Seminars
Listed below are upcoming seminars in the Department of Mathematics. To view different time periods, please refer the calendar on the right. Alternatively, seminars can be viewed by category:
- Colloquia
- Analysis and Nonlinear PDEs Seminars
- Biosystems Seminars
- Fields, Strings, and Geometry Seminars
- Geometric Mechanics and Fluids Seminars
Fronts in Non-Linear Wave Equations with Spatial Inhomogeneity
Tuesday 15 November 2011
Abstract: The non-linear wave equation (sometimes called the non-linear Klien-Gordon equation) is a much studied equation with applications in Josephson transmission lines, dislocations in crystals, DNA processes and much more. It possess many types of solutions which may include stationary front solutions. In this talk we shall consider what effect adding a step-like inhomogeneity has on the stability of such fronts and present some of the results we have derived over the last three years.
Molecular monolayers as interacting rolling balls: crystals, liquid and vapor
Wednesday 11 January 2012
Abstract: Molecular monolayers, especially water monolayers, are playing a crucial role in modern science and technology. In order to derive simplified models of monolayer dynamics, we consider the set of rolling self-interacting particles on a plane with an off-set center of mass and a non-isotropic inertia tensor. To connect with water monolayer dynamics, we assume the properties of the particles like mass, inertia tensor and dipole moment to be the same as water molecules. The perfect rolling constraint is considered as a simplified model of a very strong, but rapidly decaying bond with the surface. Since the rolling constraint is non-holonomic, it prevents the application of the standard tools of statistical mechanics: for example the system exhibits two temperatures -- translational and rotational-- for some degrees of freedom, and no temperature can be defined for other degrees of freedom.
Laguerre polynomials in dynamical systems
Friday 13 January 2012
Abstract: The famous Laguerre polynomials are orthogonal over [0,\infty) with respect to a negative exponential weight function. They are thus natural candidates for the efficient numerical approximation of such decaying exponential behaviour. We shall give a number of examples, including stable manifolds and fluid mechanics problems related to dynamical systems.
Stationary and travelling waves in lattices with saturable nonlinearities
Friday 20 January 2012
Abstract: We demonstrate existence of discrete solitons in Discrete Nonlinear Schrodinger equation (dlns) with saturable nonlinearity. We consider two types of solutions to (dlns) periodic and vanishing at infinity. In the second part of our talk, we prove the existence of periodic and solitary traveling waves in Fermi-Pasta-Ulam lattices with saturable nonlinearities. Calculus of variations and Nehari manifolds are employed to establish the existence of these solutions. We present some extensions of our results, combining the Nehari manifold approach and the Mountain Pass argument.
Numerical study of Rosensweig instability subject to diffusion of interacting particles
Friday 3 February 2012
Abstract: TBA
Towards the Probabilistic Earth System Model
Friday 10 February 2012
Abstract: TBA
Fluid-structure interaction with mean flow
Friday 17 February 2012
Abstract: TBA
The mechanics of plant root growth
Friday 24 February 2012
Abstract: Growing plant cells undergo rapid axial elongation with negligible radial expansion: high internal turgor pressure causes viscous stretching of the cell wall.
Infinite-dimensionality in "finite-dimensional" dissipative dynamics
Friday 2 March 2012
Abstract: TBA
Consensus and Polarization in a Three-State Bounded-Compromise Voter Model
Friday 9 March 2012
Abstract: It has recently been argued that the seek for "consensus" and some form of "incompatibility" are basic mechanisms to explain the dynamics of cultural change and diversity [1]. Here, we will consider a basic, but mathematically amenable, three-state bounded compromise voter model (a constrained generalization of the classic two-state voter model [2]) that includes these ingredients. In this opinion dynamics model, a population of size N is composed of "leftists" and "rightists" that interact with "centrists" on a complete graph: a leftist and centrist can both become leftists with rate (1+q)/2 or centrists with rate (1-q)/2 (and similarly for rightists and centrists), where q denotes a selective bias towards extremism (q>0) or centrism (q<0). This system admits three absorbing fixed points and a "polarization" line along which a frozen mixture of leftists and rightists coexist. In the realm of the Fokker-Planck equation, and using a mapping onto a population genetics model, we compute the fixation probability of ending in every absorbing state and the mean times for these events. We therefore show, especially in the limit of weak bias and large population size (|q|~1/N, N>>1), how fluctuations alter the mean field predictions: polarization is likely when q>0, but there is always a finite probability to reach a consensus; the opposite happens when q<0. The findings are illustrated and corroborated by stochastic simulations. This presentation is based on the recent Ref.[3]"
The evolution of transgenerational effects: when should offspring listen to their parents?
