人工神经网络方法预测八面体六卤化物MX~(n-)_6的ν_1和ν_2模的振动频率

利用ＡＮＮ－ＢＰ算法，采用逐步改变训练步长和两个惯性项的权重系数惯性调整策略，分别以单目标和双目标的三层网络对八面体六卤化物ＭＸｎ－６的八面体ν１和ν２模振动频率进行了预测，发现单、双目标下预测的结果相差不大，双目标时权重系数调整得较快，［ＭｏＦ６］２－，［ＢｉＦ６］－和［ＡｕＦ６］２－的振动频率文献值与网络的计算值或预测值相差偏大。     

人工神经网络法预测四卤化物XY_4对称伸缩模和二重简并模的振动频率

用人工神经网络法，采用控制训练步长和两个惯性项的权重系数惯性调整法，分别用单目标和双目标的三层网络对四卤化物ＸＹ４的对称伸缩模。ｖ１和二重简并模ｖ２的振动频率进行了训练和预测，并将单双目标下预测的结果作了比较。双目标时发现［ＨｇＣｌ４］２的ｖ２振动频的计算值与实验值有很大差距，多目标优化可一定程度上避免过拟合。本文程序用ＦＯＲＴＲＡＮ语言编写，用ＮＤＰ－ＦＯＲＴＲＡＮ编译程序编译运行。     

超声射流冷却CF2自由基激光诱导荧光激发谱

用直流放电产生ＣＦ２自由基，在超声射流冷却下获得了ＣＦ２Ａ＾１Ｂ１←Ｘ＾１Ａ２ ２５０ｎｍ附近的激光诱导荧光激发谱。对不同带系的３９个振动带做了归属，其中２３个振动带是新标识的。澄清了前人对ＣＦ２Ａ↑￣←Ｘ↑￣跃迁的一些不能肯定的归属。对Ｋ结构分辨谱的近１００个子带的分析，从实验上确定了ＣＦ２Ａ↑￣态两个伸缩振动频率分别是ｖ１＇＝１０１２．１ｃｍ＾－１，ｖ３＇＝１１８０．２ｃｍ＾－１。并获得了一些     

束—气条件下He（2^3S）＋CH2Cl2碰撞传能反应的动力学研究

本文在束－气条件下研究了亚稳态原子Ｈｅ（２＾３Ｓ）与ＣＨ２Ｃｌ２间的传能反应，测得了由该反应产生的ＣＨ（Ａ＾２△－Ｘ＾２П），ＣＨ（Ｂ＾２∑＾－Ｘ＾２П）ＣＨ（Ｃ＾２∑＾＋－Ｘ＾２П）和Ｈ原子（Ｂａｌｍｅｒ系）的化学发光光谱。通过对ＣＨ（Ａ，Ｂ）的光谱进行计算机模拟，推测出初手的ＣＨ（Ａ＾２△，ｖ＾１＝０－２）态振动分布为Ｎｏ：Ｎ１：Ｎ２＝１００：４０±５：１９±２，ＣＨ（Ａ＾２△，ｖ＾１＝０－０     

超声射流冷却SO2^—A2—^1A1激光诱导荧光激发谱

测得了３１５￣３３０ｎｍ超声射流冷却下ＳＯ２＾１Ａ２－＾１Ａ１激光诱导荧光（ＬＩＦ）激发谱，获得了７个有明显Ｋ结构的Ｃ型跃迁的转动子带分辨谱，并将７０个转动子带归属为（１，ｍ，１）－（０，０，０）和（０，ｎ，１）－（０，０，０）（４≤ｍ≤７，８≤ｎ≤１０）的跃迁带系。光谱分析得到ＳＯ２＾１Ａ２－＾１Ａ１跃迁的带源ｖ００、＾１Ａ２态弯曲振动频率ｖ′２，非谐性常数Ｘ２２′分别为（２７９５０±５）、（２     

