Pr^3＋掺杂的LaF3纳米微晶／氟氧化物玻璃陶瓷的4f5d能级光谱性质

用同步辐射的真空紫外(VUV)和紫外(UV)作为激发源研究了Pr^3 (0．1％)掺杂的LaF3纳米微晶，氟氧化物玻璃陶瓷的4f5d能级光谱性质。样品中存在两种不同的Pr^3 -LaF3微晶中的Pr^3 最低的4f5d能级在^1S0能级之上，玻璃中的却在^S0能级之下，通过VUV和UV激发光谱得出这两种Pr^3 最低的4f5d能级的位置。当用181nm光激发样品时，在发射光谱中同时观察到了微晶中Pr^3 4f^2→4f^2的窄谱带发射和玻璃中4f5d→4f^2的宽谱带发射。在20K时观察到了LaF3纳米微晶中作为Pr^3 光子级联发射(PCE)第二步的^3P0→H4的跃迁，室温下却没有观察到，文中详细讨论了产生这种现象的原因。     

铒离子掺杂的含LaF3纳晶氟氧化物玻璃陶瓷的制备及其发光性能

主要研究了热处理制度对掺杂Er^3＋离子的含有LaF3纳米晶体的氟氧化物玻璃陶瓷的上转换发光和近红外发光性质的影响。制备了ErF3掺杂的SiO2-Al2O3-Na2O-LaF3系统玻璃，将其在不同温度下处理不同的时间，测试其上转换和近红外的发光行为的变化，并相应进行了XRD测试，基于XRD数据计算了晶粒大小和结晶度，考察了热处理制度对该材料微观结构及发光性能的影响。结果表明：在一定的温度下保温，LaF3晶体从玻璃基体中析出，并且随着热处理温度的升高和时间的延长，晶粒不断长大，结晶度持续增加，因为上转换的发光与基质的声子环境密切相关，所以随着氟化物晶体的增多，相应的玻璃陶瓷的上转换发光的强度也增大，而在氟氧化物玻璃中检测不到上转换发光。但是，对于近红外1530nm处的铒离子发光，氟化物晶体的析出对于其发光性质并没有太大的影响。     

LaF3:Eu3+纳米粒子的水热法制备及发光性质研究

用水热法制备了LaF3及Eu^3＋掺杂的LaF3纳米粒子, 通过X射线粉末衍射（XRD）、透射电子显微镜（TEM）和荧光光谱（FS）对样品进行了表征. 结果表明： 所得的纳米粒子粒度均匀、结晶完好, 呈规则的六边形形状;研究了反应温度和时间对LaF3纳米粒子形成的影响, 初步探讨了纳米粒子的生长机制. 研究了掺杂Eu^3＋后的发光性质, 发现纳米粒子经高温煅烧后, 荧光强度有明显下降, 适宜的煅烧条件为600 ℃/6 h, Eu^3＋的掺杂量在5%（摩尔分数）时, 纳米粒子的荧光强度最强, 更高的掺杂浓度将导致荧光猝灭.     

LaF_3∶Eu~(3+)纳米粒子的水热法制备及发光性质研究

用水热法制备了LaF3及Eu3+掺杂的LaF3纳米粒子,通过X射线粉末衍射(XRD)、透射电子显微镜(TEM)和荧光光谱(FS)对样品进行了表征。结果表明:所得的纳米粒子粒度均匀、结晶完好,呈规则的六边形形状;研究了反应温度和时间对LaF3纳米粒子形成的影响,初步探讨了纳米粒子的生长机制。研究了掺杂Eu3+后的发光性质,发现纳米粒子经高温煅烧后,荧光强度有明显下降,适宜的煅烧条件为600℃/6 h,Eu3+的掺杂量在5%(摩尔分数)时,纳米粒子的荧光强度最强,更高的掺杂浓度将导致荧光猝灭。     

Ga2O3-La2O3-Yb2O3-Er2O3(HO2O3)体系光谱性质的研究

根据稀土离子能级的特点,对Ga2O3-La2O3-Yb2O3-Er2O3(HO2O3)体系的光谱性质进行了探讨,发现它们有二类发光性质:Stokes发光和反Stokes发光,研究了发光强度和发射波长与掺杂离子的依赖关系,观察到由能量的共振转移引起的荧光浓度猝灭现象,并取得了最大发光强度时的掺杂离子浓度和一些规律性结果.     

