Phase structure with nonzero ${\Theta }_{\mathrm{QCD}}$ and twisted mass fermions

Abstract

We determine the phase diagram and chiral condensate for lattice QCD with two flavors of twisted-mass fermions in the presence of nondegenerate up and down quarks, discretization errors and a nonzero value of ${\Theta }_{\mathrm{QCD}}$. Although such a theory has a complex action and cannot, at present, be simulated, the results are needed to understand how to tune to maximal twist in the presence of electromagnetism, a topic discussed in a companion paper. We find that, in general, the only phase structure is a first-order transition of finite length. Pion masses are nonvanishing throughout the phase plane except at the endpoints of the first-order line. Only for extremal values of the twist angle and ${\Theta }_{\mathrm{QCD}}$ ($\omega =0$ or $\pi /2$ and ${\Theta }_{\mathrm{QCD}}=0$ or $\pi$) are there second-order transitions.

11 pages, 6 figures Introduction expanded, results unchanged, consistent with published version

References in corpus (3)

• Ab initio calculation of the neutron-proton mass difference
• Phase diagram of non-degenerate twisted mass fermions
• Impact of electromagnetism on phase structure for Wilson and twisted-mass fermions including isospin breaking

Cited by in corpus (2)

• Phase Diagram of Dynamical Twisted Mass Wilson Fermions at Finite Isospin Chemical Potential
• Phase ambiguity of the measure for continuum Majorana fermions