Seminar talk, 18 May 2016: Difference between revisions

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| speaker = Hovhannes Khudaverdian
| speaker = Hovhannes Khudaverdian
| title = The modular class of an odd Poisson (super)manifold and odd Laplacian
| title = The modular class of an odd Poisson (super)manifold and odd Laplacian
| abstract = Second order operator <math>\Delta</math> on half-densities can be uniquely defined by its principal symbol  up to a `potential'.  If <math>\Delta</math> is an odd operator such that order of operator <math>\Delta^2</math> is less than 3 then principal symbol of this operator, an odd contravariant rank 2 tensor field  defines an odd Poisson bracket.
| abstract = Second order operator <math>\Delta</math> on half-densities can be uniquely defined by its principal symbol  up to a 'potential'.  If <math>\Delta</math> is an odd operator such that order of operator <math>\Delta^2</math> is less than 3 then principal symbol of this operator, an odd contravariant rank 2 tensor field  defines an odd Poisson bracket.


We define the modular class of an odd Poisson supermanifold in terms of <math>\Delta</math> operator.  The modular class of an odd Poisson supermanifold is an obstacle to existence of operator <math>\Delta</math> defining the Poisson structure  such that <math>\Delta^2=0</math>.  In the case of non-degenerate odd Poisson structure the modular class vanishes, and we come to canonical odd Laplacian, the operator <math>\Delta</math> such that its principal symbol defines symplectic structure, potential vanishes in Darboux coordinates and <math>\Delta^2=0</math>.
We define the modular class of an odd Poisson supermanifold in terms of <math>\Delta</math> operator.  The modular class of an odd Poisson supermanifold is an obstacle to existence of operator <math>\Delta</math> defining the Poisson structure  such that <math>\Delta^2=0</math>.  In the case of non-degenerate odd Poisson structure the modular class vanishes, and we come to canonical odd Laplacian, the operator <math>\Delta</math> such that its principal symbol defines symplectic structure, potential vanishes in Darboux coordinates and <math>\Delta^2=0</math>.

Revision as of 20:08, 22 April 2016

Speaker: Hovhannes Khudaverdian

Title: The modular class of an odd Poisson (super)manifold and odd Laplacian

Abstract:
Second order operator Δ on half-densities can be uniquely defined by its principal symbol up to a 'potential'. If Δ is an odd operator such that order of operator Δ2 is less than 3 then principal symbol of this operator, an odd contravariant rank 2 tensor field defines an odd Poisson bracket.

We define the modular class of an odd Poisson supermanifold in terms of Δ operator. The modular class of an odd Poisson supermanifold is an obstacle to existence of operator Δ defining the Poisson structure such that Δ2=0. In the case of non-degenerate odd Poisson structure the modular class vanishes, and we come to canonical odd Laplacian, the operator Δ such that its principal symbol defines symplectic structure, potential vanishes in Darboux coordinates and Δ2=0.

This operator is the main ingredient of Batalin-Vilkovisky formalism.

Then we consider an example of an odd Poisson manifolds with non-vanishing modular classes related with the Nijenhuis bracket of form-valued vector fields.

References:
Khudaverdian H.M., Peddie M. Odd Laplacians: geometrical meaning of potential, and modular class, arXiv:1509.05686