首页 | 本学科首页   官方微博 | 高级检索  
文章检索
  按 检索   检索词:      
出版年份:   被引次数:   他引次数: 提示:输入*表示无穷大
  收费全文   378篇
  免费   288篇
  国内免费   57篇
化学   68篇
晶体学   132篇
力学   29篇
综合类   8篇
数学   2篇
物理学   484篇
  2023年   4篇
  2022年   11篇
  2021年   16篇
  2020年   9篇
  2019年   6篇
  2018年   14篇
  2017年   26篇
  2016年   25篇
  2015年   19篇
  2014年   35篇
  2013年   40篇
  2012年   65篇
  2011年   78篇
  2010年   49篇
  2009年   53篇
  2008年   59篇
  2007年   39篇
  2006年   45篇
  2005年   33篇
  2004年   24篇
  2003年   15篇
  2002年   14篇
  2001年   11篇
  2000年   9篇
  1999年   3篇
  1998年   4篇
  1997年   5篇
  1996年   2篇
  1995年   6篇
  1994年   1篇
  1990年   1篇
  1988年   1篇
  1985年   1篇
排序方式: 共有723条查询结果,搜索用时 15 毫秒
11.
利用原子力显微镜分析了ZnO薄膜在具有本征氧化层的Si(100)和Si(111)基片上的表面形貌 随沉积时间的演化. 通过对薄膜生长形貌的动力学标度表征,研究了射频反应磁控溅射条件 下,ZnO薄膜的成核过程及生长动力学行为. 研究发现,ZnO在基片表面的成核过程可分为初 期成核阶段、低速率成核阶段和二次成核阶段. 对于Si(100)基片,三个成核阶段的生长指 数分别为β1=1.04,β2=0.25±0.01,β3=0.74;对 于Si(11 关键词: ZnO薄膜 磁控溅射 生长动力学 成核机制  相似文献   
12.
用射频磁控溅射法在80℃衬底温度下制备出MgxZn1-xO(x=0.16)薄膜,用X射线衍射(XRD)、光致发光(PL)和透射谱研究了退火温度对MgxZn1-xO薄膜结构和光学性质的影响.测量结果显示,MgxZn1-xO薄膜为单相六角纤锌矿结构,并且具有沿c轴的择优取向;随着退火温度的升高,(002)XRD峰强度、平均晶粒尺寸和紫外PL峰强度增大,(002)XRD峰半高宽(F 关键词: xZn1-xO薄膜')" href="#">MgxZn1-xO薄膜 射频磁控溅射 退火  相似文献   
13.
利用多靶磁控溅射技术制备了Au/SiO2纳米颗粒分散氧化物多层复合薄膜.研究了在保持Au单层颗粒膜沉积时间一定时薄膜厚度一定、变化SiO2的沉积时间及SiO2的沉积时间一定而改变薄膜厚度时,多层薄膜在薄膜厚度方向的微观结构对吸收光谱的影响.研究结果表明:具有纳米层状结构的Au/SiO2多层薄膜在560 nm波长附近有明显的表面等离子共振吸收峰,吸收峰的强度随Au颗粒的浓度增加而增强,在Au颗粒浓度相同的情况下,复合薄膜 关键词: 2纳米复合薄膜')" href="#">Au/SiO2纳米复合薄膜 多靶磁控溅射 吸收光谱 有效介质理论  相似文献   
14.
计算机模拟仿真射频磁控溅射实验制备薄膜及离于电池电极,研究了在特定实验条件下薄膜的生长过程,并分析了影响薄膜生长的部分因素。  相似文献   
15.
Thin films of a-SiOx (0 < x < 2) were prepared by reactive r.f. magnetron sputtering from a polycrystalline-silicon target in an Ar/O2 gas mixture. The oxygen partial pressure in the deposition chamber was varied so as to obtain films with different values of x. The plasma was monitored, during depositions, by optical emission spectroscopy (OES) system. Energy dispersive X-ray (EDX) measurements and infra-red (IR) spectroscopy were used to study the compositional and structural properties of the deposited layers.Structural modifications of SiOx thin films have been induced by UV photons’ bombardment (wavelength of 248 nm) using a pulsed laser. IR spectroscopy and X-ray photoemission spectroscopy (XPS) were used to investigate the structural changes as a function of x value and incident energy. SiOx phase separation by spinodal decomposition was revealed. The IR peak position shifted towards high wavenumber values when the laser energy is increased. Values corresponding to the SiO2 material (only Si4+) have been found for laser irradiated samples, independently on the original x value. The phase separation process has a threshold energy that is in agreement with theoretical values calculated for the dissociation energy of the investigated material.For high values of the laser energy, crystalline silicon embedded in oxygen-rich silicon oxide was revealed by Raman spectroscopy.  相似文献   
16.
