J Hietarinta et al 1994 J. Phys. A: Math. Gen. 27 3149 doi:10.1088/0305-4470/27/9/027
J Hietarinta, A Ramani and B Grammaticos
Show affiliationsWe discuss the freedom in the background field (vacuum) on top of which the solitons are built. If the Hirota bilinear form of a soliton equation is given by A(Dx)G.F=0, B(Dx)(F.F-G.G)=0, where both A and B are even polynomials in their variables, then there can be a continuum of vacua, parametrized by a vacuum angle phi . The ramifications of this freedom for the construction of one- and two-soliton solutions are discussed. We find, for example, that once the angle phi is fixed and we choose u=tan-1 G/F as the physical quantity, then there are four different solitons (or kinks) connecting the vacuum angles +or- phi , +or- phi +or- pi /2 (where pi is the defined modulo). The most interesting result is the existence of a 'ghost' soliton; goes over to the vacuum but interacts with 'normal' solitons by giving them a finite phase shift.
Issue 9 (7 May 1994)
J Hietarinta et al 1994 J. Phys. A: Math. Gen. 27 3149
Virginia Yong and H Thomas Hahn 2005 Nanotechnology 16 354
M Rozenfeld 1972 Phys. Med. Biol. 17 861
S Simons and I C Simpson 1974 J. Phys. C: Solid State Phys. 7 3692
Mohammad Nouri-Zonoz 2004 Class. Quantum Grav. 21 471
Irena Knezevic and David K Ferry 2004 Semicond. Sci. Technol. 19 S220
M Aketagawa et al 2006 Meas. Sci. Technol. 17 513
A B Balantekin et al 2004 J. Phys. G: Nucl. Part. Phys. 30 1225
Prakash Gupta et al 2006 J. Phys. B: At. Mol. Opt. Phys. 39 1137
Julio Gea-Banacloche 2006 J. Phys. B: At. Mol. Opt. Phys. 39 69
, and Chern–Simons–Higgs solitons on
: dimensional reduction of Chern–Pontryagin densities