It is astonishing that it is possible to infer the total density of ordinary
baryonic matter from the primordial synthesis of light nuclei
and
because it is based on well known nuclear physics. The deuterium
abundance is particularly relevant because it cannot be produced in stellar
processes. The recent determination(4) of the ratio of abundances
in uncontaminated distant
clouds through absorption of quasar radiation is explained by a ratio of
baryon to photon number densities.
![]() |
(17) |
Though this number of baryons seems very small, since its mass is around
almost 13 orders of magnitude larger than the energy of photons, it leads to
a mass density
![]() |
(18) |
![]() |
(19) |
This is the first evidence of dark matter, the baryonic one which could
reside in the MACHO's detected by microlensing that might account for up to
one third of the galactic halo, and probably more abundantly in diffuse gas
very difficult to detect except in the ray emitting intracluster gas.
Why must there be a galactic halo? It happens that according to Kepler law,
if the mass of the galaxy is the orbital velocity
of an object at a distance
from its centre is given by
![]() |
(20) |
This proves the existence of a dark halo which on the whole gives to the galaxy a mass ten times larger than its luminous part. Note that if all the halo is baryonic this would explain the ratio between Eqs.(19) and (16), leaving no room for diffuse gas.
But a very important observation has been done for clusters of galaxies
where most of baryons reside in the hot ray emitting intracluster gas. It
has been determined (5) that the ratio of baryonic and total cluster mass, to
explain its motion, is
![]() |
(21) |
![]() |
(22) |
This result, apart from giving evidence that most of baryonic dark matter must be in gaseous form, indicates that there is much more matter of non-baryonic type.