Y2O2S：Eu^3＋红色荧光粉的SnO2：Sb包覆研究

采用硫融法合成了Y2O2S：Eu^3＋红色荧光粉。用溶胶-凝胶法在其表面包覆了一层SnO2：Sb透明导电薄膜。通过x射线衍射（XRD）、透射电镜（TEM）、荧光光谱（PL）和电阻测量等检测手段分别分析了包覆处理对Y2O2S：Eu^3＋的晶体结构、表面形貌、荧光性质以及荧光粉导电性的影响。结果表明：通过该方法成功地在Y2O2S：Eu^3＋表面包覆了一层连续的SnO2：Sb薄膜;当包覆量nSoO2/nY2O2S=6％时,所得到的荧光粉同时具有较高的荧光强度和导电性;当掺杂量DSb/nSn=10％,退火温度为500℃（氧气流中退火1h）时,可以得到导电性较好的荧光粉。     

不同沉淀剂下掺杂离子的Y2O3：Eu^3＋粉体的光致发光研究

不同沉淀剂下采用均相沉淀法制备出掺杂不同金属离子（K^＋，Mg^2＋，Ba^2＋）的Y2O3：Eu^3＋荧光粉。通过XRD、IR、激发与发射等技术研究了材料的结构与发光性能，考察了沉淀剂、掺杂的金属离子种类对Y2O3：Eu^3＋发光材料的结构和发光性能的影响。结果表明：用尿素作沉淀剂制备的发光性能明显强于用草酸作沉淀剂的Y2O3：Eu^3＋荧光粉。其中，在草酸系列中，同时掺杂K^＋离子能显著增强Y2O3：Eu^3＋的发光强度，而掺杂Mg^2＋，Ba^2＋离子则会减弱其发光强度；而在尿素系列里，掺杂离子都会增强样品的发光强度。     

Ce3+共掺杂对Y2O3:Eu3+荧光粉的发光性能和颗粒形貌的影响

采用化学反应与高温固相反应相结合的方法制备了Ce3和Eu3+共掺杂Y2O3荧光粉,利用X射线衍射和扫描电镜分析,发现Ce3+离子共掺杂对Y2O3:Eu3+荧光粉的颗粒形貌有显著的影响,随着Ce3+离子浓度的改变,形貌可从球型转变为管状.荧光光谱分析表明,所制备的共掺杂荧光粉主要发射位于614纳米的红光峰和位于587纳米...     

杂质离子对Y2O3:Eu3+发光性能的影响

研究了碱金属及碱土金属离子掺杂的荧光体Y2O3:Eu^3 0.05,A^ 0.02(A=Li,Na,K)和Y2O3:Eu^3 0.05,B^2 0.02(B=Mg,Ca,Sr,Ba)的荧光，余辉发光及热释光特性，余辉光谱数据表明：杂质离子掺杂的荧光体Y2O3:Eu^3 的余辉发射主峰与未掺杂荧光体Y23:Eu^3 的荧光发射主峰（611nm)一致，为经典Eu^3 的^5D0-^7F2电偶极跃迁，杂质离子的引入明显地延缓了Y2O3:Eu^3 的余辉衰减，其中Y2O3：Eu^3 ,A^ (A=Li,Na,K)的余辉衰减趋势几乎完全一致，而Y2O3：Eu^3 ,B^2 ,B2^ (B Mg,Ca,Sr,Ba）的余辉衰减趋势由慢到快依次为Ca,Sr,Ba,Mg。热释光谱数据显示，杂质离子的掺杂导致基质中电子陷阱能级的生成，这是导致余辉衰减减慢的直接原因。Y2O3：Eu^3 ,A^ 的热释峰都位于175℃左右，相应电子陷阱能级深度为0.966eV左右，而Y2O3：Eu^3 的热释峰由高到低分别位于192℃（Ca),164℃（Sr),135℃（Ba),118℃(Mg)，电子陷阱能级深度分别为1.003eV(Ca),0.942eV（Sr),0.880eV(Ba),0.843eV(Mg)。结合余辉衰减数据，可以看到，Y2O3:Eu^3 ，A^ 和Y2O3：Eu^3 ,B^2 的热释光谱与相应荧光体的余辉衰减趋势吻合得十分好，由此可以得出，一定相同的条件下，热释峰值温度越高，杂质陷阱能级越深，相应荧光体的余辉衰减越慢。     

