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Prop铁电薄膜电容器YBCO/Pb(Ta_(0.05)Zr_( 0.48)Ti_(0.47))O_3/YBCO/Pt/TiO_2/SiO_2/Si的性质(英文)
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作者 李启亮 王栩生 +2 位作者 殷江 高兴森 刘治国 《南京大学学报(自然科学版)》 CAS CSCD 北大核心 2001年第5期619-624,共6页
铁电薄膜有望被应用于“不挥发随机存储器 (NvRAM )” ,在这其中 ,Pb(Zr,Ti)O3(PZT)铁电薄膜由于有较大的剩余极化 ,较小的矫顽场 ,高居里点 ,以及与硅集成的可能性而得到了广泛的研究 .但是 ,由于铁电薄膜与金属电极之间的界面不理想 ... 铁电薄膜有望被应用于“不挥发随机存储器 (NvRAM )” ,在这其中 ,Pb(Zr,Ti)O3(PZT)铁电薄膜由于有较大的剩余极化 ,较小的矫顽场 ,高居里点 ,以及与硅集成的可能性而得到了广泛的研究 .但是 ,由于铁电薄膜与金属电极之间的界面不理想 ,以及铁电薄膜中的晶界角度过高 ,而大大降低了铁电电容器的性能 .最近的研究表明 ,通过用导氧化物作电极 ,可部分的改善电薄膜的疲劳和保持性能 .用脉冲激光沉积法 (PLD) ,以YBa2 Cu3O7(YBCO)为隔离层 ,在Pt/TiO2 /Si(10 0 )衬底上制备Pb(Ta0 .0 5Zr0 .48Ti0 .47)O3(PTZT)铁电薄膜 ;并以YBCO为上下电极做成铁电电容器 .X衍射发现以YBCO为电极的PTZT结晶成完全钙钛矿相 .SEM结果表明PTZT晶粒大约在 180nm左右 ,YBCO/Pt ,Pt/TiO2 界面非常清晰 ,没有发现任何扩散 .在RT6 0 0 0HVS环境下 ,发现在 91kV/cm的外场下反转 1× 10 1 1 次后 ,此电容器的极化P 和P^分别只减少了 2 0 %和 6 % ;在 145kV/cm的读写外场下经过 1× 10 5s后 ,此电容器的极化基本保持不变 ;在过大的外场下 ,此电容器的疲劳特性明显变差 .由于引入YBCO过渡层 ,改善了界面 ,减少了薄膜中氧空位的聚集程度 。 展开更多
关键词 极化 疲劳 保持 铁电薄膜电容器 晶界过度 导氧化铁 YBCO 二氧化钛 脉冲激光沉积
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Dual solidification mechanisms of liquid ternary Fe-Cu-Sn alloy
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作者 WeiLi Wang XiaoMei Zhang +1 位作者 LiuHui Li BingBo Wei 《Science China(Physics,Mechanics & Astronomy)》 SCIE EI CAS 2012年第3期450-459,共10页
Liquid ternary Fe47.5Cu47.5Sn5 alloy displayed dual solidification mechanisms when it was undercooled by up to 329 K (0.19TL). Below a critical undercooling of about 196 K, it solidified just like a normal peritecti... Liquid ternary Fe47.5Cu47.5Sn5 alloy displayed dual solidification mechanisms when it was undercooled by up to 329 K (0.19TL). Below a critical undercooling of about 196 K, it solidified just like a normal peritectic alloy, even though metastable phase separation occurred to a microscopic extent. Once bulk undercooling exceeds 196 K, macroscopic segregation played a domi- nant role in solidification. In both cases, the solidification process was always characterized by two successive peritectic trans- formations: firstly primary yFe dendrites reacted with liquid phase to form (Cu) phase, and subsequently the (Cu) phase reacted with residual liquid phase to yield β-Cu5.6Sn intermetallic compound. The primary yFe dendrites achieved a maximum growth velocity of 400 mm/s and experienced a growth kinetics transition as a result of macrosegregation. Since the (Cu) phase was both the product phase of the first peritectic transformation and also the reactant phase for the second peritectic transformation, it appeared as two layers in solidification microstructures due to the microsegregation of Sn solute. The boundary continuity between the macroscopically separated Fe-rich and Cu-ricb zones was enhanced with the increase of undercooling. 展开更多
关键词 peritectic solidification phase separation MACROSEGREGATION UNDERCOOLING dendritic growth
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