Determination of Lattice QCD Equation of state at a finite chemical potential
Abstract
Exponential resummation to all orders in μB is a promising scheme which can capture contributions to all orders in μB by considering only the first few Taylor coefficients in the Taylor expansion of thermodynamic observables in lattice QCD. This approach however, gets affected by biased estimates of n-point correlation functions Dn whose effects can significantly hinder probe of finite density QCD. We present an unbiased exponential resummation formalism, which can reproduce the Taylor series up to the desired order in μB, besides retaining the original form of the all-order resummation estimate of QCD partition function.
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