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xcrunner2414
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Homework Statement
I'm asked to calculate the reflection and transmission coefficients for scattering from a potential energy barrier. The potential energy barrier is,
[tex] V(x)=\frac{\hbar^2}{2m} \frac{\lambda}{b} \delta(x) [/tex]
where [tex]\delta (x)[/tex] is the Dirac delta function.
Homework Equations
See above.
The Attempt at a Solution
Wouldn't the reflection coefficient be 1, and the transmission coefficient be 0? It seems like it's just an infinite potential well problem, except there is only one wall at x=0, so the wavefunction will be zero on the side of the barrier that is opposite the incident wavefunction. But that seems almost too simple. But then again, I'm dealing with an infinite potential barrier, so the idea that not even subatomic particles governed by quantum mechanics can penetrate it makes sense to me...
The actual solution, then, looks like this: Assuming region I is the side of the incident wavefunction, and region II is the other side, then solving the time-independent Schrodinger equation gives,
[tex]\psi_I (x) = Ae^{ikx} + Be^{-ikx} [/tex]
[tex]\psi_{II} (x) = Ce^{ikx} [/tex]
where [tex] k = \sqrt{2mE/\hbar^2} [/tex]. Since [tex] V(0)\rightarrow \infty [/tex], this means [tex] \psi(0) = 0 [/tex], so from the very first boundary condition:
[tex] \psi_I (x) |_{x=0} = \psi_{II} (x) |_{x=0} \Rightarrow A+B=C=0 \Rightarrow A=-B \Rightarrow R = \frac{j_{ref}}{j_{inc}} = \frac{{|B|}^2}{{|A|}^2} = 1 [/tex]
Right?
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