单层2H-MoTe2光电效应的理论研究

材料的禁带宽度是影响光电探测器探测范围的重要因素。单层2H-MoTe₂因具有合适的禁带宽度引起了科研人员广泛的研究兴趣。本文基于非平衡态格林函数-密度泛函理论,采用第一性原理方法,研究了单层2H-MoTe₂的光电效应。结果表明:在线性偏振光照射下,MoTe₂产生的光电流函数与唯象理论相吻合;在光子能量范围1.6~1.8 eV (690~770 nm),对应于红光,能产生较大的光电流。利用能带结构和态密度分析了产生较大光电流的原因主要来自第一布里渊区S点的电子受激跃迁。同时发现在锯齿型方向偏压为0.8 V时,光电流达到峰值;然而在扶手椅型方向偏压为0.4 V时,光电流就达到峰值。这些计算结果可用于指导基于MoTe₂光电探测器的设计,尤其是红外光电探测器的设计。     

无氧气氛中生长K2Al2B2O7晶体及其性质的研究

本文采用助熔剂法在无氧气氛的条件下成功生长出了大块透明的紫外非线性光学晶体K2Al2B2O7.这种方法有效地克服了晶体在紫外区域产生的非本征光吸收,顺磁共振谱测试表明,晶体中Fe杂质已经降低到不影响紫外透过的水平.XRD物相鉴定证明得到了K2Al2B2O7纯相,但晶体生长过程中容易形成光散射颗粒,降低了晶体的激光损伤阈值.对晶体进行化学腐蚀,采用金相显微镜观察发现有光散射颗粒的KABO晶体表面有许多腐蚀坑,而无光散射颗粒的晶体没有腐蚀坑.最后讨论了KABO晶体中光散射颗粒形成的原因以及消除的办法.     

透明SiO2-Al2O3-CaO-CaF2 微晶玻璃中Tb3+的发光性能研究

通过对1.0 mol;Tb2O3掺杂45SiO2-20Al2O3-10CaO-25CaF2玻璃进行热处理制备出透明微晶玻璃,经XRD分析微晶玻璃内析出了大小约为27 nm 的CaF2颗粒.并分别在紫外和X射线激发下研究了Tb3+在基质玻璃和透明微晶玻璃中的发光行为.结果表明:微晶玻璃中CaF2纳米晶颗粒的析出有利于提高Tb3+的发光性能,紫外激发时,Tb3+的545 nm特征发光强度增强了4倍;而X射线激发时,Tb3+的545 nm特征发光强度增加了3.5倍.     

Synthesis and X-ray Crystal Structure Analysis of CU2(CH3CH2COO)4(OP)2

The complex of [CU(CH₃CHCOO)₂(OPph)]₂ has been synthesized and its X-ray crystal structure determined at room temperature, M = 975.96, tetragonal, space group: 14_1/a(#88), Dx = 1.39 g/ cm³, The final R is 0.067 for 2087 independent observed reflections with 1 > 3α(I). The molecule has an inversion center on the middle of the Cu Cu axis. The bond-length of the Cu Cu is 2.61/(2) Å. The coordinate polyhedron of Cu corresponds to a tetragonal bipyramid. The angle of Cu O P is significantly smaller than that of its adducts [Cu(O₂CR)₂L]₂.     

Phase trajectories in CaO-Al2O3-SiO2 melts

A technique for constructing a phase diagram of the CaO-Al₂O₃-SiO₂ system on a computer using the kinematic approach to describe surfaces is proposed. The geometric structure of the diagram and its phase regions is described. Crystallization paths are considered for different parts of the diagram.     