溅射功率对多层膜质量的影响   总被引:5,自引:1,他引:4  
用磁控溅射技术制备薄膜,用X射线衍射研究在基片和靶间距离固定的情况下不同的溅射功率对薄膜结构的影响。结果表明:过低的溅射功率下淀积的薄膜有畸变的X射线衍射特征峰,特征峰强度小,半峰全宽大。而比较高溅射功率得到的薄膜有比较尖锐的X射线衍射特征峰,强度高和半峰全宽非常窄。研究表明,X射线衍射特征峰强度小和半峰全宽大的薄膜结构疏松,而强度高和半峰全宽非常窄的薄膜结构致密。  相似文献   
17.
We report on Raman scattering of VO2 films prepared by radio frequency magnetron sputtering under different conditions. Our investigations revealed that the dominated Raman peaks shift towards high frequency for both V-rich and O-rich VO2 films, compared with the stoichiometry VO2 films. The experimental evidence is presented and the cause for nonstoichiometry dependence of Raman spectra of VO2 films is discussed.  相似文献   
18.
朱慧群  丁瑞钦  胡怡 《光子学报》2006,35(8):1194-1198
报导了射频磁控溅射与沉积气氛掺氢相结合制备单层(13~20 nm厚)高质量GaAs多晶态纳米薄膜的方法,研究了氢钝化对薄膜微观结构及光学性质的影响.对GaAs薄膜进行了X射线衍射、原子力显微镜、吸收光谱、光致荧光谱的研究分析.结果表明,衬底温度500℃的掺氢薄膜和520℃的薄膜呈面心立方闪锌矿结构,薄膜的晶团尺寸较大,微观表面较为粗糙,其吸收光谱出现了吸收边蓝移和明显的激子峰,带隙光致荧光峰强明显增加,说明氢在衬底温度500℃~520℃下对薄膜有重要的钝化作用.  相似文献   
19.
Unintentionally doped and zinc-doped indium nitride (U-InN and InN:Zn) films were deposited on (0 0 0 1) sapphire substrates by radio-frequency reactive magnetron sputtering, and all samples were then treated by annealing to form In2O3 films. U-InN and InN:Zn films have similar photon absorption characteristics. The as-deposited U-InN and InN:Zn film show the absorption edge, ∼1.8-1.9 eV. After the annealing process at 500 °C for 20 min, the absorption coefficient at the visible range apparently decreases, and the absorption edge is about 3.5 eV. Two emission peaks at 3.342 eV (371 nm) and 3.238 eV (383 nm) in the 20 K photoluminescence (PL) spectrum of In2O3:Zn films were identified as the free-exciton (FE) or the near band-to-band (B-B) and conduction-band-to-acceptor (C-A) recombination, respectively.  相似文献   
20.
Indium tin oxide (ITO) thin films were deposited by mid frequency pulsed dual magnetron sputtering using a metallic alloy target with 10 wt.% tin in an atmosphere of argon and oxygen. The aim of the work was to study the interdependence of structural, electrical and optical properties of ITO films deposited in the reactive and transition target mode, respectively. The deposition rate in the transition mode exceeds the deposition rate in the reactive mode by a factor of six, a maximum value of 100 nm·m min−1 could be achieved. This corresponds to a static deposition rate of 200 nm min−1. The lowest electrical resistivity of 1.1·10−3 Ω cm was measured at samples deposited in the high oxygen flow range in the transition mode. The samples show a good transparency in the visible range corresponding to extinction coefficients being below 10−2. X-ray diffraction was used to characterise crystalline structure as well as film stress. ITO films prepared in the transition mode show a slightly preferred orientation in (211) direction, whereas films deposited in the reactive mode are strongly (222) oriented. Compared to undoped In2O3 all samples have an enlarged lattice. The lattice strain perpendicular to the surface is about 0.8% and 2.0% for films grown in the transition and the reactive mode, respectively. Deposition in the transition mode introduces a biaxial film stress in the range of −300 MPa, while stress in reactive mode samples is −1500 MPa.  相似文献   
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号