Al(2Pu)+H2(X1Σ+g)的分子反应动力学

基于多体展式方法所导出的ＡｌＨ２（Ｘ＾２Ａ１）分析势能函数,用准经典的Ｍｏｎｔｅ－Ｃａｒｌｏ轨迹法对Ａｌ（＾２Ｐｕ）＋Ｈ２（Ｘ＾１∑＾＋ｇ,ｕ＝ｊ＝０）的分子反应动力学过程进行了计算。结果表明,此反应的主产物为交换反应Ａｌ（＾２Ｐｕ）＋Ｈ２（Ｘ＾１∑＾＋ｇ,ｖ＝ｊ＝０）→ＡｌＨ（Ｘ＾１∑＾＋,Ｖ’,ｊ’）＋Ｈ（＾２Ｓｇ）的ＡｌＨ（Ｘ＾１∑＾＋,ｖ’,ｊ’）没有发现ＡｌＨ２（Ｘ＾２Ａ１）的络合物。而     

微乳液-1-(2-吡啶偶氮)-2-萘酚体系测定Cd(Ⅱ)

研究了Ｏ／Ｗ型阴离子微乳液十二烷基硫酸钠（ＳＤＳ）／正丁醇（ｎ－Ｃ４Ｈ９ＯＨ）／正庚烷（ｎ－Ｃ７Ｈ１６）／Ｈ２Ｏ对Ｃｄ（Ⅱ）与１－（２－吡啶偶氮）－２－萘酚（ＰＡＮ）显色体系的增敏增稳作用,试验结果表明,其灵敏度为ε＾５４５＝１．９３＊１０＾４Ｌ．ｍｏｌ＾－１．ｃｍ＾－１,与相同含水量的ＳＤＳ胶束体系（ε＾５４５＝１．１５＊１０＾４Ｌ．ｍｏｌ＾－１．ｃｍ＾－１）比较,其测定灵敏度显著增加,用于香烟样品分析,结果满意。     

[C5H4C(CH3)2CH2CH=CH2]Sm(OH)Cl·2MgCl2·4THF的晶体结构分析

用Ｘ－射线晶体结构衍射法测定了［Ｃ５Ｈ４Ｃ（ＣＨ３）２ＣＨ２ＣＨ＝ＣＨ２］Ｓｍ（ＯＨ）Ｃｌ·２ＭｇＣｌ２·４ＴＨＦ的晶体结构。它属三斜晶系,空间群为Ｐ＾－１,ａ＝１０．７７３（２）,ｂ＝１２．８３６（３）,ｃ＝１５．４７８（３）Ａ,ａ＝１１１．４６（３）,β＝１０７．７１（３）,γ＝９２．５４（３）°,Ｖ＝１８６８（１）Ａ＾３,Ｍｒ＝８２７．９１,Ｄｘ＝１．４７２ｇ／ｃｍ＾３,μ＝２．０００６ｍｍ     

CH2(X 3B1)自由基与O2的反应

用时间分辨富里叶红外发射谱仪（ＴＲ－ＦＴＩＲＳ）研究了ＣＨ２（Ｘ＾３Ｂ１）自由基与Ｏ２反应的通道及产物的振动动态布居，基电子态自由基ＣＨ２（Ｘ＾３Ｂ１）由３５１ｎｍ紫外激光光解ＣＨ２ＣＯ生成，观测到振动发态反应产物ＣＯ（ｖ≤１０），ＣＯ２（ｖ３≤７）ＯＨ（Ｈ２Ｏ）和Ｈ２ＣＯ的红外发射，证实存在生成Ｈ２ＣＯ的通道，由光谱拟合得到不同时刻ＣＯ（ｖ）和ＣＯ２（ｖ３）的相对振动布居，发现ｖ＝４能级的布居数     

C_2H_2分子(~1Σ_g~ ,v_2~"=1,J")态m_j定向布居及光学AC Stark效应

利用相干受激Raman抽运，选择性地激发C2H2分子（X~1Σg v2＝1，J"）单一振转态．在Ra-man泵浦与探测激光不同偏振条件下，获得紫外探测激光诱导的A1Au（v3＝1）-（X~1Σg v2＝1，J"）荧光增益光谱，从而研究了C2H2分子单一振转态的光学ACStark效应和mj的定向分布A0(1），利用stark线型加宽数值模型，从理论上计算得到的Rarnan线型与实验结果进行比较，二者符合程度相当好．     

