On periodic solutions and attractors for the Maxwell--Bloch equations
Alexander Komech
TL;DR
The paper proves the existence of time-periodic solutions with a $T$-periodic Maxwell field for the Maxwell–Bloch equations, modeled as a finite-dimensional approximation of semiclassical Maxwell–Schrödinger dynamics, under periodic pumping and for any $N\ge 1$ two-level molecules. It exploits the $U(1)$ gauge symmetry to reduce the system to the Hopf fibration, yielding a reduced dynamical system on $Y = R^2 \times S^2$, and uses a Poincaré map together with Lefschetz fixed-point theory on a compactified phase space to construct $T$-periodic solutions. A priori bounds and dissipativity imply a compact global attractor, and the method extends from the one-molecule case to many molecules via the product gauge group $(U(1))^N$. The results provide a rigorous foundation for periodic laser-action regimes in MB-type models and establish a general/topological framework for periodic solutions in dissipative gauge-invariant systems.
Abstract
We consider the Maxwell-Bloch system which is a finite-dimensional approximation of the coupled nonlinear Maxwell-Schrödinger equations. The approximation consists of one-mode Maxwell field coupled to two-level molecule. We construct time-periodic solutions to the factordynamics which is due to the symmetry gauge group. For the corresponding solutions to the Maxwell--Bloch system, the Maxwell field, current and the population inversion are time-periodic, while the wave function acquires a unit factor in the period. The proofs rely on high-amplitude asymptotics of the Maxwell field and a suitable extension of the Lefschetz theorem on fixed points and the Euler characteristic for noncompact manifolds. We also prove the existence of the global compact attractor.
