Perturbation theory infinite well

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SUMMARY

The discussion focuses on the application of perturbation theory to an infinite potential well, specifically analyzing the impact of a small potential on the total energy of the system. The total energy was calculated using the time-independent Schrödinger equation, yielding a result of E=h²/8mL² with an integral of ∫ ψkψ dx equal to zero. The participants concluded that the first-order correction in perturbation theory can indeed result in no change to the energy if the perturbation is symmetric and the wave function antisymmetric. However, the second-order correction, which accounts for changes in the wave function due to the modified potential, will yield a non-zero correction.

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  • Understanding of the time-independent Schrödinger equation
  • Familiarity with perturbation theory in quantum mechanics
  • Knowledge of wave functions and their properties
  • Basic calculus for evaluating integrals
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  • Study the implications of second-order perturbation theory in quantum mechanics
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Quantum mechanics students, physicists, and researchers interested in perturbation theory and its applications to potential wells.

Dammes
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in the infinite well with small potential shown in the attachment.
I calculated the total energy by using the time independent Schrödinger equation and adding the correction energy to the equation of the slope k=(Vo/L)x.

E=h^2/8mL^2 +∫ ψkψ dx

ψ=√(2/L) sin⁡(∏/L x)

when integrating ∫ ψkψ dx between 0 and L
I got Zero, ∫ ψkψ dx=0
∴ total energy=h^2/8mL^2 +0

so what i don't understand is when adding a small potential it doesn't affect the total energy of the system? that is what it shows when i integrated it.
 
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I suspect you've done the integral wrong. That said, it's perfectly possible for a perturbation to have no effect on the energy of any given state, especially if you only compute the change in energy to first order in perturbation theory.
 
With a symmetric density and an antisymmetric additional potential, the first order correction will be 0. The second order includes that the wave function changes (based on the modified potential), and that will give a non-zero correction.
 

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