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

Progress of Theoretical Physics

Probabilistic Interpretation and the Quantum Theory of Measurement. II

Ziro Maki

Published Oct 1, 1989• 8 citations
Publisher

Abstract

A general theory of quantum-mechanical measurement is presented. It is shown that some general conditions should be satisfied for any apparatus to carry out the ideal measurement, and the reduction of state is an inevitable consequence of the action of such an apparatus. The statistical operator (in weak sense) is defined uniquely for ensembles prepared with respect to the measured observables, without recourse to the expectation value hypothesis. The probabilistic interpretation (the Born ansatz) comes out as a natural explanation of physical contents of the statistical operator after the measurement, rather than an axiomatic presumption of quantum mechanics.

DOI
10.1143/ptp.82.638

Related papers

Probabilistic Interpretation and the Quantum Theory of Measurement

Ziro Maki

The logical foundation of the probabilistic intrepretation of quantum-mechanical states is re-examined in view of Fukuda's new theory of measurement. We suggest that the probabilistic interpretation could be viewed as a natural consequence of the reduction of states upon meaurement, rather than an a priori ansatz contained in the “external observation” framework of quantum mechanics.

Progress of Theoretical Physics•Jan 1, 1988•9 citations

Theory of Measurement

Yutaka Toyozawa

Theory of measurement is presented which is based on the statistical interpretation of quantum mechanics. The reduction of wave packet is ascribed to undue comparison of the state of an ensemble before measurement and the state of an individual system after measurement. By studying the evolution of statistical operators for subsystems and composite systems comprising an object, a measuring apparatus and an observer, one can definitely locate where the measurement is done, thus negating the principle of psycho-physical parallelism due to von Neumann. Time needed for measurement is also discussed. The Einstein-Podolsky-Rosen state is described as an eigenstate of correlation. The argument lends support to the standpoint that the physical state of a system is to be represented by the statistical operator, not by the wave function, in the conceptual foundation of quantum mechanics.

Progress of Theoretical Physics•Feb 1, 1992•0 citations

Theory of Measurement: A Note on Conceptual Foundation of Quantum Mechanics

Yutaka Toyozawa

Theory of measurement is presented which is based on the statistical interpretation of quantum mechanics. The reduction of wave packet is ascribed to undue comparison of the state of an ensemble before measurement and the state of an individual system after measurement. By studying the evolution of statistical operators for subsystems and composite systems comprising an object, a measuring apparatus and an observer, one can definitely locate where the measurement is done, thus negating the principle of psycho-physical parallelism due to von Neumann. Time needed for measurement is also discussed. The Einstein-Podolsky-Rosen state is described as an eigenstate of correlation. The argument lends support to the standpoint that the physical state of a system is to be represented by the statistical operator, not by the wave function, in the conceptual foundation of quantum mechanics.

Progress of Theoretical Physics•Feb 1, 1992•2 citations

The probability interpretation

Peter Mittelstaedt

Historical remarks The quantum mechanical formalism discovered by Heisenberg [Heis 25] an Schrödinger [Schrö 26] in 1925 was first interpreted in a statistical sense by Born [Born 26]. The formal expressions p (φ, a i ) = |(φ,φ ai )| 2 , i ∈ N, were interpreted as the probabilities that a quantum system S with preparation φ possesses the value a i that belongs to the state φ ai . This original Born interpretation, which was formulated for scattering processes, was, however, not tenable in the general case. The probabilities must not be related to the system S in state φ, since in the preparation φ the value a i of an observable A is in general not subjectively unknown but objectively undecided. Instead, one has to interpret the formal expressions p ( a i , a i ) as the probabilities of finding the value a i after measurement of the observable A of the system S with preparation φ. In this improved version, the statistical or Born interpretation is used in the present-day literature. On the one hand, the statistical (Born) interpretation of quantum mechanics is usually taken for granted, and the formalism of quantum mechanics is considered as a theory that provides statistical predictions referring to a sufficiently large ensemble of identically prepared systems S (φ) after the measurement of the observable in question. On the other hand, the meaning of the same formal terms p (φ, a i ) for an individual system is highly problematic.

Cambridge University Press eBooks•Dec 4, 1997•3 citations

Untenability of simple ensemble interpretations of quantum measurement probabilities

Daniel T. Gillespie

Some interpretations of quantum mechanics try to describe the probabilistic nature of quantum measurements in a way that allows a system in a pure state to always have precise (if not simultaneously knowable) values for all its observable variables. In what might be called a simple ensemble interpretation, the quantum mechanical state vector is assumed to define a statistical ensemble of identically prepared systems, each of which has precise values for all its observable variables, and the act of measurement is equivalenced to a straightforward sampling of that ensemble. It is shown here, in a manner that should be suitable for a first course in quantum mechanics, that a simple ensemble interpretation is not possible for some quantum systems, and hence is untenable as a general premise. The analysis is essentially a repackaging of the Bell argument against hidden variables, although hidden variables are never invoked here.

