(Ce_(0.67)Tb_(0.33))MgAl_(11)O_(19)和BaMgAl_(10)O_(17)∶Eu~(2 )荧光体的微波辐射合成及其发光性能

用微波辐射法合成了（Ｃｅ０．６７Ｔｂ０．３３）ＭｇＡｌ１１Ｏ１９（ＰＧ）和ＢａＭｇＡｌ１０Ｏ１７（ＰＢ）两种荧光体，经Ｘ射线粉末衍射分析，其ｄ值和Ｉ／Ｉ０值与ＪＣＰＤＦ３６７３和２６１６３基本一致。计算得到ＰＧ的晶胞参数ａ＝０５５８２ｎｍ，ｃ＝２１８８４ｎｍ；Ｐ－Ｂ的晶胞参数α＝０５６１６ｎｍ，ｃ＝２２６１４ｎｍ。测定了两种荧光体的激发光谱和发射光谱。Ｐ－Ｇ的色坐标ｘ＝０３１６，ｙ＝０５６５；Ｐ－Ｂ的色坐标ｘ＝０１５６，ｙ＝０１０６。与市售同类荧光粉相比，Ｐ－Ｇ的相对发光强度为８８％，Ｐ－Ｂ的相对发光强度为８０％。     

两个异亚砂基乙酰丙酮—N—芳基亚胺Pd（Ⅱ）配合物的合成 …

合成了两个异亚硝基乙酰丙酮－Ｎ－芳基亚胺的Ｐｄ（Ⅱ）配合物,ＰｄＣｌ（Ｃ６Ｈ５－ＩＡＩ）（Ｃ６Ｈ５ＮＨ２）（１）和ＰｄＣｌ（ｐ－ＣＨ３Ｃ６Ｈ４－ＩＡＩ）（ｐ－ＣＨ３Ｃ６Ｈ４ＮＨ２）（２）,并测定了配合物１的晶体结构。配合物１晶体属正交晶系,空间群为Ｐｃａ２１,晶胞参数ａ＝１．８５８７（４）ｎｍ,ｂ＝０．９３８０（２）ｎｍ,ｃ＝２．１２３７（４）ｎｍ,Ｚ＝８,Ｆ（０００）＝１７６０,μ＝１．１６０ｍ     

二次锂电池正极材料LixNi0.3Co0.7O2的XPS与XRD研究

结果表明，ＬｉｘＮｉ０．３Ｃｏ０．７Ｏ２具有六方晶系Ｒ３＾－ｍ空间群结构。当Ｘ－１，０．３１５时，其晶胞参数分别为ａ＝２．８２６ｎｍ，ｃ＝１４．１３０ｎｍ和ａ＝０．２８０８ｎｍ，ｃ＝１．４２５３ｎｍ；ＭＯ６（Ｍ＝Ｎｉ，Ｃｏ）八面体中Ｍ－Ｏ平均距离分别为０。１９４１ｎｍ和０．１９３３ｎｍ。ＸＰＳ分析结果表明ＬＩｘＮｉ０．３ＣＯ０．７Ｏ２表面存在Ｌｉ２Ｏ，同时探讨了其中过渡金属离子的３ｄ电子结构变化。     

具有不同类型桥基的双核Cu(Ⅱ)-Schiff碱配合物的合成和晶体结构

合成了３个分别以Ｃ２Ｏ２－４（［Ｃｕ２（Ｌ１）２（ｏｘ）］，１），ＡｃＯ－（［Ｃｕ２（ＡｃＯ）（Ｌ２）２］ＢＦ４，２）和酚氧（［Ｃｕ２（Ｌ３）２］（ＣｌＯ４）２，３）为桥基的双核铜配合物，并测定了１的复配合物［Ｃｕ２（Ｌ１）２（ｏｘ）］·［Ｆｅ（ＯＨ）２（Ｈ２Ｏ）４］ＣｌＯ４·Ｈ２Ｏ（１′）及２和３的晶体结构．Ｘ射线衍射结果表明：１′，２和３分别属于Ｆｄｄｄ，Ｐ２１／ｃ和Ｐ２１／ｃ空间群．晶胞参数：［Ｃｕ２（Ｌ１）２（ｏｘ）］［Ｆｅ（ＯＨ）２（Ｈ２Ｏ）４］ＣｌＯ４·Ｈ２Ｏ，ａ＝２．４３９０（４）ｎｍ，ｂ＝３．０５３８（６）ｎｍ，ｃ＝１．８４９４（６）ｎｍ，α＝β＝γ＝９０．００°；２，ａ＝０．８４７（１）ｎｍ，ｂ＝２．６５４２（８）ｎｍ，ｃ＝１．４１００（６）ｎｍ，β＝９１．３４（６）°；３，ａ＝０．７６４６（３）ｎｍ，ｂ＝１．６９８３（３）ｎｍ，ｃ＝２．４４１７（３）ｎｍ，β＝９７．１１°     

