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K_(x)Na_(1–x)NbO_(3):Pr^(3+)铁电体的光致发光和应力发光性能 被引量:1
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作者 梁爱华 王旭升 +3 位作者 李国荣 郑嘹赢 江向平 胡锐 《物理学报》 SCIE EI CAS CSCD 北大核心 2022年第16期369-379,共11页
应力发光材料具有应力-光转换特性,能在机械应力下产生发光,从而在光学信息显示方面具有很高的应用价值.本文通过改变铁电基体K_(x)Na_(1–x)NbO_(3)∶0.5%Pr^(3+)(K_(x)NNOP)的K^(+)/Na^(+)比来调节材料的晶体结构和缺陷分布,系统研究... 应力发光材料具有应力-光转换特性,能在机械应力下产生发光,从而在光学信息显示方面具有很高的应用价值.本文通过改变铁电基体K_(x)Na_(1–x)NbO_(3)∶0.5%Pr^(3+)(K_(x)NNOP)的K^(+)/Na^(+)比来调节材料的晶体结构和缺陷分布,系统研究了K+含量对光致发光和应力发光性能的影响.研究结果表明,K+含量的增加使晶体对称性提高,导致K_(x)NNOP样品的光致发光强度降低.值得注意的是,在450 nm的光激发下,在K^(+)含量较高的组分中出现了Pr^(3+)电子3P1→3H5和3P0→3H5能级跃迁引起的发射峰,这归因于Pr^(3+)和Nb5+之间距离的变化导致Pr-O-Nb内价电子电荷转移态(IVCT)的能级位置不同.在压缩应力下,K_(x)NNOP(x=0,0.01,0.02,0.1)组分展现出明亮的红色应力发光,且应力发光强度随K+含量的增加而增大,其中K0.1NNOP组分表现出最高的强度发射.特别的是,其应力发光行为具有可重复性和可恢复性的特征.通过热释光曲线研究了K_(x)NNOP样品中的陷阱能级,揭示了K0.1NNOP中应力发光的增强可能与K+含量变化引起的陷阱密度和陷阱深度的差异有关.基于这些结果,建立了一个模型来阐述K_(x)NNOP中可能的应力发光机理. 展开更多
关键词 应力发光 铁电 k_(x)na_(1–x)nbo_(3):Pr^(3+) 缺陷分布 光致发光
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A novel Na_(1−x)K_(x)TaO_(3)perovskite microwave dielectric ceramic with high permittivity and high positive temperature coefficient 被引量:1
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作者 Liu Tang Hongcheng Yang +1 位作者 Enzhu Li Chaowei Zhong 《Journal of Advanced Ceramics》 SCIE EI CAS CSCD 2023年第11期2053-2061,共9页
A novel Na_(1−x)K_(x)TaO_(3)(x=0,0.025,0.05,0.075,0.1,and 0.15)ceramic with high permittivity and high positive temperature coefficient was synthesized via the conventional solid-state method.All samples were determin... A novel Na_(1−x)K_(x)TaO_(3)(x=0,0.025,0.05,0.075,0.1,and 0.15)ceramic with high permittivity and high positive temperature coefficient was synthesized via the conventional solid-state method.All samples were determined to be pure phase orthorhombic NaTaO3 structure of space group Pmcn,and larger grain and lower porosity were observed after adding an appropriate amount of K+ions.The Q×f value is majored by the packing fraction and grain size,while the value ofτf is influenced by Ta–O bond valence.The Na_(0.95)K_(0.05)TaO_(3) ceramic possesses excellent dielectric properties ofεr=164.29,Q×f=9091 GHz(f=3.15 GHz),tanδ=3.46×10^(–4),τf=+809.52 ppm/℃,sintered at 1550℃.Compared with NaTaO_(3) ceramics,the Na_(1−x)K_(x)TaO_(3)ceramics prepared in this study demonstrate higher dielectric constants and higher positive temperature coefficients,which are promising for device miniaturization andτf compensators. 展开更多
关键词 na_(1−x)k_(x)TaO_(3)ceramics high permittivity high positive temperature coefficient PEROVSkITE
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Investigation of the phase space in lead‐free(K_(x)Na_(1-x))_(1-y)Li_(y)(Nb_(1-z)Ta_(z))O_(3) ferroelectric ceramics
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作者 Henry E.MGBEMERE Rolf JANSSEN Gerold A.SCHNEIDER 《Journal of Advanced Ceramics》 SCIE CAS CSCD 2015年第4期282-291,共10页
