共查询到20条相似文献,搜索用时 0 毫秒
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要建造大功率超强激光系统,必须将nJ量级的种子进行放大,以得到mJ量级以及更高能量的激光输出.为达到这个目的,必须使种子能量指数增加,再生腔放大器是实现这一目的的良好途径;同时,为了得到更稳定的激光输出,须采用高重复频率的泵浦源.为此,设计了一种kHz重复频率激光泵浦的再生放大器,使用15 mJ的527 nm的绿光泵浦,得到了约2.3 mJ的800 nm放大激光输出,同时,对其输出激光的光谱特性进行了测量,将带宽为40 nm的种子注入后,得到了光谱带宽约为30 nm激光输出. 相似文献
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《Current Applied Physics》2015,15(4):468-472
We developed a highly efficient and compact Ti:sapphire multipass amplifier that uses divergent seed beams to generate 20 TW/40 fs laser pulses with a repetition rate of 10 Hz. The laser system consists of a mode-locked oscillator, a regenerative amplifier, and a multipass power amplifier. The thermal lensing effect is very important in this system, especially in the multipass amplifier, as it limits the conversion efficiency. In order to compensate the thermal lensing effect, we calculated the optimum divergence of the seed beam and used the result for the multipass amplifier, where the thermal focusing is taken into account. In this way, we achieved a very high conversion efficiency of 41%, which is close to the theoretical limit. The laser system was then used with a capillary gas cell to generate stable high-energy electron beams with electron energies of about 150 MeV and a beam divergence of 4 ± 1 mrad. In this paper, details of the laser system development and experimental results for electron generation are presented. 相似文献
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介绍了基于啁啾脉冲放大(CPA)技术的100 TW级钛宝石激光装置SILEX-I。SILEX-I装置主要包括飞秒振荡器、Offner展宽器、多级放大器、以及对应的脉冲压缩器和靶室等。该装置可以输出5,30,100 TW级3个功率段,并分别配套相应的靶室系统,可以满足多种物理实验的需求。目前该装置的末级输出峰值功率达到286 TW,脉宽29.8 fs,靶面聚焦功率密度达到3.36×1020 W/cm2。 相似文献
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讨论了TW级飞秒激光放大装置中的同步时序系统原理,介绍了自行设计并建造的3套频率成分各异的TW级钛宝石飞秒激光放大装置,其中“极光Ⅱ” 和“Titan”为两级放大系统,前者预放大与主放大重复频率均为10 Hz,后者采用1 kHz的预放大和10 Hz的主放大,“极光Ⅲ”为多级放大系统,预放大重复频率为10 Hz,主放大分别为1 Hz和15 min输出一发。针对各个放大装置的不同特点和对同步精度的具体要求,自行设计并建造了不同的同步时序控制系统,实现了各个激光放大系统的有效运转,同步精度达到200 ps。 相似文献
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讨论了TW级飞秒激光放大装置中的同步时序系统原理,介绍了自行设计并建造的3套频率成分各异的TW级钛宝石飞秒激光放大装置,其中极光Ⅱ和Titan为两级放大系统,前者预放大与主放大重复频率均为10 Hz,后者采用1 kHz的预放大和10 Hz的主放大,极光Ⅲ为多级放大系统,预放大重复频率为10 Hz,主放大分别为1 Hz和15 min输出一发。针对各个放大装置的不同特点和对同步精度的具体要求,自行设计并建造了不同的同步时序控制系统,实现了各个激光放大系统的有效运转,同步精度达到200 ps。 相似文献
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Jin Woo YoonSeong Ku Lee Tae Jun YuJae Hee Sung Tae Moon JeongJongmin Lee 《Current Applied Physics》2012,12(3):648-653
We design a two-stage non-collinear optical parametric chirped pulse amplifier using BBO crystals for a high-power Ti:sapphire laser system, and numerically analyze the output characteristics of the OPCPA system. We find optimal phase-matching conditions and calculate the parametric gains as a function of pump intensity and interaction length. By constructing a two-stage OPCPA system using two BBO crystals, we obtain 12 mJ output energy corresponding to a high gain of 107, a pulse duration of 37 fs, and a contrast ratio of 5×10−8. 相似文献
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Christoph Wandt Sandro Klingebiel Sebastian Keppler Marco Hornung Markus Loeser Mathias Siebold Christoph Skrobol Alexander Kessel Sergei A. Trushin Zsuzsanna Major Joachim Hein Malte C. Kaluza Ferenc Krausz Stefan Karsch 《Laser \u0026amp; Photonics Reviews》2014,8(6):875-881
In this paper the development and implementation of a novel amplifier setup as an additional stage for the CPA pump laser of the Petawatt Field Synthesizer, currently developed at the Max‐Planck‐Institute of Quantum Optics, is presented. This amplifier design comprises 20 relay‐imaged passes through the active medium which are arranged in rotational symmetry. As the gain material, an in‐house‐developed Yb:YAG active‐mirror is used. With this setup, stretched 4 ns seed pulses are amplified to output energies exceeding 1 J with repetition rates of up to 2 Hz. Furthermore, a spectral bandwidth of 3.5 nm (FWHM) is maintained during amplification and the compression of the pulses down to their Fourier‐limit of 740 fs is achieved. To the best of our knowledge, this is the first demonstration of 1 TW pulses generated via CPA in diode‐pumped Yb:YAG. 相似文献
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Ito S. Ishikawa H. Miura T. Takasago K. Endo A. Torizuka K. 《Applied physics. B, Lasers and optics》2003,76(5):497-503
We present a 7-TW Ti:sapphire laser system operating at 50 Hz for laser Compton femtosecond X-ray generation. This laser system
delivers 8.4 W of average output power at a repetition rate of 50 Hz with a pulse width of 24 fs. It demonstrates successful
management using a dynamically stable resonator in the regenerative amplifier and compensation for thermal lensing by a convex
mirror in a ring-type four-pass power amplifier. We also present the results of closed-loop corrections for distorted wavefronts
of amplified and compressed laser pulses, using an adaptive optical system consisting of a Shack–Hartmann-type wavefront sensor
and a deformable mirror. This closed-loop correction results in dramatic improvements, reducing wavefront distortions below
0.05 λ rms.
