativity may serve as a diagnostic for contextuality in theories other than quantum mechanics.
  • Operational constraints such as no-signalling can be imposed directly on the vector representation without reference to Hilbert space.

Load-bearing premise

Every physical theory worth considering admits a representation in which states are convex combinations of real probability vectors and all transformations and measurements act linearly on those vectors.

What would settle it

An experiment on a physical system that produces outcome statistics which cannot be listed as the components of a real vector or whose allowed transformations cannot be expressed as linear maps on such vectors.

read the original abstract

We give an introduction to research associated with the generalised probabilistic theories framework, also known as the convex framework. States are real vectors representing lists of probabilities of measurement outcomes. Convex combinations of the vectors represent probabilistic combinations of different state preparations. Transformations are real matrices. Measurement outcomes are represented by functionals of the states, inner products of the state with a real vector, whose values are the probability of the measurement outcome in question. The framework generalises quantum theory. We describe the operational meaning of the framework, and how the concepts can be defined in terms of cones of states and measurement outcome vectors. We describe how the classical and quantum probability theories are represented in the framework. We describe Bell non-locality and the theory with super-quantum non-locality known as box world. We discuss generalised Hamiltonian mechanics in the discrete case and in continuous phase space, including the role of negativity of the phase space density in contextuality and tunnelling.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 2 minor

Summary. The manuscript provides an introduction to the generalised probabilistic theories (GPT) framework. States are defined as real vectors representing lists of probabilities, transformations as real matrices, and measurement outcomes as dual functionals whose inner products yield probabilities. It explains the operational foundations via cones of states and effects, represents classical and quantum theories within the framework, discusses Bell non-locality and box world, and covers generalised Hamiltonian mechanics in both discrete and continuous phase space, including the significance of negativity for contextuality and tunnelling.

Significance. As a review of an established framework with no new theorems or predictions, the paper's value lies in its potential to serve as an accessible entry point for researchers entering quantum foundations. The coverage of standard examples (classical/quantum representations, box world) and extensions (continuous phase space, negativity) consolidates known material; if the exposition is precise and well-structured, it could usefully support teaching or onboarding without advancing the research frontier.

minor comments (2)
  1. [Abstract] The abstract states that the framework 'generalises quantum theory' but does not explicitly note that quantum theory is recovered as a special case within the convex set; a brief clarification in the introduction would help readers new to the area.
  2. [Introduction (or relevant section on continuous mechanics)] The description of continuous phase space mentions negativity in the context of tunnelling but does not reference specific prior works on Wigner-function negativity or its relation to contextuality; adding one or two key citations would strengthen the review character.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their careful reading and positive assessment of the manuscript as an accessible introduction to the generalised probabilistic theories framework. We are pleased that the referee recommends acceptance and agrees that the paper consolidates known material in a manner suitable for teaching and onboarding new researchers.

Circularity Check

0 steps flagged

No significant circularity; introductory review of established framework

full rationale

The manuscript is an introductory review of the established GPT/convex framework. It defines states as real vectors of probabilities, transformations as real matrices, and measurement outcomes as dual functionals, then describes known examples including classical/quantum theories, box world, and generalised Hamiltonian mechanics. No new theorems, derivations, predictions, or empirical claims are advanced. All content consists of standard operational definitions and reviews of prior results, with no load-bearing steps that reduce by construction to fitted inputs or self-citation chains. The derivation chain is absent because the paper does not claim to derive new results from first principles.

Axiom & Free-Parameter Ledger

0 free parameters · 3 axioms · 0 invented entities

The paper is an expository introduction and does not introduce or derive new free parameters, axioms, or entities; it restates the standard operational assumptions of the GPT framework.

axioms (3)
  • domain assumption States are real vectors representing lists of probabilities of measurement outcomes.
    Stated directly in the abstract as the starting representation.
  • domain assumption Transformations are real matrices.
    Stated directly in the abstract as the representation of state changes.
  • domain assumption Measurement outcomes are represented by functionals of the states via inner products.
    Stated directly in the abstract.

