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固态电解质Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)中Li+的迁移特性
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作者 李梅 钟淑英 +2 位作者 胡军平 孙宝珍 徐波 《物理学报》 SCIE EI CAS CSCD 北大核心 2024年第13期356-366,共11页
Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)(LATP)是一种颇具前景的NASICON型锂离子固态电解质.本文通过第一性原理计算研究了不同Al掺杂浓度(x=0.00,0.16,0.33,0.50)对LATP的结构特性、电学特性以及Li^(+)迁移特性的影响.结果表明,Al能够稳... Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)(LATP)是一种颇具前景的NASICON型锂离子固态电解质.本文通过第一性原理计算研究了不同Al掺杂浓度(x=0.00,0.16,0.33,0.50)对LATP的结构特性、电学特性以及Li^(+)迁移特性的影响.结果表明,Al能够稳定掺杂进入LiTi2(PO4)3(LTP)的晶体结构当中.当Al掺杂浓度x=0.16时,Li—O键的平均键长最长,成键强度最弱,而Ti—O键强度随Al掺杂浓度变化不大.Al掺杂浓度对LATP带隙的影响不大,但Al附近的O原子聚集了更多的负电荷,形成AlO6极化中心.Li^(+)不同的迁移方式(空位迁移、间隙位迁移和协同迁移)在Al掺杂浓度不同时展现出复杂的能垒变化,Li^(+)在空位迁移中迁移势垒随Al掺杂浓度的增大而升高,而在间隙位迁移中Li^(+)的迁移势垒变化相反,由于协同迁移中涉及空位和间隙位两种位点,Li^(+)的迁移势垒表现为随Al掺杂浓度的升高先降低后升高的复杂变化.当x=0.50时,LATP具有最低的Li^(+)迁移势垒0.342 eV,这个势垒值是间隙位迁移的结果.因此,通过改变Al掺杂浓度,可改变间隙Li^(+)浓度及迁移通道结构,进而调节Li^(+)的迁移性能,提高LATP中的Li^(+)导电性能. 展开更多
关键词 全固态Li^(+)电池 AL掺杂 Li_(1+x)Al_(x)ti_(2-x)(PO_(4))_(3) Li^(+)迁移
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Ti_(x)-Ni_(1-x)-MOFs的制备及其CO选择性催化还原NO_(x)研究 被引量:3
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作者 石勇 李橙 +4 位作者 黄磊 熊巍 肇启东 孙健恒 丁越 《中国环境科学》 EI CAS CSCD 北大核心 2022年第11期5080-5087,共8页
采用溶剂热法和微波法合成了不同比例的Ti_(x)-Ni_(1-x)-MOFs材料,并用于以CO为还原剂的选择性催化脱硝反应.结果表明,双金属Ti_(x)-Ni_(1-x)-MOFs的NO还原率显著高于单金属Ni-MOF,且反应温度窗口更宽,其中,Ti_(0.2)-Ni_(0.8)-MOF表现... 采用溶剂热法和微波法合成了不同比例的Ti_(x)-Ni_(1-x)-MOFs材料,并用于以CO为还原剂的选择性催化脱硝反应.结果表明,双金属Ti_(x)-Ni_(1-x)-MOFs的NO还原率显著高于单金属Ni-MOF,且反应温度窗口更宽,其中,Ti_(0.2)-Ni_(0.8)-MOF表现出最佳的脱硝效率,在200~400℃温度范围达到100%的转化率.通过XRD,FT-IR,SEM,TGA,XPS,N2吸脱附等表征手段发现,Ti掺杂Ni-MOF后有利于改善原子分散性,Ti、Ni间金属的相互作用有利于产生丰富的高效Ni-O-Ti位点,加强Ni^(2+)+Ti^(4+)↔Ni^(3+)+Ti^(3+)氧化还原循环,从而明显提高了NO+CO催化反应性能.与溶剂热法相比,微波法制备Ti_(0.2)-Ni_(0.8)-MOF具有合成效率高、结晶度好、晶粒细小均匀的优势,并进一步提高了其低温脱硝效果. 展开更多
关键词 CO-SCR 金属有机骨架 ti_(x)-ni_(1-x)-mofs 微波法 溶剂热法
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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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Li_(1-x)Bi_(4+x)Ti_(4)O_(15)薄膜制备与表征 被引量:1
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作者 孟靖华 杨丽清 焦斌权 《无机盐工业》 CAS 北大核心 2018年第9期34-37,共4页
在LiNO_3/SiO_2/Si基板上制备了Li_(1-x)Bi_(4+x)Ti_4O_(15)系列薄膜(x=0.3、0.4、0.5、0.6),并系统分析了这些薄膜的微观结构以及铁电、介电及漏电等电学特性。研究结果表明,在氮气气氛中以600℃持温30 min制备的单一相薄膜中Li0.5Bi4.... 在LiNO_3/SiO_2/Si基板上制备了Li_(1-x)Bi_(4+x)Ti_4O_(15)系列薄膜(x=0.3、0.4、0.5、0.6),并系统分析了这些薄膜的微观结构以及铁电、介电及漏电等电学特性。研究结果表明,在氮气气氛中以600℃持温30 min制备的单一相薄膜中Li0.5Bi4.5Ti4O15薄膜的结晶效果最好,且在其表面可成长出独立晶粒分布状态;x为0.5时薄膜的剩余极化强度2Pr=53.5μC/cm2、矫顽场2Ec=144.2 k V/cm,此时薄膜的铁电性能相对最佳;该系列薄膜的介电常数介于37~100,介电损失相对偏高,介于0.7~1.0;所有薄膜的漏电流均随外加电压的增加而逐渐增大,其中Li0.5Bi4.5Ti4O15薄膜漏电流最小,外加电压为10 V时其值约为3.88×10-6A。 展开更多
