采用圆偏振啁啾飞秒激光脉冲操控CS2分子的相干拉曼散射过程

采用两束圆偏振啁啾飞秒激光脉冲,非共线相干激发三原子分子CS₂液体. 在相位匹配的方向上,探测到由CS₂频率为397 cm^-1的振动模式产生的强度对称分布的相干反斯托克斯拉曼散射(CARS)信号和相干斯托克斯拉曼散射(CSRS)信号. 当调整两束激发光的圆偏振状态时,CARS,CSRS信号的强度、偏振、波长均发生规律性的改变:CARS,CSRS信号的强度分布反映了CS₂ 在不同极化状态下的受激拉曼散射截面大小;信号光的 关键词： 啁啾脉冲 相干反斯托克斯拉曼散射(CARS) 相干斯托克斯拉曼散射(CSRS) 2')" href="#">CS₂     

超短光脉冲波形研究

本文讨论了光脉冲技术发展中的脉冲波形测量问题。介绍了一种通用的光脉冲波形测量新方法,该方法可以给出光脉冲的波形、脉宽以及光脉冲内含的频率啁啾信息。这种测量方法已应用于半导体激光器产生ps光脉冲的实验研究,其可行性得到了验证。     

光纤维中的喇曼混频

我们在656厘米^-1到1343厘米^-1的频率范围研究了光纤维的调谐喇曼混频(RM)效应。在实验中观察到下列现象:相干反斯托克斯喇曼散射(CARS)的大小与逆喇曼吸收(VRA)的大小成反比;RM对受激喇曼散射(SRS)的强度分布有强烈影响。除了观测到相干斯托克斯(CSRS)和CARS辐射,还观测到二级相干斯托克斯(SOCSRS)和相干反斯托克斯(SOCARS)辐射。对实验结果进行了讨论。 关键词：     

固态色散介质中的共心CARS和CSRS

本文报道在一定的设计条件下得到的色散介质方解石晶体中的共心CARS和CSRS的实验。     

利用自相关方法实现光脉冲时间延迟精确测量

为了满足在高精度波分复用/时分复用光采样系统中,采样光脉冲时间抖动低于100 fs的要求,开发了一套基于自相关法测量时间延迟的系统。通过光纤耦合器连接一路参考光路将光脉冲在时域上进行"复制",并使初始光脉冲和"复制"光脉冲相关,得到参考光路和被测光路的精确光程差,进而固定参考光路并接入不同被测光路从而得到多路被测光路之间相对延时。实验结果表明,利用自相关法测量脉冲时间间隔精度优于50 fs,满足波分复用/时分复用光采样系统研究需要。     

相干喇曼散射光谱中干涉效应及偏振特性的研究

本文测量了苯及一些苯衍生物在不同偏振配置下的相干喇曼谱(CARS和CSRS),分析了喇曼共振与双光子吸收共振的干涉作用对光谱线型的影响以及喇曼模的偏振特性与分子振动对称性的关系.     

基于脉冲分组的光剂量监控新算法

精确控制脉冲激光加工光剂量是保证加工产品工艺和质量的关键。在对现有的光剂量控制算法进行分析后,提出了基于脉冲分组的光剂量监控新算法,有效提高了光剂量监测精度和反馈控制速度。设计了光剂量监控系统,实现了脉冲激光加工光剂量实时监测及反馈控制。与Ophir公司的StarLab激光能量测量系统相比,500个激光脉冲以内的总能量测量,本系统测量误差不超过±0.1 5%。对一套脉冲最大重复频率为10 kHz、单脉冲最大能量为5 mJ、恒压工作下最大能量波动为±10%的脉冲激光加工系统光剂量进行了监控实验。在本系统的监控下,可将日标光剂量为150 mJ/mm~2以内的加工光剂量控制精度和重复精度分别控制在0.90%和0.100mJ/mm~2以内,同时将光剂量反馈控制速度提高了4倍。     

铜、溴化铜、铅激光光脉冲的形状和瞬时发散度

本文报道了一种简单的测量光脉冲强度的时空分布方法。用此方法得到Cu/CuBr和Ph激光的具有立体感的光脉冲形状,它包括了光脉冲结构的一些细节,以及光脉冲的瞬时发散度。     

