J H Hannay 1998 J. Phys. A: Math. Gen. 31 L53 doi:10.1088/0305-4470/31/2/002
J H Hannay
Show affiliationsA continuous cyclic sequence of quantum states has an associated geometric, or Berry, phase
. For spin J, such a sequence is described by a cyclic change in the 2J+1 coefficients
of the basis states
. The Berry phase is analysed here for the general case - that is, the coefficients
are allowed to vary in an arbitrary cyclic manner. The result is expressed in geometric terms, specifically in the democratic representation due to Majorana. This uniquely characterizes the spin state
, up to overall phase, by the positions of 2J dots on the unit sphere of directions in real space. If the positions are denoted by unit vectors
, where
, each traces out a parametrized loop on the sphere, and the Berry phase is given by an integral of combinations of these vectors.
81Q70 Differential-geometric methods, including holonomy, Berry and Hannay phases, etc.
Issue 2 (16 January 1998)
Received 28 July 1997, in final form 26 September 1997
J H Hannay 1998 J. Phys. A: Math. Gen. 31 L53
R Beals et al 1999 Inverse Problems 15 L1
R Haydock et al 1972 J. Phys. C: Solid State Phys. 5 2845
R Haydock et al 1975 J. Phys. C: Solid State Phys. 8 2591
E Saeedi et al 2008 J. Micromech. Microeng. 18 075019
Benjamin C. Allanach et al JHEP03(2003)016
Neil Anderson et al 2006 J. Opt. A: Pure Appl. Opt. 8 S227
T. Preis et al 2008 EPL 82 68005
T. Preis et al 2006 Europhys. Lett. 75 510
Margaret C. Turnbull and Jill C. Tarter 2003 ApJS 149 423