Schrodinger using a Hermite Polynomial

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The discussion focuses on solving the first energy level of the Schrödinger equation using Hermite polynomials for a one-dimensional harmonic oscillator (1D-HO). Participants confirm that the wavefunction can be derived from the ground state using the creation operator, leading to the expression for the first excited state wavefunction. They emphasize that to verify the solution, one can substitute the proposed wavefunction into the Schrödinger equation rather than solving it directly. The energy associated with this state is confirmed to be \(\frac{3}{2}\hbar\omega\). The conversation highlights the use of operator algebra typical in quantum mechanics for 1D harmonic oscillators.
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Can some1 help me solve a first energy level Schrodinger (\psi_{1})with a the Hermite polynomial and also show that it equals to \frac{3}{2}\hbar \omega?

I got as far as
<br /> \newcommand{\pd}[3]{ \frac{ \partial^{#3}{#1} }{ \partial {#2}^{#3} } }\frac{\hbar^2}{2 m} \ \pd{\Psi}{x}{2} + V \Psi = \frac{\hbar}{2m} (2N_{1}\frac{x}{\alpha}e^\frac{-1}{2\alpha^2}x^2(\frac{1}{\alpha^2}+\frac{1}{\alpha^4}x^2)<br />

Thanks.
 
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Is it for the simple 1D-HO...?That one has Hermite polynomials as eigenfunctions...

If so,how about checking any book on QM (any,all treat 1D-HO) for the famous algebraic method...?

U'll then get the \psi_{1}(x) by applying the creation operator on the ground state...

Daniel.
 
The problem says: confirm that the 1st excited state wavefunction of a 1D HO given by the Hermitian equation

H_{1}(y)= 2y y = \frac{x}{\alpha}, \alpha = (\frac{\hbar^2}{mk})^\frac{1}{4}<br />

is a solution of the Schrodinger equation and that the energy is \frac{3}{2}\hbar\omega.


Thanks.
 
Last edited:
\psi_{1}(x)=:\langle x|1\rangle


\hat{H}=\hbar\omega\left(\hat{a}^{\dagger}\hat{a}+\frac{1}{2}\hat{1}\right)

\langle x|\hat{H}|1\rangle =\hbar\omega \left(\langle x|\hat{a}^{\dagger}\hat{a}|1\rangle +\frac{1}{2} \langle x|\hat{1}|1 \rangle \right) = \hbar\omega \left\langle x\left|\left(1+\frac{1}{2}\right)\right|1 \right\rangle=\frac{3}{2} \hbar\omega \langle x|1\rangle

which means

\hat{H}\psi_{1}(x)=\left(\frac{3}{2}\hbar\omega\right) \psi_{1}(x)

Q.e.d.


NOTE:I made use of

\left \{\begin{array}{c} \hat{a}|n\rangle =\sqrt{n}|n-1\rangle ,\ \mbox{for} \ n=1 \\ \hat{a}^{\dagger}|n\rangle =\sqrt{n+1}|n+1\rangle ,\ \mbox{for} \ n=0 \end{array} \right

which are typical for the operators which form the famous Heisenberg algebra of the 1D-HO.

Daniel.
 
Yes... in order to show that a solution satisfies the equation, you don't actually have to solve the equation! Just substitute the proposed solution in and see if the resulting statement is true.
 
I don't know bracket notation or what a means, but I put it in the HW I turning in.
 
It's the only elegant way to do it,really.

Daniel.
 
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