氯化镍在12900～15000 cm-1的激光诱导荧光光谱

采用激光诱导荧光技术在12900-15000 cm^-1能量范围内研究了超声射流冷却条件下的氯化镍光谱. 通过分析,6个具有转动结构的振转带被归属为跃迁序列. 相关的转动常数、同位素位移以及(平衡)分子常数被确定. 此外, 还测量了这些振转带的寿命.     

激光诱导荧光确定NiB自由基一个新的电子激发态：在19000-22100 cm -1的2II态

Ni针放电产生的Ni原子与B₂H₆反应产生NiB自由基,得到了在19000～22100 cm^-1的激光诱导荧光光谱. 通过对激光诱导荧光激发谱和色散谱的研究,发现了一个新的电子跃迁序列[20.77]²II-X²∑⁺,序列共包括11个振动谱带,光谱分析得到了这个新的电子激发态和基态的跃迁寿命. 在光谱常数和跃迁寿命等数据的基础上,讨论了新发现电子激发态的电子构型.     

Laser-induced Fluorescence Excitation Spectrum of NiS in 15500-17200 cm-1

测量了在15500～17200 cm^-1的超声射流冷却的NiS自由基的激光诱导荧光激发谱. 15条谱带被归属为三个电子态激发态分别为：[15.65](v′=0～4)～X(v"=0),[15.69](v′=0～4)～X(v"=0),和[15.81](v′=0～4)～X(v"=0). 三个新发现的电子激发态的光谱常数为首次确定. 此外,大多数观察的振动带的寿命也得到了测量.     

The laser-induced fluorescence spectrum of CoS between 15 200 and 19 000 cm-1

测量了在15200～19000 cm^-1的超声射流冷却的CoS自由基的激光诱导荧光激发谱. 观测到[15.58]⁴Δ_7/2～X⁴Δ_7/2, [16.02]⁴Δ_7/2～X⁴Δ_7/2, [16.50]⁴Δ_7/2～X⁴Δ_7/2, [17.80]⁴П_5/2～X⁴Δ_7/2和[18.00]⁴Δ_7/2～X⁴Δ_7/2五个电子跃迁序列. 此外,还测量到了大多数观察的振动带的寿命. 并讨论了这些新的电子态的电子构型.     

~（23）Na~（39）K分子D~1∏→X~1∑~＋激光感生荧光光谱及强度研究

实验获得了Ａｒ＋激光５１４．５ｎｍ线诱导２３Ｎａ３９Ｋ分子产生的Ｄ１∏→Ｘ１∑＋跃迁荧光谱．通过测量激光感生荧光光谱强度随泵浦功率、热管炉温度及缓冲气压变化规律，详细研究了其跃迁机制．用最小二乘法拟合获得２３Ｎａ３９Ｋ分于Ｘ１∑＋态振动常数．理论计算了各跃迁谱支波长值及Ｆｒａｎｃｋ－Ｃｏｎｄｏｎ因子和光谱强度值，与实验观测值符合得相当好，充分表明本文对激光感生荧光光谱的归属以及对各支谱线振、转量子数的赋值是合理的．     

15N216O在1650-3450 cm-1的高分辨红外光谱

采用傅里叶变换红外光谱仪记录了富含¹⁵N₂¹⁶O同位素的一氧化二氮样品在1650-3450 cm^-1波段的高分辨振转光谱,得到了该同位素分子超过7300吸收谱线位置的实验值,经分析实验精确度好于5.0×10^-4 cm^-1. 基于有效哈密顿量模型预测和带带转动分析,确定了所有吸收线的归属;获得了29个新吸收带的振转光谱参数,并优化了其他44个吸收带的光谱参数值. 并且发现有效哈     

ANALYSIS OF THE HDO ABSORPTION SPECTRUM BETWEEN 9600-10200cm-1

The absorption spectrum of HD¹⁶ O was recorded at a resolution of 0.02 cm^-1 with a Bruker IFS 120HR Fourier Transform Spectrometer in the region of 9600-10200 cm^-1. As far as we know it is the first time to record and analyze the HDO spectrum in this region which was assigned as the ν₁+2ν₃ and 2ν₂+2ν₃ bands. With the strong resonance interactions between these two bands considered, the spectroscopic parameters were optimized by the nonlinear least squares method.     

