Nonlinear mirror mode-locking of efficiently diode-pumped pulsed neodymium lasers

Antonio Agnesi; Stefano Dell’Acqua; Giancarlo Reali

doi:10.1364/JOSAB.16.001236

Journal of the Optical Society of America B
Vol. 16,
Issue 8,
pp. 1236-1242
(1999)
•https://doi.org/10.1364/JOSAB.16.001236

Nonlinear mirror mode-locking of efficiently diode-pumped pulsed neodymium lasers

Antonio Agnesi, Stefano Dell’Acqua, and Giancarlo Reali

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Antonio Agnesi, Stefano Dell’Acqua, and Giancarlo Reali, "Nonlinear mirror mode-locking of efficiently diode-pumped pulsed neodymium lasers," J. Opt. Soc. Am. B 16, 1236-1242 (1999)

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The topics in this list come from the Optics and Photonics Topics applied to this article.
Previously assigned OCIS codes
- Lasers, diode-pumped (140.3480)
- Lasers, neodymium (140.3530)
- Mode-locked lasers (140.4050)

About this Article
History
- Original Manuscript: January 20, 1999
- Revised Manuscript: April 8, 1999
- Published: August 1, 1999

Abstract

We report the development of compact, efficiently diode-pumped Nd:YAG and $Nd : {YAlO}_{3}$ lasers in a pulsed regime, mode locked by a nonlinear mirror (NLM) technique. Pumping with an 80-W single-bar diode array at a repetition rate as high as 200 Hz and depending on the NLM configuration, trains of 20–100 pulses, with 25-ps pulses with energies as high as 9 µJ each, are generated. These novel pulsed picosecond sources show excellent amplitude stability (<2% amplitude fluctuation) and beam quality. Numerical simulations of the pulse-formation dynamics are presented, and the results are compared with the experiments.

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$R_{ω}$	$E_{M 3}^{(ω)}$ (µJ)	$N^{(ω, M 3)}$	$τ^{(M 3)}$ (ps)	$E_{pol}^{(ω)}$ (µJ)	$N^{(ω, pol)}$	$τ^{(pol)}$ (ps)	$E_{M 2}^{(2 ω)}$ (µJ)	$N^{2 (ω, M 2)}$
77% ML	173	75	41	—	—	—	47	50
77% ML	227	75	42	107	52	32	80	31
69% ML	370	63	45	—	—	—	133	38
69% ML	267	63	45	133	31	29	127	25
65% ML	340	100	33	—	—	—	113	100

$R_{ω}$	$E_{M 3}^{(ω)}$ (µJ)	$N^{(ω, M 3)}$	$τ^{(M 3)}$ (ps)	$E_{pol}^{(ω)}$ (µJ)	$N^{(ω, pol)}$	$τ^{(pol)}$ (ps)	$E_{M 2}^{(2 ω)}$ (µJ)	$N^{(2 ω, M 2)}$
77% ML	207	38	31	97	31	26	33	23
77% FR	887			340
69% ML	267	31	32	120	23	25	57	19
69% FR	543			147

$R_{ω}$	$E_{M 3}^{(ω)}$ (µJ)	$N^{(ω, M 3)}$	$τ^{(M 3)}$ (ps)	$E_{pol}^{(ω)}$ (µJ)	$N^{(ω, pol)}$	$τ^{(pol)}$ (ps)	$E_{M 2}^{(2 ω)}$ (µJ)	$N^{2 (ω, M 2)}$
77% ML	173	75	41	—	—	—	47	50
77% ML	227	75	42	107	52	32	80	31
69% ML	370	63	45	—	—	—	133	38
69% ML	267	63	45	133	31	29	127	25
65% ML	340	100	33	—	—	—	113	100

$R_{ω}$	$E_{M 3}^{(ω)}$ (µJ)	$N^{(ω, M 3)}$	$τ^{(M 3)}$ (ps)	$E_{pol}^{(ω)}$ (µJ)	$N^{(ω, pol)}$	$τ^{(pol)}$ (ps)	$E_{M 2}^{(2 ω)}$ (µJ)	$N^{(2 ω, M 2)}$
77% ML	207	38	31	97	31	26	33	23
77% FR	887			340
69% ML	267	31	32	120	23	25	57	19
69% FR	543			147

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