Wavefunction properties tunneling effect

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SUMMARY

The discussion centers on the tunneling effect in quantum mechanics, specifically analyzing the Hamiltonian eigenfunctions for a particle encountering a potential barrier defined for the interval \(0 \le x \le a\). The eigenfunctions are expressed as \( \psi_E(x) = \begin{cases} e^{ikx} + Ae^{-ikx} & x \le 0 \\ Ce^{ikx} & x \ge a \end{cases} \), where \( k^2 = \frac{2mE}{\hbar^2} \). A critical point raised is that if \( C = 0 \), the wavefunction becomes identically zero for \( x \ge a \), which contradicts the requirement for eigenfunctions of the Schrödinger equation to be non-zero at points where their first derivatives exist. This necessitates that \( C \neq 0 \) to maintain continuity and physical validity of the wavefunction.

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  • Knowledge of boundary conditions and continuity requirements for wavefunctions.
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Salmone
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I am considering tunnel effect with a potential barrier of a certain height that is ##\neq 0## only for ##0 \le x \le a## . I write the Hamiltonian eigenfunctions outside the barrier as:## \psi_E(x)=\begin{cases}
e^{ikx}+Ae^{-ikx} \quad \quad x \le0 \\
Ce^{ikx} \quad \quad x\ge a \\
\end{cases} ##
where ##k^2=\frac{2mE}{\hbar^2}##. This system represents a particle that goes from ##\infnty## to ##0##, one part crosses the potential barrier and continues and one part goes back.

Now what I read in my notes is

"since the eigenfunctions of SE equation must not be equal to zero in a point with their first derivatives, then ##C \neq 0##".

How can I prove this statement? I think it is related to Cauchy's problem but I don't know how this implies that the eigenfunction would be equal to zero everywhere.
 
Last edited:
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Salmone said:
## \psi_E(x)=\begin{cases}
e^{ikx}+Ae^{-ikx} \quad \quad x \le0 \\
Ce^{ikx} \quad \quad x\ge a \\
\end{cases} ##
where ##k^2=\frac{2mE}{\hbar^2}##.

Now what I read in my notes is

"since the eigenfunctions of SE equation must not be equal to zero in a point with their first derivatives, then ##C \neq 0##".
If ##C = 0##, then the eigenfunction is identically zero for ##x \ge a##. I assume there are physical considerations that do not allow that.
 
We cannot answer your question, because you don't describe the specific setup considered. In QT you have to be very precise in the problem statement. Otherwise there's no chance to understand anything. Obviously your wave function is not defined in the interval ##(0,a)##. So even your state is not completely defined.
 
Salmone said:
@PeroK @vanhees71 I've edited the question.
It's been a while since I've looked at these problems, but I thought the coefficients on either side of the barrier were determined by the continuity of ##\psi(x)## and ##\frac{\partial \psi}{\partial x}## at the boundary of the barrier. So, you would need also to consider the wavefunction in the region ##0 < x < a##. That would force ##C \ne 0##.

I don't understand what this means:

Salmone said:
"since the eigenfunctions of SE equation must not be equal to zero in a point with their first derivatives, then ##C \neq 0##".
 
Last edited:
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