Abstract:OMEGA EP is a large-scale laser system that combines optical parametric amplification and solid-state laser amplification on two beamlines to deliver high-intensity, high-energy optical pulses. The temporal contrast of the output pulse is limited by the front-end parametric fluorescence and other features that are specific to parametric amplification. The impact of the two-crystal parametric preamplifier, pump-intensity noise, and pump-signal timing is experimentally studied. The implementation of a parametric… Show more
“…The formula (5) shows that energies of protons are proportional to the square of the peak intensity, if the other parameters introduced in the equation are fixed. Figure 4 illustrates the cutoff energies (dots in the form of circles, triangles and squares) obtained in numerical calculations as a functions of the peak intensity for different values of the focal spot size.…”
Section: Estimation Of the Peak Laser Intensitymentioning
confidence: 99%
“…The formula (5) has been deduced under the assumption that the shift of protons during the interaction with the laser pulse is negligible as compared with the focal spot size, i.e. the intensity gradient retains its own value in the position of each particle.…”
Section: Estimation Of the Peak Laser Intensitymentioning
confidence: 99%
“…Over the past two decades, significant progress in short-pulse high-power laser technology has resulted in the development of petawatt-class lasers [1][2][3][4][5][6][7][8][9][10][11][12], ten petawatt-class lasers [13][14][15][16][17][18]. Even higher power laser systems have been proposed [19].…”
A new method to diagnose extreme laser intensities through measurement of angular and spectral distributions of protons directly accelerated by the laser focused into a rarefied gas is proposed. We simulated a laser pulse focused by an off-axis parabolic mirror by Stratton-Chu integrals, that enables description of laser pulse with different spatial-temporal profiles focusing in a focal spot down to the diffraction limit, that makes our theoretical predictions be a basis for experimental realization. The relationship between characteristics of the proton distributions and parameters of the laser pulse have been analyzed. The analytical and numerical results obtained justify the new method of laser diagnostics. The proposed scheme should be valuable for the commissioning of new extreme intensity laser facilities.
“…The formula (5) shows that energies of protons are proportional to the square of the peak intensity, if the other parameters introduced in the equation are fixed. Figure 4 illustrates the cutoff energies (dots in the form of circles, triangles and squares) obtained in numerical calculations as a functions of the peak intensity for different values of the focal spot size.…”
Section: Estimation Of the Peak Laser Intensitymentioning
confidence: 99%
“…The formula (5) has been deduced under the assumption that the shift of protons during the interaction with the laser pulse is negligible as compared with the focal spot size, i.e. the intensity gradient retains its own value in the position of each particle.…”
Section: Estimation Of the Peak Laser Intensitymentioning
confidence: 99%
“…Over the past two decades, significant progress in short-pulse high-power laser technology has resulted in the development of petawatt-class lasers [1][2][3][4][5][6][7][8][9][10][11][12], ten petawatt-class lasers [13][14][15][16][17][18]. Even higher power laser systems have been proposed [19].…”
A new method to diagnose extreme laser intensities through measurement of angular and spectral distributions of protons directly accelerated by the laser focused into a rarefied gas is proposed. We simulated a laser pulse focused by an off-axis parabolic mirror by Stratton-Chu integrals, that enables description of laser pulse with different spatial-temporal profiles focusing in a focal spot down to the diffraction limit, that makes our theoretical predictions be a basis for experimental realization. The relationship between characteristics of the proton distributions and parameters of the laser pulse have been analyzed. The analytical and numerical results obtained justify the new method of laser diagnostics. The proposed scheme should be valuable for the commissioning of new extreme intensity laser facilities.
“…However, the pulse energy of the directly generated mode-locked lasers is very low such that it restricts their applications. To solve this problem, different types of laser amplifiers are utilized, in which a regenerative amplifier is considered to be the most effective method for strong amplification of the mode-locked pulses [1,2,12,13]. In most cases, increasing the repetition rate and power can improve the efficiency of laser processing and laser ranging.…”
A non-pulse-leakage optical fiber pumped 100-kHz level high beam quality Nd:YVO 4 picosecond amplifier has been developed. An 80 MHz, 11.5 ps mode-locked picosecond laser is used as the seed with single pulse energy of 1 nJ. By harnessing the double β-BaB 2 O 4 (BBO) crystal Pockels cells in both the pulse picker and regenerative amplifier, the seed pulse leakage of the output is suppressed effectively with an adjustable repetition rate from 200 to 500 kHz. Through one stage traveling-wave amplifier, a maximum output power of 24.5 W is generated corresponding to the injected regenerative amplified power of 9.73 W at 500 kHz. The output pulse duration is 16.9 ps, and the beam quality factor M 2 is measured to be 1.25 with near-field roundness higher than 99% at the full output power.
“…To generate 1053 nm high-contrast seed pulses, many groups used optical parametric amplification (OPA) pumped by high-contrast psduration pulses which shared the same seed with the signal pulses [3][4][5][6][7] . With high-contrast seed injection, the contrast of the amplified pulse in the Nd:glass CPA systems had been improved, respectively [5][6][7][8] .…”
We demonstrate a high-contrast, joule-level Nd:glass laser system operating at 0.5 Hz repetition rate based on a double chirped pulse amplification (CPA) scheme. By injecting high-contrast, high-energy seed pulses into the Nd:glass CPA stage, the pulse energy is amplified to 1.9 J through two optical parametric CPA stages and two Nd:glass amplifiers. The temporal contrast of compressed pulse is measured down to the level of 10 −8 at tens of ps, and 10 −10 near 200 ps before the main pulse, respectively.
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