Microcavity lasing has many excellent properties, such as a small mode volume, high quality factor (Q), high sensitivity, effortless manipulation, and good monochromaticity, which can be applied in sensing,1 – 3 nonlinear optics,4 – 6 and cavity optomechanics.7,8 The superior features of lanthanide-doped upconversion nanoparticles (UCNPs), such as their sharp emission bands, long lifetime, nonblinking and nonbleaching characteristics, and high stability,9,10 make them an attractive gain medium for the development of upconversion microlasers. Moreover, they have real intermediate energy states as efficient media for the development of multiphoton-excited states. Lanthanide-based microcavity lasing has attracted considerable attention owing to its large anti-Stokes shifts, multiple emission bands, and narrow linewidths.11 – 14 Many advances have been made, such as the effective regulation of laser modes, the realization of low-threshold microlasers, and the achievement of upconverted lasing.15 – 19 With the miniaturization of optoelectronic devices, various applications of lanthanide-based microlasers, such as optical communication, optical storage, and polarization imaging, require selecting the appropriate laser polarization mode and controlling the laser properties remotely on-chip. However, controlling the polarization mode of microlasing, a fundamental property of microlasers, both in situ and remotely, remains challenging.