Oxygen plasma activation of Cr(CO)6 on α-Fe2O3(0001)

The chemistry of Cr(CO)₆ on the Fe₃O₄(111) surface termination of α-Fe₂O₃(0001) was explored using temperature programmed desorption (TPD), Auger electron spectroscopy (AES), static secondary ion mass spectrometry (SSIMS) and low energy electron diffraction (LEED) both with and without activation from an oxygen plasma source. No thermal decomposition of Cr(CO)₆ was detected on the surface in the absence of O₂ plasma treatment, with first layer molecules desorbing in TPD at 215 K from a close-packed overlayer. The interaction of first layer Cr(CO)₆ with the Fe₃O₄(111)-termination was weak, desorbing only ～ 30 K above the leading edge of the multilayer state. Activation of multilayer coverages of Cr(CO)₆ with the O₂ plasma source at 100 K resulted in complete conversion of the outer Cr(CO)₆ layers, presumably to a disordered Cr oxide film, with Cr(CO)₆ molecules near the surface left unaffected. Absence of CO or CO₂ desorption states suggests that all carbonyl ligands are liberated for each Cr(CO)₆ molecule activated by the plasma. AES and SSIMS both show that O₂ plasma activation of Cr(CO)₆ results in a carbon-free surface (after desorption of unreacted Cr(CO)₆). LEED, however, shows that the Cr oxide film was disordered at 600 K and likely O-terminated based on subsequent water TPD. Attempts to order the film at temperatures above 650 K resulted in dissolution of Cr into the α-Fe₂O₃(0001) crystal based on SSIMS, an observation linked to the Fe₃O₄(111) termination of the surface and not to the properties of α-Cr₂O₃/α-Fe₂O₃ corundum interface. Nevertheless, this study shows that O₂ plasma activation of Cr(CO)₆ is an effective means of depositing Cr oxide films on surfaces without accompanying carbon contamination.     

Calculation on the CO2 influences on the structure,stability of (MgO)m (m = 1–6) clusters

ABSTRACT

The concentration of carbon dioxide (CO₂) has a significant influence on the morphology of thermal decomposition products of magnesite. So, structures, stabilities and adsorption mechanisms of (MgO)_m (m?=?1–6) clusters by one or two CO₂ molecules were calculated by the GGA-PW91 method. The results show that the stability of the considered clusters is (MgO)_m(CO₂)₂ clusters > (MgO)_m(CO₂) clusters > (MgO)_m clusters by the average binding energy. Certain low-lying isomers of (MgO)_m(CO₂) and (MgO)_m(CO₂)₂ clusters which have an isolated O atom are deviating from the cluster center which possess higher kinetic activity. (MgO)_m clusters prefer to adsorb a CO₂ molecule, while (MgO)₃(CO₂) clusters prefer to adsorb a CO₂ molecule rather than the neighbors. Magnesite is difficult to transit to (MgCO₃)₂ clusters at room temperature. However, magnesite will spontaneously transit to (MgO)₂ clusters and further transit to MgO crystal which need to adsorb more energy at 700?K.     

配合物Zn3(NCS)6(L1)6(NO3)2及Ni3(NCS)6(L2)6(NO3)2的合成、光谱表征及荧光性质

以去离子水为溶剂,合成了以Zn2+及N12+为中心,以L1,L2[L1=4-氨基-3,5-二甲基-1,2,4-三唑,L2=4-氨基-1,2,4-三唑]及硫氰酸根为配体的两种配合物,对其进行了元素分析、金属离子络合滴定、摩尔电导测定,确定了配合物组成分别为Zn3(NCS)6(L1)6(NO3)2及Ni3(NCS)6(L2)6(NO3)2,同时对两种配合物做了红外光谱、紫外光谱及荧光光谱的测试表征.荧光光谱的测试表明两种配合物均在415 nm有一强的荧光发射峰,且镍配合物的荧光要明显强于锌配合物,两种配合物有望成为蓝光发光材料.     

Cs(6P)+(Ne,N2)碰撞能量转移

在气体样品池条件下,研究了Cs(6P3/2) (Ne,N2)碰撞能量转移过程.用调频半导体激光器激发Cs原子至Cs(6P3/2)态,在不同的Ne或N2气压下,测量了直接6P3/2→6S1/2荧光和转移6P1/2→6S1/2荧光,对于6P3/2与Ne的碰撞,电子态能量仅能转移为Ne原子的平动能.在与N2的碰撞中,向分子振转态的转移是重要的.利用速率方程分析,可以得到碰撞转移速率系数,对于Ne,6PJ精细结构碰撞转移速率系数为1.45×10-12cm3·s-1.对于N2,测量6P Ne和6P N2二种情况下荧光的相对强度比,确定精细结构速率系数为1.64×10-12cm3·s-1,6P态猝灭速率系数为4.88×10-12cm3·s-1.     