Tm^3＋掺杂的MFT玻璃上转换发光及光学增益

报道了一种新型ＭＦＴ（Ｍｕｌｔｉ－Ｆｌｕｏｒｉｄｅ－Ｔｅｌｌｕｒｉｄｅ）玻璃材料（组份为５０ＴｅＯ２－１９．７ＰｂＦ２－１０ＡｌＦ３－１０ＢａＦ－０．３Ｔｍ２Ｏ３）的制备方法,测量了６５０ｎｍ激发下Ｔｍ＾３＋离子掺杂在ＭＦＴ玻璃材料中源于＾１Ｄ２→＾３Ｈ６（４７６ｎｍ）跃迁的两组蓝色上转换发光研究了上转换发光强度随激光率的变化关系,并且首次应用ＡＳＥ（Ａｍｐｌｉｆｉｅｄ Ｓｐｏｎｔａｎｅｏｕｓ Ｅ     

二（2,4,4—三甲基戊基）膦酸稀土配合物的振动光谱

测定了二（２，４，４－三甲基戊基）膦酸（ＢＴＭＰＰＡ）及其稀土配合物Ｌｎ（ＢＴＭＰＰ）３在４０００～５０ｃｍ＾－１光谱区内的ＦＴ－ＩＲ光谱和部分配合物的激光拉曼光谱，对其谱带进行了经验归属。发现稀土氧键具有较高的离子键特性。由Ｌｎ－Ｏ伸缩振动频率值算出其近似力常数约８ｍ ｄｙｎ／ｎｍ。     

自由基分子CN（A^2Пi—X^2Σ^＋）的光谱研究

利用塞曼调制磁旋转光谱技术对自由基分子ＣＮ（Ａ＾２ΠＩ－ｘ＾２Σ＾＋）（１２,６）带、（７,２）带进行了测量,标识了光谱并拟合了Ａ＾２Πｉ太分子常数,从而得到Ｖ＝７Ｔ Ｖ＝１２振转谱带的Ｔｖ、Ａｖ、Ｂｖ、Ｄｖ等参数,还获得Ａ双分裂参数Ｐｖ和ｑｖ,两个带的总拟合方差分别为０．０３９和０．０４６ｃｍ＾－１。     

六氯铅铵晶体相变的拉曼散射研究

在５Ｋ～３００Ｋ温度范围内对六氯铅铵晶体进行了拉曼散射测量，该晶体在Ｔｃ＝７８Ｋ发生从立方结构（Ｏ＾５４）至三方结构（Ｃ＾２３ｉ）的二级相变，ＰｂＣｌ＾２－６八面体Ａ１ｇ模和ＮＨ＾＋４四面体Ａ１模的拉曼频移在Ｔｃ时出现极大值，八面体Ｔ２ｇ模，四面体Ｔ２模和外振动Ｔ２ｇ模在Ｔｃ以下发生连续分裂，另外在Ｔｃ以下观测到对应于高温相ＰｂＣｌ＾２－６八面体Ｔ１ｇ模的软模。     

在小硅化物SiX^m（X=Be,B,C,N,O,F,Ne,m=～4—＋2）中分子成…

此文用从头计算法，在ＨＦ，ＭＰ２，ＭＰ３水平下，使用基组６－３１Ｇ，６－３１＋Ｇ对ＳｉＯ的等电子分析ＳｉＸ＾ｍ（Ｘ＝Ｂｅ，Ｂ，Ｃ，Ｎ，Ｆ，Ｎｅ，ｍ＝－４～＋２）进行了几何优化，并计算了相应的平衡几何构型下的振动频率，对ＳｉＯ分子，使用ＱＣＩＳＤ（Ｔ）方法考虑了不同水平下的电相关效应，并考虑了不同其函数６－３１＋Ｇ和６－３１１＋Ｇ的影响。计算结果表明，所有分子的势能曲线都有稳定的极小值，并且键长与频     

Radiofrequency, Centimeter-Wave, Millimeter-Wave, and Infrared Spectra of SiHF(3): Investigation of the Ground, v(4) = 1, and v(6) = 1 Vibrational States

