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Raphaelle Bailhache (TU Darmstadt)14/11/2022, 16:45CONTRIBUTED TALK (25min +5)
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Julian Schmitt (University of Bonn)14/11/2022, 17:15CONTRIBUTED TALK (25min +5)
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Dr Keisuke Fujii (Institute for Theoretical Physics, Heidelberg University)14/11/2022, 17:45CONTRIBUTED TALK (25min +5)
The force between particles is one of the most elementary concepts from condensed-matter physics to high-energy physics. Not only the fundamental interaction mediated by gauge bosons but also the induced interaction between quasiparticles plays an essential role in modern physics.
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Recently, impurities in superfluids, called polarons, have been attracting much attention in ultracold atom... -
Felix Karbstein (Helmholtz Instiute Jena)17/11/2022, 14:30CONTRIBUTED TALK (25min +5)
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Jasmine Brewer (CERN)17/11/2022, 15:00CONTRIBUTED TALK (25min +5)
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Mr Thimo Preis (Heidelberg University )17/11/2022, 15:30CONTRIBUTED TALK (25min +5)
We study the dynamics of perturbations around nonthermal fixed points associated to universal scaling phenomena in quantum many-body systems far from equilibrium. For an N -component scalar quantum field theory in 3+1 space-time dimensions, we determine the stability scaling exponents using a self-consistent large-N expansion to next-to-leading order. Our analysis reveals the presence of both...
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Esther Menz (Helmholtz Institute Jena)18/11/2022, 09:00CONTRIBUTED TALK (25min +5)
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Mr Andreas Kirchner (ITP Heidelberg)18/11/2022, 09:30CONTRIBUTED TALK (25min +5)
It is well established that the late states of a high energy nuclear collision can be described in terms of relativistic fluid dynamics. An open problem in this context is how the actual collision and the early time dynamics directly after it can be described. Phenomenological models are currently employed here and they have several parameters that need to be fitted to experimental data.
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Using... -
Bastian Sikora (Max Planck Institute for Nuclear Physics)18/11/2022, 10:00CONTRIBUTED TALK (25min +5)
In an external magnetic field, the ground state of the $^3$He$^+$ ion is split into into four sublevels due to the combined hyperfine splitting and Zeeman effect. By measuring transition frequencies between these sublevels, it is possible to determine the $g$-factor of the bound electron, the ground-state hyperfine splitting as well as the shielded magnetic moment of the nucleus [1].
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