Gd3+,Eu3+在介孔Y2O3中的能量传递

通过模板法与溶胶-凝胶法相结合,在温和的条件下制备了介孔Y2O3.再采用水热反应法制得Eu3+、Gd3+单掺杂及Eu3+,Gd3+双掺杂的三种介孔Y2O3组装体(介孔Y2O3∶Eu3+,介孔Y2O3∶Gd3+,介孔Y2O3∶Eu3+,Gd3+).利用广角和小角X射线衍射(XRD)、透射电子显微镜(TEM)对介孔Y2O3进行了表征,结果表明,所制备的介孔Y2O3为立方相,具有六方孔道结构,孔径约10nm.对介孔Y2O3和组装体系进行了荧光光谱(PL)分析,发现在550℃热扩散处理后,介孔Y2O3∶Eu3+的发光存在基质对Eu3+的能量传递,Y2O3∶Eu3+,Gd3+体系中Gd3+对Eu3+也有能量传递作用.     

用溶胶-凝胶法制备Y2O3-SiO2∶Tb3+发光材料

采用溶胶-凝胶法制备了Y2O3-SiO2∶Tb3+发光材料.研究了Tb3+浓度、Y2O3和SiO2配比、烧结温度、烧结时间对发光强度的影响及其发光行为.     

CaO-SiO_2-B_2O_3∶Eu~(3+)、Bi~(3+)玻璃中的敏化发光及其敏化机理的研究

分别研究单掺Eu3+和Bi3+以及共掺Eu3+、Bi3+的CaO-SiO2-B2O3玻璃的发光性质。单掺Eu3+的CaO-SiO2-B2O3玻璃的发射光谱中位于591nm左右的发射峰对应于Eu3+的5D0—7F1跃迁发射,为磁偶极跃迁;位于618nm左右的发射峰对应Eu3+的5D0—7F2跃迁发射,为电偶极跃迁;位于650nm左右的发射峰分别对应于Eu3+的5D0—7F3。当共掺Bi3+、Eu3+时发现少量的Bi3+对Eu3+有明显的敏化作用。研究了Bi3+的最佳浓度和敏化机理,当Bi3+浓度为0.010%(摩尔分数)时Eu3+发光强度最大。Bi3+→Eu3+的能量传递是以光的再吸收能量传递为主。     

复合熔盐法合成Y2O3.Eu3+红色荧光粉

以草酸钇铕(Y2(C2O4)3:Eu3+)为前驱体,采用复合熔盐(NaCl+S+Na2CO3)协助焙烧法合成Y2O3:E.u3+红色荧光粉.利用XRD、SEM、光谱分析等测试和分析荧光粉粒径、颗粒形貌以及发光性能.主要考察复合熔盐配比、用量以及焙烧温度和时间对Y2O3:Eu3+荧光粉发光性能的影响.结果表明,NaCl在...     

静电纺丝技术制备Y2O3∶Eu3+ 纳米纤维

采用静电纺丝技术制备了PVP/[Y(NO3)3+Eu(NO3)3]复合纳米纤维,研究了反应体系的最佳组成,系统地讨论了静电纺丝工艺的影响,获得了最佳制备条件.将PVP/[Y(NO3)3+Eu(NO3)3]复合纳米纤维在900℃焙烧10h,获得了晶态的Y2O3∶Eu3+ 纳米纤维.XRD分析表明,PVP/[Y(NO3)3+Eu(NO3)3]复合纤维为无定型,Y2O3∶Eu3+ 发光纳米纤维属于体心立方晶系,空间群为Ia3.SEM分析表明,PVP/[Y(NO3)3+Eu(NO3)3]复合纳米纤维表面光滑,平均直径约为150nm;Y2O3∶Eu3+ 发光纳米纤维的直径约为50nm.     

用溶胶-凝胶法制备Y_2O_3-SiO_2:Tb~(3+)发光材料

采用溶胶-凝胶法制备了Y2O3-SiO2∶Tb3+发光材料。研究了Tb3+浓度、Y2O3和SiO2配比、烧结温度、烧结时间对发光强度的影响及其发光行为。     

Sr2MgSi2O7:Eu,Nd体系中Eu2+向Nd3+的能量传递

通过高温固相法合成了Sr2 MgSi2O7:Eu2+,Nd3+发光材料,测试了样品的物相结构、可见和近红外激发和发射光谱、荧光寿命等,研究了Eu2+对Nd3+的近红外发光性能的影响及近红外发光相对强度变化的规律,考察了煅烧温度、煅烧时间对近红外发光性能的影响.结果表明,1200℃下煅烧的St2 MgSi2O7:0.02Eu2+,0.01Nd3+样品近红外发光强度最强,Eu2+对Nd3+的近红外发光敏化效果最好.证实了在Sr2 MgSi2O7:Nd3+,Eu2体系中Eu2+通过无辐射传递的模式向Nd3+有效传递了能量.     

