What is the Time Evolution of a Particle in a Harmonic Potential Energy Well?

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Homework Help Overview

The discussion revolves around the time evolution of a particle in a harmonic potential energy well, specifically focusing on the wave function and probability density associated with the system. The original poster presents an initial wave function involving energy eigenfunctions of the harmonic oscillator and poses questions regarding its time evolution and probability density function.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the expression for the wave function at time t and the calculation of the probability density function. There are attempts to derive the probability density and clarify the definition of the probability density function.

Discussion Status

Some participants have provided guidance on the mathematical expressions involved, while others are questioning the correctness of their calculations. There is an ongoing exploration of the relationship between the wave function and its conjugate, as well as the implications for the probability density.

Contextual Notes

Participants are working under the constraints of the problem as posed, including the requirement to express results in terms of specific variables and functions. There is a focus on ensuring that the probability density function is symmetric and correctly calculated.

cleggy
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1. A particle in a harmonic potential energy well is in a state described by the initial wave function

Ψ(x, 0) = (1/√2) (ψ1(x)+ iψ3(x))

where ψ1(x)and ψ3(x) are real normalized energy eigenfunctions of the harmonic oscillator with quantum numbers n =1 and n = 3 respectively.

(a)
Write down an expression for Ψ(x, t) that is valid for all t> 0. Express your answer in terms of ψ1(x), ψ3(x)and ω0, the classical angular frequency of the oscillator.

(b)
Find an expression for the probability density function at any time t> 0. Express your answer in terms of ψ1(x), ψ3(x), ω0 and t.Use the symmetry of this function to show that the expectation value,<x> = 0 at all times.

Homework Equations





The Attempt at a Solution




I have reached Ψ(x, t) = (1/√2) (ψ1(x)exp(-3iw_{}0t/2+ iψ3(x)exp(-7iw_{}0t/2)


for part (b) I'm not sure how to calculate the probability density function at any time t>0 ?

I know that the probability density needs to be even function of x and so therefore being symmetrical about the centre of the well at all times.

Then using the sandwich integral to calculate <x>, it will yield zero as the integrand is an odd function.
 
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What is the definition of the probability density function?
 
it's just the |Ψ|^2 is it not? I don't know how to do the math
 
That's correct, do you now that \psi^* \psi=|\psi|^2, with \psi^* the conjugated wave function?
 
so the conjugate of Ψ(x, t) is (1/√2)(ψ1(x)exp(+3iwt/2) + iψ3(x)exp(7iwt/2)) ?
 
The exponentials disappear and then |Ψ|^2 = (1/2)(ψ1(x) - ψ3(x)).

Am I on the right tracks here?
 
That doesn't look correct to me. Write out the whole expression and show your steps, start with showing what you got for\psi^*.
 
i get \Psi\ast=(1/√2)(ψ1(x)exp(+3iwt/2) + iψ3(x)exp(7iwt/2)) for
 
That is not correct. Note that there is an i in front of \psi_3.
 
  • #10
\Psi\ast=(1/√2)(ψ1(x)exp(+3iwt/2) - iψ3(x)exp(7iwt/2))
 
  • #11
Looking good. Now multiply and be careful when working out the brackets.
 
  • #12
Right so I should have

|\Psi|^2 = 1/2 |\psi1|^2 + |\psi3|^2

+ 2\psi1\psi3sin(2wot)
 
  • #13
Almost correct, don't forget that the entire expression is multiplied by 1/2 not just the first term.

Now write down the expression for <x>.
 
  • #14
that should have been

|\Psi|^2 = [1/2][|\psi1|^2 + |\psi3|^2

+ 2\psi1\psi3sin(2wot)]
 

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