类镓等电子序列ZrX—RhXV离子的4s^24p—4s^24d,4s^24p—4s4p^2,4s^24 …

本文对类镓等电子序列ＧａＩ－ＸｅＸＸＩＶ离子４ｓ＾２４ｐ、４ｓ＾２４ｐ、４ｓ＾２４ｄ、４ｓ４ｐ＾２、４ｐ＾３和４ｓ＾２５ｓ组态组级结果和组态相互作用了理论分析，找出沿等电子序列的变化规律。     

Rh XⅢ—Cd XVI离子4s24p3—4s4p4能级与跃迁的理论计算

用HFR（Hartree-Fock with relativistic corrections）方法对Rb V—Cd XVI离子4s²4p³和4s4p⁴组态能级结构做了全面系统的理论计算研究. 通过分析能级结构参数的HFR理论计算值与基于实验能级拟合得到的计算值之比值随着原子序数Z_c变化的规律,运用广义拟合外推方法预言了这些离子能级结构参数. 由此进一步计算了Rh XⅢ,Pd XIV,Ag XV和Cd XVI离子4s²4p³（⁴S_3/2,²P_1/2,3/2,²D_3/2,5/2）和4s4p⁴（⁴P_1/2,3/2,5/2,²P_1/2,3/2,²D_3/2,5/2,²S_1/2）组态能级以及电偶极跃迁波长与振子强度. 研究表明,对于4s²4p³组态,单组态近似可以得到较满意的结果;而对于4s4p⁴组态,只有在考虑了4s²4p²4d的组态相互作用效应时,计算结果的准确性才能明显得到提高. 同时,本文还运用全相对论grasp2K-DEV程序包计算了Rh XⅢ—Cd XVI离子组态能级. 对于Rh XⅢ离子4s²4p³（²P_1/2）,Pd XIV离子4s²4p³（⁴S_3/2,²P_1/2,3/2,²D_3/2,5/2）和4s4p⁴（²P_1/2,3/2,²D_3/2,5/2,²S_1/2）,能级均无实验值;对于Ag XV和Cd XVI离子,截至目前还没实验能级数据,没有实验能级值的所有数据均仅来自本文的计算数值. 本文计算结果与已有实验值吻合得很好.     

New energy levels and transitions for the 4s4p5p configuration in Kr VI

The spectrum of five-time ionized krypton, Kr VI, was recorded in the 240-2600 Å wavelength range, resulting in 61 new classified lines as transitions between levels of configurations 4p³, 4s²5p, 4s4p4d, 4s4p5s and 4s4p5p. All the 18 energy levels belonging to 4s4p5p configuration except one were determined. Eight new energy level values corresponding to configurations 4s4p4f and 4p24d, supported by 26 new classified lines were also determined and used in the interpretation of the observed 4s4p5p configuration. The experimental data were obtained from a capillary-discharge tube and theta pinch light sources. Multiconfiguration Hartree-Fock calculations with relativistic corrections and a least-squares fitted parametric calculation has been carried out.     

光诱导雄黄矿物同质异象变化的显微成像拉曼散射研究

利用拉曼光谱研究了激光照射诱导雄黄的同质异象变化,这些结果证实了下面的反应：由于As—As键相对较弱,首先As—As键被破坏,有1个S原子加入到As—As键中,形成As—S—As键。此时由As₄S₄(Realgar类型)变化为As₄S₅相,而As₄S₅处于不稳定状态,As₄S₅相变化为 Pararealgar时有1个S原子从As—S—As键中释放出来。释放出来的S原子又加入到另外1个As₄S₄(Realgar)中,引起As₄S₄(Realgar)相变化为As₄S₅,As₄S₅进而分裂为1个S原子和As₄S₄(Pararealgar类型)。照射促进雄黄经由 As₄S₅ 分子被转换成副雄黄。     

The 4s~24p~3—4s4p~4 transition in Cd ⅩⅥ

The available experimental energies for the 4s~24p~3 and 4s~4p~4 configurations in As Ⅰ—like Sr Ⅵ—Ag Ⅹ Ⅴions are compared with the values calculated using the Hartree—Fock method including configuration interaction and relativistic corrections. Some energy values of the 4s~24p~3 configuration in Rh Ⅹ Ⅲ、Pd Ⅹ Ⅳ and Ag Ⅹ Ⅴ ions are improved and all the energies、wavelengths and transition probabilities of the 4s~24p~3—4s4p~4 transition array in Cd Ⅹ Ⅵ are presented.     