EU:Y2O3纳米晶的光谱特性与微结构

采用均相共沉淀法制备了不同粒径的Y2O3：Eu^3＋和Y2O3粉体材料,根据红外光谱和荧光光谱,探讨了纳米Y2O3：Eu^3＋粉体的微观结构与同质体微米材料相对变化.发现纳米粉体的Y（Eu）-O键吸收峰校正高度和面积随着颗粒的减小而减小,而对于同质微米材料却相反.分析认为：Y（Eu）-O键红外吸收峰校正高度和面积由Y（Eu）-O键的平均键长和Y（Eu）-O键振动态的数目两个因素决定,对于微米粉Y（Eu）-O键长起主要作用.由于纳米粉体的比表面积随粒径的减少呈指数的增加,不饱和键和悬空键的数目随粒径减小而指数增加,Y（Eu）-O键振动态的数目起主要作用.计算了纳米粉体相对微米粉的跃迁强度参量Ωt/Ωt＇值,发现Ω2和Ω4均增加,说明粉粒内部跃迁几率增加.纳米荧光粉比微米粉荧光强度减少的实验事实应是纳米粉粒表面效应引起的,与红外光谱实验的结果相符.     

超细Y2O3∶Eu荧光粉的制备及其阴极射线发光研究

介绍了尿素 溶胶法制备粒径为 10 0～ 2 0 0nm的超细Y2 O3 ∶Eu荧光粉的实验。对荧光粉的粒径和形貌进行了SEM分析 ,测量和分析了荧光粉的XRD谱图以及微观晶体结构 ,测量了 8kV电压下荧光粉的阴极射线发光的光谱和亮度 ,并与商品微米Y2 O3 ∶Eu荧光粉进行了比较。对实验结果进行了讨论     

钒硼酸钇铕荧光粉的真空紫外光谱特性研究

采用高温固相法合成了YBχV1-χO4-χ：Eu^3＋荧光粉,利用XRD变温发射光谱以及真空紫外激发的光谱对其进行研究。结果表明,在147nm的真空紫外光激发下,荧光粉的发射主峰位于619nm,与（Y,Gd）BO3：Eu^3＋相比,色纯度较好,发光亮度达86％,是彩色PDP用红色荧光粉的候选材料。     

超细Y2O3：Eu荧光粉的制备及其阴极射线发光研究

介绍了尿素-溶胶法制备粒径为100-200nm的超细Y2O3:Eu荧光粉的实验。对荧光粉的粒径和形貌进行了SEM分析，测量和分析了荧光粉的XRD谱图以及微观晶体结构，测量了8kV电压下荧光粉的阴极射线发光的光谱和亮度，并与商品微米Y2O3:Eu荧光粉进行了比较。对实验结果进行了讨论。     

喷雾热解法合成球形（Y,Gd）BO3：Eu荧光粉

采用改进的喷雾热解法合成了发光性能优异的（Y，Gd）BO3：Eu红色荧光粉，通过调节前驱体溶液的性质改善了荧光粉产物的形貌特征以提高其物理和光学性能。结果表明，在前驱体溶液中加入氨水能够影响喷雾热解过程中液滴中颗粒生成方式，以控制产物颗粒形貌，经后续热处理后获得了无团聚的致密球形荧光粉颗粒：由X射线衍射分析可知，在1100℃下后续热处理3h可以获得结晶良好的所需纯相物质。同时也考察了激活剂浓度对（Y，Gd）BO3：Eu荧光粉体发光强度的影响；在优化的掺杂浓度下，采用氨水改性的前驱体溶液经过喷雾热解,热处理后获得荧光粉产物具有优良的发光强度。     

