煅烧温度对红色长余辉发光材料Sr_3Al_2O_6:Eu~(2+),Dy~(3+)性能的影响

采用溶胶凝胶法合成了Sr3Al2O6:Eu2+,Dy3+长余辉发光材料,利用X射线衍射仪(XRD)对材料的物相进行了分析,采用荧光分光光度计、照度计测定了样品的发光特性。XRD结果表明:随着煅烧温度的升高,SrCO3杂相的衍射峰越来越弱,Sr3Al2O6相的衍射峰越来越强,1200℃时发光基质为纯的Sr3Al2O6相,1250℃时出现新的SrAl2O4杂相。激发光谱和发射光谱结果表明:长余辉发光材料的激发峰位于473nm,发射峰位于612nm,归属于Eu2+的4f65d1→4f7特征发光。温度升至1250℃时,Eu2+的发射峰为612nm和520nm,后者归属于Eu2+在发光基质SrAl2O4中的发光。综合分析得制备Sr3Al2O6:Eu2+,Dy3+发光材料合适的煅烧温度为1200℃,在此温度下,材料具有较好的初始亮度和余辉时间。     

SrBPO_5:Eu~(2+),Mn~(2+)的高温合成及其发光特性

运用高温合成的方法合成SrBPO5:Eu2+,Mn2+,用X射线衍射仪(XRD)、红外光谱仪(IR),以及荧光光度计(PL)对合成产物的结构和发光性质进行了研究。XRD测试结果表明,在1000℃下烧结6h得到SrBPO5单相。发光光谱测试表明,在350nm紫外线激发下,宽带发射最强峰位于400nm和498nm处,当Mn2+含量进一步增加时,发射光颜色从蓝色向蓝白色移动,测试结果说明SrBPO5:Eu2+,Mn2+有希望应用于白色LED方向。     

共沉淀法合成CaO:Eu~(3+)红色荧光粉的研究

采用共沉淀法合成CaO:Eu3+红色荧光粉,探讨了Eu3+离子的掺杂量、煅烧温度和煅烧时间对样品发光性能的影响,并利用X-射线衍射仪(XRD)、扫描电镜(SEM)和荧光光度仪(PL-PLE)等仪器对样品的性能进行表征.结果表明:掺杂Eu3+作为发光中心进入到CaO基质的晶格中,其最佳掺杂量为1.5%(摩尔含量);最佳煅烧温度和煅烧时间分别为1100℃和4h,样品的激发峰位于200~290nm之间,对应于Eu3+-O2-的电荷迁移跃迁(CTB),属于宽带激发;Eu3+离子主要占据严格对称的格位,其最大发射峰位于592nm,对应于5D0→7F1磁偶极跃迁,属于红色发光.     

水热-均匀沉淀法制备亚微米长余辉发光材料SrAl_2O_4∶Eu,Dy

采用水热-均匀沉淀法,以尿素为沉淀剂,在聚四氟乙烯低温反应釜中160℃水热,在较低的煅烧温度下制备了亚微米级长余辉发光材料Sr0.97Al2O4∶Eu0.01,Dy0.02。XRD结果表明,在1000℃煅烧4h能得到单相的SrAl2O4∶Eu,Dy,SEM测试显示SrAl2O4∶Eu2+,Dy3+发光材料为球状形貌,粒径大小约为200～500nm,激发和发射光谱结果表明,随着煅烧温度升高,SrAl2O4∶Eu2+,Dy3+的发光强度也随之增强,其激发光谱峰值位于360nm,发射光谱峰值位于513nm,SrAl2O4∶Eu2+,Dy3+在1100℃煅烧后的余辉衰减时间比1000℃煅烧后显著提高,其热释光谱峰值在80～90℃。     

白光LED用MSrAl3O7:Eu2+(M=Y,La,Gd)绿色发光材料合成及其光学性能

采用传统的高温固相合成技术制备出一系列组成为MSrAl3O7:Eu2+(M=Y,La,Gd)的新型绿色发射荧光体.通过X射线衍射(XRD)研究其晶体结构发现:MSrAl3O7:Eu2+系列荧光体属于M2O3-SrO-Al2O3赝三元体系的稳定结晶相.荧光光谱测试表明:MSrAl3O7:Eu3+(M=Y、La、Gd)材料均是优良的白光LED用绿色荧光体,可被近紫外(300～450nm)有效激发,产生较强的绿色发射光,发射主峰位于517nm左右,样品的紫外-可见(UV-vis)光谱进一步证实了其有效吸收近紫外光的特征.研究还发现,在MSrAl3O7:Eu2+(M=Y、La、Gd)系列荧光体中,LaSrAl3O7:Eu2+具有最强的绿色发射光,进一步地比较不同温度下LaSrAl3O7:Eu2+材料的结构与光谱特性表明,1400℃合成的样品具有稳定的结构和最佳的发光性能.     