Esters of 4-nitrocinnamic acids and 4-halogene-4’-hydroxyazobenzenes – synthesis,mesogenic and optical studies

Six new compounds were synthesized that have no alkyl chains in their structure: 4-nitrocinnonates of 4-hydroxyazobenzene, 4-nitro-4’-hydroxyazobenzene, 4-fluoro-4’-hydroxyazobenzene, 4-chloro-4’-hydroxyazobenzene, 4-bromo-4’-hydroxyazobenzene and 4-iodo-4’-hydroxyazobenzene. Using the polarizing microscopy and differential scanning calorimetry, enthalpies and temperatures of phase transitions were determined. All investigated compounds have an enantiotropic nematic phase. These compounds proved to be extremely thermally stable. Thermal decomposition was observed in temperatures above 300°C. Investigated compounds contain two different chromophore groups (i.e. azo and ethene moieties), which influenced the complex trans–cis isomerization processes of both groups (three time-separated processes were observed). It was shown that the presence of the ethene group significantly shifts the π-π* band towards higher energies. The substituent polarity in the azo group also affected the energy of this absorption band. A weak luminescence effect was observed in the 4-nitrocinnonates of 4-hydroxyazobenzene compound.     

KrVI离子能级和振子强度的理论计算

利用组态相互作用理论和参数外推法,计算了KrVI离子4s~24p—4s4p~2、4s~24p—4s~24d和4s4p~2—4p~3跃迁的能级、谱线波长和振子强度。与已有实验结果比较表明:波长的理论计算值与观测值在0.7A内很好符合,振子强度的理论计算值较大的跃迁均是实验中观测到的跃迁。     

掺Co钨酸镉单晶体的坩埚下降生长及光谱特性

应用坩埚下降法,采用70℃.cm-1的固液界面温度梯度与0.50 mm.h-1生长速度,生长出了初始Co掺杂摩尔百分浓度为0.5 mol%、尺寸为Ф25 mm×120 mm的钨酸镉单晶体。晶体呈透明深蓝色。用XRD表征了获得的晶体。观测到518,564和655 nm三个可见波段吸收带以及发光中心1 863 nm(1 323～2 220 nm)的超宽吸收带。可见波段的吸收归属于Co2+在八面晶格场中4T1(4F)→4A2(4F),4T1(4F)→4T1(4P)跃迁叠加,而红外波段的宽带吸收则为八面体场Co2+的4T1(4F)→4T2(4F)能级跃起所致。从吸收特性表明,Co离子掺杂于畸变的氧八面体中,呈现+2价态。根据吸收光谱计算出晶格场参数Dq=990 cm-1,Racah参数BC=726.3 cm-1。在520 nm波长光的激发下,观察到778 nm波段的荧光发射,归属于八面体晶格场中Co2+的4T1(4P)→4T1(4F)能级的跃迁。从吸收与荧光强度的变化推断:沿着晶体生长方向,Co2+浓度逐渐增加,有效分凝系数小于1。     

Pitch Characteristics of Homosexual Males

Objective

To investigate the common stereotype that homosexual males show pitch patterns that mirror those of heterosexual females.

Study Design

Static group comparison.

Method

Comparison of speaking fundamental frequency and pitch variation of 30 homosexual males, 56 heterosexual age-matched males, and 54 age-matched heterosexual females as demonstrated in a sample of read speech.

Results

In the homosexual males, average fundamental frequency and pitch variation were significantly higher than in the heterosexual males but also significantly lower than in the heterosexual females.

