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TH`ESE A NEW INVARIANT OF QUADRATIC LIE ALGEBRAS AND ...

TH`ESE A NEW INVARIANT OF QUADRATIC LIE ALGEBRAS AND ...

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Introduction<br />

by I. Bajo, S. Benayadi and M. Bordemann in [BBB], we prove that (Corollary 3.6.5 and Theorem<br />

3.6.8)<br />

THEOREM 13:<br />

A quasi-singular quadratic Lie superalgebra is a generalized double extension of a quadratic<br />

Z2-graded vector space. This superalgebra is 2-nilpotent.<br />

The algebras obtained in Chapter 2 and Chapter 3 lead us to the general framework as<br />

follows: let q be a complex vector space equipped with a non-degenerate bilinear form Bq and<br />

C : q → q be a linear map. We associate a vector space :<br />

J = q ⊥<br />

⊕ t<br />

to the triple (q,Bq,C) where (t = span{x1,y1},Bt) is a 2-dimensional vector space and Bt :<br />

t × t → C is the bilinear form defined by<br />

Bt(x1,x1) = Bt(y1,y1) = 0, Bt(x1,y1) = 1.<br />

Define a product ⋆ on the vector space J such that t is a subalgebra of J,<br />

y1 ⋆ x = C(x), x1 ⋆ x = 0, x ⋆ y = Bq(C(x),y)x1<br />

for all x,y ∈ q and such that the bilinear form BJ = Bq + Bt is associative. We call J the double<br />

extension of q by C. It can be completely characterized by the pair (Bq,C). Solvable singular<br />

quadratic Lie algebras and singular quadratic Lie superalgebras are only particular cases of this<br />

notion. Therefore, it is natural to consider similar algebras corresponding to the remaining<br />

different cases of the pair (Bq,C). In Chapter 4 we give a condition that J is a pseudo-Euclidean<br />

(commutative) Jordan algebra (i.e a Jordan algebra endowed with a non-degenerate associative<br />

symmetric bilinear form). Consequently, the bilinear forms Bq, Bt are symmetric, C must be<br />

also symmetric (with respect to Bq) and the product ⋆ is defined by:<br />

(x + λx1 + µy1) ⋆ (y + λ ′ x1 + µ ′ y1) = µC(y) + µ ′ C(x) + Bq(C(x),y)x1<br />

+ε λ µ ′ + λ ′ µ x1 + µµ ′ <br />

y1 ,<br />

ε ∈ {0,1}, for all x,y ∈ q, λ,µ,λ ′ , µ ′ ∈ C.<br />

Since there exist only two one-dimensional Jordan algebras, one Abelian and one simple,<br />

then we have two types of extensions called respectively nilpotent double extension and diagonalizable<br />

double extension. The first result (Proposition 4.2.1, Corollary 4.2.2, Lemma 4.2.7<br />

and Appendix D) is the following:<br />

THEOREM 14:<br />

(1) If J is the nilpotent double extension of q by C then C 3 = 0, J is k-step nilpotent, k ≤ 3,<br />

and t is an Abelian subalgebra of J.<br />

(2) If J is the diagonalizable double extension of q by C then 3C 2 = 2C 3 +C, J is not solvable<br />

and t ⋆ t = t. In the reduced case, y1 acts diagonally on J with eigenvalues 1 and 1 2 .<br />

xv

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