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Volumn 67, Issue 4, 2003, Pages 421031-4210312

Continuous quantum measurement and the quantum to classical transition

Author keywords

[No Author keywords available]

Indexed keywords

ATOMIC PHYSICS; CHAOS THEORY; ELECTROMAGNETISM; STATISTICAL METHODS;

EID: 0038308838     PISSN: 10502947     EISSN: None     Source Type: Journal    
DOI: None     Document Type: Article
Times cited : (44)

References (45)
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    • note
    • 2/dt averaged over the noise dW is positive definite.
  • 35
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    • note
    • This follows most simply by treating each observer as having access to a separate output channel, or environment, but it is clear from [22] that one could obtain the same result by dividing up the available light using a sequence of beam splitters. For an explicit treatment of multiple observers see Ref. [23]. A recent and less mathematical treatment is also given in Ref. [24].
  • 36
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    • Ph.D. thesis, University of Queensland, Australia
    • H.M Wiseman, Ph.D. thesis, University of Queensland, Australia.
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  • 39
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    • unpublished
    • S. Habib (unpublished).
    • Habib, S.1
  • 40
    • 85015794485 scopus 로고    scopus 로고
    • note
    • Positivity at this second cumulant level does not require the noise term: the covariance matrix stays positive even without the addition of this piece.
  • 41
    • 85015770285 scopus 로고    scopus 로고
    • note
    • Since complex conjugation along with P → - P leaves the algebra [X,P] = iℏ unchanged, the momentum flip along with H → -H (i.e., m → -m and F → -F) and ρ → ρ* is an invariance of Eq. 3. Thus our results also apply to the negative mass case mutatis mutandis.


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