脉冲半导体激光器时基脉冲的实验对比测量

以脉冲半导体激光器为例，对3种测量激光脉冲时基抖动技术进行了对比实验。这3种测量技术分别是：基于宽带取样示波器的时基抖动测量技术;基于相位比较检相器的相位噪声测量技术和基于频谱仪的谐波频谱分析技术。对比研究发现：基于宽带取样示波器的时基抖动测量技术适用于脉冲宽带及脉冲抖动较大的光脉冲；基于频谱仪的谐波频谱分析技术适用于低重复频率光脉冲的抖动测量；基于相位比较检相器的相位噪声技术测量精度高、动态范围大、结果可靠，对于高重复频率的超短光脉冲，建议选用相位噪声测量技术测量激光脉冲的时基抖动。     

高阶相干喇曼散射光谱研究

本文报道了利用YAG激光系统CARS装置研究方解石的高阶相干喇曼散射(CRS)的实验结果,观察到1—6阶相干反斯托克斯喇曼散射谱(CARS)和1—2阶的相干斯托克斯喇曼散射谱(CSRS),讨论了影响高阶CRS产生的因素及有关的问题。 关键词：     

Excitation profiles of resonant coherent Raman scattering by impurity molecules

The amplitudes and the excitation profiles of coherent resonant Raman scattering (coherent anti‐Stokes and Stokes Raman scattering (CARS and CSRS)) by impurity centers in crystals and/or molecules in solutions are studied, taking into account the coherence of the excited mode and the inhomogeneity of the environment. The CARS and CSRS excitation profiles can directly be related to one‐photon absorption when using the transform theory known from spontaneous resonant Raman scattering. The enlargement of the amplitude of the active mode reveals itself in an enhancement of the vibrational overtones. At large amplitudes, a splitting in the profiles caused by the contribution of two turning points of a strong coherent vibration is observed. The inhomogeneous broadening is different in the excitation profiles of CARS and CSRS. The overlapping contributions to spectrally narrow and broad transitions lead to Fano peculiarities. The effects are illustrated by model calculations. Copyright © 2011 John Wiley & Sons, Ltd.     

Chemical imaging of glucose by CARS microscopy

Glucose is one of the most fundamental molecules within life and bioengineering sciences. Present understanding of its role in cellular and bioengineering processes relies primarily on invasive, large‐scale biochemical analysis, providing no spatial information on glucose pools or fluxes. This work identifies an emerging microscopy technique based on coherent anti‐Stokes Raman scattering (CARS), which fulfills the need of quantitative imaging of glucose at the single‐cell level with submicrometer resolution. No sample preparation with reporter molecules is required, ensuring that the low‐weight metabolite is studied under natural conditions. The potential of CARS microscopy is illustrated by quantitatively mapping glucose fluxes and distributions in a microfluidic bioreactor and in lipid‐bilayer vesicles, the latter as a model for glucose transmembrane transport. Furthermore, the metabolic response to a glucose pulse was monitored in living yeast cells. This study signifies a new era within CARS microscopy for its use of monitoring carbohydrates, in particular glucose which is one of the most abundant molecules in nature. Copyright © 2010 John Wiley & Sons, Ltd.     

Selective excitation and suppression of coherent anti-Stokes Raman scattering by shaping femtosecond pulses

Femtosecond coherent anti-Stokes Raman scattering (CARS) suffers from poor selectivity between neighbouring Raman levels due to the large bandwidth of the femtosecond pulses. This paper provides a new method to realize the selective excitation and suppression of femtosecond CARS by manipulating both the probe and pump (or Stokes) spectra. These theoretical results indicate that the CARS signals between neighbouring Raman levels are differentiated from their indistinguishable femtosecond CARS spectra by tailoring the probe spectrum, and then their selective excitation and suppression can be realized by supplementally manipulating the pump (or Stokes) spectrum with the $\pi $ spectral phase step.     

Investigation of vibrational characteristics in BBO crystals by femtosecond CARS

Femtosecond time-resolved coherent anti-Stokes Raman spectroscopy (CARS) is utilized to study the ultrafast vibrational dynamics in BBO crystals at room temperature. Time-resolved two-beam and three-beam CARS are detected. The vibrational dephasing time is analyzed and the changes of vibrational mode intensities with the polarization of pump pulses are observed.     

