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arxiv: 2603.11900 · v2 · submitted 2026-03-12 · 🪐 quant-ph

Recognition: 2 theorem links

· Lean Theorem

Existence as Distinguishability: Quantum Mechanics from Finite Graded Equality

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Pith reviewed 2026-05-15 12:20 UTC · model grok-4.3

classification 🪐 quant-ph
keywords distinguishabilityquantum mechanicsBorn rulefinite dimensionalself-referential consistencycomplex projective spaceindeterminismunitary dynamics
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The pith

Existence as distinguishability derives quantum mechanics on complex projective space for each finite capacity N at least 3.

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

The paper derives finite-dimensional quantum mechanics from the principle that existence is constituted by distinguishability together with finite capacity N and self-referential consistency. Self-referential consistency expands into eight structural conditions whose final member, structural unambiguity, forces the graded kernel K equal to one minus the squared overlap. This kernel is realized uniquely on complex projective space of dimension N minus one, from which complex coefficients, the Born rule, unitary dynamics and tensor-product composition are obtained as direct consequences. Indeterminism appears automatically once the number of outcomes exceeds the finite capacity. A sympathetic reader cares because the derivation starts from an operational distinction principle rather than from Hilbert-space axioms or probability postulates.

Core claim

For each N greater than or equal to 3 the unique distinguishability space is the complex projective space of dimension N minus one equipped with the kernel K of psi and phi equal to one minus the squared modulus of their inner product. A state is identified with the profile of its distinguishability values against every other state. Complex coefficients supply the coordinates that realize this kernel, the Born rule supplies probabilities as squared moduli, dynamics must be unitary to preserve the kernel, and composite systems are formed by tensor product so that the distinguishability grading is preserved. Finite capacity forces indeterminism through overflow, while the usual quantum theory

What carries the argument

The graded distinguishability kernel K taking values in the unit interval, together with the self-referential consistency closure schema that enforces structural unambiguity and selects the geometry.

If this is right

  • Complex coefficients appear as the natural coordinates realizing the kernel on projective space.
  • Probabilities must be given by the Born rule as squared moduli to close the structure consistently.
  • Time evolution is restricted to unitary maps that leave the distinguishability kernel invariant.
  • Composite systems compose via the tensor product to keep the grading of distinguishability intact.
  • Indeterminism is required for any finite N because capacity overflow prevents deterministic assignment of outcomes.

Where Pith is reading between the lines

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

  • Indeterminism receives a direct information-capacity explanation rather than being introduced by a separate measurement postulate.
  • Hidden-variable theories can be classified according to whether they satisfy or violate the self-referential consistency conditions.
  • Finite-N models may be tested in resource-limited quantum devices where the effective number of distinguishable states is bounded.
  • The same distinguishability principle could be applied to continuous or field-theoretic settings to constrain possible extensions.

Load-bearing premise

Self-referential consistency is the correct closure needed to turn the distinguishability principle into a structurally unambiguous theory.

What would settle it

An explicit construction, for some N at least 3, of a different finite geometry or kernel that satisfies all eight conditions derived from self-referential consistency would falsify uniqueness.

Figures

Figures reproduced from arXiv: 2603.11900 by Julian G. Zilly.

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_p002_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3 [PITH_FULL_IMAGE:figures/full_fig_p014_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4 [PITH_FULL_IMAGE:figures/full_fig_p014_4.png] view at source ↗
read the original abstract

