Question about quantum harmonic oscilator

AI Thread Summary
The discussion revolves around solving the energy eigenvalue spectrum for two Hamiltonians related to a quantum harmonic oscillator. The first Hamiltonian, H = H0 + c, leads to eigenvalues of E + c, where E is the known energy of the harmonic oscillator. The second Hamiltonian was initially miswritten but corrected to H = H0 + λx, prompting a discussion on completing the square to rewrite the potential energy. This transformation allows the Hamiltonian to be expressed as a harmonic oscillator plus a constant, facilitating the solution. Concerns about whether the change of variable affects the kinetic energy term were addressed, concluding that it does not due to the linear relationship between the variables.
Miguel Paramo
Messages
7
Reaction score
0
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 + \lambdax^{2}

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.
 
Physics news on Phys.org
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)\hbar\omega

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 + \lambdax (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 + \lambdax (instead of the x being squared).

Thank you!

I think I liked it better with x^2!

Maybe try and complete the square for the two terms

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

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

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

So that the term reads

(1/2) mw^{2} y^{2} - (\lambda^{2} / 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 excercise.

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!
 
\frac{d}{dx} = \frac{dy}{dx} \frac{d}{dy} = \frac{d}{dy},

so, as you say, I don't think the kinetic energy term changes.
 
Thread 'Help with Time-Independent Perturbation Theory "Good" States Proof'
(Disclaimer: this is not a HW question. I am self-studying, and this felt like the type of question I've seen in this forum. If there is somewhere better for me to share this doubt, please let me know and I'll transfer it right away.) I am currently reviewing Chapter 7 of Introduction to QM by Griffiths. I have been stuck for an hour or so trying to understand the last paragraph of this proof (pls check the attached file). It claims that we can express Ψ_{γ}(0) as a linear combination of...
Back
Top