We fabricated several near-infrared Si laser devices (wavelength ∼1300 nm) showing continuous-wave oscillation at room temperature by using a phonon-assisted process induced by dressed photons. Their optical resonators were formed of ridge waveguides with a width of 10 µm and a thickness of 2 µm, with two cleaved facets, and the resonator lengths were 250-1000 µm. The oscillation threshold currents of these Si lasers were 50-60 mA. From near-field and far-field images of the optical radiation pattern, we observed the high directivity which is characteristic of a laser beam. Typical values of the threshold current density for laser oscillation, the ratio of powers in the TE polarization and TM polarization during oscillation, the optical output power at a current of 60 mA, and the external differential quantum efficiency were 1.1-2.0 kA/cm 2 , 8:1, 50 µW, and 1 %, respectively.Because silicon (Si) is an indirect-transition-type semiconductor, it is difficult to use it as a material for optical devices To solve these problems, in the research described here, we developed a Si laser showing continuous-wave operation at room temperature. To do so, we applied the same fabrication method and operating principle used for a Si-LED that we previously developed, which used a Si crystal having a p-n homojunction [4]. We report the results here.Similar to the fabrication of Si LEDs that we have already reported, in this work, first we formed a p-n homojunction by introducing a p dopant into an n-type Si substrate by ion implantation. Then, while irradiating the structure with light, we applied an electrical current to generate Joule heating, causing annealing. Stimulated emission was produced via a two-step transition process driven by the light irradiation. This process is described below [4,5].(i) First step: Dressed photons are generated by the light irradiation in regions where the dopant concentration in the p-n junction has a non-uniform spatial distribution. A dressed photon is a quasi-particle representing a coupled state due to the mutual interaction between a photon and an electron on the nanometer scale. The dressed photon then couples with a multi-mode phonon, generating stimulated emission that causes a conduction-band electron to transition from an initial state |E ex ; el ⊗ |E ex thermal ; phonon to an intermediate state |E g ; el ⊗ |E ex ; phonon . Here, |E ex ; el and |E g ; el respectively represent the excited state (conduction band) and ground state (valence band) of the