We derive finite-dimensional quantum mechanics from a single ontological principle, that \emph{existence is constituted by distinguishability}, together with two structural commitments: finite capacity $N$ (parametric input) and self-referential consistency (SRC, a closure schema with two equivalent forms, operational and information-theoretic). SRC unpacks into eight derived structural conditions; structural unambiguity (S5) completes the hierarchy, uniquely selecting the Born rule as the geometric/probabilistic closure. The graded distinguishability kernel $K(x,y) \in [0,1]$ realises both axioms, with a state constituted by its $K$-profile against all others. For each $N \geq 3$, the unique distinguishability space is $(\mathbb{C} P^{N-1}, K)$ with $K(\psi,\phi) = 1 - |\langle\psi|\phi\rangle|^2$, from which complex coefficients, the Born rule $p_k = |c_k|^2$, unitary dynamics, and tensor-product composition all follow. Indeterminism is forced by capacity overflow; alternatives (e.g. Bohmian mechanics) are classified rather than refuted. Standard QM is the $N \to \infty$ limit; finite $N$ is the only free parameter. The algebraic spine is machine-checked in Lean 4 modulo five imported classical theorems and the existence direction of Stone's theorem; the Appendix states the verification scope.

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

2 major / 2 minor

Summary. The paper derives finite-dimensional quantum mechanics from the single ontological principle that existence is constituted by distinguishability, together with finite capacity N (a free parameter) and self-referential consistency (SRC), a closure schema presented in operational and information-theoretic forms. SRC unpacks into eight structural conditions; structural unambiguity (S5) selects the Born rule as geometric closure. For each N ≥ 3 the unique distinguishability space is (ℂP^{N-1}, K) with K(ψ,ϕ) = 1 − |⟨ψ|ϕ⟩|^2, from which complex coefficients, p_k = |c_k|^2, unitary dynamics, and tensor-product composition follow. Indeterminism arises from capacity overflow; the algebraic spine is machine-checked in Lean 4 modulo five classical theorems and the existence direction of Stone's theorem.

Significance. If the SRC schema can be shown to be the minimal, non-circular closure entailed by distinguishability alone, the result would be a significant foundational derivation of QM structures (including the Born rule and complex Hilbert space geometry) from an ontological starting point, with the formal verification providing additional rigor. The classification of alternatives and the identification of finite N as the sole parameter are also noteworthy strengths. The current presentation, however, leaves open whether SRC is independently required or selected to yield the target space.

major comments (2)
  1. [SRC definition and unpacking (operational and information-theoretic forms)] The central uniqueness claim for (ℂP^{N-1}, K) with K(ψ,ϕ)=1−|⟨ψ|ϕ⟩|^2 rests on SRC unpacking into the eight conditions S1–S8, with S5 (structural unambiguity) enforcing the Born rule. The manuscript presents SRC as required by the distinguishability principle, yet provides no independent derivation showing these exact eight conditions are the minimal consequences of “existence constituted by distinguishability” without reference to the target features (linearity, complex scalars, inner-product geometry). This makes the derivation conditional on the choice of SRC rather than a direct consequence of the ontological axiom.
  2. [Appendix on Lean verification] The paper states that the algebraic spine is machine-checked in Lean 4 modulo five imported classical theorems and the existence direction of Stone's theorem. The verification scope should be stated more precisely: which specific lemmas establishing uniqueness of the distinguishability space (e.g., the step from the eight conditions to the complex projective geometry) are covered by the formalization, and which remain interpretive.
minor comments (2)
  1. [Definition of K] Notation for the graded kernel K(x,y) ∈ [0,1] is introduced without an explicit contrast to the standard overlap |⟨ψ|ϕ⟩|^2; a short comparison table would clarify the geometric meaning.
  2. [N → ∞ limit paragraph] The claim that standard QM is recovered in the N → ∞ limit is stated but not derived in detail; a brief sketch of how the finite-N structures converge would strengthen the presentation.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments, which help clarify the presentation of our derivation. We address each major comment below and indicate the revisions we will make.

read point-by-point responses
  1. Referee: [SRC definition and unpacking (operational and information-theoretic forms)] The central uniqueness claim for (ℂP^{N-1}, K) with K(ψ,ϕ)=1−|⟨ψ|ϕ⟩|^2 rests on SRC unpacking into the eight conditions S1–S8, with S5 (structural unambiguity) enforcing the Born rule. The manuscript presents SRC as required by the distinguishability principle, yet provides no independent derivation showing these exact eight conditions are the minimal consequences of “existence constituted by distinguishability” without reference to the target features (linearity, complex scalars, inner-product geometry). This makes the derivation conditional on the choice of SRC rather than a direct consequence of the ontological axiom.

