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Homework Statement
A particle of mass m is in a harmonic oscillator potential with spring constant k. An observable quantity is given in the Schrodinger picture by the operator:
[itex] Z = a^{\dagger}a a^{\dagger} a [/itex]
a) Determine the equation of motion of the operator in the Heisenberg picture
b) Solve the equation of motion to calculate the form of Z as a function of time.
Homework Equations
[itex]i\hbar \frac{dZ(t)}{dt} = [Z(t),H] [/itex]
[itex] Z(t) = U^{\dagger}ZU [/itex]
[itex] U = e^{-iHt/\hbar} [/itex]
[itex] <Z>_{t} = <\psi(x,0) | Z(t) |\psi(x,0)> [/itex]
The Attempt at a Solution
a)
From a textbook, it said the equation of motion for a time-independent operator (schrodinger picture) in the Heisenberg picture is:
[itex]i\hbar \frac{dZ(t)}{dt} = [Z(t),H] [/itex]
Where I am assuming [itex] H = \frac{p^2}{2m} + 1/2kx^2 [/itex] because it's a harmonic oscillator.
Is that it for this part of the problem? Just write it down? Seems a bit silly to me.
b)
This part is confusing to me. It asks for me to solve the equation of motion to get Z as a function of time. However, can't I just use
[itex] Z(t) = U^{\dagger}ZU [/itex]
[itex] U = e^{-iHt/\hbar} [/itex]
[itex] <Z>_{t} = <\psi(x,0) | Z(t) |\psi(x,0)> [/itex]
to obtain Z as a function of time? I assume this because I know with the creation and annihilation operators, I can act on [itex] <\psi(x,0)| [/itex] to (if I assume the ground state) eliminate some operators in Z(t).
Okay so this is the method I think I should go with??
writing out the last equation above, I get:
[itex] <Z>_{t} = <\psi(x,0) | U^{\dagger}ZU|\psi(x,0)> [/itex]
[itex] <Z>_{t} = <\psi(x,0) | U^{\dagger}a^{\dagger}a a^{\dagger} aU|\psi(x,0)> [/itex]
now I am stuck and not convinced i am going about this problem correctly.