Consider an electron trapped in a one-dimensional harmonic potential and it is subjected to an external electric field to the right with a magnitude of Ɛ. The Hamiltonian for this system is given as: ÂĤ = ² + + eɛâ . %3D 2m 2 ) Treating eɛâ as a perturbation, and using non-degenerate perturbation theory, calculate the first order shift in energy for the n-th quantum state, where |Øn) are the exact energy eigenstates of the unperturbed system (i.e. when the electric field is zero). a b) ( ) Repeat part (a) except now calculate the shift in energy accurate to second order.
Consider an electron trapped in a one-dimensional harmonic potential and it is subjected to an external electric field to the right with a magnitude of Ɛ. The Hamiltonian for this system is given as: ÂĤ = ² + + eɛâ . %3D 2m 2 ) Treating eɛâ as a perturbation, and using non-degenerate perturbation theory, calculate the first order shift in energy for the n-th quantum state, where |Øn) are the exact energy eigenstates of the unperturbed system (i.e. when the electric field is zero). a b) ( ) Repeat part (a) except now calculate the shift in energy accurate to second order.
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