Ústav technické a experimentální fyziky Institute of Experimental and Applied Physics

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.