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American Journal of Physics

A new look at quantal time evolution

Aparajita Bhattacharyya, Jayanta K. Bhattacharjee, Debabrata Sinha

Published May 21, 2021• 3 citations
Publisher

Abstract

Time evolution of quantum systems is normally taught using the Schrödinger equation. Here, we use the Heisenberg approach to consider three problems that are exactly solvable in the Schrödinger picture when the initial wavepacket is Gaussian: the free particle, the simple harmonic oscillator and a free particle with a spin-orbit interaction. We show that complete solutions can be obtained for the free particle (with or without spin-orbit interaction). For the simple harmonic oscillator, however, the fact that the wavepacket remains a Gaussian as time progresses has to be inferred on the basis of the skewness and kurtosis as opposed to a study of all the relevant moments.

DOI
10.1119/10.0003397

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Time evolution of quantum systems is normally taught using the Schrödinger equation. Here, we use the Heisenberg approach to consider three problems that are exactly solvable in the Schrödinger picture when the initial wavepacket is Gaussian: the free particle, the simple harmonic oscillator and a free particle with a spin-orbit interaction. We show that complete solutions can be obtained for the free particle (with or without spin-orbit interaction). For the simple harmonic oscillator, however, the fact that the wavepacket remains a Gaussian as time progresses has to be inferred on the basis of the skewness and kurtosis as opposed to a study of all the relevant moments.
The free expansion of a Gaussian wavepacket is a problem commonly discussed in undergraduate quantum classes by directly solving the time-dependent Schrödinger equation as a differential equation. In this work, we provide an alternative way to calculate the free expansion by recognizing that the Gaussian wavepacket can be thought of as the ground state of a harmonic oscillator with its frequency adjusted to give the initial width of the Gaussian, and the time evolution, given by the free-particle Hamiltonian, being the same as the application of a time-dependent squeezing operator to the harmonic oscillator ground state. Operator manipulations alone (including the Hadamard lemma and the exponential disentangling identity) then allow us to directly solve the problem. As quantum instruction evolves to include more quantum information science applications, reworking this well-known problem using a squeezing formalism will help students develop intuition for how squeezed states are used in quantum sensing.
We show that one can obtain analytic solutions of the time-dependent Schrödinger equation that are more complex than the well-known oscillating coherent wave packet. Such Hermite-Gaussian or initially square wave packets exist for a free particle or for one subject to the harmonic oscillator potential. In either case, the Hermite-Gaussian packets retain their nodal structure even after long times. There is a single class of exact solutions for the system with oscillator constant K > 0, K = 0, or K < 0, leading to wave functions for the harmonic oscillator, the free particle, and the inverted oscillator, respectively.
Until now, we have been working with time-independent states. The real world is dynamic and it changes from one time to another. The quantum world provides a basis for the real world, so it has dynamics too. In this chapter, we discuss the time evolution of quantum states. It may surprise you to learn that many research problems in quantum mechanics involve trying to understand the time evolution of complex quantum states. We still do not have an efficient way to determine the dynamical properties of complicated quantum-mechanical systems. You will get your first taste of how we describe time variation of quantum states in this chapter and why the analysis can get complicated. The specific topics covered include the Trotter product formula, magnetic resonance and MRI, the harmonic oscillator, the free expansion of a Gaussian wavepacket, the interaction representation, the Landau-Zener problem, the driven harmonic oscillator, photoproduction of hydrogen, and the XY model as a stroboscopic Ising model.