On the crystal structure type of 2 CsCl · CoCl2 · 2 H2O

The following three-component systems have been studied: CsCl MnCl₂ H₂O at 25 °C; 2 CsCl · CuCl₂ · 2 H₂O—2 CsCl · CoCl₂ H₂O at 10 °C and 2 CsCl · MnCl₂ · 2 H₂O—2 CsCl · CoCl₂ H₂O at 25 °C and 10 °C. It was established that Co²⁺-ions do not substitute isodimorphously the Cu²⁺-ions in the tetragonal salt 2 CsCl · CuCl₂ · 2 H₂O, whereas in the case of the triclinic salt 2 CsCl · MnCl₂ · 2 H₂O they can substitute isodimorphously the Mn²⁺-ions. The theoretical considerations supported by the results obtained allow to predict the existence of the double salt 2 CsCl · CoCl₂ · 2 H₂O as well as the type of its crystal structure — triclinic, space group P1 .     

Crystal Structures of (2-oxo-2H-Quinaxalin-1-yl)-acetic Acid and its Cobalt and Nickel Complexes and Their Comparison with (1,3-Dioxo-1,3-dihydro-isoindol-2-yl)-acetic Acid

Abstract The crystal structures of (2-oxo-2H-quinaxalin-1-yl)-acetic acid and its cobalt and nickel complexes are determined. The (2-oxo-2H-quinaxalin-1-yl)-acetic acid (1) crystallizes in orthorhombic, Pbca, a = 12.8571(11) ?, b = 9.4267(8) ?, c = 15.0095(13) ?, the cobalt complex of (2-oxo-2H-quinaxalin-1-yl)-acetic acid (2) crystallizes as dihydrate in triclinic, P-1 space group with a = 4.81150(10) ?, b = 11.8631(2) ?, c = 12.4867(3) ?, α = 71.7800(10)°, β = 79.2490(10)°, γ = 84.9020(10)° whereas the nickel complex of (2-oxo-2H-quinaxalin-1-yl)-acetic acid (3) crystallizes in monoclinic, P2₁/c space group with a = 14.9210(5) ?, b = 4.81730(10) ?, c = 15.7672(5) ?. and β = 99.823(2)°. The crystal structure of the ligand and the complexes are compared with structures of (1,3-dioxo-1,3-dihydro-isoindol-2-yl)-acetic acid and its cobalt and nickel complexes. Index Abstract The crystal structures of (2-oxo-2H-quinaxalin-1-yl)-acetic acid and its nickel and cobalt complexes are compared with (1,3-dioxo-1,3-dihydro-isoindol-2-yl)-acetic acid and its corresponding complexes with nickel(II) and cobalt(II).      

Structural and thermal properties of Zn2+-, Cd2+-, and Hg2+ forms of zeolite X

The exchange of Zn²⁺, Cd²⁺ and Hg²⁺ with zeolite NaX has been studied. The influence of the above cations on crystalline structure of zeolite X and its thermal stability has been shown on the grounds of X-ray diffraction, differential thermal analysis and infrared spectroscopic measurements.     

溶胶凝胶法制备WS2-SiO2可饱和吸收体的探究

WS2二维材料独特的光吸收体特性使其成为可饱和吸收体的优选材料。溶胶凝胶法具有操作方便、设备简单、成本低廉等优点。利用溶胶凝胶法在石英基片上制备SiO2材料为主体的WS2-SiO2薄膜是一种实现可饱和吸收体的新思路。本文通过改变实验过程中原料配比、热处理条件、旋涂速度等实验参数确定出溶胶凝胶法制备SiO2薄膜的最佳条件,在此基础上再加入WS2溶液制备出WS2-SiO2薄膜可饱和吸收体,通过共聚焦显微镜、透射电子显微镜、拉曼光谱、X射线衍射等方法对制备的样品进行了测试分析,结果表明采用本文提出的制作方法可以得到外观良好的WS2-SiO2薄膜可饱和吸收体、WS2在 SiO2薄膜中呈多层的多晶颗粒,晶面指数主要为(002)、(004)、(101)、(103)、(006)、(105)。     

(TMTSF)2(2,5-Tcnqbr2): Structure and Physical Properties

The 2:1 charge-transfer salt (TMTSF)₂(2,5-TCNQBr2) has been prepared and its physical properties investigated. Its crystal structure consists of segregated stacks of TMTSF donors (ring-over-bond overlap pattern; mean interplanar spacing of 3.6A) and chains of edge-on and disordered 2,5-TCNQBr2 acceptors. Infrared data are suggestive of unit charge on the 2,5-TCNQBr2 molecule and, therefore, half charge on the TMTSF donor. Resistivity data are successfully interpreted on the basis of a percolation construction. Magnetic data are also presented.     

