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
Horyzonty w czasoprzestrzeniach algebraicznie specjalnych
Spacetime geometry and measurements in (2+1)-gravity
Diffeomorphism symmetry and perfect actions in discrete gravity
How to use the isometric embedding theorem to coarse-grain a inhomogeneous cosmological model
Spinory i twistory
Gauged vortices and localisation
Spinory i twistory. Ciag dalszy referatow wygloszonych w lutym.
http://www.fuw.edu.pl/~amt/sts.pdf
Pseudo-Riemannian spin manifolds with many (conformally) Killing spinors
Physicist Figueroa-O'Farrill, Meessen and Philip showed that M-theory backgrounds with more than 24 supersymmetries (= Killing spinors) is locally homogeneous. Note that $ 24= (3/4)N$ where $N = 32$ is the rank of the spinor bundle of the Lorentzian 11-dimensional spin manifold. They conjectured that similar result is valid in other signatures and dimensions. We prove several results of such type using the natural $Spin(V)$-equivariant map $ S \otimes S \to V$ of the tensor square of the spinor $Spin(V)$-module $S$ into vectors. It allows to associate with two Killing spinors a conformal Killing vector or Killing vector. For example, we prove that a pseudo-Riemannian spin-manifold M of signature $(p,q)$ is locally homogeneous if it admits more than $(3/4)N$ ( independent) Killing spinors with the same Killing number, unless $ n = p+q \equiv 1 (mod 4)$ and $ s = p-q \equiv 3 (mod 4)$.
In these exceptional signatures we get a weaker result. In Riemannian and Lorentz cases the result is stronger : $(1/2)N$ Killing spinors are sufficient. We give also a description of (not necessarily complete) Riemannian manifolds admitting Killing spinors, which provides an inductive construction of such manifolds.
Breaking of diffeomorphism symmetry in descrete Gravity
Konforemne twierdzenie Goldberga-Sachsa II
Stron 2 z 3