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Review of the EFT treatment of quarkonium at finite temperature
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Heavy quarkonium is one of the most investigated probes of the medium produced in heavy-ion collisions. In the past few years progress has been made in the description of its in-medium dynamics from QCD. Non-relativistic EFTs in particular allow one to define and compute rigorously the potential governing the real-time evolution of the bound state from QCD, showing that it is composed of a real and an imaginary part. The latter encodes the effect of scattering with the light constituents of the plasma and is oftentimes responsible for the dissociation of the bound state. The EFT approach and its main results, as well as comparisons with recent lattice data and phenomenological applications, are briefly reviewed here.
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Quantum simulation of bottomonium dynamics in the quark-gluon plasma via the Lindblad equation
A quantum circuit simulation of the next-to-leading-order Lindblad equation for bottomonium in the quark-gluon plasma matches QuTiP and finds a small color-octet contribution to the Upsilon(1S) survival probability.
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