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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^(%PlUS%)电池 Al掺杂 li_(1%PlUS%x)Al_(x)Ti_(2-x)(PO_(4))_(3) li^(%PlUS%)迁移
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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
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作者 朱文慧 冯磊 +1 位作者 张克雄 朱俊 《物理学报》 SCIE EI CAS CSCD 北大核心 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
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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
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Zn_(3)(As_(1-x)P_(x))_(2)纳米结构制备及光谱特性研究
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作者 王浩 孙乃坤 +5 位作者 庞超 王志帅 陈上峰 李武 田辉 岱钦 《光谱学与光谱分析》 SCIE EI CAS CSCD 北大核心 2024年第7期1934-1939,共6页
Zn_(3)As_(2)与Zn_(3)P_(2)具有相同的伪立方晶格结构,它们具有较高的电子迁移率、较窄的直接带隙和良好的空气稳定性,在光电器件领域呈现出广泛的应用前景。目前关于Zn_(3)As2-Zn_(3)P_(2)固溶体纳米结构的研究相对较少,采用高气压烧... Zn_(3)As_(2)与Zn_(3)P_(2)具有相同的伪立方晶格结构,它们具有较高的电子迁移率、较窄的直接带隙和良好的空气稳定性,在光电器件领域呈现出广泛的应用前景。目前关于Zn_(3)As2-Zn_(3)P_(2)固溶体纳米结构的研究相对较少,采用高气压烧结技术得到Zn_(3)(As_(1-x)P_(x))_(2)(x=0、0.05、0.1)母合金,再利用化学气相沉积方法合成出多种形态的Zn_(3)(As_(1-x)P_(x))_(2)纳米结构,包括宏观尺寸的纳米带(长度3~10 mm;宽度1~4 mm;厚度约20μm)、纳米帆、纳米棒及纳米银簪等。系统的研究了P掺杂对相组成、元素含量、微结构以及光谱特性的影响。X射线衍射(XRD)结果表明,Zn_(3)(As_(1-x)P_(x))_(2)宏观纳米带样品的主相为α′相,随着P掺杂含量的增加,(224)衍射峰向右发生偏移,表明晶格常数减小。电子能谱分析显示P理论值(光致发光光谱)掺杂含量值x=0.05和x=0.1的Zn_(3)(As_(1-x)P_(x))_(2)母合金纳米带中P的实际含量分别为x=0.026及x=0.062。微结构分析表明,Zn_(3)As_(2)宏观纳米带的生长模式为沿〈221〉晶面菱形层状生长,P掺杂使纳米带的宏观尺寸减小,生长模式由菱形层状生长转变为纳米颗粒堆积层状生长。纳米带样品的拉曼光谱在79、97、198、320、428和1107 cm^(-1)出现特征峰,P掺杂导致拉曼光谱中1107 cm^(-1)特征峰发生蓝移,傅里叶红外光谱(FTIR)中1101和1599 cm^(-1)特征峰与PL谱中的300、422和635 nm特征峰也发生蓝移。Zn_(3)As_(2)与Zn_(3)(As_(0.974)P_(0.026))_(2)纳米带光电流与电压的线性关系良好,存在较好的欧姆特性,P掺杂后的Zn_(3)(As_(0.974)P_(0.026))2纳米带在900 nm条件下的光响应最为敏感。 展开更多
关键词 Zn_(3)(As_(1-x)P_(x))_(2) Zn_(3)As_(2)
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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
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拓扑绝缘体(Bi_(1-x)Sb_(x))_(2)Te_(3)薄膜制备及其电输运性能研究
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作者 张哲瑞 仇怀利 +3 位作者 周同 黄文宇 葛威锋 杨远俊 《合肥工业大学学报(自然科学版)》 CAS 北大核心 2023年第11期1580-1584,共5页
文章利用分子束外延(molecular beam epitaxy, MBE)法,在超高真空的条件下,于蓝宝石衬底上制备超薄的高质量拓扑绝缘体(Bi_(1-x)Sb_(x))_(2)Te_(3)薄膜。利用反射高能电子衍射(reflection high-energy electron diffraction, RHEED)仪、... 文章利用分子束外延(molecular beam epitaxy, MBE)法,在超高真空的条件下,于蓝宝石衬底上制备超薄的高质量拓扑绝缘体(Bi_(1-x)Sb_(x))_(2)Te_(3)薄膜。利用反射高能电子衍射(reflection high-energy electron diffraction, RHEED)仪、X射线衍射(X-ray diffraction, XRD)仪、显微共焦激光拉曼光谱仪(micro confocal laser Raman spectrometer)和X射线光电子能谱(X-ray photoelectron spectroscopy, XPS)仪对不同Sb掺杂量的样品进行表征,并获得最佳的制备参数。研究结果表明:衬底温度为460℃时Bi和Te的流量比为1∶16左右;在Sb温度为350、360、370、380℃时,可以制得高质量的(Bi_(1-x)Sb_(x))_(2)Te_(3)薄膜。利用霍尔效应测量系统测量样品的电阻率、霍尔系数、迁移率和载流子浓度;测量结果表明,(Bi_(1-x)Sb_(x))_(2)Te_(3)薄膜的载流子浓度和主要载流子类型随x的变化而发生相应的变化,并伴随着费米能级位置的调谐,随着x的增加,在x=0.53到x=0.68的掺杂过程中,费米能级从导带下移到带隙,最终进入价带,多数载流子类型也从自由电子转变成空穴,(Bi_(1-x)Sb_(x))_(2)Te_(3)实现了从n型到p型的转化。 展开更多
关键词 (MBE) (Bi_(1-x)Sb_(x))_(2)Te_(3)薄膜
