杨木和桉木的二维相关红外光谱

采用红外光谱结合二维相关分析技术,对两种速生阔叶树杨木和桉木进行了快速鉴别研究。结果表明,二者在一维红外光谱图上差别不明显,而二维相关红外谱图具有较大的差别。在800～1 500 cm-1波段范围内,二者的同步二维相关光谱图还比较类似,都在1 221,954,879 cm-1处出现较强的自动峰,在1 470, 1 150,1 1 05, 1 008 cm-1处出现微弱的自动峰。在1 500～1 800 cm-1波段范围内,杨木在1 655 cm-1处有一个非常强的自动峰,在1 600 cm-1附近有一个很弱的自动峰,二者形成了一对正的交叉峰;桉木在1 725,1 650和1 600 cm-1处均出现较强的自动峰,并形成一个较强的3×3峰组。除此之外,桉木还在1 580和1 510 cm-1出现2个弱的自动峰,其中1 580 cm-1和其余4个自动峰形成了较弱的负交叉峰,1 510 cm-1和其他3个自动峰形成正的交叉峰。这说明,桉木在1 500～1 800 cm-1波段对应的官能团比杨木相应的官能团对热微扰更为敏感,杨木和桉木的二维相关红外光谱差别,快速鉴别这两种木材的。     

GeS分子基态和低激发态的势能曲线与光谱性质

本文以aug-cc-pv5Z为基组, 采用考虑Davidson修正的多参考组态相互作用方法(MRCI+Q)得到了GeS分子基态(X¹Σ⁺)和5个低激发态(1¹Σ, 1¹Δ, A¹Π, 1⁵Σ⁺, 2⁵Σ⁺)的势能曲线. 计算结果表明: 2⁵Σ⁺态为排斥态, 其余5个态为束缚态; 6个态有着共同的离解通道, 离解极限均为Ge(³P)+S(³P). 利用计算得到的势能曲线得了X¹Σ⁺, 1¹Σ^-, 1¹Δ, A¹Π和1⁵Σ⁺态的垂直跃迁能T_e, 平衡键长R_e, 离解能D_e, 谐振频率ω_e, 非谐性常数ω_ex_e及平衡位置的电偶极矩. X¹Σ⁺态的R_e 为2.034 Å, D_e 为5.728 eV, ω_e为571.73 cm^-1, ω_ex_e为1.6816 cm^-1, 平衡位置的电偶极矩为1.9593 Debye. 激发态1¹Σ, 1¹Δ, A¹Π, 1⁵Σ⁺的T_e 依次为25904.81, 26209.22, 32601.19, 43770.26 cm^-1; R_e依次为2.313, 2.322, 2.188, 2.8790 Å; D_e依次为2.524, 2.487, 1.694, 0.3036 eV, ω_e依次为358.90, 353.08, 376.32, 134.96 cm^-1; ω_ex_e依次为1.2421, 1.2151, 1.6608, 1.9095 cm^-1; 平衡位置的电偶极矩依次为1.3178, 1.4719, 1.5917, -1.9785 Debye. 通过求解核运动的薛定谔方程得到了J=0时X¹Σ⁺, 1¹Σ^-, 1¹Δ, A¹Π和1⁵Σ⁺态前30个振动态的振动能级G_v和分子常数B_v, 得到的结果和已有的实验值及其他理论值符合较好.     

Computation of the electric and magnetic fields induced in a plasmacreated by ionization lasting a finite interval of time

S.C. Wilks et al. (1988) showed that when an infinite expanse of gas, carrying a linearly polarized electromagnetic wave, is instantly ionized, the initial wave is frequency upshifted. This phenomenon of frequency upconversion through flash ionization gives rise to steady-state transmitted and reflected electromagnetic waves and to a time-independent magnetic field. The case in which the final state of ionization is achieved not instantly but in a finite turn-on time, 0⩽t⩽t 0, which is followed by the steady state, is studied. It is shown that the electric field is obtained from the one-dimensional Helmholtz equation, d²F(t)/dt² +ω₀²g(t)F( t)=0, if electrons are born at rest when they are created during ionization. As a result, the instantaneous frequency of the upshifted radiation is ω(t)=√g(t). The electric field can be solved exactly for specific choices of g(t). It is solved using WKB approximations for arbitrary g(t). The magnetic field is then found by integrating Faraday's law. It is found that the steady-state electric field amplitude depends on the steady-state value o f g(t) but does not depend on the ionization time t₀. Conversely, the static magnetic field amplitude decreases with increasing turn-on time     

