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Beyond the projection postulate and back: Quantum theories with generalized state-update rules

Vincenzo Fiorentino*,† and Stefan Weigert*,‡

  • *These authors contributed equally to this work.
  • †Contact author: vincenzo.fiorentino@york.ac.uk
  • ‡Contact author: stefan.weigert@york.ac.uk

Phys. Rev. A 113, 012204 – Published 2 January, 2026

DOI: https://doi.org/10.1103/2zpm-jsh7

Abstract

Are there consistent and physically reasonable alternatives to the projection postulate? Does it have unique properties compared with acceptable alternatives? We answer these questions by systematically investigating hypothetical state-update rules for quantum systems that Nature could have chosen over the Lüders rule. Among other basic properties, any prospective rule must define unique post-measurement states and not allow for superluminal signaling. Particular attention will be paid to consistently defining post-measurement states when performing local measurements in composite systems. Explicit examples of valid unconventional update rules are presented, each resulting in a distinct, well-defined foil of quantum theory. This framework of state-update rules allows us to identify operational properties that distinguish the projective update rule from all others and to put earlier derivations of the projection postulate into perspective.

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References (98)

  1. In view of the historic developments, it would be appropriate to speak of the “Dirac–von Neumann-Lüders rule” [23], but we will continue using “Lüders rule” for simplicity. However, the projection postulate as formulated by Dirac [7] and Lüders [9] differs from von Neumann's version [8] in key aspects; see Sec. 5f.
  2. G. Chiribella and R. W. Spekkens, Quantum Theory: Informational Foundations and Foils (Springer, Dordrecht, 2016).
  3. C. H. Bennett and G. Brassard, Quantum cryptography: Public key distribution and coin tossing. Theor. Comput. Sci. 560, 7 (2014).
  4. 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).
  5. R. Colbeck, Quantum and relativistic protocols for secure multiparty computation, Ph.D. thesis, University of Cambridge, 2006.
  6. H. J. Briegel, D. E. Browne, W. Dür, R. Raussendorf, and M. Van den Nest, Measurement-based quantum computation, Nat. Phys. 5, 19 (2009).
  7. P. A. M. Dirac, The Principles of Quantum Mechanics (Oxford University Press, Oxford, 1930).
  8. J. von Neumann, Mathematische Grundlagen der Quantenmechanik (Springer, Berlin, 1932).
  9. G. Lüders, Über die Zustandsänderung durch den Meßprozeß, Ann. Phys. (Berlin, Ger.) 443, 322 (1950).
  10. A. H. Compton and A. W. Simon, Directed quanta of scattered x-rays, Phys. Rev. 26, 289 (1925).
  11. D. Bohm, A suggested interpretation of the quantum theory in terms of “hidden” variables. I, Phys. Rev. 85, 166 (1952).
  12. B. S. Dewitt and N. Graham, The Many-Worlds Interpretation of Quantum Mechanics (Princeton University Press, Princeton, Oxford, 2015).
  13. J. Bell, Against ‘measurement’, Phys. World 3, 33 (1990).
  14. G. Bacciagaluppi and E. Crull, Heisenberg (and Schrödinger, and Pauli) on hidden variables, Stud. Hist. Philos. Sci. B 40, 374 (2009).
  15. P. Busch, P. J. Lahti, and P. Mittelstaedt, The Quantum Theory of Measurement, 2nd ed., Lecture Notes in Physics Monographs (Springer-Verlag, Berlin, Heidelberg, 1996).
  16. T. Norsen, Foundations of Quantum Mechanics (Springer, Cham, 2017).
  17. J. S. Bell and M. Nauenberg, The moral aspect of quantum mechanics, Preludes in Theoretical Physics, edited by A. De Shalit, H. Feshbach, and L. van Hove (North Holland, Amsterdam,1966), pp 279–86.
  18. F. Herbut, Derivation of the change of state in measurement from the concept of minimal measurement, Ann. Phys. (NY) 55, 271 (1969).
