“…Due to the disordered structure of the NLM host, the inhomogeneous broadening of spectral lines of Tm 3+ :NLM crystal leads to the broad and relative smooth absorption and fluorescence bands [12,13], which can reduce the requirement of strict temperature control of LD pump source and provide a wide tunable range of output laser. Using a Tm 3+ :NLM crystal as gain medium, 1.9 µm quasicontinuous-wave (quasi-CW) and CW lasers with slope efficiencies of about 50% have also been demonstrated in 795 nm Ti:Sapphire laser and 805 nm single-stripe diode end-pumped linear hemispherical resonators, respectively [12,13]. However, a monolithic micro-laser, which is consisted of only a thin slice of gain medium and the cavity mirrors deposited onto the medium faces directly, has an advantage of simplicity and compactness [14][15][16], and is more useful in some industrial and military applications.…”