The description of the molecular solid phase of O2, especially its
ground-state antiferromagnetic insulating phase, is known to be quite
unsatisfactory within the conventional local and semilocal density functional
approximations used in the Kohn-Sham formalism of density functional theory.
The recently-developed van der Waals functionals that take into account
nonlocal correlations have also shown subpar performance in this regard. The
difficulty lies in the subtle balance between the van der Waals interactions
and the exchange coupling between the antiferromagnetic and ferromagnetic
molecule pairs in the molecular crystal. Here, we report that the DFT+U
approach used in combination with the vdW-DF functional performs surprisingly
well in this regard, and discuss the reasoning behind this behavior. We also
apply this approach to study the recently-reported magnetic field-induced
θ phase of solid O2.Comment: Final published versio