Wave Function: Normalization Constant

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Homework Help Overview

The discussion revolves around the normalization constant for the wave function of a free particle, which is represented as a plane wave. The wave function is defined in a specific region and participants are exploring how to find the normalization constant and sketch the real and imaginary parts of the wave function, as well as its modulus squared.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the integration of the wave function to find the normalization constant and question the validity of their methods. There are inquiries about the relationship between the wave function and its modulus squared, as well as the implications of complex numbers in this context.

Discussion Status

The discussion is ongoing with various attempts to clarify the normalization process and the properties of complex numbers. Some participants have provided guidance on how to express the modulus squared of the wave function, while others are still grappling with the integration and normalization steps.

Contextual Notes

There are indications of confusion regarding the integration of complex functions and the interpretation of results, as well as the need to adhere to specific homework constraints regarding the normalization process.

  • #31
teme92 said:
I'm getting confused over what ##(Ae^{-i{p_0}x/\hbar})^2## is. And then the integrating of that.

You are not supposed to integrate ##(Ae^{-i{p_0}x/\hbar})^2##, you are supposed to integrate ##|Ae^{-i{p_0}x/\hbar}|^2##.
 
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  • #32
So would that be ##A^2(1)## as ##|e^{-i{p_0}x/\hbar}|^2=1##?
 
  • #33
Yes.
 
  • #34
So ##A=1##? Thanks for all the help George. How do I proceed to sketch the items asked? I assume ##A## is the real part and ##e^{-i{p_0}x/\hbar}## the imaginary part and ##|\psi(x)|^2=1##. How do these look when sketched?
 
  • #35
teme92 said:
So ##A=1##?

No. Remember, you have to calculate

$$\int^{a/2}_{-a/2} \left| \psi \left(x\right) \right|^2 dx.$$
 
  • #36
Ah there's still the ##dx## left:

##\frac{a}{2}+\frac{a}{2}=a##, therefore ##A=\frac{1}{a}##
 
  • #37
Not quite. There is an A from psi, and another A from \bar{psi}.
 
  • #38
##A=\frac{1}{\sqrt{a}}##?
 
  • #39
Looks okay.
 
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  • #40
Brilliant, and regarding the sketch part?
 
  • #41
What are ##Re(e^{-i\theta})## and ##Im(e^{-i\theta})##?
 
  • #42
##Re=\theta## and ##Im=-i##?
 
  • #43
No. Recall how ##e^{i\theta}## was expressed earlier in the thread.
 
  • #44
Oh I get you. ##Re=cos\theta## and ##Im=isin\theta##?
 

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