We study collective and single-particle intersubband excitations in a
system of quantum wires coupled via weak tunneling. For an isolated wi
re with parabolic confinement, Kohn's theorem guarantees that the abso
rption spectrum represents a single sharp peak centered at the frequen
cy given by the bare confining potential. We show that the effect of w
eak tunneling between two parabolic quantum wires is twofold: (i) addi
tional peaks corresponding to single-particle excitations appear in th
e absorption spectrum, and (ii) the main absorption peak acquires a de
polarization shift. We also show that the interplay between tunneling
and weak perpendicular magnetic field drastically enhances the dispers
ion of single-particle excitations. The latter leads to a strong dampi
ng of the intersubband plasmon for magnetic fields exceeding a critica
l value. The results are obtained within a random-phase approximation
for the total potential and at low electron concentration, where the s
creening effects are treated perturbatively.