1976
DOI: 10.1103/physrevd.14.1100
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Classical vortex solution of the Abelian Higgs model

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Cited by 297 publications
(305 citation statements)
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“…[7,11,13,15] and also in a standard textbook of Vilenkin & Shellard [8]. However, we encounter a different value for C 1 : C 1 = 10.58/2π ≃ 10.57/2π ≃ 1.682 ∼ 1.684 which was obtained by Speight [10] about twenty years later than de Vega & Schaposnik [5]. Furthermore, Tong [11] gave the supergravity prediction C 1 = 8 1/4 ≃ 1.68179 .…”
Section: Jhep11(2015)073mentioning
confidence: 88%
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“…[7,11,13,15] and also in a standard textbook of Vilenkin & Shellard [8]. However, we encounter a different value for C 1 : C 1 = 10.58/2π ≃ 10.57/2π ≃ 1.682 ∼ 1.684 which was obtained by Speight [10] about twenty years later than de Vega & Schaposnik [5]. Furthermore, Tong [11] gave the supergravity prediction C 1 = 8 1/4 ≃ 1.68179 .…”
Section: Jhep11(2015)073mentioning
confidence: 88%
“…The constant C 1 has often been calculated in the literature. De Vega & Schaposnik [5] gave a semi-analytical study for axially-symmetric solutions with an arbitrary winding number k ∈ Z >0 , and constructed power-series expansions around a center of a vortex and asymptotic expressions for the opposite side. These two can be determined by only one constant D k+1 k for the power-series expansion and C k (Z k in their notation) for the asymptotic expression.…”
Section: Jhep11(2015)073mentioning
confidence: 99%
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“…This is the simplest way we found to make sure that the Abelian Higgs-Galileon system has an energy density bounded from below -other possibility might exist though. Given these preliminary results, it would be interesting to study more in general the stability of our configurations under small fluctuations, and to explore alternative methods to obtain the BPS equations for Galileon vortices, such as methods based on the energy-momentum tensor [35] or on the Lagrangian of the system rather than on the Hamiltonian [36]. We end this section showing that the static configurations discussed in section 3.4 have positive definite energy for the values of β we considered.…”
Section: The Energy Functional For the Galileon Vortexmentioning
confidence: 99%
“…In particular, for small ϑ (and consequently γ) the regular commutative Neilsen-Olesen vortex solutions of [3,28] are obtained. In addition, an obvious solution to (3.15) that satisfies the boundary conditions of the semilocal model is Q m ≡ 1.…”
Section: Examplesmentioning
confidence: 99%