ÚTEFČVUT Ústav technické a experimentální fyziky ČVUT v PrazeInstitute of Experimental and Applied Physics, CTU in Prague

Shapes of magnetic monopoles in effective SU(2) models

NázevTitle
Shapes of magnetic monopoles in effective SU(2) modelsShapes of magnetic monopoles in effective SU(2) models
Druh výsledkuResult type
Článek v časopiseJournal article
AutořiAuthors
P. Beneš, F. Blaschke
Klíčová slovaKeywords
magnetic monopole
DOIDOI
10.1103/PhysRevD.107.125002
Časopis / citaceJournal / citation
Physical Review D 107(12), 125002 (2023) · ISSN 2470-0010
RokYear
2023
JazykLanguage
eng
ZáznamyRecords
ProjektProject
Institucionální podpora na rozvoj výzkumné org.Institucionální podpora na rozvoj výzkumné org.
CitovánoCited by
5 (INSPIRE-HEP)
2023: 12024: 22025: 12026: 1
Plný text (open access)Full text (open access)
http://link.aps.org/pdf/10.1103/PhysRevD.107.125002
Citace ke staženíDownload citation
TXT · BibTeX

AbstraktAbstract

We present a systematic exploration of a general family of effective SU(2) models with an adjoint scalar. First, we discuss a redundancy in this class of models and use it to identify seemingly different, yet physically equivalent models. Next, we construct the Bogomol'nyi-Prasad-Sommerfield limit and derive analytic monopole solutions. In contrast to the 't Hooft-Polyakov monopole, included here as a special case, these solutions tend to exhibit more complex energy density profiles. Typically, we obtain monopoles with a hollow cavity at their core where virtually no energy is concentrated; accordingly, most of the monopole's energy is stored in a spherical shell around its core. Moreover, the shell itself can be structured, with several "subshells". A recipe for the construction of these analytic solutions is presented.

We present a systematic exploration of a general family of effective SU(2) models with an adjoint scalar. First, we discuss a redundancy in this class of models and use it to identify seemingly different, yet physically equivalent models. Next, we construct the Bogomol'nyi-Prasad-Sommerfield limit and derive analytic monopole solutions. In contrast to the 't Hooft-Polyakov monopole, included here as a special case, these solutions tend to exhibit more complex energy density profiles. Typically, we obtain monopoles with a hollow cavity at their core where virtually no energy is concentrated; accordingly, most of the monopole's energy is stored in a spherical shell around its core. Moreover, the shell itself can be structured, with several "subshells". A recipe for the construction of these analytic solutions is presented.

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