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LiTi_(2)(PO_(4))_(3)修饰高镍单晶三元正极材料增强结构稳定性 被引量:1
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作者 李西安 冯彦彦 《电源技术》 CAS 北大核心 2023年第5期618-622,共5页
单晶LiNi_(1-x-y)Co_(x)Mn_(y)O_(2)(SCNCM,1-x-y>0.9)正极材料由于其特殊的晶体结构,与多晶NCM材料相比,具有更优越的循环寿命。然而,SCNCM在长循环过程中由于严重的副反应和不可逆相变,导致严重的容量退化。具有较高扩散系数的LiTi... 单晶LiNi_(1-x-y)Co_(x)Mn_(y)O_(2)(SCNCM,1-x-y>0.9)正极材料由于其特殊的晶体结构,与多晶NCM材料相比,具有更优越的循环寿命。然而,SCNCM在长循环过程中由于严重的副反应和不可逆相变,导致严重的容量退化。具有较高扩散系数的LiTi_(2)(PO_(4))_(3)(LTP)可以增强Li^(+)在电极和电解质之间的传递,并防止与空气和电解质的副反应。为了优化SCNCM的电化学性能,采用液相混合和固相烧结相结合的方法对其进行表面包覆,提高单晶SCNCM循环性能。X射线衍射(XRD)和高分辨透射电子显微镜(HRTEM)结果证实,SCNCM表面包覆一层30~50 nm的LTP涂层,改性后的样品在长循环后仍然可以保持良好的层状结构。具体地说,包覆0.8%(质量分数)LTP的SCNCM正极在0.5 C循环100圈后,放电比容量为151.2 mAh/g。 展开更多
关键词 liNi_(1-x-y)Co_(x)Mn_(y)O_(2)氧化物 NCM liTi_(2)(PO_(4))_(3)包覆
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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 ε-(Al_(x)Ga_(1-x))_(2)O_(3)/ε-Ga_(2)O_(3)异质结
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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 Zn_(0.15)Nb_(0.3)Ti_(0.55-x)(Co_(1/3)Nb_(2/3))_(x)O_(2) lTCC
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WO_(3)/CdS_(x)(CO_(3))_(1-X)的制备及其光催化析氢性能的研究
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作者 魏学刚 王梅 《青海师范大学学报(自然科学版)》 2022年第4期52-57,共6页
首先采用水热法合成了WO_(3)样品,其次利用水浴法在WO_(3)表面附着了CdS_(x)(CO_(3))_(1-X)材料并构建了直接Z型WO_(3)/CdS_(x)(CO_(3))_(1-X)光催化剂.实验结果表明,WO_(3)光激发的导带电子和CdS_(x)(CO_(3))_(1-X)光激发价带的空穴在... 首先采用水热法合成了WO_(3)样品,其次利用水浴法在WO_(3)表面附着了CdS_(x)(CO_(3))_(1-X)材料并构建了直接Z型WO_(3)/CdS_(x)(CO_(3))_(1-X)光催化剂.实验结果表明,WO_(3)光激发的导带电子和CdS_(x)(CO_(3))_(1-X)光激发价带的空穴在界面处发生了复合,使得WO_(3)价带的空穴和CdS_(x)(CO_(3))_(1-X)导带的电子实现分离,从而有效地提高了WO_(3)/CdS_(x)(CO_(3))_(1-X)复合光催化剂的光催化H_(2)的析出效率. 展开更多
关键词 - H_(2) WO_(3)/CdS_(x)(CO_(3))_(1-x)
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Al_(67)Mn_8Ti_(25)合金的解理裂纹 被引量:2
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作者 文九巴 戎咏华 +1 位作者 陈世朴 胡赓祥 《中国有色金属学报》 EI CAS CSCD 北大核心 1999年第3期488-492,共5页
利用Stroh 位错塞积模型解释了L12 结构Al67 Mn8Ti25 合金室温解理裂纹的萌生。计算表明,位错塞积优先在与滑移面成35 .3°方向诱发微裂纹, 导致解理断裂。经室温弯曲断口解理面取向的电子背散射衍射(E... 利用Stroh 位错塞积模型解释了L12 结构Al67 Mn8Ti25 合金室温解理裂纹的萌生。计算表明,位错塞积优先在与滑移面成35 .3°方向诱发微裂纹, 导致解理断裂。经室温弯曲断口解理面取向的电子背散射衍射(EBSD) 测试结果验证表明,L12 结构Al67 Mn8Ti25 合金室温解理断裂裂纹优先在{110} 展开更多
关键词 l1_2结构Al_3Ti
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Crystal structure,chemical bond characteristics,infrared reflection spectrum,and microwave dielectric properties of Nd_(2)(Zr_(1−x)Ti_(x))_(3)(MoO_(4))_(9) ceramics 被引量:6
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作者 Jian BAO Yuping ZHANG +2 位作者 Hideo KIMURA Haitao WU Zhenxing YUE 《Journal of Advanced Ceramics》 SCIE EI CAS CSCD 2023年第1期82-92,共11页