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discussion (0)

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Reference graph

Works this paper leans on

57 extracted references · 9 canonical work pages · 6 internal anchors

  1. [1]

    M ¨uller,Probabilistic theories and reconstructions of quantum theory,SciPost Physics Lecture Notes(2021) 028

    M. M ¨uller,Probabilistic theories and reconstructions of quantum theory,SciPost Physics Lecture Notes(2021) 028

  2. [2]

    Pl ´avala,General probabilistic theories: An introduction,Physics Reports1033(2023) 1

    M. Pl ´avala,General probabilistic theories: An introduction,Physics Reports1033(2023) 1

  3. [3]

    Janotta and H

    P . Janotta and H. Hinrichsen,Generalized probability theories: what determines the structure of quantum theory?,Journal of Physics A: Mathematical and Theoretical47(2014) 323001

  4. [4]

    Barnum and A

    H. Barnum and A. Wilce,Post-classical probability theory, inQuantum Theory: Informational Foundations and Foils, pp. 367–420, Springer (2015)

  5. [5]

    Quantum Theory From Five Reasonable Axioms

    L. Hardy,Quantum theory from five reasonable axioms,arXiv:quant-ph/0101012v4(2001)

  6. [6]

    Why can states and measurement outcomes be represented as vectors?

    P .G. Mana,Why can states and measurement outcomes be represented as vectors?,arXiv preprint quant-ph/0305117(2003)

  7. [7]

    Ludwig,Foundations of Quantum Mechanics I, Texts and Monographs in Physics, Springer-Verlag, Berlin, Heidelberg (1983), 10.1007/978-3-642-86741-4

    G. Ludwig,Foundations of Quantum Mechanics I, Texts and Monographs in Physics, Springer-Verlag, Berlin, Heidelberg (1983), 10.1007/978-3-642-86741-4

  8. [8]

    Barnum, J

    H. Barnum, J. Barrett, M. Leifer and A. Wilce,Generalized no-broadcasting theorem,Phys. Rev. Lett.99(2007) 240501

  9. [9]

    Stueckelberg,Quantum theory in real hilbert space,Helv

    E.C. Stueckelberg,Quantum theory in real hilbert space,Helv. Phys. Acta33(1960) 458

  10. [10]

    Chiribella, G.M

    G. Chiribella, G.M. D’Ariano and P . Perinotti,Informational derivation of quantum theory,Phys. Rev. A84(2011) 012311

  11. [11]

    Masanes and M.P

    L. Masanes and M.P . M¨uller,A derivation of quantum theory from physical requirements,New Journal of Physics13(2011) 063001

  12. [12]

    Daki ´c and ˇC

    B. Daki ´c and ˇC. Brukner,Quantum theory and beyond: Is entanglement special,Deep beauty: understanding the quantum world through mathematical innovation(2011) 365

  13. [13]

    Barnum, M.P

    H. Barnum, M.P . M¨uller and C. Ududec,Higher-order interference and single-system postulates characterizing quantum theory,New Journal of Physics16(2014) 123029

  14. [14]

    Bell and A

    J.S. Bell and A. Aspect,Speakable and Unspeakable in Quantum Mechanics: Collected Papers on Quantum Philosophy, Cambridge University Press, 2 ed. (2004)

  15. [15]

    Bell,On the Einstein Podolsky Rosen paradox,Physics Physique Fizika1(1964) 195

    J.S. Bell,On the Einstein Podolsky Rosen paradox,Physics Physique Fizika1(1964) 195

  16. [16]

    Clauser, M.A

    J.F . Clauser, M.A. Horne, A. Shimony and R.A. Holt,Proposed experiment to test local hidden-variable theories,Phys. Rev. Lett.23(1969) 880

  17. [17]

    Cirel’son,Quantum generalizations of bell’s inequality,Lett

    B.S. Cirel’son,Quantum generalizations of bell’s inequality,Lett. in Mathematical Physics4(1980) 93

  18. [18]

    van de Wetering,An effect-theoretic reconstruction of quantum theory,arXiv e-prints(2018) arXiv:1801.05798 [1801.05798]

    J. van de Wetering,An effect-theoretic reconstruction of quantum theory,arXiv e-prints(2018) arXiv:1801.05798 [1801.05798]