CN（B~2Σ~＋）激发态光谱的研究

研究亚稳态原子Ｈｅ（２３Ｓ）与ＣＨ３ＣＮ的能量转移反应，获得了ＣＮ（Ｂ２Σ＋－Ｘ２Σ＋）的近紫外辐射光谱。根据光谱强度，研究了ＣＮ（Ｂ２Σ＋）的形成速率和振动布居，并探讨了传能反应机理。     

饱和激发下叶绿素荧光非线性变化及影响分析

叶绿素浓度是海洋初级生产力的重要指标之一,激光诱导荧光技术可以实现海水叶绿素浓度的快速测量。测量叶绿素浓度的传统激光诱导荧光原理,是利用叶绿素荧光与水体Raman散射的强度比值（I_F/R）进行反演,即叶绿素浓度n_chl＝CI_F/R,其中C为系统常量。这是依据叶绿素荧光685 nm、水体Raman散射强度都与激发光强呈线性关系。然而,该理论并没有考虑诱导荧光饱和现象的存在。当诱导激光强度达到一定程度后,685 nm荧光强度随激发光强非线性变化。另外,值得注意的是,水体Raman散射并不存在信号饱和现象。为了探讨饱和激发造成荧光非线性变化的影响,在激光诱导荧光技术测量叶绿素浓度的实验中,设计两种测量方案,即：不同激光功率诱导单一浓度样本的荧光测量,和固定激光功率时不同浓度样本的荧光测量。实验中利用Nd∶YAG三倍频激光355 nm激发获得叶绿素溶液的404 nm处 Raman散射和685 nm荧光。实验结果分为2部分进行讨论：（1）为了分析饱和激发造成荧光变化的非线性特性,通过调节激发光功率测量溶液的受激发射光谱,发现水体Raman散射强度与激发光强呈线性关系,而685 nm荧光强度出现饱和激发下的非线性变化。而且,随叶绿素浓度的增加,685 nm荧光的非线性趋势更为明显,Raman散射强度与激发光强的线性关系中斜率变小。数据分析表明,685 nm荧光数据拟合的4阶多项式和Raman散射效率值,可以定性地表征685 nm荧光的饱和程度。（2）考虑实际海洋激光雷达探测叶绿素浓度应用中存在饱和激发荧光非线性现象,为了分析荧光非线性对传统叶绿素浓度反演理论适用性的影响,在固定激发光强情况下对不同浓度叶绿素溶液的发射光谱进行测量。将激发光功率调节至52.00,80.70,132.10和197.30 mW·cm-2,获取相应激发光强下685 nm荧光与水体Raman散射的强度比值和叶绿素浓度之间的关系。实验表明,激发光强不变的情况下,685 nm荧光与水体Raman散射的强度比值,与叶绿素浓度仍满足线性关系。但是,在较高光强激发时,饱和激发造成的叶绿素荧光非线性变化,导致利用传统激光诱导荧光理论反演的叶绿素浓度值偏小。因此,需要对饱和激发下荧光非线性的影响进行修正,其关系为I_F/R=n_chl/C+C_F,修正值C_F不可忽略。另外,值得一提的是,修正关系中系统常量C随激发光强增加而增大。研究表明,饱和激发造成的荧光非线性,会对激光诱导荧光技术测量叶绿素浓度产生影响,但由于造成荧光非线性因素的复杂性,仅通过荧光数据拟合获得的多项式,无法定量说明其影响权重。然而,当激发光强不变时,可以实验测量获得基于激光诱导荧光原理的修正关系,从而准确反演叶绿素浓度。     

