Quasi‐Periodic Solutions of Nonlinear Evolution Equations Associated with a 3 × 3 Matrix Spectral Problem

A hierarchy of new nonlinear evolution equations associated with a 3 × 3 matrix spectral problem with three potentials is proposed. With the aid of the characteristic polynomial of Lax matrix for the hierarchy, we introduce an algebraic curve of arithmetic genus m ? 1 , and discuss in detail the properties of the associated Baker–Akhiezer function and meromorphic function. On the basis of the theory of algebraic curves, we obtain the explicit theta function representations of the Baker–Akhiezer function, the meromorphic function, and, in particular, that of solutions for the entire hierarchy of nonlinear evolution equations.     

An efficient combination of supercritical fluid extraction and high-speed counter-current chromatography to extract and purify (E)- and (Z)-diastereomers of α-asarone and β-asarone from Acorus tatarinowii Schott

In this study, supercritical fluid extraction (SFE) was used to extract essential oil from Acorus tatarinowii Schott under the pressure of 25 MPa and temperature of 35°C. Two (E)- and (Z)-diastereomers of α-asarone and β-asarone were separated and purified by high-speed counter-current chromatography (HSCCC) with a two-phase solvent system composed of n-hexane-ethyl acetate-methanol-water (1:0.2:1:0.3, v/v). The separation yielded a total of 39 mg of α-asarone and 463 mg of β-asarone from 1.0 g of essential oil in one-step separation with the purity of 98.9 and 99.1%, respectively, as determined by HPLC. The chemical structures of these compounds were identified by EI-MS, (1)H-, and (13)C-NMR.     

高功率TEA CO2激光器两波长激光切换输出技术

 以TEA CO₂激光器通常采用的平-凹光学稳定腔为基础,提出了一种新的波长选支方法——输出窗口镀膜选支方法。利用一台高平均功率TEA CO₂激光器进行了选支实验研究,结合现有光学镀膜技术,得到了中心波长为9.3 μm的激光单谱线输出,其单脉冲能量及平均功率与激光器原中心波长10.6 μm单谱线输出的相应参数基本相当。研究发现,以相同单脉冲能量激光照射热敏纸时,中心波长9.3 μm激光光斑与中心波长10.6 μm的明显不同。同时,还设计出两波长窗口密闭免调切换装置,在一台激光器上实现了10.6,9.3 μm两个中心波长激光同等功率水平的免调切换输出,切换位置误差小于5″,密封性能满足使用要求。     

氧碘化学激光器直线分段扩开型扩压器实验研究

 研究了不同几何外形参数对直线分段扩开型氧碘化学激光器(COIL)扩压器性能的影响,实验结果表明：光腔上下壁扩开全角8°时,选取4°超扩段扩散角可获得较好的压力恢复和隔离光腔流场的能力;超扩段增加2 mm竖隔板可降低光腔后部壁面静压,且截止反压提高约12%;在相同腔压下,10°截角唇口的截止反压比直角唇口和1/4圆弧唇口截止反压高出约7.6%;超扩段入口四壁增加人工粗糙带能明显改善光腔壁面静压的分布,并有效提高扩压器效率。     

基于弹光调制的红外光谱吸收法在室内VOC检测中的研究

为了保证静态干涉系统在气体定性定最分析方面稳定性高、抗干扰能力强的特点,设计了基于弹光调制实现光程静态扫描的干涉检测系统.系统由红外激光器、起偏器、弹光调制器、检偏器及CCD组成.通过弹光调制器使弹光晶体的主折射率随调制信号周期性的变化,从而产生周期性变化的光程差.通过对调制相位变化的计算,可知得到调制度随晶体长度、调...     

H2 气对脉冲磁控溅射铝掺杂氧化锌薄膜性能的影响

实验采用脉冲磁控溅射法制备铝掺杂氧化锌(AZO)薄膜.为了进一步提高AZO薄膜的光电性能,在溅射过程中加入一定流量的氢气,以高纯ZnO ∶Al₂O₃陶瓷靶为溅射靶材,制备AZO/H透明导电薄膜.通过测试薄膜的结构特性、表面形貌及其光电性能,详细地研究了氢气流量对AZO薄膜性能的影响.溅射过程中引入氢气,可以促进薄膜的晶化,提高薄膜的迁移率和透过率(400—1100 nm).采用纯氩气溅射制备AZO薄膜的电阻率为5.664×10^-4 Ω·cm 关键词： 氧化锌 氢气流量 磁控溅射 太阳电池     

倾斜相差对光纤激光相干合成的影响与模拟校正

选取不同路数和不同填充因子的合成光束模型,模拟并分析了倾斜相差对相干合成的影响.介绍了倾斜校正的关键器件--自适应光纤光源准直器.在主振荡功率放大器结构的光纤激光相干合成系统中,模拟了随机并行梯度下降(SPGD)算法校正七路激光阵列间时变倾斜相差的动态过程,分析了不同倾斜相差幅值和频率对校正能力的影响.实验表明,要提高相干合成的效果,必须校正倾斜相差;而SPGD算法校正倾斜相差的能力随着倾斜相差幅值和频率的增加而降低.文章为在实际大气环境中实现多路高功率光纤激光的相干合成提供了参考. 关键词： 光纤激光 相干合成 倾斜相位差 动态分析     