水热法制备Y_2O_3:Eu及其发光性能的研究

利用水热法制备立方相Y2O3:Eu红色荧光粉.在不同掺杂浓度、不同溶液pH值的系列样品中,均观测到Eu3+离子的特征发射.荧光强度与Eu3+离子掺杂浓度关系研究表明:在不同掺杂浓度中,Eu3+离子掺杂浓度为9%时其相对发射强度最强.在不同溶液pH值所获得的样品中,以溶液pH等于6制备的样品发光效果最好.此外通过与商用Y2O3:Eu红色荧光粉比较,发现其荧光强度相当.因此,与传统高温固相法相比,水热法合成Y2O3:Eu红色荧光粉是简单易行方案.     

Sr_2MgSi_2O_7∶Eu,Nd体系中Eu~(2+)向Nd~(3+)的能量传递

通过高温固相法合成了Sr2MgSi2O7∶Eu2+,Nd3+发光材料,测试了样品的物相结构、可见和近红外激发和发射光谱、荧光寿命等,研究了Eu2+对Nd3+的近红外发光性能的影响及近红外发光相对强度变化的规律,考察了煅烧温度、煅烧时间对近红外发光性能的影响。结果表明,1200℃下煅烧的Sr2MgSi2O7∶0.02Eu2+,0.01Nd3+样品近红外发光强度最强,Eu2+对Nd3+的近红外发光敏化效果最好。证实了在Sr2MgSi2O7∶Nd3+,Eu2+体系中Eu2+通过无辐射传递的模式向Nd3+有效传递了能量。     

Eu2+、Er3+共掺杂Sr3MgSi3O10高亮度蓝色荧光粉的制备及性质研究

采用凝胶-燃烧法在活性炭弱还原气氛下成功合成了高亮度蓝色发光材料Sr3 MgSi3 O10:Eu2+,Er3+.用X射线粉末衍射仪、荧光分光光度计对样品的物相结构和发光性质进行了分析和表征.结果表明,所合成的Sr3 MgSi3O10:Eu2+,Er3+的晶体结构与Sr2 MgSi2 O7的相似,属四方晶系.样品激发光谱是位于250 nm～450 nm的宽带,最大激发峰位于357 nm处;发射光谱也是一宽带,最强的发射峰位于466 nm处,属于Eu2+典型的4f65d1→4f7跃迁,呈蓝光发射.根据光谱测定结果和Van Uitert经验公式,推断Eu2+进入Sr3 MgSi3 O10基质后占据八配位Sr的格位.研究发现,共掺杂Er3+能有效敏化Sr3 MgSi3 O10基质中Eu2+的发光,当Er3+的掺杂摩尔分数为0.04时,样品发光强度最大,约为单掺Eu2+样品发光强度的3.3倍.     

Vitrification and Crystallization Behavior of CaO-SiO2-MgO-Al2O3-Fe2O3-Cr2O3 System

Metallurgical and Materials Transactions B - The effect of basicity and Cr2O3 content on vitrification of the CaO-MgO-SiO2-Al2O3-Fe2O3-Cr2O3 system during a melt-quenched process and the...     

Viscosity of CaO-SiO2-Al2O3-MgO-B2O3 slags

The viscosity of CaO-SiO₂-Al₂O₃ slags with 8% MgO and 4% B₂O₃ is investigated over a broad range of composition, by means of a simplex-lattice experiment design. For slag of basicity 6–8 in the upper left region of the local simplex, with 15–25% Al₂O₃, 8% MgO, and 4% B₂O₃, the viscosity is high: 9.4–26.4 P over the range 1500–1530°C. Displacement of the slags of basicity 5–8 to the lower region of the local simplex ensures high fluidity in the given range of Al₂O₃ concentration: the viscosity is 1.5–6.1 P over the range 1500–1530°C.     

Gd_2O_3-Yb_2O_3-Y_2O_3-ZrO_2热障涂层材料及涂层性能研究

使用化学共沉淀法合成了纳米Gd2O3-Yb2O3-Y2O3-ZrO（2GYYZO）粉末,并最终制备了超细晶团聚的多元稀土氧化物掺杂的GYYZO热喷涂粉末,系统的研究了材料及涂层的基本性能,重点研究了材料及涂层的高温稳定性,材料和涂层的高温相稳定性相对传统纳米8YSZ材料明显提高,对高温热处理过程中涂层孔隙收缩、晶粒长大...     

