Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Generalized Uncertainty and the WAY Theorem: Intrinsic and Operational Limits on Position Measurement

S. Zarrinkamar

Published Oct 30, 2026• 0 citations
Publisher

Abstract

The continuous and unbounded extension of the Wigner--Araki--Yanase (WAY) theorem by Kuramochi and Tajima establishes a conservation-law obstruction to exact position measurements. We investigate how this result is modified when the measured system obeys a quadratic generalized uncertainty principle (GUP), [X,P] = iℏ(1 +βP2). First, we recover the intrinsic minimal-localization scale ∆Xmin = ℏ√β. Second, assuming an additive conserved momentum, a Yanase-compatible pointer, and the usual hypotheses underlying Ozawa's noise--conservation inequality, we derive a conditional GUP-modified bound on the root-mean-square measurement noise, ϵX ≥ℏ[1 +β⟨P2S⟩]/[2√(∆PS)2 +(∆PA)2]. The result reduces to the canonical bound when β → 0 and makes explicit the dependence on both the system state and apparatus resource. We distinguish this quantitative, model-dependent statement from the intrinsic minimal-length relation and identify the operator-domain and composite-system assumptions required for a full theorem.

DOI
10.1364/opticaopen.34790334.v1

Related papers

Generalized Uncertainty and the WAY Theorem: Intrinsic and Operational Limits on Position Measurement

S. Zarrinkamar

The continuous and unbounded extension of the Wigner--Araki--Yanase (WAY) theorem by Kuramochi and Tajima establishes a conservation-law obstruction to exact position measurements. We investigate how this result is modified when the measured system obeys a quadratic generalized uncertainty principle (GUP), [X,P] = iℏ(1 +βP2). First, we recover the intrinsic minimal-localization scale ∆Xmin = ℏ√β. Second, assuming an additive conserved momentum, a Yanase-compatible pointer, and the usual hypotheses underlying Ozawa's noise--conservation inequality, we derive a conditional GUP-modified bound on the root-mean-square measurement noise, ϵX ≥ℏ[1 +β⟨P2S⟩]/[2√(∆PS)2 +(∆PA)2]. The result reduces to the canonical bound when β → 0 and makes explicit the dependence on both the system state and apparatus resource. We distinguish this quantitative, model-dependent statement from the intrinsic minimal-length relation and identify the operator-domain and composite-system assumptions required for a full theorem.

•Oct 30, 2026•0 citations

Quantum limits of measurements induced by multiplicative conservation laws: Extension of the Wigner-Araki-Yanase theorem

Gen Kimura, Bernhard K. Meister, Masanao Ozawa

The Wigner-Araki-Yanase (WAY) theorem shows that additive conservation laws limit the accuracy of measurements. Recently, various quantitative expressions have been found for quantum limits on measurements induced by additive conservation laws, and have been applied to the study of fundamental limits on quantum-information processing. Here, we investigate generalizations of the WAY theorem to multiplicative conservation laws. The WAY theorem is extended to show that an observable not commuting with the modulus of, or equivalently the square of, a multiplicatively conserved quantity cannot be precisely measured. We also obtain a lower bound for the mean-square noise of a measurement in the presence of a multiplicatively conserved quantity. To overcome this noise it is necessary to make large the coefficient of variation (the so-called relative fluctuation), instead of the variance as is the case for additive conservation laws, of the conserved quantity in the apparatus.

arXiv:0707.3238•Physical Review A•Sep 8, 2008•6 citations

Exact Solutions for Spin Conserving Models and the Wigner-Araki-Yanase Theorem

Michael Steiner, Ronald Rendell

The Wigner-Araki-Yanase (WAY) theorem is a well-known theorem regarding limitations of quantum measurement in the presence of additive conservation laws. Under the assumptions of the von Neumann measurement model, for which the system conserved quantity $L_{S}$ is bounded, given a conserved total additive system plus apparatus quantity $L_{SA}$, the measurement operator $E_{S}$ must commute with $L_{S}$. Prior proofs have exploited the properties of unitary evolution constrained by momentum conserving operations that tend to obscure the physical nature of the WAY theorem and as well lead to bounds on performance. As it is generally agreed that momentum is always exactly conserved in measurement, we instead develop a general angular momentum conserving model of measurement. This model is shown to lead to a simple explanation of the major implications of the WAY theorem and provides exact results of the effects of measurement based on the apparatus model. This is shown by both tracing the apparatus from the density matrix and also via a system-only channel model based on Kraus operators.