Friday 16 March 2012
Abstract: There is a growing realization among evolutionary biologists that heritable phenotypic variation is not always encoded in the DNA.
Horseshoes in magnetic rods and spinning tops
Friday 30 March 2012
Abstract: Motivated by electrodynamic space tethers we consider the statics problem of a conducting rod in a uniform magnetic field. This problem has close analogies with that of a spinning top in rigid-body dynamics. We show that some cases are integrable while others are nonintegrable. For the latter we use a (Hamiltonian) Melnikov approach that highlights problems with similar Melnikov applications in rigid-body dynamics in the literature as well as ways around these problems.
Quantitative recurrence for the Lorentz process
Friday 4 May 2012
Abstract: We consider the Lorentz process in the plane with periodic configuration of convex obstacles and with finite horizon. We define T(r) as the first return time of the flow to the r-neighbourhood of the initial position. We are interested in the behaviour of T(r) as r goes to zero. This is a joint work with Benoit Saussol.
Stability and mixing in two-dimensional vortices
Wednesday 9 May 2012
Abstract: In this talk I will review my previous work on stability and mixing in two-dimensional vortices. This will include a threshold calculation for the existence of nonlinear cat's eye structures and an investigation into nonlinear vorticity staircase structures in a Gaussian vortex.
The Marine Diversity Spectrum
Friday 11 May 2012
Abstract: We develop and test a mechanistic model of how diversity varies with body mass in marine ecosystems. The model predicts the form of the ``diversity spectrum,'' which quantifies the distribution of species' asymptotic body masses and is a species analogue of the classic size spectrum of individuals.
Continuum modelling of bacterial biofilm growth.
Friday 18 May 2012
Abstract: In this talk I will be presenting some of my work, in collaboration with many others, on the growth and regulation of bacterial biofilms; these are slimy colonies of non-motile bacteria on solid-fluid surfaces that have a number of implications in medicine and industry. The models to be discussed consist of nonlinear systems of PDEs and were analysed using asymptotic and computational methods. The main results and insights drawn from the work will be summarised.
Eat the specialist: Generalized models reveal stabilizing patterns in food webs
Friday 25 May 2012
Abstract: Food webs are the networks of who-eats-who in ecology. Despite being large and complex, the food webs observed in nature show relatively stable, stationary dynamics. Understanding this stability of food webs is a central challenge in ecology and could also inspire the design of more robust technical and organizational networks. Exploring food web stability is challenging because the food webs constitute high-dimensional and strongly nonlinear systems with dynamics on many different time scales.
Measure theoretic properties of rational maps missing period two orbits
Friday 1 June 2012
Abstract: Baker posed a question in the 1960's about when a rational map of degree d can be lacking periodic points of (minimum) period k. He gave the short list of pairs (d,k) that can occur. In this talk we discuss the complete solution to this problem proved by Hawkins' Ph.D. student Rika Hagihara.
Effect of surface stress on interfacial solitary wave propagation
Friday 8 June 2012
Abstract: The propagation of long wavelength disturbances on the surface of a fluid layer of finite depth is considered. An arbitrary stress is applied at the surface with both tangential and normal components.
On the (non)-minimality of free-semigroup actions on the interval which are C1-close to the identity
Friday 15 June 2012
Abstract: We consider (attracting) free semigroup actions (with two generators) on an interval. It is known that, if those two maps are sufficiently C2-close to the identity, then the (forward) minimal set. Namely, it must be an interval. (This statement is not accurate. I will give the precise statement in my talk.)
