Cr3+掺杂Al2O3-YAG共晶的生长及光谱性能研究

采用光学浮区法成功地生长出了质量良好的共晶.通过XRD分析,确认了共晶组成中仅含有Al2O3和YAG两种晶相,发现随着Cr的掺入,两相的晶胞参数相对于纯单晶略有增大.通过SEM观察发现共晶组织中两种晶相无序交错排布,共晶间距约10 μm左右.测量了室温下掺Cr共晶的吸收光谱、激发光谱和发射光谱.在402nm和556nm的激发波长下,共晶的发射谱均表现出了较好的R线发射,并在掺杂浓度达到0.4 wt;时达到极大值.其激发谱与吸收谱峰位基本一致,说明从激发态向基态跃迁时,发生无辐射跃迁的概率很小.通过与两种单晶的光谱的对比,确认进入Al2O3中八面体的Cr3+在共晶的光谱性质中起主要作用.     

区熔法制备Al2O3/MgAl2O4共晶陶瓷

利用感应区熔法制备了Al2O3/MgAl2O4共晶陶瓷.当坩埚壁温为2150℃、行走速度为5 mm/h时,获得了φ10 mm×104 mm表面光滑的圆棒.结果表明共晶陶瓷由Al2O3相和MgAl2O4相组成,分别按照(110)(311)晶面生长;Al2O3相为基体相,MgAl2O4相以非连续的片状均匀地分布在基体相之中.定向凝固共晶陶瓷的密度是理论值的99;;硬度和断裂韧性分别达到18.7 GPa和3.74 MPa·m1/2,约是预烧结体的2倍.气孔和界面非晶相的消失以及以单晶形态存在的Al2O3基体相,有效提高了材料的硬度和断裂韧性.     

Ce3+∶GdLu2Al5O12/Al2O3共晶微结构及其发光性能

稀土共晶闪烁体是通过定向凝固晶体生长技术,将具有不同折射率的两相制备成具有射线探测功能的共晶材料,其中含有激活离子的闪烁体相的折射率高于基质相。在高能射线辐照下,闪烁体相将入射高能射线转换成荧光,然后,荧光在闪烁体相和基底相的界面以全反射的形式实现定向输出,从而有效提高辐射探测成像的空间分辨率。本工作采用微下降法成功生长得到φ3 mm×117.0 mm 的1.0%(原子数分数)Ce∶GdLu₂Al₅O₁₂/Al₂O₃闪烁共晶样品。通过切割抛光加工得到φ3 mm×2.0 mm的共晶薄片,并将该共晶薄片进行微观结构、能谱分析和荧光性能等表征和测试,结果表明所得到的共晶样品由Ce∶GdLuAG和Al₂O₃两晶相构成,微观结构呈现出“中国结”结构,并在生长方向呈现出一定的有序排列。荧光光谱测试表明该共晶材料存在Gd³⁺-Ce³⁺间的能量传递,具有典型的Ce³⁺辐射跃迁,其中双宽峰发射峰最强位于560 nm。此外,根据生长速率对共晶样品发射峰强、峰位以及荧光寿命影响,优化出最佳下拉生长速率为4.0 mm/min。     

Nd3+:Na3La9O3(BO3)8晶体生长和光谱性能

采用顶部籽晶法生长Nd3+:Na3La9O3(BO3)8 晶体.在室温下测试了吸收光谱、发射光谱和荧光寿命.应用Judd-Ofelt理论评价了Nd3+:Na3La9O3(BO3)8晶体的光谱性能.812 nm处较宽的吸收峰适合AlGaAs LD泵浦的吸收.分别计算了Nd3+离子的唯象强度、谱线强度、辐射寿命、荧光分支比和荧光量子效率.     

