Jie Xu, Xiaohua Che, Hengda Li, Shumei Wang, Shuanghong Ding. Numerical Simulation of Solid-State Lasers Based on Secondary Raman Modes[J]. Chinese Journal of Lasers, 2020, 47(5): 0501001
- Chinese Journal of Lasers
- Vol. 47, Issue 5, 0501001 (2020)
Fig. 1. Pulse output characteristics versus K2/K1 when N takes different values. (a)Peak power ΦS1max of Raman light 1 and peak power ΦS2max of Raman light 2; (b) pulse energy ΦS1int of Raman light 1 and pulse energy ΦS2int of Raman light 2; (c) pulse width τS1 of Raman light 1 and pulse width τS2 of Raman light 2; (d) critical value of K2
Fig. 2. Pulse output characteristics versus K2/K1 when M2 takes different values.(a)Peak power ΦS1max of Raman light 1 and peak power ΦS2max of Raman light 2; (b) pulse energy ΦS1int of Raman light 1 and pulse energy ΦS2int of Raman light 2; (c) pulse width τS1 of Raman light 1 and pulse width τS2 of Raman light 2; (d) critical value of K
Fig. 3. Pulse output characteristics versus K2/K1 when α takes different values. (a) Peak power ΦS1max of Raman light 1 and peak power ΦS2max of Raman light 2; (b) pulse energy ΦS1int of Raman light 1 and pulse energy ΦS2int of Raman light 2; (c) pulse width τS1 of Raman light 1 and pulse width τS2 of Raman light 2; (d) critical value of K2
Fig. 4. Pulse output characteristics versus α when N takes different values. (a) Peak power ΦS1max of Raman light 1 and peak power ΦS2max of Raman light 2; (b) pulse energy ΦS1int of Raman light 1 and pulse energy ΦS2int of Raman light 2; (c) pulse width τS1 of Raman light 1 and pulse width τS2 of Raman light 2
Fig. 5. Pulse output characteristics versus M2/M1 when N takes different values. (a) Peak power ΦS1max of Raman light 1; (b) pulse energy ΦS1int of Raman light 1; (c) pulse width τS1 of Raman light 1
Fig. 6. Experimental results of peak power ΦS1max of 1097 nm Raman light versus K2/K1
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Table 1. Range of normalized parameters
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