Kalidor
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Consider the usual 1D quantum harmonic oscillator with the typical hamiltonian in P and X and with the usual ladder operators defined.
i) I have to prove that given a generic wave function [itex]\psi[/itex], [itex]\partial_t < \psi (t) |a| \psi (t)>[/itex] is proportional to [itex]< \psi (t) | a | \psi (t) >[/itex] and determine their ratio.
Here I tried to express [itex]\psi(t)[/itex] as an infinite sum of the eigenstates with time evolution operator applied to it but I think there must definitely be some less clumsy way.
ii) Construct an operator [itex]Q_k[/itex] such that it only allows transitions between the states [itex]|n>[/itex] and [itex]|n \pm k >[/itex] ([itex]|n>[/itex] being the nth eigenstate of the N operator).
In this question I really did not get why the answer couldn't just be [itex]a[/itex] or [itex]a^_\dagger[/itex].
Thanks in advance
i) I have to prove that given a generic wave function [itex]\psi[/itex], [itex]\partial_t < \psi (t) |a| \psi (t)>[/itex] is proportional to [itex]< \psi (t) | a | \psi (t) >[/itex] and determine their ratio.
Here I tried to express [itex]\psi(t)[/itex] as an infinite sum of the eigenstates with time evolution operator applied to it but I think there must definitely be some less clumsy way.
ii) Construct an operator [itex]Q_k[/itex] such that it only allows transitions between the states [itex]|n>[/itex] and [itex]|n \pm k >[/itex] ([itex]|n>[/itex] being the nth eigenstate of the N operator).
In this question I really did not get why the answer couldn't just be [itex]a[/itex] or [itex]a^_\dagger[/itex].
Thanks in advance