Denver Dang
- 143
- 1
Homework Statement
A particel is moving along the x-axis in a potential, V(x). The ground state of the wavefunction is:
\[\psi \left( x \right)={{e}^{-\frac{1}{2}{{\left( \frac{x}{a} \right)}^{4}}}},\]
where a is a constant of dimension length. We also know that V(a) = 0.
Determine V(x).
Homework Equations
The stationary Schrödinger equation:
\[-\frac{{{\hbar }^{2}}}{2m}\frac{{{d}^{2}}\psi }{d{{x}^{2}}}+V\psi =E\psi \]
The Attempt at a Solution
Well, first I derive the wavefunction two times and get:
\[\begin{align}<br /> & \frac{d}{dx}\psi \left( x \right)=-\frac{2}{{{a}^{4}}}{{x}^{3}}{{e}^{-\frac{1}{2}{{\left( \frac{x}{a} \right)}^{4}}}} \\ <br /> & \frac{d}{dx}\psi '\left( x \right)=\left( \frac{4{{x}^{6}}}{{{a}^{8}}}-\frac{6{{x}^{2}}}{{{a}^{4}}} \right){{e}^{-\frac{1}{2}{{\left( \frac{x}{a} \right)}^{4}}}} \\ <br /> \end{align}\]<br />
Then I insert it in the Schrödinger equation.
And here is where I get confused. It's been a while since I've had QM, so I can't really remember what's next.
I figure that the potential is NOT just what I get when I isolate V in the Schrödinger equation. So what's is my next step ?
Regards