宽带相干反斯托克斯光谱显微成像技术的实验研究

由于该成像系统采用的超连续谱光源,可以满足所观测样品本源分子在0～4 000 cm-1内的所有拉曼振动活性模式同时共振增强,在探测光的作用下,同时产生宽带相干反斯托克斯拉曼散射信号。然后,根据不同的化学键进行光谱图像重构,可以获得反映不同化学键在样品中的分布的图像。对110 nm的纯的聚苯乙烯珠所形成的具有一定厚度的薄膜,通过改变探测激光与超连续谱脉冲之间的时间重合度,测量形成的相干反斯托克斯拉曼散射信号的时间分布迹线图,通过其中的1 000 cm-1的化学键强度信号进行指数衰减曲线拟合,得出具体的退相时间,与文献中已报道的三色CARS的退相时间相比,判断是否属于三色CARS。为了检验系统在实际生物学成像中存在的问题,我们开展了活体小鼠组织生物学应用成像实验,对记录的数据在2 940 cm-1的CARS信号进行图像重构,获得CH化学键在组织中的分布,然后,对重构图像直接使用小波变换的去噪方式进行图像去噪,去噪后的图像具有比较清晰的轮廓,结果表明,对于对比度比较强的CARS共振信号,直接使用小波变换的去噪方式就可以获得比较好的图像效果。但是,对于信噪比比较差的共振信号,使用这种处理方法是不合适的,需要使用别的方法,先获取好的信号对比度,再根据感兴趣的化学键进行图像重构,然后,再经过小波变换对图像去噪,图像不仅会变得清晰平滑,而且,具有较好的视觉感官效果。     

Broadband coherent anti-Stokes Raman scattering spectroscopy using soliton pulse trains from a photonic crystal fiber

Pulse trains of fundamental soliton pulses with different center wavelengths and delay times from a photonic crystal fiber were generated and used as Stokes optical pulses in coherent anti-Stokes Raman scattering (CARS) spectroscopy. The pulse trains were created by shaping optical pulses with a pulse shaper and their waveforms were measured by a cross-correlation frequency-resolved optical gating method. By the use of pulse trains, the time required for obtaining broadband CARS signals was reduced to be about one third compared with our previous study without using pulse trains. With this setup, broadband CARS signals between 500 and 3100 cm⁻¹ of a single polystyrene bead sample have been measured and the most of the Raman peaks in this frequency range of samples have been observed clearly.     

基于CARS技术的超燃冲压发动机点火过程温度测量

相干anti-Stokes Raman散射（coherent anti-Stokes Raman scattering,CARS）技术作为一种非接触测量手段,已广泛应用于多种发动机模型燃烧室温度测量及地面试验.然而,目前的工作主要集中在稳态燃烧场温度的测量,缺乏用高分辨率的单脉冲来测量瞬变的燃烧火焰温度及组分浓度的研究.基于CARS理论,结合多参数拟合算法,开发了基于MATLAB的CARS光谱计算和拟合程序CARSCF;利用McKenna平面火焰炉在不同工况下进行了温度测量,并与DLR测量结果进行对比,结果显示开发的CARSCF具有较高的测量重复性和准确性;最后将CARS技术应用于测量超燃冲压发动机点火过程中的温度测量,获取了点火过程中的温度.结果显示,在来流Mach数为3的条件下,H₂/air点火过程中温度呈现急剧上升然后缓慢下降,而CARS信号则呈现急剧上升然后急剧下降随后又缓慢上升的趋势,并且在点火过程中最高温度为1 511 K.      

Diagrammatic representation of the third-order polarization in transient CARS

Summary A diagrammatic perturbative approach is adopted to derive the expression for the third-order polarization,P ⁽³⁾ which originates the anti-Stokes emission in a time-resolved CARS experiment. The various contributions toP ⁽³⁾ are calculated assuming that laser fields are off-resonance with respect to any electronic level of material system. The resonant part of the polarization consists of two terms, in which the roles of the pump and probe pulses at frequency ω₁ are exchanged. The global expression allows the direct calculation of the signal time profile in a transient CARS experiment once a model is assumed for the laser pulse shape.