Introduction to quantum field theory
Problem 1
- A particle is moving under the influence of a 3 dimensional potential [math]\displaystyle{ V(x,y,z)=\frac{m \omega^2}{2}(x^2 + y^2 + z^2) }[/math]. Calculate the possible energy levels of the particle and discuss their degeneracies.
- The potential is then modified to [math]\displaystyle{ V^{\prime}(x,y,z)=\frac{m \omega^2}{2}(x^2 + \alpha x + y^2 + z^2) }[/math], where [math]\displaystyle{ \alpha }[/math] is a small parameter. By solving the Schrödinger equation exactly, compute what effect, if any, this has on the energy levels.
- Solve the same problem (i.e. find the change in energy levels) by treating the additional contribution to the potential [math]\displaystyle{ \alpha x }[/math] as a perturbation to the original potential [math]\displaystyle{ V(x,y,z) }[/math] up to the 2nd order in [math]\displaystyle{ \alpha }[/math]. Comment on the difference(s), if any, between results obtained here and in 1.2 above. What is the range of validity of perturbation theory?
Problem 2
We solved in class the Schrödinger equation for the spectrum of the hydrogen atom as if it were isolated in the Universe. In reality, H is in an environment, which means that the Coulomb potential does not extend to infinity, but gets screened by other charges. Using first-order perturbation theory, explore the simple case of a screened Coulomb potential cut-off at a constant distance R: [math]\displaystyle{ V(r)={-\kappa\over r}\theta(R-r) }[/math], with [math]\displaystyle{ \kappa }[/math] the square of the electron charge (in Gaussian units) and [math]\displaystyle{ \theta }[/math] the Heaviside step function.
- How would you characterize the strength of the perturbation and under which conditions does perturbation theory give reliable results?
- How does the cutoff affect the spectrum? Does it lift degeneracies? Give specific answers for three values of [math]\displaystyle{ R }[/math], one for gases under standard conditions, one for liquids and one for solids (and explain how you estimate those values). Is the approximation reliable in all three cases?
- Give detailed results for the energies and the wave functions in the [math]\displaystyle{ 1s }[/math] and [math]\displaystyle{ 2s }[/math] cases.
Problem 3
Two spin-½ particles of masses [math]\displaystyle{ m_1 }[/math] and [math]\displaystyle{ m_2 }[/math] interact via a potential that may be expressed as:
[math]\displaystyle{ V = \dfrac{-e^2}{r}\left(1 + \dfrac{b}{r}\sigma^{(1)}\cdot \sigma^{(2)} \right), }[/math]
where [math]\displaystyle{ \sigma^{(i)} }[/math] corresponds to the [math]\displaystyle{ i }[/math]-th particle; [math]\displaystyle{ r = \lvert \vec{r}_{1} - \vec{r}_2 \rvert }[/math] represents the magnitude of relative separation between the two particles; and [math]\displaystyle{ b }[/math] is an arbitrary constant. Determine the bound-state energy spectrum of the combined two-particle system. What condition(s) do you need to impose upon [math]\displaystyle{ b }[/math] to avoid unphysical eigenstates?