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具有Ruddlesden-Popper结构的杂化非本征铁电体(Ca_(1-x)Sm_(x))_(3)Ti_(2)O_(7)陶瓷的制备及其物理性能
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作者 MARCO Antonio López-Aguila 柳志旭 +2 位作者 王守宇 黄聪 刘卫芳 《天津师范大学学报(自然科学版)》 CAS 北大核心 2024年第2期19-25,共7页
为探究稀土离子掺杂对Ca_(3)Ti_(2)O_(7)物理性能的调控,采用固相反应法制备了Sm^(3+)掺杂的(Ca_(1-x)Sm_(x))_(3)Ti_(2)O_(7)(x=0,0.02,0.04)陶瓷样品,通过XRD、XPS、紫外-可见光吸收光谱以及第一性原理计算等方法对样品的晶体结构、... 为探究稀土离子掺杂对Ca_(3)Ti_(2)O_(7)物理性能的调控,采用固相反应法制备了Sm^(3+)掺杂的(Ca_(1-x)Sm_(x))_(3)Ti_(2)O_(7)(x=0,0.02,0.04)陶瓷样品,通过XRD、XPS、紫外-可见光吸收光谱以及第一性原理计算等方法对样品的晶体结构、光学性能、电学性能和磁学性能进行分析.结果表明:随着Sm^(3+)含量的增加,(Ca_(1-x)Sm_(x))_(3)Ti_(2)O_(7)的晶胞参数逐渐增大.Sm^(3+)掺杂导致氧空位减少,因此样品的漏电流随着Sm^(3+)掺杂量的增加而减小.同时,随着Sm^(3+)掺杂量的增加,样品的光学带隙呈现增大趋势.此外,第一性原理研究表明,Sm^(3+)掺杂可在体系中诱导出磁性能,进一步丰富了该材料的物理性能. 展开更多
关键词 (Ca_(1-x)sm_(x))_(3)ti_(2)o_(7)陶瓷 铁电性 氧空位 光学带隙 第一性原理
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Sm_(x)Sr_(1-x)Al_(x)Ti_(1-x)O_(3)陶瓷的结构及微波介电性能研究
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作者 冯恒恒 杨启航 +3 位作者 余涛 李冬梅 王志建 余洪滔 《中国陶瓷》 CAS CSCD 北大核心 2022年第3期28-33,共6页
采用传统固相法制备了Sm_(x)Sr_(1-x)Al_(x)Ti_(1-x)O_(3)(0≤x≤0.4)陶瓷,所得陶瓷样品均为单相结构。X射线衍射精修数据证实了Sm_(2)O_(3)和Al_(2)O_(3)的掺入有效地增大了A位和B位阳离子与氧离子之间的键价值,拉曼图谱显示随着共掺... 采用传统固相法制备了Sm_(x)Sr_(1-x)Al_(x)Ti_(1-x)O_(3)(0≤x≤0.4)陶瓷,所得陶瓷样品均为单相结构。X射线衍射精修数据证实了Sm_(2)O_(3)和Al_(2)O_(3)的掺入有效地增大了A位和B位阳离子与氧离子之间的键价值,拉曼图谱显示随着共掺量增加,TO_(2)、A_(1g)振动模式增强,A位和B位离子有序度增大。另外Sm_(2)O_(3)和Al_(2)O_(3)优化了陶瓷的微观形貌。结合键价理论和拉曼分析了随x变化[TiO_(6)]八面体等结构演变对其微波介电性能的影响,陶瓷样品的介电常数逐渐下降,品质因子增加,其频率温度系数向正方向漂移。 展开更多
关键词 sm_(x)sr_(1-x)al_(x)ti_(1-x)o_(3) 晶体结构 介电性能
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高温扩散工艺制备带隙可调的β-(Al_(x)Ga_(1-x))_(2)O_(3)薄膜
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作者 谭黎 张俊 +3 位作者 张敏 赵荣力 邓朝勇 崔瑞瑞 《人工晶体学报》 CAS 北大核心 2023年第2期281-288,共8页
β-(Al_(x)Ga_(1-x))_(2)O_(3)因其优异的抗击穿及带隙可调节性在现代功率器件及深紫外光电探测等领域展现出巨大的应用前景,然而传统直接生长工艺的复杂性和难度限制了其进一步的发展。因此,本文采用较为简单的高温扩散工艺在c面蓝宝... β-(Al_(x)Ga_(1-x))_(2)O_(3)因其优异的抗击穿及带隙可调节性在现代功率器件及深紫外光电探测等领域展现出巨大的应用前景,然而传统直接生长工艺的复杂性和难度限制了其进一步的发展。因此,本文采用较为简单的高温扩散工艺在c面蓝宝石衬底上成功制备了β-(Al_(x)Ga_(1-x))_(2)O_(3)纳米薄膜。利用X射线衍射、原子力显微镜、扫描电子显微镜和紫外-可见分光光度计对其进行了表征。由于高温下蓝宝石衬底中的Al原子向Ga_(2)O_(3)层扩散,β-Ga_(2)O_(3)薄膜将转变为Al、Ga原子比例不同的β-(Al_(x)Ga_(1-x))_(2)O_(3)薄膜。实验结果显示:当退火温度从1 010℃增加到1 250℃时,薄膜中Al的平均含量从0.033增加到0.371;当退火温度从950℃增加到1 250℃时,薄膜的厚度从186 nm增加到297 nm,粗糙度从2.31 nm增加到15.10 nm;当退火温度从950℃增加到1 190℃时,薄膜的带隙从4.79 eV增加至5.96 eV。结果表明高温扩散工艺能够有效调节β-(Al_(x)Ga_(1-x))_(2)O_(3)薄膜的光学带隙,为β-(Al_(x)Ga_(1-x))_(2)O_(3)基新型光电子器件提供了实验基础。 展开更多
