X-ray luminescence of Pb-containing microcrystals dispersed in the CsCl Matrix

The process of complexing in CsCl crystals in activating them with lead haloids PbX₂ (X=Cl, Br, I) (C_{PbX 2}=1 mole %) is investigated. The formation of CsPbCl₃ and Cs₄PbCl₆ microcrystals that are dispersed in the CsCl matrix is recorded. The luminescence-kinetic characteristics of the indicated microcrystals and single Pb²⁺v _c ⁻ centers are investigated. It is noted that the formation of the CsPbCl₃ and Cs₄PbCl₆ microcrystals is hindered as the radius of the anion of the lead haloid PbX₂ (X=Cl, Br, I) increases. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 67, No. 4, pp. 480–482, July–August, 2000.     

Exciton luminescence and many-body effect of monolayer WS2 at room temperature

Monolayer transition metal dichalcogenides favor the formation of a variety of excitonic quasiparticles, and can serve as an ideal material for exploring room-temperature many-body effects in two-dimensional systems. Here, using mechanically exfoliated monolayer WS₂ and photoluminescence (PL) spectroscopy, exciton emission peaks are confirmed through temperature-dependent and electric-field-tuned PL spectroscopy. The dependence of exciton concentration on the excitation power density at room temperature is quantitatively analyzed. Exciton concentrations covering four orders of magnitude are divided into three stages. Within the low carrier concentration stage, the system is dominated by excitons, with a small fraction of trions and localized excitons. At the high carrier concentration stage, the localized exciton emission from defects coincides with the emission peak position of trions, resulting in broad spectral characteristics at room temperature.     

Exciton relaxation in PbS quantum dots

Exciton relaxation in PbS quantum dots (QDs) in glass and tetrachloroethylene have been investigated and the radiative and non‐radiative relaxation rates of the lowest 1S–1S state have been measured. An estimate of the carrier intra‐band transition rates and their transfer efficiency is calculated. The dependence of the exciton dynamics on the QD surface properties is presented and discussed. (© 2010 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

硅BC8量子点太阳能电池中的多重激子效应

多重激子效应是指在纳米半导体晶体中,量子点吸收一个高能光子而产生多个电子-空穴对的过程,该效应可以提高单结太阳电池能量转换效率。利用碰撞电离机制和费米统计模型计算了工作温度300 K的单结硅BC8量子点太阳能电池在AM1.5G太阳光谱下的能量转换效率。对于波长在280~580 nm的入射光,多重激子效应可以大幅增强硅BC8量子点直径d>5.0 nm的量子点太阳电池的能量转换效率。硅纳米量子点的直径d=6.3~6.4 nm时,最大能量转换效率为51.6%。     

激子旋转弛豫对低掺杂卟啉侧链聚合物荧光衰变过程的影响

利用激子旋转扩散理论研究了一类低掺杂卟啉侧链聚合物中卟啉侧链基团的旋转对其发光动力学过程的影响.研究表明,卟啉侧链基团的旋转行为是导致激发态无辐射能量弛豫的重要途径.基团旋转越容易,能量弛豫速度越快,这可导致一个快速的荧光衰变动力学过程.在卟啉低掺杂浓度和聚合物分子链间距离较大的情况下,卟啉侧链基团的旋转成为影响荧光寿命和发光效率的主要因素.对实验测得的两种样品的荧光弛豫过程进行了拟合,理论结果与实验结果符合较好. 关键词： 激子旋转弛豫 瞬态荧光 卟啉侧链聚合物     

II-VI族稀磁半导体微纳结构中的激子磁极化子及其发光

自旋是基本粒子（电子、光子）角动量的内在形式.固体中体现自旋特征的集体电子行为如拓扑绝缘体等是当前凝聚态物理领域关注的焦点,是基态行为.激子作为电子空穴对的激发态且寿命很短,可复合发光,它是否能体现自旋极化主导的行为?对此人们的认识远不如针对基态的电子.激子磁极化子（exciton magnetic polaron,EMP）是由磁性半导体微结构中铁磁自旋耦合态与自由激子相互作用形成的复合元激发,但其研究很有限.本文概述了我们在稀磁半导体微纳米结构中的EMP及其发光动态学光谱、自旋极化激子凝聚态的形成方面取得的一些进展,展望了未来可能在自旋光电子器件、磁控激光、光致磁性等量子技术方面的潜在应用.     

