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Journal of the Physical Society of Japan

Characterization of the Power Decays of Survival Probabilities at Long Times for Free Quantum Particle System

Manabu Miyamoto

Published Jan 1, 2003• 0 citations
Publisher

Abstract

The power-law decrease of the survival probability S ( t ) at long times for the one-dimensional free-particle system is shown to be characterized by the small-momentum behavior of the initial wave packet. We consider and compare the result based on the resolvent analysis and that on the asymptotic method of the Fourier integral, where the effect of a specialty of a one-dimensional free resolvent and that of the discontinuity of initial states at zero momentum on the behavior of S ( t ) are pointed out.

DOI
10.1143/jpsjs.72sc.69

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The power-law decrease of the survival probability S ( t ) at long times for the one-dimensional free-particle system is shown to be characterized by the small-momentum behavior of the initial wave packet. We consider and compare the result based on the resolvent analysis and that on the asymptotic method of the Fourier integral, where the effect of a specialty of a one-dimensional free resolvent and that of the discontinuity of initial states at zero momentum on the behavior of S ( t ) are pointed out.
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The behavior of both the survival S(t)S(t)S(t) and the nonescape P(t)P(t)P(t) probabilities at long times for the one-dimensional free-particle system is shown to be closely connected to that of the initial wave packet at small momentum. We prove that both S(t)S(t)S(t) and P(t)P(t)P(t) asymptotically exhibit the same power-law decrease at long times, when the initial wave packet in momentum representation behaves as km{k}^{m}km with m=0m=0m=0 or 111 at small momentum. On the other hand, if the integer m becomes greater than 1,1,1, S(t)S(t)S(t) and P(t)P(t)P(t) decrease in different power laws at long times.
A family of wave packets with power law tails are employed to analyze the long time dependence of the corresponding probability density. The densities, associated to packets for free particles in the one-dimensional space, with sufficiently long tails decay asymptotically in time following a t−βt^{-β}t−β law (with β<1β<1β<1), slower than the usual t−1t^{-1}t−1 one, including the particular case (lnt)2/t(ln t)^2/t(lnt)2/t not correctly discussed in F. Lillo and R. N. Mantegna (Phys. Rev. Lett. 84, 1061 (2000)).
We consider a hypothetical experiment where a particle is released at time t=0t=0t=0 in a fixed initial state. A detector makes instantaneous quantum measurements at regular intervals of time τ\tauτ, and keeps doing so till it detects the particle, say on the nthn^{\rm th}nth observation, at time t=nτt=n\taut=nτ. We take τ\tauτ to be small but do not take the limit of continuous measurements τ→0\tau\to 0τ→0. We examine the survival probability P(t)P(t)P(t) that the particle is un-detected till time ttt. Here we present results for a simple model of a free particle in a one-dimensional box and find that interesting features such as power-law tails are obtained for the survival probability. We provide a perturbative calculation which compares very well with numerical results. Some exact results are obtained for a mean-field model. In the limit of continuous observations, as expected, one always gets a Zeno-like effect where the particle is never detected.
The long-time behavior of scattered wave packets $\ensuremath{\psi}(x,t)$ from a finite-range potential is investigated, by assuming $\ensuremath{\psi}(x,t)$ to be initially located outside the potential. It is then shown that $\ensuremath{\psi}(x,t)$ can asymptotically decrease in the various power laws at long time, according to its initial characteristics at small momentum. As an application, we consider the square-barrier potential system and demonstrate that $\ensuremath{\psi}(x,t)$ exhibits the asymptotic behavior ${t}^{\ensuremath{-}3∕2}$, while another behavior like ${t}^{\ensuremath{-}5∕2}$ can also appear for another $\ensuremath{\psi}(x,t)$.
The time behavior of a wave packet, transmitted through a potential barrier, is investigated for all times assuming it to be initially located outside the asymmetric barrier. The survival probability of the initial state, which characterizes the decay of the unstable quantum system in three time domains, is discussed. The presence of initial, exponential, and long-time regimes is a general feature of the decay process. We analytically found the three crucial points of time that separate these regimes. These characteristic times are set by simple formulae, including momentum distribution. It is then shown that the radius of convergence of the cumulant expansion for the survival probability is always small. A long-time behavior of survival probability is described by the asymptotic series whose coefficients decrease with increasing particle energy but at different rates. To be specific, we have examined the exactly solvable model of tunneling through a finite range triangular barrier.