白光LED用荧光粉α-Sr2P2O7∶Eu^3＋的制备及其发光性能

以尿素为原料,采用溶液燃烧法合成出α-Sr2P2O7∶Eu^3＋红色荧光粉。利用XRD、FSEM和荧光光谱,研究了激活剂Eu3＋浓度、煅烧温度对荧光粉的晶体结构和发光性能的影响。光谱测量表明α-Sr2P2O7∶Eu^3＋的5 D0→7F1、5 D0→7F2跃迁发射最强,为红光发射;该荧光粉可被394nm近紫外光和464nm蓝光有效激发,有望成为一种近紫外LED和蓝光LED用的红色荧光粉。     

Photostriction of CH3NH3PbBr3 Perovskite Crystals

Organic–inorganic hybrid perovskite materials exhibit a variety of physical properties. Pronounced coupling between phonon, organic cations, and the inorganic framework suggest that these materials exhibit strong light–matter interactions. The photoinduced strain of CH₃NH₃PbBr₃ is investigated using high‐resolution and contactless in situ Raman spectroscopy. Under illumination, the material exhibits large blue shifts in its Raman spectra that indicate significant structural deformations (i.e., photostriction). From these shifts, the photostrictive coefficient of CH₃NH₃PbBr₃ is calculated as 2.08 × 10^?8 m² W^?1 at room temperature under visible light illumination. The significant photostriction of CH₃NH₃PbBr₃ is attributed to a combination of the photovoltaic effect and translational symmetry loss of the molecular configuration via strong translation–rotation coupling. Unlike CH₃NH₃PbI₃, it is noted that the photostriction of CH₃NH₃PbBr₃ is extremely stable, demonstrating no signs of optical decay for at least 30 d. These results suggest the potential of CH₃NH₃PbBr₃ for applications in next‐generation optical micro‐electromechanical devices.     

Constitution of the Ni3Cr-Ni3Al-Ni3W system

Isothermal sections of the Ni-Cr-Al-W system have been investigated at 75 at % Ni and temperatures of 1523 and 1273 K, by means of phase compositional analysis, X-ray diffraction and microscopical examination. The alloys studied lay in the range 2.5 to 10 at % Cr, 12.5 to 20 at% Al, 2.5 to 6.25 at % W, The phases formed were, and the bcc solid solution based on tungsten (designated ₂). The maximum extent of the region was found to be 3 at % each of chromium and tungsten. Preferential partitioning of tungsten to occurred. Study of an Ni-10Cr-12.5Al-2.5W alloy aged at 1273 and 1073 K, after quenching from 1573 K, showed that changes in and compositions and lattice parameters occur as a function of ageing time.     

Crystal structure of Tl3AsSe3

The structure of Tl₃AsSe₃, which has been solved by the single-crystal x-ray method, is rhombohedral, with space group R3m and cell parameters $\text{a}\text{= 9.870(2)}\text{A}\text{?}\text{, c}\text{= 7.094(3)}\text{A}\text{?}\text{, z}\text{= 3}$. A full-matrix least-squares refinement gives weighted R = 0.058. The Se atoms form equilateral triangles around Tl at 3.178Å and around As at 2.207Å. The structure may be described in terms of units formed from three TlSe₃ triangles by corner-sharing. These units share corners to produce a helical arrangement along the c axis. The triangles of AsSe₃ are isolated from each other.     

3 Cr3 Mo3 VNb 在热冲孔中的应用研究

高合金钢热冲孔冲头寿命关系到模具与产品成本、生产效率、自动化设备的使用,因此,应注重冲头的选材、材料制备与冲头制造工艺。 用 3 Cr3Mo3 VNb 作为高合金钢热冲孔冲头,为提高模具寿命,在材料制备上,优化了成分,采用电渣重熔冶炼,减少杂质,毛坯锻造两次,用大锻造比锻造,冲头热处理用真空炉,三次回火,热处理硬度取 HRC42 ~ 46 ,冲头表面处理采用镀铬工艺,开展了热冲孔工艺试验。 结果表明,用3 Cr3Mo3 VNb 可使冲孔冲头寿命平均达到 800 件以上。     