Mechanism of Ethylene Migratory Insertion and Dimerization Catalyzed by δ‐Alkyl Platinum Complexes–A DFT Study

The mechanism of ethylene insertion reactions catalyzed by cationic δ‐alkyl platinum complexes has been studied at the B3LYP level of density functional theory. The initial steps of the reactions proceed via the coordination of ethylene to the reactants L₂Pt(II)R⁺, where L₂=none, (NH₃)₂, (CHNH)₂; R=H, CH₃, C₂H₅ in which ethylene coordinates strongly to the complexes PtCH⁺₃ and PtC₂H⁺₅ (coordination energies (CE) are 296.52 and 229.28 kJ/mol, respectively), while nitrogen‐containing ligands decrease the energies: Pt(NH₃)₂CH⁺₃ (CE: 180.04 kJ/mol), Pt(NH₃)₂C₂H⁺₅ (CE: 97.86 kJ/mol), Pt(CHNH)₂CH⁺₃ (CE : 176.31 kJ/mol) and Pt(CHNH)₂C₂H⁺₅ (CE: 91.00 kJ/mol). Moreover, ethylene insertion into the Pt‐alkyl bond, which is the rate‐determining step, is endothermic with barrier heights for L₂PtCH₃(C₂H₄)⁺ decreasing in the order: PtCH⁺₃ (164.18 kJ/mol)>(NH₃)₂ PtCH⁺₃ (129.95 kJ/mol)>(CHNH)₂ PtCH⁺₃ (115.27 kJ/mol), which has the same tendency for the ethyl case. The insertion product will continually undergo β‐hydride elimination, which is exothermic. On the other hand, the effects of solvent (dichloromethane, THF and benzene) are investigated with PCM method, but the inclusion of the effects in the computations only slightly affects the results. Beside that, a complete catalytic cycle for ethylene dimerization is studied in detail and the calculations agree well with known energetic and recognized tendencies.     

Two New Cytotoxic Naphthoquinones from Didymocarpus hedyotideus

A new naphthoquinone, 6‐hydroxy‐α‐dunnione ( 1 ) and a new binaphthoquinone, methyl 1,1′,4,4′‐tetrahydro‐3‐hydroxy‐1,1′,4,4′‐tetraoxo[2,2′‐binaphthalene]‐3′‐carboxylate ( 2 ), along with ten known compounds, including naphthoquinones, anthraquinones, and phenylethanoid glucosides, were isolated from the roots of Didymocarpus hedyotideus Chun . Their structures were identified by spectroscopic analyses, particularly 1D‐ and 2D‐NMR spectroscopy. The cytotoxic activities of the two new naphthoquinones were also evaluated.     

Neptunium thiophosphate chemistry: intermediate behavior between uranium and plutonium

Black crystals of Np(PS(4)), Np(P(2)S(6))(2), K(11)Np(7)(PS(4))(13), and Rb(11)Np(7)(PS(4))(13) have been synthesized by the reactions of Np, P(2)S(5), and S at 1173 and 973 K; Np, K(2)S, P, and S at 773 K; and Np, Rb(2)S(3), P, and S at 823 K, respectively. The structures of these compounds have been characterized by single-crystal X-ray diffraction methods. Np(PS(4)) adopts a three-dimensional structure with Np atoms coordinated to eight S atoms from four bidentate PS(4)(3-) ligands in a distorted square antiprismatic arrangement. Np(PS(4)) is isostructural to Ln(PS(4)) (Ln = La-Nd, Sm, Gd-Er). The structure of Np(P(2)S(6))(2) is constructed from three interpenetrating diamond-type frameworks with Np atoms coordinated to eight S atoms from four bidentate P(2)S(6)(2-) ligands in a distorted square antiprismatic geometry. The centrosymmetric P(2)S(6)(2-) anion comprises two PS(2) groups connected by two bridging S centers. Np(P(2)S(6))(2) is isostructural to U(P(2)S(6))(2). A(11)Np(7)(PS(4))(13) (A = K, Rb) adopts a three-dimensional channel structure built from interlocking [Np(7)(PS(4))(13)](11-)-screw helices with A cations residing in the channels. The structure of A(11)Np(7)(PS(4))(13) includes four crystallographically independent Np atoms. Three are connected to eight S atoms in bicapped trigonal prisms. The other Np atom is connected to nine S atoms in a tricapped trigonal prism. A(11)Np(7)(PS(4))(13) is isostructural to A(11)U(7)(PS(4))(13). From Np-S bond distances and charge-balance, we infer that Np is trivalent in Np(PS(4)) and tetravalent in Np(P(2)S(6))(2) and A(11)Np(7)(PS(4))(13). Np exhibits a behavior intermediate between U and Pu in its thiophosphate chemistry.