    Authors: We agree that the independence of the SRC conditions from the target structure merits explicit emphasis. In the manuscript, the operational form of SRC is derived directly from the ontological principle that existence is constituted by distinguishability (any two distinct states must admit a distinguishing measurement) together with finite capacity, while the information-theoretic form follows from the requirement that the distinguishability kernel be closed under self-reference. The eight conditions S1–S8 are presented as the minimal unpacking of this closure in Section 3. To address the concern that the choice may appear tailored, we will add a new subsection (3.1) that derives each condition step-by-step from the ontological axiom and finite capacity alone, without presupposing linearity or inner-product geometry. This will make the non-circular character of the derivation clearer while preserving the existing formal structure. revision: partial

  2. Referee: [Appendix on Lean verification] The paper states that the algebraic spine is machine-checked in Lean 4 modulo five imported classical theorems and the existence direction of Stone's theorem. The verification scope should be stated more precisely: which specific lemmas establishing uniqueness of the distinguishability space (e.g., the step from the eight conditions to the complex projective geometry) are covered by the formalization, and which remain interpretive.

    Authors: We accept this recommendation. The current Appendix already notes that the algebraic spine is verified modulo five classical theorems and the existence direction of Stone's theorem, but we will expand it with an explicit table listing each lemma in the uniqueness proof (from the eight SRC conditions through the classification of the distinguishability space as (ℂP^{N-1}, K)) and indicating which steps are formally checked in Lean 4 versus those that rely on the imported theorems or interpretive steps. This will be included in the revised Appendix. revision: yes

Circularity Check

1 steps flagged

SRC closure schema selects Born rule by construction via its own unpacking conditions

specific steps
  1. self definitional [Abstract (SRC definition and unpacking)]
    "together with two structural commitments: finite capacity N (parametric input) and self-referential consistency (SRC, a closure schema with two equivalent forms, operational and information-theoretic). SRC unpacks into eight derived structural conditions; structural unambiguity (S5) completes the hierarchy, uniquely selecting the Born rule as the geometric/probabilistic closure."

    SRC is posited as required by the ontological principle, yet its unpacking is defined to produce exactly the eight conditions whose final step (S5) forces selection of the Born rule and CP^{N-1} geometry. The 'uniqueness' therefore reduces to the schema being constructed to close on the target structure, with no independent derivation shown that these precise conditions are the minimal entailment of distinguishability without reference to the desired Hilbert-space features.

full rationale

The derivation claims uniqueness of (ℂP^{N-1}, K) with K=1−|⟨ψ|ϕ⟩|^2 from the single principle 'existence is constituted by distinguishability' plus finite N and SRC. However, SRC is introduced as a closure schema whose operational unpacking directly yields eight structural conditions (S1–S8), with S5 (structural unambiguity) explicitly completing the hierarchy to select the Born rule as geometric closure. This makes the central uniqueness claim conditional on a schema whose form is defined to enforce consistency with the target probabilistic structure, reducing the step from distinguishability alone to a self-consistent choice of closure rather than an independent derivation. The algebraic spine is machine-checked, but the load-bearing ontological step remains internal to the SRC definition.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The derivation rests on one free parameter N (finite capacity) and two core axioms: the ontological principle that existence is constituted by distinguishability, and the self-referential consistency closure. No new physical entities are postulated beyond the graded kernel K, which is derived rather than invented.

free parameters (1)
  • N
    Finite capacity of the distinguishability space; the sole parametric input, with standard QM recovered only as N → ∞.
axioms (2)
  • domain assumption Existence is constituted by distinguishability
    Single ontological principle stated as the starting point.
  • ad hoc to paper Self-referential consistency (SRC)
    Closure schema with operational and information-theoretic forms that unpacks into the eight structural conditions.

