Complementarity of representations in quantum mechanics
Studies in History and Philosophy of Science Part B 35 (1):45-56 (2004)
| Abstract | We show that Bohr's principle of complementarity between position and momentum descriptions can be formulated rigorously as a claim about the existence of representations of the CCRs. In particular, in any representation where the position operator has eigenstates, there is no momentum operator, and vice versa. Equivalently, if there are nonzero projections corresponding to sharp position values, all spectral projections of the momentum operator map onto the zero element. | |||||||||
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Leon Cohen (1966). Can Quantum Mechanics Be Formulated as a Classical Probability Theory? Philosophy of Science 33 (4):317-322.
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Hans Halvorson & Rob Clifton (1999). Maximal Beable Subalgebras of Quantum-Mechanical Observables. International Journal of Theoretical Physics 38:2441-2484.
Yuichiro Kitajima (2005). Interpretations of Quantum Mechanics in Terms of Beable Algebras. INTERNATIONAL JOURNAL OF THEORETICAL PHYSICS 44 (8):1141-1156.
Paul Busch & Pekka J. Lahti (1985). A Note on Quantum Theory, Complementarity, and Uncertainty. Philosophy of Science 52 (1):64-77.
Hans Halvorson (2001). On the Nature of Continuous Physical Quantities in Classical and Quantum Mechanics. Journal of Philosophical Logic 30 (1):27-50.
Hans Halvorson (2001). On the Nature of Continuous Physical Quantities in Classical and Quantum Mechanics. Journal of Philosophical Logic 30 (1):27-50.
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