2020
DOI: 10.1364/oe.383754
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OPCPA investigation with control over the temporal shape of 1.2 ps pump pulses

Abstract: We report a study of a compact, scalable up to TW peak power OPCPA with ∼1.2 ps pump pulses delivered from a Yb:YAG laser. Passive synchronization was ensured by using a small portion of the energy to generate a stable supercontinuum in the YAG, and the rest was directed to pump the three OPCPA stages. The temporal shape of the pump pulse was controlled by the degree of depletion of fundamental radiation in a two-cascade second harmonic converter. Under optimal conditions, the energy of amplified pulses reache… Show more

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Cited by 8 publications
(4 citation statements)
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“…To this end, a compact, wavelength-tunable between 700 and 900 nm OPCPA fully based on 1-ps Yb:YAG Innoslab amplifier was designed to provide sub-30 fs pulses with 11.4 W average power at a 3.25 MHz repetition rate 115 (not shown in Fig. 5 to keep convenient aspect ratio of the plot) and several conceptually similar OPCPA setups operating at low (1 kHz) repetition rates were demonstrated as well 116,117 .…”
Section: Fig 4 | Graphical Summary Of the Performance Of Multi-millij...mentioning
confidence: 99%
“…To this end, a compact, wavelength-tunable between 700 and 900 nm OPCPA fully based on 1-ps Yb:YAG Innoslab amplifier was designed to provide sub-30 fs pulses with 11.4 W average power at a 3.25 MHz repetition rate 115 (not shown in Fig. 5 to keep convenient aspect ratio of the plot) and several conceptually similar OPCPA setups operating at low (1 kHz) repetition rates were demonstrated as well 116,117 .…”
Section: Fig 4 | Graphical Summary Of the Performance Of Multi-millij...mentioning
confidence: 99%
“…For these reasons SC generation emerges as the only reliable seed source for ultrafast optical parametric amplifiers (OPAs) [3][4][5], offering high energy stability, excellent pulse compressibility along with preservation of stable carrier envelope phase, and low time jitter between the pump and seed pulses [6]. SC generation is also widely exploited in table-top optical parametric chirped pulse amplifiers, either serving as a suitable seed directly, see e.g., [7][8][9][10][11][12] or being employed in the intermediate stages of more complex broadband seed production setups, see [13] for a review.…”
Section: Introductionmentioning
confidence: 99%
“…The highest experimentally-observed SHG efficiencies for picosecond high-repetition-rate lasers in the multi-hundred-Watt average power range are limited to 70% [20,21] and have been achieved with a single-stage SHG in Lithium Triborate (LBO) or beta-Barium Borate (BBO). A very promising approach for improving the SHG efficiency is cascaded SHG [22] which has been demonstrated with efficiencies in the range of 60-70% at 1-kHz repetition rate [18,22], and very recently with 85% for a 0.1-kHz system [23]. The first stage in cascaded SHG is used to deplete the most intense parts of the fundamental pulses, resulting in a spatiotemporally flattened fundamental at the output.…”
Section: Introductionmentioning
confidence: 99%
“…These flattened fundamental pulses are then re-used to drive a second SHG stage. Such a flattened pump pulse profile can increase the efficiency of high-power OPA stages, as it lifts the saturation limit to higher pulse energies and reduces the detrimental effects of spectral gain narrowing which is a major concern for efficient few-cycle OPCPA systems [23,24].…”
Section: Introductionmentioning
confidence: 99%