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Reference graph

Works this paper leans on

66 extracted references · 66 canonical work pages · 6 internal anchors

  1. [1]

    The closed-N= 2case and laboratory qubits The cyclic-dynamics field selection (Lemma 35) and the per-component Born ODE (Lemma 52) both require N≥3, so the framework’s behaviour atN= 2 deserves a unified statement.(i) Derived atN= 2:for a strictly closed two-state system the coefficient field isR, the sym- metry group isO(2), the state space isRP 1 ∼= S1,...

  2. [2]

    given Saturation

    (Fubini–Study uniqueness via Kobayashi–Nomizu [20]); the present Section re-derives it within the graded- equality framework via the per-component ODE form (Lemma 52). Theorem 48(The Fubini-Study Metric from Distin- guishability).The distinguishability kernelKinduces a Riemannian metric on the state space. For infinitesi- mally separated states|ψ⟩and|ψ+dψ...

  3. [3]

    quantumness

    log2 N−O(logM); anyλwithK(λ)>log 2 Nvio- lates Axiom 1. Where the fullN+ 1MUBs are unsettled (compositeN), the three-MUB case of Lemma 71(a) or the KS bound suffices. Proof of Theorem 69.Available storage is log 2 Nbits. Required storage exceeds this by Lemma 70 (univer- salN≥3) and by Lemma 71(a),(b) (M≥3 MUBs, combinatorial and Kolmogorov routes giving ...

  4. [4]

    it from bit

    withK A(ai, a′ i) =x i and aB-pair withK B =y; then the joint pairs areK AB- equal yet haveK A-distinguishableA-marginals (since x1 ̸=x 2). Operational Completeness (Theorem 7(O)) re- quires every distinction at theA-margin to be registered inK AB once aB-context fully resolves theA-channel; withy∈(0,1) theB-channel is non-trivial but does not collapse th...

  5. [5]

    is interpretive; here the relational reading is given an ontological basis (K-profilesarestates) and the Hilbert space formalism is derived. H¨ ohn [53] is the closest structural cousin: Limited Information maps onto Ax- iom 1, Complementarity onto the cyclic-dynamics con- sequences; the present contribution takes a graded ker- nel as primitive, derives I...

  6. [6]

    Existence as Distinguishability: Quantum Mechanics from Finite Graded Equality

    assume aC ∗-algebraic framework and do not address indeterminism. Born-rule, GPT, and discrete cousins.Galley– Masanes [10] and Selby–Scandolo–Coecke [9] assume op- erational probabilities; Zurek’s envariance [56] derives Born from local-unitary symmetry, complementary to the metric-compatibility route here. (X, K) maps onto the GPT framework [11] viae k(...

  7. [7]

    The logic of quantum mechanics,

    G. Birkhoff and J. von Neumann, “The logic of quantum mechanics,” Ann. Math.37, 823 (1936)

  8. [8]

    Quantum Theory From Five Reasonable Axioms

    L. Hardy, “Quantum theory from five reasonable ax- ioms,” arXiv:quant-ph/0101012 (2001)

  9. [9]

    Infor- mational derivation of quantum theory,

    G. Chiribella, G. M. D’Ariano, and P. Perinotti, “Infor- mational derivation of quantum theory,” Phys. Rev. A 84, 012311 (2011)

  10. [10]

    A derivation of quantum theory from physical requirements,

    L. Masanes and M. P. M¨ uller, “A derivation of quantum theory from physical requirements,” New J. Phys.13, 063001 (2011)

  11. [11]

    Quantum Theory and Beyond: Is Entanglement Special?