Mn2+在Mg2SnO4中的绿色长余辉发光性能研究

利用高温固相法合成了Mg2SnO4:Mn2+绿色发射长余辉发光材料,对样品进行了X射线衍射分析、荧光光谱分析、色坐标、热释发光以及发光寿命测量.分析结果表明,在1250℃下烧结6 h的Mg2SnO4为单相产物,所得Mg2SnO4:Mn2+发光材料具有良好的发光性能,在270nm紫外线激发下发出最强发射位于498nm的宽...     

红色荧光粉BaZn2(PO4)2:Eu3+的制备及其光谱特性

采用高温固相法制备了BaZn2(PO4)2:Eu3+红色荧光材料.测量了BaZn2(PO4)2:Eu3+材料的激发与发射光谱,激发峰位于360-400nm之间,发射光谱主峰位于595nm处.研究了BaZn2(PO4)2:Eu3+材料在595nm的主发射峰强度随Eu3+浓度的变化,发射峰强度先随Eu3+浓度的增加而增大;...     

白光LED用新型红色荧光粉Sr5(B03)3Cl:Eu3+的制备与发光特性EI北大核心CSCD

采用高温固相法合成了Sr5 (BO3)3Cl:Eu3+新型红色发光材料,并对其结构和发光特性进行了研究.X射线衍射测试表明合成材料为纯相Sr5 (BO3)3Cl晶体.材料的主发射峰位于587,596,613nm和626nm,对应Eu3+的5 D0 →7F1,7F2辐射跃迁.监测626nm发射峰,激发光谱主峰位于392nm,可被InGaN管芯有效激发.通过时间分辨光谱测得Eu3+离子5 D0能级的荧光寿命约为2.28ms.研究了Eu3+离子掺杂浓度对Sr5(BO3)3Cl:Eu3+发光性能的影响,结果随着Eu3+离子浓度的增大,样品的发光强度先增大后减小,最佳掺杂浓度为16％(摩尔分数).计算了Eu3+离子浓度猝灭的临界距离为1.46nm.测量了不同Eu3+浓度样品的色坐标,均位于色品图红光区,符合NTSC标准.     

Eu~(2+),Mn~(2+)在CaZn_2(PO_4)_2中的发光及Eu~(2+)→Mn~(2+)能量传递

Mn2+作为激活剂加入一些基质中,发光比较弱。因此常常选择使用合适的敏化剂来提高Mn2+的发光效率,本文的研究目就是验证Eu2+是Mn2+的良好的敏化剂。采用高温固相法合成了Eu2+,Mn2+掺杂激活的CaZn2(PO4)2荧光粉,并对其发光性质进行了研究。单掺杂Eu2+时呈现发射峰位于504nm的带谱,属于Eu2+离子的5d-4f能级跃迁辐射,激发峰位于380nm,属于Eu2+的f-d跃迁特征激发谱带。单掺Mn2+时CaZn2(PO4)2不发光。当Eu2+和Mn2+共掺时,出现Mn2+的673nm发射峰,样品发红光,表明Eu2+对Mn2+的发光有很强的敏化作用。研究了Eu2+和Mn2+掺杂浓度对激发光谱和发射光谱的影响,证明在CaZn2(PO4)2:Eu2+,Mn2+中Eu2+对Mn2+的能量传递属于共振能量传递。     

钬掺杂对SrAl_2O_4∶Eu~(2+),Dy~(3+)发光性能的影响

首次研究了Ho3+掺杂对SrAl2O4∶Eu2+,Dy3+发光性能的影响。采用燃烧合成方法,在600℃条件下,合成Ho3+掺杂的SrAl2O4∶Eu2+,Dy3+新型长余辉光致发光材料。X射线衍射分析结果表明,合成的样品为单相SrAl2O4单斜晶系磷石英结构。光致发光光谱测量显示,合成样品的发射光谱是连续宽带谱,峰值位于510nm左右,激发光谱是单峰且峰值位于356nm的连续宽带谱。利用单光子计数系统测量了材料的余辉衰减曲线,结果显示Ho3+的适量掺杂可以明显提高铝酸锶的初始发光亮度。当Ho3+的掺入摩尔比例为0.005时,初始亮度是不掺杂Ho3+时的两倍多。对初始亮度增强的机理做了初步的探讨。     

VLE data for CO2-CF2Cl2, N2-CO2, N2-CF2Cl2 and N2-CO2-CF2Cl

Knowledge about vapour-liquid (VLE) is required as a basis of reliable calculations for separation processes. Correlations available for the prediction of T, p, x, y data are less accurate for mixtures at high pressures and mixtures containing supercritical components. The results of VLE experiments are reported and compared with data calculated with equations of state.     

Preparation of ZrO2-CeO2 and HfO2-CeO2 nanopowders

We prepared weakly agglomerated powders of ZrO₂-CeO₂ and HfO₂-CeO₂ solid solutions 5–8 nm in particle size, consisting of monoclinic and tetragonal phases. After heat treatment at 1200°C, the crystallite size was 30 and 14 nm, respectively. We also examined the effect of precipitate freeze drying on the crystallization of hafnia-based solid solutions containing up to 20 mol % CeO₂.     

Thermal diffusion in binary mixtures H2-CCl2F2 and H2-CHClF2

Thermal diffusion coefficients were measured in two gaseous mixtures, in which one component was close to the critical temperature, in the pressure range (19.6–127.4)·10⁴ N/m² and at a freon concentration of 0.25–0.8.     

