Spreading of a Free-Particle Gaussian Wave Packet

Click For Summary
SUMMARY

The discussion focuses on the calculation of the position probability density for a one-dimensional free-particle Gaussian wave packet, specifically using the formula P(x,t) = sqrt(1/(1+t^2)) exp(-(x-vt)^2/(2(1+t^2))). The participant attempts to integrate this probability density using Mathematica but arrives at an incorrect result, Sqrt[2Pi]vt, which does not match the provided answer choices. The key issue identified is that the probability density P(x,t) is not properly normalized, which is crucial for accurate calculations in quantum mechanics.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly wave packets.
  • Familiarity with Mathematica for computational tasks.
  • Knowledge of probability density functions in quantum mechanics.
  • Basic calculus skills for performing integrals.
NEXT STEPS
  • Review normalization techniques for wave functions in quantum mechanics.
  • Learn how to use Mathematica for integrating functions and handling probability densities.
  • Study the concept of Gaussian wave packets and their properties in quantum mechanics.
  • Explore the implications of position uncertainty and its mathematical representation.
USEFUL FOR

Students and researchers in quantum mechanics, particularly those working with wave packets and computational methods in Mathematica. This discussion is also beneficial for anyone seeking to understand the normalization of probability densities in quantum systems.

derelictee
Messages
2
Reaction score
0

Homework Statement



It can be shown that the position probability density for the one-dimensional, free-particle Gaussian wave packet can be expressed as shown below, where m is the mass of the particle and L is the position uncertainty at time t=0, vgr = hbar *k0/m, k0 is the average wave number as discussed in class. Let x, t and P(x,t) be measured, respectively, in units of L, T=2mL^2/hbar, A=1/sqrt(2pi*L^2), then the position probability can be written as P(x,t)= sqrt(1/(1+t^2)) exp(-(x-vt)^2/(2 (1+t^2)), where v= 2 mLvgr/hbar. In order to demonstrate the spreading of the wave packet, use Mathematica to calculate <x> in units of L at time t./>

Homework Equations


<x> = integral from -infinity to infinity of x times psi squared

The Attempt at a Solution


I am both a mathematica and quantum mechanics novice, so I'm not sure where my mistake lies. Since psi[x,t]^2 = P[x,t], I integrated P(x,t)= sqrt(1/(1+t^2)) exp(-(x-vt)^2/(2 (1+t^2)) from -infinity to infinity with respect to x and got the answer Sqrt[2Pi]vt. That's not one of the answer choices. The answer choices are: 0, vt, sqrt(1+t^2 (1+v^2)), or sqrt(1+t^2 ). Where did I go wrong? [Note: I don't really understand all of that "in units of L" bit in the question.] Thanks in advance.
 
Physics news on Phys.org
P(x,t) is not properly normalized.
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
2K
Replies
2
Views
2K
Replies
9
Views
3K
  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 0 ·
Replies
0
Views
2K
  • · Replies 7 ·
Replies
7
Views
3K
Replies
24
Views
3K
Replies
7
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K