Magnetic trapping of neutral particles: Classical and quantum-mechanical study of a Ioffe-Pritchard type trap

Citation
S. Gov et al., Magnetic trapping of neutral particles: Classical and quantum-mechanical study of a Ioffe-Pritchard type trap, J APPL PHYS, 87(8), 2000, pp. 3989-3998
Citations number
30
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
JOURNAL OF APPLIED PHYSICS
ISSN journal
00218979 → ACNP
Volume
87
Issue
8
Year of publication
2000
Pages
3989 - 3998
Database
ISI
SICI code
0021-8979(20000415)87:8<3989:MTONPC>2.0.ZU;2-9
Abstract
Recently, we developed a method for calculating the lifetime of a particle inside a magnetic trap with respect to spin flips, as a first step in our e fforts to understand the quantum mechanics of magnetic traps. The one-dimen sional toy model that was used in this study was physically unrealistic bec ause the magnetic field was not curl free. Here, we study, both classically and quantum mechanically, the problem of a neutral particle with spin S, m ass m, and magnetic moment mu, moving in three dimensions in an inhomogeneo us magnetic field corresponding to traps of the Ioffe-Pritchard "clover-lea f" and "baseball" type. Defining by omega(p), omega(z), and omega(r) the pr ecessional, the axial, and the lateral vibrational frequencies, respectivel y, of the particle in the adiabatic potential V-eff =mu\B\, we find classic ally the region in the (omega(r)/omega(p))-(omega(z)/omega(p)) plane where the particle is trapped. Quantum mechanically, we study the problem of a sp in-one particle in the same field. Treating omega(r)/omega(p) and omega(z)/ omega(p) as small parameters for the perturbation from the adiabatic Hamilt onian, we derive a closed-form expression for the transition rate 1/T-esc o f the particle from its trapped ground state. In the extreme cases, the exp ression for 1/T-esc reduces to 4 pi omega(r) exp(-2 omega(p)/omega(r)) for omega(p)much greater than omega(r)much greater than omega(z), to 8 root 2 p i root omega(p)omega(i)exp(-2 omega(p)/omega(i)) for omega(p)much greater t han omega(r)=omega(z)equivalent to omega(i) and to root pi/2 omega(r)(omega (z)/omega(p))(3/2)exp(-2 omega(p)/omega(z)) for omega(p)much greater than o mega(z)much greater than omega(r). (C) 2000 American Institute of Physics. [S0021-8979(00)10005-2].