Suppose a spinless particle is bound to a fixed center by a potential V(x) so asymmetrical that
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Suppose a spinless particle is bound to a fixed center by a potential V(x) so asymmetrical that no energy level is degenerate. Using time-reversal invariance prove ? 0
For any energy eigenstate. (This is known as quenching of orbital angular momentum.) If the wave function of such a nondegenrate eigenstate is expended as?
What kind of phase restrictions do we obtain on Flm(r)?
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l m
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