准分子激光对掺杂SnO2气敏元件性能的影响

一定能量密度的准分子激光作用于掺杂ＳｎＯ２烧结型气敏元件敏感材料表面后，元件性能发生了显著的变化。元件电阻和对气体的灵敏度比作用前有明显的增加，同时材料表面颜色生变化，分析认为该过程中由于短脉冲的准分子激光作用，使ＳｎＯ２材料快速升温熔化并快速冷凝重构，导致表面变性，从而引起了材料电性能和气体敏感性能的变化。     

不同CO吸附类型对超细SnO_2气敏元件的作用

本工作采用超细ＳｎＯ２为基体，ＣＯ为检测气体，检测了烧结型ＳｎＯ２元件在不同温度下的气敏效应．同时利用流动饱和法测试了粉体不同温度下对ＣＯ的可逆及不可逆吸附量．一方面通过新材料的使用，降低了元件的工作温度；另一方面，通过吸附测试与气敏效应的关联，认为：超细粉体低温时表面可逆ＣＯ量的存在，是其能够降低工作温度的主要原因．粉体表面的不可逆ＣＯ量直接影响着元件的响应输出（灵敏度）．材料本身的吸附总量和气敏特性有着良好的对应关系．ＳｎＯ２元件气敏效应的发挥是粉体表面可逆与不可逆吸附共同作用的结果．     

半导体氧化物SnO2气敏元件研制中的几个有关机理问题

采用半导体氧化物S_nO_2材料,烧结工艺所生产的气敏元件,对被测气体有较高的灵敏度,在被检测气体含量只有十几到几百PPm时,气敏元件的阻值就可以产生很大的变化,这种阻值变化只要接上简单的电路就可以变换为电压的变化而测量出来。采用SnO_2气敏元件制成的检测仪器有较高的灵敏度、电路简单、造价低廉、使用方便等优点。因此一直处于半导体氧化物电阻式气敏传感器的主流。 SnO_2气敏元件在稳定性、互换性、定量检测以及对不同气体有较理想的选择性等方面,问题还尚未很好解决。其主要原因是导电机理表面效应牵涉的因素复杂所致。有待进一步研究。     

SnO2纳米晶薄膜栅FET式气敏元件的研制

利用溶胶－凝胶法合成出纳米晶ＳｎＯ２薄膜,该薄膜可以利用化学腐蚀方法光刻腐蚀,因此采用传统硅平面工艺可以制作出纳米晶ＳｎＯ２薄膜栅ＦＥＴ式气敏元件,实现了制备纳米晶材料的溶胶－凝胶工艺与硅平面工艺的兼容。对器件的测试结果表明,纳米晶ＳｎＯ２薄膜栅ＦＥＴ式气敏元件可以在常温下工作,元件的漏电流在乙醇气体中减小,掺杂镧以后,漏电流变化幅度增大。     

高选择性的一氧化碳气敏元件

气敏元件的选择性是当前的主要研究课题之一。以水解制得的二氧化锡为主体材料,氯化钯为活性催化剂,并添加质量分数w=(5～10)×10~(-2)的镧系稀土氧化物,来提高元件的反应选择性;改变元件的工作条件,利用元件在200℃以下对一氧化碳具有高吸附性的特点,制得具有高选择性的一氧化碳气敏元件。     

SnO_2基CO气敏材料的制备与掺杂研究

以溶胶–凝胶法制备的SnO2纳米材料为基,采用Sb2O3掺杂改性,制备出CO气敏材料。用XRD分析了材料的结构、物相和颗粒度。通过同步TGA/DSC热重分析的方法分析了材料的稳定性。结果表明:掺入w(Sb2O3)为2%时,可以抑制晶粒度的长大,同时提高了材料的稳定性。工作温度在90~110℃变化时,气敏元件电阻值波动不大((R10R20) /R10= 12%)。R10和R20分别表示元件在空气中90℃和110℃时的阻值。     

制备工艺对厚膜SnO_2气敏元件性能的影响

采用平面丝网印刷技术制备不同厚度的 Sn O2 厚膜气敏试样 ,在不同温度下进行热处理后 ,测量试样对乙醇气体的灵敏度 ,研究热处理温度及敏感膜厚度等对元件性能的影响。结果表明 ,热处理温度和膜厚的均匀性会影响元件的电阻值和灵敏度 ,准确控制热处理温度和膜厚能显著改善元件的灵敏度和一致性。     

