Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Marcin Kisielowski (IFT UW)
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Krzysztof Meissner Przedstawię rozumowanie wskazujące na proporcjonalność entropii czarnych dziur do ich powierzchni i omówię wyprowadzenie współczynnika ich proporcjonalności
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 16:15

Chun-Yen Lin Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Przemysław Małkiewicz Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Rafał Suszek Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Rafał Suszek Conformal field theories (CFT's), that is field theories with a non-anomalous conformal symmetry are ubiquitous in modern theoretical physics - suffice it to mention the minimal models that capture the dynamics of a large class of lattice theories at criticality, the gauged Wess-Zumino-Witten model that describes the continuum limit of a family of spin-chain models, the non-linear sigma model that defines a vacuum of the critical Polyakov string, or - in space-time dimensions higher than 2 - the supersymmetric gauge theories playing a central role in the AdS/CFT correspondence that provides us with precious insights into the physics of strongly-coupled condensed-matter systems.The above, in conjunction with the rich and much-explored structure, as well as a well-developed methodology of CFT, motivates taking a closer look at its generic features - a task to which the present lectures are devoted. In their course, I shall- introduce the conformal algebra and study its (quantum-)field-theoretic realisations;- indicate certain significant ramifications of conformal symmetry in the quantum theory, such as, e.g., the reconstruction of correlation functions;- briefly discuss the conformal (trace) anomaly.Once the general scheme has been laid out, I shall specialise to the particularly well-studied and important case - that of a CFT on a two-dimensional space-time. In this context, I shall- present the fundamental state-operator correspondence;- set up, using basic operator-algebraic techniques (such as, e.g., the OPE), a Hilbert-space description and embed it in the representation theory of the quantum symmetry algebra - the Virasoro algebra;- briefly discuss the concept of a current-algebra extension of the Virasoro algebra;- review chosen aspects of the conformal-bootstrap programme and address the issue of unitarity.I shall conclude the lectures by giving a long list of scandalous yet unavoidable omissions of topics from the forefront of the current research in the field.
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Jakub Mielczarek Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Romuald Janik Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Katarzyna Rejzner (DESY)
The principle of local covariance was originally proposed in the context of quantum field theory on generic spacetime. Later on it turned out that it can also be used to formulate the requirement of background independence in the perturbative approach to quantum gravity. The idea to formulate gravity in the framework of locally covariant field theory was already applied on the classical level and the perspectives for quantization are very promising. In this talk I will present the recent results in this research area and outline the program for future studies.
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Adam Latosiński (IFT UW)
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Jędrzej Świeżewski (IFT UW)
Teleparallelizm (inaczej zwany TEGR - Teleparallel Equivalent of General Relativity) to sformułowanie teorii grawitacji, które koduje równania Einsteina nie w krzywiźnie koneksji, ale w jej torsji. Podczas mojego wystąpienia sformułuję teorię podobną do TEGR, a następnie przeprowadzę dla niej transformację Legendre'a. Na koniec przeanalizuję otrzymaną algebrę więzów.
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:00

Wojciech Kamiński (IFT UW)
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Marcin Napiórkowski (KMMF UW)
A Hamiltonian defined as a polynomial in creation and annihilation operators is considered. After a minimization of its expectation value over pure Gaussian states, the Hamiltonian is Wick-ordered in creation andannihillation operators adapted to the minimizing state. I will show that this procedure eliminates from the Hamiltonian terms of degree 1 and 2 that do not preserve the particle number, and leaves only the terms thatcan be interpreted as quasiparticles excitations.
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Michał Dziendzikowski (IFT UW)
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Krzysztof A. Meissner (IFT UW)
I will discuss the Schwinger effective action for constant electric andmagnetic fields in QED and its generalization to varying fields.
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Jorma Louko (University of Nottingham)
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Andrzej Dragan (IFT UW)
Single quantum system, such as Unruh-DeWitt detector, can be used to determine absolute acceleration by local measurements on a quantum field. To show this, we consider two kinematically indistinguishable scenarios: an inertial observer, Bob, measuring the field of an uniformly accelerated cavity, and his non-inertial twin Rob accelerating and making measurements in a stationary cavity. We find that these scenarios can be distinguished in the non-relativistic regime only by measurements on highly excited massive fields, allowing one to detect non-inertialness of the reference frame.
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Wojciech Kamiński (IFT UW)
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Marcin Napiórkowski (KMMF UW)
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Wojciech Kamiński (IFT UW)
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Marcin Kaźmierczak (IFT UW)
Standard QFT relies heavily on the Poincare symmetry. This is taken to the extreme in Wigner's definition of particles as unitary irreducible representations of the Poincare group, which is now adopted in many handbooks of QFT, such as the one by Weinberg. Also, more mathematically oriented approaches, e.g. based on Wightman axiomatics, usually use the Poincare symmetry. This state of affairs is unfortunate when one tries to include gravity, in the presence of which the space-time symmetry group may be different from the Poincare, or may not exist at all. Also, when gravity itself is to be quantized in a background independent way, the space-time symmetries cannot be used.It is natural to ask whether it is unavoidable or just convenient to use the Poincare symmetry in QFT. I will present the consequently canonical and Poincare-free quantization of spinor electrodynamics. Some difficulties will appear due to the presence of constraints and spinorial matter. The techniques that will be used to deal with these problems are certainly not a novelty, but they are presented surprisingly rarely in standard treatments of QFT.
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Wojciech Kamiński (IFT UW)
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Jacek Puchta (IFT UW)
Spin Foams is a covariant approach to Loop Quantisation of Gravity. So far it has had some physical predictions such as calculation of graviton propagator. A new model, Dipol Cosmology, is an application of Spin Foams' ideas to the cosmological case. The results are very optymistic, because in the classical limit the evolution of the model gives well known Friedmann equation.
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Przemysław Majewski (KMMF UW)
How to solve evolution equations analytically for a quadratic Hamiltonian with adiabatic factor and the benefits one has from it.
Zapraszamy do Sali Dużej Teoretycznej (229), ul. Hoża 69 o godzinie 14:15

Ryszard Kostecki (IFT UW)