2019
DOI: 10.1364/ol.44.004359
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High-efficiency second-harmonic generation of low-temporal-coherent light pulse

Abstract: The nonlinear frequency conversion of low-temporal-coherent light holds a variety of applications and has attracted considerable interest. However, its physical mechanism remains relatively unexplored, and the conversion efficiency and bandwidth are extremely insufficient. Here, considering the instantaneous broadband characteristic, we establish a model of second harmonic generation (SHG) of low-temporal-coherent pulse, and reveal its differences from the coherent conditions. It is found that the second harmo… Show more

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Cited by 38 publications
(14 citation statements)
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“…The internal 12 bit AD conversion cycle is only 4S, which is several times faster than the common AD574 (conversion cycle 22s) [8]. After rough estimation, if a conventional chip is used to form a data acquisition module with the same performance as adc812, one chip of 8031, one chip of ad57427642816, two chips of dac80, and several chips of decoder, register and multi-channel switch are needed [9]. Not only the price of these chips is much higher than that of adc812, but also the cost of a single PCB is roughly the same as that of adc812.…”
Section: Design Of Data Acquisition Chipmentioning
confidence: 99%
“…The internal 12 bit AD conversion cycle is only 4S, which is several times faster than the common AD574 (conversion cycle 22s) [8]. After rough estimation, if a conventional chip is used to form a data acquisition module with the same performance as adc812, one chip of 8031, one chip of ad57427642816, two chips of dac80, and several chips of decoder, register and multi-channel switch are needed [9]. Not only the price of these chips is much higher than that of adc812, but also the cost of a single PCB is roughly the same as that of adc812.…”
Section: Design Of Data Acquisition Chipmentioning
confidence: 99%
“…1−5 Limited by the symmetry of the atomic structure, however, SHG is not supported in centrosymmetric materials. Based on the dipole approximation theory, the second-order nonlinear polarizability vanishes (i.e., χ (2) = 0) in such materials, implying that SHG is forbidden. 6 In order to overcome this limitation, symmetry breaking is generally employed to realize SHG in centrosymmetric materials.…”
Section: ■ Introductionmentioning
confidence: 99%
“…This is not only beneficial for improving the effective absorption of laser by the target and obtaining a higher compression ratio but also helps to suppress the occurrence of parametric instability in large-scale LPI. A superluminescent diode (SLD) pulse source amplified by a Nd/phosphate glass rod laser system is a very ideal seed source for ICF. Because the spectral characteristics of the pulse will not be affected by pulse time shaping. , …”
Section: Introductionmentioning
confidence: 99%
“…Based on the SLD pulse source, a DKDP crystal with a deuterium content of 17% and a size of 200 × 200 mm 2 was used to achieve 65% conversion efficiency at 1057 nm at the retracing point. The fundamental wave energy reached the kilojoule level, and the bandwidth of the second harmonic generation was 3.2 nm. , However, the dispersion of refractive index varies sharply with wavelength during the third-harmonic generation for existing nonlinear optical crystals, which limits the output bandwidth. In addition, there is also a “spectral bottleneck”, which is constrained by the narrow reception bandwidth of existing nonlinear optical crystals .…”
Section: Introductionmentioning
confidence: 99%
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