采用高温固相法合成了Li_4Ti_5O_(12)和Li_4Ti_(4.95)Ce_(0.05)O_(12)负极材料,采用X射线粉末衍射(XRD)、扫描电镜(SEM)、循环伏安(CV)和充放电测试等手段研究样品的结构和电化学性能。XRD图谱表明铈掺杂并没有改变样品的晶体结构;循环...采用高温固相法合成了Li_4Ti_5O_(12)和Li_4Ti_(4.95)Ce_(0.05)O_(12)负极材料,采用X射线粉末衍射(XRD)、扫描电镜(SEM)、循环伏安(CV)和充放电测试等手段研究样品的结构和电化学性能。XRD图谱表明铈掺杂并没有改变样品的晶体结构;循环伏安曲线表明Li_4Ti_(4.95)Ce_(0.05)O_(12)样品具有更好的可逆性,铈的掺杂有利于锂离子的可逆脱嵌;微分电容曲线表明Li_4Ti_(4.95)Ce_(0.05)O_(12)的充放电的峰电位值差比Li_4Ti_5O_(12)小,说明前者具有更小的电化学极化;充放电测试表明,5 C倍率充放电时,Li_4Ti_(4.95)Ce_(0.05)O_(12)和Li_4Ti_5O_(12)的可逆放电容量分别为120 m A·h/g和80 m A·h/g左右,说明铈的掺杂提高了Li_4Ti_5O_(12)材料的倍率容量和循环性能。展开更多
采用二步固相法制备了Li_4Ti_(4.95)Nb_(0.05)O_(12)负极材料,扫描电镜、激光粒度分布仪、充放电测试和循环伏安等测试结果表明:合成的样品粒径分布均匀,Nb掺杂改性的Li_4Ti_5O_(12)具有优良的电化学性能,0.1 C、0.5 C、1 C和10 C首次...采用二步固相法制备了Li_4Ti_(4.95)Nb_(0.05)O_(12)负极材料,扫描电镜、激光粒度分布仪、充放电测试和循环伏安等测试结果表明:合成的样品粒径分布均匀,Nb掺杂改性的Li_4Ti_5O_(12)具有优良的电化学性能,0.1 C、0.5 C、1 C和10 C首次放电比容量分别为174.1 m Ah/g、159.7 m Ah/g、147 m Ah/g和123.3 m Ah/g。10 C下,循环20次后容量保持为118.1 m Ah/g。展开更多
采用高温固相法合成Li_4Ti_5O_(12)及Li_4Ti_(4.95)Zr_(0.05)O_(12)材料,采用扫描电镜(SEM)、X射线粉末衍射(XRD)、充放电测试和循环伏安(CV)研究材料的结构和电化学性能。结果表明,两种材料均具有较小的平均粒径和窄的粒度分布,Zr4+进...采用高温固相法合成Li_4Ti_5O_(12)及Li_4Ti_(4.95)Zr_(0.05)O_(12)材料,采用扫描电镜(SEM)、X射线粉末衍射(XRD)、充放电测试和循环伏安(CV)研究材料的结构和电化学性能。结果表明,两种材料均具有较小的平均粒径和窄的粒度分布,Zr4+进入晶格结构内部,具有纯相的尖晶石结构。0.1C倍率时,Li_4Ti_(4.95)Zr_(0.05)O_(12)首次放电比容量高达248 m A·h/g,略低于Li_4Ti_5O_(12)。1.0C倍率放电比容量为145 m A·h/g,5.0C倍率140次循环后,放电比容量仍达到121 m A·h/g,明显高于纯相Li_4Ti_5O_(12)材料,具有较好倍率性能。展开更多
A temperature stable Li2Zn0.95(SrxCa1-x)0.05Ti3O8(0≤x≤1)ceramics were fabricated using a conventional solid-state route sintered at 1100℃for 4 h.The XRD results indicate that the main phase Li2ZnTi3O8 and secondary...A temperature stable Li2Zn0.95(SrxCa1-x)0.05Ti3O8(0≤x≤1)ceramics were fabricated using a conventional solid-state route sintered at 1100℃for 4 h.The XRD results indicate that the main phase Li2ZnTi3O8 and secondary phase including SrxCa1-xTiO3(0≤x≤1)solid solution and TiO2 co-exist in composite and form a stable composite system when the(CaxSr1-x)(0≤x≤1)substitutes for Zn of Li2ZnTi3O8 ceramic.As x is increased from 0 to 1,the relative permittivity(εr)increases from 26.65 to 27.12,and the quality factor(Q×f)increases from 63300 to 66600 GHz.With the increased of x,the temperature coefficient of resonant frequency(τf)increases from 0.27 to 8.23 ppm/℃,and then decreases to 3.51 ppm/℃.On the whole,the Li2Zn0.95(SrxCa1-x)0.05Ti3O8(0≤x≤1)ceramics show excellent comprehensive properties of middleεr=25-27,higher Q×f≥60000 GHz andτf≤±8.5 ppm/℃.展开更多
Ca0.4Sr0.6Bi3.95Nd0.05Ti4O15 (C0.4S0.6BNT) ferroelectric thin films were prepared on Pt/Ti/SiO2/Si substrates by sol-gel method. Effect of annealing process (time and temperature) on structures and ferroelectric p...Ca0.4Sr0.6Bi3.95Nd0.05Ti4O15 (C0.4S0.6BNT) ferroelectric thin films were prepared on Pt/Ti/SiO2/Si substrates by sol-gel method. Effect of annealing process (time and temperature) on structures and ferroelectric properties of C0.4S0.6BNT thin film was investigated. The relative intensity of (200) peak increased first then decreased with annealing temperature and became predominant at 800 ℃. In contrast, no evident change could be observed in the (001) peak. The remnant polarization (Pr) and coercive field (Ec) for C0.4S0.6BNT film annealed at 800℃ for 5 min were 21.6μC/cm2 and 68.3 kV/cm, respectively.展开更多