266nm激光激励的SO2（X^1A,A^1A2,B^1B1）体系的态间转移研究

用ＹＡＧ四马ＳＯ２分子从电子基态Ｘ＾１Ａ１激励到电子激发态Ａ＾１Ａ格Ｂ＾１Ｂ１的高振动耦合区，获得了３２０－３８０ｎｍ范围内ＳＯ２（Ｂ＾１Ｂ１→Ｘ＾１Ａ１１）的激光诱导荧光色散谱，并给出初步标识：提出一个三能太模型来处理２６６ｎｍ激光激励的ＳＯ２（Ｘ＾１Ａ１，Ａ＾１Ａ２，Ｂ＾１Ｂ１）体系的态间转移，并获得了Ａ态和Ｂ 高振动能区的耦合系数ζ及耦合达到动态平衡的弛豫时间τ，发现二者反映的是被研究体系的     

蝶状铁硒簇合物双（μ—p—甲苯硒基）六羰基二铁双膦取代…

测得并解析了２个蝶状铁硒取代衍生物（μ－ｐ－ＭｅＣ６Ｈ４Ｓｅ）２Ｆｅ２（ＣＯ）２（Ｐｈ２ＰＣＨ２ＣＨ２ＰＰｈ２）（Ａ）和（μ－ｐ－ＭｅＣ６Ｈ４Ｓｅ）２Ｆｅ２（ＣＯ）４（ｃｉｓ－Ｐｈ２ＰＣＨ＝ＣＨＰＰＨ２）（Ｂ）的＾１Ｈ－＾１ＨＣＯＳＹ谱和＾１Ｈ－＾１５ＣＣＯＳＹ谱以及Ａ的＾１Ｈ－＾１ＨＮＯＥＳＲ谱，从而进一不确证了它们的结构。     

Pd2X2（dpm）2（X=NCO^—,CH3CO2^—,SCN^—,NO^—3;dpm=Ph2PCH2PPh2）配合…

采用ＮＭＲ方法考察了室温和低温（－７８～－６０℃）下Ｐｄ２Ｘ２（ｄｐｍ）２（Ｘ＝ＮＣＯ＾－，ＣＨ３ＣＯ＾－２，ＳＣＮ＾－和ＮＯ＾－３，ｄｐｍ＝Ｐｈ２ＰＣＨ２ＰＰｈ２）与Ｈ２Ｓ在ＣＤ２Ｃｌ２或ＣＤＣｌ３中的反应。结果表明，在Ｘ＝ＮＣＯ＾－和ＣＨ３ＣＯ＾－２的情况下，Ｈ２Ｓ优先与这些Ｐｄ配合物的阴离子作用生成相应的共轭酸ＨＸ和Ｐｄ２（ＳＨ）２（ｄｐｍ）２，后者在Ｈ２Ｓ存在下又进一步转化为Ｐｄ２（ＳＨ）     

CO(υ)高振动激发态向C2H2的振动传能研究

用时间分辨富里叶红外发射谱研究了高振动激发态ＣＯ向Ｃ２Ｈ２的传能，得到了ＣＯ（ｖ＝１－３）各振动态布居及其随时间的变化。利用微分法解出弛豫微分方程组，获得ＣＯ（ｖ＝１－３）向Ｃ２Ｈ２的传能速率常数分别为：２．０±０．１，６．０±０．２和９．４±０．８（１０＾－１３ｃｍ＾３·ｍｏｌｅｃｕｌｅ＾－１·ｓ＾－１）。传能速率随着振动量子数的增加而迅速增加。ＣＯ的振动能应向Ｃ２Ｈ２的对称伸缩模ｖ２近共振Ｖ－     

