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So let's say we have a particle in the delta function potential, V = - \alpha \delta(x). I calculated that the reflection coefficient (scattering state) is
R = \frac{1}{1 + (2 \hbar^2 E/m\alpha^2)}
Now, clearly, the term 2 \hbar^2 E/m\alpha^2 is very small, as \hbar^2 has an order of magnitude of -68. This value is so small that even for classical ordered values for E, m, and \alpha, the reflection coefficient is very close to 1. Is this correct? It seems a bit strange to me that a spike in the potential where a particle's energy is above the potential causes the particle to reflect BACK almost 100% of the time... it seems as if a tank shell going at more than a mile per second goes over a cliff and reflects back...
R = \frac{1}{1 + (2 \hbar^2 E/m\alpha^2)}
Now, clearly, the term 2 \hbar^2 E/m\alpha^2 is very small, as \hbar^2 has an order of magnitude of -68. This value is so small that even for classical ordered values for E, m, and \alpha, the reflection coefficient is very close to 1. Is this correct? It seems a bit strange to me that a spike in the potential where a particle's energy is above the potential causes the particle to reflect BACK almost 100% of the time... it seems as if a tank shell going at more than a mile per second goes over a cliff and reflects back...
