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.