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1.
We present a novel technique that intrinsically mitigates the quantum-defect heating in Raman lasers. The basic principle of this so-called "coherent anti-Stokes Raman scattering (CARS)-based heat mitigation" is to suppress the phonon creation in the Raman medium by increasing the number of out-coupled anti-Stokes photons with respect to the number of out-coupled Stokes photons. We demonstrate with the aid of numerical simulations that for a hydrogen and a silicon Raman laser, CARS-based heat mitigation efficiencies of at least 30% and 35%, respectively, can be obtained.  相似文献   

2.
The feasibility of Raman spectroscopy and temperature measurements in gases by Coherent Anti-Stokes Scattering is discussed and demonstrated experimentally. Results are presented for H2 gas at room temperature and also for H2 liberated by pyrolysis in a Bunsen flame.  相似文献   

3.
Using a specially designed excimer-laser-pumped dye laser of adjustable bandwidth high-lying pure rotational transitions of both, ortho-and para-hydrogen have been identified by coherent anti-Stokes Raman scattering (CARS). As an interesting application H2-based CARS-thermometry is discussed.  相似文献   

4.
Conditions to get Coherent Anti-Stokes Raman Spectra for strong one-photon-resonance are given. The biharmonic pump was realized by a high power ns-ruby-laser and a broadband dye-laser, focussed together into a small sample cell. Resonance Raman spectra of an extension of some hundreds cm-1 are obtained during one laser shot, thus opening possibilities to investigate excited electronic states or short-living molecules.  相似文献   

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为了解决相干反斯托克斯喇曼散射(CARS)光谱CARSFT计算程序在温度拟合过程中,对初值依赖大、测量光谱信噪比差、不易收敛的问题,通过分析非线性迭代算法,采用了阻尼最小二乘算法对氮气CARS光谱进行温度拟合。针对CARS理论光谱计算公式较为复杂的特点,采用数值差分的方式来获得迭代计算时所需要的设计矩阵。分析了横向偏移、纵向偏移和温度三个主要参量对拟合残差的影响,发现纵向偏移的初值设置对温度拟合影响较大。拟合温度2000 K时的标准理论CARS光谱,设置偏离较大的初始值,采用阻尼最小二乘法获得了较好的结果。迭代计算167步后,温度拟合为2 005.6 K,残差为0.027 463。拟合光谱信噪比较差的CARS光谱,阻尼最小二乘法也能稳定收敛。结果验证了阻尼最小二乘法对初值的依赖不大,并且当拟合谱信噪比较差时也能收敛,可用于在恶劣环境下CARS测量光谱的拟合。  相似文献   

7.
By tailoring the phase of a 100 femtosecond probe pulse we are able to obtain a narrow-band coherent anti-Stokes Raman spectroscopy (CARS) resonant signal with a width of less than 15 cm(-1), which is an order of magnitude narrower than the CARS signal from a transform limited pulse. Thus, by measuring the spectrum of the CARS signal we are able to obtain a high-resolution energy level diagram of the probed sample in spite of the broad femtosecond pulse spectrum.  相似文献   

8.
Time-domain coherent anti-Stokes Raman scattering experiments have been carried out by probing vibrational and pure rotational lines of nitrogen in the Doppler broadened regime. The theoretical analysis of the transient responses outlines the role of the geometrical effects. For pure rotational CARS, it is shown that the main contribution to the dephasing of the Raman coherence results from the change in direction between the pump and anti-Stokes wave vectors whereas the difference between the modulus of these two wave vectors accounts for dephasing in vibrational CARS. Furthermore, we demonstrate that the range of operation of time-domain CARS velocimetry is extended by probing pure rotational lines. The predictions are validated by experiments which are performed both in a static gas cell and in a Mach 10 supersonic flow. Received: 30 March 2000 / Revised version: 9 June 2000 / Published online: 13 September 2000  相似文献   

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An argon ion laser and metal halide arcs are used to measure the depolarization ratios for anti-Stokes electronic Raman scattering from indium and thallium atoms. A comparison with theoretical results obtained using different assumptions about the relative phases of radial matrix elements gives conclusive evidence about which relative phases are correct. This information is essential to make a calculation of nonresonant Raman scattering cross sections possible.  相似文献   

11.
Wang K  Xu C 《Optics letters》2011,36(21):4233-4235
We demonstrate a two-color, fiber-delivered picosecond source for coherent Raman scattering (CRS) imaging. The wavelength-tunable picosecond pump is generated by nonlinear spectral compression of a prechirped femtosecond pulse from a mode-locked titanium:sapphire (Ti:S) laser. The 1064?nm picosecond Stokes pulse is generated by an all-fiber time-lens source that is synchronized to the Ti:S laser. The pump and Stokes beams are combined in an optical fiber coupler, which serves not only as the delivery fiber but also as the nonlinear medium for spectral compression of the femtosecond pulse. CRS imaging of mouse skin is performed to demonstrate the practicality of this source.  相似文献   

