  We show that bipolaron formation leads to a d-wave Bose-Einstein condensate
in cuprates. It is the bipolaron energy dispersion rather than a particular
pairing interaction which is responsible for the d-wave symmetry. The unusual
low-temperature dependence of the magnetic field penetration depth in cuprates
is explained by the localisation of bosons in the random potential. The
temperature dependence of the penetration depth is linear with positive or
negative slope depending on the random field profile.