用于1．54μm微片激光器的高Er^3＋／Yb^3＋共掺杂的氟铝酸盐玻璃

本文系统制备了980nm半导体崩浦的应用于1．54μm波段微片激光器的高Er^3 ／Yb^3 共掺杂的氟铝酸盐玻璃。通过玻璃的吸收光谱，发射光谱和上转换荧光光谱的测试，对其光学性质、浓度淬灭及其淬灭机制进行了分析和讨论。当玻璃中Er^3 离子掺杂浓度低于10mol％的情况下，浓度淬灭现象较弱，Er^3 ／Yb^3 共掺杂的氟铝酸盐玻璃在由于Er^3 离子^4 I13／2→4^I 15／2跃迁所引起的1．54μm波段的发射强度比Er^3 单掺杂的氟铝酸盐玻璃中的荧光强度要强。在Er^3 离子掺杂浓度高于10mol％的情况下，由于Er^3 与Yb^3 之间的反能量转移过程，Er^3 ／Yb^3 共掺杂的氟铝酸盐玻璃的1．54μm波段的荧光浓度淬灭效应比Er^3 离子单掺杂的情况下明显。在Er^3 离子掺杂浓度小于10mol％的情况下，实验中发现可获得1．54μm波段高发射效率的Er^3 与Yb^3 离子最佳摩尔浓度掺杂比例约为1：1。     

纳米Eu0.10Y1.90-xNdxO3-δ的光致发光特性及浓度猝灭研究

使用超声波作用下的均匀沉淀法,制备了Eu0.10Y1.90-xNdxO3-δ纳米晶荧光粉,用X射线粉末衍射、荧光光谱等对其进行表征.研究了掺杂Nd3 离子对Y2O3∶Eu3 晶格常数、晶粒尺寸及室温光致发光特性的影响.由不同掺杂浓度x=0~0.18下样品的发射光谱强度变化曲线得到猝灭浓度值,探讨了掺杂Nd3 的样品荧光浓度猝灭的机理.发光强度与浓度的关系表明,掺杂离子之间存在的Eu3 -Nd3 或Nd3 -Nd3 间交换相互作用,是导致掺杂样品浓度猝灭的主要原因.     

四方相LaVO_4：Ln（Ln=Nd/Er）近红外发光纳米材料的水热合成

本文通过EDTA辅助的水热法合成了四方相稀土矾酸盐一维纳米材料,并通过Nd3＋或Er3＋掺杂使其具有近红外发光性质.与利用柠檬酸根作为配体合成得到的单斜相纳米晶相比,四方相矾酸盐具有更高的发光强度.通过对反应条件的改变,分别考察了EDTA-稀土离子投料比和掺杂离子浓度对产物形貌及发光性质的影响,发现在纳米尺度下,稀土离子具有更高的猝灭浓度.     

Sm~(3 )在硼酸盐玻璃中的发光及Bi~(3 )对Sm~(3 )的敏化作用

早在六十年代,人们为了寻找较好的激光玻璃,曾对Sm~(3 )离子掺杂的玻璃中的光谱进行过研究。为了探寻新型的激光,发光玻璃,又进一步研究了Sm~(3 )在玻璃中的发光和敏化。我们以寻找一种高亮度,低成本的发光玻璃为目的,研究了基质玻璃组成,敏化离子及其浓度对Sm~(3 )发光性质的影响。 选择B_2O_3-BaO-M_mO_n(M_mO_n=Li_2O,Na_2O,K_2O,MgO,CaO,SrO)玻璃体系,所用原料的纯度皆为分析纯以上,用陶瓷坩埚在1250℃掺杂氧化钐(纯度均大于99％),玻璃的荧光谱和激发光谱,用MPF-4型荧光分光光度计测定。     

Tm3+/Yb3+掺杂亚碲酸盐玻璃蓝红光上转换的研究

研究了掺Tm^3 /Yb^3 亚碲酸盐玻璃室温下的上转换发光。用970nm波长的半导体激光器作为泵浦源，得到了高效率的480nm波长上转换的荧光，通过对不同掺杂浓度样品的发光比较，发现了这种玻璃上转换发光的浓度猝灭现象，找出了这种玻璃得到高效率上转换发光的适宜浓度，并对Tm^3 的浓度猝灭现象进行了分析，通过对上转换发光强度与泵浦强度关系曲线的拟合，看到这种上转换是三光子吸收过程，这与通过能级图分析得到的结果相同，另外，也对650nm波长的转换发光进行了研究。     

Die Kristallstruktur des W3CoB3 und der dazu isotypen Phasen Mo3CoB3, Mo3NiB3 und W3NiB3

Zusammenfassung Mo₃CoB₃, Mo₃NiB₃, W₃CoB₃ und W₃NiB₃ kristallisieren in einem eigenen Typ (W₃CoB₃-Struktur). Das trigonal prismatische Bauelement [T ₆B]^* ist zu Ketten vereinigt, wobei B₃-Gruppen entstehen. Die Phasen sind vermutlich Bor-reicher als obiger Formel entspricht.

---

The crystal structure of W₃CoB₃ and the isotypic phases Mo₃CoB₃, Mo₃NiB₃, and W₃NiB₃

Mo₃CoB₃, Mo₃NiB₃, W₃CoB₃, and W₃NiB₃ were found to possess a new type of crystal structure (W₃CoB₃-structure type). Trigonal prismatic groups [T ₆B]^* are linked together forming chains in such a way that B₃-groups occur. These borides do probably exist with a larger amount of boron as to compared with the formula.

