Sali Seminaryjna Teoretyczna, Hoża 69 at 11:15

Andrea Dapor 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
Sali Seminaryjna Teoretyczna, Hoża 69 at 11:15

Frederic P. Schuller 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.
Sali Seminaryjna Teoretyczna, Hoża 69 at 11:15

Jacek Pawełczyk Sali Seminaryjna Teoretyczna, Hoża 69 at 11:15

Daniele Malafarina 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.