Ritorufon
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Homework Statement
Hi guys, I'm having trouble understanding the finite potential well, in particular the boundary conditions
The well under scrutiny has potential
V(x)= 0 for |x|<a
and
V(x)=V_0 for >a
Homework Equations
\frac{d^2\psi}{dx^2}=-\sqrt{\frac{2mE}{\hbar^2}}\psi=-\alpha^2\psi (1)
\frac{d^2\psi}{dx^2}=-\sqrt{\frac{2m(V_0-E)}{\hbar^2}}\psi=\beta^2\psi (2)
with solutions to (1)
Asin\alpha x+Bcos\alpha x
and (2)
Ce^{-\beta x}+De^{+\beta x}
The Attempt at a Solution
Know that \psi(x) is single valued, finite and continuous so at the boundary x = a
\psi_{inside} (a)=\psi_{outside} (a)
and
\frac{d^2 \psi_{inside} (a)}{dx^2}=\frac{d^2 \psi_{outside} (a)}{dx^2}
so for odd parity at the border x = a
Asin\alpha a = Ce^{-\beta a} for \psi(a) continuity
and
\alpha Acos\alpha a = -\beta Ce^{-\beta a} for \frac{d^2 \psi (a)}{dx^2} continuity
so if you divide the differentials by the functions you get
tan \alpha a = -\alpha / \beta
The same can be done with the even parity but if done the same as above you get
cot \alpha a= \beta/\alpha
but this incorrect the correct answer is
tan \alpha a=\beta/\alpha
but to get this answer you would have to divide the differental by the function and not the other way around like what was done for odd solutions.
My question is how do you know whether to divide the differental by the function or the function by the differential, also what physical meaning do these solutions have in relation to the well?
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