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   258篇
  免费   2篇
  国内免费   2篇
化学   162篇
力学   10篇
数学   47篇
物理学   43篇
  2022年   2篇
  2015年   3篇
  2014年   7篇
  2013年   15篇
  2012年   14篇
  2011年   10篇
  2010年   7篇
  2009年   9篇
  2008年   17篇
  2007年   14篇
  2006年   22篇
  2005年   11篇
  2004年   13篇
  2003年   8篇
  2002年   6篇
  2001年   9篇
  2000年   4篇
  1999年   4篇
  1998年   2篇
  1997年   4篇
  1996年   4篇
  1995年   2篇
  1994年   4篇
  1993年   4篇
  1989年   2篇
  1986年   2篇
  1981年   2篇
  1978年   5篇
  1972年   3篇
  1969年   2篇
  1966年   2篇
  1964年   1篇
  1963年   1篇
  1961年   1篇
  1959年   3篇
  1958年   2篇
  1948年   3篇
  1939年   1篇
  1938年   2篇
  1937年   3篇
  1933年   1篇
  1931年   3篇
  1930年   1篇
  1929年   2篇
  1926年   1篇
  1919年   2篇
  1918年   1篇
  1917年   1篇
  1909年   3篇
  1900年   1篇
排序方式: 共有262条查询结果,搜索用时 15 毫秒
81.
Abstract This paper uses a general equilibrium optimal growth model to discuss the role of optimal discounting of future benefits from cleanup at high‐level toxic waste sites. Cleanup simultaneously generates two streams of benefits. One of these is directly from utility and the other is indirectly from the added productivity of workers. We note that the optimal discount rate is different for these two types of benefits. Along the optimal path, the former are discounted at the rate of time preference and the latter at the market rate of interest. We achieve this by identifying four components of the shadow value of the stock of toxic waste. These are the utility, productivity, cost, and abundance effects. The distinction between discount rates appears to have been overlooked in the literature but has significant implications for environmental cost‐benefit analysis due to the growing interest in applying zero time preference to environmental problems, (like waste cleanup) whose consequences extend many generations into the future. A numerical example is included to illustrate these concepts.  相似文献   
82.
83.
84.
Higher surface energy of free nanoparticles   总被引:1,自引:0,他引:1  
We present an accurate online method for the study of size-dependent evaporation of free nanoparticles allowing us to detect a size change of 0.1 nm. This method is applied to Ag nanoparticles. The linear relation between the onset temperature of evaporation and the inverse of the particle size verifies the Kelvin effect and predicts a surface energy of 7.2 J/m(2) for free Ag nanoparticles. The surface energy of nanoparticles is significantly higher as compared to that of the bulk and is essential for processes such as melting, coalescence, evaporation, growth, etc., of nanoparticles.  相似文献   
85.
This study investigates cross-speaker differences in the factors that predict voicing thresholds during abduction-adduction gestures in six normal women. Measures of baseline airflow, pulse amplitude, subglottal pressure, and fundamental frequency were made at voicing offset and onset during intervocalic /h/, produced in varying vowel environments and at different loudness levels, and subjected to relational analyses to determine which factors were most strongly related to the timing of voicing cessation or initiation. The data indicate that (a) all speakers showed differences between voicing offsets and onsets, but the degree of this effect varied across speakers; (b) loudness and vowel environment have speaker-specific effects on the likelihood of devoicing during /h/; and (c) baseline flow measures significantly predicted times of voicing offset and onset in all participants, but other variables contributing to voice timing differed across speakers. Overall, the results suggest that individual speakers have unique methods of achieving phonatory goals during running speech. These data contribute to the literature on individual differences in laryngeal function, and serve as a means of evaluating how well laryngeal models can reproduce the range of voicing behavior used by speakers during running speech tasks.  相似文献   
86.
The rank 4 locus of a general skew-symmetric 7 × 7 matrix gives the Pfaffian variety in P 20 which is not defined as a complete intersection. Intersecting this with a general P 6 gives a Calabi–Yau manifold. An orbifold construction seems to give the 1-parameter mirror-family of this. However, corresponding to two points in the 1-parameter family of complex structures, both with maximally unipotent monodromy, are two different mirror-maps: one corresponding to the general Pfaffian section, the other to a general intersection of G(2,7) P 20 with a P 13. Apparently, the Pfaffian and G(2,7) sections constitute different parts of the A-model (Kähler structure related) moduli space, and, thus, represent different parts of the same conformal field theory moduli space.  相似文献   
87.
88.
89.
90.
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