Sudden Perturbation of Potential Well

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Homework Help Overview

The discussion revolves around a quantum mechanics problem involving a particle in a potential well that suddenly changes in length. The original well has a length of 'a' with infinite potential barriers outside this range, and it is suddenly extended to a length of '2a'. The participants are exploring the implications of this change on the particle's ground state probability and the time duration for the change.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the overlap of wavefunctions before and after the potential change, questioning how the initial wavefunction behaves in the new region. There is also consideration of the time evolution of the wavefunction and whether the adiabatic approximation is applicable for the time duration of the change.

Discussion Status

The discussion is active, with participants examining the mathematical details of the overlap integral and its implications for the probability of the particle remaining in the ground state. Some have provided calculations, while others are seeking clarification on the initial conditions and the use of approximations.

Contextual Notes

There is an emphasis on the forbidden region for the wavefunction prior to the potential change, which influences the calculations being discussed. Participants are also navigating the constraints of the problem as it relates to the sudden perturbation of the potential well.

unscientific
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Homework Statement



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Part (a): Particle originally sits in well V(x) = 0 for 0 < x < a, V = ∞ elsewhere. The well suddenly doubles in length to 2a. What's the probability of the particle staying in its ground state?

Part (b): What is the duration of time that the change occur, for the particle to most likely remain in ground state?

Homework Equations





The Attempt at a Solution



Part (a)

For a well of length a, eigenfunction is:

[tex]u = \sqrt{\frac{2}{a}} sin \left(\frac{\pi x}{a}\right)[/tex]

For a well of length 2a, eigenfunction is:

[tex]v = \frac{1}{\sqrt a} sin \left(\frac{\pi x}{2a}\right)[/tex]

For probability amplitude, overlap these 2:

[tex]\frac{1}{2} \frac{\sqrt 2}{a} \int_0^{2a} 2 sin (\frac{\pi x}{a}) sin (\frac{\pi x}{2a}) dx[/tex]

[tex]\frac{1}{2} \frac{\sqrt 2}{a} \int_0^{2a} cos (\frac{3\pi x}{2a}) - cos (\frac{\pi x}{2a}) dx[/tex]

which goes to zero.

Part (b)

Am I supposed to use time evolution: ## |\psi_t> = U^{-i\frac{E}{\hbar}t}## ? Doesn't seem to help..
 
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unscientific said:
[tex]\frac{1}{2} \frac{\sqrt 2}{a} \int_0^{2a} 2 sin (\frac{\pi x}{a}) sin (\frac{\pi x}{2a}) dx[/tex]

[tex]\frac{1}{2} \frac{\sqrt 2}{a} \int_0^{2a} cos (\frac{3\pi x}{2a}) - cos (\frac{\pi x}{2a}) dx[/tex]

What is the initial wavefunction in the region [itex]a<x<2a[/itex]?
 
king vitamin said:
What is the initial wavefunction in the region [itex]a<x<2a[/itex]?

It is 0 before the change in the potential, since it is a forbidden region.
 
unscientific said:
It is 0 before the change in the potential, since it is a forbidden region.

Right. Do you see how that affects your overlap integral? It might help to explicitly sketch your before and after wavefunctions.
 
king vitamin said:
Right. Do you see how that affects your overlap integral? It might help to explicitly sketch your before and after wavefunctions.

So for a < x < 2a: the overlap is zero. While for 0 < x < a, the overlap is usual - so the limits are from 0 to a, and not from 0 to 2a.

[tex]\frac{1}{2} \frac{\sqrt 2}{a} \int_0^{a} cos (\frac{3\pi x}{2a}) - cos (\frac{\pi x}{2a}) dx[/tex]

[tex]= - \frac{8}{3\pi \sqrt 2}[/tex]

So the probability = ##\frac{32}{9\pi^2}##, which is less than 1, reassuringly.But for part (b), I haven't got a clue.
 
Do I need to use adiabatic approximation for part (b)?
 

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