Abstract
We study the phase diagram of two-flavor massless two-color QCD (QC$_2$D) under the presence of quark chemical potentials and imaginary isospin chemical potentials. At the special point of the imaginary isospin chemical potential, called the isospin Roberge--Weiss (RW) point, two-flavor QC$_2$D enjoys the $\mathbb{Z}_2$ center symmetry that acts on both quark flavors and the Polyakov loop. We find a $\mathbb{Z}_2$ 't Hooft anomaly of this system, which involves the $\mathbb{Z}_2$ center symmetry, the baryon-number symmetry, and the isospin chiral symmetry. Anomaly matching, therefore, constrains the possible phase diagram at any temperatures and quark chemical potentials at the isospin RW point, and we compare it with previous results obtained by chiral effective field theory and lattice simulations. We also point out an interesting similarity of two-flavor massless QC$_2$D with $(2+1)$d quantum anti-ferromagnetic systems.
Highlights
Quantum chromodynamics (QCD) is the fundamental theory of nuclear and hadron physics, and it provides various interesting phenomena in extreme conditions [1]
Since the system is strongly coupled in most regions of the QCD phase diagram, we should rely on the numerical lattice Monte Carlo simulation in order to obtain concrete understandings both qualitatively and quantitatively
We find the Z2 anomaly related to this center symmetry and chiral symmetry, and we discuss its implications to the finite-density phase diagram at the isospin RW point
Summary
Quantum chromodynamics (QCD) is the fundamental theory of nuclear and hadron physics, and it provides various interesting phenomena in extreme conditions [1]. We study the phase diagram of massless two-flavor QC2D in detail at finite quark chemical potentials and imaginary isospin chemical potentials This setup does not suffer from the sign problem, so our predictions can be confirmed by lattice Monte Carlo simulations. In this setup, as we shall reveal in this paper, we can discuss the spontaneous breaking of the center, chiral, and baryon-number symmetries, and the corresponding order parameters are given by the Polyakov loop P , the chiral condensate qq , and the diquark condensate qq , respectively.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.