Particle in a box: possible momentum and probability

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SUMMARY

The discussion focuses on the quantum mechanics problem of a particle in a box, specifically analyzing the wave function \(\Psi(x,0) = \frac{1}{\sqrt{L}}\) for \(|x| < L/2\). The participant explores the relationship between position uncertainty \(\Delta x\) and momentum uncertainty \(\Delta p\), concluding that \(\Delta p \geq \frac{\hbar}{2L}\). The Fourier transform of the wave function is calculated to find the momentum probability distribution, leading to the expression \(a(k) = \frac{2}{k\sqrt{L}} \sin(\frac{L}{2}k)\). The normalization of the wave function before and after the Fourier transform is confirmed to maintain normalization.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically the particle in a box model.
  • Familiarity with Fourier transforms in the context of wave functions.
  • Knowledge of normalization conditions for quantum states.
  • Basic grasp of uncertainty principles in quantum mechanics.
NEXT STEPS
  • Study the implications of the Heisenberg uncertainty principle in quantum mechanics.
  • Learn about normalization techniques for wave functions in quantum systems.
  • Explore the application of Fourier transforms in quantum mechanics, particularly for momentum space analysis.
  • Investigate the properties of wave functions in different potential wells beyond the infinite square well.
USEFUL FOR

Students of quantum mechanics, physicists working on wave-particle duality, and anyone interested in the mathematical foundations of quantum states and their properties.

C. Darwin
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Homework Statement


\Psi(x,0) = \frac{1}{\sqrt{L}}, ~~~~~~ \left|x\right| &lt; L/2

At the same instant, the momentum of the particle is measured, what are the possible values, and with what probability?

Homework Equations


The Attempt at a Solution


Well, I know that \Delta{}x = L so can I then say that since \Delta{}p \geq \frac{\hbar}{2L} p must be greater than the same amount?

As far as finding the probability goes, I think I need to do the Fourier transform a(k) = \int_{-L/2}^{L/2} \frac{1}{\sqrt{L}} e^{-ikx} dx = \frac{2}{k\sqrt{L}}sin(\frac{L}{2}k)

Now if I take the square of a(k), how do I normalize it? What are the limits of the integral? If I normalize Psi(x) before I do the Fourier transform, will it be normalized after?
 
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been a while since I've done these, but if psi is normalised, & you perform your Fourier transform with the correct constants, the momentum expression will also be normalised. (could always check on an easy function to integrate)

the momentum probability integral will have limits from -infinity to infinity.

The position integration is in essence the same, however you know psi is zero outside the box
 

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