Dynamics of Optically Driven Exciton and Quantum Decoherence

By using the normal ordering method, we study the state evolution of an optically driven excitons in aquantum well immersed in a leaky cavity, which was introduced by Yu-Xi Liu et al. [Phys. Rev. A63 (2001) 033816]. Theinfluence of the externallaser field on the quantum decoherence of a mesoscopically superposed state of the excitons isinvestigated. Our result shows that, the classical field can compensate the energy dissipation of the excitons. Althoughthe decoherence rate of the excitonic Schrodinger cat state does not depend on the external field, the phase of thedecoherence factor can be well controlled by adjusting the amplitude of the external field as well as the detuning betweenthe field and the transition frequency of the atom.     

Intermolecular Interactions in 8-Aza-D-Homogonane Crystals and their Manifestation in the IR Spectra

Crystalline modifications of 8-aza-D-homogon-1,3,5(10),13-tetraen-12,17a-dione have been investigated by IR spectroscopy and x-ray structural analysis. It is shown that this compound crystallizes from solutions of chloroform with hexane in the form of a solvate comprised of chelate hydrogen bonds between the hydrogen atom of the chloroform molecule and the oxygen atoms of the carbonyl groups of the 8-azasteroid molecule. A relation between the changes in the characteristic absorption bands of the CH₂-, C=O-, and I=C groups and the structure of the crystalline modifications has been established.     

Absorption and fluorescence of 8-azasteroids in the gas phase

Extensive studies of the spectral-luminescent characteristics of four 8-azasteroids and a model compound 2-(3,3-dimethyl-1,2,3,4-tetrahydro-1-isoquinolidene)-5,5-dimethyl-1,3-cyclohexanedion in the gas phase have been made. From the analysis of the dependences of the absorption spectra on the vapor pressure (T_low) and the fluorescence spectra on T_low and the exciting radiation wavelength (_exc) a conclusion on the presence in the vapors of the investigated 8-azasteroids of three absorption and fluorescence centers (S-, M-, and L-centers) has been drawn. The absorption spectra of these centers strongly overlap. Their long-wave absorption boundaries have been determined. The dependence of the fluorescence spectra of all three centers on _exc, which is inherent in rarefied gases of individual organic molecules, is observed. The S-centers are the molecules of the initial steroids, and the M- and L-centers are the molecules of thermo- and phototransformations of the initial steroids. The model compound in the gas phase is characterized by the same dependences of the fluorescence spectra on T_low and _exc as those inherent in 8-azasteroids. Taking into account the additional data obtained as a result of investigation of the absorption and fluorescence spectra of solutions of the substances extracted from vacuum cells after the investigation of 8-azasteroids and the model compound in the gas phase, conclusions on the nature of the M- and L-centers have been drawn.__________Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 72, No. 1, pp. 48–57, January–February, 2005.     

Anti-Stokes luminescence of microcrystals of AgCl0.95I0.05 solid solutions with adsorbed organic dye molecules

We have studied the effect of the characteristic features of aggregation of some organic dye molecules during adsorption on the parameters of low-temperature sensitized anti-Stokes luminescence (SASL) in microcrystals of AgCl_0.95I_0.05 solid solutions. We have demonstrated the possibility in principle of varying the position of the maximum in the SASL excitation spectrum and its intensity by varying the concentration of the dye molecules deposited on the surface of the AgCl_0.95I_0.05 microcrystals. We have observed that the intensity of SASL excitation for these samples increases as different types of dye aggregates form on their surface. __________ Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 73, No. 5, pp. 592–596, September–October, 2006.     

Exciton States in a Gaussian Confining Potential Well

We consider the problem of an electron-hole pair in a Gaussian confining potential well. This problem is treated within the effective-mass approximation framework using the method of numerical matrix diagonalization. The energy levels of the low-lying states are calculated as a function of the electron-hole effective mass ratio and the size of the confining potential.     

Intermolecular interactions of immunoactive 8-azasteroid

Intermolecular interactions in 2,3-dimethoxy-8-azagone-1,3,5(10),13-tetraene-12,17-dione and the molecular and crystal structure of this compound were studied by IR spectroscopy and x-ray diffraction analysis. Shortened intermolecular contacts related to the C-H?O, C-H?π, and π?π interactions were revealed in crystals of this 8-azasteroid. These contacts manifest themselves in changes in the characteristic frequencies of C-H, C=O, and C=C vibrations in the IR spectra. A relationship between the intermolecular interactions occurring in the crystalline and noncrystalline solid phases and the changes in the IR spectra of this compound was established.     

