Abstract

Quark-hadron continuity with two-flavor quarks that was proposed recently connects hadronic matter with neutron $^3P_2$ superfluidity and two-flavor dense quark matter. This two-flavor dense quark phase consists of the coexistence of the 2SC condensates and the $P$-wave diquark condensates of $d$-quarks, which gives rise to color superconductivity as well as superfluidity. We classify vortices in this phase. The most stable vortices are what we call the non-Abelian Alice strings, which are superfluid vortices with non-Abelian color magnetic fluxes therein, exhibiting so-called topological obstruction, or a non-Abelian generalization of the Alice property. We show that a single Abelian superfluid vortex is unstable against decay into three non-Abelian Alice strings. We discover that a non-Abelian Alice string carries orientational moduli of the real projective space $\mathbb{R}P^2$ corresponding to the color flux therein in the presence of the $P$-wave condensates alone. We calculate Aharanov-Bohm (AB) phases around the non-Abelian Alice string, and find that the 2SC condensates and string's orientational moduli must be aligned with each other because of single-valuedness of the AB phases of the 2SC condensates.

Highlights

  • Color superconductor is the ground state of the cold QCD matter at densities much higher than that of saturated nuclei n0 1⁄4 0.16 fm−3; the only known circumstance where we might find such kind of matter is in the core of neutron stars [1]

  • Various phases are known for color superconductivity such as color-flavor locked (CFL) phase [2] in three-flavor symmetric matter and 2-flavor superconducting (2SC) phase [3,4] in two-flavor symmetric matter

  • In the CFL phase, topologically stable superfluid vortex comes about owing to the nontrivial first homotopy group π11⁄2Uð1ÞBŠ 1⁄4 Z [6,7]. It is related with the broken Uð1ÞB symmetry in the CFL phase, which is possible as the Vafa-Witten theorem does not apply at finite density [8]

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Summary

INTRODUCTION

Color superconductor is the ground state of the cold QCD matter at densities much higher than that of saturated nuclei n0 1⁄4 0.16 fm−3; the only known circumstance where we might find such kind of matter is in the core of neutron stars [1]. The recent insights from the neutron star observations, lead to the novel phase of color superconductivity in two-flavor matter with the broken Uð1ÞB symmetry [26] This phase is called the 2SC þ hddi phase. We describe that the most stable vortices in the hddi phase are non-Abelian vortices, which support 1=3 fractional windings in Uð1ÞB as well as the color-magnetic fluxes similar to those in the CFL phase These vortices exhibit the unique features akin to the so-called Alice strings [40,41,42,43,44,45,46,47,48,49,50], we named them as “non-Abelian Alice strings”.

TWO-FLAVOR DENSE QUARK MATTER
Symmetry of the color-superconducting phase
Symmetry breaking by the hddi condensate
Symmetry breaking by the 2SC condensate
The opposite ordering
MINIMAL TOPOLOGICAL VORTEX IN hddi PHASE–NON-ABELIAN ALICE STRING
Abelian vortex The simplest vortex is a superfluid vortex of the form
Pure color flux tubes
Non-Abelian Alice strings
Topological obstruction of a non-Abelian Alice string
Generalized Aharonov-Bohm phases around vortices
Abelian string
Non-Abelian Alice string
Decay of an Abelian Uð1ÞB vortex
Single non-Abelian Alice string
CONSISTENCY WITH THE OPPOSITE ORDERING IN THE SYMMETRY BREAKING
Superfluid vortex The simplest vortex is a superfluid vortex of the form
SUMMARY AND DISCUSSIONS
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