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

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Introduction<br />

(3) There is a bijection between D(2 + 2n) and the set of semisimple Sp(2n)- orbits of<br />

P 1 (sp(2n)) that induces a bijection between D(2 + 2n) and Λn/Hn. In the reduced case,<br />

Dred(2 + 2n) is bijective to Λ + n /Hn.<br />

(4) There is a bijection between Sinv(2 + 2n) and the set of invertible Sp(2n)- orbits of<br />

P 1 (sp(2n)) that induces a bijection between Sinv(2 + 2n) and Jn/C ∗ .<br />

(5) There is a bijection between S(2 + 2n) and the set of Sp(2n)- orbits of P 1 (sp(2n)) that<br />

induces a bijection between S(2 + 2n) and D(2n)/C ∗ .<br />

As for quadratic Lie algebras, we have the notion of quadratic dimension for quadratic Lie<br />

superalgebras. In the case g having a 2-dimensional even part, we can compute its quadratic<br />

dimension as follows:<br />

dq(g) = 2 +<br />

(dim(Z(g) − 1))(dim(Z(g) − 2)<br />

.<br />

2<br />

We turn now to (g,B) a singular quadratic Lie superalgebra of type S1. By Definition 3.5.3<br />

and Lemma 3.5.5, the Lie superalgebra g can be realized as the double extension of a quadratic<br />

Z2-graded vector space q = q 0 ⊕ q 1 by a map C = C0 +C1 ∈ o(q 0) ⊕ sp(q 1). Denote by L (q 0)<br />

(resp. L (q 1)) the set of endomorphisms of q 0 (resp. q 1). We give a characterization as follows<br />

(Theorem 3.5.7).<br />

THEOREM 12:<br />

Let g and g ′ be two double extensions of q by C = C0 +C1 and C ′ = C ′<br />

0 +C ′<br />

Assume that C1 is non-zero. Then<br />

1, respectively.<br />

(1) there exists a Lie superalgebra isomorphism between g and g ′ if and only if there exist<br />

invertible maps P ∈ L (q 0), Q ∈ L (q 1) and a non-zero λ ∈ C such that<br />

(i) C ′<br />

0 = λPC0P −1 and P ∗ PC0 = C0.<br />

(ii) C ′<br />

1 = λQC1Q −1 and Q ∗ QC1 = C1.<br />

where P ∗ and Q ∗ are the adjoint maps of P and Q with respect to B|q 0 ×q 0 and B|q 1 ×q 1 .<br />

(2) there exists an i-isomorphism between g and g ′ if and only if there is a non-zero λ ∈ C<br />

such that C ′<br />

0 is in the O(q0)-adjoint orbit through λC0 and C ′<br />

1 is in the Sp(q1)-adjoint orbit through λC1.<br />

We close the problem on singular quadratic Lie superalgebras by an assertion that the dupnumber<br />

is invariant under Lie superalgebra isomorphisms (Theorem 3.5.9).<br />

In the last section of Chapter 3, we study the structure of a quadratic Lie superalgebra g<br />

such that its element I has the form:<br />

I = J ∧ p<br />

where p ∈ g ∗ 1 is non-zero and J ∈ A 1 (g 0) ⊗ S 1 (g 1) is indecomposable. We call g a quasisingular<br />

quadratic Lie superalgebra. With the notion of generalized double extension given<br />

xiv

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