Electronic Structure of [Cu(C7H4NO3S)2(H2O)4] · 2H2O Crystal

The electronic absorption spectrum and ESR spectrum of the crystal of the title compound [Cu(C₇H₄NO₃S)₂(H₂O)₄] · 2 H₂O, are measured. The experimental results are discussed quantitatively by using the ligand field theory and the radial wave function of non-free Cu(II). The electronic structure of the compound is in agreement with its crystal structure.     

EXAFS studies of glassy and liquid ZnCl2: A comparison with vitreous GeO2

The Zn-EXAFS (extended X-ray absorption fine structure) above its K-absorption edge has been measured for glassy ZnCl₂ at low temperature, through T_g (375 K), and into the supercooled and normal liquid state (mp = 593 K) at 673 K. By Fourier filtering and fitting the normalized glass spectra using α-ZnCl₂ as a model compound, the Zn²⁺Cl^? distance was determined to be (2.34 ± 0.01) Å and the average coordination number about the Zn²⁺ was found to be 5.1 ± 0.8. The latter value agrees with the value of 4.7 nearest neighbors obtained by the molecular dynamics computer simulation study of Woodcock et al., for liquid ZnCl₂ just above its melting point. The agreement is supportive of the notion that short-range order in the glass is reflective of that of the corresponding liquid from which it was quenched. Spectral measurement as a function of temperature indicates that there is considerable dynamic decoupling of the Zn²⁺ from its nearest Cl^? neighbor even below T_g. This is contrasted with similar data in glassy GeO₂ which show that the motion of Ge is strongly coupled with its four oxygen neighbors all the way to T_g. This difference in dynamic disorder substantiates the notion that glassy ZnCl₂, as well as vitreous BeF₂, provides a further weakened structural analog for glassy GeO₂ and SiO₂.     

溶胶-凝胶法制备CuAlO2粉末及其光电性能研究

采用柠檬酸络合的无机盐溶胶-凝胶法,结合自蔓延燃烧制备出铜铁矿结构的CuAlO2粉末。用DSC-TGA、X射线衍射仪、扫描电子显微镜等分析方法对CuAlO2的形成过程、物相结构、微观形貌等进行了研究。结果表明:形成CuAlO2相的温度在1092℃左右,在1100℃烧结2 h可以得到铜铁矿结构CuAlO2纳米粉末,其粒径分布在50～200 nm之间。制备的样品为p型半导体,CuAlO2片的电阻率为45.5Ω.cm;光学带隙增大,其值约为3.75 eV。     

高压下ReB2的结构特性及弹性性质

本文采用密度泛函理论中的赝势平面波法计算了ReB₂的P6₃/mmc晶体结构(即hP6-ReB₂)的结构特性及弹性性质。在计算了hP6-ReB₂的平衡结构参数后,从热力学、动力学及机械力学三方面验证了其结构稳定性。研究发现,hP6-ReB₂在高压下的弹性系数、各个弹性模量均随压强的增加而增大。泊松比显示hP6-ReB₂表现为脆性。三种类型的弹性波随压强的变化趋势显示hP6-ReB₂为弹性各向异性晶体。经估算,hP6-ReB₂结构的维氏硬度约为38.2 GPa。电子态密度揭示了hP6-ReB₂的Re—B和B—B之间存在着强共价键,并且随着压强的增加共价键逐渐增强。     

Structure and non-linear optical properties of BaO–TiO2–SiO2 glass containing Ba2TiSi2O8 crystal

The BaO–TiO₂–SiO₂ crystallized glass containing Ba₂TiSi₂O₈ crystal phase was examined using X-ray diffraction (XRD) measurement and Maker fringe technique. It has been found that the crystallized glasses with a composition of close to the stoichiometric Ba₂TiSi₂O₈ showed bulk crystallization, whereas other crystallized glasses with non-stoichiometric composition of Ba₂TiSi₂O₈ showed surface crystallization. The parameter ΔT, the difference in temperature between the crystallization onset and the glass transition temperature, strongly affects the crystallization behaviors of the present BTS glasses. The 30BaO–20TiO₂–50SiO₂ transparent surface crystallized glass with strong c-oriented Ba₂TiSi₂O₈ phase showed its second-order non-linear optical constant, d₃₃ = 6.1 pm/V.     

