Author Affiliations
1School of Mechanical and Precision Instrument Engineering, Xi’an University of Technology, Xi’an 710048, China2School of Physics and Optoelectronic Engineering, Xidian University, Xi’an 710071, Chinashow less
Fig. 1. Schematic of an off-axis end-pumped solid-state laser.
Fig. 2. Laser beam profiles with different mode distributions in the sixteen transverse displacements when the pump power is 0.25 W and the pump beam radius is 0.075 mm.
Fig. 3. Photon numbers of the mode HG00 and HG10 (a), and their percentages (b); photon numbers of the modes HG10 and HG20 (c), and their percentages (d) near the threshold.
Fig. 4. Dependence of the net gains on the pump power: (a) 0.08 mm; (b) 0.155 mm.
Fig. 5. Laser beam profiles with different mode distributions in the eight transverse displacements when the pump power is 0.5 W and the pump beam radius is 0.15 mm.
Fig. 6. Photon numbers of the modes HG00 , HG10 and HG20 (a) and their percentages (b); photon numbers of the modes HG10, HG20 and HG30 ((c), (e)) and their percentages ((d), (f)) near the threshold.
Fig. 7. Dependence of the net gains on the pump power: (a) 0.1 mm; (b) 0.2 mm.
Fig. 8. Dynamics of the photon numbers: (a) ωp = 0.075 mm, Δx = 0.08 mm, Pa = 0.5 W; (b) ωp = 0.075 mm, Δx = 0.08 mm, Pa = 5 W; (c) ωp = 0.15 mm, Δx = 0.1 mm, Pa = 0.5 W; (d) ωp = 0.15 mm, Δx = 0.1 mm, Pa = 5 W; (e) ωp = 0.15 mm, Δx = 0.2 mm, Pa = 0.5 W; (f) ωp = 0.15 mm, Δx = 0.2 mm, Pa = 5 W.
Fig. 9. Schematic of the experimental setup.
Fig. 10. Output spots with different off-axis displacements.
Fig. 11. The spot keeps unchanged with the variation of the laser power.
Fig. 12. (a) Dependence of the output power on the displacement; (b) the maximum powers of the modes.