蒜氨酸和甲基蒜氨酸的红外及拉曼光谱研究

利用傅里叶红外光谱和共聚焦显微拉曼光谱技术,比较分析了大蒜主要功能活性成分前体蒜氨酸和甲基蒜氨酸粉末纯品的红外和拉曼谱。在3 200～2 800 cm-1和1 700～200 cm-1波段检测到显著的红外和拉曼吸收峰,其中蒜氨酸在3 080,1 617,1 582,1 496,1 418,1 342,1 301,919 cm-1处有8个较强的红外吸收峰,以及在3 088,1 636,1 404,1 290,1 051,790,745,693,588 cm-1处有9个较强的拉曼振动峰,可作为蒜氨酸的特征峰;甲基蒜氨酸在1 644,1 481,1 395,1 370,1 233,1 068,1 004,892 cm-1处有8个较强的红外吸收峰,以及在1 644,1 310,1 073,1 011,998,893,846,702,676 cm-1处有9个较强的拉曼振动峰,可作为甲基蒜氨酸的特征峰。蒜氨酸和同系物甲基蒜氨酸的红外及拉曼光谱具有明显差异,红外及拉曼光谱技术为蒜氨酸及其同系物的快速、 简便的分析提供了方法。     

Adsorption of hydrogen and carbon monoxide on Rh(1 1 1)/V surface alloys

A detailed study of the interaction of hydrogen and carbon monoxide with two different Rh(1 1 1)/V surface alloys (1/3 monolayer of V in the second atomic layer or 1/3 monolayer of V in form of islands on the surface) is presented in comparison to the clean Rh(1 1 1) surface. For hydrogen a decrease in the sticking coefficient is found for both alloy surfaces. The sticking coefficient of H₂ as a function of the translational energy is similar to the Rh(1 1 1) surface, showing a direct activated adsorption mechanism. For low translational energies hydrogen adsorption is dominated by dynamical steering on Rh(1 1 1) and by a precursor mechanism on the Rh(1 1 1)/V subsurface alloy. The H₂ TPD desorption peaks are shifted to lower temperatures on the alloy surfaces, caused by the downshift of the metal d-band due to V alloying. On all three surfaces the saturation coverage of hydrogen was measured, giving 1.2, 1.0 and 0.8 monolayer for Rh(1 1 1), the Rh(1 1 1)/V subsurface alloy and for the Rh(1 1 1)/V islands, respectively. For CO the sticking coefficients and the saturation coverages are basically the same on the Rh(1 1 1) and the alloy surfaces. There is an extrinsic precursor on the ordered CO (√3×√3) phase on the Rh(1 1 1) surface, but there is no evidence for such a precursor on the Rh(1 1 1)/V subsurface alloy. On the Rh(1 1 1)/V islands surface, the extrinsic precursor exists on the Rh(1 1 1) surface between the V islands. Apparently this precursor is only stable on the ordered CO layer on Rh(1 1 1).     

Growth of epitaxial thin Pd(1 1 1) films on Pt(1 1 1) and oxygen-terminated FeO(1 1 1) surfaces

Thin Pd films (1-10 monolayers, ML) were deposited at 35 K on a Pt(1 1 1) single crystal and on an oxygen-terminated FeO(1 1 1) monolayer supported on Pt(1 1 1). Low energy electron diffraction, Auger electron spectroscopy, and Kr and CO temperature programmed desorption techniques were used to investigate the annealing induced changes in the film surface morphology. For growth on Pt(1 1 1), the films order upon annealing to 500 K and form epitaxial Pd(1 1 1). Further annealing above 900 K results in Pd diffusion into the Pt(1 1 1) bulk and Pt-Pd alloy formation. Chemisorption of CO shows that even the first ordered monolayer of Pd on Pt(1 1 1) has adsorption properties identical to bulk Pd(1 1 1). Similar experiments conducted on FeO(1 1 1) indicate that 500 K annealing of a 10 ML thick Pd deposit also yields ordered Pd(1 1 1). In contrast, annealing of 1 and 3 ML thick Pd films did not result in formation of continuous Pd(1 1 1). We speculate that for these thinner films Pd diffuses underneath the FeO(1 1 1).     

