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

Physics Letters A

Reduction of the wave function: an operational approach

Давид Николаевич Клышко

Published Jun 1, 1998• 6 citations
Publisher
DOI
10.1016/s0375-9601(98)00242-4

Related papers

The Reduction of the Wave-Function and the Reduction of Entropy

H. N. Ioannidou

Springer eBooks•Jan 1, 1980•0 citations

Delta function singularity in the Reduction of Radial Schrodinger Equation

Anzor Khelashvili, T. Nadareishvili

We obtain the extra delta-like singularity while reduction of the Laplace operator in spherical coordinates, elimination of which restricts the radial wave functions at the origin. This restriction has the form of boundary condition for the radial wave function.

arXiv:1009.3612•Sep 19, 2010•0 citations

The Collapse of the Wave Function

Stephen Gamboa‐Eastman

Physics Essays•Sep 1, 1996•1 citation

Reduction of the Wave-Function: An Operational Approach

Давид Николаевич Клышко

Possible experimental demonstration of the wave-function's reduction by means of correlation experiments with non-commuting observables and fast-response detectors is discussed. As an example, the sequential measurements of a free particle's longitudinal coordinates in the Time-of-Flight apparatus are considered.

Fortschritte der Physik•Nov 1, 1998•0 citations

The Collapse of the Wave Function

Harvard University Press eBooks•Mar 15, 1994•0 citations

Reduction of Wave Function by Stationary Phase of Macrovariable

R. Fukuda

Abstract Any microscopic object is assumed to be a point-like particle, fluctuating quite randomly in the time scale $\tau$, which is much smaller than the smallest time interval $\Delta$ we can discriminate. The trajectories in $\Delta$ scale are defined. They are exclusive of each other since they originate from one particle having a position which is an objectively existing value. The measurement of the object is performed by the wave function, which is defined by summing up trajectories in $\Delta$ scale together with the phase factor. The wave function is thus a linear combination of exclusive paths. The measurement is performed by the macrovariable denoted as X. It loses the fluctuation by the stationary phase mechanism. Using a simple model to measure the operator O of the object, it is shown that, when the detector is switched on, the stationary phase trajectory of X branches into many trajectories, each of which is mapped to the eigenstate of O. Although these trajectories are all summed up for the wave function, in the actual experiment X takes one stationary trajectory. Therefore, the object is frozen to the corresponding eigenstate and realizes the reduction. The process of the reduction is shown to be realized with the correct frequency when the experiment is repeated. A model of the position measurement is also studied and the estimation of the magnitude of the upper bound of $\Delta$ is given based on the present experimental data.

Progress of Theoretical and Experimental Physics•Sep 23, 2025•0 citations
Abstract Any microscopic object is assumed to be a point-like particle, fluctuating quite randomly in the time scale τ\tauτ, which is much smaller than the smallest time interval Δ\DeltaΔ we can discriminate. The trajectories in Δ\DeltaΔ scale are defined. They are exclusive of each other since they originate from one particle having a position which is an objectively existing value. The measurement of the object is performed by the wave function, which is defined by summing up trajectories in Δ\DeltaΔ scale together with the phase factor. The wave function is thus a linear combination of exclusive paths. The measurement is performed by the macrovariable denoted as X. It loses the fluctuation by the stationary phase mechanism. Using a simple model to measure the operator O of the object, it is shown that, when the detector is switched on, the stationary phase trajectory of X branches into many trajectories, each of which is mapped to the eigenstate of O. Although these trajectories are all summed up for the wave function, in the actual experiment X takes one stationary trajectory. Therefore, the object is frozen to the corresponding eigenstate and realizes the reduction. The process of the reduction is shown to be realized with the correct frequency when the experiment is repeated. A model of the position measurement is also studied and the estimation of the magnitude of the upper bound of Δ\DeltaΔ is given based on the present experimental data.