- Letter
- Open Access
Universality driven analytic structure of the QCD crossover: Radius of convergence in the baryon chemical potential
Phys. Rev. D 103, L071501 – Published 14 April, 2021
DOI: https://doi.org/10.1103/PhysRevD.103.L071501
Abstract
Recent lattice QCD calculations strongly indicate that the chiral crossover of QCD at zero baryon chemical potential () is a remnant of the second order chiral phase transition. Universal properties of this second order phase transition can be mapped to QCD temperature and using nonuniversal parameters determined by lattice QCD recently. Motivated by these results, first, we discuss the analytic structure of the partition function in the QCD crossover regime—the so-called Yang-Lee edge singularity—solely based on universal properties. Next, utilizing the lattice QCD results for nonuniversal parameters we map this singularity to the real and complex plane, leading to the determination of the radius of convergence in in the QCD crossover regime. These universality- and QCD-based results provide tight constraints on the range of validity of the lattice QCD calculations at . Implication of this result on the location of the conjectured QCD critical point is discussed.
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References (36)
- A. Bazavov et al. (HotQCD Collaboration), Phys. Lett. B 795, 15 (2019).
- T. Bhattacharya et al., Phys. Rev. Lett. 113, 082001 (2014).
- A. Bazavov et al., Phys. Rev. D 85, 054503 (2012).
- K. Fukushima and T. Hatsuda, Rep. Prog. Phys. 74, 014001 (2011).
- A. Bazavov et al., Phys. Rev. D 95, 054504 (2017).
- C. Bonati, M. D’Elia, M. Mariti, M. Mesiti, F. Negro, and F. Sanfilippo, Phys. Rev. D 92, 054503 (2015).
- R. Bellwied, S. Borsanyi, Z. Fodor, J. Guenther, S. D. Katz, C. Ratti, and K. K. Szabo, Phys. Lett. B 751, 559 (2015).
- S. Borsanyi, Z. Fodor, J. N. Guenther, S. K. Katz, K. K. Szabo, A. Pasztor, I. Portillo, and C. Ratti, J. High Energy Phys. 10 (2018) 205.
- M. A. Stephanov, Phys. Rev. D 73, 094508 (2006).
- G. A. Almsi, B. Friman, K. Morita, and K. Redlich, Phys. Lett. B 793, 19 (2019).
- J. Engels and F. Karsch, Phys. Rev. D 85, 094506 (2012).
- M. E. Fisher, Phys. Rev. Lett. 40, 1610 (1978).
- A. Connelly, G. Johnson, F. Rennecke, and V. Skokov, Phys. Rev. Lett. 125, 191602 (2020).
One cannot completely rule out that QCD demonstrates a weak fluctuation-induced first-order phase transition in the chiral limit for two massless quarks. Current lattice QCD calculations with staggered quarks strongly suggest that the transition is of the second order. We caution the reader that the staggered fermion lattice calculations are known to break down in the chiral limit at finite lattice spacings. The conclusion on the second order chiral phase transition is also consistent with Refs. [15, 16, 17, 18].
- F. Burger, E.-M. Ilgenfritz, M. Kirchner, M. P. Lombardo, M. Mller-Preussker, O. Philipsen, C. Urbach, and L. Zeidlewicz (tmfT), Phys. Rev. D 87, 074508 (2013).
- T. Umeda, S. Ejiri, R. Iwami, K. Kanaya, H. Ohno, A. Uji, N. Wakabayashi, and S. Yoshida, Proc. Sci., LATTICE2016 (2017) 376.
- F. Cuteri, O. Philipsen, and A. Sciarra, Proc. Sci., LATTICE2018 (2018) 170.
- G. Endrodi and L. Gonglach, Proc. Sci., LATTICE2018 (2018) 172.
- H. T. Ding et al., Phys. Rev. Lett. 123, 062002 (2019).
- H. T. Ding, P. Hegde, F. Karsch, A. Lahiri, S. T. Li, S. Mukherjee, and P. Petreczky, Nucl. Phys. A982, 211 (2019).
- S. Ejiri, F. Karsch, E. Laermann, C. Miao, S. Mukherjee, P. Petreczky, C. Schmidt, W. Soeldner, and W. Unger, Phys. Rev. D 80, 094505 (2009).
- O. Kaczmarek, F. Karsch, E. Laermann, C. Miao, S. Mukherjee, P. Petreczky, C. Schmidt, W. Soeldner, and W. Unger, Phys. Rev. D 83, 014504 (2011).
This is the so-called magnetic equation of state for three-dimensional O(4) (Z(2)) universality class if QCD has a second (first) order phase transition in the massless limit for -quarks. The mapping (2) was established for the second order phase transition in the chiral limit. Our analysis however can be extended to a first order phase transition case, if lattice QCD provides nonuniversal input on mapping parameters.
- D. Amit and V. Martin-Mayor, Field Theory, the Renormalization Group, and Critical Phenomena: Graphs to Computers Third Edition (World Scientific, Singapore, 2005).
- S.-T. Li and H.-T. Ding, Proc. Sci., LATTICE2016 (2017) 372.
We can definitively state that the so-called thermal singularities originating from zeroes of the inverse Fermi-Dirac function will not modify our analysis as they lead to the radius of convergence .
It comes with its complex conjugate pair; this is implicitly assumed in the remaining text.
- F. Gliozzi and A. Rago, J. High Energy Phys. 10 (2014) 042.
- C. Itzykson, R. B. Pearson, and J. B. Zuber, Nucl. Phys. B220, 415 (1983).
- E. Brézin and D. J. Wallace, Phys. Rev. B 7, 1967 (1973).
- G. A. Almasi, W. Tarnowski, B. Friman, and K. Redlich, Phys. Rev. D 95, 014007 (2017).
- J. Engels, L. Fromme, and M. Seniuch, Nucl. Phys. B675, 533 (2003).
We thank Anirban Lahiri for providing us this input on behalf of the HotQCD collaboration. Recent results of the HotQCD collaboration on the value of can also be found in Ref. [34].
- D. A. Clarke, O. Kaczmarek, F. Karsch, A. Lahiri, and M. Sarkar, Phys. Rev. D 103, L011501 (2021).
- I. Balog, H. Chaté, B. Delamotte, M. Marohnic, and N. Wschebor, Phys. Rev. Lett. 123, 240604 (2019).
- S. Borsanyi, Z. Fodor, J. N. Guenther, S. K. Katz, A. Pasztor, I. Portillo, C. Ratti, and K. K. Szab, Nucl. Phys. A982, 223 (2019).