Past exam of the mathematics course of the University of Cambridge 2014 iii Paper 2 2 Solution Created 2026-10-03 Updated 2026-10-06
The Weyl complete reducibility theorem states that every finite-dimensional Lie algebra representation of a finite-dimensional complex semisimple Lie algebra is a direct sum of Irreducible Lie algebra representations. Equivalently, every invariant vector subspace has an invariant complement.
We use the permitted Casimir operator properties in the following precise form. There is a central quadratic operator commuting with the action on every module; it is zero on the trivial Lie algebra representation, and on every nontrivial finite-dimensional Irreducible Lie algebra representation it is a nonzero scalar . This follows from the Schur lemma and the Casimir eigenvalue , using the Killing form normalization. We also use the permitted one-dimensional-representation fact: a complex semisimple Lie algebra has only trivial one-dimensional representations. Equivalently, it is a perfect Lie algebra, , so a character annihilating brackets must vanish. Neither fact assumes complete reducibility of the module being proved reducible.
First prove that every finite-dimensional short exact sequencewith trivial quotient splits. If is nontrivial irreducible, the Casimir operator has image in and restricts to there. Consequently is a one-dimensional invariant complement to . If is trivial irreducible, has a basis in which every action is . The Lie algebra representation identity makes , so the one-dimensional-representation fact gives and again the sequence splits.
For general , induct on . Choose an irreducible submodule . The induced sequence with kernel and middle term splits by induction. The inverse image of its invariant complement is a submodule fitting into . The irreducible-kernel case gives an invariant line in mapping isomorphically to the quotient. It is also an invariant complement to in . The case starts this induction. This proves splitting of a trivial quotient for a semisimple Lie algebra, including kernels that are not assumed completely reducible.
Now let be any invariant subspace. On the Hom representation the action isLet consist of the maps whose restriction to is a scalar multiple of . This is a submodule, and restriction givesThe right-hand map is surjective because an ordinary linear projection exists; its quotient action is trivial because a commutator with is zero. The splitting just proved supplies an invariant with . Thus intertwines the actions, , andThe cases and are immediate. Choosing an irreducible submodule and repeating this complement construction proves the Weyl complete reducibility theorem. This last step is invariant complement from an equivariant projection.
Dropping finite dimensionality gives an example with the complex simple Lie algebra . Its Verma module of highest weight zero has a basis withwhere . These actions obey , , . The span of is a proper submodule and the quotient is trivial. It has no invariant complement: such a complement would be a trivial line, while is injective on the entire module. Thus a simple Lie algebra can have an infinite-dimensional representation that is not completely reducible, even over .