关键词 铋层状钙钛矿结构 Li_(1-x)Bi_(4+x)ti_(4)O_(15)薄膜 铁电特性 介电特性 漏电流
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Al质量分数对磁控溅射Ti_(1-x)Al_(x)N薄膜结构和摩擦学性能的影响 被引量:1
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作者 张世玺 蔡海潮 +2 位作者 薛玉君 畅为航 田昌龄 《河南科技大学学报(自然科学版)》 CAS 北大核心 2021年第4期1-6,M0002,共7页
针对TiAlN薄膜耐磨性不够优异的问题,研究了Al质量分数对Ti_(1-x)Al_(x)N薄膜结构和摩擦学性能的影响。采用磁控溅射沉积技术制备了4种不同Al质量分数的Ti_(1-x)Al_(x)N薄膜。利用扫描电镜(SEM)、能谱仪(EDS)及X射线衍射仪(XRD),对薄膜... 针对TiAlN薄膜耐磨性不够优异的问题,研究了Al质量分数对Ti_(1-x)Al_(x)N薄膜结构和摩擦学性能的影响。采用磁控溅射沉积技术制备了4种不同Al质量分数的Ti_(1-x)Al_(x)N薄膜。利用扫描电镜(SEM)、能谱仪(EDS)及X射线衍射仪(XRD),对薄膜的微观形貌、元素成分与晶体结构进行了表征。采用纳米压痕仪测试薄膜的硬度和弹性模量,用摩擦磨损试验机和白光干涉三维形貌仪测试薄膜的摩擦磨损性能。研究结果表明:随着Al质量分数在一定范围内的增加,薄膜从沿c-TiN(111)晶面生长逐渐转向h-AlN(200)晶面择优取向,Ti_(1-x)Al_(x)N薄膜疏松结构得到了改善,柱状结晶发生细化,表面形貌更加致密。同时,Ti_(1-x)Al_(x)N薄膜的硬度和弹性模量得到提高,磨损机理由严重的磨粒磨损、黏着磨损转变为轻微的磨粒磨损,平均体积磨损率降低。Ti_(0.67)Al_(0.33)N薄膜的综合性能最优,硬度和弹性模量分别为14.059 GPa和203.37 GPa,摩擦因数最低为0.182,平均体积磨损率为1.321×10^(-8)mm^(3)/(N·m),呈现出较好的摩擦学性能。 展开更多
关键词 Al质量分数 磁控溅射 ti_(1-x)Al_(x)N薄膜 摩擦学性能
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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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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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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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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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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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Nb掺杂对微波制备TiCoSb Half-Heusler合金热电性能的提升
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作者 张瑞鹏 孔建彪 +6 位作者 侯仰博 薄琳 王文莹 王兴隆 赵令浩 祝军亮 赵德刚 《山东科学》 CAS 2024年第2期47-54,共8页
TiCoSb Half-Heusler合金固有的高导热性,以及传统制备方法制备周期长、成本高等缺点限制了其商业化应用。采用微波合成与急速热压烧结相结合的方法成功制备了低热导率的Ti_(1-x)Nb_(x)CoSb Half-Heusler合金,大大缩短了制备周期,同时... TiCoSb Half-Heusler合金固有的高导热性,以及传统制备方法制备周期长、成本高等缺点限制了其商业化应用。采用微波合成与急速热压烧结相结合的方法成功制备了低热导率的Ti_(1-x)Nb_(x)CoSb Half-Heusler合金,大大缩短了制备周期,同时提高了TiCoSb Half-Heusler合金的致密度。研究了Ti位Nb取代对Ti_(1-x)Nb_(x)CoSb Half-Heusler热电材料的相组成、成分分布及热电输运性能的影响。在功率因子增加和晶格热导率降低的共同作用下,Ti_(1-x)Nb_(x)CoSb样品的热电优值(ZT)得到显著优化。在725 K时,Ti 0.93 Nb 0.07 CoSb样品的最大ZT值为0.1,比相同工艺下制备的TiCoSb纯相样品高两个数量级。 展开更多
关键词 Half-Heusler合金 ti_(1-x)Nb_(x)CoSb 微波 热电性能
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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:7
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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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Structure characteristics and microwave dielectric properties of Pr_(2)(Zr_(1-x)Ti_(x))_(3)(MoO_(4))_(9) solid solution ceramic with a stable temperature coefficient 被引量:5
