We study, both classically and quantum mechanically, the problem of a neutr
al particle with a spin angular momentum S, mass m, and magnetic moment mu,
moving in one dimension in an inhomogeneous magnetic field given by B=B-0(
z) over cap+ B-perpendicular to'x (y) over cap. This problem serves for us
as a toy model to study the trapping of neutral particles. We identify K =
root[S-2(B-perpendicular to')(2)/mu mB(0)(3]), which is the ratio between t
he precessional frequency of the particle and its vibrational Frequency, as
the relevant parameter of the problem. Classically, we find that when mu i
s antiparallel to B, the particle is trapped provided that K<0.5. We also E
nd that viscous friction, be it translational or precessional, destabilizes
the system. Quantum mechanically, we study the problem of a spin S=h/2 par
ticle in the same field. Treating K as a small parameter for the perturbati
on from the adiabactic Hamiltonian, we find that the lifetime T-esc of the
particle in its trapped ground state is T-esc =(T-vib/2 pi) x(1/root 8 pi K
)exp(2/K), where T-vib = 2 pi root mB(0)/mu(B-perpendicular to')(2) is the
classical period of the particle when placed in the adiabatic potential V =
mu/B/. (C) 2000 American Association of Physics Teachers.