Microwave dielectric ceramics(MWDCs)with low dielectric constant and low dielectric loss are desired in contemporary society,where the communication frequency is developing to high frequency(sub-6G).Herein,Nd_(2)(Zr_(... Microwave dielectric ceramics(MWDCs)with low dielectric constant and low dielectric loss are desired in contemporary society,where the communication frequency is developing to high frequency(sub-6G).Herein,Nd_(2)(Zr_(1−x)Ti_(x))_(3)(MoO_(4))_(9)(NZ_(1−x)T_(x)M,x=0.02-0.10)ceramics were prepared through a solid-phase process.According to X-ray diffraction(XRD)patterns,the ceramics could form a pure crystal structure with the R3c(167)space group.The internal parameters affecting the properties of the ceramics were calculated and analyzed by employing Clausius-Mossotti relationship,Shannon’s rule,and Phillips-van Vechten-Levine(P-V-L)theory.Furthermore,theoretical dielectric loss of the ceramics was measured and analyzed by a Fourier transform infrared(IR)radiation spectrometer.Notably,when x=0.08 and sintered at 700℃,optimal microwave dielectric properties of the ceramics were obtained,including a dielectric constant(ε_(r))=10.94,Q·f=82,525 GHz(at 9.62 GHz),and near-zero resonant frequency temperature coefficient(τ_(f))=−12.99 ppm/℃.This study not only obtained an MWDC with excellent properties but also deeply analyzed the effects of Ti^(4+)on the microwave dielectric properties and chemical bond characteristics of Nd_(2)Zr_(3)(MoO_(4))_(9)(NZM),which laid a solid foundation for the development of rare-earth molybdate MWDC system. 展开更多
关键词 microwave dielectric ceramics(MWDCs) Nd_(2)(Zr_(1x)Ti_(x))_(3)(MoO_(4))_(9)(NZ_(1x)T_(x)M) Phillips-van Vechten-levine(P-V-l)theory theoretical dielectric loss
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Relationship between structure and properties of microwave dielectric ceramic Li_((1+x))2MgTi3O8 based on Li non-stoichiometry 被引量:2
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作者 Kui Liu Cheng Liu +2 位作者 Jie Li Lichuan Jin Huaiwu Zhang 《Journal of Materiomics》 SCIE CSCD 2023年第2期279-288,共10页
Li(_(1+x))2MgTi3O8(0.0≤x≤0.10)ceramics with Li non-stoichiometric ratios were prepared by the solidstate reaction method to inhibit the volatilization of Li.The effects of the Li non-stoichiometric ratios on the sin... Li(_(1+x))2MgTi3O8(0.0≤x≤0.10)ceramics with Li non-stoichiometric ratios were prepared by the solidstate reaction method to inhibit the volatilization of Li.The effects of the Li non-stoichiometric ratios on the sintering behavior,crystal structure,microscopic morphology,Raman vibrations,electron density,and dielectric properties of Li(_(1+x))2MgTi3O8 ceramics were systematically investigated.The Li(1+0.06)_(2)MgTi_(3)O_(8)ceramics demonstrate the best dielectric properties withεr=26.33,Q×f=69435 GHz(@6.87 GHz,54%improvement),tf=2.95×10^(-6)℃^(-1).For the non-intrinsic factors,the high relative density(97.15%)and larger grain size(16.78 mm)allow the dielectric properties to be improved.As for the intrinsic factors,a reasonable excess of Li improves the bond ionicity of the MgdO bond,the lattice energy of the TidO bond,and the electron cloud density,thus optimizing the dielectric properties.Raman spectroscopy leads to the same result from the point of view of lattice vibrations.At the same time,the distortion of the polyhedra is also improved,so that tf also approaches 0.The improved Li(1+0.06)2MgTi3O8 has potential applications in microwave communication technology. 展开更多
