Lattice-based QCD equation of state at finite baryon density: Cluster Expansion Model
arXiv:1807.06472 · doi:10.1016/j.nuclphysa.2018.10.068
Abstract
The QCD equation of state at finite baryon density is studied in the framework of a Cluster Expansion Model (CEM), which is based on the fugacity expansion of the net baryon density. The CEM uses the two leading Fourier coefficients, obtained from lattice simulations at imaginary , as the only model input and permits a closed analytic form. Excellent description of the available lattice data at both and at imaginary is obtained. We also demonstrate how the Fourier coefficients can be reconstructed from baryon number susceptibilities.
4 pages, 3 figures. Contribution to the Quark Matter 2018 conference proceedings
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- Lattice-based equation of state at finite baryon number, electric charge and strangeness chemical potentials
- QCD Equation of State at Finite Chemical Potentials for Relativistic Nuclear Collisions
- High-Temperature QCD: theory overview
- Lattice Constraints on the QCD Chiral Phase Transition at Finite Temperature and Baryon Density
- The fate of the critical endpoint at large
- The analytic structure of thermodynamic systems with repulsive interactions
- Critical point signatures in the cluster expansion in fugacities
- Net-baryon multiplicity distribution consistent with lattice QCD
- Lattice-based equation of state with a critical point from constant entropy contours and its comparison to effective QCD approaches
- Finite-size effects and scaling properties of chiral and baryon-number fluctuations
- Net-Baryon Number Probability Distribution As an Indicator of Phase Transition