A particle of charge q in 1-Dim. is in a simple harmonic potential with angular frequency...

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A particle of charge q in 1-Dim. is in a simple harmonic potential with angular frequency w. It is subjected to a time dependent electric field E(t)=A e^-(lembda(t))^2 where A & lembda are positive integers constants of wt < <1. If in the distant past particle was in its ground state, the probability that it will be in the first excited state as lembda--> infinity is proportional to: A particle of charge q in 1-Dim. is in a simple harmonic potential with angular frequency w. It is subjected to a time dependent electric field E(t)=A e^-(lembda(t))^2 where A & lembda are positive integers constants of wt < <1. If in the distant past particle was in its ground state, the probability that it will be in the first excited state as lembda--> infinity is proportional to:

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