超快光电测量技术

本文综述了近年来趔快光电测量技术的新进展，其中包括扭快光电材料的特性、高速光电器件的基本原理，着重介绍了若干主要的用快光电测量技术．     

Some interruption criteria for short high-frequency vacuum arcs

If the contacts of a vacuum interrupter open shortly before a current zero, the transient recovery voltage (TRV) can cause a reignition and reestablish the arc. When the current in a diffuse vacuum arc passes through zero, there is a distinct pause before the TRV builds up (approximately 40 ns for copper). During this pause the gap carries conduction current only with an ion component which depends on dI /dt, varying between 3 A for dI/dt=60 A/μs and 60 A for dI/dt=1235 A/μs. The ion current subsequently decays in tens or hundreds of nanoseconds. It can be distinguished from the displacement current at this time by varying dV/dt, keeping the other parameters constant. Among the interruption criteria for short high-frequency vacuum arcs, dI /dt prior to current zero and initial dV/dt are the most important. High values of dI/dt are more likely to precipitate reignitions, but breakdowns can occur after lower dI/dt's if the gap has been subjected to a high current for a relatively long time (>100 μs)     

Mass and lattice effects in trapping: Ar, Kr, and Xe on Pt(1 1 1), Pd(1 1 1), and Ni(1 1 1)

The trapping probabilities of argon, krypton, and xenon on Pd(1 1 1) and Ni(1 1 1) have been investigated using supersonic molecular beam techniques. The trapping probability of argon exhibits normal incident energy in a similar fashion on both Pd(1 1 1) and Pt(1 1 1) because the mass of argon is significantly less than the surface mass of either Pd or Pt. In contrast, dynamic corrugation in the gas-surface potential is observed for krypton trapping on Pt(1 1 1) and Pd(1 1 1), resulting in a decreased angular dependence of the trapping probability compared to argon. For xenon trapping on Pd significant lattice deformation during the gas-surface collision appears to give rise to total energy scaling. The trapping probability of xenon on Pd(1 1 1) remains high at unusually high incident kinetic energies due to the overall enhanced energy transfer from the incident atom to the lattice. Trapping probabilities of Ar, Kr, and Xe are significantly lower on Ni(1 1 1) than on either Pt(1 1 1) or Pd(1 1 1) despite the lower surface mass of the Ni atoms. This result is attributed to the lower binding energy of the rare gases on Ni(1 1 1) and the higher Debye temperature of Ni. The energy scaling of Ar trapping on Ni(1 1 1) is determined by static corrugation, but the energy scaling for Kr and Xe on Ni(1 1 1) may involve the effects of dynamic corrugation. In the latter cases, the greater stiffness of the nickel lattice decreases the dynamic corrugation relative to Pt(1 1 1) and Pd(1 1 1).     

稀土氟碳酸盐矿物的拉曼光谱研究

研究了氟碳钡铈矿Ｃｅ２Ｂａ［ＣＯ３］３Ｆ２、氟碳钙铈矿Ｃｅ２Ｃａ［ＣＯ３］３Ｆ２和氟碳铈矿Ｃｅ［ＣＯ３］２Ｆ等矿物的拉曼光谱特征。结果表明,钡稀土氟碳酸盐矿物（氟碳钡铈矿、氟碳铈钡矿、黄河矿）的Ｒａｍａｎ光谱特点是,ν１和ν２为单峰值,ν３和ν４为双峰值。钙稀土氟碳酸盐矿物（氟碳钙铈矿）的拉曼光谱带中ν１和ν４为双峰值,ν２和ν３为单峰值。稀土氟碳酸盐矿物（氟碳铈矿）的Ｒａｍａｎ光谱的特点是,ν１、ν２和ν４为单峰值,ν３为双峰值。     

