Infinite square well eigen-energies

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Homework Help Overview

The discussion revolves around the infinite square well problem in quantum mechanics, specifically examining the eigen-energies and eigen-functions when the well is centered at the origin with walls at -L and +L, compared to a well defined from 0 to 2L.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore whether the eigen-spectrum remains unchanged when the well is centered at the origin, questioning the form of the wave functions and discussing the implications of boundary conditions.

Discussion Status

Some participants have offered insights regarding the differential equation and boundary conditions, suggesting that the wave functions can be expressed as combinations of sine and cosine functions. There is an acknowledgment of the need to set up the Schrödinger equation correctly under the new conditions.

Contextual Notes

There are mentions of potential confusion regarding the length of the well and the implications of changing boundary conditions on the eigen-functions and eigen-energies.

Pacopag
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Homework Statement


Usually when we solve the problem of the infinite square well we place one wall at the origin and the other one at, say 2L (please notice the 2).
We get the eigen-energies
[tex]E_n = {{n^2 \pi^2 \hbar^2}\over{8ma^2}}[/tex]
and the eigen-functions
[tex]\psi_n = \sqrt{1\over a}\sin{\left({n\pi\over{2a}}x\right)}[/tex].
My question is this: If instead we placed the well centered about the origin such that the walls are at -L and +L, do we get the same spectrum, and the wave functions shifted left by L, i.e.
[tex]\psi_n = \sqrt{1\over a}\sin{\left({n\pi\over{2a}}(x+L)\right)}[/tex].
?


Homework Equations





The Attempt at a Solution


Thing is, when I do it from scratch, I don't get these wavefunctions. I get a combination of sin and cos.
 
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I take it that [tex]a[/tex] should really be [tex]L[/tex]. Your wave function is correct, since it satisfies the proper differential equation, namely [tex]-\frac{\hbar^2}{2m}\psi''(x) = E \psi(x)[/tex] and initial conditions [tex]\psi(-L) = \psi(L) = 0[/tex]. Note that in general a sum of sin and cos can be written as a sin (or cos) with a phase shift. If you combined your combination of sin and cos you should get the desired wave function.
 
Pacopag said:
My question is this: If instead we placed the well centered about the origin such that the walls are at -L and +L, do we get the same spectrum, and the wave functions shifted left by L, i.e.
[tex]\psi_n = \sqrt{1\over a}\sin{\left({n\pi\over{2a}}(x+L)\right)}[/tex].
?

The Attempt at a Solution


Thing is, when I do it from scratch, I don't get these wavefunctions. I get a combination of sin and cos.

Set up the Schrödinger equation and apply the new boundary conditions and see. You should get the same General solution since you are not changing the length of the well. If you are increasing the length "L" you will see a change in the spectrum. Also, the functions are combinations of sine and cosines (alternately even and odd wrt the center). Hint: Either the Sine term or cosine term disappears in each state...Can you solve it now?
 
Last edited:
Ok. It makes sense now. Thank you for your replies.
 

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