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排序方式: 共有118条查询结果,搜索用时 109 毫秒
1.
赵青南 《武汉理工大学学报(材料科学英文版)》2005,(4)
1Introduction Theultravioletrays(UV)insunlight(-4%)cantransmitintoroomthroughcommonfloatglass,theUVcanmakethematerialsintheroom,eg,paper,furni ture,textilefabricandplastics,becoloredanddeterio rated.ShieldingfromUVirradiationisofinterestinmanyfields.Formu… 相似文献
2.
Young?Ah?JeonEmail author Kwang?Soo?No Jong?Sung?Kim Young?Soo?Yoon 《Metals and Materials International》2003,9(4):383-387
ZnO films for electronic applications were deposited by radio-frequency (rf) sputtering onto various metal bottom electrodes
(Pt/Ti, W, Ni) to investigate such structural properties as crystallinity and surface morphology. The crystallinity, surface
morphology and composition of the as-deposited films were studied using X-ray diffraction (XRD), scanning electron microscopy
(SEM) and Rutherford back-scattering spectrometry (RBS), respectively. The preferred orientation and surface morphologies
were strongly influenced by the type of bottom electrodes. The ZnO films with (200) texturing deposited on Pt/Ti/SiO2/Si showed a smoother and smaller grain size than those deposited on W and Ni. The ZnO films on Pt and W electrodes exhibited
compressive residual stress.
This article is based on a presentation made in the 2002 Korea-US symposium on the “Phase Transformations of Nano-Materials”,
organized as a special program of the 2002 Annual Meeting of the Korean Institute of Metals and Materials, held at Yonsei
University, Seoul, Korea on October 25–26, 2002. 相似文献
3.
研究射频场频率对二分量玻色-爱因斯坦凝聚体(BEC)原子数密度长时间演化特性的影响,研究结果显示当射频场频率较小而时间较长时BEC第二分量原子数密度的演化呈现出量子力学中典型的崩塌与复苏现象;原子数密度在更长时间的动力学行为中,若射频场频率增大,则呈现出崩塌与复苏现象的原子数密度震荡曲线整体逐渐下降. 相似文献
4.
感应耦合等离子体(ICP)是微电子工业刻蚀高精度沟槽结构的首选高密度等离子体源.研究ICP的电特性与等离子体电学参量的变化显得非常重要.本文中,在平板型ICP源的感应线圈和介质窗口之间,使用了对称、均匀、呈辐射状的法拉第屏蔽板.结果表明,屏蔽板的使用不仅极大地降低了干扰等离子体参量测量的等离子体射频电位,而且也降低了线圈中的放电电流和等离子体中的轴向微分磁场信号强度,但Ar等离子体的发射光谱表明,法拉第屏蔽的采用对等离子体功率吸收的影响不大.对测量信号中出现的高次谐波行为也做了定性的讨论. 相似文献
5.
Maisara Othman Richard Ritikos Noor Hamizah Khanis Nur Maisarah Abdul RashidSaadah Abdul Rahman Siti Meriam Ab GaniMuhamad Rasat Muhamad 《Thin solid films》2011,519(15):4981-4986
Carbon nitride (CNx) thin films were deposited by radio frequency plasma enhanced chemical vapour deposition (rf PECVD) technique from a gas mixture of methane (CH4), hydrogen (H2) and nitrogen (N2). The effects of rf power on the structural properties of CNx thin films were discussed in this paper. It was found that rf power had significant effects on the growth rate, structural and morphological properties of the deposited films. The point of transition of the growth rate trend marked the equilibrium condition for primary and secondary reactions in growth kinetics of the film with respect to rf power. The films grown at this optimum rf power were most ordered in structure with high surface roughness and had the lowest N incorporation. This work showed that H etching effects and ion bombardment effects increase with increase in rf power and strongly influenced the structure of the CNx films. 相似文献
6.
R. Ye 《Thin solid films》2007,515(9):4251-4257
Synthesis of alumina nanoparticles in an Ar-O2 inductively coupled radio frequency (rf) plasma controlled by axial quench gas injection was investigated. The flow and temperature fields for various quench gas flow rates in the plasma reactor, as well as the corresponding quench rates, were predicted using a renormalization group (RNG) k-ε turbulence model. Nanosize alumina particles were synthesized from the vapor phase by oxidation of aluminum in the plasma. The collected products were characterized by means of field emission scanning electron microscopy (FE-SEM), dynamic light scattering (DLS), and BET surface area analysis. The dependences of particle size and shape on the injection position and the flow rate of the quench gas were discussed. 相似文献
7.
Anodic formation of low-aspect-ratio porous alumina films for metal-oxide sensor application 总被引:1,自引:0,他引:1
Thin nanoporous anodic alumina films, of low aspect ratio (1:1), with two distinctive pore sizes and morphologies were prepared by two-step constant-current anodising of aluminium layers on SiO2/Si substrates in 0.4 mol dm−3 tartaric (TA) and malonic acid (MA) electrolytes and then modified by open-circuit dissolution. The anodic films were employed as a support material for sputtering-deposition of thin WO3 layers in view of exploiting their gas sensing properties. The films and deposits were characterized by scanning electron microscopy, X-ray diffraction and electric resistance measurements at fixed temperatures in the range of 100-300 °C upon NH3 and CO gas exposures. Test sensors prepared from the annealed and stabilized alumina-supported WO3 active layers were insensitive to CO but showed considerably enhanced responses to NH3 at 300 °C, the sensitivity depending upon the anodic film nature, the pore size and the surface morphology. The increased sensor sensitivity is due to the substantially enlarged film surface area of the TA-supported WO3 films and the nanostructured, camomile-like morphology of the MA-supported WO3 films. Sensing mechanisms in the alumina-supported WO3 active layers are discussed. 相似文献
8.
9.
利用AES方法研究了CdIn2O4膜的成分分布。膜中的Cd、In和O成份随O浓度的变化而变化,并对膜的电学性质有重要影响。 相似文献
10.
Chihiro J. Uchibori Masayuki Okunishi T. Oku A. Otsuki Naoki Ono Masanori Murakami 《Journal of Electronic Materials》1994,23(9):983-989
The formation mechanisms of InAs/Ni/W ohmic contacts to n-type GaAs prepared by radio-frequency (rf) sputtering were studied
by measuring contact resistances (Rc) using a transmission line method and by analyzing the interfacial structure mainly by x-ray diffraction and transmission
electron microscopy. Current-voltage characteristics of the InAs/Ni/W contacts after annealing at temperatures above 600°C
showed “ohmic-like behavior.” In order to obtain the “ohmic” behavior in the contacts, pre-heating at 300°C prior to high
temperature annealing was found to be essential. The contacts showed ohmic behavior after annealing at temperatures in the
range of 500∼850°C and contact resistance values of as low as ∼0.3Ω-mm were obtained. By analyzing the interfacial structures
of these contacts, InxGa1−xAs layers with low density of misfit dislocations at the InxGa1−xAs and GaAs interface were observed to grow epitaxially on the GaAs substrate upon heating at high temperatures. This intermediate
InxGa1−xAs layer is believed to divide the high energy barrier at the contact metal and GaAs interface into two low barriers, resulting
in reduction of the contact resistance. In addition, Ni was found to play a key role to relax a strain in the InxGa1−xAs layer (introduced due to lattice mismatch between the InxGa1−xAs and GaAs) by forming an intermediate NixGaAs layer on the GaAs surface prior to formation of the InxGa1−xxAs layer. 相似文献