关键词 β-(al_(x)Ga_(1-x))_(2)o_(3) Ga_(2)o_(3) al掺杂 半导体薄膜 高温扩散 可调带隙 磁控溅射
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固相法制备(Ca_(1-x)Sr_(x))_(1.35)Sm_(0.65)Al_(0.65)Ti_(0.35)O_(4)陶瓷的微波介电性能
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作者 马才兵 《陶瓷科学与艺术》 CAS 2022年第10期92-93,共2页
用传统固相反应法制备了复杂钙钛矿结构陶瓷(Ca_(1-x)Sr_(x))_(1.35)Sm_(0.65)Al_(0.65)Ti_(0.35)O_(4)(x=0.4,0.3,0.2,0.1),用XRD表征其结构,SEM表征微观形貌,并测试样品的微波介电性能。随着Sr含量的增加其介电常数从19.8增加到24.1,... 用传统固相反应法制备了复杂钙钛矿结构陶瓷(Ca_(1-x)Sr_(x))_(1.35)Sm_(0.65)Al_(0.65)Ti_(0.35)O_(4)(x=0.4,0.3,0.2,0.1),用XRD表征其结构,SEM表征微观形貌,并测试样品的微波介电性能。随着Sr含量的增加其介电常数从19.8增加到24.1,温漂从-07ppm/℃增大到30.1ppm/℃,Q^(*)f值从65300GHz减少到36200GHz。当x=0.1时有较好的微波介电性能,介电常数为20.3,温漂为14.9ppm/℃,Q^(*)f值为65322GHz。表明复杂钙钛矿结构A2BO4的(Ca_(1-x)Sr_(x))_(1.35)Sm_(0.65)Al_(0.65)Ti_(0.35)O_(4)陶瓷是一种新型微波介电材料体系,具有很好的应用前景。 展开更多
关键词 微波介电性能 (Ca_(1-x)sr_(x))_(1.35)sm_(0.65)al_(0.65)ti_(0.35)o_(4) 固相法
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Ti_(3)(Zn_(x)Al_(1-x))C_(2)固溶体热学、电学和力学性质的理论研究
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作者 邓斐然 徐敏 +6 位作者 苗峰 黄毅 冯世全 宋明泽 肖晨达 林园园 李慧敏 《人工晶体学报》 CAS 北大核心 2022年第3期477-484,492,共9页
采用第一性原理的密度泛函理论平面波赝势法,通过投影缀加波(PAW)和广义梯度近似(GGA)系统地研究了Ti_(3)(Zn_(x)Al_(1-x))C_(2)的结构、能量、声子性质、电子性质和弹性性质。对MAX相Ti_(3)AlC_(2)晶体中A位置的Al元素用Zn元素进行替... 采用第一性原理的密度泛函理论平面波赝势法,通过投影缀加波(PAW)和广义梯度近似(GGA)系统地研究了Ti_(3)(Zn_(x)Al_(1-x))C_(2)的结构、能量、声子性质、电子性质和弹性性质。对MAX相Ti_(3)AlC_(2)晶体中A位置的Al元素用Zn元素进行替换掺杂,构建出Ti_(3)(Zn_(x)Al_(1-x))C_(2)(x=0,0.25,0.5,0.75,1)固溶体结构模型。计算分析表明:在所研究的掺杂浓度范围内Ti_(3)(Zn_(x)Al_(1-x))C_(2)均是热力学、动力学和力学稳定的脆性材料;此外,Ti_(3)(Zn_(x)Al_(1-x))C_(2)(x=0,0.25,0.5,0.75,1)均呈现金属性,在费米能级处的电子态密度主要贡献来自Ti-3d态,同时具有离子键、共价键和金属键的综合性质。随着Zn原子掺杂浓度的增加,在一定程度上其导电性和塑性均增强。 展开更多
关键词 ti_(3)(Zn_(x)al_(1-x))C_(2) MAx 低维晶态材料 第一性原理 电子性质 弹性性质 声子性质
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ε-(Al_(x)Ga_(1-x))_(2)O_(3)/ε-Ga_(2)O_(3)异质结电子输运性质研究
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作者 白雅楠 吕燕伍 《人工晶体学报》 CAS 北大核心 2022年第3期441-449,共9页
