Tomaž Prosen and Marko Žnidarič
Physics Department, Faculty of Mathematics and Physics, University of Ljubljana, Ljubljana, Slovenia
Tomaž Prosen and Marko Žnidarič 2003 New J. Phys. 5 109
We discuss quantum fidelity decay of classically regular dynamics, in particular for an important special case of a vanishing time-averaged perturbation operator, i.e. vanishing expectation values of the perturbation in the eigenbasis of unperturbed dynamics. A complete semiclassical picture of this situation is derived in which we show that the quantum fidelity of individual coherent initial states exhibits three different regimes in time: (i) first it follows the corresponding classical fidelity up to time
, (ii) then it freezes on a plateau of constant value, (iii) and after a timescale
it exhibits fast ballistic decay as
where
is a strength of perturbation. All the constants are computed in terms of classical dynamics for sufficiently small effective value
of the Planck constant. A similar picture is worked out also for general initial states, and specifically for random initial states, where
, and
. This prolonged stability of quantum dynamics in the case of a vanishing time-averaged perturbation could prove to be useful in designing quantum devices. Theoretical results are verified by numerical experiments on the quantized integrable kicked top.
81S30 Phase space methods including Wigner distributions, etc.
81Q15 Perturbation theories for operators and differential equations
81R30 Coherent states (See also 22E45); squeezed states (See also 81V80)
81Q20 Semiclassical techniques including WKB and Maslov methods
Issue 1 (August 2003)
Received 27 June 2003
Published 21 August 2003
Tomaž Prosen and Marko Žnidarič 2003 New J. Phys. 5 109
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