Comparison of the Electronic Structures of La2CuO4, Sr2CuO2Cl2, and Sr2CuO2F2

First-principles cluster calculations are reported of the local electronic structure of the three compounds: La₂CuO₄, Sr₂CuO₂Cl₂, and Sr₂CuO₂F₂. The copper ${\text{3d}}_{x^2 - y^2 } $ and the planar oxygen 2p _σ atomic orbitals exhibit a similar degree of covalency. The out-of-plane orbitals, however, are quite different with the ${\text{3}}d_{3z^2 - r^2 } $ atomic orbital lowered significantly in energy for chlorine and fluorine apical positions.     

Radial GRIN glasses in Li2O-Na2O-Al2O3-TiO2-SiO2 systems

A series of GRIN glass rods have been developed in Li2O-Na2O-Al2O3-TiO2-SiO2 systems. Negative radial refractive index profiles were generated by exchanging Na+ for Li+ ions in these glass rods. It has been observed that TiO2 plays a vital role in increase in the profile depth and maximum change in the refractive index because of its ambivalent nature. Change in the refractive index can be further increased by increasing the concentration of exchanging cation in the base glass.     

Thermoelectric power of single-phase samples of Tl2CaBa2Cu2O y and Ba2CaSr2Cu2O y

Single-phase 2122 samples of thallium and bismuth superconductors were made by the precursor matrix method. The thermopower of these samples was measured in the temperature range 250 K-T _c . The thermopower was positive and decreased linearly with increasing temperature aboveT _c (onset). The exponential enhancement of thermopower seen in the undoped and doped YBCO was not observed in these samples. The linear variation of thermopower can be explained on the basis of either a two-band model or a narrow band model.     

Si_2N_2O-Al_2O_3-La_2O_3和Si_2N_2O-Al_2O_3-CaO系统的亚固相关系

本文给出了 Si_2N_2O-Al_2O_3-La_2O_3和 Si_2N_2O-Al_2O_3-CaO 系统的亚固相图。实验结果表明:在 Si_2N_2O-Al_2O_3-CaO 系统中有一个未知结构的新化合物 CaO·Si_2N_2O,在3CaO·Si_2N_2O 和3CaO·Al_2O_3两化合物之间形成连续立方固溶体。而 Si_2N_2O-Al_2O_3-La_2O_3系统中则没有发现新化合物。在两个系统的富 Si_2N_2O区,过量的 Si_2N_2O 与 La_2O_3和 CaO 分别反应形成 Si_3N_4与 La_(10)[SiO_4]_(?)N_2(H-相)(和 CaSiO_3。所研究的这两个三元系统中,分别形成了如下几个四元相容性区。在 Si_2N_2O-Al_2O_3-La_2O_3系统内有:H-Si_3N_4-La_2O_3·Si_2N_2O-La_2O_3·Al_2O_3;H-Si_3N_4-La_2O_3·Al_2O_3-La_2O_3·11 Al_2O_3;H-Si_3N_4-La_2O_3·11 Al_2O_3-Al_2O_3;H-Si_3N_4-Al_2O_3-O′s.s;H-Si_3N_4-O′s.s-Si_2N_2O在 Si_2N_2O-Al_2O_3-CaO 系统内有:Si_3N_4-CaSiO_3-CaO·Si_2N_2O-3CaO·Al_2O_3;Si_3N_3-CaSiO_3-3CaO·Al_2O_3-2CaO·Al_2O_3·SiO_(?);Si_(?)N_(?)-CaSiO_3-2CaO·Al_2O_3·SiO_2-Al_2O_3;Si_3N_4-CaSiO_3-Al_2O_(?)-O′s.s;Si_3N_4-CaSiO_3-O′s.s-Si_(?)N_(?)O     

Elastic and Electronic Properties of Superconducting CaPd 2 As 2 and SrPd 2 As 2 vs. Non-superconducting BaPd 2 As 2

The first-principles calculations were performed to predict the elastic and electronic properties of the superconducting ThCr₂Si₂-type phases CaPd₂As₂ and SrPd₂As₂ in comparison with the non-superconducting CeMg₂Si₂-type phase BaPd₂As₂. Besides, the same properties were compared for CeMg₂Si₂- and ThCr₂Si₂-type polymorphs of BaPd₂As₂. We found that all these phases are mechanically stable and belong to soft materials with low hardness. The near-Fermi region is formed by the valence states of the blocks [Pd₂As₂] with decisive contributions of Pd 4d states. The values of N(E _F) increase in the sequence: CaPd₂As₂ < SrPd₂As₂ < BaPd₂As₂, i.e. in the reverse sequence relative to the transition temperatures T _C. Thus, the change in T _C cannot be explained by the electronic factor, i.e. by the simple correlation T _C～N(E _F). Most likely the decrease in T _C in the sequence CaPd₂As₂ → SrPd₂As₂ and the absence of a superconducting transition in BaPd₂As₂ are related to the structural factors and the peculiarities of the electron–phonon coupling mechanism.