Quantum particle reflection from a potential drop

SonOfOle
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Homework Statement


A quantum mechanical particle with mass m and energy E approaches a potential drop from the -x region, where the potential is described by:
V(x)=\left\{\stackrel{0 textrm{if} x\leq 0}{-V_0 textrm{if} x> 0}.

What is the probability it will be reflected by the potential?


Homework Equations


Incident Wave: \Psi (x,t) = A e^{k x - \omega t} \textrm{where} k= \sqrt{2 m D} /2


The Attempt at a Solution



I want to say 0, but that's without doing the math on it. The continuity equations yield 3 unknowns (A, B, C
 
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Ignore above post. I posted too soon. Here's my real question.

Homework Statement


A quantum mechanical particle with mass m and energy E approaches a potential drop from the -x region, where the potential is described by:
V(x)=\left\{\stackrel{0 \textrm{if} x\leq 0}{-V_0 \textrm{if} x> 0}.

What is the probability it will be reflected by the potential?


Homework Equations


Incident Wave: \Psi (x,t) = A e^{k x - \omega t} \textrm{where} k= \sqrt{2 m E} / \hbar

Reflected Wave: \Psi (x,t) = B e^{-k x - \omega t} \textrm{where} k= \sqrt{2 m E} / \hbar

Transmitted Wave: \Psi (x,t) = C e^{k x - \alpha t} \textrm{where} \alpha = \sqrt{2 m (E+V_0)} / \hbar

Continuity Equations: \Psi_A + \Psi_B = \Psi_C and \partial_x \Psi_A + \partial_x \Psi_B = \partial_x \Psi_C


The Attempt at a Solution



Plug in \Psi_A, \Psi_B, and \Psi_C into the continuity equations and get these two equations:

A + B = C
i A k - i B k = i C \alpha

Plug the first into the second, and get
\frac{B}{A} = \frac{k -\alpha}{k + \alpha}

which is the probability of reflection.

Now, the math makes sense, but it doesn't make sense overall because if \alpha is greater than k then the probability is negative. Also, reflecting from a drop in potential doesn't make sense intuitively... but that may just be QM.

Any ideas?
 
There should be absolute value brackets around the B/A equation, which is why alpha being greater than k doesn't produce a negative probability.
 
Hmm... Okay. Even still, wouldn't large V_0 lead to large \alpha, and thus for large V_0, |B|/|A| --> 1?
 
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