Infinite square well eigen-energies

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SUMMARY

The discussion centers on the eigen-energies and eigen-functions of the infinite square well, specifically when the well is centered at the origin with walls at -L and +L. The eigen-energies are given by E_n = {{n^2 \pi^2 \hbar^2}\over{8mL^2}} and the eigen-functions are expressed as ψ_n = √{1/a}sin{(nπ/(2a)(x+L))}. The participants confirm that the spectrum remains unchanged when the well's length is constant, and the wave functions can be represented as combinations of sine and cosine functions, satisfying the Schrödinger equation under the new boundary conditions.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly the infinite square well model.
  • Familiarity with Schrödinger equation and boundary conditions.
  • Knowledge of eigenvalues and eigenfunctions in quantum systems.
  • Basic trigonometric identities and their application in wave function representation.
NEXT STEPS
  • Study the derivation of eigen-energies for the infinite square well using different boundary conditions.
  • Explore the implications of changing the length of the well on the energy spectrum.
  • Learn about the mathematical techniques for combining sine and cosine functions to form wave functions.
  • Investigate the role of phase shifts in quantum wave functions and their physical interpretations.
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Students and educators in quantum mechanics, physicists analyzing potential wells, and anyone interested in the mathematical foundations of wave functions in quantum systems.

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
E_n = {{n^2 \pi^2 \hbar^2}\over{8ma^2}}
and the eigen-functions
\psi_n = \sqrt{1\over a}\sin{\left({n\pi\over{2a}}x\right)}.
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.
\psi_n = \sqrt{1\over a}\sin{\left({n\pi\over{2a}}(x+L)\right)}.
?


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 a should really be L. Your wave function is correct, since it satisfies the proper differential equation, namely -\frac{\hbar^2}{2m}\psi''(x) = E \psi(x) and initial conditions \psi(-L) = \psi(L) = 0. 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.
\psi_n = \sqrt{1\over a}\sin{\left({n\pi\over{2a}}(x+L)\right)}.
?

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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