2017
DOI: 10.1088/1742-6596/934/1/012046
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Transitions between topologically non-trivial configurations

Abstract: We study formation and evolution of solitons within a model with two real scalar fields with the potential having a saddle point. The set of these configurations can be split into disjoint equivalence classes. We give a simple expression for the winding number of an arbitrary closed loop in the field space and discuss the evolution scenarios that change the winding number. These non-trivial field configurations lead to formation of the domain walls in the three-dimensional physical space.

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Cited by 15 publications
(13 citation statements)
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“…Furthermore, we set R = ϕ 2 0 + χ 2 0 , see figure 1 (right panel). We performed the numerical simulation of the evolution of the initial configuration (4.2), (4.3) for N = 1, 2, 3, 4 and confirmed possibility of soliton production for all N , which was shown earlier in [64]. Our results are presented in figures 2 and 3.…”
Section: The Winding Numbersupporting
confidence: 80%
See 1 more Smart Citation
“…Furthermore, we set R = ϕ 2 0 + χ 2 0 , see figure 1 (right panel). We performed the numerical simulation of the evolution of the initial configuration (4.2), (4.3) for N = 1, 2, 3, 4 and confirmed possibility of soliton production for all N , which was shown earlier in [64]. Our results are presented in figures 2 and 3.…”
Section: The Winding Numbersupporting
confidence: 80%
“…For N > 2 the number of "humps" is increasing proportional to N (see [64] for details). If the height of the potential maximum is small enough, the fields overcome the maximum and tend to the absolute minimum in the whole space.…”
Section: The Winding Numbermentioning
confidence: 99%
“…[88][89][90][91][92][93]. Topologically non-trivial field configurations could be responsible for a variety of phenomena observed in the early Universe [94,95].…”
Section: Introductionmentioning
confidence: 99%
“…5 The mechanism of the wall formation is quite general and can be applied to those inflationary models containing extrema of their potential. Some of them where developed in [35][36][37] and in [38,39] where the potentials with saddle points were considered. It has been revealed there that the PBH mass spectrum and PBH ability depend strongly on the potential parameters and an initial field value, see discussion in Section 4 1.…”
Section: Introductionmentioning
confidence: 99%