scholarly journals Scaling behavior in the Einstein–Yang–Mills monopoles and dyons

2002 ◽  
Vol 43 (1) ◽  
pp. 597-603 ◽  
Author(s):  
Yutaka Hosotani
1982 ◽  
Vol 141 (1) ◽  
pp. 104-115 ◽  
Author(s):  
Daksh Lohiya

2014 ◽  
Vol 29 (08) ◽  
pp. 1450042
Author(s):  
Buddhi Vallabh Tripathi ◽  
Hemwati Nandan ◽  
Heinz Dehnen ◽  
K. D. Purohit

Gravitating monopoles and dyons in Einstein–Yang–Mills (EYM) or Einstein–Yang–Mills–Higgs (EYMH) systems have been extensively studied for various curved space–times, including those of black holes. We construct dyonic solutions of the EYMH theory in Vaidya space–time using a set of generalized Julia–Zee ansatz for the fields. It is found that the dyonic charge is static in nature and it does not contribute to the energy of the null dust.


2013 ◽  
Vol 28 (20) ◽  
pp. 1330029 ◽  
Author(s):  
JIHYE SOFIA SEO

In this paper, we consider the case where electrons, magnetic monopoles and dyons become massless. Here, we consider the [Formula: see text] supersymmetric Yang–Mills (SYM) theories with classical gauge groups with a rank r, SU(r+1), SO(2r), Sp(2r) and SO(2r+1) which are studied by Riemann surfaces called Seiberg–Witten curves. We discuss physical singularity associated with massless particles, which can be studied by geometric singularity of vanishing 1-cycles in Riemann surfaces in hyperelliptic form. We pay particular attention to the cases where mutually nonlocal states become massless (Argyres–Douglas theories), which corresponds to Riemann surfaces degenerating into cusps. We discuss nontrivial topology on the moduli space of the theory, which is reflected as monodromy associated to vanishing 1-cycles. We observe how dyon charges get changed as we move around and through singularity in moduli space.


1990 ◽  
Vol 150 (3-4) ◽  
pp. 159-162 ◽  
Author(s):  
A.A. Ershov ◽  
D.V. Gal'tsov

1996 ◽  
Vol 11 (26) ◽  
pp. 4745-4777 ◽  
Author(s):  
LUIS ÁLVAREZ-GAUMÉ ◽  
COSTAS KOUNNAS ◽  
JACQUES DISTLER ◽  
MARCOS MARIÑO

We analyze the possible soft breaking of (N = 2)-supersymmetric Yang–Mills theory with and without matter flavor preserving the analyticity properties of the Seiberg–Witten solution. For a small supersymmetry-breaking parameter with respect to the dynamical scale of the theory we obtain an exact expression for the effective potential. We describe in detail the onset of the confinement transition and some of the patterns of chiral symmetry breaking. If we extrapolate the results to the limit where supersymmetry decouples, we obtain hints indicating that perhaps a description of the QCD vacuum will require the use of Lagrangians containing simultaneously mutually nonlocal degrees of freedom (monopoles and dyons).


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