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作者 Huanrong Tian Jinjie Zheng +4 位作者 Lintao Liu Haitao Wu Hideo Kimura Yizhong Lu Zhenxing Yue 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2022年第21期121-129,共9页
Pr_(2)(Zr_(1−x)Ti_(x))_(3)(MoO_(4))_(9)(x=0.1-1.0)ceramics were prepared via a conventional solid-state method,the dependence of crystal structure and bond characteristics on microwave dielectric properties was invest... Pr_(2)(Zr_(1−x)Ti_(x))_(3)(MoO_(4))_(9)(x=0.1-1.0)ceramics were prepared via a conventional solid-state method,the dependence of crystal structure and bond characteristics on microwave dielectric properties was investigated systemically.The X-ray diffraction patterns indicated that the single-phase Pr_(2)Zr_(3)(MoO_(4))_(9)structure was formed in all the specimens.As the Ti^(4+)content increased,the lattice volume gradually decreased,which was ascribed to the fact that the ionic radius of Ti^(4+)was smaller than that of Zr^(4+).Notably,outstanding microwave dielectric properties withεr of 10.73-16.35,Q·f values of 80,696-18,726 GHz and minorτ_(f) values−14.1-−2.6 ppm/℃were achieved in Pr_(2)(Zr_(1−x)Ti_(x))_(3)(MoO_(4))_(9)ceramics.Theε_(r) increased with the rising x values,which was associated with the increase ofα/Vm values.The decreasing Q·f was affected by the decline of lattice energy of[Zr/TiO_(6)]octahedral.Theτf value was dominated by[Zr/TiO_(6)]octahedral distortion,Mo-O bond energy,bond strength and B-site bond valence.Furthermore,infrared reflection spectra suggested that the properties were mainly caused by the absorption of phonon,and the dielectric loss could be further reduced by optimizing the experimental process. 展开更多
关键词 Pr_(2)(Zr_(1-x)ti_(x))_(3)(MoO_(4))_(9) Normalized bond length Bond characteristics Raman spectra
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Stabilization of the Anatase Phase of Ti_(1-x)Sn_(x)O_(2) (x < 0.5) Nanofibers 被引量:2
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作者 Kandasami Asokan Jae Young Park +2 位作者 Sunwoo Choi Changhwan Chang Sang Sub Kim 《Nano Research》 SCIE EI CSCD 2010年第4期256-263,共8页
We experimentally investigate the stabilization of the anatase phase of Ti_(1-x)Sn_(x)O_(2)(x<0.5)nanofibers when synthesized by an electrospinning method.The as-spun nanofibers became nano-grained,polycrystalline ... We experimentally investigate the stabilization of the anatase phase of Ti_(1-x)Sn_(x)O_(2)(x<0.5)nanofibers when synthesized by an electrospinning method.The as-spun nanofibers became nano-grained,polycrystalline nanofibers after calcination and the diameters of the nanofibers depend on Sn content.Stabilization of the anatase phase in Ti-rich compositions and incorporation of Sn ions were confirmed by X-ray diffraction,Raman,X-ray absorption near-edge structure,and photoluminescence(PL)spectroscopies.Results from the PL study also demonstrated the tunable nature of the optical properties,with the emission maximum shifting towards higher wavelength with increasing Sn concentration. 展开更多