    B. Daki´ c andˇC. Brukner, “Quantum theory and beyond: Is entanglement special?,” inDeep Beauty: Understand- ing the Quantum World through Mathematical Innova- tion, ed. H. Halvorson (Cambridge Univ. Press, 2011), pp. 365–392; arXiv:0911.0695

  12. [12]

    Characterizing quantum theory in terms of information-theoretic con- straints,

    R. Clifton, J. Bub, and H. Halvorson, “Characterizing quantum theory in terms of information-theoretic con- straints,” Found. Phys.33, 1561 (2003)

  13. [13]

    Law without law: from observer states to physics via algorithmic information theory,

    M. P. M¨ uller, “Law without law: from observer states to physics via algorithmic information theory,” Quantum4, 301 (2020)

  14. [14]

    Trin- ity of relational quantum dynamics,

    P. A. H¨ ohn, A. R. H. Smith, and M. P. E. Lock, “Trin- ity of relational quantum dynamics,” Phys. Rev. D104, 066001 (2021)

  15. [15]

    Re- constructing quantum theory from diagrammatic postu- lates,

    J. H. Selby, C. M. Scandolo, and B. Coecke, “Re- constructing quantum theory from diagrammatic postu- lates,” Quantum5, 445 (2021)

  16. [16]

    Classification of all alter- natives to the Born rule in terms of informational prop- erties,

    T. D. Galley and L. Masanes, “Classification of all alter- natives to the Born rule in terms of informational prop- erties,” Quantum1, 15 (2017)

  17. [17]

    Post-Classical Probability Theory

    H. Barnum and A. Wilce, “Post-classical probability theory,” inQuantum Theory: Informational Founda- tions and Foils, eds. G. Chiribella and R. W. Spekkens (Springer, 2016), arXiv:1205.3833

  18. [18]

    E. M. Alfsen and F. W. Shultz,Geometry of State Spaces of Operator Algebras(Birkh¨ auser, 2003)

  19. [19]

    The problem of hidden variables in quantum mechanics,

    S. Kochen and E. P. Specker, “The problem of hidden variables in quantum mechanics,” J. Math. Mech.17, 59–87 (1967). 28

  20. [20]

    Simple test for hidden variables in spin-1 sys- tems,

    A. A. Klyachko, M. A. Can, S. Binicio˘ glu, and A. S. Shu- movsky, “Simple test for hidden variables in spin-1 sys- tems,” Phys. Rev. Lett.101, 020403 (2008)

  21. [21]

    Experimentally testable state-independent quantum contextuality,

    A. Cabello, “Experimentally testable state-independent quantum contextuality,” Phys. Rev. Lett.101, 210401 (2008); A. Cabello, S. Severini, and A. Winter, “Graph- theoretic approach to quantum correlations,” Phys. Rev. Lett.112, 040401 (2014)

  22. [22]

    A theory of program size formally identi- cal to information theory,

    G. J. Chaitin, “A theory of program size formally identi- cal to information theory,” J. ACM22, 329–340 (1975)

  23. [23]

    Three approaches to the quantita- tive definition of information,

    A. N. Kolmogorov, “Three approaches to the quantita- tive definition of information,” Probl. Inform. Transm.1, 1 (1965)

  24. [24]

    Black holes and entropy,

    J. D. Bekenstein, “Black holes and entropy,” Phys. Rev. D7, 2333–2346 (1973)

  25. [25]

    Measures on the closed subspaces of a Hilbert space,

    A. M. Gleason, “Measures on the closed subspaces of a Hilbert space,” J. Math. Mech.6, 885–893 (1957)

  26. [26]

    Kobayashi and K

    S. Kobayashi and K. Nomizu,Foundations of Differential Geometry, Vol. II (Wiley, 1969)

  27. [27]

    E. P. Wigner,Gruppentheorie und ihre Anwendung auf die Quantenmechanik der Atomspektren(Vieweg, 1931). English translation:Group Theory(Academic Press, 1959)

  28. [28]

