Question on step potentials and schrodingers equatio

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Discussion Overview

The discussion revolves around the behavior of wave functions in quantum mechanics, specifically in the context of one-dimensional step potentials and the Schrödinger equation. Participants explore the conditions under which certain solutions to the equation may vanish, the implications of potential barriers, and the nature of wave functions in different regions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that solving the Schrödinger equation for 1D step potentials yields two solutions, representing waves traveling from the left and right, but questions when one of these solutions may vanish.
  • Another participant poses a specific scenario involving a potential well with infinite potential on one side, zero in the middle, and finite potential on the right, asking whether both currents would exist in this configuration.
  • A participant elaborates on the reasoning that in a region where a wave is transmitted (x > a), only one solution should exist as there is no reflection point, leading to the conclusion that the wave traveling to the right is the only one present.
  • It is mentioned that a non-normalizable solution must vanish, particularly when it diverges to infinity, such as with the function e^{bx} in certain domains.

Areas of Agreement / Disagreement

Participants express uncertainty regarding the conditions under which solutions vanish, with multiple viewpoints on the implications of potential barriers and the behavior of wave functions in different regions. No consensus is reached on the specific rules or conditions that govern these phenomena.

Contextual Notes

Participants discuss the implications of boundary conditions and the physicality of quantum tunneling, but there are unresolved mathematical steps and assumptions regarding the behavior of wave functions in various potential scenarios.

marmot
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I have a problem. I am trying to selfteach myself QM but I got stumped with this.

Basically, in the issue of 1D step potentias, I know that you have to divide the problem into regions and solve the Schrödinger equation for each one. However, when you solve it, you always get two solutions due to the nature of the second order linear differential equation. (One representig a current oming from the left and the other from the right) However, I know sometimes one of the solutions vanishes. For ezample. if V>E in a<x<infinity, the solution will be an exponential wih negative exponent because the positive one vanishes (due to the physicallity of quantum tunneling. In certain instances there will be two solutions because of reflection, etc. However, how do I know when a solution vanishes? Are they rules of thumb or you simply solve for the coefficients using initial conditions?
 
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A specific question would be if a potential well with infinite potenial in one side, zero in the middle, and a finite potenial in the right side would have both current going to the right and the left?
 
marmot said:
I have a problem. I am trying to selfteach myself QM but I got stumped with this.

Basically, in the issue of 1D step potentias, I know that you have to divide the problem into regions and solve the Schrödinger equation for each one. However, when you solve it, you always get two solutions due to the nature of the second order linear differential equation. (One representig a current oming from the left and the other from the right) However, I know sometimes one of the solutions vanishes. For ezample. if V>E in a<x<infinity, the solution will be an exponential wih negative exponent because the positive one vanishes (due to the physicallity of quantum tunneling. In certain instances there will be two solutions because of reflection, etc. However, how do I know when a solution vanishes? Are they rules of thumb or you simply solve for the coefficients using initial conditions?

In this case (in "bold"):
Lets say the wave is sent from the negative x-axis. In the region x<a, you will have two solutions because you have a wave traveling to the right (you sent it) and a reflected one from the potential. However, in the region a<x<oo we can't have two solutions. We only have a wave traveling to the right, no wave is traveling to the left since there is no other point (like a step potential) to reflect your wave.
So imagine a wave traveling at x=a, then some been reflected and other transmitted. The one that's been transmitted will be "alone" in that region (x>a).
 
Also, a solution that is non-normalizable has to vanish. This usually happens when it goes to infinity at some point, for example a solution of e^{bx} on the domain a&lt;x. The wavefunction would go to infinity as x\to\infty so there's no way to normalize it.
 

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