Backlund transformation and L2-stability of NLS solitons
Friday 22 June 2012
Abstract: TBA
Resurgent Analysis in Matrix Models
Friday 14 September 2012
Abstract:
In order to study the weakly coupled regime of theory we often make use of perturbative expansion of the physical quantities of interest. But such expansions are often divergent and defined only as asymptotic series. In fact, this divergence is connected to the existence of non-perturbative contributions, i.e. instanton effects that cannot be captured by a perturbative analysis. The theory of resurgence is a mathematical tool which allows us to effectively study this connection and its consequences. In this talk we will make use of this theory in order to show how to construct a full non-perturbative solution from perturbative data. To write this full non-perturbative solution we need to introduce generalised multi-instanton sectors, which can then be checked by precision tests on the asymptotic data. Finally, the study of this non-perturbative sectors in matrix models allows us to have a full picture of the phase diagram of this models.
Soliton collisions on G-strands
Friday 12 October 2012
Abstract:
A G-strand is a map g :(t,s)\in RxR -> g(t,s)\in G into a Lie group G that follows from Hamilton's principle for a certain class of G-invariant Lagrangians. G-strands on finite-dimensional groups satisfy 1+1 space-time evolutionary equations. Some of these equations are completely integrable Hamiltonian systems that admit soliton solutions. For example, the SO(3)-strand equations may be regarded physically as integrable dynamics for solitons on a continuous spin chain. Various other examples will be discussed, including collisions of solutions with singular support (e.g. peakons) on Diff(R)-strands, in which Diff(R) is the group of diffeomorphisms of the real line R, for which the group product is composition of smooth invertible functions.
Correlators of Hopf Wilson loops in the AdS/CFT correspondence
Tuesday 16 October 2012
Abstract:
The Wilson loop is one of the most important observables in gauge theories. It has long been suspected that its dynamics should have a natural description in terms of strings. The AdS/CFT correspondence is a realisation of this idea: the expectation value of Wilson loops in maximally supersymmetric Yang-Mills theory (MSYM) in four dimensions is captured by the partition function of type IIB superstring theory on AdS5 x S5, satisfying suitable boundary conditions. Accordingly, the MSYM computation at strong coupling is equivalent to a semiclassical approximation on the string theory side, and amounts to finding certain minimal area surfaces in AdS5 x S5.
In this talk, we deal with the correlator of two (supersymmetric) Wilson loops with contours lying on Hopf fibers of S3. A connected classical string surface, linking two different fibers, is presented. This string theory solution describes oppositely oriented fibers, and it is able to interpolate between a supersymmetric and non-supersymmetric configuration according to the fiber position on the Hopf base. We show that the system can be thought of as a deformation of the ordinary anti-parallel lines describing the static quark-antiquark potential, which is indeed correctly reproduced, at weak and strong coupling, as the fibers approach one another.
Relative geodesics and pattern matching
Wednesday 24 October 2012
Abstract: Given a Lie group G acting smoothly on a Riemannian manifold X, let c0 ,c1 : D → X be smooth functions, where D is also a smooth manifold (possibly with boundary). A geodesic relative to (c0 , c1) is a curve g : D → G with the property that gc0(s) = c1(s) for all sD, which minimises an energy integral over all such curves.
The talk will focus on G=SE(2), X=E2, D=[0,1] and applications to curve-matching. Another case, applicable to matching grayscale images, will also be mentioned if time permits.
Computing the Schrödinger equation with no fear of commutators
Friday 26 October 2012
Abstract: In this talk I report recent work on the solution of the linear Schrödinger equation (LSE) by exponential splitting in a manner that separates different frequency scales. The main problem in discretizing LSE originates in the presence of a very small parameter, which generates exceedingly rapid oscillation in the solution. However, it is possible to exploit the features of the graded free Lie algebra spanned by the Laplacian and by multiplication with the interaction potential to split the evolution operator in a symmetric Zassenhaus splitting so that the arguments of consecutive exponentials constitute an asymptotic expansion in the small parameter. Once we replace the Laplacian by an appropriate differentiation matrix, this results in a high-order algorithm whose computational cost scales like O(N log N), where N is the number of degrees of freedom and whose error is uniform in the small parameter.
Membranes and the emergence of geometry in MSYM and ABJM
Tuesday 30 October 2012
Abstract:
In the context of gauge/string theory correspondences, the geometry of membranes and space-times must be seen as an emergent phenomenon arising from a strongly coupled quantum field theory with a large local symmetry or gauge group.
