Perturbation of the simple harmonic oscillator

Click For Summary

Homework Help Overview

The discussion revolves around the perturbation of the simple harmonic oscillator by adding an additional potential term, specifically V0e-ax2, where V and a are constants. Participants are tasked with calculating the first-order correction of the ground state energy and exploring how this correction varies with changes in the parameter a.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the integral involved in calculating the first-order correction and express uncertainty about their attempts. There is a focus on the nature of the integral and the presence of the error function.

Discussion Status

Some participants have provided guidance on the integral, noting its standard nature and the relevance of boundary conditions. There is acknowledgment of the Gaussian integral's importance in physics, but no consensus has been reached on the correctness of the original attempts.

Contextual Notes

Participants mention the assumption that the parameter a is greater than zero and express concern over the inclusion of the error function in their calculations, indicating a potential gap in their understanding of the problem.

nowits
Messages
17
Reaction score
0
[SOLVED] Perturbation of the simple harmonic oscillator

Homework Statement


An additional term V0e-ax2 is added to the potential of the simple harmonic oscillator (V and a are constants, V is small, a>0). Calculate the first-order correction of the ground state. How does the correction change when a gets bigger?

Homework Equations


[tex]E_0^1=<\psi_0^0|H'|\psi_0^0>[/tex]

The Attempt at a Solution


[tex]\alpha=\frac{m\omega}{\hbar}, E_0^1=\int ^{\infty}_{-\infty} (\frac{\alpha}{\pi})^{1/4}e^{-\alpha x^2/2}V_0e^{-ax^2}(\frac{\alpha}{\pi})^{1/4}e^{-\alpha x^2/2}dx=(\frac{\alpha}{\pi})^{1/2}V_0\int ^{\infty}_{-\infty} e^{(-\alpha -a)x^2}dx[/tex]
So I suppose this is not what is wanted.
 
Physics news on Phys.org
nowits said:

Homework Statement


An additional term V0e-ax2 is added to the potential of the simple harmonic oscillator (V and a are constants, V is small, a>0). Calculate the first-order correction of the ground state. How does the correction change when a gets bigger?

Homework Equations


[tex]E_0^1=<\psi_0^0|H'|\psi_0^0>[/tex]

The Attempt at a Solution


[tex]\alpha=\frac{m\omega}{\hbar}, E_0^1=\int ^{\infty}_{-\infty} (\frac{\alpha}{\pi})^{1/4}e^{-\alpha x^2/2}V_0e^{-ax^2}(\frac{\alpha}{\pi})^{1/4}e^{-\alpha x^2/2}dx=(\frac{\alpha}{\pi})^{1/2}V_0\int ^{\infty}_{-\infty} e^{(-\alpha -a)x^2}dx[/tex]
So I suppose this is not what is wanted.

What makes you think this is not right?
Have you tried to compute the integral? It's a standard one.
 
nrqed said:
Have you tried to compute the integral? It's a standard one.
[tex]\int e^{-\xi x^2}=\frac{\sqrt{\pi}\ erf(\sqrt{\xi}x)}{2\sqrt{\xi}}\ \ \ ?[/tex]
I've never encountered an error function before in any homework problem, so I automatically assumed that I had done something wrong.
 
That's right, the indefinite integral contains an erf.
But you have more information: you know the boundary conditions and (you should have) [itex]\xi > 0[/itex]. Using
[tex]\lim_{x \to \pm \infty} \operatorname{erf}(x) = \pm 1[/tex]
you can calculate it, and in fact it is just a Gaussian integral,
[tex]\int_{-\infty}^\infty e^{-\xi x^2} dx = \sqrt{\frac{\pi}{\xi}}[/tex]
Remember this -- it's ubiquitous in physics (at least, every sort of physics that has to do with any sort of statistics, amongst which QM, thermal physics, QFT, SFT).
 
Last edited:
Ok.

Thank you both!
 

Similar threads

  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 3 ·
Replies
3
Views
3K
Replies
1
Views
2K
Replies
4
Views
3K
  • · Replies 16 ·
Replies
16
Views
3K
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 21 ·
Replies
21
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K