Ga_(2)O_(3)是一种新兴的宽带隙半导体,在电力和射频电子系统中具有潜在的应用前景。前期研究以β-Ga_(2)O_(3)为主,并且已经对β-(Al_(x)Ga_(1-x))_(2)O_(3)/Ga_(2)O_(3)异质结构中的二维电子气(2DEG)进行了理论计算,本文主要研究ε-(A... Ga_(2)O_(3)是一种新兴的宽带隙半导体,在电力和射频电子系统中具有潜在的应用前景。前期研究以β-Ga_(2)O_(3)为主,并且已经对β-(Al_(x)Ga_(1-x))_(2)O_(3)/Ga_(2)O_(3)异质结构中的二维电子气(2DEG)进行了理论计算,本文主要研究ε-(Al_(x)Ga_(1-x))_(2)O_(3)作为势垒层对ε-(Al_(x)Ga_(1-x))_(2)O_(3)/ε-Ga_(2)O_(3)异质结电子输运性质的影响,首先介绍了ε-(Al_(x)Ga_(1-x))_(2)O_(3)/ε-Ga_(2)O_(3)异质结的结构和性质,分析计算了由于ε-(Al_(x)Ga_(1-x))_(2)O_(3)/ε-Ga_(2)O_(3)异质结的自发极化和压电极化所产生的极化面电荷密度,以及极化对2DEG浓度产生的影响,接着分析了在不同Al摩尔组分下,ε-(Al_(x)Ga_(1-x))_(2)O_(3)势垒层厚度与合金无序散射、界面粗糙度散射和极性光学声子散射之间的关系。最后通过计算得出结论:界面粗糙度散射和极性光学声子散射对ε-(Al_(x)Ga_(1-x))_(2)O_(3)/ε-Ga_(2)O_(3)异质结的电子输运性质有重要影响,合金无序散射对异质结的输运性质影响较小;2DEG浓度、合金无序散射、界面粗糙度散射和极性光学声子散射的电子迁移率强弱由ε-(Al_(x)Ga_(1-x))_(2)O_(3)势垒层的厚度和Al摩尔组分共同决定。 展开更多
关键词 2DEG浓度 电子迁移率 ε-(al_(x)Ga_(1-x))_(2)o_(3)/ε-Ga_(2)o_(3)异质结 合金无序散射 界面粗糙度散射 极性光学声子散射
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Bi_(1-x)Pr_(x)Fe_(1-x)Ti_(x)O_(3)多铁陶瓷的结构与电磁性能研究
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作者 代兴华 王旭昊 代海洋 《兵器材料科学与工程》 CAS CSCD 北大核心 2022年第1期23-27,共5页
采用快速液相烧结法制备Bi_(1-x)Pr_(x)Fe_(1-x)Ti_(x)O_(3)(x=0.00、0.03、0.06、0.12)系列多铁陶瓷样品,研究Pr-Ti共掺杂对BiFe O_(3)结构、缺陷、电学和磁学特性的影响。XRD分析结果表明:所有样品均为菱方钙钛矿结构,Pr-Ti共掺杂可... 采用快速液相烧结法制备Bi_(1-x)Pr_(x)Fe_(1-x)Ti_(x)O_(3)(x=0.00、0.03、0.06、0.12)系列多铁陶瓷样品,研究Pr-Ti共掺杂对BiFe O_(3)结构、缺陷、电学和磁学特性的影响。XRD分析结果表明:所有样品均为菱方钙钛矿结构,Pr-Ti共掺杂可有效抑制杂相生成,当掺杂量高于0.06时杂相基本消失,共掺杂引起结构畸变。正电子湮没寿命谱测试结果表明:所有样品中均存在阳离子空位型缺陷,空位尺寸和浓度均随Pr-Ti掺杂量增加而增大。电学和磁学性能测试结果表明:适量Pr-Ti共掺杂可有效提高Bi Fe O_(3)的介电、铁电和磁学性能。综合上述结果,认为BiFeO_(3)多铁性能的改善可能是由于Pr-Ti共掺杂引起晶格畸变、减少氧空位浓度、改变阳离子空位浓度等多种原因引起。 展开更多
关键词 Bi_(1-x)Pr_(x)Fe_(1-x)ti_(x)o_(3)陶瓷 共掺杂 结构 电磁性能
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Zn_(0.15)Nb_(0.3)Ti_(0.55-x)(Co_(1/3)Nb_(2/3))_(x)O_(2)陶瓷的微波介电性能研究
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作者 张文娟 《电子元件与材料》 CAS CSCD 北大核心 2021年第2期144-149,共6页
采用固相烧结法制备Zn_(0.15)Nb_(0.3)Ti_(0.55-x)(Co_(1/3)Nb_(2/3))_(x)O_(2)(x=0,0.05,0.15,0.25,0.35,0.4,0.45,0.55)陶瓷,研究了(Co_(1/3)Nb_(2/3))^(4+)取代Ti^(4+)对陶瓷的物相、微观形貌和微波介电性能的影响。实验结果表明,当(... 采用固相烧结法制备Zn_(0.15)Nb_(0.3)Ti_(0.55-x)(Co_(1/3)Nb_(2/3))_(x)O_(2)(x=0,0.05,0.15,0.25,0.35,0.4,0.45,0.55)陶瓷,研究了(Co_(1/3)Nb_(2/3))^(4+)取代Ti^(4+)对陶瓷的物相、微观形貌和微波介电性能的影响。实验结果表明,当(Co_(1/3)Nb_(2/3))^(4+)取代量x≤0.05时,Zn_(0.15)Nb_(0.3)Ti_(0.55-x)(Co_(1/3)Nb_(2/3))_(x)O_(2)陶瓷表现出纯的金红石Zn_(0.15)Nb_(0.3)Ti_(0.55)O_(2)相;当(Co_(1/3)Nb_(2/3))^(4+)取代量x>0.15时,有第二相ZnTiNb_(2)O_(8)和ZnNb_(2)O_(6)生成。陶瓷的Q×f值随x的增大而提高,介电常数(ε_(r))和谐振频率温度系数(τ_(f))则随ZnTiNb_(2)O_(8)和ZnNb_(2)O_(6)的增多而逐渐降低。当x=0.4时,Zn_(0.15)Nb_(0.3)Ti_(0.55-x)(Co_(1/3)Nb_(2/3))_(x)O_(2)陶瓷在1075℃下烧结获得最佳的微波介电性能:ε_(r)=35.44,Q×f=25862 GHz(f=5.8 GHz),τ_(f)=5.2×10^(-6)/℃。 展开更多
