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.

teme92
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Homework Statement


Consider a free particle, initially with a well defined momentum ##p_0##, whose wave function is well approximated by a plane wave. At ##t=0##, the particle is localized in a region ##-\frac{a}{2}\leq x \leq\frac{a}{2}##, so that its wave function is

##\psi(x)=\begin{cases} Ae^{-ip_0x/\hbar} & if -\frac{a}{2}\leq x \leq\frac{a}{2} \\0 & \text{otherwise} \end{cases}##

Find the normalization constant ##A## and sketch ##Re(\psi(x))##, ##Im(\psi(x))## and ##|\psi(x)|^2##.

Homework Equations

The Attempt at a Solution


So here's what I done:

##A^2\int_{-\frac{a}{2}}^\frac{a}{2} e^{-ip_0x/\hbar}dx=1##

##A^2.-\frac{\hbar}{ip_0}.e^{-ip_0x/\hbar}=1##

##A^2=-\frac{ip_0}{\hbar}.\frac{1}{e^{-ip_0a/2\hbar}-e^{-ip_0a/2\hbar}}##

Is this the correct method? Also I have no idea how to sketch the function asked. Any help would be greatly appreciated.
 
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teme92 said:
##A^2\int_{-\frac{a}{2}}^\frac{a}{2} e^{-ip_0x/\hbar}dx=1##

How did you get this?
 
I took it from ##P(t)=\int_{-\frac{a}{2}}^\frac{a}{2}|\psi(x,t)|^2=1## subbed my wave function into that then. Is this method wrong?
 
If ##\psi \left( x \right) =Ae^{-ip_0x/\hbar}##, what is ##\left| \psi \left( x \right) \right|^2##?
 
##|\psi(x)|^2=A^2e^{-2ip_0z/\hbar}##?
 
teme92 said:
##|\psi(x)|^2=A^2e^{-2ip_0z/\hbar}##?

Not quite. If ##Z## is a complex number, are ##Z^2## and ##\left|Z\right|^2## the same?
 
No, ##|Z|^2## is the modulus squared ie. ##(\sqrt{a^2+b^2})^2##
 
teme92 said:
No, ##|Z|^2## is the modulus squared ie. ##(\sqrt{a^2+b^2})^2##

Yes. What if the complex value ##Z## is expressed in polar notation?
 
Is it ##cos\theta +isin\theta##?
 
  • #10
Well, ##e^{i\theta} = \cos \theta + i \sin \theta##. What is ##\left| e^{i\theta} \right|^2## for real ##\theta##?
 
  • #11
##sin2\theta + 1##?
 
  • #12
teme92 said:
##sin2\theta + 1##?

No. You're making this more difficult than it actually is. Forget about a and b and theta. Can you express ##\left| Z \right|^2## in terms of ##Z## and the complex conjugate of ##Z##?
 
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  • #13
Remember, also. The complex conjugate of ##\psi##, and ##|\psi|^2=\psi^{*}\psi##.

Chris
 
  • #14
Oh ##|\psi|^2=z\bar{z}##
 
  • #15
Yes! And if ##z = e^{i\theta}##, then ##\bar{z} = ##?
 
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  • #16
Is it ##\bar{z}=e^{-i\theta}##?
 
Last edited:
  • #17
When complex conjugating, what is done to every ##i##?
 
  • #18
Sorry I was supposed to put a minus in that I'll edit
 
  • #19
teme92 said:
Is it ##\bar{z}=e^{-i\theta}##?

And ##z \bar{z} =##?
 
  • #20
They ##i\theta## and ##-i\theta## cancel each other out so ##e^0=1##
 
  • #21
Good. Now, go back to the original question.
 
  • #22
So ##|\psi(x)|^2 = 1##?
 
  • #23
What about the normalization constant ##A##, which, without loss of generality, can be taken to be real and positive?
 
  • #24
##A=\frac{1}{e^{-ip_0x/\hbar}}##?
 
  • #25
teme92 said:
I took it from ##P(t)=\int_{-\frac{a}{2}}^\frac{a}{2}|\psi(x,t)|^2=1## subbed my wave function into that then. Is this method wrong?

Redo the above.
 
  • #26
##A^2\int_{-\frac{a}{2}}^\frac{a}{2} e^{-2ip_0x/\hbar}dx=1##

##A^2.-\frac{\hbar}{ip_0}.e^{-i2p_0x/\hbar}=1##

##A^2=-\frac{ip_0}{\hbar}.\frac{1}{e^{-ip_0a/\hbar}-e^{-ip_0a/\hbar}}##

Is this correct and if so where do I go. Square rooting this seems wrong
 
Last edited:
  • #27
No. What is

$$\overline{e^{-ip_0x/\hbar}}?$$
 
  • #28
##e^{ip_0x/\hbar}##?
 
  • #29
Yes.
 
  • #30
I'm getting confused over what ##(Ae^{-i{p_0}x/\hbar})^2## is. And then the integrating of that.
 

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