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   7523篇
  免费   193篇
  国内免费   282篇
化学   843篇
晶体学   29篇
力学   32篇
综合类   9篇
数学   6155篇
物理学   557篇
综合类   373篇
  2023年   11篇
  2022年   21篇
  2021年   14篇
  2020年   21篇
  2019年   212篇
  2018年   236篇
  2017年   99篇
  2016年   56篇
  2015年   79篇
  2014年   255篇
  2013年   596篇
  2012年   282篇
  2011年   499篇
  2010年   405篇
  2009年   493篇
  2008年   526篇
  2007年   471篇
  2006年   403篇
  2005年   273篇
  2004年   219篇
  2003年   215篇
  2002年   164篇
  2001年   180篇
  2000年   179篇
  1999年   212篇
  1998年   198篇
  1997年   164篇
  1996年   220篇
  1995年   205篇
  1994年   201篇
  1993年   175篇
  1992年   102篇
  1991年   34篇
  1990年   21篇
  1989年   20篇
  1988年   21篇
  1987年   24篇
  1986年   17篇
  1985年   51篇
  1984年   63篇
  1983年   47篇
  1982年   51篇
  1981年   54篇
  1980年   38篇
  1979年   37篇
  1978年   38篇
  1977年   29篇
  1976年   20篇
  1975年   17篇
  1973年   12篇
排序方式: 共有7998条查询结果,搜索用时 22 毫秒
101.
A set-valued dynamical systemF on a Borel spaceX induces a set-valued operatorF onM(X) — the set of probability measures onX. We define arepresentation ofF, each of which induces an explicitly defined selection ofF; and use this to extend the notions of invariant measure and Frobenius-Perron operators to set-valued maps. We also extend a method ofS. Ulam to Markov finite approximations of invariant measures to the set-valued case and show how this leads to the approximation ofT-invariant measures for transformations , whereT corresponds to the closure of the graph of .  相似文献   
102.
This paper is concerned with BV periodic solutions for multivalued perturbations of an evolution equation governed by the sweeping process (or Moreau's process). The perturbed equation has the form –DuN C (t)(u(t))+F(t,u(t)), whereC is a closed convex valued continuousT-periodic multifunction from [0,T] to d ,N C (t)(u(t)) is the normal cone ofC(t) atu(t),F: [0,T d d is a compact convex valued multifunction and Du is the differential measure of the periodic BV solutionu. Several existence results for this differential inclusion are stated under various assumptions on the perturbationF.  相似文献   
103.
Given a Markov chain (not necessarily stationary or homogeneous) with finite state space and an initial distribution, we can construct a measure on the unit interval [0, 1]. In this work we examine the equality (up to a constant) of the Hausdorff dimension of and of a suitably defined entropy for the Markovian process. The results are applied to the so-called Rademacher-Riesz Products.  相似文献   
104.
We coasider a partially observable diffusion process (x t,yt)t60080x2715/xxlarge10878.gif" alt="ges" align="MIDDLE" BORDER="0">0 whose unobservable componentx t lives on a submanifold M ofR n . We present some general conditions under which the conditional law ofx t, given the observationsy s ,s 60080x2715/xxlarge8712.gif" alt="isin" align="MIDDLE" BORDER="0"> [0,t], admits a density w.r.t. a given measure on M. We characterize the analytical properties of this density by using appropriate Sobolev spaces.Research supported by the Hungarian National Foundation of Scientific Research No. 2290.  相似文献   
105.
The papers of R. Ramer and S. Kusuoka investigate conditions under which the probability measure induced by a nonlinear transformation on abstract Wiener space(,H,B) is absolutely continuous with respect to the abstract Wiener measure. These conditions reveal the importance of the underlying Hilbert spaceH but involve the spaceB in an essential way. The present paper gives conditions solely based onH and takes as its starting point, a nonlinear transformationT=I+F onH. New sufficient conditions for absolute continuity are given which do not seem easily comparable with those of Kusuoka or Ramer but are more general than those of Buckdahn and Enchev. The Ramer-Itô integral occurring in the expression for the Radon-Nikodym derivative is studied in some detail and, in the general context of white noise theory it is shown to be an anticipative stochastic integral which, under a stronger condition on the weak Gateaux derivative of F is directly related to the Ogawa integral.Research supported by the National Science Foundation and the Air Force Office of Scientific Research Grant No. F49620 92 J 0154 and the Army Research Office Grant No. DAAL 03 92 G 0008.  相似文献   
106.