电子激发态CH（C^2Σ^＋）自由基的猝灭速率常数的测定

用２６６ｎｍ激光光解ＣＨＢｒ３分子产生ＣＨ（Ｃ）态自由基，通过测量ＣＨ（Ｃ＾２Σ＾＋→Ｘ＾２Ⅱ）的总荧光信号强度来测定室温下Ｏ２、Ｎ２、ｎ－Ｃ５Ｈ１２、ｎ－Ｃ６Ｈ１４和ｎ－Ｃ７Ｈ１６对ＣＨ（Ｃ２Σ＾＋，ｖ′＝０）的猝灭常数。结果表明，这些碰撞伴侣（Ｏ２和Ｎ２例外）对ＣＨ（Ｘ、Ａ、Ｂ和Ｃ）的反应或猝灭速率常数ｋ存在下列关系：ｋ（Ｘ）〉ｋ（Ｂ）〉ｋ（Ａ）≈ｋ（Ｃ），且烷烃分子对ＣＨ（Ｃ）态的猝灭速率常     

Efficient Coherent Population Transfer of D2 Molecules by Stark-induced Adiabatic Raman Passage

Preparation of a high flux of hydrogen molecules in a specific vibrationally excited state is the major prerequisite and challenge in scattering experiments that use vibrationally excited hydrogen molecules as the target. The widely used scheme of stimulated Raman pumping suffers from coherent population return which severely limits the excitation efficiency. Re-cently we successfully transferred D₂ molecules in the molecular beam from (v=0, J=0) to (v=1, J=0) level, with the scheme of Stark-induced adiabatic Raman passage. As high as 75% of the excitation efficiency was achieved. This excitation technique promise to be a unique tool for crossed beam and beam-surface scattering experiments which aim to reveal the role of vibrational excitation of hydrogen molecules in the chemical reaction.     

Stark shift of the A2Pi(1/2) state in 174YbF

We have measured the Stark shift of the A2Pi(1/2)-X2Sigma+ transition in YbF. We use a molecular beam triple resonance method, with two laser transitions acting as pump and probe, assisted by an rf transition that tags a single hyperfine transition of the X state. After subtracting the known ground state Stark shift, we obtain a value of 70.3(1.5) Hz/(V/cm)2 for the static electric polarizability of the state A2Pi(1/2) (J=1/2),f by fitting our data to a purely quadratic Stark shift in the interval 0-5 kV/cm. A more exact analysis that does not assume a perfectly quadratic Stark effect yields the value mu(e)=2.48(3) D for the electric dipole moment of the A2Pi(1/2)(v=0) state.     

Energy-transfer dynamics of high-pressure rovibrationally excited molecular H2

The energy-transfer dynamics of high-pressure molecular H(2) gas initially prepared in the |X (1)Sigma(g) (+),v = 1,J = 1 state using stimulated Raman pumping are probed with rotational Raman scattering. A computer simulation that incorporates the effects of collision-induced vibrational energy transfer is described and used to fit the experimental Raman scattering results obtained as a function of the pump/probe delay time. The 4.78 x 10(-14) +/- 3.85 x 10(-16) cm(3) s(-1) molecule(-1) vibrational energy-transfer rate for decay from the |X (1)Sigma(g) (+),v = 1,J = 1 >state compares well with other lower-pressure studies.     

Efficient Preparation of D2 Molecules in v=2 by Stimulated Raman Pumping

We report the preparation of D₂ molecules in v=2 level in molecular beam condition. A single longitudinal mode laser system was used for excitation of D₂ from (v=0, j=0) to (v=2, j=0) with the scheme of stimulated Raman pumping. An excitation efficiency of 25.2% has been achieved, which was determined by the scheme of resonance-enhanced multiphoton ionization. Dependence of relative excitation efficiency on laser energy has been measured. We found that the increasing rate of excitation efficiency became slower as pulse energy of Stokes laser increase, while the excitation efficiency still increases approximately linearly with pump pulse energies up to 60 mJ. The spectral line shapes of Raman transition was also measured at different laser energies and considerable dynamical Stark effect was observed. A single peak was found on the three dimension surface of relative excitation efficiency, indicating the process occurred in the present study is a process of stimulated Raman pumping instead of stimulated adiabatic Raman passage.     

CS2+离子 C2Σg+←B2Σu+跃迁的Franck-Condon因子计算以及与光解离谱的比较

将线性三原子分子离子CS2+的对称伸缩振动简化为SC和S之间的简谐振动, 用谐振子的势能曲线和波函数对CS2+分子离子 C2Σg+和 B2Σu+电子态(对称伸缩)振动能级间跃迁的Franck-Condon因子进行了计算, 得到的结果与 C2Σg+←B2Σu+跃迁的光解离谱实验强度进行了比较, 对前人给出的分子数据(转动常数、分子平衡核间距)进行了验证和分析, 讨论了经由 C2Σg+←B2Σu+电子态振动能级间跃迁的光解离机理.     