Momentum transfer dependence of the (6σ)2 → (6σ, npπ) window resonances in N2O

Scattered electron spectra of N₂O employing 200 eV electrons have been recorded in an energy loss regime of 17 to 21 eV corresponding to excitation out of the 6σ orbital. In this region, the shapes of the (6σ, npπ) window resonance series exhibit a strong variation over a scattering angular range of 3 to 9°. For the n = 3 member, this is attributed to a change in the resonance profile index from ~ −0.2 to +0.9. Although profile index sign reversals have been measured in ejected electron spectra, their interpretation is difficult. The scattered electron aspect of our measurement lends itself to a more straightforward interpretation as a sign reversal in the transition amplitude for excitation to the modified discrete state, and our measurements provide one of the first clear-cut examples of this effect.     

The diphenylphosphino radical, (C6H5)2˙P

The diphenylphosphino radical, (C₆H₅)₂P, has been observed at room temperature in X-irradiated single crystals of triphenylphosphine oxide and diphenylphosphine sulphide and in ultra-violet irradiated polycrystalline diphenylphosphine at 77 K. The isotropic ³¹P coupling constant is deduced to be +252 MHz and the anisotropic components are approximately 504, -252, -252 MHz. The largest value of the g tensor lies perpendicularly to the direction of the largest hyperfine coupling constant, the values in diphenylphosphine sulphide being 2·0094, 2·0035 and 2·0021. X-irradiated triphenylphosphine oxide also contains the (C₆H₅)₂PO radical.     

Thermal-energy Pooling Collisions in Cesium Vapor 6P_(3/2) 6P_(3/2) →7P_J 6S_(1/2)

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CN红带A 2Пi-X 2Σ+(6, 1)和(7, 2)带振转光谱研究

通过微量CH3CN(36 Pa)与He(660 Pa)混合气体交流Penning辉光放电获得CN自由基分子, 采用光外差-磁旋转-浓度调制光谱技术, 在可见光波段16 850～17 480 cm-1进行了转动分辨光谱测量, 分别标识了CN分子红带A 2Пi-X 2Σ+(6, 1)和(7, 2)138条和118条的转动光谱(其余光谱为C2自由基及CN红带(8, 3)带光谱). 理论拟合分子常数时考虑电子态间的微扰作用, 采用有效哈密顿量矩阵对角化获得了A 2Пi(ν=6, 7)态更精确的分子常数及电子态A 2Пi(ν=7)与 X 2Σ+ (ν=11)之间的微扰常数ξ, η, 总体拟合方差均小于实验误差0.007 cm-1, 表明拟合结果是非常精确的.     

高温下CO2—N2,CO2—CO2混合气体中CO2分子的谱线压力展宽半宽度

用无限阶突变近似方法计算了ＣＯ２－Ｎ２,ＣＯ２－ＣＯ２混合气体中Ｃ承２９６－１９２９Ｋ温度下转动量子数从１到３０的谱线压力展宽半宽度。计算过程中各系统的相互作用势采用改进的Ｂｕｃｋｉｎｇｈａｍ模型势。得到的结果和现有结果符合较好。     

(C6H5R)Mo (CO)3复合体系结构的密度泛函研究

用量子化学DFT-B3LYP方法在IANL2DZ基组水平上对标题复合物体系的可能构型进行了自由优化,在此基础上进行了频率分析,得到了复合物的电子结构和红外光谱.原子净电荷、前沿轨道能量都表明,Mo(CO)3和C6H5R结合时电子从苯环向Mo转移,形成电荷转移复合物.复合物的键长、Wiberg键级表明,它们之间的结合方式和氢键的结合方式相似,且属强氢键.复合物的红外特征振动频率位于212cm-1～224 cm-1,对应于Mo(CO)3的金属垂直于C6H5R中的苯环平面的来回振动,同时形成复合物后,原来位于3200 cm-1左右的峰活性消失.     

195Pt,15N NMR spectroscopy of aqueous solutions of mixed valent oxonitrocomplexes,Pt(II,IV): K5[(NO2)3PtIV(μ-O)3 Pt 3 II (NO2)6] and K8[(NO2)6Pt 3 II (μ-O)3PtIV(μ-O)3Pt 3 II (NO2)6]

Two aqueous solutions of oxonitrocomplexes comprising di- and tetravalent platinum atoms, K₅[(NO₂)₃Pt^IV(μ-O)₃Pt ₃ ^II (NO₂)₆]· 3H₂O and K₈[(NO₂)₆Pt ₃ ^II (μ-O)₃Pt^IV (μ-O)₃Pt ₃ ^II (NO₂)₆] · 7H₂O, have been studied by¹⁹⁵Pt and¹⁵N NMR technique. Both compounds, enriched with the¹⁵N (95%) isotope, were synthesized by thermal denitrozylation of K₂[Pt(NO₂)₄]. Constants of spin-spin scalar coupling,¹⁹⁵Pt-¹⁵N and¹⁹⁵Pt^II-¹⁹⁵Pt^IV, were obtained for tetra-and heptameric complexes in aqueous solutions through multiplet simulation. The¹⁹⁵Pt and¹⁵N NMR spectra of the same solutions obtained two months after their preparation show signals from the hydrolytic forms of the tetrameric complex as well as the signals from mono- di- and trimeric oxonitrocomplex forms of divalent platinum. All signals of species formed as a result of hydrolysis were identified.     