Summary For a realization of lengthn from a covariance stationary discrete time process with spectral density which behaves like 1–2H as 0+ for 1/2<H<1 (apart from a slowly varying factor which may be of unknown form), we consider a discrete average of the periodogram across the frequencies 260.gif" alt="pgr" align="BASELINE" BORDER="0">j/n,j=1,..., m, wherem andm/n0 asn. We study the rate of convergence of an analogue of the mean squared error of smooth spectral density estimates, and deduce an optimal choice ofm.  相似文献   
107.
Summary The result linking shift-coupling to time-average total variation convergence and to the invariant -field is extended to continuous time and an analogous result established linking -couplings to smooth total variation convergence and to a smooth tail -field. Shift- and -coupling inequalities are presented.  相似文献   
108.
Summary We consider the one dimensional nearest neighbors asymmetric simple exclusion process with ratesq andp for left and right jumps respectively;q<p. Ferrari et al. (1991) have shown that if the initial measure isv 6081/xxlarge961.gif" alt="rgr" align="MIDDLE" BORDER="0">,6081/xxlarge955.gif" alt="lambda" align="BASELINE" BORDER="0"> , a product measure with densities 6081/xxlarge961.gif" alt="rgr" align="MIDDLE" BORDER="0"> and 6081/xxlarge955.gif" alt="lambda" align="BASELINE" BORDER="0"> to the left and right of the origin respectively, 6081/xxlarge961.gif" alt="rgr" align="MIDDLE" BORDER="0"><6081/xxlarge955.gif" alt="lambda" align="BASELINE" BORDER="0">, then there exists a (microscopic) shock for the system. A shock is a random positionX t such that the system as seen from this position at timet has asymptotic product distributions with densities 6081/xxlarge961.gif" alt="rgr" align="MIDDLE" BORDER="0"> and 6081/xxlarge955.gif" alt="lambda" align="BASELINE" BORDER="0"> to the left and right of the origin respectively, uniformly int. We compute the diffusion coefficient of the shockD=lim t6081/xxlarge8594.gif" alt="rarr" align="BASELINE" BORDER="0">6081/xxlarge8734.gif" alt="infin" align="MIDDLE" BORDER="0"> t –1(E(X t )2–(EX t )2) and findD=(p–q)(6081/xxlarge955.gif" alt="lambda" align="BASELINE" BORDER="0">–6081/xxlarge961.gif" alt="rgr" align="MIDDLE" BORDER="0">)–1(6081/xxlarge961.gif" alt="rgr" align="MIDDLE" BORDER="0">(1–6081/xxlarge961.gif" alt="rgr" align="MIDDLE" BORDER="0">)+6081/xxlarge955.gif" alt="lambda" align="BASELINE" BORDER="0">(1–6081/xxlarge955.gif" alt="lambda" align="BASELINE" BORDER="0">)) as conjectured by Spohn (1991). We show that in the scale 6081/440_2005_Article_BF01199027_TeX2GIFIE1.gif" alt=" $$\sqrt t$$ " align="middle" border="0"> the position ofX t is determined by the initial distribution of particles in a region of length proportional tot. We prove that the distribution of the process at the average position of the shock converges to a fair mixture of the product measures with densities 6081/xxlarge961.gif" alt="rgr" align="MIDDLE" BORDER="0"> and 6081/xxlarge955.gif" alt="lambda" align="BASELINE" BORDER="0">. This is the so called dynamical phase transition. Under shock initial conditions we show how the density fluctuation fields depend on the initial configuration.  相似文献   
109.
Summary We consider a point process with the Polish phase space (X,X) and a system of -fields (x),xX, generated by on certain sets (x)X. We define predictability for random processes indexed byX and for random measures onX and prove the existence and uniqueness of predictable and dual predictable projections under a regularity condition on . ForX= 2 + and under monotonicity assumptions on the sets x we will identify the predictable projections of some simple processes as regular versions of certain martingales.  相似文献   
110.
Summary Consider a one-dimensional walk (S k ) k having steps of bounded size, and weight the probability of the path with some factor 1–(0,1) for every single self-intersection up to timen. We prove thatS n /S S converges towards some deterministic number called the effective drift of the self-repellent walk. Furthermore, this drift is shown to tend to the basic drift as tends to 0 and, as tends to 1, to the self-avoiding walk's drift which is introduced in [10]. The main tool of the present paper is a representation of the sequence of the local times as a functional of a certain Markov process.Partially supported by Swiss National Sciences Foundation Grant 20-36305.92  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