---

---

Mit 2 Abbildungen     

Synthesis of γγγ-trifluorocarbonyl compounds

γγγ-Trifluorocarbonyl compounds are easily obtained in a good yield by introduction of the 1,1,1-trifluoroethyl moiety (CF₃-CH₂-) on the -methylene group of a ketone.     

γ-Nitro-γ-butyrolacton

γ-Nitro-γ-butyrolactone By oxidation of 3-(1-nitro-2-oxocyclohexyl)propanal ( 1 ) with KMnO₄, besides 3-(1′-nitro-2′-oxocyclohexyl)pripionic acid ( 2 ), the complete hydrolysis product 4-oxononanedioic acid ( 4 ) and the oxidized semi-hydrolysis product 5-(2-nitro-5-oxotetrahydro-2-furyl)pentanoic acid ( 3 ) were formed. The crystalline 3 decomposes at r.t. forming 4 and nitrous gases; its structure was established by X-ray determination.     

Freezing the polarization of CH3NH3PbI3 and CH3NH3PbI3-xClx perovskite films

Thin films of methylammonium lead halides, CH₃NH₃PbI₃ and CH₃NH₃PbI_3-xCl_x, were deposited onto symmetrical microstructured electrode arrays of gold or platinum on Si/SiO₂ wafers. Polarization studies were carried out on perovskite films under vacuum in the dark. For poling, a constant voltage was applied to the samples while the temperature was cycled between 295 K and 4 K. The measured current densities depending on the temperature showed distinct characteristics relating strongly to the crystal phase and the dielectric properties of the perovskite films. Voltage sweeps were carried out at different scan rates at specific temperature intervals after poling. The polarization of the films due to the migration of iodide vacancies in direction of the blocking perovskite/metal interface was frozen almost up to room temperature. Charge carriers were only able to cross the blocking barrier and contribute to the current where the ions have accumulated during poling. All J-V curves showed hysteresis: inverted and regular hysteresis at room temperature and below, respectively. Inverted hysteresis originates from the slow accumulation of ions at the blocking barrier, while regular hysteresis arises from a distortion in the adjacent crystals which will be discussed.     

K3BiSe3, Rb3BiSe3 und Cs3BiSe3 – Substitutionsvarianten des Th3P4-Typs

K₃BiSe₃, Rb₃BiSe₃, and Cs₃BiSe₃ – Derivatives of the Th₃P₄ Structure Type The compounds K₃BiSe₃, Rb₃BiSe₃, and Cs₃BiSe₃ were synthesized by heating mixtures of Bi₂O₃ and the respective alkalicarbonate in a stream of hydrogen saturated by selenium at 850°C. Thin crystals of the compounds appear red in transmitted light. They crystallize isostructural with Na₃AsS₃, space group P2₁3, lattice constants a = 9.771(5) Å, a = 10.161(3) Å, and a = 10.587(5) Å for K₃BiSe₃, Rb₃BiSe₃, and Cs₃BiSe₃, respectively. The Na₃AsS₃ structure type is a derivative of the Th₃P₄ structure type.     

3x-pyrrolizin-3-ones

Condensation of pyrrole-2-dithiocarboxylates with CH acids containing ester groups, in the KOH-DMSO system, was used to prepare previously unknown 1-alkylthio-3H pyrrolizin-3-ones. The latter, treated with secondary amines, are readily converted to the corresponding 1-amino derivatives.     

3-H-pyrrolizin-3-ones

Previously unknown 1-alkylthio-3H-pyrrolizin-3-ones have been obtained by the condensation of pyrrole-2-dithiocarboxylates with CH acids containing ester groupings in the KOH-DMSO system. On treating the products with secondary amines they are readily converted into the corresponding 1-amino derivatives.Irkutsk Branch of the Russian Academy of Sciences, Irkutsk 664033. Translated from Khimiya Geterotsiklicheskikh Soedinenii, No. 7, pp. 919–924, July, 1996. Original article submitted May 2, 1996.     

Die Akzeptoreigenschaften von AsCl3, AsBr3, asJ3, SbCl3, SbBr3 und SbJ3

Zusammenfassung Es wurden die Enthalpien der Reaktionen von AsCl₃, AsBr₃, AsJ₃, SbCl₃, SbBr₃ und SbJ₃ mit Tributylphosphat, N,N-Dimethylacetamid und Hexamethylphosphorsäuretriamid bestimmt. Das Verhalten der Addukte bei Gegenwart eines Überschusses der Donoren wird beschrieben.

---

Acceptor properties of AsCl₃, AsBr₃, AsI₃, SbCl₃, SbBr₃, and SbI₃

The enthalpies of the reactions of AsCl₃, AsBr₃, AsI₃, SbCl₃, SbBr₃ and SbI₃ with tributylphosphate, N,N-dimethylacetamide and hexamethylphosphoric acid triamide were measured. The behavior of the adducts in the presence of excess donor molecules is described.

---

---

Mit 5 Abbildungen