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   65805篇
  免费   12556篇
  国内免费   5040篇
化学   60231篇
晶体学   697篇
力学   2223篇
综合类   353篇
数学   5729篇
物理学   14168篇
  2024年   73篇
  2023年   542篇
  2022年   1027篇
  2021年   1198篇
  2020年   2288篇
  2019年   3515篇
  2018年   1896篇
  2017年   1566篇
  2016年   4487篇
  2015年   4715篇
  2014年   4901篇
  2013年   6003篇
  2012年   5426篇
  2011年   4868篇
  2010年   4643篇
  2009年   4664篇
  2008年   4348篇
  2007年   3562篇
  2006年   3150篇
  2005年   3026篇
  2004年   2640篇
  2003年   2273篇
  2002年   2925篇
  2001年   2155篇
  2000年   1910篇
  1999年   944篇
  1998年   512篇
  1997年   491篇
  1996年   462篇
  1995年   372篇
  1994年   376篇
  1993年   283篇
  1992年   229篇
  1991年   224篇
  1990年   215篇
  1989年   157篇
  1988年   165篇
  1987年   126篇
  1986年   114篇
  1985年   127篇
  1984年   98篇
  1983年   94篇
  1982年   76篇
  1981年   63篇
  1980年   63篇
  1979年   40篇
  1976年   43篇
  1975年   43篇
  1974年   51篇
  1973年   48篇
排序方式: 共有10000条查询结果,搜索用时 15 毫秒
981.
以MEH-PPV(聚[2-甲氧基-5-(2′-乙基己氧基-对苯乙烯)])和Alq3作为发光层, 成功制备出ITO/SiO2/MEH-PPV/SiO2/Al结构和ITO/SiO2/Alq3 /SiO2/Al结构的固态阴极射线器件。通过分析SSCL光谱,认为这些高速电子激发有机材料后形成Frenkel激子。当器件两个电极之间加的电压比较低时,有机薄膜层的场强也比较低,这些激子被解离的概率很小,从而产生的是激子发光的长波发射;当器件两个电极之间加的电压比较高时,有机薄膜层的场强很高, 在有机层形成的激子大部分被解离, 解离后的电子直接跃迁至LUMO(lowest unoccupancied molecular orbit),这些电子弛豫后从LUMO能级到HOMO(highest occupancied molecular orbit )能级直接辐射跃迁, 接着重新复合发光,从而产生短波发射。制作的固态阴极射线器件可以实现全色发光, 提高发光效率和加强蓝光发射。作者可以预期所研制出的这种SSCL器件必将引发平板显示领域一场新的革命性变革。  相似文献   
982.
使用Maxell方程的严格解,研究了亚微米直径光纤的单模条件、传播常数、基模分布、传播效率、非线性系数等光学特性,发现亚微米纤芯直径光纤的单模条件与标准光纤相同,非线性系数在直径为700nm左右时最大;当光纤的直径小于1μm时,传播效率骤减.这些结果有助于新型微光通信和光纤传感器件的设计.  相似文献   
983.
根据干涉成像光谱仪光谱分辨率对角向差的要求,通过对实体Sagnac干涉仪结构和光路进行分析,从三个相互垂直的方向出发,研究了光谱分辨率和棱镜角公差之间存在的关系;并推导了满足光谱仪光谱分辨率要求的实体Sagnac干涉棱镜的角公差公式;用实例说明了关系式的应用方法,如果不考虑棱镜变形引起的色散及棱镜的面型误差和付氏镜的残余像差的影响,而只考虑棱镜的角误差对光谱分辨率的影响,则通常情况下干涉棱镜的角公差要求较严,约20″以内.  相似文献   
984.
负折射指数物质中金属线对电磁波的影响   总被引:3,自引:0,他引:3       下载免费PDF全文
冯宇  吴健  宋建平 《物理学报》2006,55(6):2794-2798
构造两种结构负折射指数物质(NRM),利用数值模拟计算两种结构的S参数.由于这种结构尺度比波长小,为精确利用有限积分技术(FIT)进行模拟.通过对这两种结构中金属线位置变化对金属谐振频率影响进行模拟,最后得出由于金属线与谐振环耦合,金属线对称破缺影响谐振环谐振频率和通带,并对等效负折射指数为负的频带产生影响. 关键词: 负折射率 左手物质 通带 金属线对称破缺  相似文献   
985.
Poly(lactic acid) (PLA) is a biodegradable polymer that has a variety of applications, one of which is as biomaterial in surgery or as functional layers on implants, due to its compatibility with living tissue. This paper reports the possibilities of quantification of poly(lactic acid) (PLA) in a polymer matrix such as poly(methyl methacrylate) (PMMA) by micro Raman spectroscopy (MRS). Blends of amorphous poly(DL‐lactic acid) with poly(methyl methacrylate) were prepared by the procedure of dissolution/precipitation. Thermal properties of the blends such as the glass transition temperature (Tg) were characterized by differential scanning calorimetry (DSC). The PLA/PMMA blends exhibited only a single glass transition region, indicating that this system is miscible. The PLA/PMMA system obeys the Gordon–Taylor equation (Tg versus PLA content). Various concentration ratios of PLA blends were prepared to use as a basis for quantitative analysis by MRS. Intensities of the characteristic bands at 813 cm−1 (νCOC of PMMA) and 873 cm−1 (νC―COO of PLA) were used for the calculation. The calibration graph showed a good linear correlation with an R2 value of 0.9985. On the basis of the calibration curve obtained, the determined content of several PLA/PMMA blends was in good agreement when compared with nominal contents. The limit of detection (LOD) and quantification (LOQ) were calculated by the calibration data set as signal‐to‐noise method. The relative standard deviation of this method was lower than 10% and the accuracy better than 4%. This study demonstrated that Raman spectroscopy provides an alternative non destructive method for quantitative analysis of PLA in a PMMA matrix. Copyright © 2015 John Wiley & Sons, Ltd.  相似文献   
986.
