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Springer eBooks

Measurement of the Schrödinger Wave of a Single Particle

Yakir Aharonov, Lev Vaidman A

Published Jan 1, 1995• 2 citations
Publisher
DOI
10.1007/978-94-015-8529-3_2

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It is shown that `bipartite' wave functions can present a mathematical formalism of quantum theory for a single particle, in which the associated Schrödinger's wave functions correspond to those `bipartite' wave functions of product forms. This extension of Schrödinger's form establishes a mathematical expression of wave-particle duality and that von Neumann's entropy is a quantitative measure of complementarity between wave-like and particle-like behaviors. In particular, this formalism suggests that collapses of Schrödinger's wave functions can be regarded as the simultaneous transition of the particle from many levels to one. Our results shed considerable light on the basis of quantum mechanics, including quantum measurement.
We show that it is possible to measure the Schrödinger wave of a single quantum system. This provides a strong argument for associating physical reality with the quantum state of a single system, and challenges the usual assumption that the quantum state has physical meaning only for an ensemble of identical systems. While the Schrödinger wave is a basic element of quantum theory, it is generally believed that one cannot associate physical reality to the wave of a single particle. Rather, the Schrödinger wave is often viewed as a mathematical tool for calculating the probabilities of various outcomes of certain experiments when many such experiments are performed on an ensemble of identical systems, all in the same quantum state. Several arguments seem to support this point of view: i) We have never seen the quantum state of a single particle in a laboratory. Indeed, while a wave is typically spread over a region of space, we never see a particle simultaneously in several distinct locations. ii) If we could see a quantum state, we could presumably distinguish it from any other quantum state, but the unitary time evolution of states in quantum