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
2013-05-24 (Piątek)
Emanuele Alesci
Quantum reduced loop gravity
2013-04-26 (Piątek)
prof. Jerzy Lewandowski (IFT UW)
Geometry and evolution of the Hamiltonian constrained systems
2013-04-19 (Piątek)
Mehdi Assanioussi
Quantum Ricci scalar operator in LQG
2013-04-12 (Piątek)
prof. Krzysztof A. Meissner (IFT UW)
The De Witt equation
2013-04-05 (Piątek)
Karol K. Kozłowski (CNRS Dijon)
Asymptotic behaviour of beta ensambles
Random matrices first arose in the works of Wishart in the late 1920s. Later, in the mid-1950s, Wigner introduced them as a tool for modelling spectra of heavy nuclei. Since then, these objects have appeared in many other branches of mathematics and physics and have been observed to have many more applications, such as to combinatorial problems of counting various types of graphs. One may consider various types of random matrices, the simplest model having a single random matrix satisfying certain symmetry conditions such as being real, symmetric or hermitian. The study of statistical properties of such random matrix ensembles boils down to the analysis of certain N-fold integrals, N being the size of the square matrix. In fact, these integrals belong to the class of so-called ß-ensemble integrals, which can be thought of as representing the partition function of a one-dimensional Coulomb gas subject to an external potential V. Indeed, at specific values of the parameter ß, to wit, ß=1,2,4, one recovers the non-trivial part of partition functions associated with the so-called matrix model subordinate to the symmetric (the orthogonal ensemble), hermitian (the unitary ensemble) and hermitian self-dual (the symplectic ensemble) random matrices. Most of the information of interest to matrix models (and ß-ensembles) is related to the large-N behaviour. Therefore, its extraction demands analysing the N ? behaviour of N-fold integrals. Introducing modern methods allowing one to carry out this sort of asymptotic analysis is the very purpose of these lectures. I shall commence by introducing the ß-ensembles and discussing their relation, for ß=1,2,4, to the aforementioned matrix ensembles. I shall then make a few heuristic connections between partition functions of matrix models and enumeration problems of graphs drawn on surfaces with prescribed genera. Next, I shall proceed by entering deeper into the subject; namely, by introducing the various concepts and tools allowing one to set a convenient framework for carrying out the large-N asymptotic analysis. I shall begin by discussing certain general topological properties of spaces of probability measures over Polish spaces. This will enable me to introduce the concept of large deviations for sequences of probability measures as well as to prove various crucial theorems relevant to these constructions. At that very point, I shall be able to explain how the framework can be utilised as a powerful tool for computing the leading large-N asymptotic behaviour of the ß-ensemble integrals. Time permitting, I shall briefly expand upon techniques allowing one to compute subdominant large-N asymptotics.
2013-03-22 (Piątek)
Karol K. Kozłowski (CNRS Dijon)
Asymptotic behaviour of beta ensambles III
Random matrices first arose in the works of Wishart in the late 1920s. Later, in the mid-1950s, Wigner introduced them as a tool for modelling spectra of heavy nuclei. Since then, these objects have appeared in many other branches of mathematics and physics and have been observed to have many more applications, such as to combinatorial problems of counting various types of graphs. One may consider various types of random matrices, the simplest model having a single random matrix satisfying certain symmetry conditions such as being real, symmetric or hermitian. The study of statistical properties of such random matrix ensembles boils down to the analysis of certain N-fold integrals, N being the size of the square matrix. In fact, these integrals belong to the class of so-called ß-ensemble integrals, which can be thought of as representing the partition function of a one-dimensional Coulomb gas subject to an external potential V. Indeed, at specific values of the parameter ß, to wit, ß=1,2,4, one recovers the non-trivial part of partition functions associated with the so-called matrix model subordinate to the symmetric (the orthogonal ensemble), hermitian (the unitary ensemble) and hermitian self-dual (the symplectic ensemble) random matrices. Most of the information of interest to matrix models (and ß-ensembles) is related to the large-N behaviour. Therefore, its extraction demands analysing the N ? behaviour of N-fold integrals. Introducing modern methods allowing one to carry out this sort of asymptotic analysis is the very purpose of these lectures. I shall commence by introducing the ß-ensembles and discussing their relation, for ß=1,2,4, to the aforementioned matrix ensembles. I shall then make a few heuristic connections between partition functions of matrix models and enumeration problems of graphs drawn on surfaces with prescribed genera. Next, I shall proceed by entering deeper into the subject; namely, by introducing the various concepts and tools allowing one to set a convenient framework for carrying out the large-N asymptotic analysis. I shall begin by discussing certain general topological properties of spaces of probability measures over Polish spaces. This will enable me to introduce the concept of large deviations for sequences of probability measures as well as to prove various crucial theorems relevant to these constructions. At that very point, I shall be able to explain how the framework can be utilised as a powerful tool for computing the leading large-N asymptotic behaviour of the ß-ensemble integrals. Time permitting, I shall briefly expand upon techniques allowing one to compute subdominant large-N asymptotics.
