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Stefan Kurz | WPI Seminar Room C 714 | Mon, 19. Nov 12, 9:00 |
A new definition of a coordinate- and frame- free observer in relativistic Electrodynamics | ||
We are interested in the perception of the electromagnetic phenomenon by observers that are more general than standard inertial observers in flat MINKOWSKI space-time. We model a relativistic observer as (principal) fibre bundle, where the fibres correspond to world lines of test particles and the base space defines the observer’s relative “space”. An EHRESMANN connection on the bundle splits local tangent spaces into “space”- and time subspaces. The time subspaces point in direction of the world lines, and the “space” subspaces are their orthogonal complements, according to the hypothesis of locality. A section map on the bundle defines a time synchronization. The curvature of the connection is a measure of the non-integrability of the local “spatial” subspaces. If the connection is flat, it allows for a section that is orthogonal to the world lines in all points, hence a global EINSTEIN time- synchronization. Time synchronization can be seen as gauge on the bundle, and the formalism of gauge theories provides the right tools. Gauge potential and curvature have a kinematic interpretation as velocity and vorticity fields. This approach encompasses all meaningful spatial-temporal decompositions of space-time. With this setting we split electromagnetic field entities accordingly and describe the effect of relative motion on measurable quantities. We will present the one plus three-dimensional form of MAXWELL’s equations and the constitutive relation and analyze SCHIFF’s treatment of his 1939 paradox. In our view, the coordinate- and frame-free approach brings to light the individual layers of mathematical structure and their physical significance, and generally favours structural considerations over technical ones. We emphasize, however, that our findings can be readily translated into classical RICCI calculus, whereby all textbook results can be recovered. | ||
Note: You may download the presentation of the talk | ||
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Jerzy Kijowski | WPI Seminar Room C 714 | Mon, 19. Nov 12, 10:45 |
Gravitational energy: the Hamiltonian and quasi-local approach | ||
Dynamics of the gravitational field will be presented in the Hamiltonian context. I will prove that the generator of this dynamics must be a quasi-local quantity and can be identified with gravitational energy. However, an ambiguity remains: different boundary conditions (which have to be imposed in order to define uniquely the field evolution) lead to different Hamiltonian frameworks and, consequently, to different definitions of the energy. I will relate various definitions existing in the literature (Hawking, Geroch, Bartnik, Brown-York, Liu-Yau and myself) with different way of controlling boundary data and will argue that only one of them represents the "true" field energy. | ||
Note: You may download the presentation of the talk | ||
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Shadi Tahvildar-Zadeh | WPI Seminar Room C 714 | Mon, 19. Nov 12, 14:00 |
Integrability and Vesture for Harmonic Maps into Symmetric Spaces, with Applications to General Relativity | ||
After giving the most general formulation to date of the notion of integrability for axially symmetric harmonic maps from R 3 into symmetric spaces, we give a complete and rigorous proof that, subject to some mild restrictions on the target, all such maps are integrable. Furthermore, we prove that a variant of the inverse scattering method, called vesture (dressing) can always be used to generate new solutions for the harmonic map equations starting from any given solution. In particular we show that the problem of finding N- solitonic harmonic maps into a noncompact Grassmann manifold SU(p, q)/S(U(p) × U(q)) is completely reducible via the vesture (dressing) method to a problem in linear algebra which we prove is solvable in general. We illustrate this method by explicitly computing a 1-solitonic harmonic map for the two cases (p = 1, q = 1) and (p = 2, q = 1); and we show that the family of solutions obtained in each case contains, respectively, the Kerr family of solutions to the Einstein vacuum equations, and the Kerr-Newman family of solutions to the Einstein-Maxwell equations. Joint work with Shabnam Beheshti. | ||
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Robert Beig | WPI Seminar Room C 714 | Tue, 20. Nov 12, 9:00 |
The static 2-body problem in General Relativity | ||
The gravitational static 2-problem consists of showing that, under a suitable separation condition, two gravitating bodies can not be in static equilibrium. In Newtonian gravity such a separation condition is afforded by the assumption that the bodies in question are separated by a plane. We go on by considering a nonlinear generalization of Newtonian gravity due to Giulini and, finally, General Relativity. In both cases we prove that static 2-body configurations are ruled out under a condition which is in particular satisfied when there is a discrete symmetry interchanging the two bodies. This is work due to Rick Schoen and R.Beig. | ||
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Michael Kiessling | WPI Seminar Room C 714 | Tue, 20. Nov 12, 10:45 |
Electrostatic Maxwell-Born-Infeld fields with point charge sources / Maximal foliations with lightcone defects | ||
I show that for any finite number of point charges of arbitrary sign, magnitude, and at arbitrary positions in real three-dimensional space, there exists a unique electrostatic solution to the Maxwell-Born-Infeld field equations with finite energy. This solution is real analytic away from the point charges, and its electrostatic potential can be extended Lipschitz-continuously into the locations of these point charges. The electrostatic potential can be re-interpreted as the time function of an almost everywhere spacelike maximal hypersurface with lightcone defects. No struts between the point charges / lightcone defects occur. The results are discussed in the context of the N body problem in general relativity. | ||
Note: You may download the presentation of the talk | ||
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Volker Perlick | WPI Seminar Room C 714 | Tue, 20. Nov 12, 14:00 |
On the self-force on point charges in Born-Infeld theory | ||
