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The shifted norm of a weight is maximal only at the top weight
Statement
Assume the Axiom of Choice (The Axiom of Choice). Let be a dominant integral weight and let be a weight of the finite-dimensional simple module (Highest-weight classification, Weight and weight space). With the Weyl vector (The Weyl vector rho for a chosen positive system), with equality if and only if . Consequently is strictly positive for every weight of .
Facts & Assumptions
Given: The Axiom of Choice, a dominant integral weight , a weight of , the form on , the Weyl group and the Weyl vector .
The Axiom of Choice is assumed; it enters through the published weight-multiplicity and highest-weight suppliers, which carry it (The Axiom of Choice).
Every -orbit in has exactly one point in the closed chamber , so every weight has a unique dominant representative (Finite Weyl closed chambers and stabilizers, Finite Weyl root system, lattice and chamber conventions), and the weight multiplicities of are -invariant, so the weight set of is stable under (Simple reflections preserve weight multiplicities).
Every weight of satisfies , that is, (Highest weight modules lie below the top weight, Simple roots form a signed integral basis).
For every one has (The difference of the Weyl vector from its reflections is a sum of positive roots).
The action of on is by isometries of : (Finite Weyl root system, lattice and chamber conventions, Root reflections and the Weyl group action).
Pairings against : for one has ; for and a dominant one has , because writing with gives and , so in particular is strictly dominant (Positive coroot pairings of a dominant integral weight, Integral, dominant, and strictly dominant weights).
For a dominant integral and with reduced expression one has with every a positive root and every coefficient ; this is the reduced-word telescoping with prefix positivity from Finite Weyl strong exchange and deletion and Finite Weyl positive roots and simple reflections.
Proof
Let be the unique dominant representative of the -orbit of , which exists by [F1], and note that is also a weight of by the -invariance in [F1]; choose with and put , so that by [F2], and put , so that by [F3]; since is an isometry by [F4], and .
With steps 1.1 gives , and expanding this bilinear expression yields ; the last bracket is by symmetry and the isometry property [F4].
Hence with by step 1.1; the first term is nonnegative and the third is nonnegative because is dominant and is strictly dominant, while by positive definiteness of the form, so ; if then by [F5], so equality forces , that is, .
Suppose , so and ; then steps 1.1 and 2.1 give , and [F6] applied to writes with and coefficients , so ; by [F5] each , and the sum vanishes exactly when , that is, when , while for and clearly ; combining with step 3.1, with equality exactly for , and for every weight .
Depends on
- The Axiom of Choice
- Finite Weyl root system, lattice and chamber conventions
- Integral, dominant, and strictly dominant weights
- Root reflections and the Weyl group action
- Weight and weight space
- The Weyl vector rho for a chosen positive system
- Dominant integral weights are maxima of their Weyl orbits
- Finite Weyl closed chambers and stabilizers
- Highest weight modules lie below the top weight
- Positive coroot pairings of a dominant integral weight
- The difference of the Weyl vector from its reflections is a sum of positive roots
- Simple reflections preserve weight multiplicities
- Highest-weight classification
- Simple roots form a signed integral basis
- Finite Weyl positive roots and simple reflections
- Finite Weyl strong exchange and deletion
Used by
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Sources
- P. Etingof, Lie Groups and Lie Algebras II (MIT 18.755, Spring 2024), complete lectures (standard reference, not scraped)
- R. Borcherds, Berkeley Math 261 course notes, page on the Freudenthal multiplicity formula (standard reference, not scraped)