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Dirac structures and geometry of nonholonomic constraints

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<strong>Dirac</strong> structure<br />

Definition<br />

A <strong>Dirac</strong> structure L on a manifold M is a vector subbundle <strong>of</strong><br />

TM ⊕M T ∗ M which is maximal isotropic with respect to the metric<br />

〈Xp + ϕp | Yp + ψp〉 = 1<br />

2 (〈ψp, Xp〉 + 〈ϕp, Yp〉)<br />

<strong>and</strong> involutve with respect to Dorfman bracket<br />

[X + ϕ, Y + ψ]D = [X , Y ] + (LX ψ − ıY dϕ).<br />

We call L an almost <strong>Dirac</strong> structure when it is maximal isotropic <strong>and</strong> not<br />

involutive.<br />

KG (KMMF) Seminarium Geometryczne 13 X 2010 4 / 26

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