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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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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 Li^(%PLUS%) AL Li_(1+x)Al_(x)Ti_(2-x)(PO_(4))_(3) Li^(%PLUS%)
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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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溶剂热法制备CuIn(S_xSe_(1-x))_2纳米粉体的微观结构与光学特性
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作者 段文杰 段学臣 +2 位作者 李历历 夏慧 朱奕漪 《粉末冶金材料科学与工程》 EI 北大核心 2015年第1期86-92,共7页
以乙醇胺为溶剂,以氯化铟、氯化铜、硫化钠、硒粉为原料,采用溶剂热法制备CuIn(SxSe1-x)2(x=0-1)纳米粉末,采用X射线衍射仪(XRD)、场发射扫描电镜(FESEM)、紫外–可见分光光度计等对该粉末的物相结构、形貌及光吸收性能进行分... 以乙醇胺为溶剂,以氯化铟、氯化铜、硫化钠、硒粉为原料,采用溶剂热法制备CuIn(SxSe1-x)2(x=0-1)纳米粉末,采用X射线衍射仪(XRD)、场发射扫描电镜(FESEM)、紫外–可见分光光度计等对该粉末的物相结构、形貌及光吸收性能进行分析与表征。结果表明:CuIn(SxSe1-x)2粉末主要为黄铜矿相结构,当S元素掺杂量x〉0.5时,粉末中出现纤锌矿相CuIn(SxSe1-x)2。随x从0增加到1,CuIn(SxSe1-x)2粉末的形貌从片簇状逐渐转变为颗粒状,其吸收边出现"蓝移",禁带宽度从1.16eV增大到1.48eV。 展开更多
关键词 cuin(SxSe1-x)2
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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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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
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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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MAGNETIC PHASE DIAGRAM OF SmMn_2(Ge_(1-x)Si_x)_2 SYSTEM
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作者 Y.G. Wang F.M Yang +1 位作者 C.P. Chen, N Tang and Q.D. Wang (State Key Laboratory of Magnetism, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603,Beijing 100080, China)(Department of Materials Science and Engineering, Zheiang University Hangzhou 3 《Acta Metallurgica Sinica(English Letters)》 SCIE EI CAS CSCD 1997年第1期61-64,共4页
The magnetic phase diagram (x,T) of the SmMn2(Ge1-xSix)2 system has been studied by susceptibility and magnetization measurement. With increasing silicon concentration the temperature region of ferromagnetic ordering ... The magnetic phase diagram (x,T) of the SmMn2(Ge1-xSix)2 system has been studied by susceptibility and magnetization measurement. With increasing silicon concentration the temperature region of ferromagnetic ordering decreases on the phaae diagram. 展开更多
关键词 magnetic phase diagram susceptibility and magnetization measurement X-ray diffraction SmMn_2(Ge_(1-x)Si_x)_2 system
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(Cu_(1-x)Ba_(x))_(2)Y_(2)O_(5)色料的制备及其呈色特性研究
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作者 章文杰 汪其堃 +5 位作者 程龙 陈仁华 刘华锋 张小珍 汪永清 常启兵 《中国陶瓷》 CAS CSCD 北大核心 2022年第8期59-66,共8页
