Conservation Laws For Every Quantum Measurement Outcome
H. H. Wills Physics Laboratory, University of Bristol, Tyndall Avenue, Bristol BS8 1TL
| Published: | 2025-07-29, volume 9, page 1815 |
| Editor: | Leon Loveridge |
| Eprint: | arXiv:2404.18621v3 |
| Doi: | https://doi.org/10.22331/q-2025-07-29-1815 |
| Citation: | Quantum 9, 1815 (2025). |
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Abstract
In the paradigmatic example of quantum measurements, whenever one measures a system which starts in a superposition of two states of a conserved quantity, it jumps to one of the two states, implying different final values for the quantity that should have been conserved. The standard law of conservation for quantum mechanics handles this jump by stating only that the total distribution of the conserved quantity over repeated measurements is unchanged, but states nothing about individual cases. Here however we show that one can go beyond this and have conservation in each individual instance. We made our arguments in the case of angular momentum of a particle on a circle, where many technicalities simplify, and bring arguments to show that this holds in full generality. Hence we argue that the conservation law in quantum mechanics should be rewritten, to go beyond its hitherto statistical formulation, to state that the total of a conserved quantity is unchanged in every individual measurement outcome. As a further crucial element, we show that conservation can be localised at the level of the system of interest and its relevant frame of reference, and is independent on any assumptions on the distribution of the conserved quantity over the entire universe.

Featured image: When a superposition of angular momentum being clockwise and anti-clockwise is measured, and the outcome is that angular momentum is anti-clockwise, is angular momentum conserved for this individual run of the experiment?
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[1] Sean M. Carroll and Jackie Lodman. ``Energy non-conservation in quantum mechanics''. Found. Phys. 51, 83 (2021).
https://doi.org/10.1007/s10701-021-00490-5
[2] Yakir Aharonov, Sandu Popescu, and Daniel Rohrlich. ``On conservation laws in quantum mechanics''. Proc. Natl. Acad. Sci. USA 118, e1921529118 (2021).
https://doi.org/10.1073/pnas.1921529118
[3] Yakir Aharonov, Sandu Popescu, and Daniel Rohrlich. ``Conservation laws and the foundations of quantum mechanics''. Proc. Natl. Acad. Sci. USA 120, e2220810120 (2023).
https://doi.org/10.1073/pnas.2220810120
[4] Tim Maudlin, Elias Okon, and Daniel Sudarsky. ``On the status of conservation laws in physics: Implications for semiclassical gravity''. Stud. Hist. Phil. Sci. B 69, 67–81 (2020).
https://doi.org/10.1016/j.shpsb.2019.10.004
[5] Franck Laloe and William J. Mullin. ``Angular momentum conservation in measurements on spin Bose-Einstein condensates''. Eur. Phys. J. D 68, 47 (2014).
https://doi.org/10.1140/epjd/e2013-40481-x
[6] Stanislaw Soltan, Mateusz Fraczak, Wolfgang Belzig, and Adam Bednorz. ``Conservation laws in quantum noninvasive measurements''. Phys. Rev. Res. 3, 013247 (2021).
https://doi.org/10.1103/PhysRevResearch.3.013247
[7] Spencer Rogers and Andrew N. Jordan. ``Postselection and quantum energetics''. Phys. Rev. A 106, 052214 (2022).
https://doi.org/10.1103/PhysRevA.106.052214
[8] J. S. Bell. ``On the Einstein Podolsky Rosen paradox''. Physics 1, 195–200 (1964).
https://doi.org/10.1103/PhysicsPhysiqueFizika.1.195
[9] JF Clauser, MA Horne, A Shimony, and RA Holt. ``Proposed experiment to test local hidden-variable theories''. Phys. Rev. Lett. 23, 880–884 (1969).
https://doi.org/10.1103/PhysRevLett.23.880
[10] D Collins, N Gisin, N Linden, S Massar, and S Popescu. ``Bell inequalities for arbitrarily high-dimensional systems''. Phys. Rev. Lett. 88, 040404 (2002).
https://doi.org/10.1103/PhysRevLett.88.040404
[11] EP Wigner. ``Die messung quantenmechanischer operatoren''. Z. Phys. 133, 101–108 (1952).
https://doi.org/10.1007/BF01948686
[12] GC Wick, AS Wightman, and EP Wigner. ``The intrinsic parity of elementary particles''. Phys. Rev. 88, 101–105 (1952).
https://doi.org/10.1103/PhysRev.88.101
[13] Huzihiro Araki and Mutsuo M. Yanase. ``Measurement of quantum mechanical operators''. Phys. Rev. 120, 622–626 (1960).
https://doi.org/10.1103/PhysRev.120.622
[14] Y Aharonov and L Susskind. ``Charge superselection rule''. Phys. Rev. 155, 1428–1431 (1967).
https://doi.org/10.1103/PhysRev.155.1428
[15] Y. Aharonov and T. Kaufherr. ``Quantum frames of reference''. Phys. Rev. D 30, 368–385 (1984).
https://doi.org/10.1103/PhysRevD.30.368
[16] Stephen D. Bartlett, Terry Rudolph, and Robert W. Spekkens. ``Reference frames, superselection rules, and quantum information''. Rev. Mod. Phys. 79, 555–609 (2007).
https://doi.org/10.1103/RevModPhys.79.555
Cited by
[1] Lev Vaidman, Open Systems: Physics, Metaphysics, and Methodology 283 (2026) ISBN:9780198929246.
[2] Ovidiu Cristinel Stoica, "Observation as Physication. A single-world unitary no-conspiracy interpretation of quantum mechanics", arXiv:2412.09669, (2024).
[3] Eloi Descamps, Nicolas Fabre, Astghik Saharyan, Arne Keller, and Pérola Milman, "Superselection Rules and Bosonic Quantum Computational Resources", Physical Review Letters 133 26, 260605 (2024).
[4] Edward J. Gillis, "Wave Function Collapse, Lorentz Invariance, and the Third Postulate of Relativity", arXiv:2405.05335, (2024).
[5] Ovidiu Cristinel Stoica, "Freedom in the Many-Worlds Interpretation", Foundations of Physics 54 5, 68 (2024).
The above citations are from Crossref's cited-by service (last updated successfully 2026-08-09 16:47:07) and SAO/NASA ADS (last updated successfully 2026-08-09 16:47:08). The list may be incomplete as not all publishers provide suitable and complete citation data.
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