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   366篇
  免费   18篇
  国内免费   5篇
化学   30篇
晶体学   3篇
力学   2篇
数学   272篇
物理学   82篇
  2020年   1篇
  2019年   4篇
  2018年   4篇
  2017年   2篇
  2016年   4篇
  2015年   10篇
  2014年   17篇
  2013年   23篇
  2012年   4篇
  2011年   26篇
  2010年   16篇
  2009年   27篇
  2008年   33篇
  2007年   35篇
  2006年   25篇
  2005年   21篇
  2004年   15篇
  2003年   14篇
  2002年   9篇
  2001年   11篇
  2000年   10篇
  1999年   9篇
  1998年   6篇
  1997年   4篇
  1996年   9篇
  1995年   2篇
  1994年   8篇
  1993年   3篇
  1992年   2篇
  1991年   3篇
  1990年   2篇
  1989年   2篇
  1988年   2篇
  1987年   3篇
  1986年   4篇
  1985年   4篇
  1984年   2篇
  1983年   1篇
  1982年   5篇
  1980年   3篇
  1979年   2篇
  1978年   1篇
  1977年   1篇
排序方式: 共有389条查询结果,搜索用时 29 毫秒
1.
We study boundary value problems for the time-harmonic form of the Maxwell equations, as well as for other related systems of equations, on arbitrary Lipschitz domains in the three-dimensional Euclidean space. The main goal is to develop the corresponding theory for Lp-integrable bounday data for optimal values of p's. We also discuss a number of relevant applications in electromagnetic scattering.  相似文献   
2.
A magic labelling of a set system is a labelling of its points by distinct positive integers so that every set of the system has the same sum, the magic sum. Examples are magic squares (the sets are the rows, columns, and diagonals) and semimagic squares (the same, but without the diagonals). A magilatin labelling is like a magic labelling but the values need be distinct only within each set. We show that the number of n × n magic or magilatin labellings is a quasipolynomial function of the magic sum, and also of an upper bound on the entries in the square. Our results differ from previous ones because we require that the entries in the square all be different from each other, and because we derive our results not by ad hoc reasoning but from a general theory of counting lattice points in rational inside-out polytopes. We also generalize from set systems to rational linear forms. Dedicated to the memory of Claudia Zaslavsky, 1917–2006 Received August 10, 2005  相似文献   
3.
The minimum span of L(2,1)-labelings of certain generalized Petersen graphs   总被引:1,自引:0,他引:1  
In the classical channel assignment problem, transmitters that are sufficiently close together are assigned transmission frequencies that differ by prescribed amounts, with the goal of minimizing the span of frequencies required. This problem can be modeled through the use of an L(2,1)-labeling, which is a function f from the vertex set of a graph G to the non-negative integers such that |f(x)-f(y)|? 2 if xand y are adjacent vertices and |f(x)-f(y)|?1 if xand y are at distance two. The goal is to determine the λ-number of G, which is defined as the minimum span over all L(2,1)-labelings of G, or equivalently, the smallest number k such that G has an L(2,1)-labeling using integers from {0,1,…,k}. Recent work has focused on determining the λ-number of generalized Petersen graphs (GPGs) of order n. This paper provides exact values for the λ-numbers of GPGs of orders 5, 7, and 8, closing all remaining open cases for orders at most 8. It is also shown that there are no GPGs of order 4, 5, 8, or 11 with λ-number exactly equal to the known lower bound of 5, however, a construction is provided to obtain examples of GPGs with λ-number 5 for all other orders. This paper also provides an upper bound for the number of distinct isomorphism classes for GPGs of any given order. Finally, the exact values for the λ-number of n-stars, a subclass of the GPGs inspired by the classical Petersen graph, are also determined. These generalized stars have a useful representation on Möebius strips, which is fundamental in verifying our results.  相似文献   
4.
Angular distributions of elastic scattering and inelastic scattering from 2+1 state are measured for 16O+142,144,146Nd systems at several energies in the vicinity of the Coulomb barrier. The angular distributions are systematically analyzed in coupled channel framework. Renormalized double folded real optical and coupling potentials with DDM3Y interaction have been used in the calculation. Relevant nuclear densities needed to generate the potentials are derived from shell model wavefunctions. A truncated shell model calculation has been performed and the calculated energy levels are compared with the experimental ones. To simulate the absorption, a ‘hybrid’ approach is adopted. The contribution to the imaginary potential of couplings to the inelastic channels, other than the 2+1 target excitation channel, is calculated in the Feshbach formalism. This calculated imaginary potential along with a short ranged volume Woods–Saxon potential to simulate the absorption in fusion channel reproduces the angular distributions for 16O+146Nd quite well. But for 16O+142,144Nd systems additional surface absorption is found to be necessary to fit the angular distribution data. The variations of this additional absorption term with incident energy and the mass of the target are explored.  相似文献   
5.
