Question about quantum harmonic oscilator

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Homework Help Overview

The discussion revolves around finding the energy eigenvalue spectrum for Hamiltonians related to a quantum harmonic oscillator. The original poster presents two Hamiltonians: one with a constant term and another with a linear term in position, seeking assistance without using perturbation theory.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the implications of modifying the Hamiltonian by adding constants and linear terms. Questions arise regarding the effect of variable substitution on the kinetic energy term and the overall structure of the Hamiltonian.

Discussion Status

Some participants have provided insights into the first Hamiltonian and are working through the implications of the second Hamiltonian. There is an ongoing exploration of variable transformations and their effects on the Hamiltonian's terms.

Contextual Notes

The original poster has clarified a mistake in the problem statement regarding the form of the Hamiltonian, indicating a need to reassess the approach based on this correction.

Miguel Paramo
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Hi, I am preparing for a quantum mechanics exam, and I have this problem that I can`t solve:

I have to find the complete energy eigenvalue spectrum of a hamiltonean of the form:

H = H0 + c

and also another of the form

H = H0 + [tex]\lambda[/tex]x[tex]^{2}[/tex]

Where in both cases, H0 is the hamiltonean of an harmonic oscilator, c and lambda are constants. The variable is x.

I have to find the exact eigenvalues, cannot use perturbation theory, but I can use the fact that I already know the eigenvalues for the harmonic oscilator.

Can anybody help?

Thant you.
 
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Miguel Paramo said:
H = H0 + c

Let's do this one first. After we get this, we'll do the second one. Might have to take a supper break in the middle

Suppose |psi> is such that

H0 |psi> = E |psi>.

What does H |psi> equal?
 
Thak you.

Well, I think that H|Psi> = (Ho+C)|Psi> = (E+C)|Psi>

The the eignevalues are just E+C, where E is the harmonic oscilator energy:

E = (n+1/2)[tex]\hbar[/tex][tex]\omega[/tex]

If it is just that it was so easy, but the second part looks more complicated.

I made a mistake when I copy the problems, the hamiltonean should read:

H = H0 + [tex]\lambda[/tex]x (instead of the x being squared).

Thank you!
 
Miguel Paramo said:
I made a mistake when I copy the problems, the hamiltonean should read:

H = H0 + [tex]\lambda[/tex]x (instead of the x being squared).

Thank you!

I think I liked it better with [itex]x^2[/itex]!

Maybe try and complete the square for the two terms

[tex]\frac{1}{2}m \omega^2 x^2 + \lambda x[/itex].[/tex]
 
OK, I completed squares so the potencial energy part of the hamiltoneal reads:

(1/2) mw[tex]^{2}[/tex] [ x + ([tex]\lambda[/tex]/ (m w[tex]^{2}[/tex])) ][tex]^{2}[/tex] - ([tex]\lambda[/tex][tex]^{2}[/tex] / 2m).

I think that I should now define y as y= x + ([tex]\lambda[/tex]/ (m w[tex]^{2}[/tex]))

So that the term reads

(1/2) mw[tex]^{2}[/tex] y[tex]^{2}[/tex] - ([tex]\lambda[/tex][tex]^{2}[/tex] / 2m)

So, as a function of y, the hamiltonean is again an harmonic oscilator plus a constant, and I can solve it as the previous exercise.

My doubt is if the change of variable may alter the kinetic energy part of the hamiltonean, which depends on the second derivative of x. My guess is that not because the relation between x and y is linear.

Thank you for you help!
 
[tex]\frac{d}{dx} = \frac{dy}{dx} \frac{d}{dy} = \frac{d}{dy},[/tex]

so, as you say, I don't think the kinetic energy term changes.
 

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