Conclusions

Results do not confirm the stereotype that gay male speech mirrors the patterns of women’s speech with respect to pitch characteristics. It would seem that the pitch patterns of gay male speakers constitute an example of sociophonetic variation.     

Effects of ultrasound on the formation of alpha-benzoylbenzyl cyanide from benzyl cyanide and alkylphenyl ketone from alpha-alkylbenzyl cyanide by potassium superoxide in the presence of crown ether

Ultrasound accelerates the formation of alpha-benzoylbenzyl cyanide and benzoic acid in the reaction of benzyl cyanide with potassium superoxide in the presence of 18-crown-6. Similarly, 4-methylbenzyl cyanide, 4-methoxybenzyl cyanide and 4-chlorobenzyl cyanide gave the corresponding alpha-(4-methylbenzoyl)-4-methylbenzyl cyanide, alpha-(4-methoxybenzoyl)-4-methoxybenzyl cyanide and alpha-(4-chlorobenzoyl)-4-chlorobenzyl cyanide in 25-43% isolated yields under the same reaction conditions. Benzoic, p-toluic, 4-methoxybenzoic and 4-chlorobenzoic acids were also formed in these reactions. No reaction was observed when the mixture was simply stirred. Reflux instead of sonication gave lower yields of the products. However, alpha-alkylbenzyl cyanide produced a high yield of the phenylalkyl ketones when stirred. Interestingly, the corresponding benzoic acid was not formed in these reactions. Possible mechanisms for the formation of alpha-benzoylbenzyl cyanide from benzyl cyanide and phenylalkyl ketones from alpha-alkylbenzyl cyanide are also proposed.     

The Odd SO(3,3) Fusions and the Gauge Principle

The origin of the gauge principle generating electroweak and gravistrong interactions is shown to lie already in the quaternionic vacuum. The leptonic Dirac equations gauged in respect of the electroweak and the linearized gravistrong field are derived from the SO(3,3) fusion 6 × 4 = 20 + 4 as a part of 4 × 4 × 4 . The procedure leading to respective equations including self-interactions and gauge coupling to the full nonlinear gravistrong field via 20 ″ × 4 = 60 + 20 as a part of 4 × 4 × 4 × 4 × 4 is outlined.     

Effect of the final-state interaction on the initial core–hole lifetime: the case of the 4s-hole lifetime of Sn metal

The first theoretical study of the effect of the final-state interaction on the initial core–hole lifetime is presented. The 4s-hole lifetime width of Sn metal is calculated by an ab-initio atomic many-body theory (Green’s function method). When the final-state interaction in the 4p4d two-hole state, created by the 4s⁻¹−4p⁻¹4d⁻¹ f super Coster–Kronig (CK) transition of the initial 4s hole, is explicitly taken into account, the ab-initio atomic many-body calculation of the 4s-hole X-ray photoelectron spectroscopy (XPS) spectrum of Sn atom can provide excellent agreement with experiment in both the 4s-hole energy and the 4s-hole lifetime width. Otherwise, the many-body calculation underestimates considerably the 4s-hole lifetime width. The 4p4d two-hole state interacts strongly with the 4d triple-hole state by the 4p⁻¹4d⁻¹−4d⁻³ f super CK transition. The interaction affects greatly the initial 4s-hole lifetime width.     

RuXIV离子能级和振子强度的理论计算

利用组态相互作用理论和参数外推方法,计算RuXIV离子4s²4p,4s4p² 4s²4d和4p³组态的能级,以及4s²4p—4s4p²,4s²4p—4s²4d和4s4p²—4p³跃迁的谱线波长和振子强度。4s²4p和4s4p²组态的能级与已有实验 关键词：     

