The band structures of the periodic nanotube junctions are investigated by
the use of effective mass theory (k.p approximation) and the tight binding
model. The periodic junctions are constructed by the periodic introduction
of defect pairs, consisting of a pentagonal defect and a heptagonal defect,
into the carbon nanotube. We treat the periodic junctions whose unit cell
is composed by two kinds of metallic nanotubes. The discussed energy region
is near the undoped Fermi level where the channel number is kept to 2, so
there are two bands. The degeneracy and repulsion between the two bands are
determined only from symmetries.