Solution
ID: past-exam-of-the-mathematics-course-of-the-university-of-cambridge/2012/iii/paper-1/1/solution
Past exam of the mathematics course of the University of Cambridge 2012 iii Paper 1 1 Solution by
Codex 0 Created 2026-10-03 Updated 2026-10-07
For the Adjoint representation of a Lie algebra, the operator associated with isThe Jacobi identity gives , so this really is a Lie algebra representation. Define the lower central series of a Lie algebra by and . A nilpotent Lie algebra is one for which for some integer . If this holds, carries into , and consequently . This proves one implication without any condition on the field.
For the converse, we prove the linear form of the Engel theorem: if is a finite-dimensional Lie algebra consisting entirely of nilpotent linear maps, with finite-dimensional, then there is a nonzero vector annihilated by all of . This argument works over any field.
Induct on . The assertion is immediate when . First observe that if , then its commutator action on is nilpotent, becauseLet be a proper Lie subalgebra of . The commutator action of on therefore consists of nilpotent linear maps. Its image has dimension at most , so induction supplies a nonzero coset annihilated by . Thus , and the normalizer strictly contains . This is the Engel normalizer lemma.
Choose maximal among proper Lie subalgebras. Its normalizer must be , so is a Lie algebra ideal. Moreover : otherwise the inverse image of a one-dimensional subalgebra of would lie strictly between and . By induction,Since is an ideal, is -invariant: . Take . Its restriction to is nilpotent and hence has a nonzero kernel. A nonzero vector in that kernel is annihilated by and , and therefore by all of . This completes the induction.
Apply this result successively to , then its quotient by a common annihilated line, and so on. We obtain a complete flag with . Equivalently every element of is strictly upper triangular in one common basis; any product of such operators is zero.
Now take and . The hypothesis supplies exactly the nilpotence needed above. Every iterated bracket of length , where , is an application of adjoint operators and vanishes. These brackets span , giving . The zero algebra is already nilpotent. Thus is nilpotent if and only if every is nilpotent. The common flag is essential: separate nilpotence of unrelated operators would not imply that their mixed products vanish.
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