不同晶体取向下纳米压痕的多尺度模拟

采用准连续介质多尺度方法模拟面心立方金属铝单晶薄膜的纳米压痕变形过程.对薄膜分别采用三种不同的晶体取向(分别为x［1 1 1］,y［1 1 0］,z［1 1 2］; x［1 1 2］,y［1 1 1］,z［1 1 0］;x［1 1 0］,y［0 0 1］,x［1 1 0］),得到载荷-位移响应曲线.加载过程中,对晶体内部变形比较剧烈的部分画出原子图,并从微观角度分析产生剧烈变形的原 关键词： 纳米压痕 准连续介质方法 晶体取向 位错成核     

傅里叶红外光谱研究血清白蛋白构象

用傅里叶红外光谱法研究了ＢＳＡ及其水溶液的红外光谱。通过对其酰胺Ｉ带傅里叶自转积谱分析,为其及部分水溶液中的二级结构构象进行了指认。结果表明,ＢＳＡ水溶液状态与固态时的二级结构是不同的。随着溶液浓度的降低,酰胺Ｉ带二级结构峰存在明显的位移现象,即１６０９．８６ｃｍ＾－１位移到１６０８．２４ｃｍ＾－１,１６３３．８５位移到１６３８．３６ｃｍ＾－１,１６５３．６９ｃｍ＾－１位移到１６５６．１０ｃｍ＾－     

Recombination lasing in heliumlike silicon: a possible path to thewater window

A major goal of current X-ray laser research is the achievement of gain in the 23.3-43.7 Å wavelength region, known as the `water window'. Silicon is the lowest atomic number element for which all the heliumlike 3-2 transitions lie in this region. The authors examine the fundamental kinetics of recombination lasing in this species, and conclude that the Si XIII 1s3d¹D ₂-1s2p¹P₁ line at 39.1 Å is an attractive candidate for recombination-pumped lasing. Attainment of gain in this line is somewhat more energetically favorable than for the hydrogenic Al XIII 3-2 transitions, but radiative trapping may be somewhat more troublesome than for H-like Al     

胆囊癌的傅里叶变换红外光谱研究

运用衰减全反射(attenuated total reflection,ATR)探头与傅里叶变换红外(Fourier transform infra-red,FTIR)光谱仪,测定并分析了新鲜离体的胆囊癌组织18例和良性组织139例的FTIR光谱。结果表明:(1)胆囊癌的1 167和1 123 cm-1谱带的峰位显著地向低波数移动(P0.05),而1 309 cm-1谱带的峰位显著地向高波数移动(P0.05)。(2)胆囊癌组织光谱多个峰的相对强度I2 856/I1 461,I1 167/I1 461,I1 123/I1 461和I1 082/I1 461明显升高(P0.05)。(3)1 167和1 082 cm-1谱带的半高宽显著升高(P0.05),谱带1 461 cm-1的半高宽则显著降低(P0.05)。(4)癌组织1 750 cm-1谱带的出现几率明显增加(P0.05)。与胆囊良性组织相比较,癌组织光谱中与脂类、糖和核酸相关的谱带均发生了明显的变化。     

In situ STM study of nanosized Ru and Os islands spontaneously deposited on Pt(1 1 1) and Au(1 1 1) electrodes