三环己基锡O,O‘—二（4—氯苯基）—二硫代磷酯酯和二丁基锡双（O,O’—二…

三环己基锡Ｏ，Ｏ’－二（４－氯苯基）二硫代磷酸酯（Ｉ），Ｃ３０Ｈ４１Ｃｌ２（Ｏ２ＰＳ２Ｓｎ，Ｍｒ＝７１８．３６，单斜晶系，Ｐ２１／ｎ，ａ＝１６．１５１（２），ｂ＝９．４１５９（１），ｃ＝２２．９８７（３），Ａ，β＝１０５．６９（１）°，Ｚ＝４，Ｄｃ＝１．４１８ｇ．ｃｍ＾－３，Ｒ＝０．０６３；二丁基锡双（Ｏ，Ｏ’－二（４－甲基苯基）二硫代磷酯酯（Ⅱ），Ｃ３６Ｈ４６Ｏ４Ｐ２Ｓ４Ｓｎ，Ｍｒ＝８５１．６６     

铕—对氨基苯甲酸—邻菲咯啉配合物[Eu（p—ABA）3Phen.H2O]（C2H5OH）的…

「Ｅｕ（ｐ－ＡＢＡ）３Ｐｈｅｎ；Ｈ２Ｏ」（Ｃ２Ｈ５ＯＨ）（ｐ－０ＡＢＡ＝对氨基苯甲酸根，Ｐｈｅｎ＝邻菲咯啉）配合物晶体属三斜晶系，Ｐ１＾－空间群，ａ＝１．２２６８９３）ｎｍ，ｂ＝１．４００５（３）ｎｍ，ｃ＝１．０４４０（３）ｎｍ；ａ＝１０２．６９９２），β＝１０８．９３（２），γ＝９２．８５（２）；Ｚ＝２，Ｔ＝２７３Ｋ。     

双核钯配合物［Ph_2P（o－C_6H_4CO）PdCl］_2·2CH_2Cl_

合成了双氯桥双核钯配合物［Ｐｈ_２Ｐ（ｏ－Ｃ_６Ｈ_４ＣＯ）ＰｄＣｌ］_２·２ＣＨ_２Ｃｌ_２进行了元素分析、红外光谱表征和晶体结构测定，研究了其催化氢化性能。在３０～８０℃、氢分压１．０～５．０ＭＰａ的范围内。发现该配合物是催化氢化丙烯酸为丙酸的有效催化剂．晶体［Ｐｄ_２Ｃｌ_２（Ｃ_（１９）Ｈ_（１４）ＯＰ）_２］·２ＣＨ_２Ｃｌ_２属Ｐ１空间群，ａ＝０．９３０４（３）ｎｍ，ｂ＝１．０３９２（２）ｎｍ，ｃ＝１．１０６２（３）ｎｍ；ａ＝１０２．７８（２），Ｂ＝９７．３５（３），γ＝９５．２５（２），Ｖ＝１．０２６４ｎｍ~３，Ｍ＝１０３２．１７，２＝１，Ｄｃ＝１．６７０ｇ／ｃｍ~３，ｕ＝１３．６９５ｃｍ~（－１），Ｆ（０００）＝５１２，用１９４５个独立衍射精修结构，最终Ｒ＝０．０３６。     

