Finding Momentum and Uncertainty in Quantum Mechanics Problem 1.17

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SUMMARY

In Problem 1.17 of Griffiths' quantum mechanics textbook, the state function is defined as psi = A(a^2 - x^2) for the interval -a to a, and zero otherwise. To find the expected value of momentum p at time t = 0 and the uncertainty in p, the Fourier transform of the wave function is the appropriate method. Despite initial confusion about the definition of momentum, the Fourier transform provides a clear solution to the problem.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly wave functions.
  • Familiarity with Fourier transforms in the context of quantum mechanics.
  • Knowledge of momentum operators in quantum mechanics.
  • Basic skills in solving problems from Griffiths' "Introduction to Quantum Mechanics".
NEXT STEPS
  • Study the application of Fourier transforms to wave functions in quantum mechanics.
  • Review the concept of momentum operators and their expected values in quantum systems.
  • Explore uncertainty principles in quantum mechanics, focusing on momentum and position.
  • Practice additional problems from Griffiths' textbook to reinforce understanding of these concepts.
USEFUL FOR

Students of quantum mechanics, particularly those studying Griffiths' textbook, and anyone looking to deepen their understanding of momentum and uncertainty in quantum systems.

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Problem 1.17 in griffiths gives, at time t = 0, the state psi =A(a^2-x^2) for -a to a, and 0 otherwise. It asks then to find the expected value of momentum p at 0 and also the uncertainty in p. How do I do this? The only way momentum is defined is md<x>/dt, and since the state is only for time t, there seems to be no way to do this.

I know that if i take Fourier transform the wave function i'll get the expected momentum, but I don't think that's what the problem wants me to do. Is there a simpler way?
 
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never mind, I'm an idiot.
 
Glad we could help. :biggrin:
 
Tom Mattson said:
Glad we could help. :biggrin:
:smile: :smile: :smile:
 

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