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1.
离子束增强沉积VO2多晶薄膜的温度系数   总被引:2,自引:0,他引:2       下载免费PDF全文
李金华  袁宁一 《物理学报》2004,53(8):2683-2686
用改进的离子束增强沉积方法和恰当的退火从V2O5粉末直接制备了VO2多晶薄膜.实验测试表明,薄膜的取向单一、相变特性显著、结构致密、界面结合牢固、工艺性能良好,薄膜的电阻温度系数(TCR)最高可达4.23%/K.从成膜机理出发,较详细地讨论了离子束增强沉积 VO2多晶薄膜的TCR高于VOx薄膜的TCR的原因.分析认为,单一取向的VO2结构使薄膜晶粒具有较高的电导激活能,致密的薄膜结构减少了氧空位和晶界宽度,使离子束增强沉积 VO2多晶薄膜结构比其他方法制备的VOx薄膜更接近于单晶VO2是其具有高TCR的原 关键词: VO2多晶薄膜 离子束增强沉积 热电阻温度系数  相似文献   

2.
超高温度系数V0.97W0.03O2多晶薄膜的制备研究   总被引:1,自引:0,他引:1       下载免费PDF全文
将V2O5粉体与WO3粉体均匀混合并压制成靶,用离子束增强沉积加后退火技术在SiO2衬底上制备掺钨VO2多晶薄膜.X射线衍射表明,薄膜取向单一,为VO2结构的[002]相,晶格参数d比VO2粉晶增大约0.34%;薄膜从半导体相向金属相转变的相变温度约28℃;室温(300K)时的电阻-温度系数(TCR)可大于10%/K,是目前红外热成像薄膜TCR的四倍.W离子的半径大于V离子的半径,W的掺入在薄膜中引入了张应力,使薄膜相变温度降低到室温附近,是IBEDV0.97W0.03O2薄膜的室温电阻温度系数提高的原因.  相似文献   

3.
采用了一种用离子束增强沉积从V2O5粉末直接制备VO2薄膜的新方法,将纯度为997%的V2O5粉末压成溅射靶,在用Ar离子束溅射的同时,用氩氢混合束对沉积膜作高剂量离子注入,使沉积膜中V2O5的V—O键断裂,进而被注入的氢还原,退火后获得热电阻温度系数(TCR)高达4%的VO2薄膜.高剂量的氩氢混合束注入对薄膜引入应力,使薄膜的转换温度降低、电阻温度曲线斜率变大,是薄膜TCR增大的原因 关键词: 离子束增强沉积 VO2薄膜 热电阻温度系数  相似文献   

4.
将V2O5粉体与WO3粉体均匀混合并压制成靶,用离子束增强沉积加后退火技术在SiO2衬底上制备掺钨VO2多晶薄膜.X射线衍射表明,薄膜取向单一,为VO2结构的[002]相,晶格参数d比VO2粉晶增大约0.34%;薄膜从半导体相向金属相转变的相变温度约28;室温(300 K)时的电阻-温度系数(TCR)可大于10%/K,是目前红外热成像薄膜TCR的四倍.W离子的半径大于V离子的半径,W的掺入在薄膜中引入了张应力,使薄膜相变温度降低到室温附近,是IBED V0.97W0.03O2薄膜的室温电阻温度系数提高的原因. 关键词: 二氧化钒薄膜 薄膜掺杂 离子束增强沉积  相似文献   

5.
射频磁控溅射制备氧化钒薄膜的研究   总被引:1,自引:0,他引:1       下载免费PDF全文
马卫红  蔡长龙 《应用光学》2012,33(1):159-163
氧化钒(VOx)薄膜是一种广泛应用于红外热成像探测的薄膜材料,研究VOx薄膜的制备工艺、获取高电阻温度系数(TCR)的VOx薄膜具有重要意义。以高纯金属钒作靶材,采用射频磁控溅射的方法在室温下制备了VOx薄膜。主要研究了氩氧流量比以及功率等工艺参数对薄膜TCR的影响,获得了较好的工艺参数。采用万用表和X射线光电子能谱仪(XPS)分别测试了不同条件下射频磁控溅射法制备的VOx薄膜的电阻特性和薄膜成分,测试结果表明,采用所获得的较好工艺参数制备的VOx薄膜TCR值大于1.8%。  相似文献   

6.
以LiCoO2为阴极的全固态薄膜锂电池的研究   总被引:3,自引:0,他引:3  
采用射频磁控溅射技术制备了非晶态和不同取向的多晶LiCoO2薄膜,利用XRD和SEM研究了不同温度退火后LiCoO2薄膜的结构和形貌.以具有不同结构的LiCoO2薄膜为阴极、含氮磷酸锂薄膜为电解质以及金属锂薄膜为阳极,成功地制备了电化学性能不同的全固态薄膜锂电池.由电化学研究结果表明,LiCoO2薄膜的结构和多晶取向决定了薄膜电池的电化学性能.采用具有一定取向的多晶LiCoO2薄膜制备的全固态薄膜锂电池具有最佳的性能,稳定放电容量达到55.4μAh/cm2μm,充放电循环次数超过450次.  相似文献   