We report on an accurate intensity calibration method for low wavenumber Raman spectroscopy. It uses the rotational Raman spectrum of N2. The intensity distributions in the rotational Raman spectra of diatomic molecules are theoretically well established. They can be used as primary intensity standards for intensity calibration. The intensity ratios of the Stokes and anti‐Stokes transitions originating from the same rotational levels are not affected by thermal population. Taking the effect of rotation–vibration interactions appropriately into account, we are able to calculate these intensity ratios theoretically. The comparison between the observed and calculated ratios of the N2 pure rotational spectrum provides an accurate relative sensitivity curve (error ~5 × 10−4) in the wavenumber region of −150 to 150 cm−1. We determine the temperature of water solely from the low wavenumber Raman spectra, using a thus calibrated spectrometer. The Raman temperature shows an excellent agreement with the thermocouple temperature, with only 0.5 K difference. The present calibration technique will be highly useful in many applications of low wavenumber quantitative Raman spectroscopy. Copyright © 2015 John Wiley & Sons, Ltd.  相似文献   
987.
The sensitivity of far‐field Raman micro‐spectroscopy was investigated to determine quantitatively the actual thickness of organic thin films. It is shown that the thickness of organic films can be quantitatively determined down to 3 nm with an error margin of 20% and down to 1.5 nm with an error margin of 100%. Raman imaging of thin‐film surfaces with a far‐field optical microscope establishes the distribution of a polymer with a lateral resolution of ~400 nm and the homogeneity of the film. Raman images are presented for spin‐coated thin films of polysulfone (PSU) with average thicknesses between 3 and 50 nm. In films with an average thickness of 43 nm, the variation in thickness was around 5% for PSU. In films with an average thickness of 3 nm for PSU, the detected thickness variation was 100%. Raman imaging was performed in minutes for a surface area of 900 µm2. The results illustrate the ability of far‐field Raman microscopy as a sensitive method to quantitatively determine the thickness of thin films down to the nanometer range. Copyright © 2015 John Wiley & Sons, Ltd.  相似文献   
988.
This paper investigates the singular optics of nonparaxial light beams in the near field when the light behaves as a tractor beam. New insights into the optical pulling force, which is usually represented by integrating the stress tensor at a black box enclosing the object, are interpreted by the optical singularity of the Poynting vector. The negative nonconservative pulling force originates from the transfer of the azimuthal Poynting vector to the longitudinal component partly owing to the presence of a scatterer. The separatrice pattern and singularity shifts of the Poynting vector unanimously exhibit a differentiable near‐field distribution in the presence of optical pulling force. A new method is established to calculate the near‐field optical force using the differential Poynting vector in the far field. The results obtained provide a clear physical interpretation of the light–matter interaction and manifest the significance of singular optics in manipulating objects.

  相似文献   

989.
杨建义  冯浩 《光子学报》1994,23(4):335-343
Y分支器是集成光学中一种重要的器件单元。本文使用有限差分光束传输法(FD-BPM)系统地分析了Y分支器的工作机理,包括对称与非对称两种结构,其中着重对非对称Y分支器单元进行了分析,指出其欲完成模式分离所需满足的条件。通过对Y分支器的深入研究,我们也说明了FD-BPM法在对Y分支器及类似器件和单元的模拟分析中所具有的方便性和优越性,这为实际的设计制作工作提供了极好的基础。  相似文献   
990.
The results of a study of two types of natural-diamond crystals by dynamic nuclear polarization (DNP)-enhanced high-resolution solid-state 13C nuclear magnetic resonance (NMR) are reported. The home-built DNP magic-angle spinning (MAS) 13C NMR spectrometer operates at 54 GHz for electrons and 20.2 MHz for carbons. The power of the microwave source was about 30 W and the highest DNP enhancement factor came near to 103. It was shown that in the MAS spectra the 13C NMR linewidths of the Ib-type diamond were broader than those of IaB3-type diamond. From the hyperfine structure of the DNP enhancement as a function of frequency, four kinds of nitrogen-centred and one kind of carbon-centred free radicals could be identified in the Ib-type diamond. The hyperfine structures of the DNP enhancement curve that originated from the anisotropic hyperfine interaction between electron and nuclei could be partially averaged out by MAS. The 13C polarization time of DNP was rather long, i.e. 1500 s, and the spin—lattice relaxation time (without microwave irradiation) was about 300 s, which was somewhat shorter than anticipated. Discussions on these experimental results have been made in this report.  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