Seminarium Teorii Względności i Grawitacji
2006/2007 | 2007/2008 | 2008/2009 | 2009/2010 | 2010/2011 | 2011/2012 | 2012/2013 | 2013/2014 | 2014/2015 | 2015/2016 | 2016/2017 | 2017/2018 | 2018/2019 | 2019/2020 | 2020/2021 | 2021/2022 | 2022/2023 | 2023/2024 | 2024/2025 | Strona własna seminarium
2013-03-15 (Piątek)
Andrzej Krasiński
Dryf promieni świetlnych wywołany niesymetryczną ekspansją: możliwy test obserwacyjny jednorodności Wszechświata
Drift of light rays induced by nonsymmetric expansion: a possible observational test of homogeneity of the Universe
2013-03-08 (Piątek)
Piotr Ogonowski
Grawitacja jako pole. Zalety kwantowania grawitacji po dekompozycji Gerocha
2013-03-01 (Piątek)
Piotr Chruściel
Dwuwymiarowe diagramy w OTW
W referacie omówię diagramy Penrose'a, a także diagramy rzutowe wprowadzone w pracy arXiv:1211.1718 (napisanej z C.Oelz i S.Szybką), jako metodę wizualizacji struktury przyczynowej czasoprzestrzeni.
2013-02-22 (Piątek)
Paweł Duch
Construction of Dirac observables in General Relativity using Fermi coordinates
2013-01-25 (Piątek)
Piotr Sułkowski
Counting chord diagrams and topological recursion
2013-01-18 (Piątek)
Paweł Nurowski
Lagrange solution of 3-body problem and beyond
2013-01-11 (Piątek)
Andrea Dapor
Isotropy-breaking in Quantum Cosmology
We present a new perspective on QFT on quantum cosmological space-times. Naively, the semiclassical limit of a quantum space-time can be taken by averaging the gravitational operators on a semiclassical state of geometry. The result is an effective classical metric (which in general does not obey Einstein equation). We show that, once quantum matter is taken into account, a new possibility arises: the dynamics of matter on quantum space-time can be equivalently described by standard QFT on a classical space-time, whose geometry is encoded in a so-called "dressed metric", a classical metric which is different than the naive semiclassical one. Such matter-dependent dressed metric can be thought of as the metric "seen" by the matter field.We explore this interpretation and its consequences in various instances, such as scalar field on quantum cosmological space-times, addressing the question of observable effects on the propagation of matter. Indeed, since the dressed metric depends on the matter, Lorentz-violating phenomena are expected (such as deformation of dispersion relations). We prove that for massless field on FRW quantum spacetime [1] no violation takes place; we then address the massive case [2], and show that an isotropy-breaking is present, since the dressed metric depends on the direction of propagation of the mode of the field.References:[1] A. Ashtekar, W. Kaminski, J. Lewandowski - "Quantum field theory on a cosmological, quantum space-time", Phys. Rev. D 79, 064030 (2009)[2] A. Dapor, J. Lewandowski - "Isotropy-Breaking in Quantum Cosmology", arXiv:1211.0161
2012-12-14 (Piątek)
Frederic P. Schuller
All tensorial spacetime geometries
The class of tensor fields on a smooth manifold that can serve as a spacetime geometry is severely restricted --- namely if the geometry is required to be able to carry matter field equations that are both predictive and quantizable.So restricted in fact, that even the spacetime dynamics are completely determined by the structure of any matter field equations the tensorial geometry is required to carry.The key result is that the construction of any gravitational dynamics (including but also beyond Einstein) is reduced from a vague physical question to a clear-cut mathematical task --- namely to the mere solution of a system of linear homogeneous PDEs.These results are therefore of immediate relevance to any study of modified spacetime kinematics and gravitational dynamics, and will be explained for a general audience of relativists in this talk.
2012-12-07 (Piątek)
Jacek Pawełczyk
Quark masses in a string unification
2012-11-30 (Piątek)
Daniele Malafarina
Can observations help us distinguish black holes from naked singularities?
There is still no proof that black holes must necessary be the only final outcome of complete gravitational collapse of astrophysical objects. If naked singularities can occur and if the singularity is to be resolved at some quantum level, then solutions of Einstein equations with naked singularities could in principle describe the surroundings of some 'exotic' compact sources in the universe. We analyze some observable features of accretion disks in spacetimes containing naked singularities in order to understand if they can be observationally different from those of black holes with the same mass.
Stron 2 z 3