纳米Al2O3/GdAlO3共晶陶瓷复合粉体的醇-水加热法制备与表征

为制备分散均匀的纳米尺度的共晶陶瓷复合粉体,采用Al(NO3)3·9H2O和Gd2O3作为原材料,通过醇-水加热法制备了纳米尺度的Al2O3/GdAlO3共晶成分陶瓷粉体.研究了溶液初始浓度配比和pH值等对复合粉体粒径的影响.通过SEM、TEM、FT-IR和BET N2吸附法等手段表征了前驱体颗粒大小和分散性3确定最佳的前驱体制备工艺,对前驱体进行煅烧制得Al2O3/GdAlO3复合陶瓷粉体.结果表明,前驱体粒径和分散性受制备工艺影响较大;特别是,最佳工艺制备的前驱体平均粒径20 nm,分散性良好,形貌多呈球形;1250℃煅烧后得到的Al2O3/GdAlO3共晶陶瓷粉体的晶化良好、成分均匀,粉体粒径100～200 nm.     

Nd^3＋：Na3La9O（BO3）8晶体生长和光谱性能

采用顶部籽晶法生长Nd^3＋：Na3La9O3（BO3）8晶体。在室温下测试了吸收光谱、发射光谱和荧光寿命。应用Judd-Ofelt理论评价了Nd^3＋：Na3La9O3（BO3）8晶体的光谱性能。812nm处较宽的吸收峰适合AlGaAs LD泵浦的吸收。分别计算了Nd^3＋离子的唯象强度、谱线强度、辐射寿命、荧光分支比和荧光量子效率。     

感应区熔法制备Al2O3/MgAl2O4/ZrO2共晶陶瓷

利用感应区熔法制备了Al2O3/MgAl2O4/ZrO2共晶陶瓷.当坩埚壁温为2200℃、行走速度为2mm/h时,制备了φ10 mm ×62 mm表面光滑致密的陶瓷样品.扫描电镜微观组织图显示Al2O3相和MgAl2O4相为基体相,ZrO2相以棒状镶嵌在基体中.定向凝固共晶陶瓷硬度和断裂韧性达到12 GPa和6.1 MPa·m1/2,为预烧结体的2倍和1.7倍.气孔和晶界的消失及细小规整ZrO2相在基体中的弥散分布,有效提高了材料的硬度和断裂韧性.     

水热法合成Gd2O3∶Dy3+纳米棒及发光性能

以氢氧化钠为沉淀剂,采用水热方法制备了Gd2O3∶Dy3+纳米棒.通过红外光谱、扫描电镜及X射线衍射对前驱体及目标产物的物相结构、微观形貌进行了分析表征,通过荧光分光光度计测试了所得Gd2O3∶Dy3+的发光性能.结果表明:水热前驱体为六方相氢氧化钆(镝),经900℃焙烧得立方相的Gd2O3∶Dy3+.所得G d2O3∶Dy3为直径约100 nm,长度约500 nm～1μm的纳米棒.其激发光谱由一系列激发峰组成,峰值分别位于239 nm、279 nm、314 nm、353 nm,最强峰位于279 nm处;发射光谱主要由两部分组成,分别为460 ～500 nm的蓝光和560～590nm的黄绿光发射峰(带),均属于Dy3+的特征发射,且后者的强度远高于前者,因此,在紫外光激发下呈黄光发射.     

GdAlO3∶Tb3+-Al2O3有序共晶生长及其微结构研究

两相有序共晶材料由于具有不同折射率的两晶相呈现有序排列,可降低荧光在共晶材料内部的散射而实现导光功能,可被应用于高分辨探测成像器件中。本工作根据定向凝固原理,用微下降法生长技术制备得到了直径为3 mm的GdAlO₃∶Tb³⁺-Al₂O₃两相有序共晶。通过SEM和元素分析,探究了GdAlO₃∶Tb³⁺-Al₂O₃共晶内部的微结构,结果显示,所得共晶中GdAlO₃∶Tb³⁺晶相均匀有序地分布于基质Al₂O₃晶相中,GdAlO₃∶Tb³⁺晶相直径的大小受生长速率的影响,速率越快,直径越小。所制备得到的GdAlO₃∶Tb³⁺-Al₂O₃有序共晶在X射线辐照下发射出明亮的绿色荧光,并在GdAlO₃∶Tb³⁺晶相中定向传播,有望被用作X射线探测成像材料,提高探测器的空间分辨率。     