We provide an overview of structure and reactivity of selected bimetallic single crystal electrodes obtained by the method of spontaneous deposition. The surfaces that are described and compared are the following: Au(1 1 1)/Ru, Pt(1 1 1)/Ru and Pt(1 1 1)/Os. Detailed morphological information is presented and the significance of this work in current and further study of nanoisland covered surfaces in the catalytic and spectroscopic perspective is highlighted. All surfaces were investigated by in situ STM and by electroanalytical techniques. The results confirm our previous data that nanosized Ru islands are formed with specific and distinctive structural features, and that the Ru growth pattern is different for Au(1 1 1) and Pt(1 1 1). For Au(1 1 1), Ru is preferentially deposited on steps, while a random and relatively sparse distribution of Ru islands is observed on terraces. In contrast, for Ru deposited on Pt(1 1 1), a homogeneous deposition over all the Pt(1 1 1) surface was found. Os is also deposited homogeneously, and at a much higher rate than Ru, and even within a single deposition it forms a large proportion of multilayer islands. On Au(1 1 1), the Ru islands on both steps and terraces reach the saturation coverage within a short deposition time, and the Ru islands grow to multilayer heights and assume hexagonal shapes. On Pt(1 1 1), the Ru saturation coverage is reached relatively fast, but when a single deposition is applied, Ru nanoislands of mainly monoatomic height are formed, with the Ru coverage not exceeding 0.2 ML. For Ru deposits on Pt(1 1 1), we demonstrate that larger and multilayer islands obtained in two consecutive depositions can be reduced in size--both in height and width--by oxidizing the Ru islands and then by reducing them back to a metallic state. A clear increase in the Ru island dispersion is then obtained. However, methanol oxidation chronoamperometry shows that the surface with such a higher dispersion is less active to methanol oxidation than the initial surface. A preliminary interpretation of this effect is provided. Finally, we studied CO stripping reaction on Pt(1 1 1)/Ru, Au(1 1 1)/Ru and on Pt(1 1 1)/Os. We relate CO oxidation differences observed between Pt(1 1 1)/Ru and Pt(1 1 1)/Os to the difference in the oxophilicity of the two admetals. In turn, the difference in the CO stripping reaction on Pt(1 1 1)/Ru and Au(1 1 1)/Ru with respect to the Ru islands is linked to the effect of the substrate on the bond strength and/or adlayer structure of CO and OH_ads species.     

Structural, electronic properties and stability of the (1 × 1) PbTiO3 (1 1 1) polar surfaces by first-principles calculations

Under GGA, the structural, electronic properties and stabilities of four different (1 × 1) terminations of cubic PbTiO₃ (1 1 1) surface, the directly cleaved (1 1 1)-Ti and (1 1 1)-PbO₃ terminations and the constructed (1 1 1)-TiO and (1 1 1)-PbO₂ ones, have been systematically studied by using projector-augmented wave method implemented in VASP. For (1 1 1)-Ti and (1 1 1)-PbO₃ terminations, Ti-O bonds between the outermost two layers are enhanced after relaxation, while those between the second and the third layers are weakened. In addition, a contraction of O-O distance in surface PbO₃ layer is also found for (1 1 1)-PbO₃ termination. Moreover, electronic structures of both (1 1 1)-Ti and (1 1 1)-PbO₂ terminations are significantly influenced by structure relaxations, and the effects of the surface on the DOS are dominantly on the Ti layers, especially the CB. For a constructed (1 1 1)-TiO termination, the relaxation results show both Ti-O bonds between the outermost two layers and those between the second PbO₃ layer and the third Ti layers are enhanced. For a constructed (1 1 1)-PbO₂ termination, Ti-O bonds between the outermost two layers are also enhanced as in the (1 1 1)-TiO termination, however, inequivalent Ti-O bonds between the second layer Ti atom and the third layer O atoms are found, with two bonds expanding and the other one contracting. Results of electronic structure calculations show these two constructed terminations are all insulating and changes of DOS originate dominantly from modifications of surface compositions. Furthermore, it is found that for all four different (1 1 1) terminations, the movements of the cation and/or anion on the outermost layer along the surface normal direction after relaxation all result in a reduction of the space electric field. In O and Pb external environments, it is predicted that (1 1 1)-PbO₂ termination is the most stable one in O- and Pb-rich environments, however, the (1 1 1)-Ti termination is stable one in O- and Pb-poor conditions. The (1 1 1)-TiO termination also shows a stability domain in moderate O and Pb environments.     

