Exact Results in Quantum Theory
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
Nonperturbative effects in gauge theories
Background independent quantizations: point polymer quantization of real vector fields
Spacetime Substantivalism and General Relativity. Why four dimensions are probably not enough
TQFTs, State Sums and Geometry, part II
TQFTs, State Sums and Geometry
The EPRL Spinfoam Model, part II
The EPRL Spinfoam Model
Holomorphic families of Shroedinger operators
Decay rates in QED
Reduced phase space quantization applied to cosmology
Quantum fields corresponding to faithful representations of the Poincare group and Poincare gauge theory of gravity II
Quantum group and Hopf algebra symmetries in (2+1)-gravity
Canonical kinematics and dynamics for simplicial geometries
New connections between two- and four-dimensional quantum field theories
Group Field Theory
Fun from none: deformed Fock space and hidden entanglement
Electrically charged quantum particles: a C*-algebraic model
Charged particles cannot be separated from the electromagnetic field surrounding them and, when scattered, they produce long-range radiation. Related to these experimental facts are difficulties in the mathematical modelling of elementary particles like electrons.
A C*-algebraic model of electrons and radiation will be discussed. It avoids the complexity of the full theory, but allows the study of the "dressing" of electrons with the electromagnetic field by an analysis of its representations.
Quantum fields corresponding to faithful representations of the Poincare group and Poincare gauge theory of gravity
In standard quantum field theory, the Hilbert spaces of one-particle states correspond to irreducible unitary representations of the universal covering of the Poincare group, whereas quantum fields are classified by finite-dimensional representations of the universal covering of the Lorentz group. For a given field, these representations need to be connected vie Weinberg consistency conditions. I will investigate the possibility of using finite-dimensional faithful representations of the Poincare group to classify quantum fields. Is it possible to develop a consistent theory of the associated particles? If yes, will they differ from standard ones? This questions will be addressed.
I will also consider the inclusion of gravity, interpreted as a gauge theory of the Poincare group, to the field theories constructed in thisway. The new feature is that the translational gauge fields enter the covariant derivative of matter fields. Also, the so called Poincarecoordinates, that are normally hidden within the cotetrad (together with translational gauge fields) will now manifest themselves explicitly.