American Journal of Physics•Oct 1, 1986•9 citations

Aspects of Probability in Quantum Theory

Michael Dickson

Abstract This chapter elucidates quantum probabilities in the formal apparatus of quantum mechanics, while not taking sides about interpretive issues. A central contention is that the notion of a probability measure should not be captured in the usual classical framework, but instead in the more general framework of effect algebras. Two formulations of quantum mechanics in this framework are provided: one using projection-valued measures, another using positive-operator-valued measures. The chapter presents several versions of the Born Rule and critically examines justifications that have been proposed for the Born Rule. The chapter concludes with laying down the perennial puzzles about probability in quantum mechanics such as quantum correlations.

•Sep 1, 2011•2 citations
A general theory of quantum-mechanical measurement is presented. It is shown that some general conditions should be satisfied for any apparatus to carry out the ideal measurement, and the reduction of state is an inevitable consequence of the action of such an apparatus. The statistical operator (in weak sense) is defined uniquely for ensembles prepared with respect to the measured observables, without recourse to the expectation value hypothesis. The probabilistic interpretation (the Born ansatz) comes out as a natural explanation of physical contents of the statistical operator after the measurement, rather than an axiomatic presumption of quantum mechanics.
Theory of measurement is presented which is based on the statistical interpretation of quantum mechanics. The reduction of wave packet is ascribed to undue comparison of the state of an ensemble before measurement and the state of an individual system after measurement. By studying the evolution of statistical operators for subsystems and composite systems comprising an object, a measuring apparatus and an observer, one can definitely locate where the measurement is done, thus negating the principle of psycho-physical parallelism due to von Neumann. Time needed for measurement is also discussed. The Einstein-Podolsky-Rosen state is described as an eigenstate of correlation. The argument lends support to the standpoint that the physical state of a system is to be represented by the statistical operator, not by the wave function, in the conceptual foundation of quantum mechanics.
Theory of measurement is presented which is based on the statistical interpretation of quantum mechanics. The reduction of wave packet is ascribed to undue comparison of the state of an ensemble before measurement and the state of an individual system after measurement. By studying the evolution of statistical operators for subsystems and composite systems comprising an object, a measuring apparatus and an observer, one can definitely locate where the measurement is done, thus negating the principle of psycho-physical parallelism due to von Neumann. Time needed for measurement is also discussed. The Einstein-Podolsky-Rosen state is described as an eigenstate of correlation. The argument lends support to the standpoint that the physical state of a system is to be represented by the statistical operator, not by the wave function, in the conceptual foundation of quantum mechanics.
Historical remarks The quantum mechanical formalism discovered by Heisenberg [Heis 25] an Schrödinger [Schrö 26] in 1925 was first interpreted in a statistical sense by Born [Born 26]. The formal expressions p (φ, a i ) = |(φ,φ ai )| 2 , i ∈ N, were interpreted as the probabilities that a quantum system S with preparation φ possesses the value a i that belongs to the state φ ai . This original Born interpretation, which was formulated for scattering processes, was, however, not tenable in the general case. The probabilities must not be related to the system S in state φ, since in the preparation φ the value a i of an observable A is in general not subjectively unknown but objectively undecided. Instead, one has to interpret the formal expressions p ( a i , a i ) as the probabilities of finding the value a i after measurement of the observable A of the system S with preparation φ. In this improved version, the statistical or Born interpretation is used in the present-day literature. On the one hand, the statistical (Born) interpretation of quantum mechanics is usually taken for granted, and the formalism of quantum mechanics is considered as a theory that provides statistical predictions referring to a sufficiently large ensemble of identically prepared systems S (φ) after the measurement of the observable in question. On the other hand, the meaning of the same formal terms p (φ, a i ) for an individual system is highly problematic.
Some interpretations of quantum mechanics try to describe the probabilistic nature of quantum measurements in a way that allows a system in a pure state to always have precise (if not simultaneously knowable) values for all its observable variables. In what might be called a simple ensemble interpretation, the quantum mechanical state vector is assumed to define a statistical ensemble of identically prepared systems, each of which has precise values for all its observable variables, and the act of measurement is equivalenced to a straightforward sampling of that ensemble. It is shown here, in a manner that should be suitable for a first course in quantum mechanics, that a simple ensemble interpretation is not possible for some quantum systems, and hence is untenable as a general premise. The analysis is essentially a repackaging of the Bell argument against hidden variables, although hidden variables are never invoked here.
Abstract This chapter elucidates quantum probabilities in the formal apparatus of quantum mechanics, while not taking sides about interpretive issues. A central contention is that the notion of a probability measure should not be captured in the usual classical framework, but instead in the more general framework of effect algebras. Two formulations of quantum mechanics in this framework are provided: one using projection-valued measures, another using positive-operator-valued measures. The chapter presents several versions of the Born Rule and critically examines justifications that have been proposed for the Born Rule. The chapter concludes with laying down the perennial puzzles about probability in quantum mechanics such as quantum correlations.