Question on Finding Transmission Coefficient

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SUMMARY

The discussion focuses on calculating the transmission coefficient for the potential defined as V(x)=-α[δ(x+a)+δ(x-a)], where α and a are positive constants. The transmission coefficient T is expressed using the formula T ≡ |F|²/|A|² and an alternative formula T = 1/(1 + β²). The user expresses confusion regarding the application of these formulas due to the presence of non-zero potentials and the need to solve the Schrödinger wave equation. Key insights include the necessity of ensuring wavefunction continuity at x = ±a and the use of integration around singular points to derive relationships across these points.

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  • Understanding of quantum mechanics, specifically the Schrödinger equation.
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  • Knowledge of boundary conditions and continuity requirements for wavefunctions.
  • Basic grasp of transmission coefficients in quantum mechanics.
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  • Explore the mathematical techniques for integrating around singular points in differential equations.
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Students and professionals in quantum mechanics, particularly those dealing with potential barriers and transmission phenomena, as well as educators looking to enhance their understanding of wavefunction behavior in non-trivial potentials.

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Homework Statement


Find the transmission coefficient for the potential V(x)=-\alpha\left[\delta\left(x+a\right)+\delta\left(x-a\right)\right], where alpha and a are positive constants.

Homework Equations


T \equiv \frac{\left|F\right|^{2}}{\left|A\right|^{2}}

The Attempt at a Solution


I'm technically not sure on where to begin this problem. After reading the section (twice now), I noticed that it pretty much explicitly omits considering potentials which are not zero. And also, there is another formula for the transmission coefficient
T=\frac{1}{1+ \beta^{2}}
but, again, I'm not too sure on whether I should be using this one. My first instinct is to solve the Schrödinger wave equation, but it looks to be fairly mmessy with those dirac deltas.

Am I missing something really obvious? To recap, it looks like the book's section wanted to purposely omit non-zero potentials, and yet this problem appears to have a non-zero potential, leaving me clueless as to how to deal with it short of starting from scratch.
 
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The potential is zero in the 3 regions: x< -a, -a<x<a, a<x, so you can solve for the wavefunctions in those regions. You can obtain relations between the coefficients by demanding that certain physical conditions be satisfied. For example, the wavefunction must be continuous at x=\pm a. However, because the potential is not continuous, we cannot demand that the derivative of the wavefunction is continuous. However, Schrödinger's equation must still be valid, so we can obtain relationships across the singular points by integrating the Schrödinger equation around x=\pm a:

\int_{x=\pm a-\epsilon}^{x=\pm a+\epsilon} \left( - \frac{\hbar^2}{2m} \psi''(x) + (V(x)-E) \psi(x) \right) =0.
 
ahhh, that's right. Thanks a lot, it makes a lot more sense from your first sentence and I can make some more progress on this one now.
 

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