Question about quantum harmonic oscilator

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.
 
Hello everyone, I’m considering a point charge q that oscillates harmonically about the origin along the z-axis, e.g. $$z_{q}(t)= A\sin(wt)$$ In a strongly simplified / quasi-instantaneous approximation I ignore retardation and take the electric field at the position ##r=(x,y,z)## simply to be the “Coulomb field at the charge’s instantaneous position”: $$E(r,t)=\frac{q}{4\pi\varepsilon_{0}}\frac{r-r_{q}(t)}{||r-r_{q}(t)||^{3}}$$ with $$r_{q}(t)=(0,0,z_{q}(t))$$ (I’m aware this isn’t...
Hi, I had an exam and I completely messed up a problem. Especially one part which was necessary for the rest of the problem. Basically, I have a wormhole metric: $$(ds)^2 = -(dt)^2 + (dr)^2 + (r^2 + b^2)( (d\theta)^2 + sin^2 \theta (d\phi)^2 )$$ Where ##b=1## with an orbit only in the equatorial plane. We also know from the question that the orbit must satisfy this relationship: $$\varepsilon = \frac{1}{2} (\frac{dr}{d\tau})^2 + V_{eff}(r)$$ Ultimately, I was tasked to find the initial...
Back
Top