In this article, we develop a singular perturbation theory for describing the long time cumulative effects of weak perturbations on solitons. In all cases, the solitons behave in a similar fashion to either relativistic or Newtonian particles or nonlinear oscillators under the influence of external forces. We show how the ubiquitous nonlinear Schrödinger soliton can become synchronized to a periodic external field and how it moves in gradual field gradients. We examine how the kink of the sine-Gordon equation acts both as a relativistic particle and a Newtonian particle in the presence of a general impurity and demonstrate the relaxation of a kink-antikink pair to a breather under the influence of damping. Finally, we discuss the motion of a soliton of the Korteweg de Vries equation under various perturbations and discover that while the soliton remains dominant, the continuous spectrum is excited and plays a crucial rôle in balancing the ‘mass’ and ‘energy’ depletion rates. In each case, we briefly discuss the result in the context of a physical situation.
[1]
David J. Kaup,et al.
The Goursat and Cauchy Problems for the Sine-Gordon Equation
,
1978
.
[2]
D. G. Thomas,et al.
Auger Recombination of Excitons Bound to Neutral Donors in Gallium Phosphide and Silicon
,
1966
.
[3]
C. S. Gardner,et al.
Method for solving the Korteweg-deVries equation
,
1967
.
[4]
A. Bishop,et al.
Dynamics of sine-Gordon solitons in the presence of perturbations
,
1977
.
[5]
T. Kakutani,et al.
Effect of an Uneven Bottom on Gravity Waves
,
1971
.
[6]
A. Newell.
The inverse scattering transform, nonlinear waves, singular perturbations and synchronized solitons
,
1978
.