In standard electrodynamics the field energy in a sphere around a point charge is infinite. This gives rise to an infinite self-force and to all the well-known pathologies associated with the (Abraham-)Lorentz-Dirac equation, such as pre-acceleration and run-away solutions. In the 1930s, Born and Infeld introduced a non-linear theory of electrodynamics; they were able to show that in their theory the field energy in a sphere around a static(!) point charge is finite. However, little is known about the Born-Infeld field of an accelerated(!) point charge, in particular about its regularity. In this talk I present a method of how to analyze this problem with the help of series expansions of the electromagnetic field in terms of light cone coordinates. The final goal is to rigorously prove that the self-force of an accelerated point charge in Born-Infeld theory is finite. | ||
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Yann Brenier | WPI Seminar Room C 714 | Wed, 21. Nov 12, 9:00 |
Hidden convexity and linearization in the Born-Infeld model of Electromagnetism | ||
This is a review of some results on the Born-Infeld model: i) existence of a convex “entropy” (in the sense of the mathematical theory of hyper- bolic conservation laws) for a suitably extended version of the system; ii) Galilean invariance of the extended system; iii) conjectures on the weak completion of the model and the induced interaction between field and matter; iv) linearization of the model by gauging the ambient metric. | ||
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John Stalker | WPI Seminar Room C 714 | Wed, 21. Nov 12, 10:45 |
Scalar waves on the hyper-extreme Reissner-Nordstroem background | ||
Note: You may download the presentation of the talk | ||
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Volker Perlick | WPI Seminar Room C 714 | Wed, 21. Nov 12, 14:00 |
On photon accumulation near a black hole | ||
In the first part of the talk a Schwarzschild black hole is considered. We assume that light sources are distributed on a (big) sphere of radius R that emit, at an instant of time, photons isotropically. We calculate the resulting photon distribution and find that in the long-time limit the density becomes infinitely large near the photon sphere at r = 3 m . This suggests that every Schwarzschild black hole in Nature should be surrounded by a shell of very high photon density which could be detrimental to the health of any observer who comes close to this region. In the second part we discuss how the situation changes if a Kerr black hole is considered. The first part is based on the Bachelor Thesis of Dennis Philipp and the second part is ongoing work with Arne Grenzebach. | ||
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Yakov Itin | WPI Seminar Room C 714 | Thu, 22. Nov 12, 9:00 |
Which geometry is predicted by the electromagnetic waves? | ||
Electromagnetic waves in vacuum are described by the dispersion relation which is a rem- iniscence of the Lorentzian geometry. I will discuss a system of integral equations for two differential 2-forms.This is a most general expression of the Maxwell electromagnetism in media and in present of gravity field. A covariant jump condition on an arbitrary smooth hypersurface represents a characteristic equation of the system. I derive a dispersion rela- tion for the system with a linear local constitutive relation from the jump condition. This dispersion relation is an expression of the Finsler type geometry which is a basis of the birefrigence phenomena. The axion modification of the electrodynamics in the framework of the Carroll-Field-Jackiw (CFJ) model will be discussed. I show that in order to rep- resent the axion contribution to the wave propagation it is necessary to go beyond the geometric approximation. The axion field modifies the global topological structure of light cones surfaces. In CFJ-electrodynamics, such a modification results in violation of causal- ity. In addition, the optical metrics in axion electrodynamics are not pseudo-Riemannian. In fact, for all types of the axion field, they are even non-Finslerian. | ||
Note: You may download the presentation of the talk | ||
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Alberto Favaro | WPI Seminar Room C 714 | Thu, 22. Nov 12, 10:45 |
Fresnel versus Kummer surfaces: geometrical optics in dispersionless linear (meta)materials and vacuum | ||
Geometrical optics describes, with good accuracy, the propagation of high-frequency plane waves through an electromagnetic medium. Under such approximation, the behaviour of the electromagnetic fields is characterised by just three quantities: the temporal frequency ω, the spatial wave (co)vector k, and the polarisation (co)vector a. Numerous key properties of a given optical medium are determined by the Fresnel surface, which is the visual counterpart of the equation relating ω and k. For instance, the propagation of electromagnetic waves in a uniaxial crystal, such as calcite, is represented by two light-cones. Kummer, whilst analysing quadratic line complexes as models for light rays in an optical apparatus, discovered in the framework of projective geometry a quartic surface that is linked to the Fresnel one. Given an arbitrary dispersionless linear (meta)material or vacuum, we aim to establish whether the resulting Fresnel surface is equivalent to, or is more general than, a Kummer surface. | ||
Note: Click here for further information You may download the presentation of the talk | ||
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Felix Finster | WPI Seminar Room C 714 | Thu, 22. Nov 12, 14:00 |
Quantum oscillations can prevent the big bang singularity in an Einstein-Dirac cosmology | ||
After a brief introduction to general relativity and spinors in curved space-time, a spa- tially homogeneous and isotropic cosmological model is introduced where Dirac spinors are coupled to classical gravity. If the scale function is large, the universe behaves just like the classical Friedmann dust solution. If however the scale function is small, quantum effects lead to oscillations of the energy-momentum tensor. After explaining the basic mechanisms, it is shown numerically and analytically that these quantum oscillations can prevent the formation of a big bang or big crunch singularity. We sketch the existence proof for time-periodic solutions, where the universe goes through an infinite number of expansion and contraction cycles. This is joint work with Christian Hainzl. | ||
Note: You may download the presentation of the talk | ||
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Piotr Chrusciel | WPI Seminar Room C 714 | Fri, 23. Nov 12, 9:00 |
Space-time diagrammatics | ||
I will present a class of diagrams, which we call “projection diagrams”, which provide a useful tool to visualise the global structure of spacetimes. Various examples will be discussed in detail, including cosmological models, and the Kerr spacetimes with or without a cosmological constant. Based on joint work with Christa Oelz and Sebastian Szybka. | ||
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Dieter Brill | WPI Seminar Room C 714 | Fri, 23. Nov 12, 10:45 |
TBA | ||
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