关键词 li(1%PlUS%x)_(2)MgTi_(3)O_(8) Raman vibration FIRST-PRINCIPlES P-V-l theory Microwave dielectric
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LATP固态电解质膜在准固态锂硫电池中的性能研究
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作者 翁海瑞 王晨瑶 +3 位作者 李明娟 孙陆毅 李媛 陈鑫智 《电源技术》 CAS 北大核心 2024年第8期1588-1594,共7页
为解决固态电解质与电极间的界面接触问题,实现锂硫电池固态化。用溶胶-凝胶法制备NASICON型Li_(1+x)Al_(x)Ti_(2−x)(PO_(4))_(3)氧化物固态电解质(LATP),用水基流延法制备固态电解质膜,将使用少量电解液润湿的LATP固态电解质膜组装成... 为解决固态电解质与电极间的界面接触问题,实现锂硫电池固态化。用溶胶-凝胶法制备NASICON型Li_(1+x)Al_(x)Ti_(2−x)(PO_(4))_(3)氧化物固态电解质(LATP),用水基流延法制备固态电解质膜,将使用少量电解液润湿的LATP固态电解质膜组装成准固态锂硫电池。制备的LATP离子电导率为1.61×10^(−4)S/cm。在30℃下,Li对称电池可稳定循环,循环时间超过500 h。该准固态电池室温下5 C放电,放电比容量340 mAh/g。在30℃、0.1 C下,初始放电比容量1043 mAh/g,100次循环后放电比容量430 mAh/g。 展开更多
关键词 li_(1%PlUS%x)Al_(x)Ti_(2x)(PO_(4))_(3)
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Mechanical properties of defective L1_(2)-Al_(3)X(X=Sc,Lu)phase:A first-principles study 被引量:2
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作者 Yu Wang Ya'nan Meng +2 位作者 Junsheng Wang Chi Zhang Houbing Huang 《Journal of Rare Earths》 SCIE EI CAS CSCD 2021年第2期217-224,共8页
The mechanical properties of Al_(3)X(X=Sc,Lu)were studied by density functional theory(DFT).The elastic constants and formation enthalpy indicate that the L1_(2)-Al_(3)X(X=Sc and Lu)are mechanically and thermodynamica... The mechanical properties of Al_(3)X(X=Sc,Lu)were studied by density functional theory(DFT).The elastic constants and formation enthalpy indicate that the L1_(2)-Al_(3)X(X=Sc and Lu)are mechanically and thermodynamically stable.The bulk moduli and shear moduli show that Al_(3)Sc has better resistance to volume and shape changes than AI3 Lu.However,the calculated results show that Al_(3)Lu has better plasticity than Al_(3)Sc.The properties of structural stability and elastic moduli of the crystal containing four major types of point defects in L1_(2)-Al_(3)X(X=Sc and Lu)were calculated.The mechanical properties of point defects show that point defects cause L1_(2)-Al_(3)X lattice distortion and change the corresponding elastic constants.Point defects reduce the Young’s,shear and bulk moduli but have little effects on the crystal brittleness and toughness of Al_(3)Sc and Al_(3)Lu.Therefore,we have found that Lu addition into aluminum alloys is a very good replacement for expensive Sc addition when the L1_(2)structures are desired for nucleation or strengthening precipitates in aluminum alloys. 展开更多
关键词 Density functional theory FIRST-PRINCIPlE l1_(2)-al_(3)x Mechanical property Defects Rare earths
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PTN+L3网络承载TD-LTE移动回传的OAM运维工具研究 被引量:1
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作者 李芳 徐云斌 +1 位作者 赵俊峰 李伟 《电信网技术》 2012年第12期15-18,共4页
研究了PTN+L3网络传送TD-LTE的S1和X2业务的运维需求,为实现快速故障定位和端到端时延性能测量,创新性提出了基于Y.1731的端到端OAM运维工具,为后续TD-LTE规模商用的PTN+L3网络运维提供了高效工具。
