Complexification of a Real Lie Algebra
The complexification of a finite-dimensional real vector space V, as denoted by Vc, is the space of formal linear combinations v1+ iv2 , with v1, v2 ∈ V.
Let g be a finite-dimensional real Lie algebra and gc its complexification (as a real vector space). Then, the bracket operation on g has a unique extension to gc which makes gc into a complex Lie algebra. The complex Lie algebra gc is called the complexification of the real Lie algebra g.
Isomorphisms of Complex Lie Algebra
The Lie algebra gl(n;C), sl(n;C), so(n;C), and sp(n;C) are complex Lie algebras. In addition, there are also following isomorphisms of complex Lie algebras:
gl(n;R)c ≅ gl(n;C)
u(n)c ≅ gl(n;C)
su(n)c ≅ sl(n;C)
sl(n;R)c ≅ sl(n;C)
so(n)c ≅ so(n;C)
sp(n;R)c ≅ sp(n;C)
sp(n)c ≅ sp(n;C)
(u(n) is the space of all nxn complex skew-self-adjoint matrices. If X is any nxn complex matrix, then X = (X-X*)/2 + i(X+X*)/2i. Thus, X can be written as a skew matrix plus i times a skew matrix. Every X in gl(n;C) can be written uniquely as X1 + iX2, with X1 and X2 in u(n). It follows that u(n)c ≅ gl(n;C). If X has trace zero, then so do X1 and X2 , which has su(n)c ≅ sl(n;C))
Note that u(n)c ≅ gl(n;R)c ≅ gl(n;C). However, u(n)c is not isomorphic to gl(n;R), except when n = 1. The real algebra u(n) and gl(n;R) are called real forms of the complex Lie algebra gl(n;C).
In physics, we do not always clearly distinguish a matrix Lie algebra and its Lie algebra, or between a real Lie algebra and its complexification. For example, some references in the literature to SU(2) actually refer to the complexified Lie algebra sl(2;C).
Representation and Complexification
Let g be a real Lie algebra and gc its complexification. Then, every finite-dimensional complex representation π of g has a unique extension to a complex-linear representations of gc , also denoted as π and given by π(X+iY) = π(X) + iπ(Y) for all X, Y ∈ g. Furthermore, π is irreducible as a representation of gc if and only if it is irreducible as a representation of g.
If π is a complex representation of the real Lie algebra g, acting on the complex vector space V. Then, saying that π is irreducible means that there is no nontrivial invariant complex subspace W ⊂ V. Even though g is a real Lie algebra, when considering complex representations of g, we are interested only in complex invariant subspaces.
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