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The QCD crossover temperature and curvature coefficient from unbiased exponential resummation at physical quark masses in (2+1)-flavor lattice QCD

Published 19 Aug 2026 in hep-lat, hep-ph, hep-th, nucl-ex, and nucl-th | (2608.19330v1)

Abstract: We present the first application of the unbiased exponential resummation method to the determination of the QCD pseudocritical temperature TpcT_{\rm pc} at vanishing baryon chemical potential μ<em>Bμ<em>B. By reconstructing the finite-density baryon number susceptibility χ2<sup>Bχ_2<sup>B, we define two thermal-derivative observables whose peak positions yield T</em>pc<sup>T=160.2(4)(3)T</em>{\rm pc}<sup>T=160.2(4)(3) MeV and Tpc<sup>C=158.1(5)(3)T_{\rm pc}<sup>C=158.1(5)(3) MeV. We also show that the pseudocritical temperature, Tpc<sup>χT_{\rm pc}<sup>χ obtained from the peak of the fourth-order baryon number susceptibility χ4<sup>Bχ_4<sup>B is consistent with these determinations and with previous lattice-QCD results based on Taylor expansions \cite{Bollweg:2022Pade}. Further, we demonstrate that scaling relations \cite{Bollweg:2022fqq} between χ4<sup>Bχ_4<sup>B and the thermal derivatives of χ2<sup>Bχ_2<sup>B yield mutually consistent estimates of the leading second order curvature coefficient κ2<sup>Bκ_2<sup>B at the corresponding pseudocritical temperatures. A direct analysis of the μBμ_B dependence of the pseudocritical temperatures provides an independent but substantially less constrained determination of the curvature, which remains statistically consistent with the scaling-based estimates. These results demonstrate the consistency of unbiased exponential resummation with the expected scaling behavior and establish it as a complementary approach for probing the QCD crossover at small finite baryon density.

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