quant-pharXiv:2606.02861•Jun 3, 2026•0 citations

Uncertainty beyond the Uncertainty Principle

Charles Day

According to a new extension to an old theory, a particle's position cannot be measured precisely even if its momentum is not measured simultaneously.By Charles Day H eisenberg's uncertainty principle limits the precision with which two observables that do not commute with each other can be simultaneously measured.The Wigner-Araki-Yanase (WAY) theorem goes further.If observables A and B do not commute, and if observable A is conserved, observable B cannot be measured with arbitrary precision even if A is not measured at all.In its original 1960 formulation, the WAY theorem applied only to observables, such as spin, whose possible values are discrete and bounded.Now Yui Kuramochi of Kyushu University and Hiroyasu Tajima of the University of Electro-Communications-both in Japan-have proven that the WAY theorem also encompasses observables, such as position, that are continuous and unbounded [1].Besides resolving the decades-long problem of how to deal with such observables, the extension will likely find practical applications in quantum optics.The difficulty of extending the WAY theorem arose from how an

Physics•Nov 21, 2023•0 citations

Wigner-Araki-Yanase Theorem for Continuous and Unbounded Conserved Observables

Yui Kuramochi, Hiroyasu Tajima

The Wigner-Araki-Yanase (WAY) theorem states that additive conservation laws imply the commutativity of exactly implementable projective measurements and the conserved observables of the system. Known proofs of this theorem are only restricted to bounded or discrete-spectrum conserved observables of the system and are not applicable to unbounded and continuous observables like a momentum operator. In this Letter, we present the WAY theorem for possibly unbounded and continuous conserved observables under the Yanase condition, which requires that the probe positive operator-valued measure should commute with the conserved observable of the probe system. As a result of this WAY theorem, we show that exact implementations of the projective measurement of the position under momentum conservation and of the quadrature amplitude using linear optical instruments and photon counters are impossible. We also consider implementations of unitary channels under conservation laws and find that the conserved observable L_{S} of the system commutes with the implemented unitary U_{S} if L_{S} is semibounded, while U_{S}^{†}L_{S}U_{S} can shift up to possibly nonzero constant factor if the spectrum of L_{S} is upper and lower unbounded. We give simple examples of the latter case, where L_{S} is a momentum operator.

arXiv:2208.13494•Physical Review Letters•Nov 21, 2023•15 citations

Conservation Laws, Uncertainty Relations, and Quantum Limits of Measurements

Masanao Ozawa

The uncertainty relation between the noise operator and the conserved quantity leads to a bound on the accuracy of general measurements. The bound extends the assertion by Wigner, Araki, and Yanase that conservation laws limit the accuracy of "repeatable," or "nondisturbing," measurements to general measurements, and improves the one previously obtained by Yanase for spin measurements. The bound represents an obstacle to making a small quantum computer.