Summary. We prove that - under certain conditions - measurable solutions $f$ of the functional equation $f(x)=h(x,y,f(g_{1}(x,y)),\ldots,f(g_{n}(x,y))),\quad(x,y)\in D \subset \mathbb{R}^{s} \times \mathbb{R}^{l}$ are continuous, even if $1\le l\le s$. As a tool we introduce new classes of functions which - roughly speaking - interpolate between continuous and Lebesgue measurable functions. Connection between these classes are also investigated.  相似文献   
6.
7.
The influence of thermal treatment on a (Li2OAl2O3 SiO2) glass ceramic is studied by laser spectroscopy. At temperatures above 800 °C a fluorescence of Cr3+ ions around 693 nm appears which indicates the growth of crystallites where the Cr3+ ions occupy sites similar to those in Al2O3.  相似文献   
8.
    
Under the influence of perpendicularly applied positive electro-static field less than 78u425611m0/xxlarge8776.gif" alt="ap" align="MIDDLE" BORDER="0">103V/cm to silk fibron textiles, at the high frequency side of the C2–O bending reflection band (78u425611m0/xxlarge8776.gif" alt="ap" align="MIDDLE" BORDER="0">45078u425611m0/xxlarge8764.gif" alt="sim" align="MIDDLE" BORDER="0">350 cm–1), effect of step creation and step annihilation of the C2–O pseudo dending bands was induced in three stages at 78u425611m0/xxlarge8776.gif" alt="ap" align="MIDDLE" BORDER="0">60078u425611m0/xxlarge8764.gif" alt="sim" align="MIDDLE" BORDER="0">450 cm–1 region IR spectroscopically relating to the stepnized statistical transfer of the unbonded 2P2, 78u425611m0/xxlarge960.gif" alt="pgr" align="BASELINE" BORDER="0"> electrons in carbon which present with density of 78u425611m0/xxlarge8776.gif" alt="ap" align="MIDDLE" BORDER="0">4.0×1014/cm2 in the surface mono-layer of silk fibroin from the states formed in (–C1–C2–N–)m spiral chains upto the pseudo-bending states formed in C2–O bondings. Fine 78u425611m0/xxlarge8776.gif" alt="ap" align="MIDDLE" BORDER="0">90 steps measured overlapping on these four types of C2–O reflection bands were analysed as to consist four step series and they were shown as,y = A·Jm + B cm–1 with A=20, B=521, m=0.55 and J=1, 2...18 for the B-series.And with A=39, B=283, m=0.63 and J=1, 2 ...17 for the C-series.y J = A·J + B cm–1 with A=11.42, B=201 and J=1, 2...13, for the D-series. And, stepnized C2–O bending bands including that of permanent oscillators and pseudo-bending oscillators induced by the effect of transfer of the unbonded 2P2 electrons in carbon atoms were shown as, EN=A·N2+B·N+C (eV) with A=–1.50×10–3, B=1.65×10–2 and C=2.4×10–2.  相似文献   
9.
The ibuprofen-78h05687401004r/xxlarge946.gif" alt="beta" align="MIDDLE" BORDER="0">-cyclodextrin inclusion complex was prepared by theco-precipitation method. The identity of the obtained product was verified by X-ray and thermogravimetric techniques. The effect of 78h05687401004r/xxlarge946.gif" alt="beta" align="MIDDLE" BORDER="0">-cyclodextrin on the stability of ibuprofen was analysed.  相似文献   
10.
Given a Markov chain (not necessarily stationary or homogeneous) with finite state space and an initial distribution, we can construct a measure 78330l1u/xxlarge956.gif" alt="mgr" align="MIDDLE" BORDER="0"> on the unit interval [0, 1]. In this work we examine the equality (up to a constant) of the Hausdorff dimension of 78330l1u/xxlarge956.gif" alt="mgr" align="MIDDLE" BORDER="0"> 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   
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