We use the Kotliar-Ruckenstein slave-boson formalism to study the temperature dependence of paramagnetic phases of the one-band Hubbard model. We calculate the Fermi liquid quasiparticle spectral weight \(Z\) and identify the temperature at which it decreases significantly to a crossover to a bad metal region. Near the Mott metal-insulator transition, we find this coherence temperature \(T_\textrm{coh}\) to be much lower than the Fermi temperature of the uncorrelated Fermi gas, as is observed in a wide range of strongly correlated electron materials. We obtain the temperature-correlation phase diagram as a function of doping. We find a qualitative agreement for the temperature dependence of the double occupancy, entropy, and charge compressibility with previous results obtained with Dynamical Mean-Field Theory. We use the charge compressibility to analyse the stability of the technique and conclude that it's stable in a broad region of parameters.