Symétrie dans les systèmes dynamiques
Org:
Tanya Schmah (University of Ottawa) et
Cristina Stoica (Wilfrid Laurier University)
[
PDF]
 STEPHEN ANCO, Brock University
Symmetry multireduction method for partial differential equations with c onservation laws [PDF]

For partial differential equations (PDEs) that have $n\geq2$ independent variables and a symmetry algebra of dimension at least $n1$, an explicit algorithmic method is presented for finding all symmetryinvariant conservation laws that will reduce to first integrals for the ordinary differential equation (ODE) describing symmetryinvariant solutions of the PDE. This significantly generalizes the double reduction method known in the literature. Moreover, the condition of symmetryinvariance of a conservation law is formulated in an improved way by using multipliers, thereby allowing symmetryinvariant conservation laws to be obtained directly, without the need to first find conservation laws and then check their invariance. This cuts down considerably the number and complexity of computational steps involved in the reduction method. If the space of symmetryinvariant conservation laws has dimension $m\geq 1$, then the method yields $m$ first integrals along with a check of which ones are nontrivial via their multipliers. Several examples of interesting symmetry reductions are considered: travelling waves and similarity solutions in $1+1$ dimensions; line travelling waves, line similarity solutions, and similarity travelling waves in $2+1$ dimensions; rotationally symmetric similarity solutions in $n+1$ dimensions.
 ROY H. GOODMAN, New Jersey Institute of Technology
Instability of Leapfrogging Vortex Pairs [PDF]

We investigate the stability of a oneparameter family of periodic solutions of the fourvortex problem known as `leapfrogging' orbits. These solutions, which consist of two pairs of identical yet oppositelysigned vortices, were known to Gröbli (1877) and Love (1883), and can be parameterized by a dimensionless parameter $\alpha$ related to the geometry of the initial configuration. Simulations by Acheson (2000) and numerical Floquet analysis by Tophøj and Aref (2012) both indicate, to many digits, that the bifurcation occurs when $1/\alpha=\phi^2$, where $\phi$ is the golden ratio. This study aims to explain the origin of this remarkable value. Using a trick from the gravitational twobody problem, we change variables to render the Floquet problem in an explicit form that is more amenable to analysis. We then implement G. W. Hill's method of harmonic balance to high order using computer algebra to construct a rapidlyconverging sequence of asymptotic approximations to the bifurcation value, confirming the value found earlier. We also explain, via careful numerical study, many of the features of the nonlinear dynamics seen in earlier accounts.
 CASEY JOHNSON, Claremont Graduate University
Spectrum of different Stieltjes star graphs [PDF]

The spectrum of a single Stieltjes string, a thread bearing a finite number of point masses, is uniquely determined by the number and size of the masses. In 2002, F.R. Gantmakher and M.G. Krein solved the inverse problem which identified the location and mass of each bead given just the spectrum corresponding to Dirichlet boundary conditions and the spectrum corresponding to Neumann boundary conditions. Joining multiple Stieltjes strings of various lengths together to form a star graph shape which are often symmetric has fascinating implications on the spectrum of the graph. For these new star graphs, is the spectrum still uniquely determined? What can we say about the spectrum?
 YURI LATUSHKIN, University of Missouri
The Maslov index and the spectrum of differential operators [PDF]

We will review some recent results on connections between the Maslov and the Morse indices
for differential operators. The Morse index is a spectral quantity defined as the number of
negative eigenvalues counting multiplicities while the Maslov index is a geometric
characteristic defined as the signed number of intersections of a path in the space of
Lagrangian planes with the train of a given plane. The problem of relating these two quantities
is rooted in Sturm's Theory and has a long history going back to the classical work by Arnold,
Bott and Smale, and has attracted recent attention of several groups of mathematicians.
We will briefly mention how the relation between the two indices helps to prove the fact
that a pulse in a gradient system of reaction diffusion equations is unstable.
We will also discuss a fairly general theorem relating the indices for a broad class
of multidimensional elliptic selfadjoint operators. Connections of the Maslov index and
Hadamardtype formulas for the derivative of eigenvalues will be also discussed.
This talk is based on a joint work with M. Beck, G. Cox, C. Jones, P. Howard, R. Marangell,
K. McQuighan, A. Sukhtayev, and S. Sukhtaiev.
 MARK LEVI, Penn State
Gaussian curvature and spinning tops [PDF]

