期刊文献+
共找到17篇文章
< 1 >
每页显示 20 50 100
固态电解质Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3)中Li+的迁移特性
1
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 Li^(%PLUS%) al掺杂 Li_(1+x)al_(x)Ti_(2-x)(Po_(4))_(3) Li^(%PLUS%)
下载PDF
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
2
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
下载PDF
高温扩散工艺制备带隙可调的β-(Al_(x)Ga_(1-x))_(2)O_(3)薄膜
3
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
下载PDF
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
4
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 ε-(al_(x)ga_(1-x))_(2)o_(3)/ε-ga_(2)o_(3)异质结
下载PDF
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
5
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 Zn_(0.15)Nb_(0.3)Ti_(0.55-x)(Co_(1/3)Nb_(2/3))_(x)o_(2) LTCC
下载PDF
Al纳米孔阵列/(Al_(x)Ga_(1-x))_(2)O_(3)薄膜中的紫外波段超常透射
6
作者 朱文慧 冯磊 +1 位作者 张克雄 朱俊 《物理学报》 SCIE EI CAS 2024年第20期156-164,共9页
采用有限差分时域算法计算(Al_(x)Ga_(1-x))_(2)O_(3)薄膜衬底上的周期性三角晶格Al纳米孔阵列的透过率,研究不同(Al_(x)Ga_(1-x))_(2)O_(3)衬底的Al组分x以及Al纳米孔阵列的厚度、孔径和周期对其光学传输特性的影响.数值计算结果表明,... 采用有限差分时域算法计算(Al_(x)Ga_(1-x))_(2)O_(3)薄膜衬底上的周期性三角晶格Al纳米孔阵列的透过率,研究不同(Al_(x)Ga_(1-x))_(2)O_(3)衬底的Al组分x以及Al纳米孔阵列的厚度、孔径和周期对其光学传输特性的影响.数值计算结果表明,当x=0时,在263 nm和358 nm波长范围处出现两个强透射峰,随着x的增大,其中位于263 nm处的透射峰发生轻微蓝移,强度则先增强后下降;358 nm处的透射峰发生明显蓝移且不断加强.若纳米孔阵列的周期不变,随着空气柱孔径增大时,紫外波段两强透射峰峰值位置分别位于244 nm和347 nm处,两峰均先发生红移再蓝移,透过率不断增大,反射率减小.随着周期扩大,紫外波段两强透射峰分别位于249 nm和336 nm处,两透射峰均发生明显红移,其中249 nm处的透射峰红移至304 nm,336 nm处的透射峰红移至417 nm,并且透过率不断降低.随着Al厚度的增大,位于380 nm处的透射峰峰值位置发生蓝移,且透过率不断下降.本文数据集可在https://doi.org/10.57760/sciencedb.j00213.00036中访问获取. 展开更多
关键词 (al_(x)ga_(1-x))_(2)o_(3) al
下载PDF
La_(1-x)Ce_(x)MnO_(3)-Ba/Al_(2)O_(3)催化剂对NO选择性生成NH_(3)的影响
7
作者 宋崇林 郑庆贺 +3 位作者 吕誉 崔立峰 李云强 吕刚 《天津大学学报(自然科学与工程技术版)》 EI CAS 2024年第10期1053-1061,共9页
为了实现碳中和目标,降低内燃机碳排放,稀薄燃烧技术成为了当前重要的研究方向.该技术不仅能提高发动机燃油热效率,还能有效降低CO_(2)排放.但是稀薄燃烧往往会伴随着大量氮氧化物的产生,为了解决该问题,采用LNT-SCR耦合的NO_(x)净化技... 为了实现碳中和目标,降低内燃机碳排放,稀薄燃烧技术成为了当前重要的研究方向.该技术不仅能提高发动机燃油热效率,还能有效降低CO_(2)排放.但是稀薄燃烧往往会伴随着大量氮氧化物的产生,为了解决该问题,采用LNT-SCR耦合的NO_(x)净化技术,此时LNT的作用是将排气中部分NO_(x)转化为NH_(3),为下游的SCR提供还原剂.基于此,制备了LNT催化剂,研究催化剂对NO选择性生成NH_(3)的影响.采用溶胶-凝胶法制备了La_(1-x)Ce_(x)MnO_(3)系列钙钛矿氧化物,并通过分步浸渍法得到了La_(1-x)Ce_(x)MnO_(3)-Ba/Al_(2)O_(3)负载型催化剂.利用XRD、H_(2)-TPR、NO-TPD等表征手段研究了钙钛矿氧化物的晶相结构,以及负载型催化剂的还原特性、NO_(x)吸附-脱附性能等物化性质,并且通过H_(2)选择性催化还原NO实验探究了催化剂掺杂Ce对NO转化成NH_(3)的影响.