Tm ³⁺and Yb ³⁺, with different concentrations, co-doped Bi ₂WO ₆up-conversion luminescence materials are prepared by high temperature solid state method. The microstructure, upconversion emission spectra, and optical temperature sensing properties of the synthesized powders are characterized and analyzed. The X-ray diffraction results show that the doping of Tm ³⁺and Yb ³⁺ions has little effect on the orthorhombic structure of Bi ₂WO ₆matrix material. Under the 980 nm excitation, the maximum emission intensity of Tm ³⁺ions is obtained when the doping concentration of Tm ³⁺and Yb ³⁺are 1% and 6%, respectively. The intensities of four emission peaks of Tm ³⁺in 1%Tm ³⁺, 6%Yb ³⁺:Bi ₂WO ₆sample increase with the excitation pump power increasing from 199 to 400 mW. With the excitation power of 199–400 mW, the sample light intensity Iand the excitation power P ⁿshow a linear relationship. The relationship between the excitation pump power and the emission intensity of Tm ³⁺in this range is investigated. The four emission peaks of Tm ³⁺at 478, 650, 685 and 705 nm correspond to the nvalues of 1.01, 1.34, 1.77 and 1.75, respectively, indicating that the above emission peaks are derived from two-photon absorption. Under 980 nm excitation (power 379 mW), when the temperature increases from 298 to 573 K, the thermal coupling energy levels of Tm ³⁺in 1%Tm ³⁺, 6%Yb ³⁺:Bi ₂WO ₆samples produce 705 and 685 nm emission whose intensities are increased by 28.4 times and 31.6 times, respectively. The relationship between the fluorescence intensity ratio of the thermal coupling energy levels ( ³F ₃, ³F ₂) of Tm ³⁺in the sample and the temperature is fitted. The maximum absolute temperature sensitivity of the sample is 0.00254 K ^–1at 298 K, and the maximum relative temperature sensitivity is 0.00144 K ^–1. Under the same conditions, the relationship between the fluorescence intensity ratio of 705 and 650 nm produced by the non-thermal coupling energy level pair ( ³F ₃, ¹G ₄) and the temperature is fitted, and the maximum absolute temperature sensitivity is calculated to be 0.167 K ^–1at 573 K. The maximum relative temperature sensitivity is 0.0378 K ^–1at 298 K, which is 26 times higher than the relative maximum temperature sensitivity S _rof the thermal coupling level ( ³F ₃, ³F ₂).