Solving Ladder Operator Problem w/ 4 Terms

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Homework Help Overview

The problem involves calculating the expectation value of the fourth power of the momentum operator in the ground state of a harmonic oscillator, utilizing ladder operators. The original poster expresses uncertainty about handling terms with multiple ladder operators, as previous examples only included two terms.

Discussion Character

  • Exploratory, Assumption checking

Approaches and Questions Raised

  • Participants discuss the action of ladder operators on eigenstates and suggest applying these operators repeatedly to simplify the expression. Others propose using Schrödinger's equation and properties of hermitian operators to approach the problem differently.

Discussion Status

Participants are exploring various methods to tackle the problem, with some suggesting different approaches and others expressing progress in understanding. The original poster acknowledges a method that seems to align with their expectations, indicating a productive direction in the discussion.

Contextual Notes

The original poster is working within the constraints of a homework assignment, which may limit the methods they can use or the assumptions they can make about the problem.

Sheepattack
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Homework Statement



I have been given the following problem -
the expectation value of px4 in the ground state of a harmonic oscillator can be expressed as
<px4> = h4/4a4 {integral(-infin to +infin w0*(x) (AAA+A+ + AA+AA+ + A+AAA+) w0 dx}

I think I know how to proceed on other examples, but my given examples only have ladder operators with two terms, i.e. AA+ or A+A.
I can then use the commutation relation, AA+ - A+A =1 to remove them.

what has stuck me here is the four ladder operators in a term. I'm totally unsure on how to proceed!

any advice would be greatly appreciated!
 
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Do you know what A and A+ do to eigenstates? A+ψn = sqrt(n+1)ψn+1 and Aψn=sqrt(n)*ψn-1, so you can just keep applying the appropriate operator until you get down to a constant multiple of the eigenfunction.
 
I'd like to suggest a completely different method. Use two things here

1. Schrödinger's equation, which can be rearranged to form
[tex]p^2\psi = c (E-V)\psi[/tex] where c is some constant

2. The fact the p is hermitian

[tex] \left<p^4\right> = \left<\psi |p^4|\psi\right> = \left<p^2\psi|p^2\psi\right> = c^2 \left<(E-V)^2\right>[/tex]

The last part of the above integral can be greatly simplified using the evenness or oddness of the functions [tex]\psi[/tex] and V. Try it.
 
Many thanks for both your replies.

I think ideasrule's method was the one I am supposed to follow - managed to get the right answer! A few more clouds lifted...
thanks again
 

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