Page 13 - Physlets and Open Source Physics for Quantum Mechanics:
P. 13

Appendix

                 Wave Packet Revivals: Theory

                 Quantum-mechanical wave packet revivals have recently  received considerable
                 theoretical and experimental attention [29].   Most  often the theoretical research has
                 focused on initially localized wave packets in the infinite square well (ISW) because of
                 its well-known time scales: the classical time scale and the revival time scale.  We
                 examine the time dependence of  such an  initially localized state by choosing  a
                 standard Gaussian wave packet of the form



                                                                                         (A1)


                 where by direct calculation: <x> t = 0 = x 0, <p> t = 0 = p 0, and ∆x t =  0 = ∆x 0 = b/√2.  The
                 wave packet can be constructed from a sum of energy eigenstates as:


                                                                                         (A2)


                                                            2
                 where the expansion coefficients satisfy Σ n |c n|  = 1.  The expansion coefficients are
                 determined by an ‘overlap’ integral of the individual energy eigenstates with the initial
                 Gaussian wave packet.

                 We find that over time the wave packet spreads in a characteristic way defined by the
                                       2
                 spreading time, t 0 = mb /ħ.  For longer times, we have the so-called classical period,
                 T cl, and the revival time, T rev, which are related to each other by:


                                                         2
                         T rev = 2πħ/|E''(n 0)|/2 = 2πħ/E 0 = 4mL /πħ = 2n 0 T cl.                 (A3)


                 The classical periodicity for the ISW agrees with the classically-expected result (T cl =
                 2L/v  which  corresponds to the time it takes a  classical  particle to traverse the well
                 twice). The so-called initial ‘bounce’ at T cl/4 with one wall is of interest because of the
                 similarities and differences between the classical and quantum-mechanical cases [21,
                 22].  Also of interest in the context of the ISW, but on a considerably longer time scale
                 than the classical time scale, are the well-known exact, mirror, and fractional revivals
                 [26-28] in which the wave packet or copies (sometimes called ‘mini-packets’ or ‘clones’)
                 of the original wave  packet reform long after the  original packet ‘collapses.’  The
                 analysis of these problems often requires specialized visualization techniques because
                 of the long times involved.



                 References

                 [1] E. Cataloglu and R. Robinett, “Testing the Development of Student Conceptual and
                 Visualization Understanding in Quantum Mechanics through the Undergraduate
                 Career,” American Journal of Physics, 70, 238-251 (2002).

                 [2] M. Belloni and W. Christian,  “Physlets for Quantum Mechanics,”  Computing in
                 Science and Engineering  5, 90 (2003). The Physlet-based quantum mechanics
                 exercises from this paper are available at: http://webphysics.davidson.edu/cise_qm.
   8   9   10   11   12   13   14   15