SiO2包覆Y2O3:Er3+纳米粉的制备及发光性能

用微乳液法合成出SiO2包覆的Er3+掺杂的Y2O3粉体.X射线衍射结果表明,所制备粉体为立方Y2O3结构.透射电镜照片显示,其颗粒形状近似为球形,粒径为20～50 nm.该粉体在波长为980 nm的半导体激光器激发下发射出中心波长为562 nm的绿色和660 nm的红色上转换荧光,分别对应于Er3+离子的4S3/2/2H11/2→4I15/2跃迁和4F9/2→4I15/2跃迁,发光强度和激发功率的关系揭示其均为双光子过程.Er3+掺杂的Y2O3粉体具有高效的上转换发光性能,而经过纳米复合后制成的Y2O3(核)/SiO2(壳)在水溶液中具有较好的悬浮性,这对于其在生物荧光标记的应用具有重要意义.     

Er3+/Yb3+共掺杂氧氟硅酸盐玻璃的上转换发光

研究了Er^3 ／Yb^3 共掺氧氟硅酸盐玻璃的吸收光谱、上转换光谱和拉曼光谱。分析了氧氟硅酸盐玻璃中Yb”敏化Er^3 的上转换发光机理。结果表明：通过975nm的激光二极管激发,在室温下同时观察到蓝光(408nm)、绿光(529nm和545nm)和红光(667nm),分别是由于Er^3 离子。H9/2→^4I15/2,H11/2→^4I15/2,H3/2→^4I15/2和H9/2→^4I15/2跃迁。随Yb2O3浓度的增加。Yb^3 对Er^3 的能量转移增强,因此蓝光、绿光和红光的发光强度都增强,强烈的绿光和红光激发是由于双光子吸收过程,而微弱的蓝光是由于三光子吸收过程。拉曼光谱发现,对Er^3 离子在氧氟硅酸盐玻璃中的上转换发光。玻璃结构中的PbF2起到重要作用。     

氧化钇（铒,镱）的合成及上转换发光

采用均相沉淀,马弗炉煅烧的方法,合成了一系列Y2O3∶Er3＋,Yb3＋上转换发光材料.该类材料在波长为980 nm半导体激光器激发下发射出中心波长为564nm的绿色和662nm的红色上转换荧光,分别对应于Er3＋离子的4S3/2/2H11/2→4I15/2和4F9/2→4I15/2跃迁.探讨了不同合成条件对其上转换发光强度和波长的影响,发现沉淀时的pH值,煅烧温度和沉淀中Er3＋、Yb3＋的相对浓度对其发光有显著影响.     

水热合成六方相NaYbF4：Er^3＋／Tm^3＋的上转换白光性质

在反应温度为220℃,反应时间为48h的温和条件下,利用水热法合成单掺杂或共掺杂Tm^3＋、Er^3＋的六方相NaYbF4体系,利用X射线粉末衍射、紫外-可见-近红外漫反射吸收光谱以及荧光光谱等测试手段,分析体系的物相结构和荧光性能。在980nm红外激光的激发下,NaYbF4：Er^3＋体系能发出强的绿光和红光,两者分别对应于Er^3＋离子的（^2H11／2,^4S3/2）→^4I15／2、^4F9／2→^4I15/2能级跃迁;NaYbF4：Tm^3＋体系能发出对应于Tm^3＋离子^1D2→^3F4和^1G4→H6能级跃迁的强蓝光;而NaYbF4：Er^3＋／Tm^3＋体系能同时发出红蓝绿三种颜色的光;各发射的归属与单掺杂相同,但由于Er^3＋和Tm^3＋离子之间存在能量交叉弛豫,致使各发光强度发生变化。通过控制Er^3＋和Tm^3＋离子的浓度及其比例,可以调整NaYbF4：Er^3＋／Tm^3＋体系的上转换蓝光、绿光和红光强度的比例,结果表明,在980nm红外激光的激发下,NaYbF4：Er^3＋／Tm^3＋（0．4％／0．4％）能发出近似白光的上转换发射。因此,NaYbF4：Er^3＋／Tm^3＋有望成为单一基质的上转换白光材料。     

掺杂Er^3＋的TiO2的发射光谱研究

用无水乙醇、冰醋酸、钛酸丁酯凝胶法制备了掺杂Er^3＋的TiO2粉末，测量了其在488m激发下的Stokes发射光谱和980nm激发下的上转换发光光谱。在可见光范围内，观察到了绿光和红光，绿光从500-570nm，对应Er^3＋的^2H11/2,^4S3／2→^4I15/2，红光从650～690m，对应Er^3＋的^4F9／2→^4I15／2的跃迁。由ln Ivis-In Iin曲线可知，绿光和红光均为双光子过程，光强正比于泵浦功率的二次方，即Iout ∝Iin。初步研究了此材料的上转换过程。     

