In some interpretations of quantum mechanics, counterfactual definiteness (CFD) is the ability to speak meaningfully about the definiteness of the results of measurements, even if they were not performed.[1]
For example, by the Heisenberg uncertainty principle, one cannot simultaneously know the position and momentum of a particle. Suppose one measures the position: this act destroys any information about the momentum. The question then becomes: is it possible to talk about the outcome one would have received if one did measure the momentum instead of the position? In other words, had one conducted a different experiment, is there a single alternate time line that would have resulted from it?
Counterfactual definiteness is a basic assumption, which, together with locality, leads to Bell inequalities. In their derivation it is explicitly assumed that every possible measurement, even if not performed, would have yielded a single definite result. Bell's Theorem actually proves that every quantum theory must violate either locality or CFD.[2][3]
CFD is always present in the hidden variables interpretations.[citation needed] However CFD is not a property of the Copenhagen interpretation of quantum mechanics, as the complementarity principle is directly excluding it.[citation needed] CFD also is not a property of the many worlds interpretation with its multiplicity of results in different worlds or elements of the universal wavefunction.[citation needed] It is not a property of some other decoherent interpretations such as consistent histories.[citation needed]
See also
External links and resources
- Quantum nonlocality without counterfactual definiteness?
- On Some Consequences of the Breakdown of Counterfactual Definiteness in the Quantum World by W. De Baere
- On Bell and CFD by W. M. de Muynck1, W. De Baere, and H. Martens
- google books on CFD
- CFD by Brian Skyrms
- CFD by Stapp (1988) and 1990
References
- ^ Henry P Stapp S-matrix interpretation of quantum-theory Physical Review D Vol 3 #6 1303 (1971)
- ^ David Z Albert, Bohm's Alternative to Quantum Mechanics Scientific American (May 1994)
- ^ John G. Cramer The transactional interpretation of quantum mechanics Reviews of Modern Physics Vol 58, #3 pp.647-687 (1986)
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