Core idea

For a complex HH, the group

U(H)={U∈B(H):U∗U=UU∗=I}U(H)=\{U\in B(H):U^*U=UU^*=I\}

of , equipped with the , is a real . Its Lie algebra is

u(H)={B∈B(H):B∗=−B},[B,C]=BC−CB,\mathfrak u(H)=\{B\in B(H):B^*=-B\}, \qquad [B,C]=BC-CB,

the real Banach space of bounded skew-adjoint operators. Here B∗B^* is the .

Local charts

The operator series exp⁡B=∑n≥0Bn/n!\exp B=\sum_{n\geq0}B^n/n! maps skew-adjoint operators to unitaries. Near II, its inverse is the norm-convergent logarithm

log⁡U=∑n≥1(−1)n+1n(U−I)n(∥U−I∥<1).\log U=\sum_{n\geq1}\frac{(-1)^{n+1}}n(U-I)^n \qquad(\|U-I\|<1).

This logarithm is skew-adjoint. Translating the local chart around the group gives its manifold structure; multiplication and inversion are smooth in these charts.

Why this is stronger than an orbit-map condition

For a smooth homomorphism π:G→U(H)\pi:G\to U(H) into this Banach–Lie group, differentiation produces bounded operators on all of HH. A only makes g↦π(g)vg\mapsto\pi(g)v continuous for each vv. Its derivatives can be unbounded and require the common . The exhibits the distinction explicitly.

References
  1. Jesús Espinoza and Bernardo Uribe, Topological properties of the unitary group, §1, p. 2, discussion before Theorem 1.2. The exponential and logarithm give the local construction used above.