激子绝缘体

激子绝缘体是20世纪60年代初由诺贝尔物理学奖获得者莫特提出的一种新物相。众所周知,激子是固态系统中最典型的集体激发之一,简单地可视为电子—空穴由于库仑相互作用而形成的束缚对。在常规绝缘体或半导体材料中,单粒子能隙远大于激子束缚能。而在某些特殊的材料体系,如窄能隙半导体和二维材料中,激子的束缚能可能大于体系的单粒子能隙,因此体系内会自发形成大量的激子,进入激子绝缘体相。激子绝缘体是体系的基态,低浓度下激子可视为组合玻色子,在低温下会形成宏观相干态——激子玻色—爱因斯坦凝聚。文章简要地回顾了激子绝缘体的发展历史,并介绍了激子绝缘体、玻色—爱因斯坦凝聚和自旋超流的最新进展。     

960nm激光泵浦下Er3+和Yb3+掺杂氟氧化物微晶玻璃上转换发光特性

对经特殊退火后的Er3+和Yb3+离子共掺杂氟氧化物微晶玻璃的上转换发光特性进行了研究.研究结果表明,在960nm激光泵浦下,这种玻璃具有较高的上转换发光.通过我们的研究,弄清了在这种材料中Er3+的发光行为、上转换通道和Er3+和Yb3+离子之间的能量传递过程.     

Steady state and time-resolved studies of pyrene in solution and in single microcrystals

Single microcrystals of pyrene have been studied by steady state and time resolved fluorescence microscopy. The fluorescence spectra of microcrystals exhibit vibrational structure unlike the broad spectrum observed in pyrene excimer. A risetime is observed in the decay curves of the concentrated solutions, indicating the excimer formation. In contrast, the fluorescence decay profiles of the single microcrystals are nonexponential in nature and the decay times vary with their size and the wavelength of emission. This behaviour has been explained mainly by considering the pyrene dimer stabilized in the ground state.     

Exciton States in a Gaussian Confining Potential Well

We consider the problem of an electron-hole pair in a Gaussian confining potential well. This problem is treated within the effective-mass approximation framework using the method of numerical matrix diagonalization. The energy levels of the low-lying states are calculated as a function of the electron-hole effective mass ratio and the size of the confining potential.     

CdSe/CdZnSe超晶格的激子光学性质的研究

用分子束外延法在GaAs衬底上生长了CdSe/Cd0.65Zn0.35Se超晶格结构。利用X射线衍射（XRD）、77K下变密度激发的光致发光光谱和变温度光致发光光谱研究了CdSe/CdZnSe超晶格结构和激光复合特性，在该材料中观测到激子－激子散射发射峰，变密度激发光致发光光谱和谱温度光致发光光谱证实了这一现象，激子发射峰的线宽随着温度的升高而展宽，低温时发光峰的宽度主要是由合金组分和阱垒起伏引起的，没温时激子线宽展宽是由于激子与纵光学声子和离化的施主杂质间的散射作用引起的，光致发光的强度随着温度的升高而降低，这主要是由激子的热离化造成的，也就是说，热激发使得电子或空穴由阱中跃迁至垒上。     

NaLa(MoO4)2∶Eu3+的水热调控合成与发光特性研究

采用水热法合成了不同粒径的NaLa(MoO₄)₂∶Eu³⁺微晶.通过调节乙二醇浓度和反应时间,研究了NaLa(MoO₄)₂∶Eu³⁺微晶的形貌演变过程,在水热条件下180 ℃反应16 h获得了均一梭子形NaLa(MoO₄)₂∶Eu³⁺微晶,其晶粒长度约为2.0 μm.荧光光谱分析表明,Eu³⁺取代了NaLa(MoO₄)₂中La³⁺的格位, Eu³⁺在613 nm处红光发射(⁵D₀–⁷F₂跃迁)的浓度猝灭机理是电偶极-电四极相互作用,并发生了Eu³⁺( ⁵D₁ ) + Eu³⁺(⁷F₀ )→ Eu³⁺( ⁵D₀ ) + Eu³⁺(⁷F₃) 交叉弛豫,由此导致浓度猝灭. 关键词： 钼酸盐 水热法 稀土离子 发光