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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_(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) LTCC
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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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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:3
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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+)doping Rare earths
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