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Hazz
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Homework Statement
I am a little confused about the how self consistency conditions work and I was wondering if in the following case I have correctly understood the details?
Homework Equations
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Say we have a harmonic oscillator with a perturbation
[itex] H=\frac{\hat{p}}{2m}+\frac{1}{2}m\omega^2\hat{q}^2+\gamma \hat{q}^4 [/itex]Say we want to perform something like a Hartree-Fock approximation. We replace the ## (a+a^\dagger)^4 ## in ##\hat{q}^4## with ## \langle (a+a^\dagger)^2 \rangle (a+a^\dagger)^2 ##. Say our new Hamiltonian is then
[itex] H_{HF}=\frac{\hat{p}}{2m}+\frac{1}{2}m\omega^2\hat{q}^2+\delta (a+a^\dagger)^2 [/itex]
with ##\delta=\gamma(\frac{\hbar}{2m\omega})^2\langle (a+a^\dagger)^2 \rangle##
The Attempt at a Solution
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This is now a quadratic Hamiltonian and can be diagonalised as
[itex] H= \sqrt{\frac{\hbar\omega}{2}(\frac{\hbar\omega}{2}+2\delta)}\hat{b}^\dagger \hat{b} [/itex]
Using this ##\langle (a+a^\dagger)^2 \rangle ## can be calculated and found to be[itex] \langle (a+a^\dagger)^2 \rangle = \frac{2n_B(\hbar\omega)-1}{\sqrt{\frac{\hbar\omega}{2}(\frac{\hbar\omega}{2}+2\gamma(\frac{\hbar}{2m\omega})^2\langle (a+a^\dagger)^2 \rangle)}} [/itex]
Am I correct in thinking this equation would be the self-consistency condition we are looking for? You could then plot the RHS and LHS with respect to ##\langle (a+a^\dagger)^2 \rangle ## and see where the lines cross, if they meet anywhere then the approximation is consistent?
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