Abstract

We study a recently proposed modification of the Skyrme model that possesses an exact self-dual sector leading to an infinity of exact Skyrmion solutions with arbitrary topological (baryon) charge. The self-dual sector is made possible by the introduction, in addition to the usual three SU(2) Skyrme fields, of six scalar fields assembled in a symmetric and invertible three dimensional matrix h. The action presents quadratic and quartic terms in derivatives of the Skyrme fields, but instead of the group indices being contracted by the SU(2) Killing form, they are contracted with the h-matrix in the quadratic term, and by its inverse on the quartic term. Due to these extra fields the static version of the model, as well as its self-duality equations, are conformally invariant on the three dimensional space ℝ3. We show that the static and self-dual sectors of such a theory are equivalent, and so the only non-self-dual solution must be time dependent. We also show that for any configuration of the Skyrme SU(2) fields, the h-fields adjust themselves to satisfy the self-duality equations, and so the theory has plenty of non-trivial topological solutions. We present explicit exact solutions using a holomorphic rational ansatz, as well as a toroidal ansatz based on the conformal symmetry. We point to possible extensions of the model that break the conformal symmetry as well as the self-dual sector, and that can perhaps lead to interesting physical applications.

Highlights

  • Skyrme model does have a topological charge admitting an integral representation, it does not possess a non-trivial self-dual sector [5]

  • We present explicit exact solutions using a holomorphic rational ansatz, as well as a toroidal ansatz based on the conformal symmetry

  • We point to possible extensions of the model that break the conformal symmetry as well as the self-dual sector, and that can perhaps lead to interesting physical applications

Read more

Summary

The description of the model

We consider in this paper the Skyrme-type model proposed in [15], on a four dimensional. The quantities Hμaν correspond to the curl of Rμ, and since these satisfy the Maurer-Cartan equation, i.e. The theory (2.1) differs from the original Skyrme model [2, 3] by the fact that the group indices are not contracted by the SU(2) Killing form but instead by the symmetric matrix hab on the quadratic term in derivatives and by its inverse on the quartic term. Note that by contracting the Euler-Lagrange equation (2.9) with hab, one gets that the two terms of the Lagrangian density in (2.1) must be equal on-shell, i.e. For static configurations that implies that the two terms in the energy density in (2.17). The balance between the quadratic and quartic terms in space derivatives of the energy density of the theory (2.1), is provided by the Euler-Lagrange equations for the fields hab as shown in (2.19)

The static sector
The self-dual sector
The holomorphic ansatz
The toroidal ansatz
Conclusions
A The conformal symmetry
The analysis using the self-duality equations
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call