Physics:Wigner–Araki–Yanase theorem

From HandWiki

The Wigner–Araki–Yanase theorem, also known as the WAY theorem, is a result in quantum physics establishing that the presence of a conservation law limits the accuracy with which observables that fail to commute with the conserved quantity can be measured.[1][2][3] It is named for the physicists Eugene Wigner,[4] Huzihiro Araki and Mutsuo Yanase.[5][6]

The theorem can be illustrated with a particle coupled to a measuring apparatus.[7]: 421  If the position operator of the particle is q and its momentum operator is p, and if the position and momentum of the apparatus are Q and P respectively, assuming that the total momentum p+P is conserved implies that, in a suitably quantified sense, the particle's position itself cannot be measured. The measurable quantity is its position relative to the measuring apparatus, represented by the operator q−Q. The Wigner–Araki–Yanase theorem generalizes this to the case of two arbitrary observables A and B for the system and an observable C for the apparatus, satisfying the condition that B+C is conserved.[8][9]

Mikko Tukiainen gave a generalized version of the WAY theorem, which makes no use of conservation laws, but uses quantum incompatibility instead.[10]

Yui Kuramochi and Hiroyasu Tajima proved a generalized form of the theorem for possibly unbounded and continuous conserved observables.[11]

References

  1. ↑ Baez, John C. (1994-05-10). "Week 33". http://math.ucr.edu/home/baez/week33.html. 
  2. ↑ Ahmadi, Mehdi; Jennings, David; Rudolph, Terry (2013-01-28). "The Wigner–Araki–Yanase theorem and the quantum resource theory of asymmetry" (in en). New Journal of Physics 15 (1). doi:10.1088/1367-2630/15/1/013057. ISSN 1367-2630. Bibcode: 2013NJPh...15a3057A. 
  3. ↑ Loveridge, L.; Busch, P. (2011). "'Measurement of quantum mechanical operators' revisited" (in en). The European Physical Journal D 62 (2): 297–307. doi:10.1140/epjd/e2011-10714-3. ISSN 1434-6060. Bibcode: 2011EPJD...62..297L. 
  4. ↑ Wigner, E. P. (1995), Mehra, Jagdish, ed., "Die Messung quantenmechanischer Operatoren" (in en), Philosophical Reflections and Syntheses (Springer Berlin Heidelberg): pp. 147–154, doi:10.1007/978-3-642-78374-6_10, ISBN 978-3-540-63372-3 . For an English translation, see Busch, P. (2010). "Translation of "Die Messung quantenmechanischer Operatoren" by E.P. Wigner". arXiv:1012.4372 [quant-ph].
  5. ↑ Araki, Huzihiro; Yanase, Mutsuo M. (1960-10-15). "Measurement of Quantum Mechanical Operators" (in en). Physical Review 120 (2): 622–626. doi:10.1103/PhysRev.120.622. ISSN 0031-899X. Bibcode: 1960PhRv..120..622A. https://link.aps.org/doi/10.1103/PhysRev.120.622. 
  6. ↑ Yanase, Mutsuo M. (1961-07-15). "Optimal Measuring Apparatus" (in en). Physical Review 123 (2): 666–668. doi:10.1103/PhysRev.123.666. ISSN 0031-899X. Bibcode: 1961PhRv..123..666Y. 
  7. ↑ Peres, Asher (1995). Concepts and Methods. Kluwer Academic Publishers. ISBN 0-7923-2549-4. 
  8. ↑ Ghirardi, G. C.; Miglietta, F.; Rimini, A.; Weber, T. (1981-07-15). "Limitations on quantum measurements. I. Determination of the minimal amount of nonideality and identification of the optimal measuring apparatuses" (in en). Physical Review D 24 (2): 347–352. doi:10.1103/PhysRevD.24.347. ISSN 0556-2821. Bibcode: 1981PhRvD..24..347G. 
  9. ↑ Ghirardi, G. C.; Miglietta, F.; Rimini, A.; Weber, T. (1981-07-15). "Limitations on quantum measurements. II. Analysis of a model example" (in en). Physical Review D 24 (2): 353–358. doi:10.1103/PhysRevD.24.353. ISSN 0556-2821. Bibcode: 1981PhRvD..24..353G. 
  10. ↑ Tukiainen, Mikko (20 January 2017). "Wigner-Araki-Yanase theorem beyond conservation laws". Physical Review A 95 (1). doi:10.1103/PhysRevA.95.012127. Bibcode: 2017PhRvA..95a2127T. https://journals.aps.org/pra/export/10.1103/PhysRevA.95.012127. 
  11. ↑ Kuramochi, Yui; Tajima, Hiroyasu (2023-11-21). "Wigner-Araki-Yanase Theorem for Continuous and Unbounded Conserved Observables". Phys. Rev. Lett. 131 (21). doi:10.1103/PhysRevLett.131.210201. PMID 38072616. Bibcode: 2023PhRvL.131u0201K.