期刊
BRITISH JOURNAL FOR THE PHILOSOPHY OF SCIENCE
卷 56, 期 2, 页码 199-220出版社
OXFORD UNIV PRESS
DOI: 10.1093/bjps/axi114
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Jereon Vink ([1993]) argued that there are two options for what he called a realistic solution to the quantum measurement problem: (1) select a preferred set of observables for which definite values are assumed to exist, or (2) attempt to assign definite values to all observables simultaneously (1810-1). While conventional wisdom has it that the second option is ruled out by the Kochen-Specker theorem, Vink nevertheless advocated it. Making every physical quantity determinate in quantum mechanics carries with it significant conceptual costs, but it also provides a way of addressing the preferred basis problem that arises if one chooses to pursue the first option. The potential costs and benefits of a formulation of quantum mechanics where every physical quantity is determinate are herein examined. 1 The preferred-basis problem 2 How to solve the preferred-basis problem 3 Relativistic constraints 4 Conclusion.
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