Harmonic Oscillator Expectation Values

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SUMMARY

The discussion focuses on calculating the time-dependent expectation values and

for a particle in a harmonic oscillator potential described by the wave packet |\Psi (x,t)|^2 = \left(\frac{m\omega}{\pi\hbar}\right)^{1/2}\textrm{exp}\left[-\frac{mw}{\hbar}(x - a\textrm{cos}\omega t)^2\right]. Participants suggest using Ehrenfest's theorem and raising/lowering operators to simplify the calculations. The integral for is identified as complex, with participants discussing substitution methods to evaluate it effectively.

PREREQUISITES
  • Understanding of harmonic oscillator potential in quantum mechanics
  • Familiarity with wave functions and probability densities
  • Knowledge of Ehrenfest's theorem
  • Experience with integration techniques in quantum mechanics
NEXT STEPS
  • Study the application of Ehrenfest's theorem in quantum mechanics
  • Learn about raising and lowering operators in quantum harmonic oscillators
  • Practice evaluating integrals involving Gaussian functions
  • Explore the properties of Hermite polynomials and their role in quantum states
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Students of quantum mechanics, physicists working with harmonic oscillators, and anyone interested in calculating expectation values in quantum systems.

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Homework Statement


A particle of mass m that is confined to a harmonic oscillator potential V(x) = \frac{1}{2} m \omega^2 x^2 is described by a wave packet having the probability density,

|\Psi (x,t) |^2 = \left(\frac{m\omega}{\pi\hbar} \right )^{1/2}\textrm{exp}\left[-\frac{mw}{\hbar}(x - a\textrm{cos}\omega t)^2 \right ]

where \omega is a constant angular frequency and a is a positive real constant.

Calculate the time-dependent expectation values <x> and <p>. [Hint: Use Ehrenfest's theorem]

Homework Equations


d<x>/dt = <p/m>

The Attempt at a Solution


I'm not quite sure where to begin attacking this problem. I feel that if I can calculate <x>, then <p> should be easy given the equation above. I was thinking of trying the raising/lowering operators. Can I assume the particle is in the ground state since the only Hermite polynomial in \Psi is H_0 = 1? Is there an easier approach to this problem? I tried just calculating <x> using
\int \limits_{-\infty}^{\infty} \Psi(x,t)x\Psi^*(x,t)\textrm{d}x
but that was getting out of control fairly quickly.
 
Last edited:
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That integral is pretty straightforward to do with a simple substitution. What did you try?
 
I tried expanding the exponent term and couldn't find a way to integrate by parts that made it simpler. Looking at it again, would the simple substitution be u=(x - a*cos[wt]), du=dx?

Thanks for your reply!
 

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