Quantum Harmonic Oscillator ladder operator

Click For Summary

Homework Help Overview

The discussion revolves around the application of ladder operators on the ground eigenfunction of a quantum harmonic oscillator, specifically examining the sequence of operators acting on the state and its implications for calculating the expectation value of momentum raised to the fourth power.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the effects of applying a sequence of ladder operators on the ground state, questioning whether the result is zero. They also discuss the calculation of the expectation value of \left\langle p^4_x \right\rangle and the contributions from different operator sequences.

Discussion Status

Some participants express uncertainty about their calculations and seek clarification on the contributions of various terms. There is a recognition of the multiplicative factors introduced by the operators, and one participant indicates they have arrived at the correct answer after additional consideration.

Contextual Notes

Participants reference specific forms of the eigenfunction and the implications of the operators on the state, indicating that the discussion is framed within the constraints of quantum mechanics and the properties of ladder operators.

bobred
Messages
170
Reaction score
0

Homework Statement


What is the effect of the sequence of ladder operators acting on the ground eigenfunction [itex]\psi_0[/itex]

Homework Equations


[itex]\hat{A}^\dagger\hat{A}\hat{A}\hat{A}^\dagger\psi_0[/itex]

The Attempt at a Solution


I'm not sure if I'm right but wouldn't this sequence of opperators on the ground state result in zero?
 
Physics news on Phys.org
Yeah.
 
Thanks, I thought so. This is part of a larger question concerning the expectation value of [itex]\left\langle p^4_x \right\rangle[/itex]. We are asked to show that

[itex]\left\langle p^4_x \right\rangle=\displaystyle\frac{ \hbar^4}{4 a^4}\left[ \displaystyle\int^\infty _{-\infty} \psi^*_0 \left(\hat{A}\hat{A}\hat{A}^\dagger\hat{A}^\dagger + \hat{A}\hat{A}^\dagger\hat{A}\hat{A}^\dagger + \hat{A}^\dagger\hat{A}\hat{A}\hat{A}^\dagger\right) \psi_0 dx \right]=\displaystyle\frac{3 \hbar^4}{4 a^4}[/itex]

Where [itex]\psi_0=\left( \displaystyle\frac{1}{\sqrt{\pi}a} \right)^\frac{1}{2}e^{-x^2/2a^2}[/itex]

This is not what I get. Due to [itex]\hat{A}^\dagger\hat{A}\hat{A}\hat{A}^\dagger\psi_0=0[/itex] I get [itex]\displaystyle\frac{2 \hbar^4}{4 a^4}[/itex] am I missing something?
Thanks
 
What are you getting for the other terms? It works out as it should for me. The first term should give you a 2 by itself.
 
As the first two sequences of operators preserve the ground eigenfunction and the last sequence zero, I get

[itex]\left\langle p^4_x \right\rangle=\displaystyle\frac{ \hbar^4}{4 a^4}\left[ 2 \displaystyle\int^\infty _{-\infty} \psi^*_0 \psi_0 dx \right]=\displaystyle\frac{2 \hbar^4}{4 a^4}[/itex]

Thanks
 
Remember that the raising and lowering operators don't simply change the state but introduce a multiplicative factor as well.
 
Right so I should be looking at [itex]\hat{A}\hat{A}^\dagger-\hat{A}^\dagger\hat{A}=1[/itex]?
 
Hi

Thanks for your help what I needed was [itex]\sqrt{n}\psi_{n-1}[/itex] and [itex]\sqrt{n+1}\psi_{n+1}[/itex]. I now get the correct answer.
 

Similar threads

  • · Replies 16 ·
Replies
16
Views
3K
  • · Replies 2 ·
Replies
2
Views
4K
Replies
4
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
Replies
1
Views
2K
Replies
4
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K