What happens to the \( \Upsilon \) and \(\eta_{b}\) in the quark-gluon plasma? Bottomonium spectral functions from lattice QCD

DOI10.1007/JHEP11(2011)103zbMath1306.81318arXiv1109.4496MaRDI QIDQ2261105

Gert Aarts, M. B. Oktay, Jon-Ivar Skullerud, Maria Paola Lombardo, D. K. Sinclair, Chris Allton, Seyong Kim, Sinead M. Ryan

Publication date: 6 March 2015

Published in: Journal of High Energy Physics (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/1109.4496

zbMATH Keywords

lattice QCDthermal field theory

Mathematics Subject Classification ID

Strong interaction, including quantum chromodynamics (81V05) Quantum field theory on lattices (81T25) Statistical mechanics of plasmas (82D10) Thermal quantum field theory (81T28)

Related Items

Heavy quarkonium in extreme conditions, Thermal width and gluo-dissociation of quarkonium in pNRQCD

Cites Work

• The spin-orbit potential and Poincaré invariance in finite temperature pNRQCD
• Gravity dual corrections to the heavy quark potential at finite-temperature
• Continuum and lattice meson spectral functions at nonzero momentum and high temperature
• Heavy quarkonium in a weakly-coupled quark-gluon plasma below the melting temperature