CF_3CDCl_2分子红外多光子光热吸收谱

本文报道用铂丝光热吸收池作为探测器得到了CF_3CDCI_2的红外多光子吸收谱。并发现在线性吸收谱中944cm~(-1)处的吸收峰在多光子吸收谱中分裂为947cm~(-1)和927cm~(-1)两个吸收峰。这一现象与科里奥利力和非谐性引起的简正振动的耦合作用有关。这样,在用CF_3CDCI_2/CF_3CHCI_2体系分离氘同位素时,可以根据这一新结果选择更合适的激发波长。 实验还发现在线性吸收谱中986cm~(-1)处的吸收峰在多光子吸收谱中出现约6cm~(-2)的红移。这种红移现象起源于分子振动能级的非谐性。     

3Cu(IO3)2·2H2O晶体的电子结构研究

本文测定了3Cu(IO₃)₂·2H₂O球晶的电子吸收光谱,吸收峰位于9140cm^-1和15250cm^-1。首次观察到了高达6110cm^-1的低对称晶场分裂。吸收曲线经Gauss分解可得到八个Gauss型吸收峰,分别位于8590,10690,10870,12190,13500,14510,15330和16500cm^-1。测量其EPR谱可得g=2.141±0 关键词：     

332—362nm范围内CF2Cl自由基的共振增强多光子电离研究

用CF₂Cl₂分子直流脉冲放电的方法产生CF₂Cl自由基，结合共振增强多光子电离(REMPI)技术，测量了332—362nm波长范围内CF₂Cl自由基的(2+1)REMPI光谱，分析并标识了4s Rydberg态带源位于(ν_0—0=55371cm^-1)，两个被激活振动模ω′₃(CF₂剪式振动模)和ω₄′(OPL 关键词：     

Ag离子注入非晶SiO2的光学吸收、拉曼谱和透射电镜研究

能量为200keV的Ag离子，以1×10¹⁶，5×10¹⁶，1×10¹⁷ cm^-2的剂量分别注入到非晶SiO₂玻璃，光学吸收谱显示：注入剂量为1×10¹⁶ cm^-2的样品的光吸收谱为洛伦兹曲线，与Mie理论模拟的曲线形状一致；注入剂量较大的5×10¹⁶，1×10¹⁷ cm^-2的谱线共振吸收增强，峰位红移并出现伴峰. 透射电镜观察分析表明，注入剂量不同的样品中形成的纳米颗粒的大小、形状、分布都不同，注入剂量较大的还会产生明显的表面溅射效应，这些因素都会影响共振吸收的峰形、峰位和峰强. 当注入剂量达到1×10¹⁷ cm^-2时，Ag纳米颗粒内部可能还形成了杂质团簇. 关键词： 离子注入 纳米颗粒 共振吸收 红移     

AgI(Cr2O3)复合离子导体的光谱研究

本文研究了AgI(Cr₂O₃)复合离子导体的红外吸收光谱,近紫外、可见反射光谱。发现复合离子导体的两种谱图均与纯AgI,Cr₂O₃的不同。红外吸收光谱在882—889cm^-1处有一新吸收峰。电子谱中,AgI从430nm开始向长波方向表现的光离解特性消失。本来Cr₂O₃由配位场效应而引起的d—d吸收跃迁以410nm,530nm为中心的反射谱带,现在410nm处的谱带消失。530nm处的谱带稍有红移,且随加入Cr₂O₃量的增多而强度减弱。代之以整个紫外、可见区的较强吸收。对此,结合透射电子显微镜的分析,用双声子耦合和介质的变形极化以及配位场理论对AgI(Cr₂O₃)复合离子导体的声子谱和电子谱进行了解析。 关键词：     

Cr3+:Al2O3透明多晶陶瓷光谱特性分析

对透光性良好的Cr³⁺:Al₂O₃透明多晶陶瓷的光谱性能 进行了研究，其吸收光谱中吸收峰与单晶红宝石相一致，按吸收光谱和Tanabe-Sugano能级 图，算出其晶场强度参数D_q及Racah参数B分别为1792cm^-1， 689cm ^-1，D_q/B=2.6，陶瓷中Cr³⁺离子所处格位的晶体场强 比单晶弱一些，但Cr³⁺:Al₂O₃透明陶瓷仍属于强场晶 体材料；当Cr³⁺掺杂浓度到达0.8wt%时，陶瓷的发射谱仍保持较好的R线发射 ；随Cr³⁺掺杂浓度的增大，激发峰位发生“红移”.在Cr³⁺:Al₂O₃透明多晶陶瓷的荧光谱上，发现一个波长为670nm的发射峰，经激发 谱确认为Cr³⁺的发射峰. 关键词： 氧化铝 透明陶瓷 离子格位 光谱性质     