关键词 微波介质陶瓷 Zn_(0.15)Nb_(0.3)ti_(0.55-x)(Co_(1/3)Nb_(2/3))_(x)o_(2) 掺杂 介电性能 LTCC
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Cu_(m)-Fe_(n)/Ti_(1-x)Sn_(x)O_(2)复合催化剂的脱硝性能及抗硫活性
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作者 谭义凤 张婷 +2 位作者 张云飞 孙琦 田蒙奎 《材料导报》 EI CAS CSCD 北大核心 2022年第4期56-61,共6页
采用共沉淀法制备Ti_(1-x)Sn_(x)O_(2)复合氧化物,浸渍负载质量分数10%的CuO_(x)和FeO_(y)活性组分,制备一系列Cu_(m)-Fe_(n)/Ti_(1-x) Sn_(x)O_(2)催化剂。探究不同Ti/Sn和Cu/Fe(物质的量比)对Cu_(m)-Fe_(n)/Ti_(1-x)Sn_(x)O_(2)催化剂... 采用共沉淀法制备Ti_(1-x)Sn_(x)O_(2)复合氧化物,浸渍负载质量分数10%的CuO_(x)和FeO_(y)活性组分,制备一系列Cu_(m)-Fe_(n)/Ti_(1-x) Sn_(x)O_(2)催化剂。探究不同Ti/Sn和Cu/Fe(物质的量比)对Cu_(m)-Fe_(n)/Ti_(1-x)Sn_(x)O_(2)催化剂的NH_(3)-SCR反应活性的影响。研究结果表明,Ti_(0.67)Sn_(0.33)O_(2)载体可促进活性组分CuO_(x)和FeO_(y)的相互作用。当Cu/Fe为3∶1时,在300℃下NO_(x)的转化率达到91.3%;向反应体系通入286 mg/m^(3) SO_(2)反应3 h后,NO_(x)的转化率仅下降2.6%。X射线光电子能谱(XPS)、程序升温还原(H_(2)-TPR)、程序升温脱附(NH_(3)-TPD和NO_(x)-TPD)的表征表明,CuO_(x)和FeO_(y)之间存在相互作用,与单一的Cu/Ti_(0.67)Sn_(0.33)O_(2)和Fe/Ti_(0.67)Sn_(0.33)O_(2)对比,复合催化剂表面吸附氧浓度相对增加15%~33%,总酸量增大56%,从而提高了催化剂脱硝活性。 展开更多
关键词 NH_(3)-SCR ti_(1-x)Sn_(x)o_(2)复合氧化物 Cu_(m)-Fe_(n)/ti_(0.67)Sn_(0.33)o_(2)复合脱硝催化剂 抗硫活性
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Effect of Substitution Sr Cations on the Structure in the Gd_(1)(Ba_(2−x)Sr_(x))Cu_(3)O_(7−δ) Phases
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作者 Made Sumadiyasa Nyoman Wendri +1 位作者 Putu Suardana Ni Nyoman Rupiasih 《Journal of Materials Science and Chemical Engineering》 2020年第1期44-53,共10页
In an effort to improve the performance of superconductors in the field and high temperatures it is important to study the superconducting mechanism. For this reason, the cation substitution can be conducted. One of t... In an effort to improve the performance of superconductors in the field and high temperatures it is important to study the superconducting mechanism. For this reason, the cation substitution can be conducted. One of the high Tc superconductors Gd1Ba2Cu3O7&minus;δ phase with Sr substitution has been synthesized, i.e. Gd1(Ba2&minus;xSrx)Cu3O7&minus;δ compound. The sample was synthesized by using a solid-state reaction method with a wet mixing, sintered for 12 hours at temperature 900°C. The synthesis results are characterized by using XRD. The results of Match-3 software analysis showed high (higher 85%) Gd1Ba2Cu3O7&minus;δ phase was formed. The Sr substitution causes changes to the structure, i.e. the lattice parameters a, b and c, where the orthorhombicity tends to decrease with increasing Sr content. Refinement results show that based on the oxygen occupancy, the total oxygen content tends to increase. 展开更多
