Finding Normalization Constants for a Set of Energy Eigenstates

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SUMMARY

This discussion focuses on finding normalization constants for energy eigenstates in a one-dimensional plane wave encountering a potential barrier where the energy (E) is less than the potential (V). The equations provided are derived from Allan Adams' Lecture 12 of his 2013 Quantum Physics 1 course. Key equations include A + B = D and ikA - ikB = -aD, with solutions for D and B expressed as D = (2k)/(k + ia) and B = (k - ia)/(k + ia). The discussion emphasizes the need for normalization constants to avoid discontinuities in the wavefunction at the barrier.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically wavefunctions and energy eigenstates.
  • Familiarity with solving systems of linear equations.
  • Knowledge of normalization techniques for quantum states.
  • Basic grasp of complex numbers and their applications in quantum mechanics.
NEXT STEPS
  • Study matrix inversion techniques in the context of quantum mechanics.
  • Learn about normalization of unbound states in quantum mechanics.
  • Explore the implications of potential barriers on wavefunctions in quantum mechanics.
  • Review Allan Adams' Quantum Physics 1 Lecture 12 for deeper insights into the topic.
USEFUL FOR

Students and professionals in quantum mechanics, particularly those studying wavefunctions and energy eigenstates, as well as educators seeking to clarify concepts related to normalization in quantum systems.

jaurandt
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I do not know what I'm doing wrong but I'm working on the problem of finding the normalization constants for the energy eigenstate equation for a 1D plane wave that is traveling from the left into a potential barrier where E < V at the barrier. This is from Allan Adams' Lecture 12 of his 2013 Quantum Physics 1 lectures.

The system of equations left at x = 0 is

A + B = D
ikA - ikB = -aD (for the derivatives)

And he wrote that

D = (2k)/(k + ia)

and

B = (k - ia)/(k + ia)

He said we can "invert" the original equations to get those. After many attempts, I can't figure it out. Can someone please guide me along before I pull all of my hair out?
 
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jaurandt said:
A + B = D
ikA - ikB = -aD (for the derivatives)
I think "invert" probably refers to matrix inversion.
You have two equations and three unknowns here. That means that the system of equations has an infinite number of solutions. You could find a solution by considering A to be a parameter and solving for B and D in terms of A (treating A like a constant). Then you can set A to whatever constant value you choose (1 for example) to get corresponding values for B and D.
 
First of all, the normalization constants on both sides of the potential step have to be such that the wavefunction doesn't have a jump discontinuity at the beginning of the barrier. But that only determines the relative magnitudes of the two constants.

Unbound plane wave states are not normalized in the same way as bound states where the normalization makes the total probability of finding the particle to be 1. Maybe the correct way to set the normalization is one where the pre-factor before the barrier (when ##V=0##) is the ##1/\sqrt{2\pi \hbar}##, as in the link below.

https://quantummechanics.ucsd.edu/ph130a/130_notes/node138.html
 

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