What Defines the Energy Spectrum in a Hamiltonian System?

degerativpart
Messages
4
Reaction score
0

Homework Statement


Find the energy spectrum of a system whose Hamiltonian is
H=Ho+H'=[-(planks const)^2/2m][d^2/dx^2]+.5m(omega)^2x^2+ax^3+bx^4


I gues my big question to begin is what exactly makes up the energy spectrum. I know the equation to the first and second order perturbations but I am not sure exactly what the energy spectrum entails. Please help.

Homework Equations





The Attempt at a Solution


ive figured out that H'=ax^3+bx^4

and Ho==[-(planks const)^2/2m][d^2/dx^2]+.5m(omega)^2x^2
and lambda=1 which mean ita a full perturbation
 
Physics news on Phys.org
degerativpart said:
I gues my big question to begin is what exactly makes up the energy spectrum.
In QM, "energy spectrum" is just a stupid word that they use to mean the set of possible energy eigenvalues. I personally hate that terminology; it's so misleading.



degerativpart said:
and lambda=1 which mean ita a full perturbation
I don't know what this means.
 
haha obviously I agree with you and I read that the lambda in the equation for H=Ho+(lambda)H' when equals to zero means its an unperturbed equation and when it is equal to 1 then its fully perturbed. I don't know I read it.
But I guess my next question how many energy eigenvalues are there? Does that mean I should probably only go to the second oreder corrections?
 
degerativpart said:
... how many energy eigenvalues are there?
How many eigenvalues are there for H0? Can the perturbation remove or add any, or does it just shift them?
 
Sorry, I could say that book is the question?. thank you.
 
##|\Psi|^2=\frac{1}{\sqrt{\pi b^2}}\exp(\frac{-(x-x_0)^2}{b^2}).## ##\braket{x}=\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dx\,x\exp(-\frac{(x-x_0)^2}{b^2}).## ##y=x-x_0 \quad x=y+x_0 \quad dy=dx.## The boundaries remain infinite, I believe. ##\frac{1}{\sqrt{\pi b^2}}\int_{-\infty}^{\infty}dy(y+x_0)\exp(\frac{-y^2}{b^2}).## ##\frac{2}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,y\exp(\frac{-y^2}{b^2})+\frac{2x_0}{\sqrt{\pi b^2}}\int_0^{\infty}dy\,\exp(-\frac{y^2}{b^2}).## I then resolved the two...
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