Ti-Al-Nb2O5系原位合成Al2O3晶须的形成机理分析

本文研究了以粉埋法原位合成的Al2O3晶须的形态和反应过程以及晶须的生长机理.通过物相测试表明产物由Al2O3、TiAl3、NbAl3和少量的AlN相组成,SEM结合EDS分析表明原位合成了直径小于100nm的Al2O3晶须,晶须呈棉絮状分布于基体交界处.基于铝的过剩,TiAl3相是Ti-Al界面的唯一产物.Ti与O2以反应时间短的动力学势优先形成的TinOm中间产物是Al2O3晶须生成的控制步骤.Nb2O5与铝液的双效复合催化作用,提高了晶须的生成速率;同时Al的用量因AlN的生成而减小,导致生成晶须的催化活性点减小,而扩散到每个活性点周围的TinOm及Nb2O5浓度增加,导致晶须分布密而均匀.Al2O3晶核在催化剂的作用下以螺旋位错生长形成长径比较为理想的Al2O3晶须.     

CaO-MgO-Al2O3-Fe2O3-B2O3-SiO2系微晶釉的制备

通过引入B2O3以降低烧成温度,利用赤泥中的Fe2O3为着色剂,在1150℃左右低温烧成制备了CaO-MgO-Al2O3-Fe2O3-B2O3-SiO2系微晶釉.赤泥的加入量为20;左右时,釉面具有良好的装饰效果和显微硬度.利用XRD、SEM研究了釉的物相及显微组织.结果表明,釉中析出的微晶是普通辉石,微晶的含量随MgO及CaO的含量增加而增加,而提高Al2O3含量则抑制微晶的析出.     

Fe2O3-CO3O4共掺杂MgO-Al2O3-SiO2体系的红外辐射性能研究

采用固相反应法制备Fe2O3-Co3O4共掺杂MgO-Al2O3-SiO2体系的复合陶瓷材料,并通过XRD、SEM、XPS以及红外辐射测试等方法研究了样品的结晶行为与红外辐射性能.结果表明:Fe2 O3和Co3 O4共掺杂MgO-Al2 O3-SiO2体系后离子分布改变并生成混合尖晶石,从而引起品格畸变,从而有效提高材料的红外辐射性能.材料的红外发射率与其晶格畸变程度具有相同的变化趋势,并随Fe2 O3与Co3O4质量之比(R)的增加呈非线性变化.当R=3∶2时,材料在8 ～ 14 μm波段的辐射率可达0.92.     

EPR and magnetic susceptibility studies of B2O3–Bi2O3–Gd2O3 glasses

Glasses of the xGd₂O₃ · (100 − x)[B₂O₃ · Bi₂O₃] system with 0.5 ⩽ x ⩽ 10 mol% were studied by electron paramagnetic resonance (EPR) and magnetic susceptibility measurements. Data obtained show that for low gadolinium oxide contents of the samples (x ⩽ 3 mol%) the Gd³⁺ ions are randomly distributed in the host glass matrix and are present as isolated and dipole–dipole coupled species. For higher gadolinium oxide contents of the samples (x > 3 mol%) the Gd³⁺ ions appear as both isolated and antiferromagnetically coupled species. The EPR spectra of the glasses reveal resonance sites with an unexpected high crystalline field in addition to the ‘U’ spectrum, typical for Gd³⁺ ions in disordered systems. This absorption line is due to Gd³⁺ ions that replace Bi³⁺ ions from the host glass matrix and could play the network unconventional former role in the studied glasses.     