Vibrational spectra of Te(OH)6·X2SO4 (X = Tl,Na)

The IR and Raman spectra of Te(OH)₆·X₂SO₄ (X = Tl, Na) have been recorded and analysed. The splitting of the nondegenerate mode of the sulphate ion suggests factor group interaction between the vibrating ions. The linear distortion of the sulphate ions is found to be more in Te(OH)₆·Na₂SO₄ than in Te(OH)₆·Tl₂SO₄. The tellurate ion seems to be less distorted than the sulphate ion. The appearance of Raman inactive modes of the tellurate ion indicate the presence of strain produced by the crystalline field. The anions are also found to coexist independently.     

Paramagnetic center Cd+(2 S 1/2) in natural carbonate apatites Ca5(PO4)3 ? n (CO3) n (F,OH)

The stable paramagnetic center Cd⁺(² S _1/2) in natural sedimentary calcium phosphates containing a cadmium impurity has been studied using electron paramagnetic resonance. The parameters of the spectrum have been determined, and the influence of different radiation types on the paramagnetic center has been investigated.     

Bridge-bonded CO in Ni(110)-p2mg(2× 1)-CO: a SEXAFS study

Surface-extended X-ray-absorption fine-structure measurements have been performed to determine the adsorption site of CO in the densely-packed system Ni(110)-p2mg(2 × 1)-CO. The analysis shows that CO adsorbs in a tilted configuration on short-bridge sites yielding a nearest-neighbour O-Ni distance of 2.84 ± 0.05 Å. Tilted CO molecules in on-top positions can be definitely ruled out.     

Structure and magnetic properties of the intermetallic La2Co17−xMox (x=0.5, 1, 1.5, 2) and La2Co16−yFeyMo (y=0, 1, 2, 3, 4, 6) compounds

The effect of Mo and Fe atoms on the crystal structure and magnetic properties of the intermetallic La₂Co_17−xMo_x (x=0.5, 1, 1.5, 2), and La₂Co_16−yFe_yMo (y=0, 1, 2, 3, 4, 6) compounds have been studied by X-ray diffractometry, magnetic measurements and Mössbauer spectroscopy. All samples belong to the rhombohedral Th₂Zn₁₇-type structure and their lattice parameters a and c increase both with Mo and Fe content. From the La–Co–Mo samples only the one with x=0.5 presents planar anisotropy, whereas from the La–Co–Fe–Mo samples only the y=1 has uniaxial anisotropy. The magnetization M_S and the Curie temperature T_C decrease upon Mo substitution, whereas the anisotropy field H_A does not change significantly. In the Fe-substituted compounds M_S increases, but the Curie temperature increases slightly for 0⩽y⩽4 but decreases in y=6. The low temperature M–T curve shows that the samples La₂Co_16.5Mo_0.5, and La₂Co₁₀Fe₆Mo present a spin reorientation transitions at 70 and 260 K, respectively. Mössbauer samples were obtained for all Fe-containing samples in the temperature range 20–300 K. Above 260 K a jump in the values of the hyperfine fields and quadrupole splitting parameters is observed which can be associated to the spin reorientation.     

[(μ-CF3CO2)2Ln (μ-CF3HCO2) Al (i-Bu)2·2THF]2(Ln=Nd,Y)配合物的NMR和X-射线衍射研究

对[μ-CF₃CO₂)₂Ln(μ-CF₃HCO₂)Al(i-Bu)₂·THF]₂(Ln=Nd,Y)配合物单晶结构的X-射线分析指出,配合物具有中心对称性,配位中心由两个稀土和两个Al离子组成,稀土由两个THF和6个TFA分子配位形成畸变的三盖三棱柱结构,Al由两个TFAG和两个i-Bu配位形成四面体结构。桥连Al与两个稀土的TFA分子的羧基发生歧化加氢,其碳原子由SP²型转变为SP³型.NMR研究表明,在THF溶液中,该配合物保持了它在单晶中的配位结构,所不同的是两个i-Bu在溶液中有两种异构形成,二者间为慢交换过程。     

H_2CO+OH~-反应的理论研究(英文)

用量化从头算方法在MP4(SDTQ)理论水平上首次考察了甲醛和氢氧根负离子反应的所有可能的反应通道.用6-311 G(3df,3pd)基组对所有的反应中间体、过渡态和产物开展了结构优化和单点能量计算,并经频率分析和内禀反应反应坐标计算(IRC)确认反应物、中间体、过渡态和产物的相关性.在H2CO OH-所有可能的反应通道中生成CHOO- H2的通道是该反应的最可几通道,而由于羰基的存在生成H3O-的通道更容易分解产生CHOO- H2.在高计算水平下计算的氢交换反应结果与文献报道相同.通过计算提出亲核加成过程的反应通道,主要产物生成H2和生成COOH-/HCOO-/OCHO-异构体.所有反应通道的反应几率顺序为COOH- H2>H3O- CO>HCHO OH->CHO- H2O>HCOO- H2>OCHO- H2.