Abstract. The anisotropy of thermal lensing and the photo-elastic effect is characterized for diode-pumped Nd:KGd(WO 4 ) 2 crystals cut along the N p and N g optical indicatrix axes and along its optical axis, O = N g +43°, at a laser wavelength of 1067 nm. Distortions in the spatial profile of output laser beam are analyzed. The thermal lens is astigmatic; the orientation of its principal meridional planes, A and B, is determined by the anisotropy of photo-elastic effect. The thermal lens has opposite signs for rays lying in the principal meridional planes for N pand O-cut crystals; and it is positive for an N g -cut crystal. The increase of thermal lens optical power after absorption of 1 W of pump power, i.e. the thermal lens sensitivity factors M A(B) , and astigmatism degree S = |M A -M B | are determined. The photo-elastic effect was found to increase the optical power of thermal lens and was significant for all studied crystal orientations. [5][6][7][8] low-threshold diode-pumped lasers operating in the vicinity of 1 and 1.3 μm. KGW is a biaxial crystal, with three crystal orientations having been employed so far for laser engineering: along the b (N p ) axis [1][2][3][5][6][7][8], along the N g axis [9][10][11][12] and along the optical axis (O) [13,14], i.e. N g +43° in the N p -N g plane [15]. Strong astigmatism of the thermo-optical properties of the material results in significant variation in the sign and value of the thermal lens in crystals cut for light propagation along the N p and N g axes under diode-or flash-lamp pumping [9,12,15,16]. Thermal lens measurements were reported previously for the N p and N g -cut Nd:KGW crystals at the wavelength of 1.06 μm under the flash-lamp-pumping [9,15,16] and at the wavelength of 1.35 μm under the diode -pumping [12].
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