2017
DOI: 10.1364/oe.25.023254
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Modelocking of a thin-disk laser with the frequency-doubling nonlinear-mirror technique

Abstract: We demonstrate a frequency-doubling nonlinear-mirror (NLM) modelocked thin-disk laser. This modelocking technique, composed of an intracavity second harmonic crystal in combination with a dichroic output coupler, offers robust operation decoupled from cavity stability (as in semiconductor saturable absorber mirror (SESAM) modelocking) combined with an ultrafast saturable loss and high modulation depth (as in Kerr-lens modelocking (KLM)). With our NLM diode-pumped Yb:YAG thin-disk laser we achieve 21 W of avera… Show more

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Cited by 26 publications
(10 citation statements)
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“…The design rules presented in this paper can be applied to Mamyshev mode-locking of other solid-state platforms such as thin disk lasers that promise ever higher pulse energy and average power [36][37][38]. Recently, such cascaded quadratic nonlinearity in PPLN waveguide has been utilized to demonstrate supercontinuum generation with a spectrum that spans multiple octaves [39].…”
Section: Discussionmentioning
confidence: 99%
“…The design rules presented in this paper can be applied to Mamyshev mode-locking of other solid-state platforms such as thin disk lasers that promise ever higher pulse energy and average power [36][37][38]. Recently, such cascaded quadratic nonlinearity in PPLN waveguide has been utilized to demonstrate supercontinuum generation with a spectrum that spans multiple octaves [39].…”
Section: Discussionmentioning
confidence: 99%
“…This topic has recently received significant attention in the community, as it is well-known that even for soliton modelocking, higher modulation depths are desired to reach shortest pulses at high power [42]. Several directions are currently being explored [43], and we believe a potential route to achieve this could be the implementation of an all-reflective NPE.…”
Section: Discussion On Possible Practical Implementationmentioning
confidence: 99%
“…M1, M2, M3, and M4 form a z-type cavity and the length of the resonant cavity is 1.3 m. The size of MgO:LN is 5 mm × 5 mm × 5 mm (w × h × l), and the phase-matching angle of MgO:LN is cut to be θ = 79.2°, φ = 90°. To date, most of the studies on NLM have focused on a particular wavelength, such as laser sources around 1, 1.3, and 2 µm [10][11][12][13][14][15][16][17][18][19][20][21][22][23][24]. However, tunable picosecond lasers with output powers at the watt level are also of interest.…”
Section: Methodsmentioning
confidence: 99%
“…The peak power of the output laser is commonly at the kilowatt level while a bulk laser crystal is utilized, as shown in Figure 1. Combined with a thin-disk (TD) laser crystal, NLM disk (TD) laser crystal, NLM could generate ultrafast lasers within several hundreds of femtoseconds and with peak powers up to 10 MW [23,24].…”
Section: Introductionmentioning
confidence: 99%