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Degree of Parabolic Quantum Groups - Dipartimento di Matematica ...

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1. Poisson algebraic <strong>Groups</strong> 12<br />

1.3.2 Poisson Lie group<br />

The definition <strong>of</strong> Poisson algebraic group formulated in the language <strong>of</strong> points<br />

can be easily carried over to the case <strong>of</strong> Poisson Lie groups. The principal<br />

<strong>di</strong>fficulty is that the comultiplication maps goes into C ∞ (G × G) but not<br />

necessarily into C ∞ (G) ⊗ C ∞ (G) = C ∞ (G × G)<br />

Definition 1.3.3. Let G be a Lie group and at the same time, a Poisson<br />

manifold. We say that G is a Poisson Lie Group if the multiplication m :<br />

G × G → G is a Poisson map.<br />

Note. Poisson Lie groups form a category, with morphisms being homomorphisms<br />

which are the same time Poisson maps.<br />

Proposition 1.3.4. Let G be both a Lie group and a Poisson manifold, and<br />

let π be the bivector field correspon<strong>di</strong>ng to the Poisson manifold structure on<br />

G. Then G is a Poisson Lie group if and only if π satisfies the following<br />

con<strong>di</strong>tion:<br />

π(g1g2) = (lg1 )∗π(g2) + (rg2 )∗π(g1)<br />

for any g1, g2 ∈ G, where lg is the left multiplication and rg is the right<br />

multiplication.<br />

Pro<strong>of</strong>. See [KS98], page 19.<br />

Corollary 1.3.5. The unit element <strong>of</strong> a Poisson Lie group is always a zero<strong>di</strong>mensional<br />

symplectic leaf<br />

In this thesis we always used Poisson algebraic groups so we shall describe<br />

Poisson brackets on the algebras <strong>of</strong> regular functions.<br />

Example 1.3.6. Every Lie group G with trivial Poisson bracket is a Poisson<br />

Lie group.<br />

Example 1.3.7. Consider the abelian Lie group G = C n . Note that by<br />

linearity it suffices to define the Poisson bracket on the coor<strong>di</strong>nate function.<br />

To get a Poisson Lie group structure we can take:<br />

{xi, xj} =<br />

n<br />

k=1<br />

c k i,jxk<br />

where xm, m = 0...n, are the coor<strong>di</strong>nate function, and the structure constant<br />

ck i,j satisfy the following con<strong>di</strong>tion:<br />

c k i,j = −c k j,i<br />

n <br />

c l i,jc m l,k + clj,k cml,i + clk,i cm <br />

l,j = 0<br />

l=1

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