（Y（NTO）2NO3（H2O）5）.2H2O的制备,晶体结构和热分解机理的…

合在了（Ｙ（ＮＴＯ）２ＮＯ３（Ｈ２Ｏ）５）．２Ｈ２Ｏ（ＮＴＯ为３－硝基－１，２，４－三唑－５－酮）并测定了晶体结构，晶体属单斜晶系，空间群Ｃｍ，晶胞参数：ａ＝０．６７７３（２）ｎｍ，ｂ＝２．０８６６（２）ｎｍ，ｃ＝０．６５５１（１）ｎｍ；β＝１０２．９８（２）°Ｖ＝０．９０２１（１）ｎｍ＾３，Ｚ＝２，Ｄｃ＝１．９７０ｇ．ｃｍ＾－３，μ＝３３．４９ｃｍ＾－１，Ｆ（０００）＝５４０，Ｒ＝０．０３２，中     

二价铕中性芳烃配合物［Eu（C_6Me_6）（AlCl_4）_2_4·Me_4

首次合成了二价铕中性芳烃配合物［Ｅｕ（Ｃ６Ｍｅ６（ＡｌＣｌ４）２］·Ｍｅ４Ｃ６Ｈ２，并经红外光谱，激发光谱和荧光光谱表征，测定了晶体结构。配合物属单斜晶系，Ｐ２／ｃ空间群，晶胞参数ａ＝１．７６５２（４）ｎｍ，ｂ＝１．５９１８（４）ｎｍ，ｃ＝１．８７５２（５）ｎｍ；β＝９７．６１（５）°，Ｚ＝２，Ｒ＝０．０４９６，Ｒｗ＝０．０４６２。     

[Mn2（bzacen）2（MeOH）2（μ—4,4‘—bipy）]（ClO4）2的合成,结构…

合成了〔Ｍｎ２（ｂｚａｃｅｎ）２（ＭｅＯＨ）２（μ－４，４′－ｂｉｐｙ）〕（ＣｌＯ４）２化合物，并测定其晶体结构。该晶体属单斜晶系，空间群Ｐ２１／ｎ，晶胞参数：ａ＝１．３０８２（３）ｎｍ，ｂ＝１．２７１３（３）ｎｍ，ｃ＝１．８００６（５）ｎｍ，β＝１１０．９１（２）°，Ｚ＝２，μ＝５．９７ｃｍ＾－１，Ｒ＝０．０５８０，ＧＯＦ＝１．６６。在配合物阳离子中，４，４′－联吡啶桥联２个〔Ｍｎ（ｂｚａｃｅｎ     

High-precision measurements of 17O/16O and 18O/16O of O2 and O2/Ar ratio in air

A method for high-precision and high-accuracy mass spectrometric measurements of the ratios among the three oxygen isotopes, and of the O(2)/Ar ratio, is presented. It involves separation of the O(2)-Ar mixture from air and includes a fully automated system that ensures highly reliable sample processing. Repeated measurements of atmospheric oxygen yield the repeatability (+/-SE x t, standard error of the mean (n = 12) multiplied by Student's t-factor for a 95% confidence limit) of 0.004, 0.003 and 0.2 per thousand for delta(18)O, delta(17)O and delta O(2)/Ar, respectively.     

High precision measurements of 17O/16O and 18O/16O ratios in H2O

We have optimized the method of water fluorination using the solid reagent CoF3 to produce O2. This allows isotope ratio measurements by dual-inlet mass spectrometry with very high precision of 0.01 to 0.03/1000 for both delta17O and delta18O. Using this method, delta17O and delta18O of atmospheric O2 were determined as 12.08 and 23.88/1000 vs. VSMOW, respectively. Likewise, delta17O and delta18O of GISP were -13.12 and -24.73/1000, and for SLAP they were -29.48 and -55.11/1000 vs. VSMOW, respectively. Analysis of these data in a ln(delta17O + 1) vs. ln(delta18O + 1) plot yields a line with a regression coefficient (lambda) of 0.5279 +/- 0.0001 (R2 = 0.999999). We also determined the fractionation factors 17alpha and 18alpha in liquid-vapor equilibrium, and found that the ratio ln 17alpha/ln 18alpha is constant (0.529 +/- 0.001) over the temperature range 11.4 to 41.5 degrees C.     

