Relativity Seminar (past)
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Tue, 30/04 12:00 |
Arthur Lipstein (Oxford) |
Relativity Seminar |
L3 |
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Tue, 12/03 12:00 |
Donal O'Conell (Neils Bohr Institute) |
Relativity Seminar |
Gibson 1st Floor SR |
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Tue, 26/02 12:00 |
Lars Andersson (Golm) |
Relativity Seminar |
L3 |
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Tue, 19/02 12:00 |
David Skinner (Princeton IAS/Cambridge) |
Relativity Seminar |
L3 |
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Tue, 12/02 12:00 |
Prof Kirill Krasnov (University of Nottingham) |
Relativity Seminar |
L3 |
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Tue, 22/01 12:00 |
Tim Adamo (Oxford) |
Relativity Seminar |
L3 |
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Tue, 27/11/2012 12:00 |
Dr Congkao Wen (Queen Mary College, London) |
Relativity Seminar |
L3 |
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Tue, 13/11/2012 12:00 |
James Drummond (Cern) |
Relativity Seminar |
L3 |
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Tue, 06/11/2012 12:00 |
Dr Ricardo Monteiro (Neils Bohr Institute) |
Relativity Seminar |
L3 |
| We will discuss the origin of the conjectured colour-kinematics duality in perturbative gauge theory, according to which there is a symmetry between the colour dependence and the kinematic dependence of the S-matrix. Based on this duality, there is a prescription to obtain gravity amplitudes as the "double copy" of gauge theory amplitudes. We will first consider tree-level amplitudes, where a diffeomorphism algebra underlies the structure of MHV amplitudes, mirroring the colour algebra. We will then draw on the progress at tree-level to consider one-loop amplitudes. | |||
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Tue, 23/10/2012 12:00 |
David Skinner (IAS Princeton) |
Relativity Seminar |
L3 |
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Thu, 21/06/2012 14:30 |
Lars Andresson (AEI Golm) |
Relativity Seminar |
Gibson 1st Floor SR |
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Tue, 12/06/2012 12:00 |
Dr Taghavi Chabert (Masaryk University) |
Relativity Seminar |
L3 |
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Fri, 08/06/2012 15:00 |
David McGady (Princeton) |
Relativity Seminar |
Gibson 1st Floor SR |
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Abstract: In this talk, I will discuss the proportionality between tree amplitudes and the ultraviolet divergences in their one-loop corrections in Yang-Mills and (N < 4) Super Yang-Mills theories in four-dimensions. From the point of view of local perturbative quantum field theory, i.e. Feynman diagrams, this proportionality is straightforward: ultraviolet divergences at loop-level are absorbed into coefficients of local operators/interaction vertices in the original tree-amplitude. Ultraviolet divergences in loop amplitudes are also calculable through on-shell methods. These methods ensure manifest gauge-invariance, even at loop-level (no ghosts), at the expense of manifest locality. From an on-shell perspective, the proportionality between the ultraviolet divergences the tree amplitudes is thus not guaranteed. I describe systematic structures which ensure proportionality, and their possible connections to other recent developments in the field. |
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Tue, 29/05/2012 12:00 |
Dr M Dunajski (University of Cambridge) |
Relativity Seminar |
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| Solitons are localised non-singular lumps of energy which describe particles non perturbatively. Finding the solitons usually involves solving nonlinear differential equations, but I shall show that in some cases the solitons emerge directly from the underlying space-time geometry: certain abelian vortices arise from surfaces of constant mean curvature in Minkowski space, and skyrmions can be constructed from the holonomy of gravitational instantons. | |||
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Tue, 15/05/2012 14:30 |
Prof Sergiu Klainerman (Princeton) |
Relativity Seminar |
Gibson 1st Floor SR |
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Tue, 01/05/2012 12:00 |
Song He (AEI Golm) |
Relativity Seminar |
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Tue, 06/03/2012 12:00 |
Dr Martin Wolf (Surrey) |
Relativity Seminar |
L3 |
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Tue, 28/02/2012 12:00 |
Mahdi Godazgar (DAMTP, Cambridge) |
Relativity Seminar |
L3 |
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Abstract: In this talk, I will discuss the peeling behaviour of the Weyl tensor near null infinity for asymptotically flat higher dimensional spacetimes. The result is qualitatively different from the peeling property in 4d. Also, I will discuss the rewriting of the Bondi energy flux in terms of "Newman-Penrose" Weyl components. |
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Tue, 21/02/2012 12:00 |
Tim Adamo (Oxford) |
Relativity Seminar |
L3 |
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Abstract: |
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Tue, 17/01/2012 12:00 |
Prof Graeme Segal (Oxford) |
Relativity Seminar |
L3 |
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The WZW functional for a map from a surface to a Lie group has a role in the theory of harmonic maps, and it also arises as the determinant of a d-bar operator on the surface, as the action functional for a 2-dimensional quantum field theory, as the partition function of 3-dimensional Chern-Simons theory on a manifold with boundary, and as the norm-squared of a state-vector. It is intimately related to the quantization of the symplectic manifold of flat bundles on the surface, a fascinating test-case for different approaches to geometric quantization. It is also interesting as an example of interpolation between commutative and noncommutative geometry. I shall try to give an overview of the area, focussing on the aspects which are still not well understood. |
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