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   1205篇
  免费   302篇
  国内免费   329篇
测绘学   130篇
大气科学   93篇
地球物理   466篇
地质学   674篇
海洋学   100篇
天文学   132篇
综合类   121篇
自然地理   120篇
  2024年   4篇
  2023年   16篇
  2022年   37篇
  2021年   38篇
  2020年   53篇
  2019年   76篇
  2018年   67篇
  2017年   56篇
  2016年   63篇
  2015年   79篇
  2014年   66篇
  2013年   82篇
  2012年   86篇
  2011年   82篇
  2010年   63篇
  2009年   97篇
  2008年   82篇
  2007年   86篇
  2006年   73篇
  2005年   55篇
  2004年   84篇
  2003年   75篇
  2002年   49篇
  2001年   51篇
  2000年   46篇
  1999年   49篇
  1998年   35篇
  1997年   30篇
  1996年   25篇
  1995年   25篇
  1994年   23篇
  1993年   17篇
  1992年   9篇
  1991年   6篇
  1990年   12篇
  1989年   8篇
  1988年   5篇
  1987年   2篇
  1986年   3篇
  1985年   5篇
  1984年   2篇
  1983年   4篇
  1982年   3篇
  1981年   2篇
  1979年   3篇
  1978年   1篇
  1954年   1篇
排序方式: 共有1836条查询结果,搜索用时 30 毫秒
81.
82.
The detailed analysis of landforms, drainages and geology of the area between the rivers Amaravati and Karjan was carried out in order to understand the tectonic history of the lower Narmada basin. Movement along the various faults in the area was studied on the basis of the drainage offsetting. Horizontal offsetting of stream channels was found quite demonstrable along NNW-SSE trending transverse faults. Tectonic landforms including systematic deflection of stream channels and ridges, alignment of fault scarp and saddles and displacement in the basement rocks and alluvial deposits show that the area is undergoing active deformation driven by the NSF system.  相似文献   
83.
84.
1997年11月8日西藏Mw7.5级玛尼地震是干涉雷达技术应用于地震观测以来的一次重要事件.在第一部分中,我们应用广泛使用的Okada线弹性位错模型,假设断层的各个分段滑动量均匀,反演得到断层各个分段的几何参数和均匀滑动量.本部分的反演进一步去除滑动均匀假设,并利用更能反映断层真实状态的角形元位错模型(线弹性),在第一部分反演得到断层几何的基础上,反演断层面的静态位错分布.反演结果表明,线弹性滑动分布模型能够更好地解释观测数据,进一步提高反演的数据拟合程度.最终得到了断层面上的走滑和倾滑位错分布.首次得到的断层面滑动分布显示断层面滑动在浅部(0~12 km)比较集中,地震破裂长度约170 km,最大左旋走滑位移达4.8 m;反演结果还表明局部段落存在较大倾滑位移,量值达到1.9 m,这在断层模型中是不能忽略的,它可能是断层两侧形变不对称的原因之一;反演得到的标量地震矩为2.18×1020 N·m,相当于矩震级Mw7.5,与Velasco等利用地震波形反演得到的结果一致.  相似文献   
85.
再论拟准检定法的原理、实施和应用   总被引:2,自引:0,他引:2  
综合阐述了拟准检定法的原理和特点、研究思路。拟准检定法的关键是如何正确选择拟准观测,文章介绍了初选的复选拟准观测的实施要点。列举了拟准检定法在图相关情况下的相差检测,形变分析中的异常探测以及GPS相位观测的周跳检测和修复等方面的应用例子。  相似文献   
86.
87.
湘东─赣西NNE向走滑构造   总被引:6,自引:3,他引:6  
湘东─赣西构造岩浆带位于郯庐断裂南延的关键性部位。中生代以来,该区 NNE向左旋走滑构造主要由会聚走滑和 K─ E离散走滑构造叠加而成。会聚走滑作用造就了 NNE向雁列式剪切断裂系、剪切弯曲和旋转构造、压剪性煤盆地以及断层动热变质─剪切重熔型花岗岩;而离散走滑作用则控制了该区广泛发育的张剪性红盆地、盆岭式构造地貌、以及大规模中低温热液矿床的形成。湘东─赣西复杂的平移构造型式很可能与该区地壳结构分层特征、前期断裂构造格局、平移幅度和多期走滑构造作用四个因素有关。  相似文献   
88.
走滑拉分作用与相山产铀火山盆地的就位   总被引:1,自引:1,他引:1  
相山火山盆地是我国著名的产铀火山盆地。本文依据相山盆地深部地质研究成果以及大陆动力学理论,探讨了相山产铀火山盆地的就位机制。研究表明,相山火山盆地火山活动划分为两个旋回,其就位受制于区域深断裂的走滑拉分作用。即第一旋回的火山机构就位于NE向深断裂右旋走滑复活产生的EW向拉分构造,形成了东西向展布的裂隙式火山喷溢带;第二旋回的火山机构就位于NE向深断裂左旋走滑复活产生的SN向拉分构造与EW向基底断裂的结点,产生了中心式火山岩浆喷溢侵出。此外,还探讨了富大铀矿的形成机制。  相似文献   
89.
Abstract Drilling was carried out to penetrate the Nojima Fault where the surface rupture occurred associated with the 1995 Hyogo-ken Nanbu earthquake. Two 500 m boreholes were successfully drilled through the fault zone at a depth of 389.4 m. The drilling data show that the relative uplift of the south-east side of the Nojima Fault (south-west segment) was approximately 230 m. The Nojima branch fault, which branches from the Nojima Fault, is inferred to extend to the Asano Fault. From the structural contour map of basal unconformity of the Kobe Group, the vertical component of displacement of the Nojima branch–Asano Fault is estimated to be 260–310 m. Because the vertical component of displacement on the Nojima Fault of the north-east segment is a total of those of the Nojima Fault of the south-west segment and of the Nojima branch–Asano Fault, it is estimated to total to 490–540 m. From this, the average vertical component of the slip rate on the Nojima Fault is estimated to be 0.4–0.45 m/103 years for the past 1.2 million years.  相似文献   
90.
Several strike–slip faults at Crackington Haven, UK show evidence of right-lateral movement with tip cracks and dilatational jogs, which have been reactivated by left-lateral strike–slip movement. Evidence for reactivation includes two slickenside striae on a single fault surface, two groups of tip cracks with different orientations and very low displacement gradients or negative (left-lateral) displacements at fault tips.