文摘采用高温固相法合成了Li_4Ti_5O_(12)和Li_4Ti_(4.95)Ce_(0.05)O_(12)负极材料,采用X射线粉末衍射(XRD)、扫描电镜(SEM)、循环伏安(CV)和充放电测试等手段研究样品的结构和电化学性能。XRD图谱表明铈掺杂并没有改变样品的晶体结构;循环伏安曲线表明Li_4Ti_(4.95)Ce_(0.05)O_(12)样品具有更好的可逆性,铈的掺杂有利于锂离子的可逆脱嵌;微分电容曲线表明Li_4Ti_(4.95)Ce_(0.05)O_(12)的充放电的峰电位值差比Li_4Ti_5O_(12)小,说明前者具有更小的电化学极化;充放电测试表明,5 C倍率充放电时,Li_4Ti_(4.95)Ce_(0.05)O_(12)和Li_4Ti_5O_(12)的可逆放电容量分别为120 m A·h/g和80 m A·h/g左右,说明铈的掺杂提高了Li_4Ti_5O_(12)材料的倍率容量和循环性能。
文摘采用二步固相法制备了Li_4Ti_(4.95)Nb_(0.05)O_(12)负极材料,扫描电镜、激光粒度分布仪、充放电测试和循环伏安等测试结果表明:合成的样品粒径分布均匀,Nb掺杂改性的Li_4Ti_5O_(12)具有优良的电化学性能,0.1 C、0.5 C、1 C和10 C首次放电比容量分别为174.1 m Ah/g、159.7 m Ah/g、147 m Ah/g和123.3 m Ah/g。10 C下,循环20次后容量保持为118.1 m Ah/g。
文摘采用高温固相法合成Li_4Ti_5O_(12)及Li_4Ti_(4.95)Zr_(0.05)O_(12)材料,采用扫描电镜(SEM)、X射线粉末衍射(XRD)、充放电测试和循环伏安(CV)研究材料的结构和电化学性能。结果表明,两种材料均具有较小的平均粒径和窄的粒度分布,Zr4+进入晶格结构内部,具有纯相的尖晶石结构。0.1C倍率时,Li_4Ti_(4.95)Zr_(0.05)O_(12)首次放电比容量高达248 m A·h/g,略低于Li_4Ti_5O_(12)。1.0C倍率放电比容量为145 m A·h/g,5.0C倍率140次循环后,放电比容量仍达到121 m A·h/g,明显高于纯相Li_4Ti_5O_(12)材料,具有较好倍率性能。
基金Funded by the Open Project Program of Key Laboratory of Inorganic Functional Materials and Devices,Chinese Academy of Sciences(No.KLIFMD201606)the Open Fund of National Innovation Platform(No.2017YJ163)+1 种基金the National Natural Science Foundation of China(Nos.51502220,51521001,and 51672197)the Open Foundation of Hubei Key Laboratory of Theory and Application of Advanced Materials Mechanics(Wuhan University of Technology)(No.TAM201802)。
文摘A temperature stable Li2Zn0.95(SrxCa1-x)0.05Ti3O8(0≤x≤1)ceramics were fabricated using a conventional solid-state route sintered at 1100℃for 4 h.The XRD results indicate that the main phase Li2ZnTi3O8 and secondary phase including SrxCa1-xTiO3(0≤x≤1)solid solution and TiO2 co-exist in composite and form a stable composite system when the(CaxSr1-x)(0≤x≤1)substitutes for Zn of Li2ZnTi3O8 ceramic.As x is increased from 0 to 1,the relative permittivity(εr)increases from 26.65 to 27.12,and the quality factor(Q×f)increases from 63300 to 66600 GHz.With the increased of x,the temperature coefficient of resonant frequency(τf)increases from 0.27 to 8.23 ppm/℃,and then decreases to 3.51 ppm/℃.On the whole,the Li2Zn0.95(SrxCa1-x)0.05Ti3O8(0≤x≤1)ceramics show excellent comprehensive properties of middleεr=25-27,higher Q×f≥60000 GHz andτf≤±8.5 ppm/℃.
基金supported by the Natural Science Foundation of Shandong Province (Y2007F36)the National Natural Science Foundation of China (50872075)
文摘Ca0.4Sr0.6Bi3.95Nd0.05Ti4O15 (C0.4S0.6BNT) ferroelectric thin films were prepared on Pt/Ti/SiO2/Si substrates by sol-gel method. Effect of annealing process (time and temperature) on structures and ferroelectric properties of C0.4S0.6BNT thin film was investigated. The relative intensity of (200) peak increased first then decreased with annealing temperature and became predominant at 800 ℃. In contrast, no evident change could be observed in the (001) peak. The remnant polarization (Pr) and coercive field (Ec) for C0.4S0.6BNT film annealed at 800℃ for 5 min were 21.6μC/cm2 and 68.3 kV/cm, respectively.