1969
DOI: 10.1119/1.1975279
|View full text |Cite
|
Sign up to set email alerts
|

On the Interpretation of Measurement within the Quantum Theory

Abstract: An interpretation of the process of measurement is proposed which can be placed wholly within the quantum theory. The entire system including the apparatus and even the mind of the observer can be considered to develop according to the Schrödinger equation. No separation, in principle, of the observer and the observed is necessary; nor is it necessary to introduce either the type I process of von Neumann or wave function reduction.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
9
0

Year Published

1973
1973
2015
2015

Publication Types

Select...
5
4
1

Relationship

0
10

Authors

Journals

citations
Cited by 33 publications
(9 citation statements)
references
References 0 publications
0
9
0
Order By: Relevance
“…This theory has subsequently been generalized. In the second category of theories, perhaps the most radical is the one proposed by Everett, Wheeler, Cooper, DeWitt, and others [2][3][4][5][6][7] between 1957 and 1970, which shows that even if one assumes that the wave function containing the observer evolves causally according to the Schrödinger equation, the observer will subjectively experience wave function collapse. Zeh, Kübler, Joos, Machida, Namiki, Zurek, Unruh, Cini, Peres, Partovi, Gallis, Fleming, Hartle and others [8][9][10][11][12][13][14][15][16][17][18][19][20] have strengthened this position by showing that for macroscopic objects, their inevitable interaction with the environment leads to a dynamic reduction of the density matrix (what is widely known as wave function collapse) and superselection rules.…”
Section: Introductionmentioning
confidence: 99%
“…This theory has subsequently been generalized. In the second category of theories, perhaps the most radical is the one proposed by Everett, Wheeler, Cooper, DeWitt, and others [2][3][4][5][6][7] between 1957 and 1970, which shows that even if one assumes that the wave function containing the observer evolves causally according to the Schrödinger equation, the observer will subjectively experience wave function collapse. Zeh, Kübler, Joos, Machida, Namiki, Zurek, Unruh, Cini, Peres, Partovi, Gallis, Fleming, Hartle and others [8][9][10][11][12][13][14][15][16][17][18][19][20] have strengthened this position by showing that for macroscopic objects, their inevitable interaction with the environment leads to a dynamic reduction of the density matrix (what is widely known as wave function collapse) and superselection rules.…”
Section: Introductionmentioning
confidence: 99%
“…But then, clearly, Bohr admits that macroscopic systems, usually described classically, can be described also quantummechanically. This opens up the alley of treating the macroscopic objects on the same footing as the microscopic ones (cf [19], [20], [21]).…”
Section: More On Von Neumann Bohr and Everettmentioning
confidence: 99%
“…At the center of the controversy stands the so called collapse postulate, according to which the time-evolution of the wavefunction is occasionally not governed by the Schrödinger equation, but described by a discontinuous random jump, a socalled "collapse". This postulate was introduced to explain the apparently random outcomes of certain quantum measurements, but is completely unnecessary according to the Everett interpretation [23][24][25][26][27][28], also known as the "many worlds interpretation". The debate continues about the underlying philosophical and ontological issues (see, e.g., [29,31]), but these are not crucial to the argument in this paper.…”
Section: A Brief Review Of the No Collapse Interpretationmentioning
confidence: 99%