7.
 在基底清洗、薄膜沉积和薄膜后处理三个阶段均采用离子束技术,制备了氧化铪薄膜,并对薄膜的光学性能、表面特性和激光损伤阈值特性进行测试和研究。结果表明,利用离子束技术清洗基底可以增强表面吸附;离子束辅助沉积在合适离子束能量下可以得到高堆积密度、高损伤阈值的薄膜;离子束后处理氧化铪薄膜可以降低表面粗糙度,改善抗激光损伤阈值。说明在三个薄膜制备阶段同时采用合适的离子束参数可以制备出结构致密、阈值高、表面粗糙度好的氧化铪薄膜。  相似文献   

8.
溶胶-凝胶VO2薄膜转换特性研究   总被引:14,自引:0,他引:14       下载免费PDF全文
利用溶胶凝胶法在SiO2Si衬底上沉积高取向的V2O5薄膜,在压强低于2Pa,温度高于400℃的条件下,对V2O5薄膜进行真空烘烤,获得了电阻率变化3个数量级以上、弛豫宽度为62℃的VO2多晶薄膜.以X射线衍射(XRD)、扫描电子显微镜(SEM)图和电阻率转换特性等实验结果为依据,详细分析了溶胶凝胶薄膜在真空烘烤时从V2O5向VO2的转化,它经历了从VnO2n+1(n=2,3,4,6)到VO2的过程.实验证明,根据选择合适的成膜热处理条件和真空烘烤条件是实现溶胶凝胶V2O5结构向VO2结构成功转换的关键 关键词: 溶胶-凝胶法 氧化钒薄膜 VO2膜转换特性  相似文献   

9.
采用直流磁控溅射和后退火氧化的方法在掺铝氧化锌(AZO)导电玻璃上制备了二氧化钒(VO2)薄膜,研究了不同的退火温度、退火时间对VO2/AZO复合薄膜制备的影响,并对复合薄膜的结构、组分、光电特性进行了测试与分析.结果表明,导电玻璃上的AZO没有改变VO2的取向生长,但明显改变了VO2薄膜的表面形貌特征.与用相同工艺和条件在普通玻璃基底上制备的VO2薄膜相比,VO2/AZO复合薄膜的相变温度降低约25?C,热滞回线宽度收窄至6?C,相变前后可见光透过率均在50%以上,1500 nm处红外透过率约为55%和21%,电阻率变化达3个数量级.该复合薄膜表面平滑致密,制备工艺简单,性能稳定,可应用于新型光电器件.  相似文献   

10.
采用离子束增强沉积方法在Si和SiO2/Si衬底上制备In-N共掺杂ZnO薄膜(INZO),溅射靶是用ZnO和2 atm% In2O3粉体均匀混合并压制而成,在氩离子溅射ZnO靶的同时,氮、氩混合离子束垂直注入沉积的薄膜.实验结果显示INZO薄膜具有(002)的择优取向,并且为p型导电,电阻率最低为0.9Ωcm.薄膜在氮气、氧气气氛下退火,对薄膜的结构和电学特性与成膜和退火条件的关系进行了分析. 关键词: 氧化锌薄膜 p型掺杂 离子束增强沉积  相似文献   

11.
VO2 thin films with semiconductor-to-metal phase-transition properties were prepared by inorganic sol-gel and IBED (ion-beam-enhanced deposition) methods on SiO2/Si substrate. The crystalline phase and the shape and width of the hysteresis curves of these VO2 films were significantly different. For sol-gel VO2 films, the transition started at close to 62 °C upon heating. The temperature interval needed to complete the phase transition was 8 °C, the ratio of resistance (R20 °C/R80 °C) reached three orders and the hysteresis width was 6 °C. However, the IBED film post-annealed in Ar at 700 °C underwent a phase transition from 45 °C to 80 °C, the ratio of resistance was more than two orders and the hysteresis width was 2 °C. In addition, the TCR (temperature coefficient of resistance) at 22 °C of the IBED film was 3.5%/K, much larger than the 0.7%/K TCR of the sol-gel film. PACS 73.50.F; 73.66.E; 81.20; 81.05.Z; 81.15  相似文献   