关键词 Wet Mixing Gd_(1)(Ba_(2-x)sr_(x))Cu_(3)o_(7-δ) Compound sr Substitution Lattice Parameters orthorhombicity
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Progress and perspective of Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3) ceramic electrolyte in lithium batteries 被引量:2
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作者 Ke Yang Likun Chen +2 位作者 Jiabin Ma Yan-Bing He Feiyu Kang 《InfoMat》 SCIE CAS 2021年第11期1195-1217,共23页
The replacement of liquid organic electrolytes with solid-state electrolytes(SSEs)is a feasible way to solve the safety issues and improve the energy density of lithium batteries.Developing SSEs materials that can wel... The replacement of liquid organic electrolytes with solid-state electrolytes(SSEs)is a feasible way to solve the safety issues and improve the energy density of lithium batteries.Developing SSEs materials that can well match with high-voltage cathodes and lithium metal anode is quite significant to develop high-energy-density lithium batteries.Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)(LATP)SSE with NASICON structure exhibits high ionic conductivity,low cost and superior air stability,which enable it as one of the most hopeful candidates for all-solidstate batteries(ASSBs).However,the high interfacial impedance between LATP and electrodes,and the severe interfacial side reactions with the lithium metal greatly limit its applications in ASSBs.This review introduces the crystal structure and ion transport mechanisms of LATP and summarizes the key factors affecting the ionic conductivity.The side reaction mechanisms of LATP with Li metal and the promising strategies for optimizing interfacial compatibility are reviewed.We also summarize the applications of LATP including as surface coatings of cathode particles,ion transport network additives and inorganic fillers of composite polymer electrolytes.At last,this review proposes the challenges and the future development directions of LATP in SSBs. 展开更多
关键词 crystal structure interfaces ionic conductivity Li_(1+x)al_(x)ti_(2-x)(Po_(4))_(3) lithium batteries
