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[4. Applications]
Transmission coefficient.
A particle moving along the x-axis, with mass m and energy E, approaches
from the left a potential barrier with energy U > E. According to
quantum mechanics, the probability that the particle penetrates the potential barrier
(blue line in the draw) is not null. The transmission coefficient T is the probability
that the particle reaches the point a , thus passing the potential barrier and
penetrating into the region on the right.
Let φ (x) = e-x k a solution of the first
Schrödinger equation applied to the particle inside the potential barrier, where
.
A rough approximation for the transmission coefficient is given by the quotient of
φ (a) by φ (0). This quotient is e-a k ;
the square of its module gives the probability that the particle passes the potential barrier.
This probability is, by definition, the transmission coefficient.
Thus T = | φ (a) / φ (0) | 2 =
| e - a k |2 = e - 2 a k .
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