SiO2凝胶玻璃中联吡啶S2→S0S辐射跃迁

联吡啶以分子水平掺入SiO2凝胶玻璃中，显示出独特的光谱性质。其发射光谱除了正常的S1→S0跃迁产生的中心位于400nm的发射峰外，还出现了中心位于454nm的激基缔合物发射峰。经200℃处理后，联吡啶分子受Si-O网络刚性约束，激基缔合发射峰消失，出现了基于S2→S0辐射跃迁产生的325nm高能级发射峰。至550℃处理后，因联吡啶分子基本进入Si-O三维网络的间隙，发射光谱中只剩下振动结构明显的高能级荧光峰。上述结果为表征有机／无机复合材料微结构演变提供了荧光探针工具。     

SiO2凝胶玻璃中联吡啶S2→S0辐射跃迁

联吡啶以分子水平掺入SiO2凝胶玻璃中, 显示出独特的光谱性质. 其发射光谱除了正常的S1→S0跃迁产生的中心位于400 nm的发射峰外, 还出现了中心位于454 nm的激基缔合物发射峰. 经200 ℃处理后, 联吡啶分子受Si-O网络刚性约束, 激基缔合发射峰消失, 出现了基于S2→S0辐射跃迁产生的325 nm高能级发射峰. 至550 ℃处理后, 因联吡啶分子基本进入Si-O三维网络的间隙, 发射光谱中只剩下振动结构明显的高能级荧光峰. 上述结果为表征有机/无机复合材料微结构演变提供了荧光探针工具.     

S2激光器的发展

本文回顾硫双原子分子激光器的发展历史,通过借鉴已有激光器件在设计上积累的成功经验和存在的不足之处,提出一种新型可拆卸式横向脉冲快放电Ｓ２激光管的设计方案并给出此激光管设计的截面图和立体图。     

Theory of the 2S–2P Lamb shift and 2S hyperfine splitting in muonic hydrogen

The 7σ$7\sigma$ discrepancy between the proton rms charge radius from muonic hydrogen and the CODATA-2010 value from hydrogen spectroscopy and electron-scattering has caused considerable discussions. Here, we review the theory of the 2S–2P Lamb shift and 2S hyperfine splitting in muonic hydrogen combining the published contributions and theoretical approaches. The prediction of these quantities is necessary for the determination of both proton charge and Zemach radii from the two 2S–2P transition frequencies measured in muonic hydrogen; see Pohl et al. (2010) [9] and Antognini et al. (2013) [71].     

H2S和H2S+的振动光谱和电子能谱计算

本文基于MOLPRO软件包使用从头算方法计算了星际分子H₂S及其阳离子H₂S⁺的势能面及光电子能谱.首先,在(U)CCSD/cc-pVQZ理论水平下获取了H₂S沿法线坐标展开的势能面,势能面直观描述了不同振动模式耦合对分子能量变化的影响,S-H键的非对称伸缩振动和面内弯曲振动共同作用使得系统势能变化范围明显变大.振动多组态相互作用方法被用来计算非谐振动频率和振动光谱,计算结果显示,倍频和组合频之间出现了强烈的费米共振,使得相应波段处的红外强度显著增强.最后,使用拉曼波函数和收缩不变Krylov子空间方法首次计算了H₂SΧ¹A₁→H₂S⁺ X²B₁的光电子能谱.此项研究有助于进一步理解星际分子的内部结构,并为实验研究及星际观测提供参考.     

La_2O_2S和Ti~(4+)激活的La_2O_2S的发光光谱特性

对于很多稀土激活剂来说,具有A-型稀土氧化物结构的La_2O_2S是一种有效的基质晶体。本文报导Ti~(4+)在这种基质中的光谱特性。Ti~(4+)具有d°电子能态,而不存在明显的与它通常所发射的光相对应的原子能级,因而,Ti~(4+)发射的性质和机理还不十分清楚。我们知道,为了获得Ti~(4+)的高效发光,经常需要大于10％克分子的高浓度激活剂,这比大多数过渡金属和稀土激活剂所需要的浓度大得多。Ti激活的化合物的发光仅仅在氧化条件下制备的     

Phase Transition in Ag2S and the Relative Position of Atomic Planes of the α-Ag2S and β-Ag2S Phases

JETP Letters - The relative position of atomic planes of low-temperature monoclinic acanthite α-Ag2S and high-temperature bcc argentite β-Ag2S has been determined from X-ray and electron...     

IR impurity absorption in Sb2S3–GeS2(Ge2S3) chalcogenide glasses

The IR optical transmission spectra in the 4000–1000 cm⁻¹ (2.5–10 μm) region in the chalcogenide glasses (ChG) of the ternary Ge–Sb–S system of stoichiometric Sb₂S₃–GeS₂ and non-stoichiometric Sb₂S₃–Ge₂S₃ compositions are studied. The compositional dependences of the measured IR spectra connected with influence of O-, H- and C-based absorbed impurites are analyzed.     

