How Can Quantum Mechanics Constants Be Deduced from Average Energy?

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Homework Help Overview

The discussion revolves around deducing constants related to a normalized wave function in quantum mechanics, specifically in the context of a particle in a one-dimensional potential well. The average energy of the system is provided, prompting inquiries about the implications for the constants involved.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between the average energy and the constants in the wave function. Questions arise regarding the eigenenergies of the states involved and whether the wave function represents a linear combination of these states.

Discussion Status

The discussion is active, with participants providing insights into the nature of the wave function and the requirements for normalization. Some guidance has been offered regarding the relationship between coefficients and eigenenergies, though multiple interpretations of the problem are still being explored.

Contextual Notes

Participants note the constraints of the potential well and the normalization condition for the wave function, which requires the sum of the squares of the coefficients to equal one.

greisen
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Hey,

I have a normalized wave function

PSI = c_1 psi_1(x) + c_2 psi_1(x)

where c_1 and c_2 are constants with the eigenfunctions equal to ground and first excited state. The average energy of the system is pi^2hbar^2/(ma^2) - what can one deduce about the constant and how?

Thanks in advance
 
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greisen said:
Hey,

I have a normalized wave function

PSI = c_1 psi_1(x) + c_2 psi_1(x)

where c_1 and c_2 are constants with the eigenfunctions equal to ground and first excited state. The average energy of the system is pi^2hbar^2/(ma^2) - what can one deduce about the constant and how?

Thanks in advance

I'm thinking energy expectation value, similar to your problem on creation/anihiliation. What are the eigenenergies of the two states?
 
The particle is in a one dimensional well with V(x) = 0 for o <= x <= a and otherwise it is infinity. Is it a linear combination between the two states ?

Again thanks very much
 
greisen said:
The particle is in a one dimensional well with V(x) = 0 for o <= x <= a and otherwise it is infinity. Is it a linear combination between the two states ?

Again thanks very much
Yes it is a linear combination of states. With orthonormal basis functions and normalized PSI the sum of the squares of the coefficients has to be 1. The products of coefficients times eigenenergies has to be the total energy
 

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