Homework Help: Triangular Potential Well

1. May 5, 2012

TMSxPhyFor

1. The problem statement, all variables and given/known data
find Transmission and Reflection coefficients (QM) for the following triangular potential well:

U=U$_{0}$(1-$\frac{x}{a}$) : x$\geq$0 and U= 0 : x<0

and U$_{0}$>0 , a>0

2. Relevant equations

3. The attempt at a solution
Basically constructing the wave functions is very easy (from the left side of the plane we have flat de'broel wave, from the right side we have a solution of superposition of Airy's functions of the first and second kinds), but then the problems arise:

1- first problem that i can't understand, is when our wave function is super position (coefficients still maybe complex) purely real, the current will be anyway equal to zero (in case of right side with Airy functions), this mean that our particle will reflect with 100% probability, while the wave function still not zero at the right side (what means that the particle may be discovered there), how I should understand that? all of the books I checked keeps silent regarding this case.

2- the general solution has 3 coefficients (1 in the flat incoming & reflecting flat wave from the left and 2 for Airyi's right solution) and i have only two boundary conditions to combine the two solutions at x=0, and please note that in case of this problem divergence of Bi is not a threat here and the both functions are bounded, so there is no other boundary conditions that can be used, and we can't suppose that our wave function is asymptotically flat at x->\infinity becuase at that point interaction of the field with the particle is not zero as usually supposed (not so physical but anyway..)

I couldn't find a similar problem anywhere, except that a similar thing happens in studding semiconductors as is written here :http://www.iue.tuwien.ac.at/phd/gehring/node47.html#s:gundlach that mentioned some "GUNDLACH Method" that i couldn't find in other references to it, plus as i understood the suppose additional boundary condition not available for this problem.