The power loss P of hot Dirac fermions through the coupling to the intrinsic intravalley and intervalley acoustic and optical phonons is analytically investigated in silicene as a function of electron temperature Te and density ns. At very low Te, the power dissipation is found to follow the Bloch-Grüneisen power-law ∝ T 4 e and n −0.5 s , as in graphene, and for Te 20−30 K, the power loss is predominantly due to the intravalley acoustic phonon scattering. On the other hand, dispersionless low energy intervalley acoustic phonons begin to dominate the power transfer at temperatures as low as ∼30 K, and optical phonons dominate at Te 200 K, unlike the graphene. The total power loss increases with Te with a value of ∼10 10 eV/s at 300 K, which is the same order of magnitude as in graphene. The power loss due to intravalley acoustic phonons increases with ns at higher Te, whereas due to the intervalley acoustic and optical phonons is found to be independent of ns. Interestingly, the energy relaxation time in silicene is about 4 times higher than that in graphene. For this reason, silicene may be superior over graphene for its applications in bolometers and calorimeters. Power transfer to the surface optical phonons PSO is also studied as a function of Te and ns for silicene on Al2O3 substrate and it is found to be greater than the intrinsic phonon contribution at higher Te. Substrate engineering is discussed to reduce PSO.