Finding normalization constant and exponent for harmonic oscillator ground state

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The ground state of a one-dimensional Harmonic oscillator described by the Hamiltonian [itex]H = \frac{p^2}{2m} + \frac{kx^2}{2}[/itex] is of the form, [itex]\psi = Ae^{-ax^2}[/itex]. Determine 'A' and 'a' so that the wavefunction [itex]\psi[/itex] is a normalized eigenstate of the Hamiltonian. What is the energy eigenvalue of the wavefunction?

Well, I was able to normalize the wavefunction and obtained the value of 'A'.
[tex]\int_{-\infty}^{\infty}\psi \psi^* dx =1[/tex]

[tex]A^2\int_{-\infty}^{\infty}e^{-2ax^2}dx =1[/tex]

[tex]A^2\sqrt{\frac{\pi}{2a}} =1[/tex]

[tex]A = (\frac{2a}{\pi})^{1/4}[/tex]

How do I determine 'a'? Any clues to obtain energy eigen value?
 
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Sorry, I could not correct my errors yesterday. I have rectified the LaTeX typos. Now can someone help me...?
 
How do I determine 'a'? Any clues to obtain energy eigen value?
I would say use the definitions of "eigenstate" and "eigenvalue".
 
Hurkyl said:
I would say use the definitions of "eigenstate" and "eigenvalue".
You mean use the eigenfunction and obtain the eigenvalue?
[tex]i \hbar \frac{\partial}{\partial t} \psi = \mathcall H \psi[/tex]
 
Just apply the harmonic oscillators hamiltonian to the eigenfunction. And I don't think you can determine a but you can set some constraints on it. a just tells you how wide the gaussian is.
 
You mean use the eigenfunction and obtain the eigenvalue?
The definitions are that [itex]\psi[/itex] is an eigenfunction of H with eigenvalue [itex]\lambda[/itex] if and only if [itex]H \psi = \lambda \psi[/itex].
 
yep you should just be able to operate on the wavefunction with the hamiltonian to obtain the eigenvalues which are the energy values
 
inha said:
Just apply the harmonic oscillators hamiltonian to the eigenfunction. And I don't think you can determine a but you can set some constraints on it. a just tells you how wide the gaussian is.

qtp said:
yep you should just be able to operate on the wavefunction with the hamiltonian to obtain the eigenvalues which are the energy values

Thank you for your time.

[tex]H = {p^2 \over 2m} + {1\over 2} m \omega^2 x^2[/tex]

[tex]p = -i \hbar \partial / \partial x[/tex]

[tex]{-\hbar^2\over 2m}{\partial^2 \psi \over \partial x^2} + {1\over 2} m \omega^2 x^2 \psi = E_n \psi[/tex]

Looks familiar to me, energy eigen values given by:
[tex]E_n = \hbar \omega \left(n + {1\over 2}\right)[/tex]