How to Calculate Transmission Coefficient for a Quantum Rectangular Barrier?

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Homework Help Overview

The discussion revolves around calculating the transmission coefficient for a quantum particle tunneling through a rectangular potential barrier. The problem involves understanding wave functions in different regions of the potential and applying boundary conditions to relate the coefficients of these wave functions.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to derive relations among constants from wave functions in different regions and questions how to equate the transmission coefficient. Some participants suggest clarifying the relationship between the incident and transmitted wave probabilities. Others explore the implications of boundary conditions on the coefficients.

Discussion Status

Participants are actively discussing the setup of the problem and the relationships between wave functions. Some guidance has been offered regarding the interpretation of the transmission coefficient, and there is an ongoing exploration of how to apply boundary conditions effectively.

Contextual Notes

There are mentions of specific boundary conditions at x=0 and x=a that need to be applied to eliminate certain coefficients, but the original poster expresses uncertainty about the process. The discussion reflects a lack of consensus on the exact steps to take next.

judonight
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Ok, so I've been dealing with this problem for a while and can't figure it out. (I tried to clean it up, but I don't know LaTeX, hopefully it is more clean in post #2; problem stated in #1, and my work in #2)

--Consider a (plane-wave) particle tunneling through a rectangular barrier potential w/ height v, and width a (the particle has E<v)...

a) write general solutions of stationary state functions in each 'region' of the potential.

--Done, no problem.

b)Find four relations among the five arbitrary constants in part a).

--Again, no problem

c) Use relations in part b) to equate transmission coefficient.


--Part c) is the problem, I have no idea what to do...
 
Last edited:
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Homework Statement





Homework Equations



a)

Region I: x<0 : psi(x)= A exp[i k x] + B exp [-i k x]

Region II: 0<x<a: psi(x)= C exp [K x]+ D exp [-K x]

Region III x>a : psi(x)= E exp [i k x]


[tex]\newcommand{\pd}[3]{ \frac{ \partial^{#3}{#1} }{ \partial {#2}^{#3} } }i \hbar \pd{\Psi}{t}{} =- \frac{\hbar^2}{2 m} \ \pd{\Psi}{x}{2} + V \Psi[/tex]

k^2= 2mE/hbar^2
K62= 2m(E-v)/hbar^2

c) took derivative of psi I = derivative psi II, at x=o.

Derivative psi II = derivative psi III, at x=a

psi(o)I=psi(0)II

psi(a)II=psi(a)III

The Attempt at a Solution



I tried to linearly add:

psi(0)I + d/dx psi(o)I = psi(o)II + d/dx psi(o)II

and same for when x=a for psi II and III.

I attempted to eliminate C and D constants, and solve for E. I let A =1 (thinking other waves than the incident have some multiple of amplitude.)

I thought that abs(E)^2= transmittion coeficient, is this not true? And B would be the reflection coefficient?

Where am I going wrong?
 
Last edited:
The transmission coefficient represents the probability flux of the transmitted wave relative to that of the incident wave.
I hope this help you
 
ziad1985 said:
The transmission coefficient represents the probability flux of the transmitted wave relative to that of the incident wave.
I hope this help you


Ok, so the probability of incident wave over transmitted?

How do I get there from general solutions though?

(A*A)/(E*E) ?
 
ziad1985 said:
The transmission coefficient represents the probability flux of the transmitted wave relative to that of the incident wave.
I hope this help you


I finally figured it out.

Eliminate coefficients of general solution for inside the barrier by applying boundary conditions at x=0, x=a.

Solve for coefficient of transmission, take abs, square it, bam, it's done.
 

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