    Note on Wigner’s theorem on symmetry operations,

    V. Bargmann, “Note on Wigner’s theorem on symmetry operations,” J. Math. Phys.5, 862–868 (1964)

  29. [29]

    Reed and B

    M. Reed and B. Simon,Methods of Modern Mathematical Physics I: Functional Analysis(Academic Press, 1980)

  30. [30]

    Communication in the presence of noise,

    C. E. Shannon, “Communication in the presence of noise,” Proc. IRE37, 10–21 (1949)

  31. [31]

    Relational quantum mechanics,

    C. Rovelli, “Relational quantum mechanics,” Int. J. Theor. Phys.35, 1637–1678 (1996); arXiv:quant- ph/9609002

  32. [32]

    Evolution without evo- lution: Dynamics described by stationary observables,

    D. N. Page and W. K. Wootters, “Evolution without evo- lution: Dynamics described by stationary observables,” Phys. Rev. D27, 2885–2892 (1983)

  33. [33]

    Quantum Darwinism,

    W. H. Zurek, “Quantum Darwinism,” Nature Phys.5, 181 (2009)

  34. [34]

    Decoherence, einselection, and the quan- tum origins of the classical,

    W. H. Zurek, “Decoherence, einselection, and the quan- tum origins of the classical,” Rev. Mod. Phys.75, 715 (2003)

  35. [35]

    Generalized entropic uncertainty relations,

    H. Maassen and J. B. M. Uffink, “Generalized entropic uncertainty relations,” Phys. Rev. Lett.60, 1103 (1988)

  36. [36]

    Acz´ el,Lectures on Functional Equations and Their Ap- plications(Academic Press, 1966)

    J. Acz´ el,Lectures on Functional Equations and Their Ap- plications(Academic Press, 1966)

  37. [37]

    E. P. Klement, R. Mesiar, and E. Pap,Triangular Norms (Kluwer/Springer, 2000)

  38. [38]

    Schweizer and A

    B. Schweizer and A. Sklar,Probabilistic Metric Spaces (North-Holland, 1983)

  39. [39]

    Local tomography and the Jordan structure of quantum theory,

    H. Barnum and A. Wilce, “Local tomography and the Jordan structure of quantum theory,” Found. Phys.44, 192 (2014)

  40. [40]

    Pitowsky,Quantum Probability—Quantum Logic (Springer, 1989)

    I. Pitowsky,Quantum Probability—Quantum Logic (Springer, 1989)

  41. [41]

    An intro- duction to QBism with an application to the locality of quantum mechanics,

    C. A. Fuchs, N. D. Mermin, and R. Schack, “An intro- duction to QBism with an application to the locality of quantum mechanics,” Am. J. Phys.82, 749 (2014)

  42. [42]

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

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

  43. [43]

    On the reality of the quantum state,

    M. F. Pusey, J. Barrett, and T. Rudolph, “On the reality of the quantum state,” Nat. Phys.8, 475 (2012)

  44. [44]

    On SIC-POVMs and MUBs in Dimension 6

    M. Grassl, “On SIC-POVMs and MUBs in dimension 6,” arXiv:quant-ph/0406175 (2004)

  45. [45]

    Prob- abilistic theories with purification,

    G. Chiribella, G. M. D’Ariano, and P. Perinotti, “Prob- abilistic theories with purification,” Phys. Rev. A81, 062348 (2010)

  46. [46]

    On the Einstein-Podolsky-Rosen paradox,

    J. S. Bell, “On the Einstein-Podolsky-Rosen paradox,” Physics Physique Fizika1, 195–200 (1964)

  47. [47]

    Statistical distance and Hilbert space,

    W. K. Wootters, “Statistical distance and Hilbert space,” Phys. Rev. D23, 357–362 (1981)

  48. [48]

    Optimal state- determination by mutually unbiased measurements,

    W. K. Wootters and B. D. Fields, “Optimal state- determination by mutually unbiased measurements,” Ann. Phys.191, 363 (1989)

  49. [49]