八角茴香与其伪品莽草的红外光谱三级鉴定研究

采用红外光谱三级鉴定的方法区分和鉴别了八角茴香及其伪品莽草。红外光谱三级鉴定即依次采用一维红外光谱、二阶导数谱和二维相关红外光谱,分辨率逐渐提高,谱图的差别也进一步放大。一维谱图中,两者整体峰形比较相似,但在3 400 cm-1附近八角茴香只出现一个特征峰3 392 cm-1,而莽草则出现3 482和3 387 cm-1两个特征峰。二阶导数谱在850～1 180 cm-1波段八角茴香的几个强峰峰强相对比较接近,其中1 015 cm-1为图中最强峰,而莽草的最强峰在1 070 cm-1附近;在1 180～1 500 cm-1波段八角茴香在1 469,1 454,1 442 cm-1附近的３个特征峰峰强明显强于1 292,1 276,1 266 cm-1附近的特征峰,而莽草则刚好相反。二维相关红外光谱中差异更明显,850～1 165 cm-1波段八角茴香在主对角线上的自动峰较强峰出现在1 153和1 000 cm-1,而莽草峰强较强的自动峰出现在911和878 cm-1;1 165～1 500 cm-1波段八角茴香呈现2个自动峰,而莽草则出现5个自动峰。可见红外三级鉴定方法是一种快速有效的鉴定中药材的方法。     

核磁共振氢谱方法对红外光谱碳氟键伸缩振动变化的研究

采用傅里叶转换红外光谱方法测定了三种1,2-二-[β-(α-甲基-α'对位取代基苯基)噻吩]六氟环戊烯化合物Ⅰ、Ⅱ、Ⅲ的红外光谱.在确认主要红外吸收峰归属并对图谱进行解析的基础上观测到环戊烯环上的碳氟键吸收频率依化合物Ⅰ,Ⅱ,Ⅲ次序逐一相应增高,发生规律性变化.化合物Ⅰ:vas C-F=1 332.21cm-1,vs C-F=1 231.91 cm-1,δ C-F=1 159.99 cm-1;化合物Ⅱ:vas C-F=1 338.18 cm1,vs C-F=1 254.31cm-1,δ C-F=1 179.22 cm-1;化合物Ⅲ:vas C-F=1 360.99 cm-1,vs C-F=1 263.29 cm-1,δ C-F=1 194.00cm-1.对此不仅从红外光谱吸收原理进行了定性讨论,而且采用核磁共振谱测定化合物氢谱的方法给出了定量描述:化合物Ⅰ,Ⅱ,Ⅲ的H-1,H-2化学位移δ值,均为Ⅰ＞Ⅱ＞Ⅲ,反映出取代基引起苯环质子周围的电子云密度增加.因此可确认红外吸收的诱导效应与共轭效应共同作用是导致化合物环戊烯环上的碳氟键伸缩振动频率发生规律性变化的原因.这说明核磁共振氢谱是红外光谱解析的有力工具.     

三大产地（波罗的海、多米尼加和缅甸）琥珀红外光谱鉴别特征

采用镜面反射法和溴化钾压片透射法对波罗的海、多米尼加和缅甸琥珀进行红外光谱测试,获得了不同产地的红外光谱鉴别特征。经仔细分析认为,尽管不同产地琥珀的红外光谱具有共同特征,但某些吸收峰位置或相对强度仍存在差异。3 000～2 800 cm-1范围内,波罗的海琥珀有两个明显的吸收峰和一个弱肩峰,多米尼加琥珀有两个吸收峰,缅甸琥珀具有三个特征吸收峰;1 740～1 690 cm-1范围内,波罗的海琥珀出现1 732 cm-1附近强吸收峰,多尼米加和缅甸琥珀有两个吸收峰,分别位于1 730和1 695 cm-1附近,但是多米尼加琥珀1 730 cm-1峰强度小于1 695 cm-1,与缅甸琥珀相反;1 300～1 000 cm-1范围内,波罗的海琥珀具有典型的“波罗的海肩峰”及1 163 cm-1附近的强吸收,多米尼加琥珀出现1 240 cm-1附近吸收峰,缅甸琥珀在此范围内的强吸收峰组成“山”字型;波罗的海琥珀R（A_{1 381 cm-1}/A_{1 456 cm-1}）值约为0.9,多米尼加琥珀约0.8,而缅甸为0.7。上述差异可以作为判断琥珀产地的鉴别依据。不同产地琥珀的红外光谱出现差异,可能与其形成年代、植物种源和地质环境不同有关。根据红外光谱中与环外C=C双键有关的吸收峰的存在和强度,推断三个产地的琥珀形成时间由早到晚分别为缅甸、波罗的海、多米尼加。红外光谱在识别琥珀产地方面具有重要的宝石学意义,同时在考古学研究与应用中有潜在意义。