PdⅩⅣ-CdⅩⅥ离子4s24p3和4s4p4组态精细结构能级与跃迁的扩展分析

用多组态HXR理论方法对KrⅣ-CdⅩⅥ离子4s^24p^3和4s4p^4组态的精细结构能级进行了分析计算。在已有研究工作的基础上,通过对4s^24p^3和4s4p^4组态能级的实验观测值与HXR计算结果之差AE沿等电子序列变化规律的分析．找出了△E随有效核电荷数Zc变化的规律,预言并计算了PdⅩⅣ-CdⅩⅥ离子4s^24p^3和4s4p^4组态能级,大部分预言计算值与实验结果的偏差小于100cm^-2。由此还进一步计算了PdⅩⅣ-CdⅩⅥ离子4s^24p^3—4s4p^4跃迁的谱线波长、振子强度和跃迁概率。结果表明：除了4s^24p^3D5/2-4s4p^4^2D5/2跃迁的谱线波长(29．992nm)与实验值相差0．018nm外．对于其余5条谱线．预言值与实验值的偏差均不超过0．005nm。     

高压下NH_4ClO_4结构、电子及弹性性质的第一性原理研究

研究高压下NH_4ClO_4的结构和性质对于NH_4ClO_4在固体推进剂和炸药的安全应用具有重要意义.采用基于色散校正密度泛函理论的第一性原理方法,研究了0—15 GPa静水压力下NH_4ClO_4的晶体结构、分子结构、电子性质和弹性性质,计算结果与实验值具有较好的一致性.在压强为1,4和9 GPa时,NH_4ClO_4的晶体参数、键长和分子构型等均出现不连续变化,说明了在压强作用下结构发生变化.随着压强增加,氢键增多且作用增强,由分子内氢键向分子内和分子间的氢键转变;导带态密度峰值增加,电子局域性增强,晶体内N-H和Cl-O共价键作用增强,带隙增大,不同相变区域内带隙呈线性关系.0—15 GPa条件下NH_4ClO_4的弹性常数满足力学稳定性标准,采用Voigt-Reuss-Hill方法计算了体积模量B,剪切模量G和杨氏模量E,根据Cauchy压力和B/G值,说明NH_4ClO_4属于韧性材料,随着压强增加韧性增强.     

若干钠锗酸盐晶体和熔体的温致结构变化及其锗配位数的拉曼光谱研究

本文测定了Na4GeO4、Na2GeO3、Na2Ge4O9和Na4Ge9O20等晶体从273K到1413K升温及熔体的拉曼光谱,结合分析金红石型GeO2的相关结构和光谱,研究了其微结构单元在升温过程中的变化、熔体中的形态和锗的氧配位数及其温致变化。Na4GeO4和Na2GeO3晶体结构单元为GeO4四面体,在升温过程及其熔体中锗维持四配位。Na2Ge4O9和Na4Ge9O20晶体结构单元为GeO4四面体和GeO6八面体共存,升温过程中,GeO6八面体将发生结构转变,在熔融状态全部转变为GeO4四面体,并产生与钠离子等摩尔分数的非桥氧,在熔体中锗的氧配位数为4。研究还表明,桥氧的对称弯曲振动模可以反映不同微结构单元间的连接,并且随着温致结构的变化而产生特征性的变化。     

GF-AAS法测定处理污水灌溉土壤中铅最佳基体改进剂的选择及其应用

研究了石墨炉原子吸收法（GF-AAS法）测定一级处理污水灌溉土壤中铅最佳基体改进剂的选择及在最佳改进剂条件下测定污水灌溉土壤中铅的GF-AAS法。试验了磷酸二氢铵, 磷酸铵, 氯化铵, Pd-Mg和磷酸二氢铵+硝酸镁+硝酸铵等基体改进剂对测定一级处理污水灌溉土壤铅的基体改进作用,并根据基体改进剂的改进效果,最佳灰化温度和原子化温度, 选定了最佳基体改进剂和测定条件。40 g·L-1的磷酸二氢铵作为基体改进剂,灰化温度为850 ℃,原子化温度为1 600 ℃时,用氘灯校正背景GF-AAS法进行测定,测定方法的RSD为2.6% ,回收率在92.4%～104%之内。     

