The Discontinuity of Wave Functions in a Dirac Delta Potential

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Discussion Overview

The discussion revolves around the behavior of wave functions in the presence of a Dirac delta potential, specifically addressing the continuity of wave functions and their derivatives at the potential's location. Participants explore the implications of discontinuities in the wave function and its derivative, touching on concepts of momentum and boundary conditions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents a scenario involving a particle in a Dirac delta potential and notes that the wave functions on either side are not continuous at the potential's location.
  • Another participant questions the meaning of the derivative of the wave function and its implications for momentum.
  • A participant suggests that the derivative of the wave function relates to momentum and expresses confusion about the continuity of momentum at the potential.
  • There is a discussion about the physical meaning of an abrupt change in momentum near a barrier and whether this presents a problem.
  • One participant introduces a separate issue regarding the momentum operator having complex eigenvalues while being a Hermitian operator.

Areas of Agreement / Disagreement

Participants express differing views on the implications of the discontinuity of the wave function and its derivative, particularly regarding momentum. The discussion remains unresolved with multiple competing perspectives on the physical interpretations involved.

Contextual Notes

Participants reference boundary conditions and the physical meanings of derivatives without reaching consensus on the implications of these concepts in the context of the Dirac delta potential.

hokhani
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consider a particle in one dimension. there is a dirac delta potential such as V=-a delat(x)
the wave functions in two sides(left and right) are Aexp(kx) and Aexp(-kx) respectively.
so the differential of the wave functions are not continious at x=0. what is the justification here?
 
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Good question. What do you think the answer might be? What is the meaning of the derivative of the wavefunction?
 
it is a criterion of the momentum and maybe they have opposite momentum. but i can't understand it exactly. i just know that one of the boundary conditions is the continuity of the differential of wave function!
 
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If you want me to help, I will. But you're going to have to work with me. Write in proper English, and don't scream at me by putting a bunch of exclamation points at the end.

Go back a step - what is the physical meaning of the derivative of the wavefunction?
 
ok. excuse me
i think the derivative of a wave function gives the momentum.
 
OK, good. Now, what's the derivative dp/dx of momentum?
 
i think it is the kinetic energy of the particle.
 
No, it's not, but you're close. Let's come at it from a different direction - I think I'm confusing you. And please write in correct English. Capital letters, punctuation, the whole thing.

You say that the derivative of the wavefunction is momentum, and you are worried that the momentum is discontinuous. What would it mean if the momentum as a function of position were not continuous?
 
sorry for my English and thank you for pointing that out.
my idea is that when the momentum direction is changed, we have a collision.
 
  • #10
Another problem:
Here the momentum operator P has complex eigenvalues while P is a Hermitian operator.
 
  • #11
OK, so you have an abrupt change of momentum near a barrier. Is that a problem?

On to your second question - if you have a different question, you should ask it on a different thread. Since you refuse to use proper English, such as capital letters, you'll have to find someone else to help you.
 

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