Are Eigenkets for the Creation Operator Valid?

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Swatch
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Homework Statement



The problem is to find the eigenkets for the creation operator ,[tex]a^{\dagger}[/tex] if they exist

Homework Equations



[tex]a^{\dagger}|\Psi>=\lambda|\Psi>[/tex]
[tex]a^{\dagger}=\frac{1}{\sqrt{2*\hbar*m*\omega}}*(-\hbar*\frac{d}{dx}+m*\omega*x)[/tex]

The Attempt at a Solution


I use the expression for the creation operator above and set up the differential equation.
The boundary conditions for the wavefunction should be that it is zero when x goes to +- infinity.
When I solve it I get this result.
[tex]0=\lambda*x\right|_{-\infty}^{+\infty} - \frac{1}{2}\sqrt{\frac{m*\omega}{2*\hbar}}*x^{2} \right|_{-\infty}^{+\infty}[/tex]

I know the creation operator is not hermitian and it is not an observable but could this answer be correct?
Could someone please comment on this
 
Swatch said:

Homework Statement



The problem is to find the eigenkets for the creation operator ,[tex]a^{\dagger}[/tex] if they exist

Homework Equations



[tex]a^{\dagger}|\Psi>=\lambda|\Psi>[/tex]
[tex]a^{\dagger}=\frac{1}{\sqrt{2*\hbar*m*\omega}}*(-\hbar*\frac{d}{dx}+m*\omega*x)[/tex]

The Attempt at a Solution


I use the expression for the creation operator above and set up the differential equation.
The boundary conditions for the wavefunction should be that it is zero when x goes to +- infinity.
When I solve it I get this result.
[tex]0=\lambda*x\right|_{-\infty}^{+\infty} - \frac{1}{2}\sqrt{\frac{m*\omega}{2*\hbar}}*x^{2} \right|_{-\infty}^{+\infty}[/tex]

I know the creation operator is not hermitian and it is not an observable but could this answer be correct?
Could someone please comment on this

If eigenkets of [itex]a^\dagger[/itex] exist. What is their overlap with the vacuum?
 
What is their overlap with vaccum?
I don't understand!
 
By "vacuum" I just mean the state [itex]|0\rangle[/itex] that satisfies
[tex] a|0\rangle=0[/tex]

By "overlap with the vacuum" I mean, what is
[tex] \langle 0 |\lambda\rangle[/tex]
equal to?
 
...where [itex]|\lambda\rangle[/itex] is the eigenket of [itex]a^\dagger[/itex] with eigenvalue [itex]\lambda[/itex]
 
The overlap with the vacuum is zero
but how does this help me?:confused:
 
Swatch said:
The overlap with the vacuum is zero
but how does this help me?:confused:

So, the overlap with the vacuum is zero. Good.

Now, what is the overlap with the "one-particle" state
[tex] |1\rangle = a^\dagger |0\rangle\;[/tex]
?
 
I believe the overlap of [tex]|\lambda>[/tex] with the one particle state to be zero
 
Swatch said:
I believe the overlap of [tex]|\lambda>[/tex] with the one particle state to be zero

So, given that, what's the overlap of [tex]|\lambda>[/tex] with the 2-particle state |2>? I hope you realize what the nth question is going to be.
 
I think I understand this.
since the overlap of [tex]\lambda[/tex] and the vacuum is zero and also the overlap with the one, two and so one particle functions is zero, [tex]\lambda[/tex] must be zero.
Am I right?
 
Swatch said:
I think I understand this.
since the overlap of [tex]\lambda[/tex] and the vacuum is zero and also the overlap with the one, two and so one particle functions is zero, [tex]\lambda[/tex] must be zero.
Am I right?

The notation you are using above confuses the state with it's eigenvalue.

What we have just seen is that if the *eigenvalue* [itex]\lambda[/itex] is non-zero then the *state* [itex]|\lambda>[/itex] must be zero--i.e., there are no eigenstate of [itex]a^\dagger[/itex] with non-zero eigenvalues.