Vienna Theory Lunch Seminar by Christopher Lepenik (UV), Maximillian Löschner (UV), Alexander Soloviev (VUT) Tuesdays 12:15-13:30
held alternately at:
We thank our kind sponsors: |
Idee: |
Wie auf vielen Universitäten praktiziert wollen wir ein Lunch-Seminar etablieren, das aktuelle Themen der Theoretischen Physik, die von DiplomandInnen, DoktorandInnen und PostDocs behandelt werden, aufgreift.
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We want to establish a lunch seminar as practiced at other universities. The focus is on recent theoretical research done by Master students, PhDs and PostDocs.
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Wie kann ich teilnehmen? |
Einfach erscheinen! Um per Email informiert zu werden, bitte in die Mailingliste eintragen. |
Just attend! To receive informations via email register for the Mailinglist. |
Oct 11 2016 |
Arjun Bagchi |
Tensionless strings and related fun things I will talk about the formulation of the tensionless limit of closed bosonic and superstring theory from the point of view of worldsheet symmetries. The talk would be based principally on the papers 1507.04361 and 1606.09628. |
Oct 18 2016 |
Prof. Dr. Jörg Schmiedmayer |
Scrambling, Relaxation and the emergence of thermalization in an isolated many body quantum system The evolution of an isolated quantum system is unitary. This is simple to probe for small systems consisting of few non-interacting particles. But what happens if the system becomes large and its constituents interact? In general, one will not be able to follow the evolution of the complex many body eigenstates. Ultra cold quantum gases are an ideal system to probe these aspects of many body quantum physics and the related quantum fields. Our pet systems are one-dimensional Bose-gases. Interfering two systems allows studying coherence between the two quantum fields and the full distribution functions and correlation functions give detailed insight into the many body states and their non-equilibrium evolution. In our experiments we study how the coherence created between the two isolated one-dimensional quantum gases by coherent splitting slowly degrades by coupling to the many internal degrees of freedom available. We find that a one-dimensional quantum system relaxes to a pre-thermalisatized quasi steady state which emerges through a light cone like spreading of ’de-coherence’. The pre-thermalized state is described by a generalized Gibbs ensemble. Finally, we investigate the further evolution away from the pre-thermalized state. On one hand we show that by engineering the Quasiparticles we can create many body quantum revivals. On the other hand, we point to two distinct ways for further relaxation towards a final state that appears indistinguishable from a thermally relaxed state. The system looks like two classically separated objects. This illustrates how classical physics can emerge from unitary evolution of a complex enough quantum system. We conjecture that our experiments points to a universal way through which relaxation in isolated many body quantum systems proceeds if the low energy dynamics is dominated by scrambling of the eigenmodes of long lived excitations (quasi particles). |
Oct 25 2016 |
Benjamin Ramberger |
RPA forces for solids In electronic structure simulations, one is usually interested in the groudstate energy of a many electron system which can often only be calculated approximately. A particular useful method to approximate the energy of a quantum many body system is the random phase approximation (RPA). For many systems it is superior to the widely used density functional theory (DFT), especially when van-der-Waals interactions are important. However, the computational demand for RPA simulations of solids was far out of reach for many years. Fortunately there has been a lot of progress in the development of computer simulations employing the RPA recently, so that RPA-correlation energies became accessible for large systems. For solids however, there is not yet an efficient way to calculate forces in the RPA. Since the calculation of forces is crucial for the simulation of elastic and vibrational properties as well as for structure relaxations, this is a promising area for further investigation. The problem of force calculations within the RPA is adressed by a subproject of the Special Research Program (SFB) Vienna Computational Materials Laboratory (ViCoM) supported by the Austrian Science Fund (FWF). After a general introduction to the topic, the challanges of RPA forces calculations will be discussed and recent results of the project will be presented. |
Nov 1 2016 |
No Lunch Seminar |
Allerheiligen - All Saints' Day |
Nov 8 2016 |
Esteban Castro Ruiz |
Entanglement of quantum clocks through gravity In general relativity, the picture of spacetime for a given observer assigns an ideal clock to each spacetime point. Being ideal, gravitational effects due to these clocks are ignored and the flow of time according to one clock is not affected by the presence of surrounding clocks. However, if time is defined operationally, as a pointer position of a physical clock that obeys the laws of quantum mechanics and general relativity, such a picture is at most a convenient fiction. We show that the mass-energy equivalence implies gravitational interaction between the clocks, while the superposition of energy eigenstates leads to a non-fixed metric background. Based only on the assumption that both quantum mechanics and general relativity are valid in this situation, we show that the clocks necessarily get entangled through time dilation effect, which eventually leads to a loss of coherence of a single clock. Hence, the time as measured by a single clock is not well-defined. However, the general relativistic notion of time is recovered in the classical limit of clocks. |
Nov 15 2016 |
No Lunch Seminar |
Tag des Landespatrons - Day of the Patron Saint of Vienna |
Nov 22 2016 |
Peter Eigenschink |