Multicolor up-conversion emissions of Tm3+/Er3+/Yb3+ tri-doped YF3 phosphors

Tm3+/Er3+/Yb3+ tri-doped yttrium fluoride (YF3) phosphors were prepared by a facile hydrothermal method. X-ray topographic analysis found that the phosphors were crystallized products. Their sizes and morphologies were characterized by scanning electron microscopy (SEM, Hitachi S-4800), which indicated that most of the YF3 phosphors were hundreds of nanometers in size. Up-conversion (UC) spectra were recorded under 980-nm diode laser excitation at room temperature with a fluorescence spectrometer (Hitachi F-4500). Plenty of UC emissions of Tm3+ and Er3+ were observed from ultraviolet to red. For Tm3+ ions, a five-photon process (approximately 291 nm and approximately 347 nm), a four-photon process (approximately 362 nm and approximately 452 nm), and a three-photon process (approximately 475 nm) were identified in the UC spectra. The UC emissions from the Er3+ were: approximately 380 nm, approximately 408 nm, approximately 521 nm, approximately 537 nm, and approximately 652 nm. Therefore, cyan-white light can be observed by the naked eye at 980-nm excitation, even under low excitation power density. By comparing the UC spectra of the phosphors annealed at different temperatures, we found that the intensity of the UC luminescence increased as annealing temperature increased. Furthermore, the spectral dependencies on Tm3+ doped concentrations were studied. The energy transfer processes and fluorescence dynamics in the tri-doped system are currently being investigated.     

(La2/3Ca1/3)(Mn(3-x)/3)Fex/3)O3体系磁电阻行为的研究

通过系统地测量（La_2/3Ca_1/3）（Mn_{（3-x）／3}Fe_x／3）O₃（x＝0、0.1、0．2、0．3的体系样品的电阻率-温度关系以及一定温度下磁电阻率与磁场的关系,发现随x的变化其磁电阻率峰和电阻率峰均发生位移,磁电阻率峰值增大,并伴生磁电阻率峰展宽效应．作者认为由于Fe的替代,引起体系中Mn³⁺／Mn⁴⁺比率及磁矩的变化,加之外场对磁有序结构的调制作用,从而影响了Mn³⁺－O^－Mn⁴⁺的双交换作用,最终导致磁电阻行为发生变化．     

The Ni3Al-Ni3Cr-Ni3Ru section of the Ni-Cr-Al-Ru system

An investigation is reported of the 75 at% nickel section of the Ni-Cr-Al-Ru system at 1523 and 1273 K. Constitutional data obtained by electron probe microanalysis, X-ray diffraction and microscopical examination are presented as partial isothermal sections. At 1523 K, the major part of the section consists of phase, while the aluminium-rich region contains a and+ region; the extent of the solid solution of chromium and ruthenium in totals ~ 4 at%. The ruthenium-rich corner of the section shows a two-phase region consisting of + ruthenium-rich solid solution. At 1273 K the,+ and + ruthenium regions increase in extent. The/ mismatch values in the equilibrated alloys studied lie in the range ~ –0.08 to –0.39%. Constitutional features of as-cast alloys are also reported.     

The Ni3Al-Ni3Cr-Ni3Mo section of the Ni-Cr-Al-Mo system

An investigation is reported of the constitution of the 75 at % nickel section of the Ni-Cr-Al-Mo system in the temperature range 1523 to 1073 K. Alloys in the region 10 to 20 at % Al were annealed at 1523, 1273, and 1073 K, respectively, and subjected to electron microprobe analysis, X-ray diffraction, and microscopical and hardness examination. Constitutional data are presented as partial isothermal sections and as vertical sections. At 1523 K the section consists only of fields containing ,+ and , the last mentioned phase being predominant. With decreasing temperature the and + fields increase in extent. Also, the NiMo and Ni₃Mo phases were encountered in the ternary Ni-Al-Mo alloy studied. The quaternary + alloys showed small lattice mismatch values, i.e. up to 0.25%. Raft like morphologies of were found in the quaternary alloys, resulting from directional coarsening. Observations of as-cast structures are also reported.