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Kostant's nilradical cohomology theorem
Statement
Assume the Axiom of Choice. Let be a finite-dimensional complex semisimple Lie algebra with Cartan subalgebra , chosen positive system and , and let be dominant integral with . Then for every there is an isomorphism of -modules where is the one-dimensional -module of weight and . Equivalently, is multiplicity free with weights exactly the pairwise distinct weights over the length- elements, and .
Facts & Assumptions
Given: The Axiom of Choice; the finite-dimensional data and the operators of The Chevalley–Eilenberg Laplacian is scalar on weight components.
The harmonic projection identifies with the harmonic cochains , and these are spanned by the extremal cochains: (Each extremal harmonic space is one-dimensional).
Each is a nonzero cocycle of weight (The extremal weight cochain of a Weyl element is closed and unique).
The identifications and the direct sum are isomorphisms of -modules: the -action of The normalizer acts on Lie algebra cohomology commutes with , the harmonic projection is obtained from the -stable subspaces and , and the displayed identity for in The Chevalley–Eilenberg Laplacian is scalar on weight components exhibits as a polynomial in operators that commute with one another, so commutes with the -action as well.
The dot weights are pairwise distinct: is regular, with trivial stabilizer, by (Positive coroot pairings of a dominant integral weight, Integral, dominant, and strictly dominant weights, The Weyl vector rho for a chosen positive system); and each weight space is one-dimensional (Extremal Weyl-orbit weights, Highest-weight classification, Weight and weight space, Length and longest Weyl-group element, Chevalley–Eilenberg cochains, Lie algebra cohomology).
Proof
By [F1] the space is isomorphic to , and by [F3] this isomorphism is -linear.
Each summand is the one-dimensional -module of weight by [F2], and the weights for distinct Weyl elements are pairwise distinct by the regularity of recorded in [F4]. Hence the direct sum in step 1.1 is exactly as an -module.
Counting dimensions in step 2.1 gives and shows that the multiplicity of every occurring weight is one; in particular is multiplicity free with the stated weights, and all groups are finite dimensional because is finite.
Depends on
- Each extremal harmonic space is one-dimensional
- The extremal weight cochain of a Weyl element is closed and unique
- The Chevalley–Eilenberg Laplacian is scalar on weight components
- The normalizer acts on Lie algebra cohomology
- Positive coroot pairings of a dominant integral weight
- Integral, dominant, and strictly dominant weights
- The Weyl vector rho for a chosen positive system
- Length and longest Weyl-group element
- Weight and weight space
- Extremal Weyl-orbit weights
- Highest-weight classification
- Chevalley–Eilenberg cochains
- Lie algebra cohomology
- The Axiom of Choice
Used by
- Kostant cohomology in degrees zero and top Corollary
- The Kostant Euler character recovers the Weyl numerator Corollary
- Degree-one Kostant classes correspond to simple reflections Example
- Kostant cohomology for sl2 Example
- Kostant cohomology for the trivial sl3 module Example
- Kostant cohomology and BGG characters give the same Weyl numerator Proposition
Dependency tree · two levels
83 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Faisal Al-Faisal, On the Representation Theory of Semisimple Lie Groups (University of Waterloo MMath thesis, 2010), §3.4 printed pp.73–77 (standard reference, not scraped)
- Peter Woit, Lie Algebra Cohomology and the Borel–Weil–Bott Theorem (Math G4344, Spring 2012), printed pp.1–7 (standard reference, not scraped)