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   216091篇
  免费   1568篇
  国内免费   628篇
化学   118260篇
晶体学   3272篇
力学   8408篇
综合类   6篇
数学   23375篇
物理学   64966篇
  2020年   1974篇
  2019年   2265篇
  2018年   3206篇
  2017年   3114篇
  2016年   4273篇
  2015年   2376篇
  2014年   3825篇
  2013年   9281篇
  2012年   6911篇
  2011年   8452篇
  2010年   6080篇
  2009年   5931篇
  2008年   8157篇
  2007年   8223篇
  2006年   7662篇
  2005年   6963篇
  2004年   6182篇
  2003年   5657篇
  2002年   5516篇
  2001年   5956篇
  2000年   4701篇
  1999年   3476篇
  1998年   3013篇
  1997年   3046篇
  1996年   2838篇
  1995年   2334篇
  1994年   2438篇
  1993年   2479篇
  1992年   2620篇
  1991年   2675篇
  1990年   2575篇
  1989年   2540篇
  1988年   2474篇
  1987年   2448篇
  1986年   2364篇
  1985年   3047篇
  1984年   3205篇
  1983年   2563篇
  1982年   2836篇
  1981年   2710篇
  1980年   2515篇
  1979年   2727篇
  1978年   2847篇
  1977年   2864篇
  1976年   2844篇
  1975年   2694篇
  1974年   2678篇
  1973年   2817篇
  1972年   1876篇
  1967年   1833篇
排序方式: 共有10000条查询结果,搜索用时 8 毫秒
991.
992.
Capabilities of the imaging techniques, in which X-rays are converted to electrons and then the emitted electrons are registered by means of an electron microscope, are analyzed, the focus being on the factors limiting lateral resolution at the stage of electron emission. Bearing in mind the tendency to use harder synchrotron X-rays for some combined X-ray-electron microscopy methods, calculations were made for two significantly different X-ray energies: E = 1.828 keV (K-edge of Si) and E = 11.923 keV (L3-edge of Au). By using Monte Carlo simulations of the electron trajectories beneath the surface of the sample we show that the radius of the spot from which photoelectrons are emitted could be as small as 1 nm. However, when proper account is taken of an entire electron cascade associated with the re-building of electron shells after photoelectron emission, spots more than one order of magnitude larger result, limiting the best lateral resolution to 20–30 nm.  相似文献   
993.
In this paper we approximate the solution of a linear initial-value problem, making use of a Schauder basis for certain Banach space associated with such a differential problem. In addition, we apply that results in order to calculate numerically the response from a structure modelled by a three degree-of-freedom mass–damper–spring system.  相似文献   
994.
The synthesis of 2-hydroxymethyl-2-propylmorphine ( 5 ) and 2-hydroxymethyl-2-propylnormorphine ( 7 ), the major rat urinary metabolites of 3-O-t-butylmorphine ( 3 ) are described.  相似文献   
995.
996.
997.
998.
The connection is considered of multiplicity distributions in three stages: partonic, hadronization, and hadronic. An interpretation of the LoPHD parameter is found. It is shown that under specific hypotheses on the form of the mass spectrum, the statistical bootstrap model leads to the negative binomial distribution (NBD) at the hadronic stage of development of the multiple production process with specific analytic dependences of the parameters of the NBD.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 5, pp. 28–32, May, 1991.One of the authors (V. I. Kuvshinov) is thankful to R. Hagedorn and G. Burgers for numerous discussions.  相似文献   
999.
1000.
Coupled and decoupled Taylor-Galerkin algorithms are considered for viscoelastic flow and a model problem—transient startup Poiseuille flow in a channel under a fixed pressure gradient. All algorithms reproduce the steady-state solutions and are stable at high elasticity numbers (E). For a fixed mesh, the coupled and decoupled versions (TGC and TGD) give exceptional time-accuracy at low elasticity numbers [to within O(1%) at E = 1] and reasonable accuracy at high elasticity numbers [to within O(10%) at E = 10, 100]. By definition, the decoupled false-transient scheme (TGF), which uses different time scales for velocity and stress time stepping, provides a poor transient history. Where the main requirement is to compute a steady-state algorithm efficiency is crucial. The TGF scheme attains a steady state between six to eight times faster than does the TGC scheme, and the latter is over twice as fast as the TGD form. © 1994 John Wiley & Sons, Inc.  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