Normalizing Wave Function of A Ring

Click For Summary
SUMMARY

The discussion focuses on normalizing the wave function of a ring, represented by the equation \(\psi_{n}(\theta)=A_{n} \exp(\imath n \theta)\). The normalization condition leads to the calculation of the factor \(A_{n}\) over the interval \(\theta = 0\) to \(\theta = 2\pi\). The correct normalization yields \(A_{n}=\frac{1}{\sqrt{2\pi}}\), confirming that the wave function is properly normalized. Additionally, it is noted that multiplying \(A_{n}\) by any phase factor still satisfies the normalization condition.

PREREQUISITES
  • Understanding of wave functions in quantum mechanics
  • Familiarity with complex exponentials and their properties
  • Knowledge of normalization conditions in quantum mechanics
  • Basic calculus, particularly integration over defined intervals
NEXT STEPS
  • Study the properties of complex numbers and their magnitudes
  • Learn about normalization techniques in quantum mechanics
  • Explore the implications of phase factors in wave functions
  • Investigate the role of boundary conditions in quantum systems
USEFUL FOR

Students and professionals in quantum mechanics, physicists working with wave functions, and anyone interested in the mathematical foundations of quantum theory.

mdmman
Messages
5
Reaction score
0

Homework Statement



<br /> \psi_{n}(\theta)=A_{n} \exp(\imath n \theta)<br />
where n is an integer

Calculate the factor A_{n} if the wave function is normalized between
\theta = 0 and \theta = 2\pi.

Homework Equations


NA

The Attempt at a Solution



<br /> 1=\int_0^{2\pi} |\psi_{n}(\theta)|^2 d\theta<br />

<br /> 1=|A_{n}|^2\int_0^{2\pi} \exp(2\imath n \theta) d\theta<br />

<br /> 1=|A_{n}|^2 [\frac{.5sin(2n\theta)}{n} - \frac{.5cos(2n\theta)}{n} \imath]_0^{2\pi}<br />

<br /> 1=|A_{n}|^2 [0]<br />

<br /> 1=0<br />

Obviously 1 does not equal 0 :) . Am I missing something?
 
Physics news on Phys.org
What does \| \exp(\imath n \theta) \|^2 equal?
 
<br /> \| \exp(\imath n \theta) \|^2 = \| \exp(2\imath n \theta) \| = \|cos(2n\theta)+sin(2n\theta)\imath \|<br />

correct?
 
You just took the square of the wavefunction, instead of the absolute value squared.
 
If z = a + \imath b, where a and b are both real, what does |z|^2 equal?
 
<br /> \| \exp(\imath n \theta) \|^2 = 1<br />

Man, I can't believe I missed that!

<br /> 1=|A_{n}|^2\int_0^{2\pi} \|\exp(\imath n \theta)\|^2 d\theta<br />

<br /> 1=|A_{n}|^2\int_0^{2\pi} 1 d\theta<br />

<br /> 1=|A_{n}|^2[\theta]_0^{2\pi}<br />

<br /> 1=|A_{n}|^2*2\pi<br />

<br /> A_{n}=\frac{1}{\sqrt{2\pi}}<br />

This is the correct solution, right?
 
mdmman said:
This is the correct solution, right?

This looks good and is probably the expected answer, but note that multiplying your A_n by any phase factor would give something that also works.
 

Similar threads

Replies
7
Views
2K
  • · Replies 16 ·
Replies
16
Views
4K
Replies
4
Views
1K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 12 ·
Replies
12
Views
2K
Replies
6
Views
4K
  • · Replies 20 ·
Replies
20
Views
2K
Replies
2
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 14 ·
Replies
14
Views
2K