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<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/"><rdf:Description rdf:about="https://repozitorij.uni-lj.si/IzpisGradiva.php?id=165161"><dc:title>How Gubser flow ends in a holographic conformal theory</dc:title><dc:creator>Banerjee,	Avik	(Avtor)
	</dc:creator><dc:creator>Mitra,	Toshali	(Avtor)
	</dc:creator><dc:creator>Mukhopadhyay,	Ayan	(Avtor)
	</dc:creator><dc:creator>Soloviev,	Alexander	(Avtor)
	</dc:creator><dc:subject>relativistic hydrodynamics</dc:subject><dc:subject>Gubser flow</dc:subject><dc:description>Gubser flow is an axis-symmetric and boost-invariant evolution in a relativistic quantum field theory which is best studied by mapping $\bf{R}$$^{3,1}$ to $dS_3 \times \bf{R}$ when the field theory has conformal symmetry. We show that at late de-Sitter time, which corresponds to large proper time and central region of the future wedge within $\bf{R}$$^{3,1}$, the holographic conformal field theory plasma can reach a state in which $\epsilon = P_T = - P_L$, with $\epsilon$, $P_T$  and $P_L$ being the energy density, transverse and longitudinal pressures, respectively. We further determine the full sub-leading behaviour of the energy–momentum tensor at late time. Restricting to flows in which the energy density decays at large transverse distance from the central axis in $\bf{R}$$^{3,1}$, we show that this decay should be faster than any power law. Furthermore, in this case the energy density also vanishes in $\bf{R}$$^{3,1}$ faster than any power as we go back to early proper time. Hydrodynamic behavior can appear in intermediate time.</dc:description><dc:date>2024</dc:date><dc:date>2024-11-25 14:25:38</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>165161</dc:identifier><dc:language>sl</dc:language></rdf:Description></rdf:RDF>
