Wave Function: Normalization Constant

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SUMMARY

The discussion centers on finding the normalization constant ##A## for a wave function of a free particle, represented as ##\psi(x)=Ae^{-ip_0x/\hbar}## within the interval ##-\frac{a}{2}\leq x \leq\frac{a}{2}##. The correct normalization condition leads to the conclusion that ##A=\frac{1}{\sqrt{a}}##. Participants also clarified the relationship between the wave function's modulus squared and its complex conjugate, emphasizing that ##|\psi(x)|^2 = A^2## within the defined region. Additionally, they discussed how to sketch the real and imaginary parts of the wave function.

PREREQUISITES
  • Understanding of wave functions in quantum mechanics
  • Familiarity with complex numbers and their properties
  • Knowledge of normalization conditions in quantum mechanics
  • Ability to perform integrals involving complex exponentials
NEXT STEPS
  • Study the derivation of normalization constants in quantum mechanics
  • Learn about the properties of complex conjugates and their applications
  • Explore graphical representations of wave functions and their components
  • Investigate the implications of wave function normalization on probability distributions
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Students of quantum mechanics, physicists working with wave functions, and anyone interested in the mathematical foundations of quantum theory.

  • #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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