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quantum539
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Hi, I am trying to find the wavefunction of a coherent state of the harmonic oscillator ( potential mw2x2/2 ) with eigenvalue of the lowering operator: b.
I know you can do this is many ways, but I cannot figure out why this particular method does not work.
It can be shown (and you can find this easily on the internet) that the eigenvalue b evolves as:
b(t)=b0e-iwtWhat I did was find the coherent state wavefunction u(x,t) by using the eigenfunction equation with the lowering operator a:
a[u(x,t)]=b*u(x,t)
with a=(mwx+(h-bar)*d/dx)/sqrt(2mw(h-bar))
that gives
u(x,t)=const*e-(1/l2)*(x-l*b)2
where l=sqrt(2(h-bar)/mw)
now, when I put in the time evolution of b I get:
u(x,t)=const*e-(1/l2)*(x-lb0e-iwt)2
(I plugged in b(t) from before in for b)
This state does not satisfy the schodinger equation, for one thing it cannot be normalized because the integral over all x of the norm squared of the wavefunction varies in time.
This confuses me because b(t) comes from treating the coherent state as a superposition of harmonic oscillator energy eigenstates, which come from the schrodinger equation. Since the schrodinger equation conserves the integral over all x of probability density, why do I get a state which does not do so from harmonic oscilator states (and thus, by extension, the schrodinger equation)?
Thanks so much in advance, I have done this over several times over the last day and cannot find out anything I did wrong nor a solution online.
I know you can do this is many ways, but I cannot figure out why this particular method does not work.
It can be shown (and you can find this easily on the internet) that the eigenvalue b evolves as:
b(t)=b0e-iwtWhat I did was find the coherent state wavefunction u(x,t) by using the eigenfunction equation with the lowering operator a:
a[u(x,t)]=b*u(x,t)
with a=(mwx+(h-bar)*d/dx)/sqrt(2mw(h-bar))
that gives
u(x,t)=const*e-(1/l2)*(x-l*b)2
where l=sqrt(2(h-bar)/mw)
now, when I put in the time evolution of b I get:
u(x,t)=const*e-(1/l2)*(x-lb0e-iwt)2
(I plugged in b(t) from before in for b)
This state does not satisfy the schodinger equation, for one thing it cannot be normalized because the integral over all x of the norm squared of the wavefunction varies in time.
This confuses me because b(t) comes from treating the coherent state as a superposition of harmonic oscillator energy eigenstates, which come from the schrodinger equation. Since the schrodinger equation conserves the integral over all x of probability density, why do I get a state which does not do so from harmonic oscilator states (and thus, by extension, the schrodinger equation)?
Thanks so much in advance, I have done this over several times over the last day and cannot find out anything I did wrong nor a solution online.
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