  19. F. Hellmann, W. Kamiński, and R. P. Kostecki, Quantum collapse rules from the maximum relative entropy principle, New J. Phys. 18, 013022 (2016).
  20. R. P. Kostecki, Lüders’ and quantum Jeffrey's rules as entropic projections, arXiv:1408.3502.
  21. S. Martinez, A search for the physical content of Lüders' rule, Synthese 82, 97 (1990).
  22. P. Busch and J. Singh, Lüders theorem for unsharp quantum measurements, Phys. Lett. A 249, 10 (1998).
  23. A. Sudbery, Whose projection postulate? arXiv:2402.15280.
  24. M. Ozawa, Quantum measuring processes of continuous observables, J. Math. Phys. 25, 79 (1984).
  25. L. Masanes, T. D. Galley, and M. P. Müller, The measurement postulates of quantum mechanics are operationally redundant, Nat. Commun. 10, 1361 (2019).
  26. B. C. Stacey, Masanes-Galley-Müller and the state-update postulate, arXiv:2211.03299.
  27. T. D. Galley, L. Masanes, and M. P. Müller, Reply to “Masanes-Galley-Müller and the state-update postulate”, arXiv:2212.03629.
  28. A. Kent, The measurement postulates of quantum mechanics are not redundant, Quantum 9, 1749 (2025).
  29. L. Masanes, T. D. Galley, and M. P. Müller, Response to “The measurement postulates of quantum mechanics are not redundant”, Quantum 9, 1592 (2025).
  30. B. C. Stacey, Contradictions or curiosities? On Kent's critique of the Masanes–Galley–Müller derivation of the quantum measurement postulates, arXiv:2405.17733.
  31. A. Kent, Nonlinearity without superluminality, Phys. Rev. A 72, 012108 (2005).
  32. A. Kent, Quantum state readout, collapses, probes, and signals, Phys. Rev. D 103, 064061 (2021).
  33. M. Kleinmann, Sequences of projective measurements in generalized probabilistic models, J. Phys. A: Math. Theor. 47, 455304 (2014).
  34. J. Barrett, Information processing in generalized probabilistic theories, Phys. Rev. A 75, 032304 (2007).
  35. L. Hardy, Quantum theory from five reasonable axioms, arXiv:quant-ph/0101012.
  36. P. Janotta and H. Hinrichsen, Generalized probability theories: What determines the structure of quantum theory? J. Phys. A: Math. Theor. 47, 323001 (2014).
  37. H. Barnum, J. Barrett, M. Leifer, and A. Wilce, Cloning and broadcasting in generic probabilistic theories, arXiv:quant-ph/0611295.
  38. J. Oppenheim and S. Wehner, The uncertainty principle determines the nonlocality of quantum mechanics, Science 330, 1072 (2010).
  39. V. J. Wright, Gleason-type theorems and general probabilistic theories, Ph.D. thesis, University of York, 2019.
  40. S. Popescu and D. Rohrlich, Quantum nonlocality as an axiom, Found. Phys. 24, 379 (1994).
  41. R. W. Spekkens, Evidence for the epistemic view of quantum states: A toy theory, Phys. Rev. A 75, 032110 (2007).
  42. S. D. Bartlett, T. Rudolph, and R. W. Spekkens, Reconstruction of Gaussian quantum mechanics from Liouville mechanics with an epistemic restriction, Phys. Rev. A 86, 012103 (2012).
  43. B. Galvan, Generalization of the Born rule, Phys. Rev. A 78, 042113 (2008).
  44. T. D. Galley and L. Masanes, Classification of all alternatives to the Born rule in terms of informational properties, Quantum 1, 15 (2017).
  45. M. Erba and P. Perinotti, The composition rule for quantum systems is not the only possible one, arXiv:2411.15964.
  46. C. M. Bender and D. W. Hook, PT-symmetric quantum mechanics, Rev. Mod. Phys. 96, 045002 (2024).
  47. B. W. Roberts, Observables, disassembled, Stud. Hist. Philos. Sci. Part B 63, 150 (2018).
  48. E. C. G. Stueckelberg, Quantum theory in real Hilbert space, Helv. Phys. Acta 33, 727 (1960).
  49. M.-O. Renou, D. Trillo, M. Weilenmann, T. P. Le, A. Tavakoli, N. Gisin, A. Acín, and M. Navascués, Quantum theory based on real numbers can be experimentally falsified, Nature (London) 600, 625 (2021).
  50. D. Finkelstein, J. M. Jauch, S. Schiminovich, and D. Speiser, Foundations of quaternion quantum mechanics, J. Math. Phys. 3, 207 (1962).