Crystal structures of 2-(2-methoxyphenyl) perimidine and its hemihydrate

The crystal structures of the title compound and that of its hemihydrate have been determined. The anhydrous compound is roughly planar due to an intramolecular hydrogen bond (IMHB). The orange color can be related to its planarity and to the greater degree of overlapping between the perimidine and the phenyl group than in the hemihydrate. The yellow hemihydrate is not planar and the water molecule joins through O-HN hydrogen bonds two molecules related by a crystallographic twofold axis. In solution the compound behaves like the anhydrous form.     

Crystal Structure,Spectroscopic and Computational Studies of N2O2 Type Salen-Based Schiff Base and Its Di-boron Complex

Journal of Chemical Crystallography - The presented study describe the crystal structure of a Schiff base and its dinuclear boron compounds that formulated as 1 (H2L) and 2 [B2F4(L)], respectively,...     

二维MoS2/WSe2异质结的光电性能研究

近年来基于二维半导体过渡金属硫族化合物如MoS₂的光电晶体管被广泛研究。虽然基于单层MoS₂的光电探测器表现出较高的响应度,但是其较低的载流子迁移率也限制了响应时间,约在秒量级。二维半导体的相互堆垛可以形成具有低缺陷态且空间均匀的范德华异质结构,是提高二维光电探测器性能的有效途径。基于此本文通过机械剥离转移法构筑MoS₂/WSe₂垂直pn异质结,其较强的空间电荷区能有效地分离光生载流子,所以在自驱动状态下仍具有较好的光电探测能力,光响应度和探测率分别达到2.12×10³ A/W和2.33×10¹¹ Jones,同时极大地缩短了响应时间,响应时间达到40 ms。这种二维异质结器件制备方法简易,性能优异,在光电子领域具有广阔的应用前景。     

Crystal structure of a seven-coordinate cobalt(II) complex with a new polyfunctional hydrazonic ligand, [Co(H4dapis)(OH2)2]Cl2·9/2H2O

A seven-coordinate cobalt(II) complex has been synthesized with a new hydrazonic ligand, H₄dapis, and its crystal structure determined by X-ray diffraction methods and refined toR 0.0564 for 2763 independent reflections. The structure consists of [Co(H₄dapis)(OH₂)2] cations, Cl anions, and lattice H₂O molecules interlinked by hydrogen bonds. The cobalt atom has a distorted pentagonal bipyramidal environment with two axial H₂O molecules and the H₄dapis ligand forming the basal plane.     

A neutron diffraction study of the phase transition of fully deuterated triglycine sulphate (ND2CD2COOD)3.D2SO4

Using neutron single crystal and powder diffraction, the first thorough investigation of the structure of fully deuterated triglycine sulphate, (ND₂CD₂COOD)₃.D₂SO₄ is presented, including its evolution with T, through its structural phase transition. This includes new precise structural parameters determined at several key temperatures above and below T_C using single crystal diffraction, and for the first time a parametric study has been undertaken over a wide temperature range — from 4 to 500 K in 2 K steps. It was found that fully deuterated TGS shows a structure consistent with hydrogenous TGS and partially deuterated TGS. The evolution of several key hydrogen bond lengths suggests that weakening of the H‐bond network with T is crucial in decoupling the polarising glycine molecules from the other glycines and allowing the long‐range ferroelectric order to break down. A new parameterisation of the phase transition is demonstrated. Contrary to results of physical properties measurements, there is no evidence of a second low temperature phase transition in TGS – no low temperature anomalies were observed in the crystal structure.