12.
Ganikhanov F  Evans CL  Saar BG  Xie XS 《Optics letters》2006,31(12):1872-1874
We demonstrate a new approach to coherent anti-Stokes Raman scattering (CARS) microscopy that significantly increases the detection sensitivity. CARS signals are generated by collinearly overlapped, tightly focused, and raster scanned pump and Stokes laser beams, whose difference frequency is rapidly modulated. The resulting amplitude modulation of the CARS signal is detected through a lock-in amplifier. This scheme efficiently suppresses the nonresonant background and allows for the detection of far fewer vibrational oscillators than possible through existing CARS microscopy methods.  相似文献   

13.
We report all-UV coherent anti-Stokes Raman scattering (CARS) in calcite with 250-280 nm pump, Stokes, probe, and anti-Stokes light. UV CARS efficiency is approximately 7x higher than for comparable scattering in the visible, 480-540 nm. Time-resolved UV CARS reveals lengthening of the dephasing time of 1086 cm(-1) CO3(2-) internal vibrations from 4 to 7 ps with increasing vibrational excitation, consistent with a phonon depletion model.  相似文献   

14.
Polarization coherent anti-Stokes Raman scattering microscopy   总被引:3,自引:0,他引:3  
Cheng JX  Book LD  Xie XS 《Optics letters》2001,26(17):1341-1343
We report polarization coherent anti-Stokes Raman scattering (P-CARS) microscopy that allows vibrational imaging with high sensitivity and spectral selectivity. The nonresonant background signals from both Raman scatterers and the solvent are efficiently suppressed in P-CARS microscopy. We demonstrate P-CARS imaging of unstained cells based on the contrast of the protein amide I band.  相似文献   

15.
We report a novel Fourier-transform-based implementation of coherent anti-Stokes Raman scattering (CARS) microscopy. The method employs a single femtosecond laser source and a Michelson interferometer to create two pulse replicas that are fed into a scanning multiphoton microscope. By varying the time delay between the pulses, we time-resolve the CARS signal, permitting easy removal of the nonresonant background while providing high resolution, spectrally resolved images of CARS modes over the laser bandwidth (approximately 1500 cm(-1)). We demonstrate the method by imaging polystyrene beads in solvent.  相似文献   

16.
New applications of a nonlinear optical microscope using coherent anti-Stokes Raman scattering (CARS) are presented. Excellent molecular discrimination using chemically similar molecular species and signal contrast enhancement using digital image processing are demonstrated. Limitations of the technique and future applications are discussed.  相似文献   

17.
Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 48, No. 4, pp. 574–579, April, 1988.  相似文献   

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相干反斯托克斯拉曼散射显微成像技术研究   总被引:1,自引:0,他引:1       下载免费PDF全文
刘双龙  刘伟  陈丹妮  屈军乐  牛憨笨 《物理学报》2016,65(6):64204-064204
基于全量子理论对相干反斯托克斯拉曼散射(CARS)过程进行了分析, 在此基础上搭建了单频CARS显微成像系统, 获得了不同尺寸聚苯乙烯微球高对比度的CARS显微图像. 为了标定成像系统的空间分辨率, 采用逐点扫描方式对直径为110 nm聚苯乙烯微球成像, 从而重构出系统的点扩展函数. 结果表明: 该CARS显微成像系统的横向空间分辨率约为600 nm, 而由阿贝衍射极限决定的理论空间分辨率约为300 nm. 分析了导致分辨率降低的原因, 并提出了解决方案. 为实现纳米分辨的CARS显微成像打下了坚实的基础.  相似文献   

20.
尹君  于凌尧  刘星  万辉  林子扬  牛憨笨 《中国物理 B》2011,20(1):14206-014206
In broadband coherent anti-Stokes Raman scattering (CARS) spectroscopy with supercontinuum (SC), the simultaneously detectable spectral coverage is limited by the spectral continuity and the simultaneity of various spectral components of SC in an enough bandwidth. By numerical simulations, the optimal experimental conditions for improving the SC are obtained. The broadband time-resolved CARS spectrography based on the SC with required temporal and spectral distributions is realised. The global molecular vibrational spectrum with well suppressed nonresonant background noise can be obtained in a single measurement. At the same time, the measurements of dephasing times of various molecular vibrational modes can be conveniently achieved from intensities of a sequence of time-resolved CARS signals. It will be more helpful to provide a complete picture of molecular vibrations, and to exhibit a potential to understand not only both the solvent dynamics and the solute-solvent interactions, but also the mechanisms of chemical reactions in the fields of biology, chemistry and material science.  相似文献   

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