The theorem can be illustrated with a particle coupled to a measuring apparatus.[7]: 421 If the position operator of the particle is and its momentum operator is , and if the position and momentum of the apparatus are and respectively, assuming that the total momentum 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 . The Wigner–Araki–Yanase theorem generalizes this to the case of two arbitrary observables and for the system and an observable for the apparatus, satisfying the condition that 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]
^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". Physical Review D. 24 (2): 347–352. doi:10.1103/PhysRevD.24.347. ISSN0556-2821.