How to Calculate Expectation Values in Spherical Coordinates?

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SUMMARY

To calculate expectation values in spherical coordinates, one must express the wave function, Ψ, in terms of spherical coordinates (r, θ, φ). The expectation value is computed using the integral formula: <A> = ∫(Volume) ψ*(r, θ, φ)∆Aψ(r, θ, φ), where ∆A is the operator corresponding to the observable A. This method is particularly relevant in problems involving spherical symmetry, such as potential wells.

PREREQUISITES
  • Understanding of wave functions in quantum mechanics
  • Familiarity with spherical coordinates (r, θ, φ)
  • Knowledge of Schrödinger's equation
  • Basic concepts of quantum operators
NEXT STEPS
  • Study the derivation of wave functions in spherical coordinates
  • Learn about potential wells in quantum mechanics
  • Explore the application of quantum operators in expectation value calculations
  • Investigate examples of spherical symmetry in quantum systems
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Students and professionals in physics, particularly those focusing on quantum mechanics, as well as researchers working on problems involving spherical symmetry and potential wells.

M. next
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Hey,

can you explain how to find expectation value in spherical coordinates?
and give me a numeric example?

to make this clearer, if we considered potential wells..
how can this question be included in such an exercise?


thanks loads, answer as much as you can.. whatever comes to mind
 
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Without further information, all I can say is you find expecation values pretty much the same way you usually do. For example:
[tex] \langle A \rangle = \int_{\sigma} \Psi^{*}\hat{A}\Psi[/tex]
however you will want [itex]\Psi[/itex] to be in spherical coordinates. In other words, you want your solution to Schrödinger's equation to reflect the symmetry of the problem (which I imagine is spherical). For instance if you are working in 3D:
[tex] \langle A \rangle = \int_{\text{Volume}} \psi^{*}(r,\theta,\phi)\hat{A}\psi(r,\theta,\phi)[/tex]
will give you the expectation value of [itex]A[/itex].
 

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