Topoi 14 (1):45-54 (1995)
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Abstract |
On Bohm''s formulation of quantum mechanics particles always have determinate positions and follow continuous trajectories. Bohm''s theory, however, requires a postulate that says that particles are initially distributed in a special way: particles are randomly distributed so that the probability of their positions being represented by a point in any regionR in configuration space is equal to the square of the wave-function integrated overR. If the distribution postulate were false, then the theory would generally fail to make the right statistical predictions. Further, if it were false, then there would at least in principle be situations where a particle would approach an eigenstate of having one position but in fact always be somewhere very different. Indeed, we will see how this might happen even if the distribution postulate were true. This will help to show how loose the connection is between the wave-function and the positions of particles in Bohm''s theory and what the precise role of the distribution postulate is. Finally, we will briefly consider two attempts to formulate a version of Bohm''s theory without the distribution postulate.
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DOI | 10.1007/BF00763478 |
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References found in this work BETA
The Undivided Universe: An Ontological Interpretation of Quantum Theory.David Bohm - 1993 - Routledge.
A Suggested Interpretation of the Quantum Theory in Terms of ‘Hidden’ Variables, I and II.David Bohm - 1952 - Physical Review (85):166-193.
The Theory of the Universal Wavefunction.Hugh Everett - 1973 - In B. DeWitt & N. Graham (eds.), The Many-Worlds Interpretation of Quantum Mechanics. Princeton UP.
”Relative State’ Formulation of Quantum Mechanics.Hugh Everett - 1957 - Reviews of Modern Physics 29 (3):454--462.
Citations of this work BETA
The Emergence and Interpretation of Probability in Bohmian Mechanics.Craig Callender - 2007 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 38 (2):351-370.
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