Wave Function: Normalization Constant

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The discussion focuses on finding the normalization constant for a wave function of a free particle, given by a plane wave in a localized region. The participants derive the normalization condition and clarify the relationship between the wave function and its modulus squared, ultimately determining that the normalization constant \( A \) is \( \frac{1}{\sqrt{a}} \). They also discuss the need to integrate the modulus squared of the wave function to ensure proper normalization. The conversation concludes with guidance on sketching the real and imaginary parts of the wave function, as well as its probability density.
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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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