Can stimulated Raman pumping cause large population transfers in isolated molecules?

When stimulated Raman pumping (SRP) is applied to a stream of isolated molecules, such as found in a supersonic molecular beam expansion, we show that SRP can neither saturate nor power broaden a molecular transition connecting two metastable levels that is resonant with the energy difference between the pump and Stokes laser pulses. Using the optical Bloch-Feynman equations, we discuss the pumping of the hydrogen molecule from H(2) (v = 0, J = 0, M = 0) to H(2) (v = 1, J = 2, M = 0) as an illustration of how coherent population return severely reduces the SRP pumping efficiency unless the pump and Stokes laser pulses are applied with an appropriate relative delay and ratio of intensities.     

Dipole moment for the v2 = 1 vibrational state of 15NH3 by saturation laser stark spectroscopy

An intracavity Stark cell was used to observe inverse Lamb dips of five transitions of the ¹⁵NH₃v₂ band, saturated by CO₂ laser lines. Accurate values of the electric dipole moment of v₂ = 1, (J,K) = (4,4); (7,7); (8,8) and (11,9) states and of the (J,K) = (5,3) vibrational ground state have been obtained.     

Influence of vibrational excitation on the nonadiabatic reactions of metal atoms with H2

The reactions of alkaline earth metal atoms, Mg(3s3p 1P1) and Ca(4s4p 1P1), with H2(v = 1, j) are studied using a pump-probe technique combined with stimulated Raman pumping and coherent anti-Stokes Raman spectroscopy. For the Ca(4 1P1) case, the energy deposited in the v = 1 level enlarges the H2 bond distance to help facilitate the reaction without opening an additional pathway. For the Mg(3 1P1) case, the vibrational excitation of H2 leads to enhancement of the low rotational component of the rotational distribution and the MgH(v = 0)/MgH(v = 1) ratio. These results can be predicted with quasi-classical trajectory calculations and interpreted with a kinematic collision model.     

Spectral properties of Eu(III) compound with antibacterial agent ciprofloxacin (cfqH). Crystal structure of [Eu(cfqH)(cfq)(H2O)4]Cl2 · 4.55H2O

A novel europium complex of fluoroquinolone ciprofloxacin (cfqH) with formula [Eu(cfqH)(cfq)(H₂O)₄]Cl₂ · 4.55H₂O (1) was synthesized and its crystal structure determined by X-ray crystallography. The coordination number of europium is eight and in this structure two bidentate, O,O-bonded quinolone molecules and four aqua ligands are coordinated to the metal. One molecule of quinolone is anionic whereas the other is zwitterionic. Additionally, two chloride ions are also present in the structure to compensate the charge of the europium(III) whilst disordered solvent water molecules too are present. The spectral properties (IR, Raman, luminescence) of compound 1 were studied. Analysis of the Stark structure of the luminescence spectra was carried out and the scheme of the electronically excited states and photophysical processes of compound 1 was arranged. The spectral properties show that europium–ciprofloxacin complexes could be suitable for various applications based on their solution-state stability as measured by ¹H and ¹⁹F NMR.     

A molecular-beam optical Stark study of lines in the (1,0) band of the F4delta(7/2)-X4delta(7/2) transition of iron monohydride, FeH

A supersonic molecular beam of iron monohydride, FeH, has been generated using a laser ablation/chemical reaction scheme and probed at near-natural linewidth resolution by optical Stark spectroscopy utilizing laser-induced fluorescence detection. The observed Stark splitting in Q(3.5) and R(3.5) lines of the F4delta(7/2) <-- X4delta(7/2) (1,0) transition were analyzed to determine values for the magnitudes of the permanent electric dipole moments, absolute value(mu), which were found to be 2.63(3) and 1.29(3) D for the X4delta (v = 0) and F4delta (v = 1) states, respectively. A comparison with ab initio theoretical predictions is made. The lambda doubling in the low-J levels of the F4delta(7/2) (v = 1) state is also modeled.