~(39)K_2分子C~1Ⅱ_u-X~1∑_9~+(J′=105)Q支激光诱导荧光光谱及电偶极跃迁矩变化率研究

用4415.6(?)CW激光线获得了~(39)K_2分子C~1II_u(v′=0,J′=105)-X~1∑_g~+(v″=1～10,J″=105)Q支激光诱导荧光(LIF)光谱.用最小二乘法拟合出了~(39)K_2分子X~1∑_g~+态振动常数和C~1II_u态电子谱项值T_e.光谱分析表明C~1II_u态T_e=22968cm~(-1)是合适的.用~(39)K_2分子Morse势计算了(V′=0,J′=105)-(v″=1～10,J″=105)跃迁的Franck-Condon因子和跃迁强度,强度计算值和激光诱导荧光光谱测量值之间有令人满意的符合,进一步的r重心近似分析给出了~(39)K_2分子C~1II_u→X~1∑_g~+电偶极跃迁矩R_(?)随核间距r的归一化变化率为-0.157～-0.168 debye/(?)(4.22(?)相似文献   

Vibrational spectra of rare earths: o-chlorobenzoic acid in the region 800-200 cm-1

The vibrational spectra of Pr³⁺ and Nd³⁺: o-clorobenzoic acid in solid state in the region 800-200 cm^-1 have been recorded. About 24 bands have been observed. They have been assigned.     

用可调谐二极管激光光谱仪观测3657—3708cm-1区域CO2高分辨振转光谱

用可调谐二极管激光光谱仪观测到3657—3708cm^-1区域内CO₂各种同位素分子的9个振转谱带。首次观测到¹²C¹⁶O¹⁷O的10011—00001谱带和¹²C¹⁶O¹⁸O的11111—01101谱带,对其余7个谱带则扩充了其观测振转线的数目。用最小二乘方拟合法计算了各谱带的光谱常数,发现CO₂分子常数表中¹²C¹⁶O¹⁷O的10011—00001谱带中心v的计算值比本实验观测值大0.287cm^-1,而¹²C¹⁶O¹⁸O的11111—01101谱带中心v₀的计算值则比本实验观测值小0.048cm^-1。 关键词：     

双层石墨烯位于1800—2150cm~(-1)频率范围内的和频拉曼模

文章利用拉曼光谱研究了双层石墨烯在1800—2150 cm-1范围内的和频拉曼模.基于双共振拉曼散射理论,利用多波长激光拉曼散射结合声子色散曲线分别从实验上和理论上分析发现,双层石墨烯在此频率范围内主要存在4个拉曼模,它们主要由LO和LA或iTA按不同共振散射方式所组成的4个和频模,而iTO和oTO参与和频的可能性很小.文章澄清了学术界在1800—2150 cm-1频率范围内和频模的解释,有助于进一步深入理解多层石墨烯在此范围内的和频模.     

Measurements of atmospheric water vapour using the absorption band at 7250 cm-1

Measurements of the integrated absorption of the 7250 cm^-1 (1.38 μm) band of water vapour have been made for a 0.5 km horizontal path through the atmosphere. Using published band intensities the absorption values were converted to precipitable water amounts which were found to be about 10% smaller than values determined by wet and dry hygrometry. This difference is probably caused by inaccuracies in the published line parameter values, particularly those involving high rotational energy.     

氧化镍位于510～610 nm的激光诱导荧光光谱 (cited: 1)

采用激光诱导荧光技术在510～650 nm研究了超声射流冷却下的氧化镍光谱,观测了55个振转谱带. 通过转动分析发现激发态的同位素位移、振转间隔和转动常数都表现出高度的不规则性,26个[Ω=0,1]-X³∑^-₀的跃迁谱带被暂时归属为5个振动序列. 此外实验中还观测了部分谱带的色散谱和寿命.     

激光诱导击穿光谱在薄膜损伤分析中的应用

提出了应用激光诱导击穿光谱技术对薄膜损伤特性进行表征的方法,研究了纳秒脉冲激光作用下薄膜损伤时的等离子体光谱特征,并应用该技术对薄膜的抗激光损伤特性进行了测量.实验测得,HfO2单层膜在78mJ的激光能量的辐照下,薄膜损伤时的等离子体温度为2 807.4K,且电子密度为7.4×1017cm-3.利用识别薄膜损伤时的等离子体光谱的特征,准确地判断了薄膜是否损伤,避免了薄膜损伤的误判现象.结果表明,激光诱导击穿光谱技术适用于薄膜的激光损伤测试中,并且是一种非常有效的测试分析方法.     