采用燃烧法制备了(Cu_(1-x)Ba_(x))_(2)Y_(2)O_(5)系绿色色料,系统的研究了钡含量及煅烧温度对其呈色性能的影响。此外,(Cu_(1-x)Ba_(x))_(2)Y_(2)O_(5)色料在陶瓷釉中的着色性能及机制也进行了深入探究。结果表明:钡的引入能够调节Cu_(... 采用燃烧法制备了(Cu_(1-x)Ba_(x))_(2)Y_(2)O_(5)系绿色色料,系统的研究了钡含量及煅烧温度对其呈色性能的影响。此外,(Cu_(1-x)Ba_(x))_(2)Y_(2)O_(5)色料在陶瓷釉中的着色性能及机制也进行了深入探究。结果表明:钡的引入能够调节Cu_(2)Y_(2)O_(5)色料的呈色性能。随着钡含量的增大,色料从深绿色逐渐转变为浅绿色,当x=0.1时,(Cu_(1-x)Ba_(x))_(2)Y_(2)O_(5)色料的呈色性能最佳。物相分析表明,钡离子并未进入Cu_(2)Y_(2)O_(5)晶格,而是形成了Cu_(2)Y_(2)O_(5)/BaCuY_(2)O_(5)复相色料。(Cu_(1-x)Ba_(x))_(2)Y_(2)O_(5)色料在陶瓷釉中的着色机理为离子着色,钡的引入同样有利于提升色料的着色性能。 展开更多
关键词 (Cu_(1-x)Ba_(x))_(2)Y_(2)O_(5) 绿
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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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Thermodynamic equilibrium theory-guided design and synthesis of Mg-doped LiFe_(0.4)Mn_(0.6)PO_(4)/C cathode for lithium-ion batteries
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作者 Wei Lyu Wenlong Cai +5 位作者 Tuan Wang Xiaobo Sun Enhao Xu Jinxuan Chen Kaipeng Wu Yun Zhang 《Journal of Energy Chemistry》 SCIE EI CAS CSCD 2024年第4期619-627,共9页
Mn-rich LiFe_(1-x)Mn_(x)PO_(4)(x>0.5),which combines the high operation voltage of LiMnPO_(4)with excellent rate performa nce of LiFePO4,is hindered by its sluggish kinetic properties.Herein,thermodynamic equilibri... Mn-rich LiFe_(1-x)Mn_(x)PO_(4)(x>0.5),which combines the high operation voltage of LiMnPO_(4)with excellent rate performa nce of LiFePO4,is hindered by its sluggish kinetic properties.Herein,thermodynamic equilibrium analysis of Mn^(2+)-Fe^(2+)-Mg^(2+)-C_(2)O_(4)^(2-)-H_(2)O system is used to guide the design and preparation of insitu Mg-doped(Fe_(0.4)Mn_(0.6))_(1-x)Mg_(x)C_(2)O_(4)intermediate,which is then employed as an innovative precursor to synthesize high-performance Mg-doped LiFe_(0.4)Mn_(0.6)PO_(4).It indicates that the metal ions with a high precipitation efficiency and the stoichiometric precursors with uniform element distribution can be achieved under the optimized thermodynamic conditions.Meanwhile,accelerated Li+diffusivity and reduced charge transfer resistance originating from Mg doping are verified by various kinetic characterizations.Benefiting from the contributions of inherited homogeneous element distribution,small particle size,uniform carbon layer coating,enhanced Li+migration ability and structural stability induced by Mg doping,the Li(Fe_(0.4)Mn_(0.6))_(0.97)Mg_(0.03)PO_(4)/C exhibits splendid electrochemical performance. 展开更多
关键词 (Fe_(0.4)Mn_(0.6))_(1-x)MgxC_(2)0_(4) precursors Thermodynami cequilibrium CO-PRECIPITATION Mg doping Lithium-ion batteries
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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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Cu_(2)Zn(Sn_(1-x)Ge_(x))(S,Se)_(4)太阳能电池的制备和表征
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作者 姜雨虹 李佳烨 +3 位作者 李雪 李丹 赵佳丽 刘洋 《吉林师范大学学报(自然科学版)》 2023年第4期8-12,共5页
