Let $M$ be a compact real-analytic manifold, equipped with a real-analytic
Riemannian metric $g,$ and let $\beta$ be a closed real-analytic 2-form on $M$,
interpreted as a magnetic field. Consider the Hamiltonian flow on $T^*M$ that
describes a charged particle moving in the magnetic field $\beta$. Following an
idea of T.
We consider a particle moving on a 2-sphere in the presence of a constant
magnetic field. Building on earlier work in the nonmagnetic case, we construct
coherent states for this system. The coherent states are labeled by points in
the associated phase space, the (co)tangent bundle of S^2. They are constructed
as eigenvectors for certain annihilation operators and expressed in terms of a
certain heat kernel. These coherent states are not of Perelomov type, but
rather are constructed according to the "complexifier" approach of T.
Let G be a connected complex semisimple group, assumed to have trivial
center, and let K be a maximal compact subgroup of G. Then G/K, with a fixed
G-invariant Riemannian metric, is a Riemannian symmetric space of the complex
type. Now let Gamma be a discrete subgroup of G that acts freely and
cocompactly on G/K. We consider the Segal--Bargmann transform, defined in terms
of the heat equation, on the compact quotient Gamma\G/K. We obtain isometry and
inversion formulas precisely parallel to the results we obtained previously for
globally symmetric spaces of the complex type.
We consider the weighted Bergman spaces HL^2(B^d,\mu_{\lambda}), where
d\mu_\lambda(z)=c_{\lambda}(1-|z|^2)^lambda d\tau, \tau being the hyperbolic
volume measure. These spaces are nonzero if and only if \lambda>d. For
0<\lambda\leq d, spaces with the same formula for the reproducing kernel can be
defined using a Sobolev-type norm. We define Toeplitz operators on these
generalized Bergman spaces and investigate their properties.