2011
DOI: 10.1364/ol.36.000734
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High-energy temporally shaped nanosecond-pulse master-oscillator power amplifier based on ytterbium-doped single-mode microstructured flexible fiber

Abstract: We present a versatile master-oscillator power amplifier system at 1053 nm in the few-nanoseconds regime meeting the high-level requirements of high-power laser facility front ends. Thanks to temporal shaping, more than 1.5 mJ pulse energy at 1 kHz with an excellent optical signal-to-noise ratio has been obtained in a single-mode 40 µm core flexible fiber.

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Cited by 27 publications
(15 citation statements)
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“…Amplification of nanosecond pulses lies in between, targeting the highest energy per pulse. In the past decade and in the nanosecond regime, many research teams have developed YDFA delivering nanosecond pulses with pulse energy over 1 mJ [22][23][24] and even 25 mJ using Yb-doped large mode area fibers [25][26]. All those results were achieved by cascading multiple YDFA pumped by laser diodes centered at 976 nm and working at a repetition rate around 10 kHz.…”
Section: Introductionmentioning
confidence: 99%
“…Amplification of nanosecond pulses lies in between, targeting the highest energy per pulse. In the past decade and in the nanosecond regime, many research teams have developed YDFA delivering nanosecond pulses with pulse energy over 1 mJ [22][23][24] and even 25 mJ using Yb-doped large mode area fibers [25][26]. All those results were achieved by cascading multiple YDFA pumped by laser diodes centered at 976 nm and working at a repetition rate around 10 kHz.…”
Section: Introductionmentioning
confidence: 99%
“…The well-known phenomena of Stimulated-Brillouin-Scattering (SBS) takes place among the most deleterious limitations for the production of high energies [1][2][3][4] using all-fiber MasterOscillator-Power-Amplifiers (MOPA). They occur in the backward direction of propagation, thus leading to power transmission issues, severe pulse distortions and possibly catastrophic damage effects in the optical components.…”
Section: Introductionmentioning
confidence: 99%
“…Plus or minus efficient techniques may be used to cancel out or reduce SBS effects, using Large-Mode-Area fibers. A very common option is based on the use of active phase-modulation [5,6], to be selected for single-frequency operation [2,3]. Other options [7][8][9][10] either consist of specific fiber core-clad designs or of the application of thermomechanical constraints by external means, when fibers are long enough.…”
Section: Introductionmentioning
confidence: 99%
“…Our MO solution of choice is amplitude-modulated diode lasers [22][23][24]. These lasers naturally support the generation of agile pulse waveforms, in which pulse duration and temporal profile as well as inter-pulse time interval can be dynamically and precisely controlled via electronics on a pulse-to-pulse basis, as demonstrated by their ubiquitous use in optical telecommunication transmitters.…”
Section: Introductionmentioning
confidence: 99%
“…This issue has been addressed by means of specialty fibers, in which fundamental transverse mode operation is retained through particular designs and/or techniques. One example is ''photonic crystal'' fibers (PCFs), in which good BQ from exceedingly large cores (up to 100 lm diameter) is ensured by making the core/cladding index step exceedingly low (core numerical aperture 60.04), which supports the guidance of only few transverse modes [19,[21][22][23]29,30,[32][33][34][35]. This very weak in-core wave-guidance is obtained by means of a carefully designed cross-sectional microstructure of high-index-contrast regions.…”
Section: Introductionmentioning
confidence: 99%