关键词 PTN%PlUS%l3 TD-lTE l3VPN OAM S1 x2
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Crystal structure and enhanced microwave dielectric properties of the Ce_(2)[Zr_(1−x)(Al_(1/2)Ta_(1/2))_(x)]_(3)(MoO_(4))_(9) ceramics at microwave frequency 被引量:6
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作者 Chao FENG Xu ZHOU +2 位作者 Bingjing TAO Haitao WU Shifeng HUANG 《Journal of Advanced Ceramics》 SCIE EI CAS CSCD 2022年第3期392-402,共11页
Dense microwave dielectric ceramics of Ce_(2)[Zr_(1−x)(Al_(1/2)Ta_(1/2))_(x)]_(3)(MoO_(4))_(9)(CZMAT) (x = 0.02–0.10) were prepared by the conventional solid-state route. The effects of (Al1/2Ta1/2)^(4+) on their mic... Dense microwave dielectric ceramics of Ce_(2)[Zr_(1−x)(Al_(1/2)Ta_(1/2))_(x)]_(3)(MoO_(4))_(9)(CZMAT) (x = 0.02–0.10) were prepared by the conventional solid-state route. The effects of (Al1/2Ta1/2)^(4+) on their microstructures, sintering behaviors, and microwave dielectric properties were systematically investigated. On the basis of the X-ray diffraction (XRD) results, all the samples were matched well with Pr_(2)Zr_(3)(MoO_(4))_(9) structures, which belonged to the space group R3¯c. The lattice parameters were obtained using the Rietveld refinement method. The correlations between the chemical bond parameters and microwave dielectric properties were calculated and analyzed by using the Phillips—Van Vechten—Levine (P—V—L) theory. Excellent dielectric properties of Ce_(2)[Zr_(0.94)(Al_(1/2)Ta_(1/2))_(0.06)]_(3)(MoO_(4))_(9) with a relative permittivity (ε_(r)) of 10.46, quality factor (Q × f) of 83,796 GHz, and temperature coefficient of resonant frequency (τ_(f)) of −11.50 ppm/℃ were achieved at 850 ℃. 展开更多
关键词 microwave dielectric ceramics Ce_(2)[Zr_(1x)(Al_(1/2)Ta_(1/2))_(x)]_(3)(MoO_(4))_(9)(CZMAT) Phillips-Van Vechten-levine(P-V-l)theory low sintering temperature
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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:6
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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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Progress and perspective of Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3) ceramic electrolyte in lithium batteries 被引量:8
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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%PlUS%x)Al_(x)Ti_(2-x)(PO_(4))_(3) lithium batteries
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移动PTN-L3核心层POOL模式的应用研究 被引量:2
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作者 黄晓强 《电信快报(网络与通信)》 2015年第10期22-25,39,共5页
随着近年中国移动TD-LTE网络大规模建设,无线基站传送流量持续增长,同时核心层EPC(分组核心演进)采用异址建POOL池模式,严重影响传送网PTN-L3网络架构及容量的规划与建设。文章基于TD-LTE系统e NB基站流量对移动PTN-L3的网络要求,在满... 随着近年中国移动TD-LTE网络大规模建设,无线基站传送流量持续增长,同时核心层EPC(分组核心演进)采用异址建POOL池模式,严重影响传送网PTN-L3网络架构及容量的规划与建设。文章基于TD-LTE系统e NB基站流量对移动PTN-L3的网络要求,在满足业务发展需求的同时,分析移动PTN-L3核心层网络的传送效益,研究移动PTN-L3核心层的网络目标架构,并统一规划、逐步部署。 展开更多
关键词 PTN—l3核心层 POOl S1 x2
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