排序方式: 共有56条查询结果,搜索用时 15 毫秒
21.
22.
FLUX CREEP, FLUX PINNING AND CRITICAL CURRENT DENSITY OF Y-, Gd-, AND Tl-BASED SUPERCONDUCTIVE THIN FILMS
下载免费PDF全文
![点击此处可从《中国物理》网站下载免费的PDF全文](/ch/ext_images/free.gif)
Magnetic hysteresis loops have been measured for YBa2Cu3O6+x, GdBa2Cu3O6+x and Tl2Ba2Ca2Cu3O10-y films at different temperatures with a vibrating sample magnetometer. Based on Bean model, magnetic critical current density Jcm has been derived approximately. The field and temperature dependence of Jcm for all samples can be written as: Jcm= Jc0(T)×f(B,T), Where f(B,T) = 1 - Aln(B/B0(T)), which is similar to the transport critical density strongly affected by flux creep: Jct = Jc0(B,t)(1 - (kBT/U0)ln(BΩd/Ec)). The extraordinary similarity suggests that Jcm is determined not only by flux pinning but also by flux creep. In the first formula, f(B,T) may be correlated with the effect of flux creep on Jcm, and Jc0(T) is determined by flux pinning. Jc0(T) is independent of magnetic field and is proportional to (Tc - T). Similar results have also been found for other samples. It may be the common characteristic of high-Tc superconductors. Magnetic relaxation of YBa2Cu3O6+x and GdBa2Cu3O6+x films has been measured at LN2 temperature. Using the equation of Hagen et al., effective activation energy U0 has been deduced, which is about 0.3eV, one order bigger than the value obtained by A = kBT/U0. U0 is almost independent of the field in the field range selected. 相似文献
23.
a—SiNx:H薄膜对a—Si:H TFT阈值电压的影响 总被引:4,自引:0,他引:4
介绍了测定a-Si:HTFT闽值电压的实验方法。重点研究了改变a-SiNx:H薄膜淀积时反应气体NH3/SiH4流速比以及a-SiNx:H膜厚对a-Si:HTFT阈值电压的影响。对实验结果进行了分析。实验结果表明:a-Si:HTFT的阈值电压随a-SiNx:H的膜厚增加而增大;增大X-SiNx:H薄膜淀积时NH3/SiH4气体流速比,可明显减小a-Si:HTFT的阈值电压。 相似文献
24.
25.
采用新电极结构的PECVD技术,在高功率密度、高氢稀释比、低温、偏压及低反应气压的条件下,在SiO2玻璃表面形成双等离子流,增加了SiO2表面SiC的成核几率,增强成核作用,形成纳米晶。采用高H2等离子体刻蚀弱的、扭曲的、非晶Si-C及Si-Si和Si-H等键时,由于H等离子体对纳米SiC晶粒与非晶态键的差异刻蚀作用,产生自组织生长,发生晶化。Raman光谱和透射电子衍射(EM)的测试结果表明,纳米晶SiC是4H-SiC多型结构。实验结果指出,SiC纳米晶的形成必须经过偏压预处理成核,并且其晶化存在一个功率密度阈值;当低于这一功率密度阈值时,晶化消失;当超过这一阈值时,纳米晶含量随功率密度的提高而增加,晶粒尺寸加大。电子显微照片表明晶粒尺寸为10-28nm,形状为微柱体。随着晶化作用的加强,电导率增加,导电机理是渗流作用所致。 相似文献
26.
27.
通过磁控溅射沉积以及高温热退火处理,在5.08 cm(2 inch)c-plane蓝宝石异质衬底上制备出单晶β-Ga2O3薄膜,研究了溅射气氛中氧分压对β-Ga2O3薄膜的晶体结构以及光学特性的影响.通过调控氧分压,获得了具有{-2 01}晶面族X射线衍射峰的β-Ga2O3薄膜,其最大晶粒尺寸达到138 nm,在300~800 nm波段透射率大于80%,最大光学带隙达5.12 eV.最优的薄膜表面粗糙度达0.401 nm,800 nm波长处折射率为1.94.实验结果表明,降低氧分压有利于溅射粒子动能增大、数量增多,从而提升β-Ga2O3薄膜结晶质量、增加薄膜透射率和光学带隙;适当提高氧分压则有利于改善薄膜表面平整度,并提高致密度. 相似文献
28.
29.
30.
基于SST89C54/58的单片机仿真器的设计 总被引:1,自引:0,他引:1
介绍美国SST公司的51系列单片机SsT89C54/58的程序存储器的结构特点以及基于SST89C54/58的KEILC51单片机仿真器的设计。 相似文献