Evidence for the relative age of the two strike–slip movements is (1) the first formed tip cracks associated with right-lateral slip are deformed, whereas the tip cracks formed during left-lateral slip show no deformation; (2) some of the tip cracks associated with right-lateral movement show left-lateral reactivation; and (3) left-lateral displacement is commonly recorded at the tips of dominantly right-lateral faults.

The orientation of the tip cracks to the main fault is 30–70° clockwise for right-lateral slip, and 20–40° counter-clockwise for left-lateral slip. The structure formed by this process of strike–slip reactivation is termed a “tree structure” because it is similar to a tree with branches. The angular difference between these two groups of tip cracks could be interpreted as due to different stress distribution (e.g., transtensional/transpressional, near-field or far-field stress), different fracture modes or fractures utilizing pre-existing planes of weakness.

Most of the dx profiles have similar patterns, which show low or negative displacement at the segment fault tips. Although the dx profiles are complicated by fault segments and reactivation, they provide clear evidence for reactivation. Profiles that experienced two opposite slip movements show various shapes depending on the amount of displacement and the slip sequence. For a larger slip followed by a smaller slip with opposite sense, the profile would be expected to record very low or reverse displacement at fault tips due to late-stage tip propagation. Whereas for a smaller slip followed by larger slip with opposite sense, the dx profile would be flatter with no reverse displacement at the tips. Reactivation also decreases the ratio of dmax/L since for an original right-lateral fault, left lateral reactivation will reduce the net displacement (dmax) along a fault and increase the fault length (L).

Finally we compare Crackington Haven faults with these in the Atacama system of northern Chile. The Salar Grande Fault (SGF) formed as a left-lateral fault with large displacement in its central region. Later right-lateral reactivation is preserved at the fault tips and at the smaller sub-parallel Cerro Chuculay Fault. These faults resemble those seen at Crackington Haven.  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