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   2784篇
  免费   93篇
  国内免费   22篇
化学   1592篇
晶体学   27篇
力学   153篇
数学   368篇
物理学   759篇
  2023年   8篇
  2022年   35篇
  2021年   56篇
  2020年   45篇
  2019年   49篇
  2018年   22篇
  2017年   26篇
  2016年   59篇
  2015年   71篇
  2014年   96篇
  2013年   146篇
  2012年   183篇
  2011年   208篇
  2010年   135篇
  2009年   119篇
  2008年   206篇
  2007年   140篇
  2006年   159篇
  2005年   137篇
  2004年   111篇
  2003年   88篇
  2002年   94篇
  2001年   68篇
  2000年   66篇
  1999年   40篇
  1998年   37篇
  1997年   23篇
  1996年   43篇
  1995年   37篇
  1994年   35篇
  1993年   40篇
  1992年   30篇
  1991年   36篇
  1990年   22篇
  1989年   20篇
  1988年   24篇
  1987年   16篇
  1986年   15篇
  1985年   19篇
  1984年   19篇
  1983年   21篇
  1982年   16篇
  1981年   10篇
  1980年   5篇
  1979年   10篇
  1978年   11篇
  1977年   11篇
  1976年   7篇
  1974年   4篇
  1972年   4篇
排序方式: 共有2899条查询结果,搜索用时 234 毫秒
21.
Given a series-parallel network (network, for short)N, its dual networkN′ is given by interchanging the series connection and the parallel connection of networkN. We usually use a series-parallel graph to represent a network. LetG[N] andG[N′] be graph representations ofNandN′, respectively. A sequence of edgese1, e2,…,ekis said to form a common trail on (G[N], G[N′]) if it is a trail on bothG[N] andG[N′]. If a common trail covers all of the edges inG[N] andG[N′], it is called adouble Euler trail.However, there are many different graph representations for a network. We say that a networkNhas a double Euler trail (DET) if there is a common Euler trail for someG[N] and someG[N′]. Finding a DET in a network is essential for optimizing the layout area of a complementary CMOS functional cell. Maziasz and Hayes (IEEE Trans. Computer-Aided Design9(1990), 708–719) gave a linear time algorithm for solving the layout problem in fixedG[N] andG[N′] and an exponential algorithm for finding the optimal cover in a network without fixing graph representations. In this paper, we study properties of subnetworks of a DET network. According to these properties, we propose an algorithm that automatically generates the rules for composition of trail cover classes. On the basis of these rules, a linear time algorithm for recognizing DET networks is presented. Furthermore, we also give a necessary and sufficient condition for the existence of a double Euler circuit in a network.  相似文献   
22.
A succinct series expression is derived for describing the limit distribution of the number of times r consecutive elements are all records (in a sequence of independent and identically distributed random variables with a common continuous distribution) for all r ≥ 2. Previously, only the limit distributions for r = 1, 2, and 3 were known. © 2005 Wiley Periodicals, Inc. Random Struct. Alg., 2005  相似文献   
23.
In the Wick-Cutkosky model we analyze nonperturbatively, in light-front dynamics, the contributions of two-body and higher Fock sectors to the total norm and electromagnetic form factor. It turns out that two- and three-body sectors always dominate. For a maximal value of the coupling constant α = 2π, corresponding to the zero bound-state mass M = 0, they contribute 90% to the norm. With decrease of α the two-body contribution increases up to 100%. The form factor asymptotic is always determined by a two-body sector.  相似文献   
24.
Ternary fission of 252Cf was studied at Gammasphere using eight ΔE×E particle telescopes. Helium, beryllium, boron, and carbon light charged particles (LCPs) emitted with kinetic energy more than 9, 21, 26, and 32 MeV, respectively, were identified. The 3368-keV γ transition from the first 2+ excited state in 10Be was found and the population probability ratio N(2+)/N(0+) = 0.160 ± 0.025 was estimated. No evidence was found for 3368-keV γ rays emitted from a triple molecular state. For the first time, charge distributions are obtained for ternary fission fragments emitted with helium, beryllium, and carbon LCPs.  相似文献   
25.
26.
We study the large-time behavior and rate of convergence to the invariant measures of the processes dX (t)=b(X) (t)) dt + (X (t)) dB(t). A crucial constant appears naturally in our study. Heuristically, when the time is of the order exp( – )/2 , the transition density has a good lower bound and when the process has run for about exp( – )/2, it is very close to the invariant measure. LetL =(2/2) – U · be a second-order differential operator on d. Under suitable conditions,L z has the discrete spectrum
- \lambda _2^\varepsilon ...and lim \varepsilon ^2 log \lambda _2^\varepsilon = - \Lambda \hfill \\ \varepsilon \to 0 \hfill \\ \end{gathered} $$ " align="middle" vspace="20%" border="0">  相似文献   
27.
28.
29.
30.
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