Abstract

We find a novel confinement mechanism in the two-flavor dense quark matter proposed recently, that consists of the 2SC condensates and the P-wave diquark condensates of d-quarks. This quark matter exhibiting color superconductivity as well as superfluidity is classified into two phases; confined and deconfined phases of vortices. We establish that the criterion of the confinement is color neutrality of Aharonov-Bohm (AB) phases: vortices exhibiting color non-singlet AB phases are confined by the so-called AB defects to form color-singlet bound states. In the deconfined phase, the most stable vortices are non-Abelian Alice strings, which are superfluid vortices with fractional circulation and non-Abelian color magnetic fluxes therein, exhibiting color non-singlet AB phases. On the other hand, in the confined phase, these non-Abelian vortices are confined to either a baryonic or mesonic bound state in which constituent vortices are connected by AB defects. The baryonic bound state consists of three non-Abelian Alice strings with different color magnetic fluxes with the total flux canceled out connected by a domain wall junction, while the mesonic bound state consists of two non-Abelian Alice strings with the same color magnetic fluxes connected by a single domain wall. Interestingly, the latter contains a color magnetic flux in its core, but this can exist because of color neutrality of its AB phase.

Highlights

  • Color confinement is one of the most challenging unsolved problems in modern high energy physics

  • The baryonic bound state consists of three non-Abelian Alice strings with different color magnetic fluxes with the total flux canceled out connected by a domain wall junction, while the mesonic bound state consists of two non-Abelian Alice strings with the same color magnetic fluxes connected by a single domain wall

  • The baryonic bound state consists of three non-Abelian Alice strings with different color magnetic fluxes with the total flux canceled out, which are connected by a domain wall junction

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Summary

Introduction

Color confinement is one of the most challenging unsolved problems in modern high energy physics. In the CFL phase, Abelian superfluid vortices exist as the topologically stable configuration due to the nontrivial homotopy group π1[U(1)B] = Z [57, 58] This is unstable against a decay into a triad of more stable vortices [59,60,61], which are non-Abelian vortices with color magnetic fluxes and fractional circulation of the Abelian vortices [56, 59, 62,63,64]. We show that in the confined phase, these non-Abelian vortices are confined to either a baryonic or mesonic bound state in which constituent vortices are connected by AB defects [19,20,21] that appear to compensate nontrivial color non-singlet (generalized) AB phases of the 2SC condensates around vortices. The mesonic bound state consists of two non-Abelian Alice strings with the same color magnetic fluxes connected by a single domain wall. In appendix B, we summarize the derivation of generalized AB phases

Two-flavor dense quark matter
Symmetry breaking by the dd condensate
Symmetry breaking by the 2SC condensate
The opposite ordering of symmetry breakings
Topological vortices in dd phase
Non-Abelian Alice strings
Doubly-wound non-Abelian strings
Generalized Aharonov-Bohm phases
Vortex confinement
Aharonov-Bohm defects in 2SC condensate Φ2SC
Baryonic molecule
Mesonic molecule
Baryons-to-mesons decay
Consistency with the opposite ordering in the symmetry breaking
Superfluid vortex The configuration of a superfluid vortex is
Summary and discussions
A Pure color flux tubes
B Generalized Aharonov-Bohm phases around vortices
Aharonov-Bohm phase around Abelian superfluid strings
Aharonov-Bohm phase around pure color flux tubes
Aharonov-Bohm phase around non-Abelian Alice strings
Aharonov-Bohm phase around doubly-wound non-Abelian strings
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