Research on Glass Forming Ability of Er2O3 -Al2O3 -B2O3 -SiO2 System

The glass forming range of Er2O3-Al2O3-B2O3-SiO2 system was explored, and the effect of the content of Al2 O3 and Er2 O3 on glass-forming region was experimentally examined. It is shown that the region of glass formation range expends when the content of Al2O3 is changed from 15% to 20%, while it shrinks when the content of Er2O3 is changed from 20% to 30%. At the same time, the glass forming ability of Er2O3-Al2O3-B2O3-SiO2 system was also discussed using a value of β, which is an indication of crystallization tendency of glasses, calculated from thermo-analysis data. It is found that the glass forming ability of Er2O3-Al2O3-B2O3- SiO2 glasses is poor, while the glasses network may be enhanced when Al2O3 is added to the system, the glass forming ability being heightened. In addition, the crystallization temperatures of the rare earth glasses were determined using differential thermal analysis technique. The Er2O3-Al2O;-B2O3-SiO2 glass samples were heat treated at 1000,1100 and 1260℃ respectively. The results show that it is the Er2O3 phase that separates out from the glasses after crystaline heat treatment, and it is tiered up in glasses, as detected through XRD and SEM. This indicates that the phase separation occurs when the glasses are heated, Er3 being mainly distributed in the boron rich phase, then separated out from glasses, while the silicate rich phase remaining glassy state.     

CaO-La2O3-B2O3-Eu2O3转光玻璃的合成及荧光性质

X射线衍射研究表明CaO-La2O3-B2O3-Eu2O3体系的玻璃化温度在1025℃附近。荧光光谱和ESR谱研究表明,在CaO-La2O3-B2O3-Eu2O3玻璃体系中存在着Eu2 和Eu3 两种价态离子。316,360,379,394,413,462和532nm锐线激发峰和592,616和650红区发射峰分别对应Eu3 的f-f激发跃迁和5D0-7FJ(J=1,2,3)跃迁发射;351nm和427nm宽带激发峰和蓝区发射分别对应Eu2 的5d-4f激发跃迁和发射。     

Wettability of silicon carbide ceramic by Al2O3/Dy2O3 and Al2O3/Yb2O3 systems

Wettability is an important phenomenon in the liquid phase sintering of silicon carbide (SiC) ceramics. This work involved a study of the wetting of SiC ceramics by two oxide systems, Al₂O₃ /Dy₂O₃ and Al₂O₃ /Yb₂O₃, which have so far not been studied for application in the sintering of SiC ceramics. Five mixtures of each system were prepared, with different compositions close to their respective eutectic ones. Samples of the mixtures were pressed into cylindrical specimens, which were placed on a SiC plate and subjected to temperatures above their melting points using a graphite resistance furnace. The behavior of the melted mixtures on the SiC plate was observed by means of an imaging system using a CCD camera and the sessile drop method was employed to determine the contact angle, the parameter that measures the degree of wettability. The results of variation in the contact angle as a function of temperature were plotted in graphic form which showed that the curves displayed a fast decline and good spreading. All the samples of the two systems presented final contact angles of 40° to 10° indicating their good wetting on SiC in the argon atmosphere. The melted/solidified area and interface between SiC and melted/solidified phase were evaluated by scanning electron microscopy (SEM) and their crystalline phases were identified by X-ray diffraction (DRX). The DRX analysis showed that Al₂O₃ and RE₂O₃ reacted and formed the Dy₃Al₅O₁₂ (DyAg) and Yb₃Al₅O₁₂ (YbAg) phases. The results indicated that the two systems had a promising potential as additives for the sintering of SiC ceramics.     

Interactions in the Al2O3-ZrO2-Y2O3 system

The phase diagram of the Al₂O₃-ZrO₂ system was replotted over a broad range of concentrations (0–100 mole %) and temperatures (1150–2800°C). The polymorphic transformation of zirconium F ? T occurs via the metatectic reaction F ? T + L at 2260°C. Phase triangulation was employed to plot the diagrams of the partially quasibinary sections in the Al₂O₃-ZrO₂-Y₂O₃ system. Since there is a wide solubility range based on ZrO₂ in the binary ZrO₂-Y₂O₃ system, the triangulation conodes are displaced in the F-solid solution corners. The two-phase regions Y₃A₅-F are quite broad. The reactions in all three are of the eutectic type. The ternary solid solution fields in the Al₂O₃-ZrO₂-Y₂O₃ system had no observable width.     

镁砂中Fe2O3、Al2O3、P2O5、TiO2的联合测定

镁砂产品检验中,采用碱熔融法共同预处理样品,在同一母液中,联合测定铁、铝、磷、钛的含量,缩短了检测时间。通过分别控制各元素的显色酸度,各元素线性良好,测得的Fe2O3、Al2O3、P2O5、TiO2的相对标准偏差分别小于1.11%、2.78%、4.84%、5.88%。实验结果表明,方法的准确度和精密度都较高。