2013-03-15 (Piątek)
Adam Latosiński (IFT UW)
Problems with unitary gauge
2013-03-08 (Piątek)
Antonio Vassallo (Instytut Filozofii UW)
From Bohmian Mechanics to Bohmian Quantum Gravity
Bohmian mechanics represents an effective physical implementation of the bare formalism of quantum mechanics. It is a deterministic but non-local hidden variables theory which is able to reproduce all the empirical predictions of quantum mechanics. Moreover, Bohmian mechanics avoids all the interpretational drawbacks of the standard Copenhagen interpretation of quantum mechanics by providing a simple explanation for the appearance of wave-function collapses, superpositions and fluctuations at the quantum level.In this talk, I will consider the possibility of extending the Bohmian approach to the canonical quantum gravity programme and I will sketchhow a hypothetical theory of Bohmian quantum gravity should looklike. In the end, I will propose a straightforward interpretation ofthis theory which is able to overcome many conceptual problems related to the disappearance of spacetime at the Planck scale and its re-emergence in the continuum limit.
2013-03-01 (Piątek)
Jacek Kasprzak (Institut Neel, CNRS)
On the quantum light-matter coupling in a semiconductor nanostructure
Milestone achievements in cavity quantum electrodynamics (cQED) have just been awarded with the Nobel prize in physics [1]. The underlying experiments were performed on individual atomic systems exploring light-matter interaction on a quantum level [2]. cQED effects can now be observed also in solid state systems, which owing to their intrinsicstability are better suited for a scalable technology and commercialization. When a single bosonic mode strongly couples to a single fermionic mode, a Jaynes-Cummings (JC) ladder is formed. This is realized here by combining photons confined in a micropillar cavity [3] with a single exciton (electron-hole pair bound by their electrostatic attraction), so as tocreate dressed states called polaritons.In this talk, I will present the measurements and modeling of the coherent anharmonic response of this strongly-coupled exciton-cavity system at resonance. Injecting two photons into the cavity, we demonstrate a \sqrt{2} larger polariton splitting with respect to the vacuum Rabi splitting [3]. This is achieved using coherent nonlinear spectroscopy, specif-ically four-wave mixing (FWM) [4], where the coherence between ground state and first (second) rung of the JC ladder can be interrogated for positive (negative) delays between laser pulses driving the FWM signal.As an outlook, I will highlight our recent spectroscopic studies of a multiexciton-cavity system, enabling pioneering investigations of its Tavis-Cummings physics [5] and thus paving the way towards long-range radiative coupling in a solid.[1] S. Haroche and D. J. Wineland[2] M. Brune et al Phys. Rev. Lett. 76 1800 (1996)[3] J. Kasprzak et al. Nature Mater. 9, 304 (2010).[4] W. Langbein and B. Patton Opt. Lett. 31, 1738 (2006)[5] F. Albert et al. Nature Comm. (2013)
2013-02-22 (Piątek)
dr Przemysław Małkiewicz (NCBJ)
Wavelet quantum cosmology
2013-01-25 (Piątek)
Tomasz Pawłowski (KMMF UW)
Computable framework of Loop Quantum Gravity
I will present a framework of a non-perturbative quantization of general relativity coupled to dust and other matter fields. The irrotational dust provides a natural time variable, leading to a physical Hamiltonian with spatial diffeomorphism symmetry. The surprising feature is that the Hamiltonian is not a square root. This property, together with the kinematical structure of loop quantum gravity, provides a complete theory of quantum gravity with strict control over the physical Hilbert space, action of the Hamiltonian on it and the construction of physical observables. This puts in technical reach applications to cosmology, quantum gravitational collapse and Hawking radiation.
2013-01-18 (Piątek)
prof. Piotr Chankowski (IFT UW)
Baryogenesis
I will first briefly overview possible mechanismsof the cosmological baryon number generationand then will describe an extension of the standardmodel which allows for baryon number generationduring the electroweak phase transistion.
