Green pulse regenerative amplification using a Pr3+:LiYF4 crystal pumped by GaN blue laser diodes

• Published in: Optics express 2024-11, Vol.32 (23), p.40499
• Main Authors: Yada, Hiroyuki, Ichikawa, Yuki
• Format: Article
• Language: English
• ISSN: 1094-4087; 1094-4087
• DOI: 10.1364/OE.541513

Direct regenerative amplifications of green pulses (522 nm) were investigated using a Pr3+-doped LiYF4 crystal pumped by GaN blue laser diodes. Green pulses with two different temporal duration regimes, i.e. sub-picosecond (sub-ps) and sub-nanosecond (sub-ns), were prepared from the second harmonic generation of the mode-locked Yb3+-doped fiber laser at the repetition rate of 100.86 kHz and used as a seed for the comparison of the amplification processes. For the sub-ps (0.63 ps) and sub-ns (0.3-0.4 ns) seeds, the amplifications resulted in 1.25 µJ and 1.53 µJ in the pulse energies, 0.60 nm and 0.27 nm bandwidths, and the beam qualities of (M2x = 2.26, M2y = 1.25) and (M2x = 1.47, M2y = 1.23), respectively. A comparison of the B integrals confirmed that the wider bandwidth and the lower beam quality of the sub-ps seed amplification versus the sub-ns seed amplification were caused by the nonlinear effects in the sub-ps amplification.Direct regenerative amplifications of green pulses (522 nm) were investigated using a Pr3+-doped LiYF4 crystal pumped by GaN blue laser diodes. Green pulses with two different temporal duration regimes, i.e. sub-picosecond (sub-ps) and sub-nanosecond (sub-ns), were prepared from the second harmonic generation of the mode-locked Yb3+-doped fiber laser at the repetition rate of 100.86 kHz and used as a seed for the comparison of the amplification processes. For the sub-ps (0.63 ps) and sub-ns (0.3-0.4 ns) seeds, the amplifications resulted in 1.25 µJ and 1.53 µJ in the pulse energies, 0.60 nm and 0.27 nm bandwidths, and the beam qualities of (M2x = 2.26, M2y = 1.25) and (M2x = 1.47, M2y = 1.23), respectively. A comparison of the B integrals confirmed that the wider bandwidth and the lower beam quality of the sub-ps seed amplification versus the sub-ns seed amplification were caused by the nonlinear effects in the sub-ps amplification.