From the number operator commutator ,
so is proportional to . Its squared norm is
With the conventional phase choice,
Orthogonality of the energy eigenstates gives
Using the lowering-operator action from part (a) and shifting the summation index,
Thus this coherent state is a normalized eigenstate of with eigenvalue .
The number probabilities are
a Poisson distribution of parameter . Hence
The relative uncertainty is , which tends to zero as the mean occupation tends to infinity.
The quantum harmonic oscillator Hamiltonian is
. Therefore
so the evolved state remains an -eigenstate, with eigenvalue
.
The coherent-state overlap gives
For the classical period , this probability equals one whenever .

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