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Journal of Physics A Mathematical and General

On shrinking and expansion of radial wave packets

Mauro Antonio ANDREATA, V. V. Dodonov

Published Jun 11, 2003• 10 citations
Publisher

Abstract

We study the effect of initial ‘shrinking’ of radial ‘ring-shaped’ wave packets with zero initial velocity distribution in two and more dimensions. Considering time evolution of probability densities described by explicit exact solutions of the free Schrödinger equation in d dimensions, we introduce and compare two different families of quantitative measures of ‘expansion’. The measures of the first type are based on the mean values of arbitrary powers of radius, they characterize the ‘total extension’ of the packet. The measures of the second type quantify the ‘internal’ size of the packet (or an effective width of the ‘ring’). We find that the effect of initial ‘in-spreading’, which is very small in two dimensions and absent in higher dimensions with respect to the mean value of radius, is much more pronounced, if one uses mean values of ⟨ r α ⟩ with α < 1 and especially α < 0 as the measure of packet extension. In this sense, the case of two dimensions is not distinguished, and shrinking packets exist in more than two dimensions, as well. On the other hand, we show that the effect of initial ‘shrinking’ or ‘expansion’ strongly depends on the chosen measure of spatial extension (‘total’ or ‘internal’) of the packet. Moreover, the conclusions concerning the initial evolution of the ‘internal’ packet extensions based on the ‘volume’ probability density |ψ| 2 may be sometimes opposite to the conclusions based on the ‘radial probability density’ r d −1 |ψ| 2 .

DOI
10.1088/0305-4470/36/25/314

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We study the effect of initial ‘shrinking’ of radial ‘ring-shaped’ wave packets with zero initial velocity distribution in two and more dimensions. Considering time evolution of probability densities described by explicit exact solutions of the free Schrödinger equation in d dimensions, we introduce and compare two different families of quantitative measures of ‘expansion’. The measures of the first type are based on the mean values of arbitrary powers of radius, they characterize the ‘total extension’ of the packet. The measures of the second type quantify the ‘internal’ size of the packet (or an effective width of the ‘ring’). We find that the effect of initial ‘in-spreading’, which is very small in two dimensions and absent in higher dimensions with respect to the mean value of radius, is much more pronounced, if one uses mean values of ⟨ r α ⟩ with α < 1 and especially α < 0 as the measure of packet extension. In this sense, the case of two dimensions is not distinguished, and shrinking packets exist in more than two dimensions, as well. On the other hand, we show that the effect of initial ‘shrinking’ or ‘expansion’ strongly depends on the chosen measure of spatial extension (‘total’ or ‘internal’) of the packet. Moreover, the conclusions concerning the initial evolution of the ‘internal’ packet extensions based on the ‘volume’ probability density |ψ| 2 may be sometimes opposite to the conclusions based on the ‘radial probability density’ r d −1 |ψ| 2 .
Standard eikonal methods, as asymptotic perturbation expansions in 1/\ensuremath{\Elzxh}, are incapable of describing fully the dispersive spreading of a wave packet. By simple models, we distinguish the two types of dispersion associated with a packet having initially uniform and nonuniform distributions of wave number. A nonperturbative extension of the eikonal approximation is applied to two initial-value problems for the free-particle Schr\"odinger equation and compared with exact solutions. The method maintains the ray picture fully. Applications of the method to more general classes of problems are discussed.
The propagation of an initially Gaussian wave packet of width [Formula: see text] in Gross–Pitaevskii equation is extensively studied both for attractive and repulsive interactions. It is predicted analytically and verified numerically that for a free particle with attractive interaction, the dynamics of the width is governed by an effective potential which is sensitive to initial conditions. If [Formula: see text] is equal to a corresponding critical width [Formula: see text], then the packet will propagate in time with very little change in shape. These are in essence like coherent states. Whereas, if [Formula: see text], depending on the nature of the effective potential for chosen [Formula: see text] and the interaction strength [Formula: see text], the width of the packet in course of time, either oscillates with bounded width or will spread like a free particle. For a simple harmonic oscillator (SHO) also, we find that for [Formula: see text] smaller than a critical value, there always exists a coupling strength for which the packet simply oscillates about the mean position without changing its shape, once again providing a resemblance to a coherent state. We also consider the Morse potential, which interpolates between the free particle and the oscillator. For large attractive interactions, the two limiting dynamics (free and simple harmonic) are indeed observed but in the intermediate form of the potential where the nonlinear terms dominate in the dynamics, an initial Gaussian wave packet does not retain its shape. For repulsive interaction, the Gaussian packet always changes shape no matter what the system parameters are.
We study two-dimensional quantum Gaussian packets with a fixed value of mean angular momentum. This value is the sum of two independent parts: the ‘external’ momentum related to the motion of the packet center and the ‘internal’ momentum due to quantum fluctuations. The packets minimizing the mean energy of an isotropic oscillator with the fixed mean angular momentum are found. They exist for ‘co-rotating’ external and internal motions, and they have nonzero correlation coefficients between coordinates and momenta, together with some (moderate) amount of quadrature squeezing. Variances of angular momentum and energy are calculated, too. Differences in the behavior of ‘co-rotating’ and ‘anti-rotating’ packets are shown. The time evolution of rotating Gaussian packets is analyzed, including the cases of a charge in a homogeneous magnetic field and a free particle. In the latter case, the effect of initial shrinking of packets with big enough coordinate-momentum correlation coefficients (followed by the well known expansion) is discovered. This happens due to a competition of ‘focusing’ and ‘de-focusing’ in the orthogonal directions.
We discuss four general features of the force-free evolution of wave packets: (1) The spatial spread of a packet changes with time in a simple way. (2) For sufficiently short durations (related to the spread in the momentum of the packet) the probability distribution will move with uniform speed and little change in shape. (3) After a sufficiently long time (related to the initial spatial spread) the wave function converges to a simple form that is simply related to the momentum distribution of the packet. In this asymptotic regime the shape of the probability distribution no longer changes, and its scale increases linearly with the time. (4) There is an infinite denumerable set of simple wave packets (the Hermite-Gauss packets) that do not change shape at any time during their evolution.
Time evolution of radial wave packets built from the eigenstates of Dirac equation for a hydrogenic system is considered. Radial wave packets are constructed from the states of different n quantum numbers and the same lowest angular momentum. In general they exhibit a kind of breathing motion with dispersion and (partial) revivals. Calculations show that for some particular preparations of the wave packet one can observe interesting effects in spin motion, coming from inherent entanglement of spin and orbital degrees of freedom. These effects manifest themselves through some oscillations in the mean values of spin operators and through changes of spatial probability density carried by upper and lower components of the wave function. It is also shown that the characteristic time scale of predicted effects (called T ls ) is much smaller for radial wave packets than in other cases, reaching values comparable to (or even less than) the time scale for the wave packet revival.