1999
DOI: 10.1016/s0375-9601(99)00323-0
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Berry phase from a quantum Zeno effect

Abstract: We exhibit a specific implementation of the creation of geometrical phase through the state-space evolution generated by the dynamic quantum Zeno effect. That is, a system is guided through a closed loop in Hilbert space by means a sequence of closely spaced projections leading to a phase difference with respect to the original state. Our goal is the proposal of a specific experimental setup in which this phase could be created and observed. To this end we study the case of neutron spin, examine the practical … Show more

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Cited by 39 publications
(37 citation statements)
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References 19 publications
(19 reference statements)
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“…At the same time, the dynamics of system B becomes unitary in this limit, and this is an example of the so-called "quantum Zeno dynamics" [12]. However, we stress that our interest lies in a different situation: we keep the time interval τ between measurements finite and nonvanishing.…”
mentioning
confidence: 97%
“…At the same time, the dynamics of system B becomes unitary in this limit, and this is an example of the so-called "quantum Zeno dynamics" [12]. However, we stress that our interest lies in a different situation: we keep the time interval τ between measurements finite and nonvanishing.…”
mentioning
confidence: 97%
“…This is an example of the so-called "quantum Zeno dynamics." 12,14,15) We are however interested in a different situation: we repeat the measurement with a nonvanishing (not necessarily small) τ . The probability P (τ ) (N ) would decay out completely for such a finite τ , but we are interested in the asymptotic behavior of the state of system B, ρ In order to clarify the evolution of system B under the Zeno-like measurement on system A, let us consider the eigenvalue problem of the projected time-evolution operator V φ (τ ).…”
Section: )mentioning
confidence: 99%
“…We let the total system evolve with the Hamiltonian (14) and confirm repeatedly at regular intervals τ that oscillator a is in the coherent state |α . The time-evolution operator (between adjacent measurements), e −iHτ , is calculated exactly to be (15) in terms of the τ -dependent functions…”
Section: )mentioning
confidence: 99%
“…A special kind of experimentations which attract many discussions by many authors (Aharono and Vardi, 1980;Bixon, 1982;Chiu et al, 1977;Facchi et al, 1999;Giulini et al, 1996;Itano et al, 1990;Kofman and Kurizki, 1996;Kurizki et al, 1995;Misra and Sudarshan, 1977;Pascazio and Namiki, 1994;Peres, 1989;Peres and Ron, 1990;Simonius, 1978;Wilkinson et al, 1997) are those in which a large number of experiments are involved. Among these one may note the special role played by those in which the time duration of each of the involved experiments tends to become infinitesimally small.…”
Section: Introductionmentioning
confidence: 99%