采用简单的溶胶-凝胶法制备了高质量的Cu_(2)Zn(Sn_(1-x)Ge_(x))(S,Se)_(4)(CZTGSSe)前驱体薄膜.在500℃下进行17 min的硒化,得到了高质量的CZTGSSe薄膜.利用X射线衍射仪(XRD)、扫描电子显微镜(SEM)、紫外-可见分光光度计(UV-Vis)等研究... 采用简单的溶胶-凝胶法制备了高质量的Cu_(2)Zn(Sn_(1-x)Ge_(x))(S,Se)_(4)(CZTGSSe)前驱体薄膜.在500℃下进行17 min的硒化,得到了高质量的CZTGSSe薄膜.利用X射线衍射仪(XRD)、扫描电子显微镜(SEM)、紫外-可见分光光度计(UV-Vis)等研究了CZTGSSe薄膜的物理化学性质.实验结果表明,利用在CZTSSe吸收层中掺杂Ge的方法可以得到较高的迁移率和光电转换效率(PCE).与Cu_(2)ZnSn(S,Se)_(4)(CZTSSe)太阳能电池相比,观察到5%-CZTGSSe太阳能电池的开路电压(V_(oc))增加了104 mV,PCE也从3.14%增加到5.28%.因此,在CZTSSe层中掺杂Ge不仅是一种可以获得具有较高V_(oc)和PCE的CZTSSe基太阳能电池的方法,也是一种可以促进晶粒生长、提高薄膜质量的有效途径. 展开更多
关键词 Cu_(2)Zn(Sn_(1-x)Ge_(x))(S Se)_(4) -
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H_2S硫化CuInSe_2生成CuIn(S_xSe_(1-x))_2薄膜的XRD及Raman分析
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作者 张鑫狄 江国顺 《光谱实验室》 CAS CSCD 2012年第1期9-15,共7页
将CuInSe_2薄膜在H_2S与Ar的混合气体中硫化是制备CuIn(S_xSe_(1-x))_2薄膜的一种常用方法。硫化所用到的CuInSe_2薄膜是用溶剂热法生成的CuInSe_2纳米颗粒旋涂而成。不同于其他真空条件下制备CuInSe_2薄膜的方法.溶剂热法的优点是其相... 将CuInSe_2薄膜在H_2S与Ar的混合气体中硫化是制备CuIn(S_xSe_(1-x))_2薄膜的一种常用方法。硫化所用到的CuInSe_2薄膜是用溶剂热法生成的CuInSe_2纳米颗粒旋涂而成。不同于其他真空条件下制备CuInSe_2薄膜的方法.溶剂热法的优点是其相对简单的制备工艺和较低廉的成本。对硫化过程进行研究后发现,硫化温度和时间直接影响CuIn(S_xSe_(1-x))_2薄膜的质量,诸如薄膜成分、结晶度、均匀性和带隙宽度都可以通过改变这些实验条件来进行控制。 展开更多
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Mo原子固溶对Cr_(2)AlC力学性能及摩擦学性能的影响
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作者 何乃如 黄琰 +2 位作者 周昊 方媛 文怀兴 《中国陶瓷》 CAS CSCD 北大核心 2021年第2期7-16,共10页
采用热压烧结技术制备Cr_(2)AlC材料,并通过Mo元素复配对Cr_(2)AlC进行固溶强化,研究不同固溶比下(Cr_(1-x)Mo_(x))_(2)AlC陶瓷的力学性能及宽温域摩擦学性能影响。研究结果表明,Mo原子固溶导致Cr_(2)AlC晶格畸变,力学性能显著提升,但是... 采用热压烧结技术制备Cr_(2)AlC材料,并通过Mo元素复配对Cr_(2)AlC进行固溶强化,研究不同固溶比下(Cr_(1-x)Mo_(x))_(2)AlC陶瓷的力学性能及宽温域摩擦学性能影响。研究结果表明,Mo原子固溶导致Cr_(2)AlC晶格畸变,力学性能显著提升,但是当Cr/Mo原子比为1时,固溶材料的硬度、抗弯强度与断裂韧性急剧下降。由于Mo原子的固溶强化作用,(Cr_(1-x)Mo_(x))_(2)AlC在中低温环境下表现出更好的耐磨性能,但是在高温环境下(Cr_(1-x)Mo_(x))_(2)AlC磨痕表面并没有形成连续的釉质层或润滑膜,相比于Cr_(2)AlC,固溶材料表现出较差的高温摩擦学性能。 展开更多
关键词 (Cr_(1-x)Mo_(x))_(2)AlC固溶体
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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+x)Al_(x)Ti_(2-x)(PO_(4))_(3) lithium batteries
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Fabrication and properties of non-stoichiometric Tb_(2)(Hf_(1-x)Tb_(x))_(2)O_(7-x)magneto-optical ceramics 被引量:2
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作者 Lixuan ZHANG Xiaoying LI +5 位作者 Dianjun HU Ziyu LIU Tengfei XIE Lexiang WU Zhaoxiang YANG Jiang LI 《Journal of Advanced Ceramics》 SCIE EI CAS CSCD 2022年第5期784-793,共10页
Non-stoichiometric Tb_(2)(Hf_(1-x)Tb_(x))_(2)O_(7-x)(x=-0.07-0.45)magneto-optical ceramics were fabricated by solid-state reactive sintering in vacuum combined with hot isostatic pressing(HIP)posttreatment without any... Non-stoichiometric Tb_(2)(Hf_(1-x)Tb_(x))_(2)O_(7-x)(x=-0.07-0.45)magneto-optical ceramics were fabricated by solid-state reactive sintering in vacuum combined with hot isostatic pressing(HIP)posttreatment without any sintering aids.The phase composition,densification process,microstructure,optical transmittance,and Verdet constant of Tb_(2)(Hf_(1-x)Tb_(x))_(2)O_(7-x)ceramics were investigated.The in-line transmittance of(Tb_(0.93)Hf_(0.04))_(2)Hf_(2)O_(7.07)ceramics with a thickness