See coherent state.

Bargmann-Segal transform is the integral transform whose kernel is the overlap between the projective measure corresponding to the coherent states and a measure corresponding to an orthonormal basis comeing from some polarization for $L^2$-sections. The kernel is a special case of a Bergman kernel? in complex analysis.

Classical case of Heisenberg group:

- V. Bargmann,
*On a Hilbert space of analytic functions and an associated integral transform*, Communications on Pure and Applied Mathematics**14**(1961) 187-214 MR0157250 doi

Vectors in the Hilbert space can be represented in the coherent state representation: $|f\rangle = \int |z\rangle\langle z|f\rangle d\mu$; if $f$ is in $L^2$ then $\langle z|f\rangle$ is a holomorphic function and this passage is called the Bargmann-Segal transform (referring to Irving Segal); this way certain Hilbert space of holomorphic function appears, the Bargmann-Fock space.

Further generalization is to Perelomov coherent states.

More recent generalized Segal-Bargmann transform of Hall:

Created on November 12, 2012 at 23:47:23. See the history of this page for a list of all contributions to it.