Ni掺杂ZnS的第一性原理计算

采用基于密度泛函理论(DFT)赝势平面波方法计算了ZnS体系Ni掺杂前后的能带结构、态密度和光吸收系数曲线。结果表明:纯ZnS的能带结构是直接带隙,态密度显示属离子性较强而共价键较弱的混合键半导体材料。掺Ni的ZnS禁带宽度随掺杂量增加逐渐减小,能带简并度增大,且向低能方向移动;在价带顶出现杂质能级,说明是p型掺杂。纯ZnS在3.9 eV以下无吸收,红外透过率较高。掺Ni后吸收边红移,且在低能端(绿光区)出现新的吸收峰。     

Transport properties and anomalous fatigue effect of Ag/Bi0.9La0.lFeO3/La0.7Sr0.3MnO3 heterostructures

The transport properties and fatigue effect of Ag/Bi0.9La0.lFeO3/La0.7Sr0.3MnO3 heterostructures are described. By examining the I-V curves, an anomalous fatigue effect was found and its influences on resistive states were studied. I-V curves combined with C-f spectra were used to directly analyze the transport properties and fatigue effect. Compared to the first I-V cycle state, this structure shows more than one order increase of resistance after 100 cycles of ＂I-V curve training＂. The redistribution of oxygen vacancies in the depletion layer of Ag/Bi0.9La0.lFeO3 is believed to be responsible for the different resistance mechanisms and tenfold magnitude drop in resistance. The resistive switching is understood to be caused by electric field-induced carrier trapping and detrapping, which changes the depletion layer thickness at the Ag/Bi0.9La0.lFeO3 interface.     

Transport properties and anomalous fatigue effect of Ag/Bi_(0.9)La_(0.1)FeO_3/La_(0.7)Sr_(0.3)MnO_3 heterostructures

The transport properties and fatigue effect of Ag/Bi0.9La0.1FeO3/La0.7Sr0.3MnO3 heterostructures are described. By examining the I–V curves, an anomalous fatigue effect was found and its influences on resistive states were studied. I–V curves combined with C– f spectra were used to directly analyze the transport properties and fatigue effect. Compared to the first I–V cycle state, this structure shows more than one order increase of resistance after 100 cycles of "I–V curve training". The redistribution of oxygen vacancies in the depletion layer of Ag/Bi0.9La0.1FeO3 is believed to be responsible for the different resistance mechanisms and tenfold magnitude drop in resistance. The resistive switching is understood to be caused by electric field–induced carrier trapping and detrapping, which changes the depletion layer thickness at the Ag/Bi0.9La0.1FeO3 interface.     

锆钛酸铅薄膜的溶胶-凝胶制备工艺及结构与物性的研究

采用溶胶-凝胶匀胶法制备锆钛酸铅铁电薄膜,研究了前驱体影响因素(如有机溶剂、前驱单体加入顺序、添加剂)、溶胶影响因素(如溶胶浓度、pH值)、匀胶速度和退火温度对成膜质量及薄膜微结构、铁电性的影响.结果表明:采用乙二醇甲醚为溶剂对pb2+、Zr4+和Ti4+金属盐进行溶解优于乙醇和乙二醇,但由于乙二醇甲醚对硝酸锆的溶解性差,对硝酸锆应先用乙醇溶解再加入乙二醇甲醚的方法来进行溶解;以硝酸锆为Zr源配制溶胶时,只有先将Pb前驱液滴加到Ti前驱液中,然后再滴入Zr前驱液的方式才能得到澄清前驱体.将锆钛酸铅溶胶浓度和pH值分别控制在0.2～0.3 mol/L和2～3较为适宜,与此溶胶相适应的匀胶参数:转速为4000 r/min,时间为60 s.随退火温度升高,薄膜的晶化程度增加,且逐渐表现出(100)晶面择优取向,晶格常数c和四方率c/a逐渐增加,而晶格常数a逐渐减小;随退火温度升高,晶粒尺寸逐渐增大,使得剩余极化强度逐渐增加,矫顽场强逐渐减小.当退火温度为850 ℃时制备的锆钛酸铅薄膜具有均匀的晶粒、较低的表面粗糙度和最为优异的铁电性.     

钙钛矿太阳能电池中电子传输层现状研究

有机-无机杂化钙钛矿型太阳能电池(简称钙钛矿太阳能电池)的最高光电转换效率已经达到25.5%,是最有希望取代硅基太阳能电池并实现广泛应用的太阳能电池之一。作为钙钛矿太阳能电池的基本组成部分,电子传输层对电池的性能起着至关重要的作用。本文阐述了钙钛矿太阳能电池中电子传输层的种类、尺寸以及界面修饰等对器件性能的影响,为继续提升钙钛矿太阳能电池性能提供参考。     

微波烧结制备铁酸铋陶瓷的介电性和铁电性

采用微波烧结法制备铁酸铋多铁陶瓷,研究了微波烧结时间对其显微结构、介电性和铁电性的影响.结果表明:在4 kW下烧结35～40 min制备出基本为纯相的铁酸铋陶瓷;随烧结时间增加,铁酸铋陶瓷结构越来越致密,晶粒尺寸有一定程度增大;在-10～90℃范围内,介质损耗随烧结时间增加而增大;随微波烧结时间增加,剩余极化强度增大,而矫顽场强先增加后减小,且铁电性具有明显的频率依赖性;铁酸铋陶瓷的漏电流随微波烧结时间增加而减小,这是结构致密化的结果.     

水热法制备纳米线研究进展

纳米线因其显著的边界效应、易单晶化、高比线径、大比表面积、高强度、高韧性、低导电性等特点,广泛应用于电子器件、太阳能转换、纤维合成、微电池制造等领域.水热法是制备纳米线的常用方法,本文综述了水热法工艺参数,矿化剂种类、反应温度、反应时间等对调控纳米线表面形貌与性能影响的研究进展,并提出研究中需要解决的问题.矿化剂种类对纳米线的形成及形貌有显著影响,矿化剂浓度的升高会促进纳米线的形成,但是超过某一临界值又会反过来影响纳米线的形貌与抑制纳米线的形成;反应温度直接影响晶粒的生长,温度过高会导致杂相的产生,不利于形成稳定晶型,温度太低又不足以提供纳米线生长的动力;随着反应时间的增加,纳米线长径比增加,比表面积增加,表面变得更光滑,当反应时间过长时,纳米线横向过度生长,纳米线长径比降低,纳米线变为纳米棒.     

钇掺杂铌酸锶陶瓷的微观结构与电性能研究

采用固相法制备了Nb2Sr2-xYxO7陶瓷.研究了掺Y对陶瓷的晶体结构、表面形貌、铁电、介电和压电性能的影响.研究结果表明:钇掺杂Sr2 Nb2 O7陶瓷,Y3+取代了A位Sr2+,形成Nb2 Sr2-xYxO7固溶体,并提高了铌酸锶陶瓷铁电、介电和压电性能.在x=0.05时,Nb2 Sr2-xYxO7陶瓷的铁电性能达到最大(剩余极化强度Pr=0.254μC/cm2);在x=0.1时,Nb2Sr2-xYxO7陶瓷的介电性能达到最大(相对介电常数εr=90,介电损耗tarδ≤0.01).