A library of ceramic compounds based on the lead-free(K_(x)Na_(1-x))1-yLiy(Nb1-zTaz)O_(3)solid solution has been synthesized and characterized using high-throughput experimentation(HTE)method.The phase space previousl... A library of ceramic compounds based on the lead-free(K_(x)Na_(1-x))1-yLiy(Nb1-zTaz)O_(3)solid solution has been synthesized and characterized using high-throughput experimentation(HTE)method.The phase space previously reported by Saito and Takao has been expanded to{{x,0.1,1.0},{y,0,0.1},{z,0,0.2}},and new phase boundaries are observed.The relative density values show that with the appropriate sintering temperature,~92%of the theoretical density can be reached.The relative permittivity values show that with increasing amount of K+and Ta5+,the dielectric constant values increase.The effect of density on the dielectric constant values is however minimal.Resistivity values ranging from 109 to 1013Ω·cm are obtained for the samples.The piezoelectric charge coefficient values for selected compositions show that higher values are obtained close to the phase boundaries rather than away from them.The properties for the ceramic library using the HTE method are generally 15%-20%less than from the conventional method.This method is therefore more suited for screening of sample compositions than for producing samples with high piezoelectric properties. 展开更多
关键词 FERROELECTRICS high-throughput synthesis (k_(x)na_(1-x))nbo_(3)(kNN) lead-free ceramics
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Phase transition and piezoelectric property of (Ag,K)NbO_(3) ceramics
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作者 Lin Chen Mingyuan Zhao +3 位作者 Jing Wang Suwei Zhang Fuhua Sun Lei Zhao 《Journal of Materiomics》 SCIE 2022年第4期863-872,共10页
AgNbO_(3) is an antiferroelectric (AFE) material with double hysteresis loop. Both the antiferroelectricityand ferroelectricity can be enhanced by doping. Herein, the ferroelectricity of AgNbO_(3) ceramics wasenhanced... AgNbO_(3) is an antiferroelectric (AFE) material with double hysteresis loop. Both the antiferroelectricityand ferroelectricity can be enhanced by doping. Herein, the ferroelectricity of AgNbO_(3) ceramics wasenhanced via K-doping and the phase diagram of the (Ag_(1-x)K_(x))NbO_(3) ceramics was upgraded. In details,(Ag_(1-x)K_(x))NbO_(3) ceramics are ferrielectric (FIE) M1 phase as x=5.00-5.50 mol% and ferroelectric (FE) Ophase as x=5.75-6.00 mol% before poling, and FE O phase as x=5.00-6.00 mol% after poling at roomtemperature. With increasing temperature, (Ag_(1-x)K_(x))NbO_(3) ceramics show the phase evolutions from FIEM1, AFE M2 to paraelectric (PE) T phase at x=5.00-5.50 mol% and from FE O, FE T to PE T phase at x=5.75-6.00 mol% before poling, and from FE O, FE T to PE T phase at x=5.00-6.00 mol% after poling.High d33 values of 180 pC/N and 285 pC/N are obtained at the FE O-FE T and FE T-PE T phase boundaries.This work sheds light on a novel and promising lead-free piezoelectric system. 展开更多
关键词 (Ag_(1-x)k_(x))nbo_(3)ceramics Phase diagram Piezoelectric property
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