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超短激光脉冲对比度的三阶相关测量 总被引:4,自引:3,他引:1
在超强超短激光脉冲与物质相互作用过程中,良好的激光脉冲对比度是一个非常重要的参数指标.为了扩大对超短激光脉冲对比度的测量范围,准确地测量超短激光脉冲的对比度,利用非线性晶体对激光脉冲强度变化十分敏感的特性,研究了超短激光脉冲三阶相关信号的产生过程,并在此基础上,研制了一台三阶相关仪,对一台飞秒激光振荡器进行了脉冲对比度的测量研究.测量结果表明,通过在测量光路中加入聚焦透镜进行聚焦准直,可以有效提高激光脉冲的倍频效率,从而大幅提高该三阶相关仪的可测动态范围.该测量系统目前可实现的可测动态范围达到约108. 相似文献
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高能量低重复频率超短激光脉冲的测量 总被引:2,自引:0,他引:2
利用非线性晶体 (BBO)的非共线匹配倍频效应 ,研制了实时测量高能量低重复频率超短激光脉冲宽度的单脉冲自相关仪 ,并对飞秒 (fs)参量放大器的输出脉冲宽度进行了测量 ,测得了 10 3fs的超短激光脉冲宽度。 相似文献
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基于超短脉冲激光光谱技术诊断癌症的研究 总被引:1,自引:1,他引:0
目的:研究用于癌症诊断与治疗的光敏剂血卟啉(HPD)的超快光动力学过程;方法:采用超短脉冲激光光谱技术和皮秒时间相关单光子计数系统,测量经血卟啉培养的活体癌细胞与正常细胞的荧光光谱、荧光寿命特性及荧光峰值强度随时间变化曲线,并测量单一细胞内部不同位置的荧光寿命特性;结果:癌细胞样品在645nm处具有特有的光谱谱峰;癌细胞样品荧光寿命的快成分约150ps慢成分约1200ps,而正常细胞样品快成分约300ps慢成分约2500ps;癌细胞样品的荧光峰值强度经12小时衰减约10%,而正常细胞样品衰减约55%;在细胞内部荧光寿命300ps的快成分十分显著,且中心部位血卟啉浓度最高;结论:癌细胞与正常细胞的荧光光谱、荧光寿命特性及荧光峰值强度随时间变化曲线相差十分明显,反映了癌细胞与正常细胞对血卟啉亲和性有显著的差异;测量结果确认了荧光光谱技术诊断与治疗癌症的可行性,并对发展超短脉冲激光光谱技术早期诊断与治疗癌症具有重要的指导意义和临床应用价值。 相似文献
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研究了从亚皮秒到皮秒范围内的不同脉宽和不同能量密度的激光作用下单晶硅材料表面瞬态光学性质的演化规律。这项工作基于考虑了相变潜热的双温方程、载流子数密度模型,通过计算激光辐照过程中的载流子温度、晶格温度和激发态载流子数密度和介电常数,模拟了光子到电子以及电子到声子的能量传递过程,最终得到了单晶硅表面折射率和消光系数的变化结果。有助于揭示亚皮秒到皮秒脉冲宽度范围的超短脉冲激光辐照下,单晶硅材料瞬态光学性质的演化机理。理论结果表明,若单个激光脉冲无法使单晶硅熔化,则不同的激光能量密度和不同的激光脉宽对最小折射率的影响非常有限,在0.3~0.4 J/cm2的激光能量密度范围内,每0.01 J/cm2的能量密度改变引起的最小折射率变化率小于0.5%。若单个激光脉冲能使单晶硅熔化,则不同能量密度和不同脉宽的激光对硅表面的折射率和消光系数有不同程度的影响。该研究结果可为基于超短脉冲激光的单晶硅材料加工和表面改性提供一定的理论指导。 相似文献
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皮秒和飞秒激光技术的迅速发展,为激光等离子体物理开辟了新的理论和实验研究领域.自生磁场是激光与等离子体相互作用中很多物理过程的结果,反过来,自生磁场又对等离子体的运动产生直接或间接的影响.到目前为止,对环形磁场的理论和实验研究比较多.相比之下,对轴向磁场的探索则很不充分,尤其在超短激光脉冲与等离子体作用中,对轴向磁场的研究尚属空白.本文利用法拉第效应,对超短激光脉冲同等离子体相互作用中产生的轴向磁场进行了首次测量.实验中通过引入延迟光路的方法,大大降低了打靶激光发与发之间的涨落带来的误差.使用飞… 相似文献
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Akhmanov S. Chirkin A. Drabovich K. Kovrigin A. Khokhlov R. Sukhorukov A. 《Quantum Electronics, IEEE Journal of》1968,4(10):598-605
A theory of nonstationary nonlinear wave phenomena occurring in the field of ultrashort high-intensity light pulses is developed (harmonic generation and parametric amplification stimulated Raman scattering). The main equations are given, the group velocity mismatch effects are studied, and special attention is paid to the high-conversion conditions. The possibilities of picosecond pulse narrowing on account of linear and nonlinear nonresonance parametric amplification and harmonic generation are studied in detail. The factors that determine the minimum light-pulse duration (dispersion broadening) are examined. A nonstationary theory of stimulated Raman scattering (SRS) is developed. Expressions for minimum pulse duration in forward and backward SRS are given. Reduction of Raman amplification with a picosecond pump is discussed. 相似文献
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A new technique for the display of picosecond light pulses is presented. Ultrashort (6 ps) green light pulses passing through a light-scattering medium are photographed from the side by a camera positioned behind a shutter of 10-ps framing time. The shutter is an ultrafast Kerr cell driven by infrared pulses 8 ps in duration. Color photographs show a bright spot on a dark background, revealing the unambiguous presence of well-isolated picosecond light pulses. The shape of the spot is the result of a convolution involving the three-dimensional shape of the green pulse and the time transmission function of the shutter, this