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
- DOIDOI
- 10.1103/PhysRevD.107.125002
- Časopis / citaceJournal / citation
- Physical Review D. 2023, 107(12), 125002-1-125002-14. ISSN 2470-0010.
- RokYear
- 2023
- JazykLanguage
- eng
- WoSWoS
- 001011699800003
- ScopusScopus
- 2-s2.0-85161960898
- RIVRIV
- RIV/68407700:21670/23:00369629!RIV24-MSM-21670___
- ProjektProject
- Institucionální podpora na rozvoj výzkumné org.Institucionální podpora na rozvoj výzkumné org.
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.