eneralized complex structures were introduced by Hitchin and further studied by Gualtieri. They encompass symplectic structures and complex structures as extreme cases. In the general case, a generalized complex manifold can be seen as an even dimensional Poisson manifold equipped with additional structures. In the first part of the talk, we will review the definition of generalized complex structures and outline their relation with Poisson geometry, Lie algebroids and Lie groupoids. In the second part of the talk, we will propose “generalized contact bundles” as odd dimensional analogues of generalized complex manifolds. Finally, we will outline the relation between generalized contact bundles and Jacobi manifolds, Lie algebroids and Lie groupoids.
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Giovanni Moreno (IMPAN)
Batalin-Vilkovisky (BV) theories are classical field theories where the target space is Z-graded. They are particularly well-suited for gauge symmetry reduction. A BV theory comprises an action functional, a symplectic form, and a homological vector field: from the action functional one obtains the Euler-Lagrange (EL) field equations, the homological vector field encodes the gauge symmetries of the theory, and the symplectic form captures their interrelationship. Under physically reasonable assumptions, these data allows for a nice cohomological description of the tangent space to the so-called EL-moduli space (the space of solutions to the EL equations, modulo gauge symmetries), at a smooth point.In this two-parts seminar (based on the paper “Classical BV Theories on Manifolds with Boundary”, by A.S. Cattaneo et al., Commun. Math. Phys., 2014), I will review the main features of the BV formalism on closed manifolds. Then I will switch to manifolds with boundary, and show that a BV theory induces a so-called Batalin-Fradkin-Vilkovisky (BFV) theory on the boundary, in a compatible way: the result is a particular case of a BV-BFV theory. In the BV-BFV context, the symmetry reduction, and the corresponding cohomological “infinitesimal” description of the EL-moduli space at a smooth point, go along the same conceptual lines as in the BV case, but the actual procedure is more delicate, since it has to take into account the additional boundary structures. The final output will be the symplectic EL-moduli space, which fulfils the expected gluing properties, indispensable for quantisation.
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Giovanni Moreno (IMPAN)
Batalin-Vilkovisky (BV) theories are classical field theories where the target space is Z-graded. They are particularly well-suited for gauge symmetry reduction. A BV theory comprises an action functional, a symplectic form, and a homological vector field: from the action functional one obtains the Euler-Lagrange (EL) field equations, the homological vector field encodes the gauge symmetries of the theory, and the symplectic form captures their interrelationship. Under physically reasonable assumptions, these data allows for a nice cohomological description of the tangent space to the so-called EL-moduli space (the space of solutions to the EL equations, modulo gauge symmetries), at a smooth point.In this two-parts seminar (based on the paper “Classical BV Theories on Manifolds with Boundary”, by A.S. Cattaneo et al., Commun. Math. Phys., 2014), I will review the main features of the BV formalism on closed manifolds. Then I will switch to manifolds with boundary, and show that a BV theory induces a so-called Batalin-Fradkin-Vilkovisky (BFV) theory on the boundary, in a compatible way: the result is a particular case of a BV-BFV theory. In the BV-BFV context, the symmetry reduction, and the corresponding cohomological “infinitesimal” description of the EL-moduli space at a smooth point, go along the same conceptual lines as in the BV case, but the actual procedure is more delicate, since it has to take into account the additional boundary structures. The final output will be the symplectic EL-moduli space, which fulfils the expected gluing properties, indispensable for quantisation.
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Giovanni Moreno (IMPAN)
In Mechanics, the cotangent space to the configuration space, understood as the space of initial data for (regular) Lagrangian theories, is equipped with a natural symplectic structure. Similarly, in field theory, one gets an infinite-dimensional symplectic space of boundary fields, containing the space of initial data as a Lagrangian submanifold: such spaces are at the heart of the so-called BV-BFV theories with boundary, which are enjoying a renewed interest. In this talk, I will review a recent work with J. Kijowski, where the symplectic structures behind higher-order fields theories have been studied in detail. The so-obtained framework, based on an obvious jet-theoretic analogy with Mechanics, represents probably the simplest geometric description of the dynamics of a Lagrangian field theory. The symplectic structures involved are defined ‘fibre-by-fibre’ and, in this sense, they can be treated as finite-dimensional.
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Piotr Waluk (KMMF)
The Ricci flow is a technique for analyzing Riemannian manifolds by evolving their metric with respect to a certain differential equation. The method was first introduced by Hamilton in his paper form 1982, as means to solve a problem concerning classification of 3-dimensional compact manifolds. My talk will be a short introduction to the topic of the Ricci flow, explaining its basic ideas and illustrating them with some application examples.