Er3+单掺,Er3+/Yb3+共掺杂氟化物中红绿上转换荧光机理实验探索

制备了稀土离子Er^3＋单掺,Er^3＋-Yb^3＋共掺杂氟化物样品。在980nm波长激光激发下,室温时观察到了清晰可见的红（650nm）绿（545nm）上转换荧光,它们分别对应^4S3/2,^2H11/2-^4I15/2和^4F9／2-^4I15/2的发射。同时发现红绿上转换荧光的比值随Er^3＋的浓度增加而减少（对共掺而言）。上换荧光强度与激发光强度的关系表明红绿上转换荧光都是双光子上转换过程,在此基础上,根据能量匹配的原理,讨论了红绿上转换荧光的可能实现机制。     

YLiF4:Er3+,Yb3+中敏化剂浓度对发光的影响

用水热法合成了YLiF4：Er^3＋,Yh^3＋,Er^3＋的浓度固定为2mol％,Yb^3＋浓度变化范围是0～7mol％。在这个浓度范围内,980nm附近的吸收随着Yb^3＋浓度的增大而增强。用980nm激发得到的上转换发光强度随Yb^3＋浓度的增大而增强。在Yb^3＋浓度低于6mol％时,上转换发光强度随Yb^3＋浓度的增大变化的比较缓慢,当Yb^3＋浓度超过6mol％时,上转换发光突然增强。以Yb^3＋浓度是2mol％的样品为代表,研究了Er^3＋对应红光、绿光发射的激发光谱,并测试了不同波长激发下的红光发射和绿光发射,证明红光发射是来源于^4F9/2→^2I15/2,绿光是来自^4S3/2→^2I15/2和^2H11/2→^2I15/2。它们的上转换过程都是双光子过程。     

Er^3+,Cr^3+共掺杂BaAl2Si2O8荧光粉的发光性质及能量传递

利用高温固相法合成BaAl2Si2O8:Cr^3+,Er^3+系列荧光粉,研究了Cr^3+和Er^3+掺杂对BaAl2Si2O8材料发光特性的影响.BaAl2Si2O8:Er^3+荧光样品在393 nm激发波长下只呈现出峰值为550 nm的绿色荧光,来源于2H11/2→4I15/2和4S3/2→4I15/2跃迁的叠加.BaAl2Si2O8:Cr^3+荧光样品在550 nm激发波长下呈现峰值为694 nm的红色荧光,来源于2E→4A2的跃迁.在共掺杂样品BaAl2Si2O8:Cr^3+,Er^3+中,用Cr^3+激发峰的凹槽处380 nm作为激发光,得到的发射峰不仅有Er^3+的发射峰位,还有Cr^3+的发射峰位,说明两个离子之间可能存在辐射能量传递;对共掺杂BaAl2Si2O8:1%Cr^3+,x%Er^3+样品的荧光光谱进行测试,随着x的增加,Cr^3+的激发和发射光谱强度均有所增加,并且当x=0.5时,光谱强度是原来的4倍.另外,当固定Cr^3+的浓度时,随着Er^3+的浓度增加,Cr^3+的荧光寿命逐渐增加;当固定Er^3+的浓度时,随着Cr^3+的浓度增加,Er^3+的荧光寿命逐渐减小.这些现象表明了Er^3+和Cr^3+之间存在共振能量传递,通过理论计算得到Er^3+和Cr^3+之间的能量临界距离为4.5 nm,属于电偶极-电偶极相互作用.     

Sr3B2O6：Tb^3＋，Li^＋绿色荧光粉的发光特性

用高温固相法合成了Sr3B2O6：Tb^3＋,Li^＋绿色荧光粉,并研究粉体的发光性质。发射光谱由位于黄绿区的4个主要荧光发射峰组成,峰值分别位于495,548,598,625nm,对应了Tb^3＋的^5D4→^7F6,^5D4→^7F5,^5D4→^7和^5D4→^7F3特征跃迁发射,548nm的发射最强。激发光谱表现从200—400nm的宽带,可以被近紫外光辐射二极管（near-ultraviolet light-emitting diodes,UVLED）管芯产生的350-410nm辐射有效激发。研究了Tb^3＋掺杂和电荷补偿剂对样品发光亮度的影响。Sr3B2O6：Tb^3＋,Li^＋是一种适用于白光LED的绿色荧光粉。     

SiO2包覆Y2O3:Er3+纳米粉的制备及发光性能

用微乳液法合成出SiO2包覆的Er3+掺杂的Y2O3粉体.X射线衍射结果表明,所制备粉体为立方Y2O3结构.透射电镜照片显示,其颗粒形状近似为球形,粒径为20～50 nm.该粉体在波长为980 nm的半导体激光器激发下发射出中心波长为562 nm的绿色和660 nm的红色上转换荧光,分别对应于Er3+离子的4S3/2/...     