Global existence for the Einstein-Vlasov System with massive and massless particles The Cauchy problem in general relativity is of fundamental interest. What is known depends crucially on the choice of a reasonable matter model coupled to the Einstein equation. One of the simplest matter models one can choose is Vlasov matter, which represents collisionless gas and is governed by a continuity equation, the Vlasov equation. For a spherically symmetric spacetime and appropriate initial data it is known that for either massive or massless Vlasov matter the Einstein-Vlasov system has global solutions without singularities. But the way those results are obtained are inherently different. For that reason it is of interest if global solutions without singularities also exist in the case of a combination of massive and massless Vlasov matter. We show that for certain initial data, global stability of solutions of the spherically symmetric Einstein-Vlasov system with a combination of both, massive and massless matter, still holds. As an intermediate result, which is crucial for the final conclusion, we also show that for such initial data, massive and massless particles separate after finite time in an appropriate way. |
Nov 29 2016 |
Philipp Kleinert |
Thermalisation of Wightman Two-Point Functions in AdS/CFT In this talk, we will discuss applications of the AdS/CFT correspondence to far-from-equilibrium physics. In the first part, we address the issue of generalizing the holographic dictionary to out-of-equilibrium situations. In the second part, we consider a concrete example of a holographic model of non-equilibrium physics: thermalization following a global quench in 2d CFTs dual to AdS-Vaidya spacetime. At first sight, non-local and local probes in these holographic models of thermalization reach their equilibrium values on very different time scales. As an example of non-local probes, we study the evolution of Wightman two-point functions and show that these two-point functions, after being Fourier transformed to momentum space, decay towards their thermal values with a rate set by the quasinormal modes of the final state black hole spacetime. The quasinormal modes also set the thermalisation time scale of local probes which suggests a unified picture of thermalisation times of one- and two-point functions. Based on: 1412.2806 and 1511.08187 |
Dec 6 2016 |
Carla Schuler & Gabriel Sommer |
Electroweak models with classical scale-invariance We study versions and extensions of the standard model (SM) with classical scale-invariance, which are of great interest nowadays. In these models the Lagrange density does not contain any mass terms, which are responsible for the breakdown of scale-invariance. The generation of the masses of all particles is then described by the Coleman-Weinberg mechanism, where spontaneous symmetry breaking (SSB) occurs as the consequence of quantum corrections rather than the negative Higgs mass term in the Lagrangian. With the particle content of the SM, it is not possible to formulate the SM as a classically scale-invariant theory with the experimentally measured mass values of the Higgs boson and the t-quark. An enlarged SM Higgs-Sector with additional scalar fields and an extension of the SM gauge-group by (non)-Abelian factors provide possible solutions. |
Dec 13 2017 |
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Hilbert Series and SUSY gauge theories The Hilbert series counts gauge invariant chiral operators and encodes information on the moduli space of supersymmetric vacua of a theory. In this talk I will introduce the use of Hilbert series in example of 4d N=1 theories. Thereafter, I proceed to 3d N=4 theories and focus on the Coulomb branch Hilbert series. |
Jan 10 2017 |
Bernadette Kolbinger |
Measuring the Ground State Hyperfine Splitting of Antihydrogen
The ASACUSA (Atomic Spectroscopy And Collisions Using Slow Antiprotons) collaboration at the Antiproton Decelerator at CERN aims to test the CPT symmetry by measuring the ground state hyperfine structure of antihydrogen which, according to the theorem of CPT, is predicted to have the same electromagnetic spectrum as hydrogen. |
Jan 17 2017 |
Friedrich Kupka |
Numerical time integration and studies of stellar convection Convection is one of the main physical mechanisms operating in stars to transport heat and angular momentum, to mix the plasma they consist of, to generate magnetic fields, and to drive and damp global oscillations that are used to study their interior structure. A deeper understanding of the physics of these processes requires numerical simulations and their main challenge is the huge spread of scales in space and time they operate on. After an overview on this basic challenge we report on new numerical methods for efficient and reliable time integration, originally developed for the ANTARES general purpose hydrodynamical simulation code, which are of general use for similar mathematical classes of equations. We demonstrate the versatility of ANTARES with examples from general hydrodynamics, solar physics, and the physics of white dwarf stars. Specifically, these are a demonstration of layer formation in double diffusive flows, how to catch driving and damping of stellar osciallations, and how fluid is mixed by convection into stably stratified regions of a star. Each of these examples is also motivated by explaining the general physical and specific astrophysical interests in underlying questions driving that kind of research. |
Jan 24 2017 |
Prof. Stefan Fredenhagen |
Aspects of higher spins Interacting gauge theories of fields of higher spins are difficult to construct, and the only known examples are the Vasiliev theories. I will try to explain the approach taken in these constructions, in particular the so-called unfolded formulation of the equations of motion. Although the Vasiliev theories in principle provide consistent non-linear systems of higher-spin gauge fields, attempts to extract concrete equations of motion have run into difficulties, and I will sketch some of the resulting conceptual challenges. |
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