Transverse quasi-static electromagnetic modes (ωkc≪1 , where ω and k are the mode frequency and the wavenumber, respectively, and c is the speed of light) are studied in laser heated relativistic plasmas, where the electron thermal energy could be comparable to or greater than the electron rest mass energy. A dispersion relation of these modes valid in the whole collisionality regime is derived with the use of the relativistic Vlasov-Landau and Maxwell equations. The dissipative part of the dispersion relation is calculated with the Maxwell-Boltzmann-Jüttner distribution function, as a function of the Knudsen number kλei, where λei is the electron mean-free-path. It is shown that the dissipative part exhibits a continuous transition from the collisional regime [∼kλei2] to the Landau collisionless one [∼kλei3]. The relativistic electrical conductivity is also deduced and compared with the results reported in the literature. Taking into account the anisotropy of the distribution function induced by the inverse bremsstrahlung absorption, the stability analysis of the electromagnetic modes is presented. It is found that for typical inertial confinement fusion plasmas, strong growing modes could be driven.