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
2011-06-24 (Piątek)
Marcin Kisielowski (IFT UW)
Spin Foams encoded in Operator Spin Network Diagrams
2011-06-03 (Piątek)
Krzysztof Meissner
Entropia czarnych dziur
Przedstawię rozumowanie wskazujące na proporcjonalność entropii czarnych dziur do ich powierzchni i omówię wyprowadzenie współczynnika ich proporcjonalności
Chun-Yen Lin
Gravity from Loop Quantum Gravity
2011-05-27 (Piątek)
Przemysław Małkiewicz
The reduced phase space approach to the Kasner universe and the problem of time
2011-05-20 (Piątek)
Rafał Suszek
An introduction to Conformal Field Theory II
2011-05-13 (Piątek)
Rafał Suszek
An introduction to Conformal Field Theory I
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.
2011-04-29 (Piątek)
Jakub Mielczarek
Anomaly-free perturbations in loop quantum cosmology
2011-04-15 (Piątek)
Romuald Janik
Całkowalność w korespondencji AdS/CFT - wprowadzenie
2011-04-08 (Piątek)
Katarzyna Rejzner (DESY)
Local covariance principle and perspectives in quantum gravity
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.
2011-04-01 (Piątek)
Adam Latosiński (IFT UW)
Lagranżjan Heisenberga-Eulera w granicy silnego pola
2011-03-25 (Piątek)
Jędrzej Świeżewski (IFT UW)
Między ogólną teorią względności a elektrodynamiką - hamiltonowski opis pewnej teorii pola
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.
2011-03-18 (Piątek)
Wojciech Kamiński (IFT UW)
Własności spektralne operatorów Jacobiego
2011-02-25 (Piątek)
Marcin Napiórkowski (KMMF UW)
On the minimization of Hamiltonians over pure Gaussian states
A Hamiltonian defi ned 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.
2011-02-18 (Piątek)
Michał Dziendzikowski (IFT UW)
Geometric framework for constrained hamiltonian systems
2011-01-21 (Piątek)
Krzysztof A. Meissner (IFT UW)
Light on light scattering in QED
I will discuss the Schwinger effective action for constant electric andmagnetic fields in QED and its generalization to varying fields.
2011-01-14 (Piątek)
Jorma Louko (University of Nottingham)
How often does an accelerated particle detector click?
2011-01-07 (Piątek)
Andrzej Dragan (IFT UW)
Quantum accelerometer
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.
2010-12-17 (Piątek)
Wojciech Kamiński (IFT UW)
Renormalization and microlocal analysis
2010-12-03 (Piątek)
Marcin Napiórkowski (KMMF UW)
A simplified proof of the stability of matter, part II
2010-11-19 (Piątek)
Wojciech Kamiński (IFT UW)
Diagramy Younga i reprezentacje grup Sl(n,C)
2010-11-05 (Piątek)
Marcin Kaźmierczak (IFT UW)
Is it necessary to employ the Poincare invariance when quantizing electrodynamics with fermionic matter?
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.
2010-10-29 (Piątek)
Wojciech Kamiński (IFT UW)
All the 3-connected relativistic BC and EPRL spin-networks are integrable
2010-10-22 (Piątek)
Jacek Puchta (IFT UW)
Vacuum Friedmann equation out of Spin Foams
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.
2010-10-15 (Piątek)
Przemysław Majewski (KMMF UW)
Exact solutions for Quantum Field Theory with certain quadratic Hamiltonian
How to solve evolution equations analytically for a quadratic Hamiltonian with adiabatic factor and the benefits one has from it.
2010-10-08 (Piątek)
Ryszard Kostecki (IFT UW)