全文获取类型
收费全文 | 69418篇 |
免费 | 3809篇 |
国内免费 | 4883篇 |
专业分类
测绘学 | 3223篇 |
大气科学 | 6425篇 |
地球物理 | 13301篇 |
地质学 | 31214篇 |
海洋学 | 6077篇 |
天文学 | 11461篇 |
综合类 | 1794篇 |
自然地理 | 4615篇 |
出版年
2023年 | 393篇 |
2022年 | 1001篇 |
2021年 | 1206篇 |
2020年 | 1070篇 |
2019年 | 1211篇 |
2018年 | 4694篇 |
2017年 | 4282篇 |
2016年 | 3328篇 |
2015年 | 1730篇 |
2014年 | 1936篇 |
2013年 | 2727篇 |
2012年 | 3281篇 |
2011年 | 5291篇 |
2010年 | 4881篇 |
2009年 | 5213篇 |
2008年 | 4265篇 |
2007年 | 4832篇 |
2006年 | 2043篇 |
2005年 | 2182篇 |
2004年 | 1880篇 |
2003年 | 1856篇 |
2002年 | 1581篇 |
2001年 | 1272篇 |
2000年 | 1173篇 |
1999年 | 1054篇 |
1998年 | 940篇 |
1997年 | 919篇 |
1996年 | 764篇 |
1995年 | 678篇 |
1994年 | 650篇 |
1993年 | 529篇 |
1992年 | 473篇 |
1991年 | 424篇 |
1990年 | 428篇 |
1989年 | 396篇 |
1988年 | 332篇 |
1987年 | 433篇 |
1986年 | 331篇 |
1985年 | 428篇 |
1984年 | 448篇 |
1983年 | 447篇 |
1982年 | 411篇 |
1981年 | 395篇 |
1980年 | 388篇 |
1979年 | 342篇 |
1978年 | 339篇 |
1977年 | 304篇 |
1976年 | 312篇 |
1975年 | 303篇 |
1973年 | 278篇 |
排序方式: 共有10000条查询结果,搜索用时 125 毫秒
81.
We consider the effects of projection, internal absorption, and gas-or stellar-velocity dispersion on the measured rotation curves of galaxies with edge-on disks. Axisymmetric disk models clearly show that the rotational velocity in the inner galaxy is highly underestimated. As a result, an extended portion that imitates nearly rigid rotation appears. At galactocentric distances where the absorption is low (i.e., it does not exceed 0.3–0.5m kpc?1), the line profiles can have two peaks, and a rotation curve with minimum distortions can be obtained by estimating the position of the peak that corresponds to a higher rotational velocity. However, the high-velocity peak disappears in high-absorption regions and the actual shape of the rotation curve cannot be reproduced from line-of-sight velocity estimates. In general, the optical rotation curves for edge-on galaxies are of little use in reconstructing the mass distribution in the inner regions, particularly for galaxies with a steep velocity gradient in the central region. In this case, estimating the rotation velocities for outer (transparent) disk regions yields correct results. 相似文献
82.
Of the impact craters on Earth larger than 20 km in diameter, 10-15% (3 out of 28) are doublets, having been formed by the simultaneous impact of two well-separated projectiles. The most likely scenario for their formation is the impact of well-separated binary asteroids. If a population of binary asteroids is capable of striking the Earth, it should also be able to hit the other terrestrial planets as well. Venus is a promising planet to search for doublet craters because its surface is young, erosion is nearly nonexistent, and its crater population is significantly larger than the Earth's. After a detailed investigation of single craters separated by less than 150 km and “multiple” craters having diameters greater than 10 km, we found that the proportion of doublet craters on Venus is at most 2.2%, significantly smaller than Earth's, although several nearly incontrovertible doublets were recognized. We believe this apparent deficit relative to the Earth's doublet population is a consequence of atmospheric screening of small projectiles on Venus rather than a real difference in the population of impacting bodies. We also examined “splotches,” circular radar reflectance features in the Magellan data. Projectiles that are too small to form craters probably formed these features. After a careful study of these patterns, we believe that the proportion of doublet splotches on Venus (14%) is comparable to the proportion of doublet craters found on Earth (10-15%). Thus, given the uncertainties of interpretation and the statistics of small numbers, it appears that the doublet crater population on Venus is consistent with that of the Earth. 相似文献
83.
84.
Piero F. Spinnato Michael Fellhauer Simon F. Portegies Zwart 《Monthly notices of the Royal Astronomical Society》2003,344(1):22-32
We study the efficiency at which a black hole or dense star cluster spirals in to the Galactic Centre. This process takes place on a dynamical friction time-scale, which depends on the value of the Coulomb logarithm (ln Λ). We determine the accurate value of this parameter using the direct N -body method, a tree algorithm and a particle-mesh technique with up to two million plus one particles. The three different techniques are in excellent agreement. Our measurement for the Coulomb logarithm appears to be independent of the number of particles. We conclude that ln Λ= 6.6 ± 0.6 for a massive point particle in the inner few parsec of the Galactic bulge. For an extended object, such as a dense star cluster, ln Λ is smaller, with a value of the logarithm argument Λ inversely proportional to the object size. 相似文献
85.
86.
The ordinary kriging method, a geostatistical interpolation technique, was applied for developing contour maps of design storm depth in northern Taiwan using intensity–duration–frequency (IDF) data. Results of variogram modelling on design storm depths indicate that the design storms can be categorized into two distinct storm types: (i) storms of short duration and high spatial variation and (ii) storms of long duration and less spatial variation. For storms of the first category, the influence range of rainfall depth decreases when the recurrence interval increases, owing to the increasing degree of their spatial independence. However, for storms of the second category, the influence range of rainfall depth does not change significantly and has an average of approximately 72 km. For very extreme events, such as events of short duration and long recurrence interval, we do not recommend usage of the established design storm contours, because most of the interstation distances exceed the influence ranges. Our study concludes that the influence range of the design storm depth is dependent on the design duration and recurrence interval and is a key factor in developing design storm contours. Copyright © 2003 John Wiley & Sons, Ltd. 相似文献
87.
88.
89.
Non-Newtonian topographic relaxation on Europa 总被引:1,自引:0,他引:1
Models of topographic support on Europa by lateral shell thickness variations have previously assumed a Newtonian ice viscosity. Here I show that using a more realistic stress-dependent viscosity gives relaxation times which can be significantly different. Topography of wavelength 100 km cannot be supported by lateral shell thickness variations for ∼50 Myr, unless the shell thickness is <10 km or the ice grain size >10 mm. Shorter wavelength topography would require even thinner shells, but may be supported elastically. Global-scale variations in shell thickness, however, can be supported for geological timescales if the shell thickness is O(10 km). 相似文献
90.