The GW approximation is a well-established method for calculating
ionization potentials and electron affinities in solids and molecules. For
numerous years, obtaining self-consistent GW total energies in solids has
been a challenging objective that is not accomplished yet. However, it was
shown recently that the linearized GW density matrix permits a reliable
prediction of the self-consistent GW total energy for molecules [F. Bruneval
et. al. J. Chem. Theory Comput. 17, 2126 (2021)] for which self-consistent GW
energies are available. Here we implement, test, and benchmark the linearized
GW density matrix for several solids. We focus on the total energy, lattice
constant, and bulk modulus obtained from the GW density matrix and compare
our findings to more traditional results obtained within the random phase
approximation (RPA). We conclude on the improved stability of the total energy
obtained from the linearized GW density matrix with respect to the mean-field
starting point. We bring compelling clues that the RPA and the GW density
matrix total energies are certainly close to the self-consistent GW total
energy in solids if we use hybrid functionals with enriched exchange as a
starting point.Comment: 16 pages, 8 figure