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)
- 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.