Pr2O3对含Cr2O3辉石系矿渣微晶玻璃晶化行为的影响

以白云鄂博西尾矿和粉煤灰为主要原料,分别制备了添加0,2.0wt;,4.0wt;和6.0wt; Pr2O3的辉石系矿渣微晶玻璃;综合采用基于DSC/DTA结果的析晶活化能Ek、Avrami指数以及粘流活化能Eη和背散射电子SEM显微形貌分析研究了Pr2O3对析晶的影响.结果表明在所研究范围内,Pr2O3含量的提高在整体上抑制了辉石相的析出.其原因除了与富Pr颗粒相对辉石相在析晶过程中的“钉扎”有关外,还与Pr2O3含量提高后使基础玻璃网络聚合程度加大,从而增大了辉石相形成所需离子扩散的阻力有关.     

Yb2O3-Y2O3-Gd2O3-ZrO2热障涂层制备及性能研究

以Yb2O3、Y2O3 、Gd2O3稀土氧化物粉末和ZrOCl2·8H2O粉末为原料,采用化学共沉淀法制备了Yb2O3-Y2O3-Gd2O3-ZrO2 (YYGZO)热喷涂用粉末,采用大气等离子喷涂技术制备了YYGZO涂层,利用场发射扫描电镜(FESEM)、X射线衍射(XRD)研究了YYGZO粉末及涂层的微观组织形貌、相结构.结果表明,制备的热喷涂YYGZO粉末大部分呈规则实心球体状,且球形度良好,颗粒粒径均匀,大部分颗粒粒径分布为30～60μm,流动性能较好,满足大气等离子喷涂的要求.YYGZO涂层具有较好的高温相结构稳定性.所制备YYGZO热障涂层组织结构比较致密,涂层各个界面结合紧密,孔隙率约为9.23;,结合强度为35.2 MPa.     

Thermal expansion and transition temperature of glasses in the systems BeO–Al2O3–B2O3 and MgO–Al2O3–B2O3

Researches were conducted for glasses in the systems BeO–Al₂O₃–B₂O₃ and MgO–Al₂O₃–B₂O. The following characteristics have been determined: thermal expansion coefficient within 20–300 °C, structural thermal expansion coefficient (STEC) and glass transition temperature. The discussed properties of Be-aluminoborate and Mg-aluminoborate glasses have been compared with those of Ca-, Sr- and Ba-aluminoborate glasses. TEC of studied glasses gets higher going from Be-aluminoborate glasses to Ba-aluminoborate ones, but T_g decreases under the same succession. The dependence of STEC on the nature of a given cation is more complicated. The pattern of dependence of the properties on composition is due to changing the boron coordination number with respect to oxygen, which is the main network-former, and to competition between the aluminium and boron for the oxygen brought by an ion-modifier. The difference between the effect of one ion-modifier and that of another is determined by decreasing the radius of an ion and increasing its electric field strength in the succession from Ba²⁺ to Be²⁺. The ions of Be and Mg can also act as network-former to some extent.     

BaTiO3-Nb2O5-Fe2O3陶瓷介电性能的研究

利用传统方法制备了BaTiO3-Nb2O5-Fe2O3(BTNF)陶瓷,采用X射线衍射仪、电容测试仪、电滞回线测量仪等测试手段研究了不同添加剂(Fe2O3、Co2O3、Nb2O5)对陶瓷晶体结构、介电性能及铁电性的影响.结果表明:Nb2O5是施主掺杂,易引起晶格畸变,使四方率增大;而Fe2O3为受主掺杂,其可提高氧空位浓度,促进BaTiO3陶瓷晶粒生长.同时掺杂Fe2O3、Nb2O5时,可以相互补偿.当Fe2O3浓度约为0.15;摩尔分数,Nb2O5浓度为0.79;摩尔分数时,陶瓷的介电常数达到4443,温度特性≤±10;,可以满足Y5P瓷料的要求.     

