A geometric realization of an integrable system is an evolution of curves on a manifold M, invariant under the action of a group G, and such that it becomes the integrable system when the action of G is mod out. The best known geometric realization is the Vortex filament flow (VF), a flow of curves in Euclidean space which is invariant under the Euclidean group. The VF equation becomes the nonlinear Shrodinger equation when written in terms of the natural curvatures of the flow - Hasimoto proved this way the integrability of VF -. In this talk I will review what is known about the classical geometry of curves in homogeneous spaces and its relation to different types of integrable systems. In particular we will talk about how one can reduce different Hamiltonian structures to the space of curvatures (Euclidean, projective, conformal, etc) and how those reductions indicates the existence of biHamiltonian (integrable) systems. We will also describe how curvatures of Schwarzian type for curves in homogeneous spaces usually describe evolutions of KdV type. I will present background material so the talk should be accessible, at least in part, to different audiences.
The shadowing problem is related to the following question: under which condition, for any pseudotrajectory (approximate trajectory) of a vector field there exists a close trajectory? We study $C^1$-interiors of sets of vector fields with various shadowing properties. In the case of discrete dynamical systems generated by diffeomorphisms, such interiors were proved to coincide with the set of structurally stable diffeomorphisms for most general shadowing properties.
We prove that the $C^1$-interior of the set of vector fields with Oriented shadowing property contains not only structurally stable vector fields. Also, we have found additional assumptions under which the $C^1$-interiors of sets of vector fields with Lipschitz, Oriented and Orbit shadowing properties contain only structurally stable vector fields.
Some of these results were obtained together with my advisor S.Yu.Pilyugin.
We recapture the orthofermion algebra by means of a q-deformed particle
algebra A_p(q) whose deformed number operator has a finite spectrum
which is given by the deformed integers 0,[1],...[p]
Henry & Lucy Moses Professor of Science Lai-Sang Young
Institution:
Courant Institute of Mathematical Sciences
Time:
Monday, May 11, 2009 - 2:00pm
Location:
NS2 1201
I will discuss the reliability of large networks of coupled oscillators in response to fluctuating inputs. The networks considered are quite generic. In this talk, I view them as idealized models from neuroscience and borrow some of the associated language. Reliability is the opposite of trial-to-trial variability; a system is reliable if a signal elicits identical responses upon repeated presentations. I will address the problem on two levels: neuronal reliability, which concerns the behavior of individual neurons (or oscillators) embedded in the network, and pooled-response reliability, which measures total outputs from subpopulations. The effects of network structure, cell heterogeneity and noise on reliability will be discussed. Our findings are based largely on dynamical systems ideas (with a slight statistical mechanics flavor) and are supported by simulations. This is joint work with Kevin Lin and Eric Shea-Brown.
Henry & Lucy Moses Professor of Science Lai-Sang Young
Institution:
Courant Institute of Mathematical Sciences
Time:
Wednesday, May 13, 2009 - 4:00pm
Location:
RH 306
I will discuss the phenomenon of shear-induced chaos in driven dynamical systems. The unforced system is assumed to be nonchaotic with certain simple structures (such as attracting periodic orbits). Specifics of the defining equations are unimportant. A geometric mechanism for producing chaos - equivalently promoting mixing - is proposed. This mechanism involves the amplification of the effects of the forcing by shearing in the unforced system. Rigorous results establishing the presence of strange attractors will be discussed. Statistical information is deduced by comparing these attractors to countable-state Markov chains. The phenomenon of shear-induced chaos manifests itself in many different guises. Examples presented will include periodically kicked oscillators, slow-fast systems, PDEs undergoing Hopf bifurcations and coupled oscillators.