Transmission Coefficient for two step potential

In summary, the conversation discusses a step potential wave setup and the calculation of the transmission coefficient. The usual transmission coefficient formula is given, but it is noted that the velocity of the wave may affect the probability flux. The correct formula for the transmission probability is provided as the ratio of the probability flux of the transmitted and incident waves.
  • #1
th5418
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0

Homework Statement


[tex]E>V_1 & V_2[/tex]
So it's a step potential wave, setup. Let's set it up along the x axis. At x=0, there is the first step where it is [tex]V_1[/tex]. At x=a, there is another step, where [tex]V_2>V_1[/tex]. Show that the transmission coefficient is...
[tex]T=\frac{4k_1k_2^{2}k_3}{k_2^{2}(k_1+k_2)^{2}+(k_3^{2}-k_2^{2})(k_1^{2}-k_2^{2})sin^{2}k_2a}[/tex]

Homework Equations


So the usual transmission is just [tex]T=(\frac{A}{F})^{2}[/tex] where A is the coefficient for incoming wave, and F is coefficient for leaving wave. However, one of my friend says that the transmission coefficient has extra terms in it because the velocity of the wave is different. Please help!

The Attempt at a Solution


I have the eigenfunctions..
[tex]\varphi_1 = Ae^{ik_1x} + Be^{-ik_1x} [/tex]

[tex]k_1 = \sqrt{\frac{2mE}{h}}[/tex]

[tex]\varphi_2 = Ce^{ik_2x} + De^{-ik_2x}[/tex]

[tex]k_2 = \sqrt{\frac{2m(E-V_1)}{h}}[/tex]

[tex]\varphi_3 = Fe^{ik_3x} [/tex]

[tex]k_3 = \sqrt{\frac{2m(E-V_2)}{h}}[/tex]
 
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  • #2
The velocity of a complex plane wave has no effect on its (average) probability density.1 However, I think that you have the expression upside down.



1I say average to account for the small-scale fluctuations that can result from interference.
 
  • #3
The velocity of the wave affects the probability flux of the wave. The transmission probability is properly defined as the ratio of the probability flux of the transmitted and the incident wave. In the potential step case the transmission probability is then

[tex]T = \frac{|\boldsymbol{k}'|}{|\boldsymbol{k}|}\frac{|F|^2}{|A|^2}[/tex]

if [tex]A[/tex] is the amplitude of the incident wave, [tex]\boldsymbol{k}[/tex] is its wave vector, [tex]F[/tex] the amplitude of the transmitted wave and [tex]\boldsymbol{k}'[/tex] its wave vector. It is described in more detail http://quantummechanics.ucsd.edu/ph130a/130_notes/node149.html" . (On the bottom of the page there is a link to the probability flux discussion).
 
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1. What is the Transmission Coefficient for two step potential?

The Transmission Coefficient for two step potential is a measure of the probability that a particle will pass through a potential barrier in a two-step process. It is defined as the ratio of the transmitted wave to the incident wave, and is used to determine the transmission probability of a particle through a potential barrier.

2. How is the Transmission Coefficient calculated?

The Transmission Coefficient is calculated using the Schrödinger wave equation, which describes how a particle's wave function evolves over time. The transmission coefficient is found by solving the wave equation for the potential barrier and taking the ratio of the transmitted wave to the incident wave.

3. What factors can affect the Transmission Coefficient?

The Transmission Coefficient is affected by the height and width of the potential barrier, as well as the energy and momentum of the particle. The mass and charge of the particle also play a role in determining the transmission coefficient.

4. How is the Transmission Coefficient used in quantum mechanics?

The Transmission Coefficient is a fundamental concept in quantum mechanics, as it allows us to understand and predict the behavior of particles passing through potential barriers. It is used in various fields such as solid state physics, nuclear physics, and quantum computing.

5. Can the Transmission Coefficient be greater than 1?

No, the Transmission Coefficient cannot be greater than 1. This would imply that the probability of the particle passing through the barrier is greater than the probability of it not passing through, which goes against the fundamental principles of quantum mechanics.

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