Phase diagram of QCD matter with magnetic field: domain-wall Skyrmion chain in chiral soliton lattice

Abstract QCD matter in strong magnetic field exhibits a rich phase structure. In the presence of an external magnetic field, the chiral Lagrangian for two flavors is accompanied by the Wess-Zumino-Witten (WZW) term containing an anomalous coupling of the neutral pion π 0 to the magnetic field via th...

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Main Authors: Minoru Eto, Kentaro Nishimura, Muneto Nitta
Format: Article
Language:English
Published: SpringerOpen 2023-12-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP12(2023)032
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author Minoru Eto
Kentaro Nishimura
Muneto Nitta
author_facet Minoru Eto
Kentaro Nishimura
Muneto Nitta
author_sort Minoru Eto
collection DOAJ
description Abstract QCD matter in strong magnetic field exhibits a rich phase structure. In the presence of an external magnetic field, the chiral Lagrangian for two flavors is accompanied by the Wess-Zumino-Witten (WZW) term containing an anomalous coupling of the neutral pion π 0 to the magnetic field via the chiral anomaly. Due to this term, the ground state is inhomogeneous in the form of either chiral soliton lattice (CSL), an array of solitons in the direction of magnetic field, or domain-wall Skyrmion (DWSk) phase in which Skyrmions supported by π 3[SU(2)] ≃ ℤ appear inside the solitons as topological lumps supported by π 2(S 2) ≃ ℤ in the effective worldvolume theory of the soliton. In this paper, we determine the phase boundary between the CSL and DWSk phases beyond the single-soliton approximation, within the leading order of chiral perturbation theory. To this end, we explore a domain-wall Skyrmion chain in multiple soliton configurations. First, we construct the effective theory of the CSL by the moduli approximation, and obtain the ℂP 1 model or O(3) model, gauged by a background electromagnetic gauge field, with two kinds of topological terms coming from the WZW term: one is the topological lump charge in 2+1 dimensional worldvolume and the other is a topological term counting the soliton number. Topological lumps in the 2+1 dimensional worldvolume theory are superconducting rings and their sizes are constrained by the flux quantization condition. The negative energy condition of the lumps yields the phase boundary between the CSL and DWSk phases. We find that a large region inside the CSL is occupied by the DWSk phase, and that the CSL remains metastable in the DWSk phase in the vicinity of the phase boundary.
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spelling doaj.art-e5ed198b502843cea19f81135138cc922024-03-31T11:08:46ZengSpringerOpenJournal of High Energy Physics1029-84792023-12-0120231212210.1007/JHEP12(2023)032Phase diagram of QCD matter with magnetic field: domain-wall Skyrmion chain in chiral soliton latticeMinoru Eto0Kentaro Nishimura1Muneto Nitta2Department of Physics, Yamagata UniversityResearch and Education Center for Natural Sciences, Keio UniversityResearch and Education Center for Natural Sciences, Keio UniversityAbstract QCD matter in strong magnetic field exhibits a rich phase structure. In the presence of an external magnetic field, the chiral Lagrangian for two flavors is accompanied by the Wess-Zumino-Witten (WZW) term containing an anomalous coupling of the neutral pion π 0 to the magnetic field via the chiral anomaly. Due to this term, the ground state is inhomogeneous in the form of either chiral soliton lattice (CSL), an array of solitons in the direction of magnetic field, or domain-wall Skyrmion (DWSk) phase in which Skyrmions supported by π 3[SU(2)] ≃ ℤ appear inside the solitons as topological lumps supported by π 2(S 2) ≃ ℤ in the effective worldvolume theory of the soliton. In this paper, we determine the phase boundary between the CSL and DWSk phases beyond the single-soliton approximation, within the leading order of chiral perturbation theory. To this end, we explore a domain-wall Skyrmion chain in multiple soliton configurations. First, we construct the effective theory of the CSL by the moduli approximation, and obtain the ℂP 1 model or O(3) model, gauged by a background electromagnetic gauge field, with two kinds of topological terms coming from the WZW term: one is the topological lump charge in 2+1 dimensional worldvolume and the other is a topological term counting the soliton number. Topological lumps in the 2+1 dimensional worldvolume theory are superconducting rings and their sizes are constrained by the flux quantization condition. The negative energy condition of the lumps yields the phase boundary between the CSL and DWSk phases. We find that a large region inside the CSL is occupied by the DWSk phase, and that the CSL remains metastable in the DWSk phase in the vicinity of the phase boundary.https://doi.org/10.1007/JHEP12(2023)032Phase Diagram or Equation of StateChiral LagrangianSolitons Monopoles and Instantons
spellingShingle Minoru Eto
Kentaro Nishimura
Muneto Nitta
Phase diagram of QCD matter with magnetic field: domain-wall Skyrmion chain in chiral soliton lattice
Journal of High Energy Physics
Phase Diagram or Equation of State
Chiral Lagrangian
Solitons Monopoles and Instantons
title Phase diagram of QCD matter with magnetic field: domain-wall Skyrmion chain in chiral soliton lattice
title_full Phase diagram of QCD matter with magnetic field: domain-wall Skyrmion chain in chiral soliton lattice
title_fullStr Phase diagram of QCD matter with magnetic field: domain-wall Skyrmion chain in chiral soliton lattice
title_full_unstemmed Phase diagram of QCD matter with magnetic field: domain-wall Skyrmion chain in chiral soliton lattice
title_short Phase diagram of QCD matter with magnetic field: domain-wall Skyrmion chain in chiral soliton lattice
title_sort phase diagram of qcd matter with magnetic field domain wall skyrmion chain in chiral soliton lattice
topic Phase Diagram or Equation of State
Chiral Lagrangian
Solitons Monopoles and Instantons
url https://doi.org/10.1007/JHEP12(2023)032
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AT kentaronishimura phasediagramofqcdmatterwithmagneticfielddomainwallskyrmionchaininchiralsolitonlattice
AT munetonitta phasediagramofqcdmatterwithmagneticfielddomainwallskyrmionchaininchiralsolitonlattice