- #1
sgod88
- 6
- 0
1. Quantum well structure can be realized by sandwiching layers of semiconductor and two insulators.
This sandwiching problem was often treated with 1 D infinite well. Suppose now the problem is 3 dimensional well with length L at z direction from 0 to L, at which
V(x,y,z)= 0 when 0<z<L
infinity otherwise
where V(x) and V(y) is 0. We assume x and y be infinitely large.
Wht is the total energy and the wave function of the electron in such well?
2. I have done the separation of varibales in the Schrodinger equation and obtained the three independent wavefunction.
[tex]-\frac{\hbar^{2}}{2m}\psi_{x_{i}}=E \psi_{x_{i}} [/tex]
But i don't know what is the boundary condition of the x and y.
I only got psi(z) is the psi of the one d wavefunction.
[tex]\psi_{z}=\sqrt{\frac{2}{L}}sin(\frac{n \pi z}{L})[/tex]
I just cannot get the constant for the wavefunctions for x and y.
I know that
[tex]\psi(x)=\psi(x+2\pi)[/tex]
but I still cannot get the value of the constant and the energy.
This sandwiching problem was often treated with 1 D infinite well. Suppose now the problem is 3 dimensional well with length L at z direction from 0 to L, at which
V(x,y,z)= 0 when 0<z<L
infinity otherwise
where V(x) and V(y) is 0. We assume x and y be infinitely large.
Wht is the total energy and the wave function of the electron in such well?
2. I have done the separation of varibales in the Schrodinger equation and obtained the three independent wavefunction.
[tex]-\frac{\hbar^{2}}{2m}\psi_{x_{i}}=E \psi_{x_{i}} [/tex]
But i don't know what is the boundary condition of the x and y.
I only got psi(z) is the psi of the one d wavefunction.
[tex]\psi_{z}=\sqrt{\frac{2}{L}}sin(\frac{n \pi z}{L})[/tex]
I just cannot get the constant for the wavefunctions for x and y.
I know that
[tex]\psi(x)=\psi(x+2\pi)[/tex]
but I still cannot get the value of the constant and the energy.
Last edited: