Abstract
We show that some lasers and nonlinear optical devices with dissipation have in common certain characteristics that lead to a kind of phase anholonomy when such dissipative systems undergo a periodic motion with some frequency, say. The amount of the phase anholonomy accumulated in a period of 2/ is defined generally for such systems and further calculated for a subclass of such systems near the Hopf-bifurcation point. It turns out that the phase accumulation is generally determined by the size of the periodic orbit. By constructing a simple Hamiltonian, we show precisely that the phase anholonomy in these dissipative sytems can indeed be interpreted as Berrys phase.
Original language | English (US) |
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Pages (from-to) | 6410-6413 |
Number of pages | 4 |
Journal | Physical Review A |
Volume | 43 |
Issue number | 11 |
DOIs | |
State | Published - Jan 1 1991 |
Externally published | Yes |
ASJC Scopus subject areas
- Atomic and Molecular Physics, and Optics