Quick QM Question Homework: Find Probability & Average Energy

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Homework Help Overview

The discussion revolves around quantum mechanics, specifically focusing on the time evolution of a wave function and the calculation of probabilities and average energy for a particle described by energy eigenfunctions.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the formulation of the wave function at a later time and the implications of expressing it as a linear combination of energy eigenfunctions. Questions arise regarding the calculation of probabilities associated with energy measurements and the interpretation of complex coefficients.

Discussion Status

Participants are actively engaging with the problem, clarifying the relationship between the wave function and energy eigenstates. Some guidance has been provided regarding the expression for the wave function and the interpretation of coefficients, but there is no explicit consensus on the interpretation of complex probabilities.

Contextual Notes

There is a mention of formatting issues with LaTeX, which may affect the clarity of mathematical expressions shared in the discussion.

iamalexalright
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Homework Statement


Given an initial ave function [tex]\Psi(x)[/tex] at t=0, and a complete set of energy eigenfunctions [tex]\varphi_{n}(x)[/tex] with corresponding eigenenergies E_n for a particle, and no other information, in therms of the given find:


a. Find the state of the particle at a later time

Solution: [tex]\Psi(x,t) = T(t)*\varphi_{n}(x) = e^{-iE_{n}t/\hbar}\varphi_{n}(x)[/tex]

b. what is the probability that a measurement of energy will yield a particular value E_n?
[tex]<E> = \sum_{n}C_{n}P(C_n)[/tex]
Where P is the probability but I don't know where to go from here.

c. Find an expression for the average energy of the particle in terms of the energy eigenvalues:
[tex]<E>=1/n \sum_{i=1}^{n}E_{n}[/tex]

All seems right besides b? Any hints on b?
 
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One important point you're missing is that [tex]\psi[/tex] can be any linear combination of the energy eigenfunctions [tex]\phi_n[/tex]. Try the problem armed with the knowledge that:

[tex] \Psi(x,t) = \Sigma_n \phi_n(x,t)[/tex]

I would be glad to answer any further questions, but this seemed to be the major stumbling block.
 
Last edited:
oh, duh...

a.
[tex]\Psi(x) = \sum b_{n}\varphi_{n}(x)[/tex]

which implies

[tex]\Psi(x,t) = \sum b_{n}e^{-iE_{n} t/ \hbar} \varphi_{n}[/tex]

Which means in part b the probability of yielding E_n is simply b_n, correct?

[tex]b_{n} = <\varphi_{n}|\Psi(x)>[/tex]
 
hrm, LaTeX is either messing up for me or I missed something in my formatting but hopefully you can see what I meant for Psi in my second post
 
Note that
[tex] b_{n} = <\varphi_{n}|\Psi(x)>[/tex]
Can be a complex number. Does a complex probably mean anything? Hint hint...
 

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