I Wavefunction properties tunneling effect

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The discussion centers on the tunneling effect and the properties of wavefunctions in quantum mechanics, specifically regarding a potential barrier. The Hamiltonian eigenfunctions are defined outside the barrier, and there is a question about proving that the coefficient C must be non-zero to avoid the eigenfunction being identically zero for x ≥ a. The continuity of the wavefunction and its derivative at the boundaries of the barrier is emphasized as crucial for determining the coefficients. Additionally, the need for a precise problem statement in quantum theory is highlighted to ensure clarity in the analysis. Understanding these concepts is essential for accurately describing the behavior of particles in quantum mechanics.
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.
 
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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##".
 
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Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. Towards the end of the first lecture for the Qiskit Global Summer School 2025, Foundations of Quantum Mechanics, Olivia Lanes (Global Lead, Content and Education IBM) stated... Source: https://www.physicsforums.com/insights/quantum-entanglement-is-a-kinematic-fact-not-a-dynamical-effect/ by @RUTA

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