Time dependent dispersion (Quantum Mechanics)

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SUMMARY

The discussion focuses on determining the time-dependent variance \(\sigma(t)\) of a free particle's wave function, initially represented as a normalized Gaussian distribution. The relevant equation for the wave function is given by \(\Psi(x,t) = \int_{-\infty}^{\infty} a(k) e^{i(kx - \omega t)} dk\), where \(a(k) = \frac{A \sigma}{\sqrt{2\pi}} \exp\left[-\frac{(k - k_0)^2 \sigma^2}{2}\right]\). The solution for the variance over time is established as \(\sigma(t) = \sqrt{\sigma^2(0) + \left(\frac{\hbar t}{2m \sigma(0)}\right)^2}\). The discussion emphasizes the importance of determining the dispersion relation \(\omega(k)\) for accurate calculations.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly wave functions.
  • Familiarity with Gaussian distributions and their properties.
  • Knowledge of the dispersion relation in quantum mechanics.
  • Basic proficiency in integral calculus for evaluating wave function expressions.
NEXT STEPS
  • Study the derivation of the dispersion relation \(\omega(k)\) for free particles.
  • Learn about the implications of wave packet spreading in quantum mechanics.
  • Explore the mathematical techniques for evaluating integrals involving Gaussian functions.
  • Investigate the physical significance of time-dependent variance in quantum systems.
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Students and researchers in quantum mechanics, particularly those studying wave functions and dispersion in free particle systems.

emol1414
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Homework Statement


The initial wave function [itex]\Psi (x,0)[/itex] of a free particle is a normalized gaussian with unitary probability. Let [itex]\sigma = \Delta x[/itex] be the initial variance (average of the square deviations) with respect to the position; determine the variance [itex]\sigma (t)[/itex] in a moment later.

Homework Equations


I'm not sure which equations should I start from... but, as for a gaussian distribution, I'm thinking of
[itex]\Psi (x,t) = \int^{\infty}_{-\infty} a(k) e^{i(kx - \omega t)} dk[/itex],
being

[itex]a(k) = \frac{A \sigma}{\sqrt{2\pi}} \exp{\left[-\frac{(k - k_0)^2 {\sigma}^2}{2}\right]}[/itex]


The Attempt at a Solution


I don't know how to start it... once I describe the wave function, find A, I don't know how to construct this time dependent dispersion. I know the packet will 'spread', and its width will increase, but no ideas on how to describe this in terms of the dispersion... I know the result is [itex]\sigma (t) = \sqrt{\sigma^2(0) + (\frac{\hbar t}{2m \sigma(0)})^2}[/itex]
 
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Sorry you haven't gotten an answer on this yet, but if it's still relevant: I'd start by determining the dispersion relation [itex]\omega(k)[/itex] for the particle and plugging that in. The eventual goal is to take the explicitly time-dependent expression you have,
[tex]\Psi (x,t) = \int^{\infty}_{-\infty} a(k,\sigma) e^{i(kx - \omega t)} dk[/tex]
and rewrite it as an implicitly time-dependent expression
[tex]\Psi (x,t) = \int^{\infty}_{-\infty} a(k,\sigma(t)) e^{ikx} dk[/tex]
which should give you the expression you need.
 

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