结果表明,Ce掺杂催化剂具有良好的NH_(3)产物选择性,并且显著提高了NO转化率.温度是NO转化和NH_(3)产物选择性生成的决定性因素,而H_(2)和NO体积比是NO转化和NH_(3)产物选择性生成的关键性因素.其中,La_(0.95)Ce_(0.05)MnO_(3)-Ba/Al_(2)O_(3)在低温下催化活性表现最佳,在350℃、H_(2)和NO体积比为5.0时NH_(3)产物选择性为65%,NO转化率为100%.此外,所制备的La_(1-x)Ce_(x)MnO_(3)都形成了钙钛矿型结构,而且Ce掺杂催化剂的大部分Ce离子可以进入到LaMnO_(3)结构中.在催化剂适量掺杂Ce后,H_(2)消耗总面积增大、还原峰的峰值温度降低,表明掺杂Ce改善了催化剂的还原特性;同时NO吸附和脱附面积增大,表明Ce掺杂改变了催化剂的NO_(x)吸附-脱附性能. 展开更多
关键词 La_(1-x)Ce_(x)Mno_(3)-Ba/al_(2)o_(3)催化剂 H_(2)选择性催化还原No NH_(3)产物选择性 No转化率 No_(x)吸附-脱附
下载PDF
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
8
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 al-Mgo-al_(2)o_(3)耐火材料 (al_(2)oC)x(alN)1-x
下载PDF
Progress and perspective of Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3) ceramic electrolyte in lithium batteries 被引量:8
9
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
原文传递
Preparation of the Solid Electrolytes Li_(4+x)Al_xSi_(1-x)O_4-yAl_2O_3 by the Sol-Gel Method and Study of Their Ionic Conductivity
10
作者 陈汝芬 宋秀芹 《Chinese Journal of Chemistry》 SCIE CAS CSCD 2002年第1期18-21,共4页
The Li_(4+x)Al_xSi_(1-x)O_(4-y)Al_2O_3 (x = 0 to 0.5, y = 0 to 0.5) ionconductors were prepared by the Sol-Gel method and examined in detail. The powder and sinteredsamples were characterized by TG-DTA, XRD, SEM, and ... The Li_(4+x)Al_xSi_(1-x)O_(4-y)Al_2O_3 (x = 0 to 0.5, y = 0 to 0.5) ionconductors were prepared by the Sol-Gel method and examined in detail. The powder and sinteredsamples were characterized by TG-DTA, XRD, SEM, and AC impedance techniques. The experimentalresults show that the conductivity and sinterability increase with the amount of excess Al_2O_3 inthe silicate. The particle size of the powder samples is about 0.13 μm. The maximum conductivity at18 ℃ is 3.057 * 10^(-5) s/cm for Li_(4.4)Al_(0.4)Si_(0.6)O_4-0.3 Al_2O_3. 展开更多
关键词 Li_(4+x)al_xSi_(1-x)o_(4-y)al_2o_3 solid electrolyte ionic conductivity sol-gel method
原文传递
直接热处理法制备R-TiO_(2)晶须及其生长机制研究
11
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)
下载PDF
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 被引量:2
12
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
原文传递
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
13
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.
