What Happens When a Particle Encounters a Step Potential Higher Than Its Energy?

heardie
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Hi...I've come across this question on a past exam, and I can't seem to resolve it!

A particle is incident on a step potential at x=0. The total energy of the particle E, is less then the height of the step, U. The particle has wavefunctions
$\begin{array}{l}<br /> \psi (x) = \frac{1}{2}\{ (1 + i)e^{ikx} + (1 - i)e^{ - ikx} \} ,x \ge 0 \\ <br /> \psi (x) = e^{ - kx} ,x &lt; 0 \\ <br /> \end{array}$<br />

Note that k is the same on both sides of the step
a) ….
b.) How must k be related to E and U on both sides of the step and determine the ration E/U

Well on the left, it is just a free wave-function where k=$k = \frac{{\sqrt {2mE} }}{\hbar }$<br />
On the right k= $k = i\kappa = \frac{{i\sqrt {2m(U - E)} }}{\hbar }$<br />
Since the k’s are equal this immediately implies that U=0, does it not? In which case the ratio E/U is infinite…
 
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heardie said:
Since the k’s are equal this immediately implies that U=0, does it not? In which case the ratio E/U is infinite…
No, but you are thinking along the right lines. You have recognized that the requirement on k puts strong restriction on ... something. Attack the problem firstly as if k were different in the two regions, and then see what conditions have to be met so that the wavefunction can be put in the given form. (Biggest hint: Notice that there is an i in the exponent in one region and not in the other.)

One thing I just noticed: it appears to me that the particle is incident from the right so you may have your suggestions backwards.
 
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Ok so if I call the region II solution k'
$k&#039; = \frac{{\sqrt {2m(E - U)} }}{\hbar }$

Since U > E this is complex.
$k&#039; = \frac{{i\sqrt {2m(U - E)} }}{\hbar } = i\kappa $<br />

This leads to the exponential solution
$e^{ - \kappa x} $<br />

If I then impose
$\kappa = k$ i get
$\begin{array}{l}<br /> \frac{{\sqrt {2mE} }}{\hbar } = \frac{{\sqrt {2m(U - E)} }}{\hbar } \\ <br /> \sqrt E = \sqrt {U - E} \\ <br /> E = U - E \\ <br /> 2E = U \\ <br /> E = \frac{U}{2} \\ <br /> \end{array}$<br />

oh hey...i definatly did that yesterday...musta been dropping a negative somewhere!

Ok, seems my latex sucks but how is E=U/2??

Cheers!
 
heardie said:
... how is E=U/2??
That was my initial gut feeling about it. Are you asking how it is possible, or are you asking if I think this is correct? I think it is probably correct (without actually combing through your calculations).
 
Turin - I don't think I would ever ask if something is possible in QM, per se, since things that seem impossible always seem to fall out of QM! So much more to learn as well - makes me wonder what other things (classically impossible) will occur
 
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
If we release an electron around a positively charged sphere, the initial state of electron is a linear combination of Hydrogen-like states. According to quantum mechanics, evolution of time would not change this initial state because the potential is time independent. However, classically we expect the electron to collide with the sphere. So, it seems that the quantum and classics predict different behaviours!
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