Using an ansatz [T. Matsuda, Lett. Nuovo Cimento 24 (1979) 207] which
is an exact collective variable (CV) solution for kink-kink (K-K) and
kink-antikink (K-A) interactions as well as for the breather in the un
perturbed sine-Gordon (SG) equation and uses only one CV r(t), the sep
aration between the kinks, we study the effects of microshort and micr
oresistor perturbations in a Josephson junction transmission line on K
-K interactions. Representing the energy stored in microshorts and mic
roresistors, these perturbations can profoundly alter the motion of fl
uxons, which we term kinks, in Josephson junction transmission lines.
With this ansatz, we describe particle characteristics, including rela
tivistic effects, of K-K and K-A interactions and the breather in the
unperturbed SG system. Because, in a perturbed SG system, this ansatz
is no longer exact, we modify it by treating the slope of the kinks Ga
mma(t) as a CV. We derive the masses of the r and Gamma CVs, the inter
action potentials, and the Hamiltonians for K-K and K-A. The inclusion
of Gamma(t) qualitatively and quantitatively changes the results of t
he one-CV r(t) description. Significantly, moderately strong microshor
t (microresistor) perturbations and highly relativistic initial veloci
ties increase (decrease) the time advance tau, defined as delta/nu, wh
ere nu is the single kink velocity and delta is the kinks' increased s
eparation or phase shift due to their interaction, in two-CV K-K scatt
ering relative to the unperturbed tau, by almost a factor of two for t
he microshort, whereas these conditions produce the reverse qualitativ
e and a smaller quantitative effect on the one-CV K-K tau. In contrast
, for weaker perturbations and slower initial velocities, a microshort
(microresistor) decreases (increases) the tau compared to the unpertu
rbed tau for both the one- and two-CV descriptions. (C) 1998 Elsevier
Science B.V.