(a) The Hamiltonian is

we can take Az = Ax = 0, Ax = Bx, i.e. A = Bx\(\hat y\), and write the Schrodinger equation as

(b) As \([\hat P_y, \hat H] = [\hat P_z, \hat H] =0\), Py and Pz are conserved. Choose H, Py, Pz as a complete set of mechanical variables and write the SchrGdinger equation as

The above shows that \(\hat H - \frac{\hat P_x^2}{2m}\) is the Hamiltonian of a one-dimensional harmonic oscillator of angular frequency w = \(\frac{eB}{mc}\). Hence the energy levels of the system are
E = (n + 1/2)h\(\omega\) + Pz2/2m, n = 0, 1, 2, . . .
Because the expression of E does not contain Py explicitly, the degeneracies of the energy levels are infinite.
(c) In the coordinate frame chosen, the energy eigenstates correspond to free motion in the z direction and circular motion in the x - y plane, i.e. a helical motion. In the z direction, the mechanical momentum mwz = Pz is conserved, describing a uniform linear motion. In the x direction there is a simple harmonic oscillation round the equilibrium point x = -cPy/eB. In the y direction, the mechanical momentum is mvy = Py + eBx/c = eB\(\xi\) /c = m\(\omega\xi\) and so there is a simple harmonic oscillation with the same amplitude and frequency.