Potential barrier problem

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Homework Help Overview

The problem involves a particle with kinetic energy E incident on a potential barrier of height U, where E is greater than U. The objective is to derive an expression for the reflection coefficient R in terms of the ratio e = E/U.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the wavefunctions for regions to the left and right of the barrier, noting the need for continuity conditions at the boundary. There is exploration of the implications of E being greater than U on the wavefunctions and the reflection coefficient.

Discussion Status

Participants are actively engaging with the problem, sharing their wavefunction forms and continuity conditions. Some guidance has been offered regarding the relationship between the wave numbers k and L, and there is an ongoing exploration of how to express the reflection coefficient in terms of E/U.

Contextual Notes

There is a mention of the challenge in obtaining the ratio E/U from the expressions for k and L, indicating potential confusion or missteps in the derivation process. Participants are questioning assumptions about the nature of k and L in the context of the problem.

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Homework Statement


a particle of kinetic energy E is incident from left on a potential barrier,height U, situated at the origin.the barrier is infinitely wide and E>U

obtain an expression for the reflection coefficient R of the particle as a fuction ratio e=E/U


Homework Equations





The Attempt at a Solution



to left of barrier wavefunctions are free particle waves
barrier at x=0
psi(x,t)=Aexp(ikx-wt)+ Bexp(-ikx-wt) x<0

within barrier wavefunction also is oscillatory

E=h(cross)*w

considering case for E<U and using TISE on psi(x,t) within barrier we get

a=([2m(U-E)]^0.5)/h(cross)

but now E>U and as a result a becomes imaginary. introducing new wavenumber L and barrier wavefunction becomes

psi(x,t) =Cexp(-iLx-wt)+Dexp(iLx-wt) x>0 (note this is equation is only for a barrier of finite width)

but now everywhere to right from origin x=0 is the barrier wavefunction given above . to keep psi(x,t) from diverging for large x we must take D=0 leaving only decaying wave and this is where i am up to i was just wanting to know if i am on the right track
 
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You need two sets of wavefunctions, one for x<0 and another one for x>0. The first set for x<0 has two pieces, one representing the incident wave and one representing the reflected wave. For x>0 you have only one wave, the transmitted wave traveling to the right. Since E > U, all waves are represented by complex exponentials. These are basically sinusoidals and do not decay with x.
 
ok i see thanks so now my wavefunctions are

psi(x,t)=Aexp(ikx-wt)+Bexp(-ikx-wt) x<0
psi(x,t)=Dexp(iLx-wt) x>0

so now wavefunctions must be joined smoothly following the conditions
A+B=D cont of psi
ikA-ikB=iLD cont of d(psi)/dx

solving for D i get

A(1-k/L)=B(-1-k/L)

B/A= -(1-k/L)/(1+k/L)

reflection coefficient is given by R=|B^2|/|A^2| but i need to obtain an expression in terms of ratio E/U

so i tried to substitute k=(2mE/h(cross))^0.5 and L=i(2m(U-E)/h(cross))^0.5 into equation but was unsuccessful to get the ratio out am i on the right track?
 
Aren't k and L both real and isn't the ratio L/k related to U/E somehow?
 
yes sorry both L and k are real and i get E/U =-1/2 when i put them equal to each other but now I am kind of lost
 
I don't see how you get E/U = -1/2. What are your (correct) expressions for k and L?
 

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