2014
DOI: 10.1088/1751-8113/47/20/205401
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Chiral Dirac–Born–Infeld solitons with SDiff symmetry

Abstract: We propose a new DBI extension of a Skyrme type model which allows for BPS topological solitons with arbitrary value of the baryon charge. The model is built out of the baryon density squared and in the limit of small fields tends to the BPS Skyrme model. We consider some generalizations to higher dimensions and other K-deformed actions.

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Cited by 3 publications
(5 citation statements)
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“…if the potential satisfies the above-mentioned system of equations for V. A similar result was obtained in [36]. In this case, obtaining general expression for V (i.e.…”
Section: K-deformation In the Non-gauged Casesupporting
confidence: 72%
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“…if the potential satisfies the above-mentioned system of equations for V. A similar result was obtained in [36]. In this case, obtaining general expression for V (i.e.…”
Section: K-deformation In the Non-gauged Casesupporting
confidence: 72%
“…Now, the next step is to check if, when the equations ( 34)-( 36) are satisfied, equations (43) hold. Thus, we insert ( 40)-( 42) into ( 34)- (36). Hence, we get a system of partial differ ential equations for V. It has turned out that V = V(ω, ω * ) and the solution of this system, for U = U(ωω * ), is:…”
Section: A Short Introductionmentioning
confidence: 99%
“…We started from finding the most general form of the functions R j = R j (ω, ω * , A 1 , A 2 ), (j = 1, 2), in the density of the topological invariant (16), written down in complex field variables, and the most general form of these functions in the density of the topological invariant (an analogon to ( 16)), written down in real field variables u, v. It has turned out that R…”
Section: Discussionmentioning
confidence: 99%
“…This generalization makes possible, deriving of Bogomolny decomposition, for more wide class of the potentials. When we need to express (16) in real functions u = ℜ(ω), v = ℑ(ω), then:…”
Section: The Concept Of Strong Necessary Conditionsmentioning
confidence: 99%
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