Fine structure and isotope shift of the 3s4d 3 D-3s3p 3 P, 3s5d 3 D-3s3p 3 P and 3p 2 3 P-3s3p 3 P Transitions of MgI

Summary We report the measurements of the³ D(3s4d)-³ P(3s3p)³ D(3s5d)-³ P(3s3p), and³ P(3p ²)-³ P(3s3p) transition frequency of MgI, the fine-structure separation and isotope shift between²⁴Mg and²⁶Mg. The measurements have been performed in a metastable atomic beam; a good agreement is found for data already existing in the literature. The accuracy of the measurements reported in this paper is mainly limited by the Doppler broadening of theI ₂ transitions used as a reference and by the precision in the knowledge of the related wavelengths.     

The gas phase infrared band contours of s-triazine and s-triazine-d3: The fundamentals of C3N3H3 and C3N3D3 and some overtone and combination bands of C3N3H3

The systematic application of band contour techniques to account for most of the observed features of the ir spectra of s-triazine and s-triazine-d₃ have been made as well as a critique as to the limitations of such methods. The experimental and computer methods used to study the gas phase infrared band contours of s-triazine and s-triazine-d₃ are out-lined. Contours of the five E′ fundamentals of s-triazine have been recorded under moderate resolution and analyzed to give the Coriolis constants $\text{ζ}{}_{\mathrm{i}}{}^{\mathrm{z}}$, i = 6–10. The effects of l-resonance are very apparent for ν₈ and ν₉, in the form of holes in the Q branches of these bands. Under the highest resolution available, ν₆ and ν₁₀ also show l-resonance effects. Values of the l-doubling constants $\text{q}{}_{\mathrm{i}}{}^{\mathrm{(+)}}$ were obtained for these four fundamentals. One of the parallel A₂″ fundamentals of C₃H₃N₃ (ν₁₂) has also been studied. It lies close to ν₁₀(E′) and an A × E type of second-order Coriolis resonance may be the cause of the intensity enhancement observed in the inner wings of the ν₁₂ and ν₁₀ bands. Hot bands of the type (ν_i + nν₁₄ ? nν₁₄) have been observed in the contours of ν₈, ν₁₀, and ν₁₂. This is felt to be responsible for the large difference between our observed zeta sum (?1.30) and the theoretical sum (?1.00).The gas phase infrared band contours of the five E′ and 2A₂″ fundamentals of C₃N₃D₃ have also been recorded under moderate resolution. From P-R separations and by computer simulation of the contours, values of the Coriolis constants $\text{ζ}{}_{\mathrm{i}}{}^{\mathrm{z}}$ have been obtained for the E′ modes. The effects of l-resonance have been observed for ν₈(E′) and ν₁₀(E′) and values of the l-doubling constants $\text{q}{}_{\mathrm{i}}{}^{\mathrm{(+)}}$ have been estimated. An extensive series of hot bands of the type (ν₁₂ + nν₁₄ ? nν₁₄) has been observed in the contour of the ν₁₂ (A₂″) fundamental. The mass effect on the Coriolis constants has been discussed.Infrared band contours of the overtone 2ν₇ and seven degenerate E′ combination bands of C₃N₃H₃ have been recorded under moderate resolution. Analysis of these contours using the P-R separation method and computer simulation of the contours has given values of $\text{ζ}{}_{\mathrm{<mtext>eff</mtext>}}{}^{\mathrm{z}}$ for these bands. Fermi resonance between 2ν₇ and ν₆ has been analyzed. The importance of considering both the observed contour as well as the observed frequency when assigning higher tone bands is illustrated.     