In2O3 and tin-doped In2O3 nanocrystals prepared by glass crystallization

Glasses in the system Na₂O/B₂O₃/Al₂O₃/In₂O₃/(SnO₂) were melted and subsequently tempered in the range from 540 to 700 °C. This led to the crystallization of In₂O₃, besides also NaBO₂ and Na₂Al₂B₂O₇ were formed. The crystallite sizes were in the range from 12 to 34 nm, depending on the temperature of thermal treatment, as calculated from XRD-line broadening. Crystal sizes determined by TEM were in the same range. Particle size histograms show a narrow crystal size distribution. After crystallization, the glass matrices and the non indium-containing crystalline phases were dissolved in diluted acetic acid. Spectra of the obtained suspensions containing tin-doped In₂O₃ nanocrystals exhibited a sharp UV-cut off, high transmission in the visible range and strongly decreasing transmission at wavelengths >1000 nm.     

Structural properties of Cr2O3–Fe2O3–P2O5 glasses,Part I

The structural properties of xCr₂O₃–(40 − x)Fe₂O₃–60P₂O₅, 0 ⩽ x ⩽ 10 (mol%) glasses have been investigated by Raman and Mössbauer spectroscopies, X-ray diffraction (XRD) and differential scanning calorimetry (DSC). The Raman spectra show that the addition of up to 5.3 mol% Cr₂O₃ does not produce any changes in the glass structure, which consists predominantly of pyrophosphate, Q¹, units. This is in accordance with O/P ≈ 3.5 for these glasses. The increase in glass density and T_g that occurs with increasing Cr₂O₃ suggests the strengthening of glass network. The Mössbauer spectra indicate that the Fe²⁺/Fe_tot ratio increases from 0.13 to 0.28 with increasing Cr₂O₃ content up to 5.3 mol%, which can be related to an increase in the melting temperature from 1423 to 1473 K. After annealing, the 10Cr₂O₃–30Fe₂O₃–60P₂O₅ (mol%) sample was partially crystallized and contained crystalline β-CrPO₄ and Fe₃(P₂O₇)₂. The SEM and AFM micrographs of the partially crystallized sample revealed randomly distributed crystals embedded in a homogeneous glass matrix. EDS analysis indicated that the glass matrix was rich in Fe₂O₃ (39.6 mol%) and P₂O₅ (54.9 mol%), but contained only 5.5 mol% of Cr₂O₃. These results suggest that the maximum solubility of chromium in these iron phosphate melts is 5.5 mol% Cr₂O₃.     

TiO2烧结助剂对纳米η-Al2 O3制备Al2 O3-Cr2 O3固溶体的影响研究

以纳米η-Al₂O₃粉和工业铬绿为原料,以摩尔比1:1配比制备Al₂O₃-Cr₂O₃固溶体,以TiO₂为烧结助剂,在还原气氛下经1400 ℃、1500 ℃和1600 ℃固相烧结.研究了TiO₂的加入对纳米η-Al₂O₃制备Al₂O₃-Cr₂O₃固溶体的致密度、线收缩率、相组成、晶胞参数、互扩散程度和微观结构的影响.结果表明:TiO₂的加入能促进Al₂O₃-Cr₂O₃固溶体的致密化;当温度为1600 ℃,TiO₂的添加量为2wt;时,试样的体积密度最大为4.57 g·cm^-3,线收缩率为19.8;;TiO₂的加入能使Al₂O₃-Cr₂O₃固溶体中Al³⁺和Cr³⁺的互扩散程度增加;微观结构表明,TiO₂的加入能使Al₂O₃-Cr₂O₃固溶体晶粒之间结合更紧密,实验温度范围内,随着TiO₂添加量的增加晶粒从沿晶断裂向穿晶断裂转变,只在晶间和晶内存在极少量气孔,当温度为1600 ℃,TiO₂的添加量为2wt;时,晶粒大小较均匀,平均晶粒尺寸约10μm.