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Effects of Er^(3+)doping on structure and thermal properties of(Sm_(1-x)Er_(x))_(2)Zr_(2)O_(7)ceramics for thermal barrier coating
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作者 Min Xie Shengli An +2 位作者 Xiwen Song Jinxiao Bao Fen Zhou 《Journal of Rare Earths》 SCIE EI CAS CSCD 2022年第12期1920-1926,I0004,共8页
Rare earth Er^(3+)doped(Sm_(1-x)Er_(x))_(2)Zr_(2)O_(7)(x=0.1,0.2,and 0.3)ceramic samples were synthesized using a solid state reaction method.The microstructure and thermal properties of these ceramics were investigat... Rare earth Er^(3+)doped(Sm_(1-x)Er_(x))_(2)Zr_(2)O_(7)(x=0.1,0.2,and 0.3)ceramic samples were synthesized using a solid state reaction method.The microstructure and thermal properties of these ceramics were investigated to evaluate their potential as thermal barrier coating materials.The results show that ceramics are compact with regular-shaped grains of 1-5μm size.(Sm_(1-x)Er_(x))_(2)Zr_(2)O_(7)has a pyrochlore structure mainly determined by ionic radius ratio,but the ordering degree decreases with increase of the Er_(2)O_(3)content.There is no phase transformation from 1000 to 1200℃,and the(Sm_(1-x)Er_(x))_(2)Zr_(2)O_(7)ceramics exhibit excellent phase stability during thermal treatment at 1200℃for 100 h and 1400℃for 50 h.The thermal conductivities of dense(Sm_(1-x)Er_(x))_(2)Zr_(2)O_(7)ceramics range from 1.52 to 1.59 W/(m·K),which is lower than that of Sm_(2)Zr_(2)O_(7),and decrease as the Er2O3content increases.Besides,the thermal expansion coefficient of(Sm_(1-x)Er_(x))_(2)Zr_(2)O_(7)is higher than that of Sm_(2)Zr_(2)O_(7). 展开更多
关键词 (sm_(1-x)Er_(x))_(2)Zr_(2)o_(7) Pyrochlore structure Thermal-physical properties Er^(3+)doping Rare earths
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The electronic structure and optical properties of Ca_(3)(Mn_(1-x)Ti_(x))_(2)O_(7) from first-principle calculations
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作者 Fengqi Wang Wei Cai +5 位作者 Chunlin Fu Rongli Gao Gang Chen Xiaoling Deng Zhenhua Wang Chaoyang Zhang 《Journal of Advanced Dielectrics》 CAS 2019年第1期47-54,共8页
