Transmission over a linear barrier (QM)

cc94
Messages
19
Reaction score
2

Homework Statement


Suppose we have a potential such that $$
V =
\left\{
\!
\begin{aligned}
0 & \text{ if } x<0\\
\mathcal{E}x & \text{ if } x>0, x<L\\
\mathcal{E}L & \text{ if } x>L
\end{aligned}
\right.
$$

for some electric field ##\mathcal{E}##. I'm trying to find the transmission coefficient ##T## for a plane wave incoming from the left.

Homework Equations


Solving Schrodinger's equations, I believe we have:
$$
\psi =
\left\{
\!
\begin{aligned}
Ae^{ikx} + Be^{-ikx} & ; x<0\\
C\text{Ai}(\zeta) + D\text{Bi}(\zeta) & ; x>0, x<L\\
Fe^{i\kappa x} & ; x>L
\end{aligned}
\right.
$$

Where ##\zeta## is a change of variable involving ##x##, ##E##, and ##\mathcal{E}##, and we only keep a forward traveling wave for the region ##x>L##. Since one of the coefficients is arbitrary, we can choose ##F## = 1

Then we have boundary conditions:
$$\psi_I(0) = \psi_{II}(0) \\
<=> A + B = C\text{Ai}(\zeta_0) + D\text{Bi}(\zeta_0)$$
$$\psi_I'(0) = \psi_{II}'(0) \\
<=> ik(A - B) = C\text{Ai}'(\zeta_0)(\zeta'_0) + D\text{Bi}'(\zeta_0)(\zeta'_0)$$
$$\psi_{II}(L) = \psi_{III}(L) \\
<=> C\text{Ai}(\zeta_L) + D\text{Bi}(\zeta_L) = e^{i\kappa L}$$
$$\psi_{II}'(L) = \psi_{III}'(L) \\
<=> C\text{Ai}'(\zeta_L)(\zeta'_L) + D\text{Bi}'(\zeta_L)(\zeta'_L) = i\kappa e^{i\kappa L}$$

The Attempt at a Solution


Then we get the matrix (using a little bit of shorthand):

$$\begin{bmatrix}
1 & 1 & -\text{Ai}_0 & -\text{Bi}_0 & 0 \\
ik & -ik & -\text{Ai}'_0\zeta '_0 & -\text{Bi}'_0\zeta '_0 & 0 \\
0 & 0 & \text{Ai}_L & \text{Bi}_L & e^{i\kappa L} \\
0 & 0 & \text{Ai}'_L\zeta '_L & \text{Bi}'_L\zeta '_L & i\kappa e^{i\kappa L}
\end{bmatrix}$$

I used MATLAB to solve this symbolically, and then we know that ##T = \lvert\frac{F}{C}\rvert ^2 = \frac{1}{|C| ^2}##. So I plugged in various energies above the highest V and plotted T. But the transmission turns out to always be larger than 1, which makes no sense. Is my math wrong, or do I need to find a typo in my code somewhere? Has anyone solved this problem?
 
Last edited:
Physics news on Phys.org
I finally found the answer here: http://aapt.scitation.org/doi/10.1119/1.11582[/URL]. I don't know how he got it, because even using a diff eq solver I couldn't get that result. But I'll assume it's correct and I'm just missing something.
 
Hello everyone, I’m considering a point charge q that oscillates harmonically about the origin along the z-axis, e.g. $$z_{q}(t)= A\sin(wt)$$ In a strongly simplified / quasi-instantaneous approximation I ignore retardation and take the electric field at the position ##r=(x,y,z)## simply to be the “Coulomb field at the charge’s instantaneous position”: $$E(r,t)=\frac{q}{4\pi\varepsilon_{0}}\frac{r-r_{q}(t)}{||r-r_{q}(t)||^{3}}$$ with $$r_{q}(t)=(0,0,z_{q}(t))$$ (I’m aware this isn’t...
Hi, I had an exam and I completely messed up a problem. Especially one part which was necessary for the rest of the problem. Basically, I have a wormhole metric: $$(ds)^2 = -(dt)^2 + (dr)^2 + (r^2 + b^2)( (d\theta)^2 + sin^2 \theta (d\phi)^2 )$$ Where ##b=1## with an orbit only in the equatorial plane. We also know from the question that the orbit must satisfy this relationship: $$\varepsilon = \frac{1}{2} (\frac{dr}{d\tau})^2 + V_{eff}(r)$$ Ultimately, I was tasked to find the initial...
Back
Top