CaO-Al2O3二元系晶体和玻璃的拉曼光谱研究

实验测定了CaO-Al₂O₃二元系中晶体和玻璃的拉曼光谱,并利用密度泛函理论(DFT)计算了CaAl₄O₇晶体的拉曼光谱活性振动波数和散射活性。结果表明CaAl₄O₇的中波数区(400～700 cm^-1)对应Al-O_b-Al的弯曲振动,高波数区(700～1 000 cm^-1)则对应Al-O_nb的伸缩振动。采用激光悬浮加热装置制备了一系列玻璃样品,对其进行拉曼光谱研究发现,550和780 cm^-1附近观察到两个明显的特征峰,分别对应Al-O_b-Al的弯曲振动和Al-O_nb的伸缩振动。随着CaO/Al₂O₃比例的增加,550 cm^-1特征峰发生蓝移,而780 cm^-1特征峰发生红移,表明复杂网络结构逐渐解聚。此外,随Al<...     

Eu3+或Tb3+掺杂Y2O3纳米材料紫外激发光谱

采用燃烧法制备了不同Ln³⁺(Ln=Eu或Tb)掺杂浓度和不同平均粒径的Y₂O₃:Ln纳米晶体粉末和体材料样品。研究发现随着粒径的减小,Y₂O₃:Eu电荷迁移带的位置发生红移;并且,由于存在于近表面低结晶度环境中的Eu³⁺数量的增加,小粒径样品(5nm)的电荷迁移带还向长波方向发生了明显的展宽。实验中还观察到Y₂O₃:Tb纳米晶激发谱中4f5d(4f⁸→4f⁷5d¹)跃迁吸收对应激发峰(带)的谱线形状随样品粒径变化存在较大的差异,这是由于Tb³⁺存在于近表面的低结晶度和颗粒内部的高结晶度两种不同环境中,Tb³⁺的4f5d跃迁在两种环境中对应的吸收峰位置不同,当样品粒径发生变化时Tb³⁺处于两种环境中的比例随之变化,造成相应吸收跃迁对应的激发峰(带)强度发生变化,并改变了激发谱的谱线形状。实验中还发现,随着Tb³⁺(或Eu³⁺)浓度的减小,Y₂O₃基质激子跃迁吸收的激发峰对比4f5d跃迁(或电荷迁移带)激发峰的相对强度随之增强。     

CF自由基二光子共振增强多光子电离研究：5p Rydberg态观测与分析

报道260—360nm波长范围内CF自由基(2+1)共振增强多光子电离(REMPI)激发谱的研究-CF自由基通过Ar/CF₄,Ar/CF₂Cl₂或Ar/CF₃COOH混合气体的直流脉冲放电产生-在260—295nm波长范围内,观测到一个新的高Rydbery态振动序列,其带源位于295-22nm(2hν=67746cm^-1),分析表明,该振动序列来源于5p Rydberg态的二光子共振激发,测得的振 关键词：     

吡啶B1(nπ*)态(2+3)偏振共振多光子电离谱中6a10带型模拟及转动常量确定

通过模拟吡啶B₁(nπ^*)态(2+3)偏振共振多光子电离谱中转动结构可部分分辨的6a¹₀带型,获得了该态上吡啶分子的转动常量,分别为A′=0.21670cm^-1,B′=0.16758cm^-1,C′=0.09450cm^-1.表明氮原子上的一个孤对电子跃迁进入π^*轨道后氮原子自身电负性减弱,吡啶分子构架总体上张开.此外,比较6a^关键词：     

High resolution infrared spectrum of the ν1 band of 14N16O2

The infrared spectrum of the ν₁ band of ¹⁴N¹⁶O₂ has been recorded with a resolution of about 0.025 cm^?1 in the region extending from 1480 to 1270 cm^?1. From about 1350 cm^?1, the absorption became progressively weaker and no absorption at all could be detected below the band origin located at 1319.797 cm^?1. Because series with low values of K_a could not be measured, constants which depend strongly upon the molecular asymmetry could not be determined.     

