1. You can now attempt any problem from Gasiorowicz G3 chapter 11, p1857, or chapter 14, p2335(G2 chapter 16, p2778, or chapter 18, p3078). Alternatives are any problems in Liboff, chapters 12 or 13. Try any problems from these chapters for credit, discussing with me first if you are not sure which to do. 
2. Pertubation theory and matrix methods: On problem sheet #3 we discussed the energy level splittings in the (molecular) rotation problem caused when the moment of inertia I_{1} about the xaxis is almost equal to I_{2} about the yaxis, but is not equal to I_{3} about the zaxis. Revise this topic by writing short notes in your own words about the procedures used, and explore the separation into blockdiagonal submatrices, and the relationship to (degenerate) perturbation theory. See how far you can get in applying the same methods to the case when the angular momentum quantum number l = 3. 
3. Variational principle and the square well: A particle in one dimension
is bound in an infinite well a/2 < x < a/2, with a parabolic bottom (drawing
supplied). The total energy V'(x), can be written as a sum of two terms, V'(x) =
V(x) + v(x); here V(x) is the same well with a flat bottom, for which the Schroedinger
equation can be solved exactly, and v(x) = Cx^{2} can be treated as a
perturbation. (a) Give the expressions for the eigenenergies and normalized eigenfunction for V(x). (b) Calculate the lowest oddparity state in V'(x), the approximate eigenenergy, and the first three terms in the eigenfunction in terms of solutions to V(x).

This problem was set in the Track 2 Basic QM exam in January 2000. 
4. Variational principle and the SHO (this problem is also on set#4): Compare the accuracy of the variational principle with first order perturbation theory, in the case of a 1D simple harmonic oscillator with quartic anharmonicity (i.e. a perturbation of the form lx^{4}). Use the operator formalism, so that you do not need to work out integrals. How does your approach to this problem change if the restoring frequency of the SHO tends to zero. Is there an exact solution in this latter case, and can you derive it? (In case this problem sounds daunting, it is basically G3 problem 6 p186 (G2 problem 3, p277), coupled with G3 problem 11 p235 (G2, problem 11, p307.) 
5. a) Two neutrons are trapped in a spherical potential V(r) = 0 if r < R and V(r)
= + infinity if r > R. Ignoring the interactions between the neutrons,
find the ground state wave function of system (including the spin wave function).
b) Assume now that the neutrons interact with each other through the potential V_{i} = As_{1}. s_{2}, where s_{i} is the Pauli spin matrix for the ith neutron, and A is a constant. Treating V_{i} as a perturbation, find the approximate ground state energy. 
This problem was set in the Track 2 Basic QM exam in August 1995. 
6. Consider a two level system which obeys the Schroedinger equation: 1) Obtain expressions for the energy levels and normalized eigenstates of this Hamiltonian. 2) Assume now that W_{1} = W_{2} and that at t = 0 the system is intially in the state a = 1, b = 0. Find the time t it takes for the system to reach a (relative) maximum probability of being in the state a = 0, b = 1. (Note: the above Schroedinger equation is an approximation to the following physical situation: two atoms can bind an electron, one with energy W_{1} and the other with energy W_{2}. The electron initally on the left atom is represented by a = 1, b = 0; on the right atom by a = 0, b = 1. If the atoms are close together, the electron can hop between the atoms.) 
This problem was set in the Track 2 Basic QM exam in August 1996. 
7. A system that has three unperturbed states can be represented by the
perturbed Hamiltonian matrix
, where F > E. The quantities a and b are to be regarded
as perturbations that are of the same order, and are small compared with FE.
(a) diagonalize the matrix to find the exact eigenvalues. 
This problem was set in the Track 1 QM exam in January 2000. 
8. The absorption spectrum of HCl gas is the subject of this problem. 1) (30%) Explain the meaning of the term absorption spectrum of a gas, and explain how such a spectrum can be measured in the laboratory. 2) (70%) In HCl gas, an number of absorption lines have been observed with the following wavenumbers (in cm^{1}): 83.03, 103.73, 124.30, 145.03, 165.51, and 185.86. Are these vibrational or rotational transitions? (You may assume that transitions involve quantum numbers that change by only one unit.) Explain your reasoning briefly. 2a) If the transitions are vibrational, estimate the spring constant (in dyne/cm). 2b) If the transitions are rotational, estimate the separation between the H and Cl nuclei. What J values do they correspond to, and what is the moment of inertia of HCl (in gmcm^{2})? 
This problem was set in the Track 2 Basic QM exam in January 1996. 
9. If the above questions do not give you enough choice, or too much challenge, feel free to do other problems from Gasiorowicz and/or Liboff. Some further Comps questions have been put onto a separate sheet, and you may submit any such questions as equivalent to single questions. 