InSb的Li嵌入电压轮廓曲线从头计算

InSb是很有应用前途的Li离子电池非碳类负极材料. 使用基于密 度泛函理论的第一原理赝势法，计算了InSb 在Li嵌入时的125种不同情况下的总能、形成能 以及平衡体积等，进而参考电压轮廓实验曲线，筛选出了若干条理论上可能的反应路径，得到了Li嵌入时的电压轮廓曲线. 结果表明，从体InSb相到Li＿3Sb相之间没有中间经历五个相及五个相以上的反应路径；中间经历一个相的最可能反应过程为Li+In＿4Sb＿4→Li＿1In＿4Sb＿4,11Li+Li＿1In＿4Sb＿4→Li＿12Sb＿4+4In；中间经 历四个相的仅有一条反应路径：Li+In＿4Sb＿4→Li＿1In＿4Sb＿4,2Li+Li＿1In＿4Sb＿4→ Li＿3In＿4Sb＿4,4Li+Li＿3In＿4Sb＿4→Li＿7In＿3Sb＿4+In,3Li+Li＿7In＿3Sb＿4→Li＿10In＿2Sb＿4+In,2Li+Li＿10In＿2Sb＿4→Li＿12Sb＿4+2In. 关键词： InSb Li嵌入 电压轮廓曲线 从头计算     

基质发光材料Na5Eu(MoO4)4和NaEu(MoO4)2的制备和发光

本文研究了化学计量的基质发光材料Na5Eu(MoO4)4和NaEu(MoO4)2.它们都属于四方晶系,空间群为I41/α .NaEu(Mo04)2属于白钨矿(scheelite)结构,一个晶胞中有2个分子式NaEu(MoO4)2(z=2);而Na5Eu(Mo4O)4属于类自钨矿(scheelite-like)结构,一个晶胞中有4个分子式Na5Eu(MoO4)4(z=4).X射线衍射确定的晶胞常数,对Na5Eu(MoO4)4,α=1.1439nm和c=1.1486nm(密度d计算=4.01g/cm3,z=4);对NaEu(MoO4)2,α=0.5236nm和c=1.1439nm(密度d计算=5.24g/cm3,z=2).由差热法和X射线衍射法确定了Na2MoO4-Eu2(MoO4)3的相图.Na5Eu(MoO4)4分解为NaEu(MoO4)2的温度是700℃.本文确定了制备纯 Na5Eu(MoO4)和NaEu(MoO4)2的方法,并研究了上述两种材料的激发光谱和发光光谱.确定了用X射线粉末衍射谱和发光光谱鉴别Na5Eu(MoO4)4和NaEu(MoO4)2的方法.在365nm紫外光激发下,Na5Eu(MoO4)4的发光比Na5Eu(WO4)4的强得多,在室温下,Na5Eu(MoO4)4,NaEu(MoO4)2和Na5Eu(WO4)4的相对发光积分亮度比为3.8:3.2:1.0.     

1—(4—吡啶甲酰)—4—芳基氨基硫脲类和3—(4—吡啶基)—4—芳基—1,2,4—三唑啉—5—硫酮类化合物~(13)C—NMR谱研究

本文测定了新合成的,具有生理活性的1-(4-吡啶甲酰)-4 -苯基氨基硫脲,1-(4-吡啶甲酰)-4-对氯苯基氨基硫脲,1-(4 -吡啶甲酰)-4-对溴苯基氨基硫脲3-(4-吡啶基)-4-苯基-1,2,4,-三唑啉-5-硫酮,3-(4-吡啶基)-4-对氯苯基-1,2,4,-三唑啉-5-硫酮,3-(4-吡啶基)-4-对溴苯基-1,2,4-三唑啉-5-硫酮六个新化合物的~(13)C-NMR谱,并通过~(13)C-NMR谱中的宽带去偶,偏共振及APT技术,模型化合物对照,讯号强度对比及芳基取代基常数计算等方法,进行了上述化合物~(13)C-NMR谱峰的归属,并得到了甲酰肼基在吡啶环4位取代后对吡啶环各碳所产生的取代基效应.