arXiv:quant-ph/0112154•Physical Review Letters•Jan 23, 2002•68 citations
The continuous and unbounded extension of the Wigner--Araki--Yanase (WAY) theorem by Kuramochi and Tajima establishes a conservation-law obstruction to exact position measurements. We investigate how this result is modified when the measured system obeys a quadratic generalized uncertainty principle (GUP), [X,P] = iℏ(1 +βP2). First, we recover the intrinsic minimal-localization scale ∆Xmin = ℏ√β. Second, assuming an additive conserved momentum, a Yanase-compatible pointer, and the usual hypotheses underlying Ozawa's noise--conservation inequality, we derive a conditional GUP-modified bound on the root-mean-square measurement noise, ϵX ≥ℏ[1 +β⟨P2S⟩]/[2√(∆PS)2 +(∆PA)2]. The result reduces to the canonical bound when β → 0 and makes explicit the dependence on both the system state and apparatus resource. We distinguish this quantitative, model-dependent statement from the intrinsic minimal-length relation and identify the operator-domain and composite-system assumptions required for a full theorem.
The continuous and unbounded extension of the Wigner--Araki--Yanase (WAY) theorem by Kuramochi and Tajima establishes a conservation-law obstruction to exact position measurements. We investigate how this result is modified when the measured system obeys a quadratic generalized uncertainty principle (GUP), [X,P] = iℏ(1 +βP2). First, we recover the intrinsic minimal-localization scale ∆Xmin = ℏ√β. Second, assuming an additive conserved momentum, a Yanase-compatible pointer, and the usual hypotheses underlying Ozawa's noise--conservation inequality, we derive a conditional GUP-modified bound on the root-mean-square measurement noise, ϵX ≥ℏ[1 +β⟨P2S⟩]/[2√(∆PS)2 +(∆PA)2]. The result reduces to the canonical bound when β → 0 and makes explicit the dependence on both the system state and apparatus resource. We distinguish this quantitative, model-dependent statement from the intrinsic minimal-length relation and identify the operator-domain and composite-system assumptions required for a full theorem.
The Wigner-Araki-Yanase (WAY) theorem shows that additive conservation laws limit the accuracy of measurements. Recently, various quantitative expressions have been found for quantum limits on measurements induced by additive conservation laws, and have been applied to the study of fundamental limits on quantum-information processing. Here, we investigate generalizations of the WAY theorem to multiplicative conservation laws. The WAY theorem is extended to show that an observable not commuting with the modulus of, or equivalently the square of, a multiplicatively conserved quantity cannot be precisely measured. We also obtain a lower bound for the mean-square noise of a measurement in the presence of a multiplicatively conserved quantity. To overcome this noise it is necessary to make large the coefficient of variation (the so-called relative fluctuation), instead of the variance as is the case for additive conservation laws, of the conserved quantity in the apparatus.
The Wigner-Araki-Yanase (WAY) theorem is a well-known theorem regarding limitations of quantum measurement in the presence of additive conservation laws. Under the assumptions of the von Neumann measurement model, for which the system conserved quantity LSL_{S}LS​ is bounded, given a conserved total additive system plus apparatus quantity LSAL_{SA}LSA​, the measurement operator ESE_{S}ES​ must commute with LSL_{S}LS​. Prior proofs have exploited the properties of unitary evolution constrained by momentum conserving operations that tend to obscure the physical nature of the WAY theorem and as well lead to bounds on performance. As it is generally agreed that momentum is always exactly conserved in measurement, we instead develop a general angular momentum conserving model of measurement. This model is shown to lead to a simple explanation of the major implications of the WAY theorem and provides exact results of the effects of measurement based on the apparatus model. This is shown by both tracing the apparatus from the density matrix and also via a system-only channel model based on Kraus operators.
According to a new extension to an old theory, a particle's position cannot be measured precisely even if its momentum is not measured simultaneously.By Charles Day H eisenberg's uncertainty principle limits the precision with which two observables that do not commute with each other can be simultaneously measured.The Wigner-Araki-Yanase (WAY) theorem goes further.If observables A and B do not commute, and if observable A is conserved, observable B cannot be measured with arbitrary precision even if A is not measured at all.In its original 1960 formulation, the WAY theorem applied only to observables, such as spin, whose possible values are discrete and bounded.Now Yui Kuramochi of Kyushu University and Hiroyasu Tajima of the University of Electro-Communications-both in Japan-have proven that the WAY theorem also encompasses observables, such as position, that are continuous and unbounded [1].Besides resolving the decades-long problem of how to deal with such observables, the extension will likely find practical applications in quantum optics.The difficulty of extending the WAY theorem arose from how an
The Wigner-Araki-Yanase (WAY) theorem states that additive conservation laws imply the commutativity of exactly implementable projective measurements and the conserved observables of the system. Known proofs of this theorem are only restricted to bounded or discrete-spectrum conserved observables of the system and are not applicable to unbounded and continuous observables like a momentum operator. In this Letter, we present the WAY theorem for possibly unbounded and continuous conserved observables under the Yanase condition, which requires that the probe positive operator-valued measure should commute with the conserved observable of the probe system. As a result of this WAY theorem, we show that exact implementations of the projective measurement of the position under momentum conservation and of the quadrature amplitude using linear optical instruments and photon counters are impossible. We also consider implementations of unitary channels under conservation laws and find that the conserved observable L_{S} of the system commutes with the implemented unitary U_{S} if L_{S} is semibounded, while U_{S}^{†}L_{S}U_{S} can shift up to possibly nonzero constant factor if the spectrum of L_{S} is upper and lower unbounded. We give simple examples of the latter case, where L_{S} is a momentum operator.