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61.
以氟化镁为基底材料, 采用基底、金属网栅与频率选择表面一体化设计方法设计了一种雷达波与光学波段双带通的结构. 利用模式匹配法对设计结构的传输特性进行了仿真研究, 并将设计结果与制备样件的测试结果进行了对比分析. 结果发现: 采用一体化设计的方法设计光学透明频率选择表面, 不仅能够快速得到电场基函数而且还能够准确预估其谐振尺寸, 从而在提高计算效率的同时避免了模式互作用零点的出现. 采用一体化设计方法获得了具有稳定滤波特性的光学透明频率选择表面, 为雷达/红外双模制导头罩的电磁屏蔽技术和隐身技术提供了一种有效技术方案.
关键词:
复合制导
频率选择表面
金属网栅
一体化设计 相似文献
62.
由于雷达天线系统自身工作的特点, 他必须保证自身雷达波的正常接收和发射, 常用的隐身措施无法简单地在雷达天线隐身中获得应用. 采用频率选择表面 (FSS) 技术与天线罩技术相结合形成FSS天线罩, 可以使天线罩获得频率选择的功能. 即FSS天线罩对雷达的工作频段提供带通的传输特性, 同时改变雷达工作频段以外的雷达散射截面 (RCS) 特性, 可以实现带外隐身. 本文分析了FSS天线罩制备的基本思路, 综述了国内外FSS天线罩在结构设计、制造工艺等方面的研究状况, 并从多频FSS天线罩、智能FSS天线罩、厚屏FSS天线罩、 微型化FSS天线罩以及各技术的组合等方面对FSS天线罩的发展进行了展望.
关键词:
频率选择表面(FSS)
多频FSS天线罩
智能FSS天线罩
厚屏FSS天线罩 相似文献
63.
以互补频率选择表面 (CFSS)结构的强耦合作用为基础, 设计一种具有极化分离作用的频率选择表面 (PSS), 当容性表面与感性表面沿周期排布方向具有横向位移时, CFSS成为具有TM带通、TE带阻的极化分离结构. 建立等效电路模型分析PSS结构极化分离原理, 采用耦合积分方程法计算极化分离结构的传输特性以及容性表面和感性表面的电场分布. 理论分析与实验测试结果均表明: PSS具有良好的极化分离特性和角度稳定性, 为极化波产生器和极化分离结构的设计提供借鉴.
关键词:
频率选择表面
极化选择
互补屏频率选择表面 相似文献
64.
为了实现双通带频率选择表面(FSS)在较厚介质基底、 较大频带间隔和入射角度下的工程应用, 设计制备了一种性能优良的Ku/Ka波段双频FSS结构. 利用FSS栅瓣图分析了FSS具有稳定滤波特性的条件. 应用矢量模式匹配法计算了基于分形技术和复合图形技术的FSS的传输特性. 根据单元谐振模式和FSS传输特性归纳了厚介质基底、较远双通带FSS的设计原则, 最终优化出一种由方环复合“Y”环单元组成的FSS结构. 结果表明: 该结构在6.7 mm厚介质基底上0°-45°扫描范围内, 在Ku/Ka波段具有稳定的双频传输特性, 透过率均优于75%. 这为设计基底厚度较大、频带间隔较远、入射角度要求较高的双带FSS结构提供了理论参考与实验依据.
关键词:
频率选择表面
双通带
分形结构FSS
复合结构FSS 相似文献
65.
M.S. Zei 《Surface science》2006,600(9):1942-1951
The growth and structures of aluminum oxides on NiAl(1 0 0) have been investigated by RHEED (reflection high energy electron diffraction), complemented by LEED (low energy electron diffraction), AES (Auger electron spectroscopy) and STM (scanning tunneling microscopy). Crystalline θ-Al2O3 phase grows through gas-phase oxidation on the NiAl(1 0 0) substrate with its a and b-axes parallel to [0 −1 0] and [0 0 1] direction of the substrate, respectively, forming a (2 × 1) unit cell. Whilst, three-dimensional nano-sized NiAl(1 0 0) protrusions and Al2O3, NiAl(0 1 1) clusters were found to co-exit at the surface, evidenced by extraordinary transmission spots superposed to the substrate reflection rods in the RHEED patterns. Particularly, the NiAl(0 1 1) clusters develop with their (0 1 1) plane parallel to the NiAl(1 0 0) surface, and [1 0 0] axis parallel to the [0 −1 1] direction of the substrate surface. STM observation combined with information from AES and TPD (temperature programmed desorption) suggest the formation of these 3D structures is closely associated with partial decomposition of the crystalline oxides during annealing. On the other hand, smoother (2 × 1) oxide islands with thickness close to a complete monolayer of θ-Al2O3 can be formed on NiAl(1 0 0) by electro-oxidation, in contrast with the large crystalline films formed by gas-oxidation. 相似文献
66.
