Abstract
We exploit the SU(N) irreducible Schwinger boson to construct SU(N) coherent states. This construction of an SU(N) coherent state is analogous to the construction of the simplest Heisenberg–Weyl coherent states. The coherent states belonging to irreducible representations of SU(N) are labeled by the eigenvalues of (N − 1) SU(N) Casimir operators and characterized by (N − 1) complex orthonormal vectors describing the SU(N) group manifold.
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