Gaussian wavefunction; expectation energy

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SUMMARY

The discussion focuses on calculating the expectation value of energy, denoted as , using the Gaussian wavefunction in quantum mechanics. The operator for the Hamiltonian is defined as = / 2m, where represents the momentum squared. The key insight provided is that the momentum operator, p, is proportional to the derivative with respect to position, specifically p ∝ ∂/∂x, which simplifies the calculation of using the integral = ∫ ψ* Ĥ ψ dx.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically wavefunctions and operators.
  • Familiarity with the Hamiltonian operator and its role in quantum systems.
  • Knowledge of integration techniques in the context of quantum mechanics.
  • Basic understanding of the momentum operator in the position representation.
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  • Study the derivation of the Hamiltonian operator in quantum mechanics.
  • Learn about the properties of Gaussian wavefunctions and their applications.
  • Explore the concept of expectation values in quantum mechanics.
  • Investigate the relationship between momentum and position operators in quantum systems.
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Students and professionals in quantum mechanics, particularly those working with wavefunctions and energy calculations, will benefit from this discussion.

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Homework Statement



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Homework Equations


The Attempt at a Solution



The issue I'm having here is that the problem should be able to be done rather quickly. I can see how to solve for <H> using the operator, but there's a quick way that I'm not picking up on.

I thought about solving <H> = <p^2> / 2m, but getting <p^2> is just as much of a pain.

Any help ?
 
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By definition,

\langle H \rangle = \int \psi^* \hat H \psi \, dx
where, as you said
\hat H = \frac{p^2}{2m}

and you should be able to do that using the second hint (remember that p \propto \partial/\partial x in the position representation).
 

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