of 2.0 mm reaches 74.6%at 1064 nm.The Verdet constant of Tb_(2)(Hf_(1-x)Tb_(x))_(2)O_(7-x)ceramics is-153.4,-155.8,and-181.2 rad/(T-m)at the wavelength of 633 nm when x=-0.07,0,and 0.1,respectively.The Verdet constant increases with the increase of Tb content,and these values are higher than that of the commercial Tb_(3)Ga_(5)O_(12) crystal,indicating that non-stoichiometric Tb_(2)(Hf_(1-x)Tb_(x))_(2)O_(7-x)ceramics have a great potential for the application in Faraday isolators. 展开更多
关键词 magneto-optical ceramics Tb_(2)(Hf_(1-x)Tb_(x))_(2)O_(7-x)ceramics reactive sintering Verdet constant
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Tunable electronic band structure,luminescence properties and thermostability of(Gd_(1-x)La_(x))_(2)Si_(2)O_(7):Ce scintillator by adjusting La/Gd ratio 被引量:1
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作者 Qinhua Wei Zhenzhen Zhou +4 位作者 Weijie Zhang Gao Tang Qian Liu Laishun Qin Hongsheng Shi 《Journal of Rare Earths》 SCIE EI CAS CSCD 2021年第6期657-665,I0002,共10页
Mixed crystal strategy is an effective approach of improving the luminescence properties of optical materials and has been adopted widely in many systems.In this paper,the La-mixed Gd_(2)Si_(2)O_(7):Ce polycrystalline... Mixed crystal strategy is an effective approach of improving the luminescence properties of optical materials and has been adopted widely in many systems.In this paper,the La-mixed Gd_(2)Si_(2)O_(7):Ce polycrystalline samples were successfully synthesized by a sol-gel method.The crystal structure and luminescence properties were confirmed and discussed by XRD,UV-Vis luminescence spectra,and XEL,respectively.The vacuum ultraviolet excitation spectra and thermoluminescence glow curves were also systematically investigated and discussed at varied temperature.A combination of the first-principles calculations and optical characterization experiments was employed to study the electronic band structure of host material,revealing that the band gap is narrowed and the 5d_(1) level of Ce^(3+) shifts to higher energy as the La content increases.The luminescence the rmo-stability and activation energy were also measured and calculated.It indicates that thermo-stability is strongly dependent on the La concentration.An effective approach is developed to tune the electronic band structure,luminescence properties and thermostability of(Gd_(1-x)La_(x))_(2)Si_(2)O_(7):Ce scintillator by adjusting La/Gd ratio. 展开更多
关键词 First-principles calculations Scintillator (Gd_(1-x)La_(x))_(2)Si_(2)O_(7):Ce Band structure tunable Luminescence properties Rare earths
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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 被引量:1
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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%PLUS%)doping Rare earths
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