  We compute an approximate set of longitudinal quasiparticle modes for a
hydrogen condensate as produced in the MIT experiments. An expansion in
quasiparticles using a simple one-dimensional Bogoliubov picture shows however
that at the high temperatures (\approx 44muK) and in the very shallow trap
employed (omega_z = 2\pi\times 10.2Hz) the contribution to the density from the
quasiparticles is about 20% of that from the condensate mode, leading to an
effective $ g_2(x,x) which varies between 1 and 3 depending on the position in
the condensate.
