Operator Bonanza

Suppose H ^ a ^ + ψ n = ( E n + h ω ) a ^ + ψ n \hat { H } { \hat { a } }_{ + }{ \psi }_{ n } = ({E}_{n}+h\omega) { \hat { a } }_{ + }{ \psi }_{ n } , where H ^ ψ n = E n ψ n \hat{H} {\psi}_{n} = {E}_{n} {\psi}_{n} and H ^ \hat{H} is a Hamiltonian operator for energy. Also, ψ n {\psi}_{n} is a completely valid quantum state.

What can one say about a ^ + ψ n {\hat{a}}_{+}{\psi}_{n} ?

It is a stationary state and it is proportional to ψ n {\psi}_{n} . Nothing can be said from the given information. It is a stationary state and it is not proportional to ψ n {\psi}_{n} . It is not a stationary state and so, must vary with time.

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1 solution

From the relation H ^ ψ n = E n ψ n \hat{H} {\psi}_{n} = {E}_{n} {\psi}_{n} , we can clearly see that ψ n {\psi}_{n} is an eigenfunction for the Hamiltonian operator H ^ \hat{H} , i.e. an operator for energy, and so, ψ n {\psi}_{n} is an energy eigenstate. Hence, it must be time independent and therefore, a stationary state.

Secondly, if we assume a ^ + ψ n {\hat{a}}_{+} {\psi}_{n} is directly proportional to ψ n {\psi}_{n} , we can write a ^ + ψ n = k ψ n {\hat{a}}_{+} {\psi}_{n} = k{\psi}_{n} , for some constant k k . But, this must imply that:

H ^ a ^ + ψ n = H ^ k ψ n = k H ^ ψ n \hat{H} {\hat{a}}_{+} {\psi}_{n} = \hat{H} k {\psi}_{n} = k \hat{H} {\psi}_{n}

Now, from the first relation, we can write, H ^ ψ n = E n ψ n \hat{H} {\psi}_{n} = {E}_{n} {\psi}_{n} , which gives us:

H ^ a ^ + ψ n = E n k ψ n = E n a ^ + ψ n \hat{H} {\hat{a}}_{+} {\psi}_{n} = {E}_{n} k{\psi}_{n} = {E}_{n} {\hat{a}}_{+} {\psi}_{n}

But, from the question, this is not true, as H ^ a ^ + ψ n = ( E n + ω ) a ^ + ψ n \hat{H} {\hat{a}}_{+} {\psi}_{n} = ({E}_{n} + \hbar \omega) {\hat{a}}_{+} {\psi}_{n}

Hence, by proof with contradiction, we can clearly say that, our initial assumption is wrong and so, a ^ + ψ n {\hat{a}}_{+} {\psi}_{n} is not directly proportional to ψ n {\psi}_{n} .

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