Quantum Physics - Electron in a 1d Potential Well Question

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SUMMARY

The discussion centers on a Quantum Physics problem involving an electron in a one-dimensional potential well, where the potential V = 0 for |x| ≤ a and V = ∞ otherwise. The energy eigenfunctions are defined as Un = a^(-1/2) cos (n∏x/2a) for odd n and Un = a^(-1/2) sin (n∏x/2a) for even n, with the lowest energy level E1 set at 37.6 eV. The participant successfully expressed the wavefunction as a linear combination of energy eigenfunctions, ψ = 2u1 + u2, and normalized it to ψ (norm) = ψ/√5. However, confusion arose regarding the second energy eigenvalue E2, which is determined to be 4 times E1, necessitating further clarification through the Schrödinger equation.

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  • Understanding of Quantum Mechanics principles, specifically potential wells.
  • Familiarity with energy eigenfunctions and their mathematical representation.
  • Knowledge of normalization of wavefunctions in quantum systems.
  • Basic comprehension of the Schrödinger equation and its application to quantum systems.
NEXT STEPS
  • Study the derivation of energy eigenvalues for the infinite square well potential.
  • Learn about the normalization process for quantum wavefunctions in detail.
  • Explore the application of the Schrödinger equation to find eigenvalues in quantum systems.
  • Review the relationship between wavefunctions and their corresponding energy measurements in quantum mechanics.
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Students and enthusiasts of Quantum Physics, particularly those studying potential wells and energy eigenvalues, as well as educators seeking to clarify concepts related to wavefunctions and measurements in quantum systems.

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Homework Statement



This is a Quantum Physics problem.

An electron moves in a one-dimensional potential well such that the potential V = 0 for |x| ≤ a, and V = ∞ otherwise.

The system has energy eigenfunctions:

Un = a^(-1/2) cos (n∏x/2a), for n odd, and
Un = a^(-1/2) sin (n∏x/2a) for n even.

(Those are both for |x| ≤ a)

and Un = 0 for |x| > a.

The lowest energy level of the system is 37.6 eV.

At t=0, the wavefunction for the system is

ψ(x, t = 0) = a^(-1/2) (2 cos (∏x/2a) + sin (∏x/a)).

(1) Write the wavefunction as a linear combination of energy eigenfunctions, and hence normalise the wavefunction.

(2) What are the possible results of a measurement of electron energy?


Homework Equations



Not really sure!

The Attempt at a Solution



Okay, so I think I have 1) complete. The wavefunction as a linear combination of energy eigenfunctions is ψ = 2u1 + u2.

Also, I normalised it and got ψ (norm) = ψ/√5. I'm pretty sure I understand all this.

My problem is with (2). I know that the possible results of an energy measurement are either u1 or u2.

And u1 = E1 = 37.6 eV (given in question)
But I don't understand how to get E2. Apparently E2 = 4 (E1)?? Why would that be true.. I don't understand where that 4 came from? :/

Sorry, I'm an absolute beginner to Quantum Physics so I'm going very very slowly!

Any help would be appreciated :)
 
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But I don't understand how to get E2. Apparently E2 = 4 (E1)?? Why would that be true.. I don't understand where that 4 came from? :/
... you should have this already in your notes when you covered the infinite square well in general. If not, then you'll have to put U2 through the Schrödinger equation to find the eigenvalue. (H-E2)U2=0.

I know that the possible results of an energy measurement are either u1 or u2.
And u1 = E1 = 37.6 eV
The possible outcomes of a measurement are the eigenvalues, not the wavefunctions. Important not to mix them up. It is never correct to write "u1=E1" for example.
 

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