  19. [19]

    Tsirelson,Some results and problems on quantum bell-type inequalities,Hadronic Journal Supplement8(1993) 329

    B.S. Tsirelson,Some results and problems on quantum bell-type inequalities,Hadronic Journal Supplement8(1993) 329

  20. [20]

    Barrett,Information processing in generalized probabilistic theories,Phys

    J. Barrett,Information processing in generalized probabilistic theories,Phys. Rev. A75(2007) 032304

  21. [21]

    Popescu and D

    S. Popescu and D. Rohrlich,Quantum nonlocality as an axiom,Foundations of Physics24(1994) 379

  22. [22]

    Gross, M

    D. Gross, M. M ¨uller, R. Colbeck and O.C. Dahlsten,All reversible dynamics in maximally nonlocal theories are trivial,Phys. Rev. Lett.104 (2010) 080402

  23. [23]

    Branford, O.C.O

    D. Branford, O.C.O. Dahlsten and A.J.P . Garner,On defining the Hamiltonian beyond quantum theory,Foundations of Physics48(2018) 982

  24. [24]

    Pusey,Stabilizer notation for spekkens’ toy theory,Foundations of Physics42(2012) 688

    M.F . Pusey,Stabilizer notation for spekkens’ toy theory,Foundations of Physics42(2012) 688

  25. [25]

    Spekkens,Evidence for the epistemic view of quantum states: A toy theory,Phys

    R.W. Spekkens,Evidence for the epistemic view of quantum states: A toy theory,Phys. Rev. A75(2007) 032110

  26. [26]

    Pl ´avala and M

    M. Pl ´avala and M. Kleinmann,Operational theories in phase space: toy model for the harmonic oscillator,Phys. Rev. Lett.128(2022) 040405

  27. [27]

    Pl ´avala and M

    M. Pl ´avala and M. Kleinmann,Generalized dynamical theories in phase space and the hydrogen atom,arXiv preprint arXiv:2212.12267 (2022)

  28. [28]

    Zachos, D

    C. Zachos, D. Fairlie and T. Curtright,Quantum mechanics in phase space: an overview with selected papers,

  29. [29]

    Jiang, D.R

    L. Jiang, D.R. Terno and O. Dahlsten,Framework for generalized hamiltonian systems through reasonable postulates,Phys. Rev. A109 (2024) 032218

  30. [30]

    Jiang, D.R

    L. Jiang, D.R. Terno and O. Dahlsten,Unification of energy concepts in generalized phase space theories,Phys. Rev. Lett.132(2024) 120201

  31. [31]

    How often is the coordinate of a harmonic oscillator positive?

    B. Tsirelson,How often is the coordinate of a harmonic oscillator positive?,arXiv preprint quant-ph/0611147(2006)

  32. [32]

    Bengtsson and K

    I. Bengtsson and K. ˙Zyczkowski,Geometry of quantum states: an introduction to quantum entanglement, Cambridge University Press (2017)

  33. [33]

    Spekkens,Contextuality for preparations, transformations, and unsharp measurements,Phys

    R.W. Spekkens,Contextuality for preparations, transformations, and unsharp measurements,Phys. Rev. A71(2005)

  34. [34]

    Spekkens,Negativity and contextuality are equivalent notions of nonclassicality,Phys

    R.W. Spekkens,Negativity and contextuality are equivalent notions of nonclassicality,Phys. Rev. Lett.101(2008) 020401

  35. [35]

    Lin and O.C

    Y .L. Lin and O.C. Dahlsten,Necessity of negative wigner function for tunneling,Phys. Rev. A102(2020) 062210

  36. [36]

    Razavy,Quantum theory of tunneling, World Scientific (2013)

    M. Razavy,Quantum theory of tunneling, World Scientific (2013)

  37. [37]

    Marinov and B

    M. Marinov and B. Segev,Quantum tunneling in the wigner representation,Phys. Rev. A54(1996) 4752

  38. [38]

    Kriman, N

    A. Kriman, N. Kluksdahl and D. Ferry,Scattering states and distribution functions for microstructures,Phys. Rev. B36(1987) 5953