Electrooptic response of smectic O and smectic O

We present the results of our investigations on the electrooptic properties of the smectic O and O* phases of m7tac (1-methylheptyl terephthalylidene-bis-4-aminocinnamate). At low voltages, we observed striking electrochromic effects and, in O* at high voltages, a field induced phase transition. Freely suspended thick films of m7tac in the O and O* phases are weakly biaxial. A framework is proposed to account for our observations.     

Electrooptic response of smectic O and smectic O

Abstract

We present the results of our investigations on the electrooptic properties of the smectic O and O* phases of m7tac (1-methylheptyl terephthalylidene-bis-4-aminocinnamate). At low voltages, we observed striking electrochromic effects and, in O* at high voltages, a field induced phase transition. Freely suspended thick films of m7tac in the O and O* phases are weakly biaxial. A framework is proposed to account for our observations.     

Laser Raman studies on compounds 7.O4O.7 and 7.O5O.7

Laser Raman studies on two compounds of the α,ω-bis(4-alkylanilinebenzylidene -4′-oxy)alkane series were carried out in the spectral regions 1140–1220 and 1550–1650 cm^-1 as a function of temperature. Compounds 7.O4O.7 and 7.O5O.7, exhibit SmA and SmF phases. The structural differences between these liquid crystal dimers, having either an odd or an even number of carbon atoms in the spacer, are remarkably existent in the room temperature Raman spectra. The results are rationalized on the basis of the tendency of these compounds to exhibit bent shapes, and how this manifests in the odd-even effect at the molecular level assuming a semi-rigid core region of the dimeric molecule. It is found that the behaviour of the odd spacer dimer (7.O5O.7) agrees with the molecular model, whereas the even spacer dimer (7.O4O.7) behaves in a similar fashion to monomeric compounds such as the nO.m. compounds. In both cases, dynamic changes around the C=N bond have a profound effect both on the molecular shape in the different phases and on phase behaviour.     

Hyperthermal reactions of O and O2 with a hydrocarbon surface: direct C-C bond breakage by O and H-atom abstraction by O2

A C-C bond-breaking reaction has been observed when a beam containing hyperthermal oxygen was directed at a continuously refreshed saturated hydrocarbon liquid (squalane) surface. The dynamics of this C-C bond-breaking reaction have been investigated by monitoring time-of-flight and angular distributions of the volatile product, OCH3 or H2CO. The primary product is believed to be the methoxy radical, OCH3, but if this radical is highly internally excited, then it may undergo secondary dissociation to form formaldehyde, H2CO. Either the primary or the secondary product may scatter directly into the gas phase before thermal equilibrium with the surface is reached, or they may become trapped on the surface and desorb in thermal equilibrium with the surface. Direct, single-collision scattering events that produce a C-C bond-breaking product are described with a kinematic picture that allows the determination of the effective surface mass encountered by an incident O atom, the atom-surface collision energy in the center-of-mass frame, and the fraction of the center-of-mass collision energy that goes into translation of the scattered gaseous product and the recoiling surface fragment. The dynamical behavior of the C-C bond-breaking reaction is compared with that of the H-atom abstraction reaction, which was the subject of an earlier study. Another reaction, H-atom abstraction by O2 (which is present in the hyperthermal beam), has also been observed, and the dynamics of this reaction are compared with the inelastic scattering dynamics of O2 and the dynamics of H-atom abstraction by O. The dynamics involving direct inelastic and reactive scattering of O2 are also described in terms of a kinematic picture where the incident O2 molecule is viewed as interacting with a local region of the surface.     

W/O与O/W，W/O与双连续结构微乳液的界面电性质

无探针伏安法和电容法测定结果表明,在质量比H_2O/n-C_5H_(11)OH = 50/50条件下,SDS总含量<3%时,上相呈W/O结构,下相呈O/W结构,随着体系SDS 总含量的增大,界面上SDS量增加,界面电势ΔE、界面电容C、界面电荷传递电流 i_p均增加,而界面电阻率ρ_i则减小;当体系 SDS总含量≥3%时,上相呈W/O结构 ,下相呈双边续结构,各界面电性质变化幅度均变缓。