关键词 Electrospinning nanofiber ti_(1-x)Sn_(x)O_(2) x-ray absorption near-edge structure(xANES)
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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 被引量:1
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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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A comprehensive study on Li_(4)Si_(1-x)Ti_(x)O_(4) ceramics for advanced tritium breeders
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作者 Yichao GONG Lin LIU +6 位作者 Jianqi QI Mao YANG Junjie LI Hailiang WANG Hao GUO Guojun ZHANG Tiecheng LU 《Journal of Advanced Ceramics》 SCIE CAS CSCD 2020年第5期629-640,共12页
Hetero-element doped lithium orthosilicates have been considered as advanced tritium breeders due to the superior performances.In this work,Li_(4)Si_(1-x)Ti_(x)O_(4) ceramics were prepared by proprietary hydrothermal ... Hetero-element doped lithium orthosilicates have been considered as advanced tritium breeders due to the superior performances.In this work,Li_(4)Si_(1-x)Ti_(x)O_(4) ceramics were prepared by proprietary hydrothermal process and multistage reactive sintering.The reaction mechanism of Li_(4)Si_(1-x)Ti_(x)O_(4) was put forward.XRD and SEM analyses indicate that insertion of Ti leads to lattice expansion,which promotes the grain growth and changes the fracture mode.The compressive tests show that the crush load increases almost four times by increasing x from 0 to 0.2.However,the thermal conductivity and ionic conductivity are the best when x=0.05 and x=0.1,respectively.Thermal cycling stability of Li_(4)Si_(1-x)Ti_(x)O_(4) pebbles was further appraised through investigating the changes of microstructure and crush load.After undergoing thermal cycling,the Li_(4)Si_(1-x)Ti_(x)O_(4) still show higher crush load compared with Li_(4)SiO_(4),despite Ti segregation in some samples.The x=0.05 sample exhibits excellent thermal cycling stability.In summary,proper amount of Ti doping can improve the crush load,thermal and ionic conductivity,and thermal cycling stability of Li_(4)SiO_(4). 展开更多
关键词 tritium ceramic breeders Li_(4)Si_(1-x)ti_(x)O_(4) solid solutions crush load conductivity thermal cycling
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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:4
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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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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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