A modified potentiostatic method, termed the ‘pulse pontentiostatic method’ (PPSM) was used to get nano fibrillar poly(diphenylamine) (PDPA) film on Indium tin oxide (ITO) coated glass electrode and also for making modified electrode with platinum particles dispersed in PDPA. Platinum clusters were electrodispersed under constant potential on PDPA films to obtain catalytic electrodes for methanol oxidation. Energy dispersive analysis of X-rays (EDAX) results showed that the Pt microparticles are deposited into PDPA film. Scanning electron micrograph, SEM images show that the deposition results spherical catalytic particles. X-ray photoelectron spectroscopy (XPS) results inform that the net electronic charge on carbon atom and also the imine/amine ratio was not affected by Pt loadings. The modification of electrode surface by nano fibular PDPA improves the electrocatalytic activity for methanol oxidation. 相似文献
67.
唐亚楠 《原子与分子物理学报》2017,34(6)
采用基于密度泛函理论的第一性原理方法研究了单个CO 和O2气体分子在金属原子修饰石墨烯表面的吸附和反应过程. 结果表明: 空位缺陷结构的石墨烯能够提高金属原子的稳定性, 金属原子掺杂的石墨烯体系能够调控气体分子的吸附特性. 通入混合的CO和O2作为反应气体, 石墨烯表面容易被吸附性更强的O2分子占据, 进而防止催化剂的CO 中毒. 此外, 对比分析两种催化机理(Langmuir-Hinshelwood和Eley-Rideal)对CO氧化反应的影响. 与其它金属原子相比, Al原子掺杂的石墨烯体系具有极低的反应势垒(< 0.4 eV), 更有助于CO氧化反应的迅速进行. 相似文献
68.
High temperature oxidation of metals leads to residual stresses both in the metal and in the growing oxide. In this work, the evolution of this residual stresses is theoretically predicted in the growing oxide layers. The origin of these stresses is based on a microstructural model. Using experimental results providing from the oxidation kinetics, and an analysis proposed to describe the growth strain occurring in the thin layers, a set of equations is established allowing determining the stresses evolution with oxidation time. Then, the model is compared with experimental results obtained on both α-Fe and phosphated α-Fe, oxidised at different temperatures. Numerical data are extracted from experiments either with an asymptotic formulation or with an inverse method. These two methods give good agreement with experiments and allow extracting the model parameters. 相似文献
69.
Shufeng Zuo 《Applied Surface Science》2006,253(5):2508-2514
Al-pillared clays supported rare earths (RE/Al-PILC) are prepared and used as supports of palladium catalysts for deep oxidation of low concentrations of benzene (130-160 ppm). The supports and catalysts are characterized by X-ray powder diffraction (XRD), FT-IR, BET, transmission electron microscopy (TEM) and temperature-programmed reduction (H2-TPR). The results show that Al-pillaring results in a strong increase in the basal spacing (d0 0 1) from about 1.2 to 1.8 nm, and an increase in the BET surface area from 63.6 (±3.2) to 238.8 (±11.9) m2/g. Activity tests of deep oxidation of low concentration benzene show catalysts supported on Al-PILC and RE/Al-PILC are obviously more active than that on raw clay. Pd/6% Ce/Al-PILC, in particular, can catalyze the complete oxidation of low concentration benzene at a temperature as low as about 290 °C. 相似文献
70.
W. G. J. H. M. van Sark P. L. T. M. Frederix D. J. van den Heuvel A. A. Bol J. N. J. van Lingen C. de Mello Donegá H. C. Gerritsen A. Meijerink 《Journal of fluorescence》2002,12(1):69-76
Room-temperature time-resolved luminescence measurements on single CdSe/ZnS quantum dots (QDs) are presented. Fluorescence emission spectra were recorded over periods of up to 30 minutes with a time resolution as small as 6 ms. For QDs in ambient air, a clear 30–40 nm blue shift in the emission wavelength is observed, before the luminescence stops after about 2–3 minutes because of photobleaching. In a nitrogen atmosphere, the blue shift is absent while photobleaching occurs after much longer times (i.e., 10–15 minutes). These observations are explained by photoinduced oxidation. The CdSe surface is oxidized during illumination in the presence of oxygen. This effectively results in shrinkage of the CdSe core diameter by almost 1 nm and consequently in a blue shift. The faster fading of the luminescence in air suggests that photoinduced oxidation results in the formation of non-radiative recombination centers at the CdSe/CdSeOx interface. In a nitrogen atmosphere, photoinduced oxidation is prevented by the absence of oxygen. Additionally, a higher initial light output for CdSe/ZnS QDs in air is observed. This can be explained by a fast reduction of the lifetime of the long-lived defect states of CdSe QDs by oxygen. 相似文献