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Volumn 66, Issue 5, 1998, Pages 396-402

The uncertainty principle for energy and time. II

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EID: 0032389967     PISSN: 00029505     EISSN: None     Source Type: Journal    
DOI: 10.1119/1.18880     Document Type: Article
Times cited : (58)

References (32)
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    • note
    • With Bohr the symbol Δ does not denote the standard deviation but some unspecified relevant measure of width.
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    • note
    • It should be noted that, even when the states are orthogonal, a measurement of φ may not be capable of distinguishing with certainty between them, i.e., the distributions of φ values in the two states may still overlap. For example, a measurement of the spin component of a spin one-half particle in any direction other than the z direction does not allow one to distinguish with certainty between the two orthogonal eigenstates of the spin in the z direction. However, a measurement of the spin component in the z direction does. Generally, if two states are orthogonal, there are variables a measurement result of which enables one to distinguish with certainty between the states.
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    • The uncertainty principle for energy and time
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    • This article is reprinted in J. A. Wheeler and W. H. Zurek, Quantum Theory and Measurement (Princeton U.P., Princeton, 1983), pp. 9-52, and in Niels Bohr, Collected Works, edited by J. Kalckar (Elsevier, Amsterdam, 1996), Vol. 7, pp. 339-381.
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    • edited by J. Kalckar (Elsevier, Amsterdam)
    • This article is reprinted in J. A. Wheeler and W. H. Zurek, Quantum Theory and Measurement (Princeton U.P., Princeton, 1983), pp. 9-52, and in Niels Bohr, Collected Works, edited by J. Kalckar (Elsevier, Amsterdam, 1996), Vol. 7, pp. 339-381.
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    • In Ref. 3, pp. 224-228
    • In Ref. 3, pp. 224-228.
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    • This is Fig. 8 of Ref. 3
    • This is Fig. 8 of Ref. 3.
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    • edited by J. Kalckar (Elsevier, Amsterdam)
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    • In Ref. 3, p. 215
    • In Ref. 3, p. 215.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.