LaGaO3:RE3+(RE3+=Eu3+,Ho3+)的光谱

本文用固态反应合成了钙钛矿型的LaGaO3和LaGaO3:RE3+(RE3+=Eu3+,Ho3+)荧光体,并观察了物相随不同的激活离子浓度的变化。测量了化合物在室温下的反射光谱,激发光谱和荧光光谱。研究了Eu3+的D0→7F2和Ho3+的5S2→5I8的荧光强度与激活离子浓度的关系,发现了浓度猝灭,并得到了最大荧光强度的浓度值。     

Infrared spectra of matrix isolated BH3NH3, BD3ND3, and BH3ND3

The infrared spectra of ammonia-borane, BH₃NH₃, and two of its deuterated isotropic species, BD₃ND₃ and BH₃ND₃, isolated in argon matrix at liquid hydrogen temperature have been measured. Well resolved bands for these three isotopic species have been observed for all the fundamentals. A complete frequency assignment based on C₃v molecular symmetry has been made. A set of force constants have been calculated from the data for the two isotopes BH₃NH₃ and BD₃ND₃ using a valence force field. The agreement between experiment and frequencies calculated from these force constants for the mixed isotopic species, BH₃ND₃, substantiates the present assignment.     

Dielectric investigations of solid solutions SrTiO3-KTaO3 and SrTiO3-KNbO3

The temperature dependences of the dielectric constant and dielectric hysteresis loops in ceramic samples of (1 ? x)SrTiO_3?x KNbO₃ and (1 ? x)SrTiO_3?x KTaO₃ (0 ≤ x ≤ 0.3) solid solutions prepared using different heat treatments have been investigated. Phase diagrams of the studied solid solutions have been constructed in the T-x coordinates. It has been shown that, after quenching of samples (spontaneous cooling at room temperature after long-term heating at the sintering temperature of the ceramic samples), the temperature of the induced phase transition increases because of the weakening of random electric fields associated with nonisovalent impurities due to their “frozen” nonequilibrium redistribution. For small concentrations x, strong dielectric relaxation is observed in the temperature range of 150–250 K. A model of relaxing centers, which is based on the local charge compensation of heterovalent impurities, has been proposed.     

O_3 fast and simple treatment-enhanced p-doped in Spiro-MeOTAD for CH_3NH_3I vapor-assisted processed CH_3NH_3PbI_3 perovskite solar cells

We demonstrate a simple and fast post-deposition treatment with high process compatibility on the hole transport material(HTM) Spiro-MeOTAD in vapor-assisted solution processed methylammonium lead triiodide(CH_3NH_3PbI_3)-based solar cells. The prepared Co-doped p-type Spiro-MeOTAD films are treated by O_3 at room temperature for 5 min,10 min, and 20 min, respectively, prior to the deposition of the metal electrodes. Compared with the traditional oxidation of Spiro-MeOTAD films overnight in dry air, our fast O_3 treatment of HTM at room temperature only needs just 10 min,and a relative 40.3% increment in the power conversion efficiency is observed with respect to the result of without-treated perovskite solar cells. This improvement of efficiency is mainly attributed to the obvious increase of the fill factor and short-circuit current density, despite a slight decrease in the open-circuit voltage. Ultraviolet photoelectron spectroscopy(UPS) and Hall effect measurement method are employed in our study to determine the changes of properties after O_3 treatment in HTM. It is found that after the HTM is exposed to O_3, its p-type doping level is enhanced. The enhancement of conductivity and Hall mobility of the film, resulting from the improvement in p-doping level of HTM, leads to better performances of perovskite solar cells. Best power conversion efficiencies(PCEs) of 13.05% and 16.39% are achieved with most properly optimized HTM via CH_3NH_3I vapor-assisted method and traditional single-step method respectively.     

Ba3La(BO3)3基质中Tb3+的光致发光

以高温固相法合成了Ba3La(BO3)3∶Tb3 发光材料。在254nm紫外光激发下,研究了Ba3La(BO3)3∶Tb3 的激发光谱、发射光谱、发光强度与Tb3 浓度的关系。确定了Ba3La(BO3)3基质中Tb3 的自身浓度猝灭机理;探讨了助熔剂LiCO、敏化剂Ce3 、Bi3 的加入对荧光粉的发光强度的影响。     

Terahertz Vibrational Modes in CH3NH3PbI3 and CsPbI3 Perovskite Films

JETP Letters - Films of CH3NH3PbI3 organometallic perovskite, which is currently considered as a promising basic material for new-generation solar cells, as well as films containing CsPbI3...     

Far Infrared Spectra of Ammonia-Boron Trifluoride: NH3BF3 and ND3BF3

Abstract

Spectra of polycrystalline samples of NH₃BF₃ and ND₃BF₃ at 300 K and 98 K have been recorded in the frequency range 20-400 cm^?1. Isotopic frequency ratios are used to interpret the observed features in terms of the known molecular and crystal structures.