Tunneling and transmission coefficient

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SUMMARY

The discussion centers on quantum tunneling and the behavior of particles encountering a potential barrier where the barrier height (V0) exceeds the particle energy (E). It is established that while the wavefunction decays exponentially within the barrier, the reflection coefficient (R) approaches unity, indicating that the probability of transmission (T) approaches zero as the barrier width increases. This results in an extremely small probability amplitude for detecting particles within the barrier, especially in the case of a very wide barrier. The provided Shockwave movie illustrates the relationship between barrier width and probability density behavior.

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If an ensemble of quantum partcles, with energy E, traveling in x direction encounter a very wide potential barrier V0 > E, the ensemble wavefunction will exponentially decay within the barrier.

I thought that meant that there was a small probability of detecting an electron within the barrier. But the reflection coefficient of the probability current is unity. So what’s going on here?
 
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For a very wide barrier, the inverse if the transmission coefficient (T) goes to infinity, so T --> 0 and R --> 1, like you said. The probability density of the wavefunction does decay exponentially within the barrier, but the amplitude decreases as the width of the barrier increases. So, for a very wide barrier, the probability amplitude inside the barrier would be extrememly small. If we take the extreme case where R = 1, then the probability amplitude would basically be zero.

Here is a Shockwave movie that might help. Modify the width, and watch the behavior of the probability density.

http://phys.educ.ksu.edu/vqm/html/qtunneling.html
 
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