2013-01-11 (Piątek)
prof. Krzysztof A. Meissner (IFT UW)
Axions
I will discuss theoretical motivations for the existence ofaxions as well as reasons why they are natural Cold DarkMatter candidates. I will describe how the weakness of their couplingsis naturally explained within the Conformal Standard Model by thesmallness of neutrino masses.
2012-12-14 (Piątek)
Wojciech Kamiński (IFT UW)
Asymptotics of 6j symbols (part II)
Wigner 6j symbols are defined in terms of recoupling theory forrepresentations of SU(2). They exhibit surprising connections tothe geometry of tetrahedra and disctete 3d gravity (Regge action) in thelarge spin limit. I will present a simple proof of this fact due to L. Charles by the methods of geometric quantization and explain its (conjectured) extensionto the case of quantum SU_q(2), where similar asymptotics are also known.
2012-12-07 (Piątek)
Michał Oszmaniec (CFT PAN)
Justification of statistical mechanics for systems described by finite dimensional Hilbert spaces
In the talk I will present the survey of recent results concerning the justification of statistical mechanics for systems described by finite dimensional Hilbert spaces. Theorems I will discuss take their origin in the early paper of John von Neumann from 1929. Yet, they use tools of modern mathematics: Lie groups, homogeneous spaces and the phenomenon of concentration of measure. A the beginning I shall introduce the necessary mathematics that in the latter part will allow me to state the theorems in the compact and clear fashion.
2012-11-30 (Piątek)
Wojciech Kamiński (IFT UW)
Asymptotics of 6j symbols
Wigner 6j symbols are defined in terms of recoupling theory for representations of SU(2). They exhibit surprising connections to the geometry of tetrahedra and disctete 3d gravity (Regge action) in the large spin limit. I will present a simple proof of this fact due to L. Charles by the methods of geometric quantization and explain its (conjectured) extension to the case of quantum SU_q(2), where similar asymptotics are also known.
2012-11-23 (Piątek)
Przemysław Majewski (KMMF UW)
Conformal actions, Kummer tables and hypergeometric-type functions
The aim of the talk is to show how the action of the symmetry group SO(6,C) and the choice of a nice set of parameters help one to understand and present logically a whole bunch of special functions.
2012-11-16 (Piątek)
Igor Khavkine
Time delay in classical and quantum gravity
A class of diffeomorphism invariant, physical observables, so-called astrometric observables, is introduced. A particularly simple example, the time delay, which expresses the difference between two initially synchronized proper time clocks in relative inertial motion, is analyzed in detail. It is found to satisfy some interesting inequalities related to the causal structure of classical Lorentzian spacetimes. Thus it can serve as a probe of causal structure and in particular of violations of causality. A quantum model of this observable as well as thecalculation of its variance due to vacuum fluctuations in quantum linearizedgravity are sketched. The question of whether the causal inequalities are still satisfied by quantized gravity, which is pertinent to the nature of causality in quantum gravity, is raised, but it is shown that perturbative calculations cannot provide a definite answer. Some potential applications of astrometric observables in quantum gravity are discussed.[arXiv:1111.7127]
2012-10-26 (Piątek)
Jacek Puchta (IFT UW)
Amplituda przejścia w pianach spinowych - lorentzowski model EPRL
Transition Amplitudes in spin-foams - Lorentzian EPRL model
Model EPRL pozwala na obliczanie amplitud przejścia dla kwantowychhistorii pola grawitacyjnego w teorii pian spinowych. Model ten madwie wersje: euklidesową - zdefiniowaną na grupie SO(4), orazlorentzowską - zdefiniowaną na grupie SL(2,C). Dotychczas większośćrachunków przeprowadzonych zostało w pierwszym podejściu.W moim wystąpieniu przedstawię lorentzowski model EPRL, wprowadzającniezbędne aspekty reprezentacji unitarnych grupy SL(2,C), a następnieprzedstawię pewne techniczne problemy występujące przy typowychrachunkach w tym modelu.
2012-10-19 (Piątek)
Adam Torenc
Topological invariants of 3-manifolds and quantum gravity in 3D
2012-10-12 (Piątek)
Marcin Napiórkowski (KMMF UW)
Free Energy Functional of Interacting Bose Gas
2012-10-05 (Piątek)
prof. Jerzy Lewandowski (IFT UW)