Received: 31 October 2002 / Revised version: 3 March 2003 / Published online: 5 May 2003
RID="*"
ID="*"Corresponding author. Fax: +81-298/61-3349, E-mail: ito@festa.or.jp 相似文献
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A hybrid amplifier chain composed of Ti:chrysoberyl and Ti:sapphire is proposed to control spectral gain narrowing in this letter. The Ti:chrysoberyl crystal is employed as the host material of the frontier amplification stage with the polarization parallel to a axis. According to the numerical simulation, the seeding pulse with a proper wavelength center is required to generate a broader spectrum, and spectra broader than 120 nm are available with total net gain from 104 to 1010. The simulation proves that the amplified spectrum can even support pulse shorter than the seed pulse. 相似文献
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A broadband (~ 176 nm, R > 98%, λ0 = 800 nm) and high laser-induced damage threshold (LIDT =2.4 J/cm2) TiO2/HfO2/SiO2 high reflector (HR) for Ti:sapphire chirped-pulse amplification (CPA) laser system is fabricated by the electron beam evaporation. The refractive index and extinction coefficient of TiO2 and HfO2 films are calculated from single-layer films' transmittance spectra. The properties of HR are mainly determined by the high refractive index material. The high refractive index leads to wide bandwidth. A low extinction coefficient indicates low absorption and high LIDT. The possible damage mechanism of HR is discussed. 相似文献
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Hong-jun Liu Wei Zhao Guo-fu Chen Yi-shan Wang Lian-jun Yu Chi Ruan Xue-feng Li 《Optics & Laser Technology》2004,36(4):3482-314
Experimental investigations of a type-I noncollinear phase-matched optical parametric amplification based on lithium triborate, which was pumped by a 5-ns second-harmonic pulses from a Q-switched Nd:YAG, seeded by a cw Ti:sapphire laser at 800 nm, was presented. The experiments generated 2-ns signal output pulses at 800 nm, the maximum signal output pulse energy reached 19 μJ, the corresponding parametric gain was 44 dB. Furthermore, the experiments demonstrate that the 65 nm-FWHM parametric fluorescence gain spectrum could also be observed. A quantitative account of the ultrabroadband parametric fluorescence gain spectrum was given with our theory. The experimental measurements are in agreement with theoretical calculations. 相似文献
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Based on a combined scheme of doubled chirped-pulse amplification and a femtosecond noncollinear optical-parametric amplifier, a high-contrast femtosecond laser pulse with energy of up to 32.3 J has been generated by improving the gain efficiency and boosting the pump energy to 120 J in the final amplifier. Our measurements show that the contrast ratio of the main laser pulse is around 10(10) within the time scale of -400 ps and the duration of compressed pulse is 27.9 fs, corresponding to a peak power of 1.16 PW. 相似文献
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针对啁啾脉冲放大技术建成的钛宝石激光装置,提出一种获得高重复率激光脉冲列的方法.通过改变钛宝石再生放大器中泡克耳斯盒电光开关的传统工作模式,使得腔内放大的脉冲从某特定时刻起,每当在腔内往返一次就以一定的倒出比例(倒出率)倒出腔内脉冲能量的一部分,从而可以在有限的时间段内产生高重复率的啁啾激光脉冲列.基于Franz-Nodvik放大理论,建立了该高重复率再生放大器的理论模型,通过数值计算,系统地分析了初始增益、倒出时刻、倒出率对输出的脉冲序列的影响.在抽运功率为35mJ、倒出率为1/2的实验条件下,通过腔外的脉冲数量选择器,在一个抽运周期内的有限时间段内已获得了14个幅度相近、单脉冲能量约为0.02mJ、重复率为100MHz的啁啾脉冲序列.从此啁啾脉冲列中选取数个脉冲,通过10TW级的激光系统放大和压缩,已获得100MHz重复率的飞秒太瓦级脉冲列.
关键词:
高重复率
多通放大
啁啾脉冲放大
钛宝石激光器 相似文献
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S. Ito H. Nagaoka T. Miura K. Kobayashi A. Endo K. Torizuka 《Applied physics. B, Lasers and optics》2002,74(4-5):343-347
We have measured detailed thermal lensing in a power amplifier of a terawatt Ti:sapphire laser operating at 50 Hz. The thermal
lensing in the amplifier was evaluated by measuring the optical path difference (OPD) using a Shack–Hartmann-type wavefront
sensor. It was found that the radial dependence of the OPD was almost quadratic in the pumping region, despite inhomogeneous
pumping. Therefore, a simple spherical lens or convex mirror effectively compensates for the thermal lens in our amplifier.
We found that the thermal lens profile was temporally stable, and did not degrade the pointing stability of the amplified
laser pulses. We also found that the time constant of the thermal distortion in our power amplifier was approximately 0.5 s.
Received: 3 September 2001 / Revised version: 23 January 2002 / Published online: 14 March 2002 相似文献
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We demonstrate the direct generation of 12 fs pulses from a Ti:sapphire regenerative amplifier system at a 1 kHz repetition rate utilizing properly designed broadband components for chirped-pulse amplification. Optimized designs of a regenerative amplifier with a multilayer gain-narrowing compensator and an adaptive dispersion compensator with a spatial light modulator contribute to the shorter pulse amplification. 相似文献