Strengths and air-broadened widths of H2O lines in the 2950–3400 cm-1 region

Measurements of the strengths and air-broadened widths of 223 lines of water vapor have been made with high resolution in the region 2950–3400 cm^-1. The strength data of the lines in the 2ν₂ and ν₁ bands are analyzed to determine the band strengths and the coefficients of the F factors. The band strengths of the 2ν₂ and ν₁ bands were found to be 1.75±0.08 and 10.3±1.1 cm^-2 atm^-1 at 296 K, respectively. The selection rules of the lines observed in the ν₃ band are forbidden in the symmetric-rotor limit. The majority of the measured strengths of these lines differ from the calculated values because of different asymmetries in the upper and lower vibrational states. Also, Coriolis perturbations in several lines of the ν₁ and ν₃ bands were observed in the strength measurements. The direct method was applied to determine the air-broadened line widths. The results are compared to the computed values of Benedict and Kaplan. There is good agreement between this work and the computed results for line width values greater than 0.05 cm^-1 atm^-1. However, for line widths less than 0.05 cm^-1 atm^-1, the measured values are smaller than the computed widths. A value of 0.018 cm^-1 atm^-1 is given for the width of the line at 3378.071 cm^-1, whereas the calculated value is 0.032 cm^-1 atm.     

Analysis of the laser performance of Tm3+, Tb3+(Ho3+):YVO4 crystals at ～1.5μm wavelength

The absorption spectra of Tb,Tm:YVO_4 and Ho,Tm:YVO_4 are measured. The radiant and non-radiant transition probabilities from higher level to lower level, A_{i,j} and ω_{i,j}, and the cross-elaxation probability are calculated in virtue of Judd－Ofelt and Dexter theories. The fluorescence lifetime of Tm^{3+} in the Tb^{3+} (or Ho^{3+}) co-doped crystal is calculated. It indicates that the lifetime of initial level {}^3H_4 of the laser transition can be shorter than that of terminal level {}^3F_4 of the transition if the atomic percentage of Tb^{3+} (or Ho^{3+}) ions is bigger than about 1 at%: namely, by means of the co-doping Tb^{3+} (or Ho^{3+}) ions the self-termination phenomenon of laser light can be eliminated. Inserting the optic parameters to the formula deduced here on the laser threshold power P^{(4)}_{th} and the slope efficiency η^{(4)}_s of the four-energy-level system, we obtain the relationship of threshold power P^{(4)}_{th} to the concentration of Tm^{3+} ions and discuss the effect of Tb^{3+} (or Ho^{3+}) ion concentration on the laser threshold power P^{(4)}_{th} around 1.5μm wavelength. The result shows that Tb,Tm:YVO_4 crystal is a better choice to make the laser at ～1.5μm wavelength than Ho,Tm:YVO_4 crystal. We give the appropriate composition of (1－2) at% Tb, (1－2) at% Tm:YVO_4, just for reference.     

激光诱导荧光诊断中荧光频率极限的实验研究

在用激光诱导荧光法测量多偶极腔体中的氩等离子体的离子速度分布函数的实验中,研究了激光频率与信号强度的关系。在给定等离子体放电参数条件下,发现存在一个入射激光诱导荧光的极限频率,大于该频率时荧光强度不再增加。该诱导荧光的极限频率随荧光收集系统中透镜组中的小孔大小而改变。     

Scattering and absorption properties of CO2 ice spheres in the region 360–4000 cm-1

We present the results of Mie calculations for CO₂ ice particles of radius a = 0.1, 1 and 10 μm in the region 360–4000 cm^-1. Since CO₂ possesses a very small imaginary refractive index, the larger particles behave as conservative scatters. This is quite different from the equivalent water ice particles. The results presented in this study will be useful for investigation of the Martian atmosphere and surface.