A Lie group is a finite-dimensional smooth manifold with a group structure for which multiplication and inversion are smooth. The group defined here is the compact symplectic group , rather than the full complex symplectic group. Also, the displayed matrix expression requires to be ; the printed size is incompatible with .
Since , we have . The matrix exponential commutes with conjugation, as follows term by term from its absolutely convergent power series. Consequently
To construct logarithm charts for the compact symplectic group, consider the real vector space
Differentiating the defining identities at gives precisely these conditions. Conversely if , is unitary and
so . These are the infinitesimal conditions of the compact symplectic Lie algebra.
Near , the convergent matrix logarithm series is smooth and inverse to the matrix exponential near zero. These local inverses respect transpose, conjugate transpose, and conjugation; also when both matrices are sufficiently close to . Shrink their neighborhoods accordingly. If there, unitarity gives
The symplectic identity is equivalent to , so, putting , it gives , equivalently . Thus this local logarithm restricts to a bijection between a neighborhood of in and an open neighborhood of zero in . Its inverse is the restricted matrix exponential. These restrictions are manifold charts; left multiplication translates them to every via . The chart overlaps are smooth compositions of multiplication, exponential and logarithm. The subspace topology is Hausdorff and second countable, inherited from the finite-dimensional matrix space, so these charts give a smooth manifold.
Closure under products and inverses follows from and unitarity. Matrix multiplication is polynomial in real and imaginary entries, and inversion on the unitary group is , a real linear operation. Their restrictions are smooth in the charts just constructed. Hence is a Lie group without needing a closed-subgroup theorem.
Write in blocks. The two infinitesimal conditions give
The skew-Hermitian matrix has real parameters; the complex symmetric matrix has complex parameters, hence real parameters. Therefore
For , any two-by-two matrix satisfies , so the group is . Explicitly,
The rows are orthonormal and the determinant is one; conversely unitarity and determinant one force this form. This is the SU(2) as the three-sphere parametrization. The map and its inverse, extraction of the first row, are smooth. Thus is diffeomorphic to .

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