I shall discuss the dual description of membranes in terms of long, gauge-invariant, local operators in the Maldacena and ABJM correspondences, focusing primarily on a class of D-branes known as giant gravitons. These restricted Schur polynomial operators in the MSYM and ABJM theories form complete, exactly orthonormal bases with respect to the free field, two-point correlation functions and are built using the representation theory of the permutation group.
Various BPS, non-spherical, D3-brane and D4-brane giant graviton configurations, embedded into and moving on the compact spaces S5 and CP3, will be constructed in type IIB string theory on AdS5xS5 and type IIA string theory on AdS4xCP3 respectively. In the latter case, the D4-brane giants embedded into the complex projective space CP3 are descendants of M5-brane giant gravitons in S7 under the compactification on the S1 Hopf fibre which takes S7 to CP3.
I shall finally discuss to what extent it has so far proven possible to view the non- trivial geometry of these membranes from the perspective of the dual operators.
Can we interpret swimming as a limit cycle?
Wednesday 31 October 2012
Abstract:
Fish appear to swim by periodically moving their fins. Additionally, if they momentarily stop or swim through a tangle of seaweed they appear to recover speed very quickly soon after. This mixture of stability and oscillatory behavior suggests that swimming is a limit cycle. I will provide theoretical evidence which suggests the answer is ``yes''. This will be done by defining a transitive Lie groupoid which can be used for fluid structure interaction. The base of this groupoid will be a set of embeddings of a body into space. We will then define the Lagrangian on the Lie algebroid, and add a time periodic force to the shape of the body as well as a viscous dissipation force due to the non-zero viscosity of the fluid. We will then perform a reduction by SE(3) to obtain a Lie groupoid where the base is the shape space of the swimmer. We will go over some arguments which suggest that a limit cycle could exists in this reduced system. Assuming a limit cycle does exist, we can use reconstruction formulas to obtain the motion of the fish. However, many analytical issues remain to be discussed.
Generalising the geometry of space-time: from gravity to supergravity
Friday 9 November 2012
Abstract:
Einstein's theory of General Relativity beautifully realises gravity as a theory of geometry: matter causes space-time to curve. "Supergravity" is an very particular and intricate extension of Einstein's theory that appears as a low-energy limit of string theory. In this talk, I will describe how, despite its apparently complexities, supergravity also has an elegant geometrical description that unifies the different symmetries of the theory in a direct analogue of Einstein's theory. The appropriate extension of conventional differential geometry is a version of "generalised geometry" first introduced by Hitchin. This formulation gives hints as to what notions of geometry might underlie string theory, and hence perhaps our own space-time. It also gives a number of unexpected extensions to conventional complex, symplectic and Kähler geometries.
Takiff affine Lie superalgebras and related CFT
Tuesday 13 November 2012
Abstract:
Motivated by an attempt to formulate (non chiral) conformal field theories of principal chiral models on manifolds of supergroups with vanishing Killing form as an OPE current algebras, we consider a related class of non semisimple affine (and non affine) (super)algebras, their representation theory and construct from them a chiral CFT. We address the questions of their representations, characters, fusion rules, and modular properties.
[Transparencies]
Aspects of gauge strings duality and some applications
Tuesday 20 November 2012
Abstract:
I will discuss some recent developments and applications on the duality between gauge fields and strings.
Invariant theory and free energy for liquid crystals
Friday 23 November 2012
Phase transitions for liquid crystals are typically characterized in terms of bifurcations of critical points for a free energy function. In a widely used model for the free energy due to Katriel et al. (1986) natural symmetries arise from the action of the group SO(3) wr Z_2 (wreath product) acting on 5x5 matrices through left/right multiplication and transposition. We investigate invariants for this group action, and also describe some bifurcation behaviour after a standard reduction is made to more tractable 2x2 matrices and the finite group D_3 wr Z_2 .