I will describe the hidden role of Gaussuan curvature in the dynamics of the Lagrange top and will relate this to the Jacobi fields for geodesic flows. I will also describe the recently discovered phenomenon of “ponderomotive magnetism”. This is based on joint work with Oleg Kirillov and Graham Cox.
 GEORGE PATRICK, University of Saskatchewan
Geometric mechanics and the lump dynamics of the $CP^1$ sigma model on the sphere. [PDF]

Usually the potential energy of a simple mechanical system breaks the larger
symmetry of its kinetic energy. However, the $CP^1$ sigma model is a lagrangian
field theory of potential plus kinetic type where the potential has the larger
symmetry. In this case equilibria are not isolated but rather occur in a
nongeneric way on group orbits of the symmetry of the potential, and the
dynamics near such equilibria may be approximated by a geodesic flow. Applied
to the $CP^1$ sigma model [J.M. Speight, Lowenergy dynamics of a $CP^1$ lump
on the sphere], this yields a finite dimensional simple mechanical system with
the additional feature that its configuration space has nontrivial (constant
type) isotropy, thereby providing a specific example of the general situation
considered in the 1983 technical report [R. Montgomery, The structure of
reduced cotangent phase spaces for nonfree group actions].
 MANUELE SANTOPRETE, Wilfrid Laurier University
On the Relationship between Two Notions of Compatibility for BiHamiltonian Systems [PDF]

BiHamiltonian structures are of great importance in the theory of integrable Hamiltonian systems. The notion of compatibility of symplectic structures is a key aspect of biHamiltonian systems. Because of this, a few different notions of compatibility have been introduced. In this talk we show that, under some additional assumptions, compatibility in the sense of Magri implies a notion of compatibility due to Fass\`o and Ratiu, that we dub biaffine compatibility. There are at least two proofs of this fact. The first one uses the uniqueness of the connection parallelizing all the Hamiltonian vector fields tangent to the leaves of a Lagrangian foliation. The second proof uses DarbouxNijenhuis coordinates and symplectic connections. In this talk we will attempt to outline both proofs.
 ALEXEY F. SHEVYAKOV, University of Saskatchewan
Symbolic computation of symmetries and first integrals in dynamical systems [PDF]

While the solution structure of dynamical systems given by ordinary differential equations (ODE) and ODE systems is well understood, and the solution behaviour can be analyzed locally and globally using various analytical methods, for the vast majority of nonlinear systems, it is not possible to write down the general solution in a closed form. In many cases, however, it is possible to reduce the differential order of the ODEs. Order can be reduced when one knows a conserved quantity (a first integral) that is constant on solutions, and/or a local symmetry group that leaves the ODE system invariant. A sufficient number of first integrals and/or local symmetries known for a given ODE model leads to its complete integration.
Lie groups of point, contact, and higherorder symmetries can be systematically computed using the Lie's algorithm, which, however, may require heavy computations.
Similarly, conservation laws of partial differential equations, and as a special case, first integrals of ODEs, can be computed using the direct (multiplier) method and the Euler differential operator that annihilates divergences. Such computations are also algorithmic, but for nontrivial examples, can be computationally demanding.
In this talk, we will demonstrate symbolic computations of symmetries and first integrals of ODEs using the \verbMaplebased \verbGeM symbolic software package. Examples of dynamical systems based on ODEs and nonlinear PDEs, such as shallow water models and the $b$family of peakon equations, will be presented.
 MICHAEL WARD, UBC
The Slow Dynamics of Spot Patterns for ReactionDiffusion Systems on the Sphere [PDF]

In the singularly perturbed limit corresponding to large a diffusivity
ratio between two components in a reactiondiffusion (RD) system, many
such systems admit quasiequilibrium spot patterns, where the solution
concentrates at a discrete set of points in the domain. In this context,
we derive and study the differential algebraic equation (DAE) that
characterizes the slow dynamics for such spot patterns for the
Brusselator
RD model on the surface of a sphere. Asymptotic and numerical
solutions are presented for the system governing the spot strengths,
and we describe the complex bifurcation structure and demonstrate the
occurrence of imperfection sensitivity due to higher order effects.
Localized spot patterns can undergo a fast time instability and we
derive the conditions for this phenomena, which depend on the spatial
configuration of the spots and the parameters in the system. In the
absence of these instabilities, our numerical solutions of the DAE
system for $N = 2$ to $N = 10$ spots suggest a large basin of
attraction to a small set of possible steadystate configurations. We
discuss the connections between our results and the study of point
vortices on the sphere, as well as the problem of determining a set of
elliptic Fekete points, which correspond to globally minimizing the
discrete logarithmic energy for $N$ points on the sphere.