What is the 3D wave function and energy of an electron in an extended 1D well?

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The discussion focuses on the 3D wave function and energy of an electron in an extended 1D quantum well, specifically a structure defined by V(x,y,z) = 0 for 0 < z < L and infinite otherwise. The separation of variables in the Schrödinger equation yields independent wave functions, with the z-component represented as ψ(z) = √(2/L) sin(nπz/L). The boundary conditions for the x and y components are clarified as non-zero, indicating free particle behavior, with the wave function expressed as ψ(x) = e^(i(kx - wt)). The challenge lies in determining the constants for the wave functions in the x and y dimensions.

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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 Schrödinger equation and obtained the three independent wavefunction.
-\frac{\hbar^{2}}{2m}\psi_{x_{i}}=E \psi_{x_{i}}
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.
\psi_{z}=\sqrt{\frac{2}{L}}sin(\frac{n \pi z}{L})
I just cannot get the constant for the wavefunctions for x and y.
I know that
\psi(x)=\psi(x+2\pi)
but I still cannot get the value of the constant and the energy.
 
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Why do you assume periodic boundary conditions?

It is an infinite well. Remember, that means the wavefunction is zero at all boundaries of the well.
 
But now V(x,y,z)=V(z), where V is not a function of x and y anymore.
With this condition, in x and y, the wavefunction is certainly not zero, it is a free particle.
\psi_{x}=e^{i(kx-wt)}
 

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