  51. G. P. Beretta, E. P. Gyftopoulos, J. L. Park, and G. N. Hatsopoulos, Quantum thermodynamics. A new equation of motion for a single constituent of matter, Nuovo Cimento B 82, 169 (1984).
  52. D. S. Abrams and S. Lloyd, Nonlinear quantum mechanics implies polynomial-time solution for NP-complete and #P problems, Phys. Rev. Lett. 81, 3992 (1998).
  53. M. Ferrero, D. Salgado, and J. L. Sánchez-Gómez, Nonlinear quantum evolution does not imply supraluminal communication, Phys. Rev. A 70, 014101 (2004).
  54. J. Rembieliński and P. Caban, Nonlinear evolution and signaling, Phys. Rev. Res. 2, 012027(R) (2020).
  55. S. Weinberg, Testing quantum mechanics, Ann. Phys. (NY) 194, 336 (1989).
  56. N. Gisin, Weinberg's non-linear quantum mechanics and supraluminal communications, Phys. Lett. A 143, 1 (1990).
  57. C. Simon, V. Bužek, and N. Gisin, No-signaling condition and quantum dynamics, Phys. Rev. Lett. 87, 170405 (2001).
  58. A. Bassi and K. Hejazi, No-faster-than-light-signaling implies linear evolution. A re-derivation, Eur. J. Phys. 36, 055027 (2015).
  59. M. Czachor, Nonlocal-looking equations can make nonlinear quantum dynamics local, Phys. Rev. A 57, 4122 (1998).
  60. B. Helou and Y. Chen, Extensions of Born's rule to non-linear quantum mechanics, some of which do not imply superluminal communication, J. Phys.: Conf. Ser. 880, 012021 (2017).
  61. A. Kent, Causal quantum theory and the collapse locality loophole, Phys. Rev. A 72, 012107 (2005).
  62. P. Busch, Is the quantum state (an) observable? Potentiality, Entanglement and Passion-at-a-Distance: Boston Studies in the Philosophy of Science, edited by R. S. Cohen, M. Horne, and J. Stachel (Springer, Dordrecht, 1997), Vol. 194, pp. 61–70.
  63.  A subnormalized state is a non-negative operator on a Hilbert space with trace less than or equal to 1, i.e. ρ∈S¯(H)={λρ:λ∈[0,1],ρ∈S(H)}.
  64. Postulate (B) is understood to assign outcome probabilities to each individual measurement. Consequently, Born's rule on its own does not account for correlations between outcomes of multiple measurements. Instead, the update rule is also responsible for the joint probabilities for the outcomes of measurements carried out sequentially, or by distinct parties in composite systems. This subtle point proves significant when examining modifications of the Lüders rule (L); see the appendix for further discussion.
  65. It is only possible to conclude that the pre-measurement state ρAB assigns a non-zero probability to obtaining the outcome PxA.
  66. The update rule also seems to be incomplete if one were to use a different formulation of (L), stating that, after a measurement, the system resides in an eigenstate of the measured observable.
  67. Recall that, mathematically, the state that correctly reproduces the experimental findings is obtained in the following way: Write the initial state corresponding to ρAB as a superposition of product terms, using the eigenstates of the operator MA for the first factor. Then, identify the term with the label x, the value of the observed measurement outcome in a given run. The second factor in this expression characterises the correct post-measurement state for subsystem B.
  68. Anticipating the discussion of Sec. 4c on the role of proper and improper mixed states, we assume for now that the density operators we consider represent either pure states or improper mixed states, i.e., those arising from entanglement with other systems.
  69.  A different formula is generally required to describe the update of proper mixed states, i.e., those due to the incomplete knowledge about the preparation of a system (cf. Sec. 4c).
  70. S. Kochen and E. P. Specker, The problem of hidden variables in quantum mechanics, J. Math. Mech. 17, 59 (1967).
  71. T. Heinosaari and M. Ziman, The Mathematical Language of Quantum Theory: From Uncertainty to Entanglement (Cambridge University Press, Cambridge, 2011).
  72. Quantum operations are linear, completely positive and trace non-increasing maps defined on the space L(H) of bounded operators acting on H. Quantum instruments are usually defined as mappings from an outcome space (X,Σ) to the set of quantum operations. However, since we will only deal with discrete observables, an instrument is completely determined by the finite set of operations {Ix}x.
  73. If the outcome PxA is never observed, Tr(PxAρi)=0, then ωA(PxA,ρi)=O, where O is the zero operator, and the experimenter learns that the system was not prepared in the state ρi.
  74. If ρA denotes either a pure or an improper mixed state, we can associate the trivial Gemenge G={(1,ρA)}, describing a system prepared in the state ρA with probability 1.
  75. The possibility of noncollapsing measurements was listed by von Neumann [8] as early as 1932 as one of three possible reactions of a physical system to a measurement.
  76. S. Aaronson, A. Bouland, J. Fitzsimons, and M. Lee, The space “just above” BQP, Proceedings of the 2016 ACM Conference on Innovations in Theoretical Computer Science 271 (ACM, New York, 2016).
  77. T. Ando and M.-D. Choi, Non-linear completely positive maps, North-Holland Math. Stud. 122, 3 (1986).
  78. M. Czachor and M. Kuna, Complete positivity of nonlinear evolution: A case study, Phys. Rev. A 58, 128 (1998).
  79. V. Fiorentino and S. Weigert, A quantum theory with noncollapsing measurements, Phys. Lett. A 559, 130903 (2025).
  80. Specifically, it belongs to the class of trivial instruments.
  81. Setting λ=0 recovers the locally-Lüders rule ωABlocL of Eq. (19).
  82. One could, however, modify (36) into a valid update rule by, for example, fixing a preferred set Bx for each experiment yielding the outcome PxA, and subsequently extending the map to composite systems via complete positivity.
  83. If U=I, we recover the passive measurements of Sec. 5c, which are consistent with A3.
  84. G. Lüders, Concerning the state-change due to the measurement process, Ann. Phys. (Berlin, Ger.) 518, 663 (2006).
  85. F. Herbut, On compatibility and improvement of different quantum state assignments, J. Phys. A: Math. Gen. 37, 5243 (2004).
  86. A. Khrennikov, Von Neumann and Lüders postulates and quantum information theory, Int. J. Quantum Inform. 07, 1303 (2009).
  87. K. Flatt, S. M. Barnett, and S. Croke, Gleason-Busch theorem for sequential measurements, Phys. Rev. A 96, 062125 (2017).
  88. M. Wilson and N. Ormrod, On the origin of linearity and unitarity in quantum theory, arXiv:2305.20063.
  89. G. Cassinelli and N. Zanghi, Conditional probabilities in quantum mechanics. I.—Conditioning with respect to a single event, Nuovo Cimento B 73, 237 (1983).
  90. J.-P. Marchand and W. Wyss, Statistical inference and entropy, J. Stat. Phys. 16, 349 (1977).
  91. D. Dieks and P. Veltkamp, Distance between quantum states, statistical inference and the projection postulate, Phys. Lett. A 97, 24 (1983).
  92. N. Hadjisavvas, Distance between states and statistical inference in quantum theory, Ann. Inst. Henri Poincaré Sect. A 35, 287 (1981).
  93. M. Ozawa, Quantum state reduction: An operational approach, Fortschr. Phys. 46, 615 (1998).
  94. F. Herbut, Minimal-disturbance measurement as a specification in von Neumann's quantal theory of measurement, Int. J. Theor. Phys. 11, 193 (1974).
  95. M. Friedman and H. Putnam, Quantum logic, conditional probability, and interference, Dialectica 32 305 (1978).
  96. E. B. Davies, Quantum Theory of Open Systems (Academic Press, London, 1976).
  97. P. Busch, M. Grabowski, and P. J. Lahti, Repeatable measurements in quantum theory: Their role and feasibility, Found. Phys. 25, 1239 (1995).
  98. M. Marinković, M. Damnjanović, and I. D. Ivanović, A note on the Lüders-von Neumann formula of collapse, Phys. Lett. A 99, 22 (1983).

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