SnO2厚膜NO2新型气敏元件的研制

根据霍耳效应,用真空镀膜法制备之SnO2厚膜,制备了NO2新型气敏元件,并对其气敏性能进行了测试。结果表明:在一定的温度和湿度下,即使没有加热,元件对体积分数为20×10–6的NO2气体的灵敏度可达5.94,响应时间为36 s,恢复时间为22 s。因此,利用霍耳效应来制作气敏元件是一条可行的新思路。     

Pd掺杂SnO2气敏薄膜XPS分析及其气敏性能研究

分别在氧气和氩气气氛下,于纯SnO<,2>气敏薄膜上溅射金属Pd制备了Pd掺杂SnO<,2>,气敏薄膜.利用XPS分析了溅射气氛和老化处理对该气敏薄膜表面元素含量变化的影响.结果表明:溅射气氛和老化处理对气敏薄膜的表面吸附氧含量和其他元素的含量均有很大影响,如氩气气氛下制备的Pd/SnO<,2>气敏薄膜在老化前与400...     

Strain‐Mediated Inverse Photoresistivity in SrRuO3/La0.7Sr0.3MnO3 Superlattices

In the pursuit of novel functionalities by utilizing the lattice degree of freedom in complex oxide heterostructure, the control mechanism through direct strain manipulation across the interfaces is still under development, especially with various stimuli, such as electric field, magnetic field, light, etc. In this study, the superlattices consisting of colossal‐magnetoresistive manganites La_0.7Sr_0.3MnO₃ (LSMO) and photostrictive SrRuO₃ (SRO) have been designed to investigate the light‐dependent controllability of lattice order in the corresponding functionalities and rich interface physics. Two substrates, SrTiO₃ (STO) and LaAlO₃ (LAO), have been employed to provide the different strain environments to the superlattice system, in which the LSMO sublayers exhibit different orbital occupations. Subsequently, by introducing light, we can modulate the strain state and orbital preference of LSMO sublayers through light‐induced expansion of SRO sublayers, leading to surprisingly opposite changes in photoresistivity. The observed photoresistivity decreases in the superlattice grown on STO substrate while increases in the superlattice grown on LAO substrate under light illumination. This work has presented a model system that demonstrates the manipulation of orbital–lattice coupling and the resultant functionalities in artificial oxide superlattices via light stimulus.     

Large,Temperature‐Tunable Low‐Field Magnetoresistance in La0.7Sr0.3MnO3:NiO Nanocomposite Films Modulated by Microstructures

Magnetic properties and low‐field magnetoresistance (LFMR) in La_0.7Sr_0.3MnO₃ (LSMO):NiO nanocomposite films grown on SrTiO₃ (001) substrates, which are shown to be tunable with different microstructures, are investigated. The LSMO:NiO nanocomposite films with NiO volume ratio of 50% have a checkerboard‐like structure and show a large LFMR in a temperature range from 200 to 300 K (≈17% at 250 K with a magnetic field of 1 T). As the NiO volume ratio is increased to 70%, a nano‐columnar structure formed in the films. Their LFMR is significantly enhanced at a wide temperature range of 10–210 K. The highest value of LFMR with 41% is achieved at 10 K in a magnetic field of 1 T. The enhanced LFMR can be considered to result from the electron scattering at the ferromagnetic LSMO/NiO interfaces and magnetic tunnel junctions (MTJs) of LSMO/NiO/LSMO at the nanometer scale. These results demonstrate that large and tunable LFMR from low temperature to room temperature can be realized by controlling the microstructures in the epitaxial La_0.7Sr_0.3MnO₃:NiO nano­composite thin films, which will be expected to be applied in the devices using for a wide temperature range.     

射频磁控溅射参数对 Ba0.7Sr0.3TiO3薄膜结构和性能的影响

采用射频磁控溅射法在 Pt/TiO2/SiO2/Si(100) 衬底上制备了Ba0.7Sr0.3TiO3薄膜,研究了工作气压、衬底温度等溅射参数对Ba0.7Sr0.3TiO3薄膜结构和电学性质的影响.使用 XRD 分析了工作气压为 2Pa、衬底温度分别为 200 ℃、400 ℃、600℃(组a),以及衬底温度为600℃、工作气压分别为 1.5Pa、2.0Pa、2.5Pa、3.0Pa 和 5.0Pa (组b)两组薄膜的微结构,结果表明工作气压在 2.5Pa 以下、衬底温度为 600℃时沉积的薄膜具有较好的钙钛矿结构.在 1.5Pa 条件下溅射的薄膜具有明显的(111)择优取向.在2.5Pa时,Pt/Ba0.7Sr0.3TiO3/Pt电容有最优铁电性能,在外加4 V电压(电场为 80 kV/cm)下,剩余极化 (Pr) 和矫顽场(Ec)分别为 2.32 μC/cm2、21.1 kV/cm.     