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Rafał R Suszek (KMMF)
I shall formulate and illustrate on a simple and physically meaningful example the general principle by which (generalised Cheeger-Simons) differential characters and related transport operators defined by geometrisations of de Rham classes on the configuration bundle of a field theory with topological charges realise - in a concrete and computable manner - Segal's ambitious dream of functorial quantisation within and beyond the topological category. Time permitting, I shall also discuss certain important consequences of that principle.
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Javier de Lucas Arraujo (KMMF)
In the context of the Floquet theory, using a variation of parameter argument, we show that the logarithm of the monodromy of a real periodic Lie system with appropriate properties admits a splitting into two parts called dynamic and geometric phases. The dynamic phase is intrinsic and linked to the Hamiltonian of a periodic linear Euler system on the co-algebra. The geometric phase is represented as a surface integral of the symplectic form of a co-adjoint orbit
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Piotr Kopacz (Akademia Morska w Gdyni, Uniwersytet Jagielloński)
We consider the solutions to the Zermelo navigation problem on Riemannian manifolds, under perturbation represented by the weak vector field, in Finsler geometry with application of Randers metric. We compare it to the variational solutions via the Euler-Lagrange equations with non-restricted wind distribution. We focus on the river-type perturbation in the corresponding low-dimensional examples in the context of real applications in navigation. We also propose the geometric modi fication of the standard search patterns in case of acting vector field basing on the time-optimal paths.
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Michał Jóżwikowski (IMPAN)
I will discuss the SR geodesic problem from the point of view developed by Witold Respondek and myself in arxiv:1509.01628. The most important points of this approach are: (i) the Hamiltonian formalism is obsolete (ii) geometric reasonings are elementary (iii) the emphasis is put on the flows rather than on Lie brackets. If time allows I will address issues concerning local optimality of solutions.
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Andrzej Dragan (FUW)
We show that no device built according to the rules of quantum field theory can measure proper time along its path. Highly accelerated quantum clocks experience the Unruh effect, which inevitably influences their time rate. This contradicts the concept of an ideal clock, whose rate should only depend on the instantaneous velocity.
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Giovanni Moreno (IMPAN)
It is an easy exercise to show that the two-dimensional Monge-Ampère equations are the only two-dimensional second-order PDEs that are invariant under the natural action of the affine group of the plane. In three dimensions, an analogous statement can be proved, though it requires much more computations. In four dimensions, computations are simply unendurable, and the necessity of a more conceptual approach to the problem begins to show. In this talk I will recall that hypersurfaces of Lagrangian Grassmannians and second-order PDEs are basically the same thing, so that the notion of the invariancy (with respect to a given Lie group G) of a (multidimensional) second-order PDE can be formulated in terms of the G-invariancy of the corresponding hypersurface of the Lagrangian Grassmannian. Via the Plucker embedding, hypersurfaces of Lagrangian Grassmannians can be embbeded in a projective space. Such a projective space turns out to be a natural G-module, so that repesentation theory can be used for finding all the (relative) G-invariants polynomials, whose zero loci corresponds to G-invariant hypersurfaces. Up to 3 independent variables, such a method reveals nothing new, and it is just another way to show that Monge-Ampère equations correspond precisely to GL(n)-invariant hypersurfaces. Surprisingly enough, for n=4, a new unexpected class of invariant second-order PDEs pops out, which is not made of Monge-Ampère equations.This talk is based on a joint work with D. Alekseevsky and G. Manno.
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Mikołaj Rotkiewicz (MIMUW)
The full linearization functor enables studying graded bundles in a framework of multi-vector bundles. I will explain an unexpected relation between the linearization of graded bundles (of degree 2) and symplectic and metric double vector bundles discussed recently by Jotz Lean. This will be preceded by a gentle introduction to a beautiful theory of double vector bundles.
Zapraszamy do sali 106 IM PAN, ul. Śniadeckich 8, Ip o godzinie 14:15

Mikołaj Rotkiewicz (MIMUW)
The full linearization functor enables studying graded bundles in a framework of multi-vector bundles. I will explain an unexpected relation between the linearization of graded bundles (of degree 2) and symplectic and metric double vector bundles discussed recently by Jotz Lean. This will be preceded by a gentle introduction to a beautiful theory of double vector bundles.