(a) Derive the following general relation for the first order correction to the energy, E, in time-independent perturbation theory %3D where the y are the eigen-functions of the unperturbed Hamiltonian Ho and H' is the time independent perturbation. (b) A particle moves in a potential given by Vo sin(ax/a) for 0 < x < a V = otherwise where Vo is a small constant. Treat this as a perturbation for the case of a particle in an infinitely deep square well of width a and calculate the change in energy of the lowest energy state to first order in Vo.

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(a) Derive the following general relation for the first order correction to the energy,
E, in time-independent perturbation theory
where the 0 are the eigen-functions of the unperturbed Hamiltonian Ho and H'
is the time independent perturbation.
(b) A particle moves in a potential given by
Vo sin(ax/a) for 0 < x < a
V :
%D
otherwise
where Vo is a small constant. Treat this as a perturbation for the case of a particle
in an infinitely deep square well of width a and calculate the change in energy of
the lowest energy state to first order in Vo.
Transcribed Image Text:(a) Derive the following general relation for the first order correction to the energy, E, in time-independent perturbation theory where the 0 are the eigen-functions of the unperturbed Hamiltonian Ho and H' is the time independent perturbation. (b) A particle moves in a potential given by Vo sin(ax/a) for 0 < x < a V : %D otherwise where Vo is a small constant. Treat this as a perturbation for the case of a particle in an infinitely deep square well of width a and calculate the change in energy of the lowest energy state to first order in Vo.
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