function being dictated by the shape of the infrared pulse. The experiment indicates that a new technique for visualizing light pulses consists in simply observing their flight through a scattering medium from behind an ultrafast shutter having a framing time equal to the time resolution desired. The new technique has many advantages over the two-photon fluorescence display technique, such as higher sensitivity, wider spectral range, and easier interpretation. The ultrafast camera also can be used for the photographic measurement of ultrashort relaxation times in dielectrics and in fluorescent dyes. 相似文献
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In this paper, we extend the recently introduced linear technique for temporal phase reconstruction using optical ultrafast differentiation (PROUD) to achieve full characterization of ultrashort optical pulses with durations down to the picosecond regime using a well-characterized temporal stretcher (e.g., dispersive optical fiber). The proposed method is experimentally demonstrated by precisely characterizing the amplitude and phase temporal profiles of microwatt-power picosecond pulses ranging from 4 to 20 ps with both continuous and discrete temporal phase variations. Using this simple mechanism, the same PROUD setup can be used to characterize optical pulses with durations ranging from the picosecond to the nanosecond regime. We provide a comprehensive mathematical analysis of this general PROUD technique: we evaluate in detail the influence of the key specifications (e.g., different sources of noise) of the used components and instruments, namely, optical differentiator, linear temporal stretcher, and time-domain intensity test equipment, on the performance of the PROUD measurement system, particularly in terms of phase sensitivity in the optical pulse characterization. 相似文献
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In a non-Gaussian noise environment, it is theoretically possible to design a delay estimator that performs significantly better than the conventional linear correlator. We study the maximum likelihood estimator for passive time delay in non-Gaussian noise. We show that the form of the best estimator depends strongly on signal-to-noise ratio (SNR), and the estimator optimal at low SNR can fail catastrophically at high values of SNR. The paper uses simulations to examine this sensitivity problem and proposes an ad hoc instrumentation that is reasonably robust over a wide range of SNR values 相似文献
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《IEEE transactions on information theory / Professional Technical Group on Information Theory》1968,14(3):382-389
The detection of stationary Gaussian signals in a background of stationary Gaussian noise by the analog multiplier correlator, the polarity coincidence correlator (PCC), and the sample polarity coincidence correlator (SPCC) is considered. It is assumed that signal and noise have identical normalized autocovariance functions, and they are not cross correlated with each other. The main contributions of this paper are the exact expressions for the output signal-to-noise ratio (SNR) for the correlators mentioned for all values of the input SNR. It is shown that there exists a critical value of the input SNR, such that, whenever this value is exceeded, the PCC output SNR exceeds that of the analog correlator. A sufficient condition for this gain in output SNR is obtained in terms of the input SNR. This result is illustrated for stationary Gauss-Markov processes. 相似文献