The present paper deals with the analysis of the microwave, millimeter-wave, and infrared spectra of (28)SiHF(3) in its ground, v(6) = 1 and v(4) = 1 excited states. The former was observed up to 1055 GHz leading to the determination of one octic centrifugal distortion constant, L(J) = -0.0749(55) μHz. Furthermore the interaction term ||h(3,GS) || = 1.1032(70) mHz has been fitted from splittings of six K = 3 lines. The excited states have been regarded as isolated ones. This enabled fits according the Q-, D-, and QD-reduction schemes proposed by E. I. Lobodenko, O. N. Sulakshina, V. I. Perevalov, and Vl. G. Tyuterev, (J. Mol. Spectrosc. 126, 159-170 (1987)) and further developed by J. K. G. Watson, C. Gerke, H. Harder, and K. Sarka, (J. Mol. Spectrosc. 187, 131-141 (1997)) and Harder (J. Mol. Spectrosc. 194, 145 (1999)). A multiple fit analysis was performed confirming the assumption that the excited states are not affected by intervibrational resonances. Finally the millimeter spectrum of (29)SiHF(3) and (30)SiHF(3) in their ground state was also measured up to 460 GHz and accurate rotational and centrifugal distortion parameters were derived. Copyright 2000 Academic Press.     

含MoFe3S4单元的μ2—OR或μ2—SR桥联双类立方烷簇合物的红？…

对下列含ＭｏＦｅ３Ｓ４单元的μ２－ＯＲ或μ２－ＳＲ桥联双类立方烷簇合物的红外光谱进行了研究：（Ｅｔ４Ｎ）３「Ｍｏ２Ｆｅ６Ｓ８Ｃｌ６（ＯＭｅ）３」（１）,（Ｅｔ４Ｎ）３「Ｍｏ２Ｆｅ６Ｓ８（ＳＰｈ）６（ＯＭｅ）３」（２）,（Ｂｕ４Ｎ）３「Ｍｏ２Ｆｅ６Ｓ８（ＳＰｈ）６（ＯＭｅ）３」（３）（Ｅｔ４Ｎ）３「Ｍｏ２Ｆｅ６Ｓ８（ＳＢｕ＾ｔ）６（ＯＭｅ０３」（４）ｍ,（Ｅｔ４Ｎ）３「Ｍｏ２Ｆｅ６Ｓ８（ＳＰｈ）９」     

High-Resolution Infrared and Millimeter-Wave Study of the Fermi-Coupled v(2) = 1 and v(3) = 2 States of DSiF(3)

The nu(2) (nu(eff.) 854.841 cm(-1)) and 2nu(3) infrared bands (nu(eff.) 840.083 cm(-1)) of DSiF(3) have been studied with a resolution of 2.5 x 10(-3) cm(-1). Moreover, millimeter-wave transitions in the v(2) = 1 and v(3) = 2 states up to J" = 33 have been measured. The assignments and fit of the poorly resolved, compressed cluster-type 2nu(3) IR transitions have been confirmed by a simultaneous study of the 2nu(3)-nu(3) band. The constant W = 5.116 cm(-1) of the Fermi interaction between the v(2) = 1 and v(3) = 2 levels has been determined from frequency effects which are in agreement with relative intensities of the nu(2) and 2nu(3) bands. The deperturbed (B(0) - B(v)) and (C(0) - C(v)) values of the states involved agree with their ab initio predictions within 7% in the worst case. Copyright 2001 Academic Press.     

瓜环与咪唑[4,5,f]-1,10-菲咯啉衍生物相互作用模式的测试

以合成的三种的咪唑[4,5,f]-1,10-菲咯啉衍生物为客体,以瓜环(cucurbit[n]uriln=6～8)为主体,利用1H NMR技术,荧光光谱和紫外吸收光谱方法,测试了主客体相互作用形式、形成包结物的结构特征及其光学性质,三种方法得到的结果相同.研究表明,六元瓜环(Q[6])仅能与2-(4-甲基苯基)-咪唑-[4,5,f]菲咯啉(W1)盐酸盐相互作用(包结比为1:1);七元瓜环(Q[7])与三种客体2-(4-甲基苯基)-咪唑-[4,5,f]菲咯啉,2-(2-甲基苯基)-咪唑-[4,5,f]菲咯啉(W2)以及2-(3-甲氧基苯基)-咪唑-[4,5,f]菲咯啉(W3)的盐酸盐均以1:1的物质的量比发生相互作用;而八元瓜环(Q[8])除与W1形成的是1:2的包结物外,与另外两种客体W2,W3也是形成1:1的包结配合物.     

