Use zero-based labels to agree with in the later parts. The normalized infinite square well energy eigenstates and energy eigenvalues areThe position matrix elements in a symmetric infinite square well, obtained by integrating the product of the two wavefunctions against , areThe integral in the question uses positive integer labels; replacing them by is essential here. Only opposite-parity states, odd, contribute, as also follows from the parity operator selection rule.
Second-order nondegenerate perturbation theory now gives the requested infinite sum:In fully explicit form this isThe symbol here denotes the electron mass, not a summation index. For the ground state , every denominator in the first form is negative, so the ground energy level moves downward. For excited states, contributions from lower and higher energy levels have opposite signs.
Articles by others on the same topic
There are currently no matching articles.