ψ(2S)→ρπ及ψ(2S)→KK衰变的研究

利用在北京谱仪上获取的1.27×10⁶ψ(2S)事例研究了末态为矢量介子与赝标量分子的ψ(2S)两体衰变过程,ψ(2S)→ρπ及KK,得到它们的衰变分支比上限在90%置信度下分别为3.6×10^－5(ρπ),2.5×10^－5(K+K-+C.C.)(C.C.代表电荷共轭态)及1.2×10^－4(K0K0+C.C.).这些结果在新的实验灵敏度水平上证实了ψ(2S)相对于J/ψ强衰变中的反常压制现象的存在.     

α-In2S3 and β-In2S3 phases produced by SILAR technique

In₂S₃ films have been deposited by the successive ionic adsorption and reaction technique (SILAR) at room temperature. The films have been examined to evaluate the structural and optical properties. X-ray diffraction spectra have revealed the presence of both the α-In₂S₃ (cubic) and β-In₂S₃ (tetragonal) phases. The presence of the α-In₂S₃ phase at room temperature is attributed to the richness of In in the deposited materials. The presence of both phases is also supported by FESEM observations. The crystallinity of the material has been observed to improve with increasing thickness. Direct band gap of the deposits decreased from 2.89 to 2.37?eV with increasing thickness.     

Energy Interval 1S–2S in Muonic Hydrogen and Helium

Journal of Experimental and Theoretical Physics - The interval of a large structure of energy spectrum (1S–2S) in muonic helium and hydrogen is calculated using a quasi-potential method in...     

Stability of Thin-Film Cu–As2S3 and Ag–As2S3 Structures

Technical Physics - Thin-film Cu–As2S3 and Ag–As2S3 structures obtained by successively evaporating Cu(Ag) and As2S3 in vacuum on glass substrates have been studied. Samples of these...     

自旋S=3/2和S=2 Blume-Capel模型相变的Monte Carlo研究

利用计算机MonteCarlo模拟,研究自旋S=3/2和S=2Blume-Capel模型的相图。与最近刚发展起来的适用于研究S>1的关联有效场相比较,得出如下结论:对于S=3/2和S=2,关联有效场过高地估计了它们的相变温度对于S=3/2的相图,除了有二级相变线外,还发现了一级相变线对于S=2,关联有效场同样过高地估计了三临界点的值。 关键词：     

H_2S晶体振动光谱计算

Ｈ２Ｓ晶体振动光谱计算曾维扬毛延哲（兰州大学物理系兰州７３００００）高祥萍（上海电缆研究所上海２０００９３）ＬａｔｉｃｅＤｙｎａｍｉｃｓｏｆｓｏｌｉｄＨ２ＳＺｅｎｇＷｅｉｙａｎｇ，ＭａｏＹａｎｚｈｅ（ＬａｎｚｈｏｕＵｎｉｖｅｒｓｉｔｙＬａｎｚｈｏｕ７...     

Molecular dynamics simulation of sulphur nucleation in S–H2S system

The mechanism of sulphur nucleation in S–H₂S system is investigated by molecular dynamics simulation with the ReaxFF reactive force field. The results indicate that the nucleation of sulphur requires certain conditions. The nucleus of sulphur will form once the allotropes of sulphur dissolve from polysulphanes. Separate sulphur atoms aggregate into the cluster in the initial stage of nucleation according to the snowball effect. The cluster of nucleation is judged by the average distance of the neighbour sulphur atoms, which is identified as 2.8 Å through a parametric study. The sustainable process of nucleation depends on whether the cluster can overcome its critical state. The formation of the cluster may accelerate its own nucleation/coalescence and H₂S decomposition.     

Radiation-stimulated changes in the transmission of chalcogenide glasses of As2S3−Ge2S3

The radiative-optical properties of chalcogenide glass-like semiconductors of the As₂S₂−Ge₂S₃ system in the region of a topological 2D-3D-phase transition are investigated. It is shown that γ-irradiation of samples by an absorbed dose of 4.4 · 10⁶ Gy leads to a longwave shift of their optical-transmission edge in the spectrum. The effect observed depends on the structural type of the glasses investigated and changes considerably near the 2D-3D-phase transition. Two components of the transmission-edge shift are detected: a static component, which remains unchanged for a long time after irradiation of the samples, and a dynamic one, which gradually fades in 2–3 months. It is suggested that the microstructural mechanism of these changes is attributable to processes of coordination defect formation in the structural skeleton of the samples. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 66, pp. 657–660, September–October, 1999.     

H2S2分子的阻碍内旋转势能函数

应用无波函烽微扰理论导出了分子障碍内旋转能谱的解析式，基于扭转频率光谱数据，确定了Ｈ２Ｓ２分子的阻碍内旋转势能函数。