A Lie group is a group which is a finite-dimensional smooth Hausdorff second-countable manifold, with smooth multiplication and inversion. For the special unitary group, consider the real vector space
The diagonal entries of a skew-Hermitian matrix supply real parameters, and the entries above the diagonal supply ; the trace-zero condition removes one real parameter. Thus .
The matrix facts used to construct charts are these: the matrix exponential is analytic, its derivative at zero is the identity, and it has an analytic inverse matrix logarithm on a sufficiently small neighborhood of the identity. On those neighborhoods , , and . For a unitary matrix in that neighborhood, the spectral theorem writes with principal angles close to zero, and is skew-Hermitian.
Choose a norm ball of radius small enough to lie in the exponential's inverse domain. If is unitary, and in operator norm, then
so its trace is zero. Conversely gives and . Thus the logarithm identifies an open neighborhood of in , with its matrix subspace topology, with the open ball . Choosing a real linear identification turns this into a chart.
For every take the translated chart
Their overlap maps are wherever both charts are defined, so they are real analytic. They cover the group; the matrix topology is Hausdorff and second-countable. This constructs the real manifold directly, rather than merely counting equations. Matrix multiplication is polynomial in real/imaginary entries and inversion here is ; in the logarithm charts both are smooth. The logarithm charts for the special unitary group therefore prove
For it is the one-point group of dimension zero.
For , let the first column be , of unit norm. Every unit vector orthogonal to it is a scalar of modulus one times . The determinant of the resulting matrix is that scalar, so determinant one fixes it to . Hence
is bijective, with inverse given by taking the first column. The forward map is real polynomial in the four coordinates; composing with the local logarithm charts verifies smoothness into the constructed manifold. The inverse is a smooth matrix-coordinate projection and, in the usual embedded sphere charts, is smooth into . Thus , the explicit realization of SU(2) as the three-sphere.