原文传递
Band-gap tunable(Ga_(x)In_(1−x))_(2)O_(3)layer grown by magnetron sputtering
14
作者 Fabi ZHANG Jinyu SUN +11 位作者 Haiou LI Juan ZHOU Rong WANG Tangyou SUN Tao FU Gongli XIAO Qi LI Xingpeng LIU Xiuyun ZHANG Daoyou GUO Xianghu WANG Zujun QIN 《Frontiers of Information Technology & Electronic Engineering》 SCIE EI CSCD 2021年第10期1370-1378,共9页
Multicomponent oxide(Ga_(x)In_(1−x))_(2)O_(3)films are prepared on(0001)sapphire substrates to realize a tunable band-gap by magnetron sputtering technology followed by thermal annealing.The optical properties and ban... Multicomponent oxide(Ga_(x)In_(1−x))_(2)O_(3)films are prepared on(0001)sapphire substrates to realize a tunable band-gap by magnetron sputtering technology followed by thermal annealing.The optical properties and band structure evolution over the whole range of compositions in ternary compounds(Ga_(x)In_(1−x))_(2)O_(3)are investigated in detail.The X-ray diffraction spectra clearly indicate that(Ga_(x)In_(1−x))_(2)O_(3)films with Ga content varying from 0.11 to 0.55 have both cubic and monoclinic structures,and that for films with Ga content higher than 0.74,only the monoclinic structure appears.The transmittance of all films is greater than 86%in the visible range with sharp absorption edges and clear fringes.In addition,a blue shift of ultraviolet absorption edges from 380 to 250 nm is noted with increasing Ga content,indicating increasing band-gap energy from 3.61 to 4.64 eV.The experimental results lay a foundation for the application of transparent conductive compound(Ga_(x)In_(1−x))_(2)O_(3)thin films in photoelectric and photovoltaic industry,especially in display,light-emitting diode,and solar cell applications. 展开更多
关键词 (ga_(x)In_(1−x))_(2)o_(3)films Band-gap tunable Magnetron sputtering
原文传递
Ga-Cd-O的电子结构和光学性质的第一性原理计算
15
作者 张法碧 苗国斌 +2 位作者 张荣辉 周娟 周飞 《桂林电子科技大学学报》 2022年第2期87-94,共8页
采用基于密度泛函理论的第一性原理计算方法,研究了Cd掺杂对β-Ga_(2)O_(3)物理性能的影响。通过建立β-Ga_(2)O_(3)模型,用Cd原子替代部分的Ga原子后构建了不同Cd掺杂量模型(Cd_(x)Ga_(1-x))_(2)O_(3)(x=12.5%、25%、50%),然后对不同... 采用基于密度泛函理论的第一性原理计算方法,研究了Cd掺杂对β-Ga_(2)O_(3)物理性能的影响。通过建立β-Ga_(2)O_(3)模型,用Cd原子替代部分的Ga原子后构建了不同Cd掺杂量模型(Cd_(x)Ga_(1-x))_(2)O_(3)(x=12.5%、25%、50%),然后对不同的掺杂模型进行了几何结构优化,获得了稳定的晶格结构和晶格参数,并对它们的能带结构、态密度以及光学性质等进行了分析。计算结果表明,Cd掺杂会导致β-Ga_(2)O_(3)晶胞体积增大,稳定性减小。随着Cd掺杂浓度的增加,(Cd_(x)Ga_(1-x))_(2)O_(3)体系的带隙表现出先减小后增大的趋势;并且随着Cd掺杂量的不同(12.5%、25%、50%),掺杂体系(Cd_(x)Ga_(1-x))_(2)O_(3)的材料性质发生了变化,由β-Ga_(2)O_(3)的间接带隙材料先变为直接带隙材料(Cd浓度为12.5%、25%),然后又变回到间接带隙材料(Cd浓度为50%)。此外,掺入Cd后降低了体系在一定能量范围内(6~25 eV)的吸收系数和反射率,从而提高了透光率。以上研究表明,选择合适的掺杂浓度可以实现光电性质丰富可调的(Cd_(x)Ga_(1-x))_(2)O_(3)合金材料。 展开更多
关键词 (Cd_(x)ga_(1-x))_(2)o_(3)合金 β-ga_(2)o_(3)
下载PDF
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
16
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)
下载PDF
Giant piezotronic effect in ferroelectric field effect transistor
17
作者 Haiming Zhang Mengshuang Chi +6 位作者 Shidai Tian Tian Liang Jitao Liu Xiang Zhang Lingyu Wan Zhong Lin Wang Junyi Zhai 《Nano Research》 SCIE EI CSCD 2024年第9期8465-8471,共7页
The piezotronics effect utilizes a piezopotential to modulate and control current in piezo-semiconductors.Ferroelectric materials,as a type of piezoelectric materials,possess piezoelectric coefficients that are signif... The piezotronics effect utilizes a piezopotential to modulate and control current in piezo-semiconductors.Ferroelectric materials,as a type of piezoelectric materials,possess piezoelectric coefficients that are significantly larger than those found in conventional piezoelectric materials.Here,we propose a strain modulated ferroelectric field-effect transistor(St-FeFET)utilizing external strain instead of gate voltage to achieve ferroelectric modulation,which eliminates the need for gate voltage.By applying a very small strain(0.01%),the St-FeFET can achieve a maximum on-off current ratio of 1250%and realizes a gauge factor(GF)of 1.19×10^(6),which is much higher than that of conventional strain sensors.This work proposes a new method for realizing highly sensitive strain sensors and presents innovative approaches to the operation methods of ferroelectric field-effect transistors as well as potential applications for coupling of strain sensors and various devices across different fields. 展开更多
关键词 ferroelectric field-effect transistors piezotronics [Pb(Mg_(1/3)Nb_(2/3))o_(3)]_((1-x)^(-))[PbTio_(3)]_(x)(PMN-PT) strain sensors
原文传递
上一页 1 下一页 到第
使用帮助 返回顶部