  39. [39]

    Barrett,Information processing in generalized probabilistic theories,Phys

    J. Barrett,Information processing in generalized probabilistic theories,Phys. Rev. A.75(2007) 032304

  40. [40]

    Mielnik,Generalized quantum mechanics,Commun

    B. Mielnik,Generalized quantum mechanics,Commun. Math. Phys.37(1974) 221

  41. [41]

    Mueller, J

    M.P . Mueller, J. Oppenheim and O.C. Dahlsten,The black hole information problem beyond quantum theory,Journal of High Energy Physics2012(2012) 1

  42. [42]

    Muller, O.C.O

    M.P . Muller, O.C.O. Dahlsten and V. Vedral,Unifying typical entanglement and coin tossing: on randomization in probabilistic theories, Communications in Mathematical Physics316(2012) 441

  43. [43]

    Short and S

    A.J. Short and S. Wehner,Entropy in general physical theories,New Journal of Physics12(2010) 033023

  44. [44]

    Barnum, J

    H. Barnum, J. Barrett, L.O. Clark, M. Leifer, R. Spekkens, N. Stepanik et al.,Entropy and information causality in general probabilistic theories,New Journal of Physics12(2010) 033024. 52Generalised Probabilistic Theories

  45. [45]

    Better Late than Never: Information Retrieval from Black Holes

    S.L. Braunstein and K. ˙Zyczkowski,Entangled black holes as ciphers of hidden information,arXiv:0907.1190(2009)

  46. [46]

    Quantum state merging and negative information

    M. Horodecki, J. Oppenheim and A. Winter,Quantum state merging and negative information,Comm. Math. Phys.269(2006) 107 [quant-ph/0512247]

  47. [47]

    The mother of all protocols: Restructuring quantum information's family tree

    A. Abeyesinghe, I. Devetak, P . Hayden and A. Winter,The mother of all protocols: Restructuring quantum information’s family tree, quant-ph/0606225

  48. [48]

    Braunstein and A.K

    S.L. Braunstein and A.K. Pati,Quantum information cannot be completely hidden in correlations: Implications for the black-hole information paradox,Phys. Rev. Lett.98(2007) 080502

  49. [49]

    Uhlmann,The ”transition probability” in the state space of a*-algebra,Reports on Mathematical Physics9(1976) 273

    A. Uhlmann,The ”transition probability” in the state space of a*-algebra,Reports on Mathematical Physics9(1976) 273

  50. [50]

    Garner, O.C

    A.J. Garner, O.C. Dahlsten, Y . Nakata, M. Murao and V. Vedral,A framework for phase and interference in generalized probabilistic theories,New Journal of Physics15(2013) 093044

  51. [51]

    Garner,Interferometric computation beyond quantum theory,Foundations of Physics48(2018) 886

    A.J. Garner,Interferometric computation beyond quantum theory,Foundations of Physics48(2018) 886

  52. [52]

    Marinov and B

    M.S. Marinov and B. Segev,Quantum tunneling in the wigner representation,Phys. Rev. A54(1996) 4752

  53. [53]

    Kriman, N.C

    A.M. Kriman, N.C. Kluksdahl and D.K. Ferry,Scattering states and distribution functions for microstructures,Phys. Rev. B36(1987) 5953

  54. [54]

    Roy and A

    C.L. Roy and A. Khan,A general study of tunnelling through multibarrier systems,Physical Status Solidi B176(1993) 101

  55. [55]

    L ¨utkenhaus and S.M

    N. L ¨utkenhaus and S.M. Barnett,Nonclassical effects in phase space,Phys. Rev. A51(1995) 3340

  56. [56]

    Bell,On the problem of hidden variables in quantum mechanics,Reviews of Modern Physics38(1966) 447

    J.S. Bell,On the problem of hidden variables in quantum mechanics,Reviews of Modern Physics38(1966) 447

  57. [57]

    Spekkens,Contextuality for preparations, transformations, and unsharp measurements,Phys

    R.W. Spekkens,Contextuality for preparations, transformations, and unsharp measurements,Phys. Rev. A71(2005) 052108