NUCLEAR
Nuclear Physics B393 (1993) 65—78 P HY S I CS B
North-Holland _________________
Skyrmion model in 2 + 1 dimensions with soliton
bound states
Bernard Piette and Wojtek J. Zakrzewski
Department of Mathematical Sciences, Unirersity of Durham, Durha,n DI-Il 3LE, UK
Received 7 September 1992
Accepted for publication 20 October 1992
We consider a class of skyrmion models in 2+ I dimensions which possess bound stable
solitons. We show that these models have one-soliton solutions as well as static solutions
corresponding to their bound states. We study the scattering and stability properties of these
solutions, compute their energies and estimate their binding energies.
1. Introduction
Over the last few years, many physical processes have been described by
nonlinear partial differential equations. These include areas like solid-state physics,
hydrodynamics and classical field theories. Integrable models, in particular, have
been popular because of their properties and the existence of methods to construct
all their solutions. The integrable equations possess stable solutions (solitons)
which keep their shape as they move or interact with each other. Most of the
studied equations depend only on two space (or space-time) variables, and not
much work has been done yet on higher-dimensional models.
Integrable equations in 1 + I dimensions usually exhibit lump-like solutions
which propagate at a constant speed. When two lumps are sent towards each
other, they collide, modify their shape, and eventually emerge as if nothing has
happened apart from a phase shift. In one space dimension the collision can only
be head-on as there is no impact parameter. In higher dimensions, solitons look
like extended structures with localised energy density, which can move in any
direction. Not only can these objects perform a head on collision, but they can
scatter at a nonzero impact parameter.
In field theories, the models we are interested in are Lorentz invariant.
Unfortunately, so far, nobody has been able to construct a model in 2 + 1
dimensions which is both Lorentz invariant and integrable. In our previous papers
[1—3],we studied a class of (2 + 1)-dimensional minkowskian models which ap-
peared to be not integrable but had many features in common with integrable
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