Li2B4O7晶体的晶格振动光谱

在室温下测量了Li₂B₄O₇单晶的各种振动类的偏振Raman散射谱和该晶体粉末样品的红外吸收谱(200—4000cm^-1)。根据LO-TO劈裂的实验结果,计算出该晶体极化模的有效电荷和振子强度。通过与BBO和LBO晶体的结构和B—O伸缩振动模频率比较,得出:Li₂B₄O₇晶体可能有较大的非线性光学系数。 关键词：     

Selective desorption from the binary coadsorbate C2H6CH3FNaCl by resonant vibrational excitation with laser infrared radiation

After measuring the linear infrared absorption spectrum of the coadsorbate, selective desorption of CH₃F from the binary coadsorbate C₂H₆CH₃FNaCl under ultrahigh vacuum conditions at 12o K stimulated by resonant CO₂ laser pulses of small fluence ～ 0.1 J·cm^t?2 has been carried out. No desorption of ethane, which is slightly more volatile, but has no significant infrared absorption at the laser frequency, was observed. The primary activation step is the resonant multiphoton excitation of the most intense internal CH₃FNaCl adsorbate vibration, the CF stretching mode ν₃. The substance separation seems to indicate high localisation of the activation in this desorption and could be of interest for applications.     

Optical study of RE 1 + x Ba 2 - x Cu 3 O 6 (RE = Nd, Sm) aaand YBa 2 Cu 3 O 6 in the mid infrared range

Infrared reflectance, and transmission measurements as well as Raman scattering have been used to study the RE_1+xBa_2-xCu₃O₆ (RE = Nd, Sm) and YBa₂Cu₃O₆ absorption bands in the 1100-1500 cm^-1 infrared range as a function of temperature and beam polarization. In addition to two-phonon absorption between 1100 and 1170 cm^-1, we observe excitations around 1400 cm^-1, occurring in oxygen rich enclosures within the samples, and assign them to an excitation involving two-phonons plus the 270 cm^-1 local mode related to Cu-O broken chains. Thus, the previously reported possible magnetic origin of the 1436 cm^-1 sharp absorption band in YBa₂Cu₃O₆ is contested. Received 14 February 2001 and Received in final form 12 April 2001     

Oxygen in Ge crystals grown by the B2O3 encapsulated Czochralski method

Local vibrations of oxygen in Ge crystals grown by the Czochralski method adopting liquid-B₂O₃ encapsulation and GeO₂ powder doping were investigated by Fourier-transform infrared spectroscopy. Strong absorption peaks at 855 cm⁻¹, originating in local vibration of interstitially dissolved oxygen O_i as Ge–O_i–Ge quasi-molecules, developed depending on the doped amount of GeO₂. Similarly, an absorption peak related to the combined vibration of Ge–O_i–Ge was found at 1264 cm⁻¹ and the conversion factor from the peak intensity to the oxygen concentration was evaluated to be 1.15×10¹⁹ cm⁻². By prolonged annealing at 350 °C an absorption peak developed at 780 cm⁻¹, indicating formation of oxygen-related thermal donors. From the variations of carrier density and oxygen concentration, one donor was found to possess about 15 O_i atoms.     

Influence of collisions and pulse intensity on multiple photon absorption in SF6

Using a pyroelectric detector, the multiple photon absorption (MPA) of the SF₆ molecule in a wide range of pressures (10^-3 -1 torr) has been studied. The significant role of collisions in MPA has been shown. The fraction of molecules excited under essentially collisionless conditions has been defined. It is shown that under collisionless excitation of SF₆ (p < 10^-2 torr) at energy fluences E < 10^-1 J/cm² the intensity of the laser pulse plays the essential role, while in presence of collisions MPA is determined mainly by the energy fluence in the pulse.     

The Matrix Isolation Spectrum of the CH2 Ion

For CH₂⁺ molecular ions at 5 K we simulate the infrared absorption spectrum, and tabulate all strong absorption lines from 0 to 16 000 cm⁻¹. We use ab initio potential energy, dipole moment, and transition moment surfaces in conjunction with our program system RENNER, which allows for the Renner-Teller effect and spin-orbit coupling in a full-dimensions calculation. This is done for the purpose of guiding our search for the matrix isolation spectrum; our attempts at finding this spectrum are also described.     

OH-吸收带作为铌酸锂晶体缺陷结构的探针

本文报道了一组不同Li/Nb比和另一组不同掺Mg浓度的LiNbO₃晶体室温OH^-吸收带的实验结果,观察到OH^-吸收带的三峰结构及其随Li/Nb比的变化,以及重掺Mg晶体中(6mol％MgO)OH^-吸收带转变为双峰结构,并向高能端移动54cm^-1。根据LiNbO₃的晶体结构以及Abrahams和Smyth的缺陷结构模型,对化学计量晶体、一致熔化晶体和掺Mg晶体分别进行讨论。并提出重掺Mg晶体中OH^-吸收带向高能端的移动可能是由于当掺Mg浓度超过阈值后Mg²⁺离子开始进入Nb位而引起的。 关键词：