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Dual Coxeter number for the normalized invariant form
Definition
For a finite-dimensional complex simple Lie algebra as in Loop algebra of a simple Lie algebra, use the invariant form normalized by long roots of square in Residue two cocycle on a loop algebra. The local trace calculation below shows that the Casimir from Casimir operator relative to an invariant form acts in the adjoint representation as for a unique positive real scalar . Define the dual Coxeter number by . If a compact real form from Compact real form of a complex semisimple Lie algebra is additionally supplied, then for every -orthonormal basis one has . This is the normalization used in the affine central term and every Sugawara denominator below; existence of a compact real form is not needed to define .
Facts & Assumptions
Given: A nonzero finite-dimensional complex simple Lie algebra and its normalized invariant form . A compact real form is extra input only for step 3.1.
The normalization is for a positive real scalar ; is nondegenerate, symmetric and invariant (Residue two cocycle on a loop algebra). The Lie algebra is nonzero (Loop algebra of a simple Lie algebra).
For -dual bases , the adjoint Casimir operator is (Casimir operator relative to an invariant form).
The Killing form is (Killing form). The endomorphism trace is the sum of the diagonal entries in any finite basis (The basis-independent trace of an endomorphism of a finite-dimensional vector space, The trace as the sum of the diagonal entries).
A supplied compact real form has negative-definite restricted Killing form (Compact real form of a complex semisimple Lie algebra). A finite-dimensional positive-definite real inner-product space has an orthonormal basis by finite Gram–Schmidt (Every finite-dimensional real or complex inner product space has an orthonormal basis).
Proof
Given: The Lie algebra and normalized form above; write .
Fix one finite basis and its -dual basis , so . If , then by duality. Therefore [F3] gives . All choices here are finite and is nondegenerate by [F1].
For arbitrary , [F2], symmetry and invariance give Indeed the first conversion uses with , and the second uses the same identity with , followed by symmetry. Step 1.1 identifies the final sum with . Thus , with no compact real form or spectral assertion.
By [F1], . Step 1.2 implies for every , so nondegeneracy yields for every . Hence with . The scalar is unique because . Its half is therefore well defined and positive without a compact-form existence theorem or a choice axiom.
If a compact real form is supplied, [F1] and [F4] make positive definite. Take a finite -orthonormal real basis by [F4]; it is also a complex basis of because is a real form. Its -dual basis is , since . Thus [F2] gives , and step 2.1 identifies this with . This proves the conditional compact-basis formula without constructing a compact real form or inferring its existence from its definition.
Depends on
- Casimir operator relative to an invariant form
- Residue two cocycle on a loop algebra
- Loop algebra of a simple Lie algebra
- Killing form
- The basis-independent trace of an endomorphism of a finite-dimensional vector space
- The trace $\operatorname{tr}(A)$ as the sum of the diagonal entries
- Compact real form of a complex semisimple Lie algebra
- Every finite-dimensional real or complex inner product space has an orthonormal basis
Used by
- The normalized Sugawara formula is undefined at critical level Counterexample
- Sugawara modes and their normal ordering Definition
- The critical-level sl2 affine vertex algebra and its current OPE Example
- The level-one sl2 Sugawara central charge Example
- The level-zero trivial sl2 module Example
- Sugawara current commutators on every restricted module Lemma
- The Sugawara mode-one commutator Lemma
Dependency tree · two levels
24 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
- David Ben-Zvi and Edward Frenkel, Geometric Realization of the Segal–Sugawara Construction, §2.1 (standard reference, not scraped)
- Antony Wassermann, Kac–Moody and Virasoro Algebras, Chapter I §13 (standard reference, not scraped)