TH`ESE A NEW INVARIANT OF QUADRATIC LIE ALGEBRAS AND ...
TH`ESE A NEW INVARIANT OF QUADRATIC LIE ALGEBRAS AND ...
TH`ESE A NEW INVARIANT OF QUADRATIC LIE ALGEBRAS AND ...
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1.4. Invertible orbits<br />
Let us now consider C ∈ gε, C invertible. Then, m must be even (obviously, it happened if<br />
ε = −1), m = 2n (see Appendix A). We decompose C = S + N into semisimple and nilpotent<br />
parts, S, N ∈ gε by its Jordan decomposition. It is clear that S is invertible. We have λ ∈ Λ if<br />
and only if −λ ∈ Λ (Appendix A) where Λ is the spectrum of S. Also, m(λ) = m(−λ), for all<br />
λ ∈ Λ with the multiplicity m(λ). Since N and S commute, we have N(V ±λ ) ⊂ V ±λ where V λ<br />
is the eigenspace of S corresponding to λ ∈ Λ. Denote by W(λ) the direct sum<br />
Then<br />
Define the equivalence relation R on Λ by:<br />
W(λ) = V λ ⊕V −λ .<br />
λRµ if and only if λ = ±µ.<br />
C 2n =<br />
⊥<br />
λ∈Λ/R<br />
W(λ),<br />
and each (W(λ),B λ ) is a vector space with the non-degenerate form B λ = Bε| W(λ)×W(λ).<br />
Fix λ ∈ Λ. We write W(λ) = V+ ⊕V− with V± = V ±λ . Then, according to the notation in<br />
Lemma 1.4.2, define N ±λ = N±. Since N|V− = −N∗ λ , it is easy to verify that the matrices of<br />
N|V+ and N|V− have the same Jordan form. Let (d1(λ),...,dr (λ)) be the size of the Jordan<br />
λ<br />
blocks in the Jordan decomposition of N|V+ . This does not depend on a possible choice between<br />
N|V+ or N|V− since both maps have the same Jordan type.<br />
Next, we consider<br />
D = <br />
{(d1,...,dr) ∈ N r | d1 ≥ d2 ≥ ··· ≥ dr ≥ 1}.<br />
r∈N ∗<br />
Define d : Λ → D by d(λ) = (d1(λ),...,dr λ (λ)). It is clear that Φ ◦ d = m where Φ : D → N<br />
is the map defined by Φ(d1,...,dr) = ∑ r i=1 di.<br />
Finally, we can associate to C ∈ gε a triple (Λ,m,d) defined as above.<br />
Definition 1.4.3. Let Jn be the set of all triples (Λ,m,d) such that:<br />
(1) Λ is a subset of C \ {0} with ♯Λ ≤ 2n and λ ∈ Λ if and only if −λ ∈ Λ.<br />
(2) m : Λ → N∗ satisfies m(λ) = m(−λ), for all λ ∈ Λ and ∑ m(λ) = 2n.<br />
λ∈Λ<br />
(3) d : Λ → D satisfies d(λ) = d(−λ), for all λ ∈ Λ and Φ ◦ d = m.<br />
Let I (2n) be the set of invertible elements in gε and I (2n) be the set of Iε-adjoint orbits<br />
of elements in I (2n). By the preceding remarks, there is a map i : I (2n) → Jn. Then we<br />
have a parametrization of the set I (2n) as follows:<br />
Proposition 1.4.4.<br />
The map i : I (2n) → Jn induces a bijection i : <br />
I (2n) → Jn.<br />
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