Particle in a box momentum uncertainty

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SUMMARY

This discussion focuses on the quantum mechanics problem of a particle in an infinite potential well, specifically addressing the calculation of position and momentum uncertainties (\(\Delta x\), \(\Delta p\), and \(\Delta x \Delta p\)). The wave functions for the particle are defined using trigonometric functions, and the energy levels are derived from the formula \(E_n = \frac{h^2}{2m}\left(\frac{n\pi}{a}\right)^2\). The conversation also explores the transition of the particle when the potential well's boundaries are expanded, requiring the calculation of probabilities for the particle being in the ground and first excited states of the new potential.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically the infinite potential well model.
  • Familiarity with wave functions and their properties in quantum systems.
  • Knowledge of the uncertainty principle in quantum mechanics.
  • Ability to perform calculations involving eigenstates and probabilities in quantum systems.
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  • Study the derivation of wave functions for the infinite potential well using trigonometric functions.
  • Learn how to calculate the variance of position and momentum for quantum states.
  • Research the implications of the uncertainty principle on quantum states and measurements.
  • Explore the concept of probability amplitudes and their role in determining state probabilities in quantum mechanics.
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Students and professionals in physics, particularly those specializing in quantum mechanics, as well as educators looking for practical examples of quantum state transitions and uncertainty calculations.

Vaal
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this is for a particle in a box (infinite potential well):
For the wave functions calculate (as a function of n)
\Deltax
\Deltap
\Deltax\Deltap

Homework Equations


h = h bar below

u+n(x)=(1/\sqrt{a} )cos((n-1/2)(pi)x/a)
u-n(x)=(1/sqrt{a})sin(n(pi)x/a)
E-n=h2/(2m)(n(pi)/a)2
E+n=h2/(2m)((n-1/2)(pi)/a)2

The Attempt at a Solution


ok i think the Delta x is easy, just find the variance of u+n(x)2 and u-n(x)2 as a function of n (correct me if i am wrong)

where i am lost is on the momentum, i can obviously get it from the energy but i don't see how to determine its variance or even how it would change within one state. i would just use the uncertainty principle but that seems to be what they want you to show in the next step (also it is an inequality not an exact equation)

thanks for any help and sorry if this is an absurd question, it has been awhile since i have done any of this sort of stuff.
 
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Find \langle \hat{p}^2 \rangle where

\hat{p} = \frac{\hbar}{i}\frac{\partial}{\partial x}
 
Ok, I think I figured out the first part described above, although I can't seem to make the numbers come out right.

I am lost on the next problem, even more so than the last.

My well currently has walls at +/- a and a particle is in the ground state. the walls are suddenly moved to +/- b with b>a,
what is the probability the particle will be in ground state of new potential? & what is probability of the particle being in first excited state?

i realize the ground state of the new potential has less energy so the particle is more likely to be at a higher state than it was in the old potential but i have no idea how to make it quantitive and get the exact probabilities. any help would be greatly appreciated. thanks
 
Vaal said:
My well currently has walls at +/- a and a particle is in the ground state. the walls are suddenly moved to +/- b with b>a,
what is the probability the particle will be in ground state of new potential? & what is probability of the particle being in first excited state?

i realize the ground state of the new potential has less energy so the particle is more likely to be at a higher state than it was in the old potential but i have no idea how to make it quantitive and get the exact probabilities. any help would be greatly appreciated. thanks
Let the particle be in the state |\psi\rangle and let |\phi_n\rangle for n=1, 2, 3, … denote the eigenstates of the new Hamiltonian. You can express |\psi\rangle in terms of the new eigenstates:

|\psi\rangle = c_0|\phi_0\rangle + c_1|\phi_1\rangle + \cdots

where the cn's are constants, possibly complex. You need to find what the cn's are for n=0 and n=1. The probability of finding the particle in a particular state is equal to the modulus squared of the corresponding constant.
 

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