“…This generation of high energy, highly charged heavy ions with the intense laser field may lead to a new approach for laser-driven extraction and acceleration of exotic nuclei, especially of unstable nuclei with extremely short life times, which cannot be investigated with present high energy ion accelerators [4]. J-KAREN is a PW-class Ti:sapphire laser developed at KPSI [5]. This laser system, after initial operation in 2000, has been improved to reduce prepulses for higher contrast to ~ 2x10 12 by introducing optical parametric chirped-pulse Figure 1.…”
Section: Ultrashort Pulse Laser For High Field Science: J-karenmentioning
Following three different types of high power lasers at Kansai Photon Science Institute are overviewed and controlling the laser damages in these laser systems are described: (1) PW-class Ti:sapphire laser for high field science, (2) zigzag slab Nd:glass laser for x-ray laser pumping, and (3) high-repetition Yb:YAG thin-slab laser for THz generation. Also reported is the use of plasma mirror for characterization of short-wavelength ultrashort laser pulses. This new method will be useful to study evolution of plasma formation which leads to laser damages.
“…This generation of high energy, highly charged heavy ions with the intense laser field may lead to a new approach for laser-driven extraction and acceleration of exotic nuclei, especially of unstable nuclei with extremely short life times, which cannot be investigated with present high energy ion accelerators [4]. J-KAREN is a PW-class Ti:sapphire laser developed at KPSI [5]. This laser system, after initial operation in 2000, has been improved to reduce prepulses for higher contrast to ~ 2x10 12 by introducing optical parametric chirped-pulse Figure 1.…”
Section: Ultrashort Pulse Laser For High Field Science: J-karenmentioning
Following three different types of high power lasers at Kansai Photon Science Institute are overviewed and controlling the laser damages in these laser systems are described: (1) PW-class Ti:sapphire laser for high field science, (2) zigzag slab Nd:glass laser for x-ray laser pumping, and (3) high-repetition Yb:YAG thin-slab laser for THz generation. Also reported is the use of plasma mirror for characterization of short-wavelength ultrashort laser pulses. This new method will be useful to study evolution of plasma formation which leads to laser damages.
“…High-energy lasers using neodymium doped glass extend their capability toward shorter pulse duration and improved temporal pulse contrast necessary for such applications using optical parametric chirped-pulse amplification (OPCPA) [6,7] . Lasers relying on titanium doped sapphire (Ti 3+ :Al 2 O 3 /TiSa) currently demonstrate the highest peak power for pulses in the sub-50 fs range [5,[8][9][10][11] . However, all those systems rely on flash lamps to some extent and are thus limited in pulse repetition rate due to thermal load.…”
We report on the energetic and beam quality performance of the second to the last main amplifier section HEPA I of the PEnELOPE laser project. A polarization coupled double-12-pass scheme to verify the full amplification capacity of the last two amplifiers HEPA I and II was used. The small signal gain for a narrow-band continuous wave laser was 900 and 527 for a broadband nanosecond pulse, demonstrating 12.6 J of output pulse energy. Those pulses, being spectrally wide enough to support equivalent 150 fs long ultrashort pulses, are shown with an excellent spatial beam quality. A first active correction of the wavefront using a deformable mirror resulted in a Strehl ratio of 76% in the single-12-pass configuration for HEPA I.
“…In the context of the continuously increasing average power of high-energy class diode pumped solid-state lasers (HECDPSSLs), careful treatment of the thermal effects due to the parasitic absorption of power in optical components has become tremendously important for the further development of HEC-DPSSLs [1][2][3][4] . One of the most seriously affected optical components is the Faraday isolator (FI), because of the relatively high absorption (∼10 −3 cm −1 ) of the currently available magneto-optical elements (MOEs).…”
Faraday effect measurements of holmium oxide (Ho 2 O 3 ) ceramics-based magneto-optical materials, highly potential material candidates for high-energy laser Faraday isolators, are presented in this paper. Temperature dependence of the Verdet constant of nondoped Ho 2 O 3 ceramics was measured for temperatures 15-305 K at 1.064 µm wavelength. The Verdet constant dispersion for wavelengths 0.5-1 µm and 1.064 µm was measured for both nondoped Ho 2 O 3 ceramics and Ho 2 O 3 ceramics doped with terbium Tb 3+ (0.2 at. %) and cerium Ce 3+ (0.1 at. %) ions. The results suggest that the relatively low level of doping of Ho 2 O 3 with these ions has no significant boosting impact on the Faraday effect. Therefore, other compositions of Ho 2 O 3 ceramics-based magneto-optical materials, as well as various doping concentrations, should be further examined.
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