Vertical (La,Sr)MnO3 Nanorods from Track‐Etched Polymers Directly Buffering Substrates

A novel and general methodology for preparing vertical, complex‐oxide nanostructures from a sol–gel‐based polymer‐precursor solutions is developed using track‐etched polymers directly buffering substrates. This method is able to develop a nanostructure over the entire substrate, the dimensions and localization of the vertical nanostructures being preset by the polymeric nanotemplate. Thereby, nanostructures with lateral sizes in the range of 100 to 300 nm and up to 500 nm in height have been grown. Two examples are presented herein, the latter being the evolution of the initial, metastable nanostructure. Specifically, La_0.7Sr_0.3MnO₃ polycrystalline rods are grown at mild temperatures (800 °C); upon strong thermal activation (1000 °C) they suffer a profound transformation into vertical, single‐crystalline (La,Sr)_xO_y nanopyramids sitting on a La_0.7Sr_0.3MnO₃ epitaxial wetting layer. The driving force for this outstanding nanostructural evolution is the minimization of the total energy of the system, which is reached by reducing the grain‐boundary, total‐surface, and strain‐relaxation energies. Finally, advanced electron‐microscopy techniques are used to highlight the complex phase separation and structural transformations occurring when the metastable state is overcome.     

La0.7Ca0.3MnO3多晶薄膜的sol-gel法制备及表征

以La、Ca、Mn的无机盐替代相应的醇盐,以冰乙酸为溶剂,乙酰丙酮(AcAc)为螯合剂,采用sol-gel法在Si(110)衬底上制备了La0.7Ca0.3MnO3(LCMO)多晶薄膜,并用FTIR、XRD、SEM、EDS和TEM等分析手段对薄膜进行了表征,通过不同磁场下电阻一温度(R-T)曲线,研究了样品的输运性质及...     

CuO对(Ni_(1/3)Nb_(2/3))_(0.7)Ti_(0.3)O_2微波陶瓷低温烧结性能的影响

采用传统固相反应法制作(Ni1/3Nb2/3)0.7Ti0.3O2微波陶瓷,研究了CuO掺杂对所制陶瓷低温烧结性能、微观结构、相构成及微波介电性能的影响。结果表明,掺杂少量的CuO就能显著降低(Ni1/3Nb2/3)0.7Ti0.3O2陶瓷的烧结温度,且能改善陶瓷τf。当CuO掺杂量(质量分数)为1.0%时,(Ni1/3Nb2/3)0.7Ti0.3O2在950℃烧结,显示出良好的微波介电性能:εr=67.65,Q·f=3708GHz,τf=14.3×10-6/℃。     

掺Sm2O3的SnO2纳米粉体对C2H2气敏特性的研究

用化学沉淀法制备了SnO2纳米材料,利用XRD和SEM对合成产物进行了表征.采用旁热式结构制成了以SnO2为基体材料,掺杂Sm2O3的气体传感器.通过元件对C2H2气敏特性的测试表明:Sm2O3的掺杂可以明显地提高SnO2气敏材料对C2H2气体的灵敏度,当工作温度为180℃,C2H2浓度为1000ppm时,元件的灵敏度为64,响应恢复时间分别为3和20s.讨论了不同相对湿度对元件气敏特性的影响.     

掺Sm2O3的SnO2纳米粉体对C2H2气敏特性的研究

用化学沉淀法制备了SnO2纳米材料,利用XRD和SEM对合成产物进行了表征.采用旁热式结构制成了以SnO2为基体材料,掺杂Sm2O3的气体传感器.通过元件对C2H2气敏特性的测试表明:Sm2O3的掺杂可以明显地提高SnO2气敏材料对C2H2气体的灵敏度,当工作温度为180℃,C2H2浓度为1000ppm时,元件的灵敏度为64,响应恢复时间分别为3和20s.讨论了不同相对湿度对元件气敏特性的影响.