Studying 1D Particle in Potential V=-Fx: Energy Spectrum & Wavefunctions

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Homework Help Overview

The discussion revolves around a quantum mechanics problem involving a one-dimensional particle subjected to a linear potential, specifically V = -Fx, where F is a constant. Participants are tasked with finding the energy spectrum and wavefunctions of the system, while noting the absence of boundary conditions.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to solve for the momentum space wave function and expresses confusion regarding the lack of boundary conditions affecting the energy spectrum. Some participants question the implications of the linear potential and its relation to the concept of a free particle.

Discussion Status

Participants are exploring the implications of the potential on the energy levels and wavefunctions. There is recognition that the absence of boundary conditions leads to unrestricted energy levels, akin to a free particle scenario. Some guidance has been offered regarding the relationship between momentum-space and position-space wave functions, as well as references to Airy functions.

Contextual Notes

Participants note the potential's linear nature and its implications for the particle's behavior, comparing it to classical scenarios such as a particle moving against a gravitational potential. There is an ongoing discussion about the nature of the potential and its effects on quantization.

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Homework Statement


This is from an old exam I'm studying from. It goes:

"A particle of mass m is traveling in one dimension under the influence of a potential

V = -Fx

where F is a known constant. Find the energy spectrum and wavefunctions.

Hint: You may want to work in momentum space, but do not have to."

Homework Equations



Schrödinger eqn, other fundamental quantum relations


The Attempt at a Solution



I solved for the momentum space wave function and got an exponential solution ~ exp[(i/hF)(p^3-E*p)], I think, or something much like that. But how can I find an energy spectrum when I don't seem to have any boundary conditions? It does not say anything about, say, an infinite potential for x < 0 or anything.

I also tried using

d<p>/dt= <-dV/dx>

but that didn't seem to help.

It seems like the energy could be anything. Could that be all I need to say? And what about the wave functions?

It just seems like a weird problem. I'm wondering if there could have been a typo or something obvious I'm missing. I can post more of my work if it will help.
 
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You got it. No boundary conditions means no restriction on the allowed energies, similar to the case of a free particle.

The potential corresponds to a particle in a constant force field. Classically, the energy would just allow you to locate where the turning point was. Quantum mechanically, that's where the wave function should go from being oscillatory to decaying. I haven't worked it out, but I'd expect that changing E just shifts the wave function left or right.

Since you have the momentum-space wave function, you can Fourier transform it to obtain the position-space wave function.

You might want to look up Airy functions as well.
 
vela said:
You got it. No boundary conditions means no restriction on the allowed energies, similar to the case of a free particle.


If V = V(x) = F*x, this seems like a linear potential, not that of a free particle.

Is that not so? If so: a constant force (gradient of potential) would be on the particle, rather like the quantum picture of a particle ascending a hill against a gravitational potential. No?
 
bjnartowt said:
If V = V(x) = F*x, this seems like a linear potential, not that of a free particle.

Is that not so? If so: a constant force (gradient of potential) would be on the particle, rather like the quantum picture of a particle ascending a hill against a gravitational potential. No?
Yes, you're right. They're different potentials. My point was that you don't get quantized energy levels with V=-Fx because the particle is unbounded, just like you don't get quantized energy levels with V=0 because again the particle is unbounded. The potential in both cases does not confine the particle to a finite region of space.
 
Oh, I see. You said "SIMILAR" to a free particle. Sorry about that: details are not my strong suit.
 

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