The interaction properties of atoms are, at low
temperatures, fully determined by the s-wave scattering length of
the interatomic interaction potential. The magnitude and sign of
this quantity strongly depend on the presence of bound states in
this potential and, more precisely, on the energy of the bound
state that is closest to the continuum threshold. In the
multichannel case of a Feshbach resonance, the energy of the two
colliding atoms in the incoming open channel is close to the
energy of a bound state, i.e., a molecular state, in a coupled
closed channel.