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K fields, compactons and thick branes

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C Adam1, N Grandi2, J Sánchez-Guillén1 and A Wereszczyński3

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K fields, that is, fields with a non-standard kinetic term, allow for soliton solutions with compact support, i.e., compactons. Compactons in 1+1 dimensions may give rise to topological defects of the domain wall type and have finite thickness in higher dimensions. Here we demonstrate that, for an appropriately chosen kinetic term, the propagation of linear perturbations is completely suppressed outside the topological defect, confining the propagation of particles inside the domain wall. On the other hand, inside the topological defect the propagation of linear perturbations is of the standard type, in spite of the non-standard kinetic term. Consequently, this compacton domain wall may act like a brane of finite thickness which is embedded in a higher dimensional space, but to which matter fields are constrained. In addition, we find strong indications that, when gravity is taken into account, location of gravity in the sense of Randall–Sundrum works for these compacton domain walls. When seen from the bulk, these finite thickness branes, in fact, cannot be distinguished from infinitely thin branes.


PACS

11.25.Wx String and brane phenomenology

02.40.-k Geometry, differential geometry, and topology

98.80.Cq Particle-theory and field-theory models of the early Universe (including cosmic pancakes, cosmic strings, chaotic phenomena, inflationary universe, etc.)

11.27.+d Extended classical solutions; cosmic strings, domain walls, texture

11.10.Lm Nonlinear or nonlocal theories and models

MSC

83F05 Cosmology

85A40 Cosmology (For relativistic cosmology, see 83F05)

81T30 String and superstring theories; other extended objects (e.g., branes) (See also 83E30)

Subjects

Mathematical physics

Gravitation and cosmology

Particle physics and field theory

Astrophysics and astroparticles

Dates

Issue 21 (30 May 2008)

Received 3 April 2008

Published 8 May 2008


A Corrigendum for this article has been published in 2009 J. Phys. A: Math. Theor. 42 159801


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