Radially polarized light attracts much attention because of its applications in high-precise metal cutting, optical tweezers and other fields. Many schemes have been developed to force the radial-polarization excitation in laser resonator by employing various intracavity polarization selectors, such as birefringent crystal and/or conical Brewster window [1]. These methods, however, are applicable only in a limited range of laser output power [1], and encounter big challenges in improving the laser efficiency, beam's cylindrical symmetry and polarization purity simultaneously. In recent years the photonic crystal grating (PCG), one kind of threedimensional sub-wavelength gratings, appeared as an effective polarization-dependent element which can provide the specified reflectivity/transmission to the radial polarization and thus can play as the output coupler of laser resonator for desired polarization. Such grating mirror shows unique superiority when combining with compact and end-pumped microchip laser in providing high polarization purity and excellent modal symmetry as well as high laser efficiency embodied in the radial-polarization emission [2]. However, the thermal lens effect in the end-pumped microchip gain medium remained as an obstacle for further power scaling, and so far the output power from such laser is kept in the hundreds milliwatts level. An efficient, high-power and compact solid state laser that emits radially polarized light with high polarization purity would be extremely desirable.In this report, we presented an efficient, watt-level and radially polarized Nd:YAG laser. We used a 2-mm thick and 1-at.% doped Nd:YAG crystal, which is bonded with two 3-mm thick and un-doped YAG end caps, as the gain medium. The high thermal conductivity of this bonded structure could weaken the temperature gradient in the lasing area and thereafter the thermal lens effect was alleviated considerably at the presence of intensive pumping. This composite crystal was pumped by a fiber-coupled 808-nm laser diode, and its front surface was coated with high transmission at 808nm and high reflectivity at 1064nm. Its rear surface was coated with high transmission at 1064nm. We used a PCG mirror, which has a reflectivity of about 83% for transverse electric wave (TE wave, radial polarization) and is transparent to transverse magnetic wave (TM wave, tangential polarization) at 1064nm, as the couput coupler. The total length of the laser cavity was 35mm.In the study, above the lasing threshold of 2.67-W absorbed pump power (P abs ), as shown in Fig. 1, the beam power increased linearly with P abs in a slope efficiency of 46.5%, and reached 1.29W at P abs =5.45W with a polarization purity of 97.9%. We didn't observe the saturation of laser output power when the pump power increased further. Nevertheless, we noticed that, when P abs was kept within the range of 2.67W to 5.45W, the laser beam showed a single-ring and doughnut beam profile; when P abs was larger than 5.45W, the laser oscillated at high-order transverse mode ...