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Research paper thumbnail of Lattice QCD thermodynamics in the presence of the charm quark

Nuclear Physics A, 2013

In order to perform a continuum extrapolation for the trace anomaly, defined as I(T ) = T ∂(p/T 4... more In order to perform a continuum extrapolation for the trace anomaly, defined as I(T ) = T ∂(p/T 4 )/∂T , we interpolate the results for the four available lattice spacings, corresponding to N t = 6, 8, 10, 12 by means of a standard cubic spline ansatz. Notice that, with respect to our previous publication [10], a new set of N t = 12 points has been obtained, thereby making a spline interpolation possible. One high-precision point at N t = 16 has been simulated as a further check. We then varied the details of the spline interpolation to account for the statistical 2. Continuum estimate for the N f = 2 + 1 EOS

Research paper thumbnail of Lattice QCD thermodynamics in the presence of the charm quark

Nuclear Physics A, 2013

In order to perform a continuum extrapolation for the trace anomaly, defined as I(T ) = T ∂(p/T 4... more In order to perform a continuum extrapolation for the trace anomaly, defined as I(T ) = T ∂(p/T 4 )/∂T , we interpolate the results for the four available lattice spacings, corresponding to N t = 6, 8, 10, 12 by means of a standard cubic spline ansatz. Notice that, with respect to our previous publication [10], a new set of N t = 12 points has been obtained, thereby making a spline interpolation possible. One high-precision point at N t = 16 has been simulated as a further check. We then varied the details of the spline interpolation to account for the statistical 2. Continuum estimate for the N f = 2 + 1 EOS

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