The electronic structure and optical properties of Ca_(3)(Mn_(1-x)Ti_(x))_(2)O_(7)(x¼0,1/8,2/8,3/8,4/8)were studied by first-principle calculations within the generalized gradient approximation approaches(GGA).Th... The electronic structure and optical properties of Ca_(3)(Mn_(1-x)Ti_(x))_(2)O_(7)(x¼0,1/8,2/8,3/8,4/8)were studied by first-principle calculations within the generalized gradient approximation approaches(GGA).The lattice constants of Ca_(3)(Mn_(1-x)Ti_(x))_(2)O_(7) increase with the increase of Ti^(4+)content caused by the substitution of Ti^(4+)with larger ionic radius for Mn^(4+).Ca_(3)(Mn_(1-x)Ti_(x))_(2)O_(7) is a direct band gap semiconductor,and the band gap(Eg)increases with the increase of Ti^(4+)content.From the density of states,the introduction of Ti-3d states can weaken the effects of Mn-3d states on the bottom of conduction band and has little influence on O-2p states on the top of valence band.The introduction of nonmagnetic Ti^(4+)ions can weaken the magnetism of Ca_(3)(Mn_(1-x)Ti_(x))_(2)O_(7).According to the Mulliken population analysis,it is found that the introduction of Ti^(4+)enhances the electronic accepting capacity of oxygen ions and enhances the electronic losing capacity of manganese ions.The bond strength of Ti–O covalent bond is stronger than that of Mn–O covalent bond.Furthermore,the optical properties of Ca_(3)(Mn_(1-x)Ti_(x))_(2)O_(7) was calculated.As Ti^(4+)content increases,the absorption edge of Ca_(3)(Mn_(1-x)Ti_(x))_(2)O_(7) has a blue shift,the static refractive index n0 decreases,the static dielectric constant"1(0)decreases,the position of loss peak moves to higher energy. 展开更多
关键词 FIRST-PRINCIPLE Ca_(3)(Mn_(1-x)ti_(x))_(2)o_(7) band structure density of states optical properties.
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升温制度对Al-MgO-Al_(2)O_(3)耐火材料物相组成及显微结构的影响 被引量:3
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作者 赵臣瑞 孙洋 +3 位作者 牛智旺 李勇 李宏宇 梁保青 《耐火材料》 CAS 北大核心 2021年第2期107-110,共4页
以金属Al粉、电熔镁砂和电熔棕刚玉为原料,热固性酚醛树脂为结合剂,制备了Al-MgO-Al_(2)O_(3)耐火材料试样。在空气条件下以两种升温制度对其进行热处理:1)直接升温至1500℃保温2 h;2,先升温至580℃保温2 h后再升温至1500℃保温2 h。利... 以金属Al粉、电熔镁砂和电熔棕刚玉为原料,热固性酚醛树脂为结合剂,制备了Al-MgO-Al_(2)O_(3)耐火材料试样。在空气条件下以两种升温制度对其进行热处理:1)直接升温至1500℃保温2 h;2,先升温至580℃保温2 h后再升温至1500℃保温2 h。利用XRD、SEM等探究了升温制度对材料相组成及显微结构的影响。结果表明:1)直接升温至1500℃热处理后,材料中生成的非氧化物相主要为Al 4O 4C;2,580℃保温2 h有利于金属铝在高温下以Al 2O(g)的形式参与反应,进而使材料中生成(Al 2OC)x(AlN)1-x纤维;3)先580℃保温再1500℃热处理后材料中形成了以镁铝尖晶石和(Al 2OC)x(AlN)1-x纤维为主成分的致密层。 展开更多
关键词 升温制度 al-Mgo-al_(2)o_(3)耐火材料 (al_(2)oC)x(alN)1-x 相组成 显微结构
