  We show that the low-temperature physics of molecular nanomagnets, contrary
to the prevailing one-molecule picture, must be determined by the long-range
magnetic ordering due to many-body dipolar interactions. The calculations here
performed, using Ewald's summation, suggest a ferromagnetic ground state with a
Curie temperature of about 130 mK. The energy of this state is quite close to
those of an antiferromagnetic state and to a glass of frozen spin chains. The
latter may be realized at finite temperature due to its high entropy.
