Normalizing wavefunction obtained from Lorentzian wave packet

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Homework Help Overview

The discussion revolves around normalizing a wavefunction derived from a Lorentzian wave packet. The original poster presents an integral expression for the wavefunction and attempts to find the normalization constant.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to solve an integral to derive the wavefunction and subsequently seeks to normalize it. They express confusion regarding the convergence of the integral used for normalization. Some participants question the evaluation of the contour integral and suggest that multiple contours may be necessary.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the contour integral evaluation. Guidance has been offered regarding the application of Jordan's Lemma, but no consensus has been reached on the correct approach to the problem.

Contextual Notes

There is uncertainty regarding the correctness of the wavefunction and the normalization process, as well as the implications of using different contour paths in the integral evaluation.

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Homework Statement
1. Consider a wave packet with $$ A(k) = \frac {N}{k^2 + \alpha^2} $$
where ##\alpha## is some positive constant. This is Lorentzian wave packet.

a. Find the form of ##\psi(x) ## (You may have to use your knowledge of contour integrals in Complex analysis)
b. Find normalization N such that $$ \int_{-\infty}^{\infty} dx\left | \psi(x) \right |^2 = 1 $$
Relevant Equations
Wave obtained by superposing waves with different amplitude ##A(k)## depending on k is given by:
$$\psi(x) = \int_{-\infty}^{\infty} A(k)e^{ikx}dk $$
Part a: Using the above equation. I got
$$\psi(x) = \int_{-\infty}^{\infty} \frac{Ne^{ikx}}{k^2 + \alpha^2}dk $$

So basically I needed to solve above integral to get the wave function. To solve it, I used Jordan's Lemma & Cauchy Residue Theorem.
And obtained $$\psi(x) = \frac {N \pi e^{-x\alpha}}{\alpha} $$

For part b, I need to find value of N by solving the equation: $$ \frac {\pi ^2 N^2}{\alpha^2} \int_{-\infty}^{\infty} e^{-2x\alpha} dx = 1 $$
Which I obtained as $$|\psi(x)|^2 = \frac {N^2\pi^2}{\alpha^2} e^{-2x\alpha} $$
Now, this integral is not converging. So either my wavefunction is incorrect or I'm doing something wrong in part b. A friend of mine also got same ##\psi(x) ## due to which I'm really confused as to where could we be going wrong.
 
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You didn't evaluate the contour integral correctly. You should have two contours, one for ##x>0## and one for ##x<0##.
 
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Likes   Reactions: vanhees71
I'm not able to understand why it will have two contours and not 1 i.e ##x = -\infty## to ## x=+\infty##. Can you please explain
 

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