12.
A comparative study of the out-of-plane anisotropic magnetoresistance (AMR) in single crystalline and polycrystalline thin films of phase separated manganite Nd0.51Sr0.49MnO3 has been carried out. On-axis DC magnetron sputtering was used to deposit the single crystalline films (30 and 100 nm in thickness) on single crystal (0 0 1) LaAlO3 (LAO) and polycrystalline films (100 nm) on (1 0 0) Yttrium-stabilized ZrO2 (YSZ) substrates. The in-plane and out-of-plane magnetotransport properties of these films differ significantly. A large low field AMR is observed in all the films. AMR shows a peak below the insulator-metal transition temperature in the single crystalline films, while the same increases monotonically in the polycrystalline film. Relatively larger low field AMR (∼20% at T=78 K and H=1.7 kOe) in the polycrystalline films suggests the dominance of the shape anisotropy.  相似文献   

13.
In the present study we report the precise resistivity measurements for the polycrystalline bulk sample as well as highly oriented thin-films of La0.8Ca0.2MnO3. The poly crystalline sample was prepared by standard solid-state reaction route and the oriented thin film was prepared by pulsed laser deposition (PLD). The phase purity of these samples was confirmed by X-ray diffraction and the back-scattered electron imaging using scanning electron microscopy (SEM). The oxygen stoichiometry analysis was done by iodimetry titration. The resistivities of these samples were carried out with four-probe resistivity measurement setup. The observed temperature dependence of resistivity data for both the samples was fitted using the polaron model. We have found that polaronic model fits well with the experimental data of both polycrystalline and single crystal samples. A new phenomenological model is proposed and used to estimate contribution to the resistivity due to grain boundary in the ferromagnetic state of polycrystalline manganites and it has been shown that the scattering of electrons from the grain boundary (grain surface) is a function of temperature and controlled by the effective grain resistance at that temperature.  相似文献   

14.
Mandal P  Speck A  Ko C  Ramanathan S 《Optics letters》2011,36(10):1927-1929
We present results on terahertz (THz) spectroscopy on epitaxial vanadium dioxide (VO(2)) films grown on sapphire across the metal-insulator transition. X-ray diffraction indicates the VO(2) film is highly oriented with the crystallographic relationship: (002)(film)//(0006)(sub) and [010](film)//[2 ?1 ?10](sub). THz studies measuring the change in transmission as a function of temperature demonstrate an 85% reduction in transmission as the thin film completes its phase transition to the conducting phase, which is much greater than the previous observation on polycrystalline films. This indicates the crucial role of microstructure and phase homogeneity in influencing THz properties.  相似文献   

15.
用掠入射X射线衍射法观察到钛酸铅多晶铁电薄膜表面层与体内的相变温度不同,表面层的结构参数也有异于体内;唯象地把多晶铁电薄膜抽象为一个表面层为细晶粒、低应变层,体内为粗晶粒、高应变层的两层结构,根据应力和晶粒尺寸效应对铁电相变的影响,解释了钛酸铅多晶铁电薄膜的相变特征 关键词:  相似文献   

16.
<正>This paper reports that GaSb thin films have been co-deposited on soda-lime glass substrates.The GaSb thin film structural properties are characterized by Raman spectroscopy.The Sb-A1g/GaSb-TO ratio decreases rapidly with the increase of substrate temperature,which suggests a small amount of crystalline Sb in the GaSb thin film and suggests that Sb atoms in the thin film decrease.In Raman spectra,the transverse optical(TO) mode intensity is stronger than that of the longitudinal optical(LO) mode,which indicates that all the samples are disordered.The LO/TO intensity ratio increases with increasing substrate temperature which suggests the improved polycrystalline quality of the GaSb thin film.A downshift of the TO and LO frequencies of the polycrystalline GaSb thin film to single crystalline bulk GaSb Raman spectra is also observed.The uniaxial stress in GaSb thin film is calculated and the value is around 1.0 GPa.The uniaxial stress decreases with increasing substrate temperature.These results suggest that a higher substrate temperature is beneficial in relaxing the stress in GaSb thin film.  相似文献   

17.
It was observed clearly that the sputter damage due to Ar+ ion bombardment on metal single crystalline surfaces is extremely low and the local surface atomic structure is preserved, which is totally different from semiconductor single crystalline surfaces. Medium energy ion scattering spectroscopy (MEIS) shows that there is little irradiation damage on the metal single crystalline surfaces such as Pt(111), Pt(100), and Cu(111), in contrast to the semiconductor Si(100) surfaces, for the ion energy of 3–7 keV even above 1016–1017 ions/cm2 ion doses at room temperature. However, low energy electron diffraction (LEED) spots became blurred after bombardment. Transmission Electron Microscopy (TEM) studies of a Pt polycrystalline thin film showed formation of dislocations after sputtering. Complementary MEIS, LEED and TEM data show that on sputtered single-crystal metal surfaces, metal atoms recrystallize at room temperature after each ion impact. After repeated ion impacts, local defects accumulate to degrade long range orders.  相似文献   

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