RbH(X1∑+,v=O～2)能级与H2碰撞振动能量转移

利用积分时间分辨荧光光谱方法,研究了RbH(X1∑+,v=0～2)与H2间的振动碰撞能量转移.在Rb-H2混合样品池中,泵浦激光双光子激发Rb原子至6D态,Rb(6D)与H2反应生成RbH(x1∑+)分子,探测激光延迟泵浦激光20 ns,通过激光感应荧光光谱(LIF)的测量,确定了X1∑+(v=0～2,J)原生态的转动...     

The v(1)+v(3) Bands of the (16)O(17)O(16)O and (16)O(16)O(17)O Isotopomers of Ozone

Using 0.002 cm(-1) resolution Fourier transform absorption spectra of an (17)O enriched ozone sample, an extensive analysis of the v(1)+v(3) bands of the (16)O(17)O(16)O and (16)O(16)O(17)O isotopomers of ozone has been performed for the first time. The experimental rotational levels of the (101) vibrational states were satisfactorily reproduced using a Hamiltonian matrix that takes into account the observed rovibrational resonances. More precisely, for (16)O(17)O(16)O, as for the other C(2v)-type ozone isotopomers, it was necessary to account for the Coriolis type resonances linking the (101) rotational levels with the levels of the (200) and (002) vibrational states and the Darling-Dennison interaction coupling the levels of (200) with those of (002). For the C(s)-type isotopomer, namely (16)O(16)O(17)O, as for (16)O(16)O(18)O and (16)O(18)O(18)O, it proved necessary to also account for an additional DeltaK(a)&equals+/-2 resonance involving the rotational levels from (101) and (002) (J.-M. Flaud and R. Bacis, Spectrochimica Acta Part A 54, 3-16 (1998)). Using a Hamiltonian matrix which takes these resonances explicitly into account, precise vibrational energies and rotational and coupling constants were deduced, leading to the following band centers: v(0)(v(1)+v(3))=2078.3496 cm(-1) for (16)O(17)O(16)O and v(0)(v(1)+v(3))=2098.8631 cm(-1) for (16)O(16)O(17)O. Copyright 2001 Academic Press.     

Generation of mid-infrared pulses by X(3) difference frequency generation in CaF(2) and BaF(2)

Tunable mid-IR pulses in the range 1300-4200 cm(-1) (7.7-2.4 microm) are generated through a phase-matched four-wave mixing process in ordinary mid-IR window materials such as CaF(2) and BaF(2) . In this process the difference frequency v(3)=2v(2)-v(1) is generated from pump fields v(1) and v(2) . The process can be phase matched to different frequencies by adjustment of the angle between the pump fields.     

Vibrational Spectroscopic Investigation and Theoretical Calculations of (E)-3-Phenyl-N-[4-(Phenyl-Amino) Quinazoline-7-yl] Acrylamide

ABSTRACT

Optimized geometrical structure and harmonic vibration frequencies of prior synthesized (E)-3-phenyl-N-[4-(phenyl-amino) quinazoline-7-yl] acrylamide were computed by ab initio HF and DFT/B3LYP methods using both 6-31G* and 6-311G** basis sets and the Moller–Plesset second-order perturbation (MP2) method merely at the 6-31G* level. The infrared (IR) spectrum of the title compound has been measured in the range of 400–4000 cm^?1. Complete vibrational assignments of the IR spectra were proposed. Moreover, the calculated wavenumbers of the title compound were compared with the experimental data. The correlation analyses indicate that good linearity relationships exist between the scaled theoretical vibration frequencies and the experimental values. Additionally, the atoms in molecules (AIM) method was applied to explore the possible intramolecular interactions in the title compound.     

State-to-state quantum dynamics of N(~2D)+HD(v=0,j=0) reaction

The N(~2D) + HD(v = 0, j = 0) reaction has been studied by a quantum time-dependent wave packet approach with a second-order split operator on the potential energy surface of Li et al.(Li Y, Yuan J, Chen M, Ma F and Sun M J. Comput.Chem. 34 1686). The rovibrationally resolved reaction probability, vibrationally integral cross section, and differential cross section of the NH + D and ND + H channel are investigated at the state-to-state level of theory. The experimental data of the thermal rate constant of two output channels is very scare, but the sum of the two output channels is in excellent agreement with the experimental data which was reported by Umemoto et al. It may imply that the thermal rate constants of the two output channels are accurate and reliable.