A quaternionic formulation of the point vortex equations on the sphere
Wednesday 28 November 2012
Abstract:
Point vortices are singularities in the vorticity field of a perfect fluid. Physically, they show up as points in the fluid around which the fluid rotates, much like the fluid rotating around the core of a hurricane in the atmosphere. From a fluid-dynamical point of view, the dynamics of point vortices forms a (finite-dimensional) Hamiltonian system, the solutions of which are weak solutions of Euler's equation, and there is consequently a great deal of interest in modeling and simulating the dynamics of point vortices.
Despite the fact that the equations of motion are Hamiltonian, however, this system has a number of special features which make direct numerical simulation hard: the vector field is not Lipschitz continuous, the symplectic form preserved is not the standard one, and there exists no Lagrangian formulation. The latter two problems especially make the construction of a symplectic integrator for this system a non-trivial task.
In this talk I will use the Hopf fibration to develop a new formulation of the point vortex equations on the sphere S^2. More specifically, I will show that there exists a nonlinear-Schrodinger-like equation on the Lie group SU(2), or alternatively the space of unit quaternions, whose solutions project down onto the trajectories of point vortices in S^2. Using the connection one-form of the Hopf fibration, I will also construct a Lagrangian for these equations, and we will investigate some symplectic integrators based on this formulation. We will illustrate the long-term qualitative features of these integrators with a number of examples from the recent literature, such as the spherical von Karman vortex street.
Holography of 3d N=4 superconformal quiver theories
Tuesday 4 December 2012
Abstract:
3d N=4 superconformal quiver theories arise as the low energy description of intersecting D3/D5/NS5 branes. I will discuss the backreacted solutions describing the near horizon of such configurations. The CFT partition function can be computed using localization technqiues and matched to the supergravity results.
Poisson structures transverse to coadjoint orbits and Kleinian singularities
Wednesday 5 December 2012
Abstract:
We give a brief general review of the ADE classification problem. The survey includes simple Kleinian singularities, symmetries of Platonic solids, finite subgroups of SU(2), the Mckay correspondence, integer matrices of norm 2 and Brieskorn’s theory of subregular orbits. We conclude with some joint work with H. Sabourin and P. Vanhaecke on transverse Poisson structures to subregular orbits in semisimple Lie algebras. We show that the structure may be computed by means of a simple Jacobian formula, involving the restriction of the Chevalley invariants on the slice. In addition, using results of Brieskorn and Slodowy, the Poisson structure is reduced to a three dimensional Poisson bracket, intimately related to the simple rational singularity that corresponds to the subregular orbit. Finally we present some recent results on the minimal orbit.
Iterative methods for computing canards
Wednesday 12 December 2012
On the size of random covering sets
Friday 25 January 2013
Abstract: Given a sequence of positive numbers $(\ell_n)$ and a sequence of independent random variables $(\xi_n)$ uniformly distributed on the circle $S^1$, define the random covering set $E$ as follows:
E={x\in S^1 | x\in [\xi_n,\xi_n+\ell_n] for infinitely many n}=limsup[\xi_n,\xi_n+\ell_n].
The random covering set has full Lebesgue measure almost surely, precisely when $\sum_n \ell_n=\infty$. Otherwise the set is almost surely Lebesgue null. A classical problem originally posed by Dvoretzky asks when is $E=S^1$ almost surely. A full answer was given by Shepp in 1972. For the zero Lebesgue measure case, the almost sure Hausdorff dimension of E has been found by Fan and Wu. We generalize their result by calculating the dimension of affine type random covering sets in the d-dimensional torus $T^d$.
Integrability for the AdS3/CFT2 correspondence
Tuesday 5 February 2013
Abstract:
An interesting instance of the AdS/CFT correspondence is the case of AdS3/CFT2. Strings on AdS_3xS^3xS^3xS^1 can be completely understood when the background is purely NSNS thanks to 2-dimensional conformal symmetry. Unfortunately this symmetry is not as useful in the case of RR backgrounds. However, it appears that the integrability techniques that proved successful in understanding the planar limit of AdS5/CFT4 may be applicable also here, which sparked new interest and efforts in this field.
I will review such techniques and report on some recent developments (arXiv:1211.5119, 1212.0505) in the understanding of the string spectrum on AdS_3xS^3xS^3xS^1, exploring in particular the limit in which one S^3 blows up to a flat space.

