QUANTUM MECHANICS 329cyclotronfrequency and theharmonic motion is centered at thepoint
which depends upon Theeigenvalues andeigenfunctions arewhere are the eigenfunctions for the one-dimensional harmonic oscil-
lator.
5.75 Electric and Magnetic Fields (Princeton)
a) Many vectorpotentialsA(r) can be chosen so that For
the present problem the most convenient choice is Thus the
Hamiltonian isThe abovechoice isconvenientsince only fails tocommutewithH,so
and are constants ofmotion. Bothpotentials have been made to depend
onb) Since and are constants ofmotion, we canwrite theeigenstates
and energies asThe lastequation determines theeigenvalue andeigenfunctions
The potential isa combination oflinear andquadratic terms in So the
motion behaves as asimpleharmonicoscillator,where the termslinear in
determine thecenter ofvibration. Aftersome algebra we canwrite the