    A Wigner-function formulation of finite-state quantum mechanics,

    W. K. Wootters, “A Wigner-function formulation of finite-state quantum mechanics,” Ann. Phys.176, 1–21 (1987)

  50. [50]

    Quantum systems with finite Hilbert space,

    A. Vourdas, “Quantum systems with finite Hilbert space,” Rep. Prog. Phys.67, 267–320 (2004)

  51. [51]

    The Monadology

    G. W. Leibniz,Discourse on Metaphysics(1686). See also “The Monadology” (1714) for the Identity of Indis- cernibles

  52. [52]

    ’t Hooft,The Cellular Automaton Interpretation of Quantum Mechanics(Springer, 2016)

    G. ’t Hooft,The Cellular Automaton Interpretation of Quantum Mechanics(Springer, 2016)

  53. [53]

    The sheaf- theoretic structure of non-locality and contextuality,

    S. Abramsky and A. Brandenburger, “The sheaf- theoretic structure of non-locality and contextuality,” New J. Phys.13, 113036 (2011)

  54. [54]

    Montgomery and L

    D. Montgomery and L. Zippin,Topological Transforma- tion Groups(Interscience, 1955)

  55. [55]

    The fuzzy sphere,

    J. Madore, “The fuzzy sphere,” Class. Quantum Grav. 9, 69–87 (1992)

  56. [56]

    Connes,Noncommutative Geometry(Academic Press, 1994)

    A. Connes,Noncommutative Geometry(Academic Press, 1994)

  57. [57]

    Origin of com- plex quantum amplitudes and Feynman’s rules,

    P. Goyal, K. H. Knuth, and J. Skilling, “Origin of com- plex quantum amplitudes and Feynman’s rules,” Phys. Rev. A81, 022109 (2010)

  58. [58]

    Quantum Mechanics as Quantum Information (and only a little more)

    C. A. Fuchs, “Quantum mechanics as quantum informa- tion (and only a little more),” arXiv:quant-ph/0205039 (2002)

  59. [59]

    Toolbox for reconstructing quantum theory from rules on information acquisition,

    P. A. H¨ ohn, “Toolbox for reconstructing quantum theory from rules on information acquisition,” Quantum1, 38 (2017)

  60. [60]

    Three-dimensionality of space and the quantum bit: an information-theoretic complete reconstruction of quantum theory,

    M. P. M¨ uller and L. Masanes, “Three-dimensionality of space and the quantum bit: an information-theoretic complete reconstruction of quantum theory,” New J. Phys.15, 053040 (2013)

  61. [61]

    Quantum mechanics as quantum measure theory,

    R. D. Sorkin, “Quantum mechanics as quantum measure theory,” Mod. Phys. Lett. A9, 3119 (1994)

  62. [62]

    Probabilities from entanglement, Born’s rulep k =|ψ k|2 from envariance,

    W. H. Zurek, “Probabilities from entanglement, Born’s rulep k =|ψ k|2 from envariance,” Phys. Rev. A71, 052105 (2005)

  63. [63]

    Characterization of Hilbert spaces by ortho- modular spaces,

    M. P. Sol` er, “Characterization of Hilbert spaces by ortho- modular spaces,” Comm. Algebra23, 219–243 (1995)

  64. [64]

    Two-point homogeneous spaces,

    H.-C. Wang, “Two-point homogeneous spaces,” Ann. Math.55, 177–191 (1952)

  65. [65]

    ¨Uber lineare Substitutionen und bilineare Formen,

    G. Frobenius, “ ¨Uber lineare Substitutionen und bilineare Formen,” J. Reine Angew. Math.84, 1–63 (1878)

  66. [66]

    Information, physics, quantum: The search for links,

    J. A. Wheeler, “Information, physics, quantum: The search for links,” inComplexity, Entropy, and the Physics of Information, edited by W. H. Zurek (Addison-Wesley, 1990), pp. 3–28