Solving QM Griffiths 2.28: Transmission Coefficient

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The discussion centers on calculating the transmission coefficient for a wave packet encountering Dirac delta wells of strength alpha at positions x = -a and x = +a. The solution involves segmenting the problem into three intervals and applying boundary conditions to reduce the number of unknowns. The derived transmission coefficient is expressed as T = 1 / (1 + 2β²[(1 + β²) + (1 - β²)cos(4ka) - 2βsin(4ka)]), where β = (mα)/(ħk). The participants emphasize the importance of validating calculations independently to ensure accuracy.

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genxhis
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The problem asks for the transmission coefficient for a wave packet with energy approximately E passing through a potential function with dirac delta wells of strength alpha at x = -a and x = +a. To solve the problem I split the region into the three obvious intervals [-inf, -a], [-a, a], and [a, +inf]. For the first two regions I expressed the solutions as (A or C) exp(i k x) + (B or D) exp(-i k x) and for the last as E exp(i k x) where k = sqrt(2 m E)/hbar. I then applied the two contraints at the two boundary conditions to reduce the five unknowns to just one. Finally I did some more algebra to find the trasmission coefficient as the square of (E/A). But the entire process was lengthy and tedious. I was wondering if someone could validate this answer:

[tex]T = \frac{1}{1 + 2 \beta^2[ (1+\beta^2) + (1-\beta^2)\cos 4ka -2\beta \sin4ka ]}[/tex]​


where [tex]\beta = (m \alpha)/(\hbar k)[/tex].
 
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There's no better checking than the one you can do it yourself by making sure your method & calculations were correct.

I think no one around here will do the calculations at this problem,just to agree or disagree with your answer.

Daniel.
 
your right, sorry. i was hoping someone could recognize this as a special case of a more general problem or simply point out that the answer is unviable. but, I've looked it over more carefully, and i think it is. in any case, recapitulating what i did helps me understand it a little better.
 

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