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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 />

In this thesis, we study Lie algebras, Lie superalgebras, Jordan algebras and Novikov algebras<br />

equipped with a non-degenerate associative bilinear form. Such algebras are considered<br />

over the field of complex numbers and finite-dimensional. We add the condition that the bilinear<br />

form is symmetric or even, supersymmetric in the graded case. We call them respectively<br />

quadratic Lie algebras, quadratic Lie superalgebras, pseudo-Euclidean Jordan algebras<br />

and symmetric Novikov algebras.<br />

Let g be a finite-dimensional algebra over C and (X,Y ) ↦→ XY be its product. A bilinear<br />

form B : g × g → C is called associative (or invariant) if it satisfies:<br />

B(XY,Z) = B(X,Y Z)<br />

for all X,Y,Z in g and non-degenerate if B(X,g) = 0 implies X = 0. Such a bilinear form has<br />

arisen in several areas of Mathematics and Physics. It can be seen as a generalization of the<br />

Killing form on a semisimple Lie algebra, the inner product of an Euclidean Jordan algebra or<br />

simply, as the Frobenius form of a Frobenious algebra. The associativity of a bilinear form also<br />

can be found in the conditions of an admissible trace function defined on a power-associative<br />

algebra. For details, the reader can refer to a paper by M. Bordemann [Bor97].<br />

We begin with a quadratic Lie algebra g and its product, the bracket [ , ]. A result in the<br />

work of G. Pinczon and R. Ushirobira [PU07] leads to our first problem: define the 3-form I on<br />

g by I(X,Y,Z) = B([X,Y ],Z) for all X,Y,Z in g. Then I satisfies {I,I} = 0 where { , } is the<br />

super-Poisson bracket defined on A (g), the Grassmann algebra of skew-symmetric multilinear<br />

forms on g by:<br />

{Ω,Ω ′ n<br />

k+1<br />

} = (−1) ∑ ιXj<br />

j=1<br />

(Ω) ∧ ιXj (Ω′ ), ∀ Ω ∈ A k (g),Ω ′ ∈ A (g)<br />

in a fixed orthonormal basis {X1, ..., Xn} of g.<br />

In this case, the element I is called the 3-form associated to g. Conversely, given a quadratic<br />

vector space (g,B) and a non-zero 3-form I on g such that {I,I} = 0, then there is a non-Abelian<br />

quadratic Lie algebra structure on g such that I is the 3-form associated to g. By a classical result<br />

in a N. Bourbaki’s book [Bou58] that is also recalled in Proposition 2.2.3, we set the following<br />

vector space:<br />

VI = {α ∈ g ∗ | α ∧ I = 0}<br />

The dup-number dup(g) of a non-Abelian quadratic Lie algebra g is defined by dup(g) =<br />

dim(VI). It measures the decomposability of the 3-form I and its range is {0,1,3}. For instance,<br />

I is decomposable if and only if dup(g) = 3 and then the corresponding quadratic Lie algebra<br />

vi

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