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直接热处理法制备R-TiO_(2)晶须及其生长机制研究
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作者 郭林秀 盖建丽 《中国陶瓷》 CAS CSCD 北大核心 2021年第9期65-72,共8页
一维金红石型纳米二氧化钛(R-TiO_(2))由于其特殊的结构,在可再生清洁能源领域被广泛研究和应用。本文以Ti_(3)Si_(1-x)Al_(x)C_(2)固溶体块体材料为基体,研究了Ti_(3)Si_(1-x)Al_(x)C_(2)固溶体中的Al含量、环境因素对R-TiO_(2)纳米晶... 一维金红石型纳米二氧化钛(R-TiO_(2))由于其特殊的结构,在可再生清洁能源领域被广泛研究和应用。本文以Ti_(3)Si_(1-x)Al_(x)C_(2)固溶体块体材料为基体,研究了Ti_(3)Si_(1-x)Al_(x)C_(2)固溶体中的Al含量、环境因素对R-TiO_(2)纳米晶须生长的影响。表明,随Ti_(3)Si_(1-x)Al_(x)C_(2)固溶体中的Al含量的增加,R-TiO_(2)长晶须逐渐生成,当x≥0.25时,表面排成列或扎堆生成约2μm的R-TiO_(2)长晶须;而纳米晶须随着O含量的增加生成量减少;升高温度,样品表面会生成α-Al_(2)O_(3)纳米片(x≥0.5时)。因此,Ti_(3)Si_(1-x)Al_(x)C_(2)固溶体在800℃、100 Pa条件下直接热处理成功制备出R-TiO_(2)纳米晶须,开发了一种简单且环境友好的方法。 展开更多
关键词 tio2 ti_(3)Si_(1-x)al_(x)C_(2) al_(2)o_(3) 纳米晶须 纳米片
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陶瓷-聚合物复合固态电解质膜的制备与性能研究 被引量:2
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作者 黄东雪 李锁 +4 位作者 姜兴涛 宁玉娟 张宇 伍澎贵 梁兴华 《广西科技大学学报》 2022年第1期123-129,共7页
NASICON型快离子导体Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)(LATP)具有较高的离子电导率、较宽的电化学窗口及良好的水和空气稳定性,但其界面接触性能差。石榴石型Li_(7)La_(3)Zr_(2)O_(12)(LLZO)锂离子电导率高、电化学窗口较宽且热稳定... NASICON型快离子导体Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)(LATP)具有较高的离子电导率、较宽的电化学窗口及良好的水和空气稳定性,但其界面接触性能差。石榴石型Li_(7)La_(3)Zr_(2)O_(12)(LLZO)锂离子电导率高、电化学窗口较宽且热稳定性好,但其立方相结构不稳定,影响其实际应用。采用溶液浇筑法,制备纯PVDF-LiTFSI电解质膜和以PVDF为基、3种不同质量比的Li_(6.4)La_(3)Zr_(1.4)Ta_(0.6)O_(12)(LLZTO)和Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)的固态电解质膜,并探讨纯PVDF-LiTFSI电解质膜和3种不同质量比的活性无机电解质填料对复合固态电解质离子电导率的影响。结果表明,Li_(6.4)La_(3)Zr_(1.4)Ta_(0.6)O_(12)和Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)质量比为1∶1时,电解质膜的XRD图谱的衍射峰比纯PVDF-LiTFSI下降更为明显,电化学窗口为3.9 V左右,表现出更好的稳定性。在不同温度下分别测量其离子电导率发现,Li_(6.4)La_(3)Zr_(1.4)Ta_(0.6)O_(12)和Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)质量比为1∶1时的电解质膜均高于纯PVDF-LiTFSI电解质膜和Li_(6.4)La_(3)Zr_(1.4)Ta_(0.6)O_(12)和Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)质量比为2∶1和3∶1时的电解质膜。将其装配成电池后发现,0.1C下电池首次充放电比容量分别为90 m A·h/g和87 m A·h/g。以0.5C的电流循环25圈,放电比容量从57 mA·h/g衰减至51mA·h/g,容量保持率为99.7%。所以,以PVDF为基、Li_(6.4)La_(3)Zr_(1.4)Ta_(0.6)O_(12)和Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)质量比为1∶1的固态电解质膜有优良的倍率性能和循环稳定性能。 展开更多
关键词 Li_(6.4)La_(3)Zr_(1.4)Ta_(0.6)o_(12) Li_(1+x)al_(x)ti_(2-x)(Po_(4))_(3) 聚偏氟乙烯 固体电解质 离子电导率
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