全文获取类型
收费全文 | 4108篇 |
免费 | 934篇 |
国内免费 | 450篇 |
专业分类
测绘学 | 273篇 |
大气科学 | 581篇 |
地球物理 | 2832篇 |
地质学 | 590篇 |
海洋学 | 425篇 |
天文学 | 302篇 |
综合类 | 225篇 |
自然地理 | 264篇 |
出版年
2024年 | 15篇 |
2023年 | 50篇 |
2022年 | 101篇 |
2021年 | 147篇 |
2020年 | 158篇 |
2019年 | 166篇 |
2018年 | 153篇 |
2017年 | 145篇 |
2016年 | 134篇 |
2015年 | 164篇 |
2014年 | 205篇 |
2013年 | 182篇 |
2012年 | 199篇 |
2011年 | 233篇 |
2010年 | 222篇 |
2009年 | 230篇 |
2008年 | 234篇 |
2007年 | 300篇 |
2006年 | 277篇 |
2005年 | 267篇 |
2004年 | 269篇 |
2003年 | 243篇 |
2002年 | 211篇 |
2001年 | 136篇 |
2000年 | 151篇 |
1999年 | 141篇 |
1998年 | 121篇 |
1997年 | 107篇 |
1996年 | 89篇 |
1995年 | 105篇 |
1994年 | 81篇 |
1993年 | 62篇 |
1992年 | 50篇 |
1991年 | 30篇 |
1990年 | 32篇 |
1989年 | 29篇 |
1988年 | 18篇 |
1987年 | 10篇 |
1986年 | 7篇 |
1985年 | 4篇 |
1984年 | 5篇 |
1983年 | 1篇 |
1981年 | 1篇 |
1979年 | 2篇 |
1977年 | 2篇 |
1954年 | 3篇 |
排序方式: 共有5492条查询结果,搜索用时 46 毫秒
121.
四川地区强震发生条件的综合分析 总被引:2,自引:0,他引:2
根据发震断层的时代,发震构造的应力和几何结构条件,对四川地区的强震发生条件进行了综合分析,结果表明,四川地区孕育和发生强震的断层主要晚更新世以来,特别是全新世以来活动的断裂;强震多发生在主压力方向与断层交角成30°~60°之间的最危险滑动角值范围,走滑断层的斜列状结构,断裂的交叉结构,断裂的枢纽结构,断裂上的弯曲,转折部位以及断裂带上的横向隆起,拗陷及其交接部位都是发震构造的结构特征,有利于强震的 相似文献
122.
山西省平陆地区位于山西地震带南端,为了分析该地区未来的长期强需求潜势,本较系统地分析当地的破坏性地震及1500年以来的有地震地震资料,并进一步应用中国在陆特征的地震轮回模式及其复发时间概率模型估算法当前特征地震轮回的平均时间间隔,以及从1995年起未来百年内复发强震的概率,结果表明:未来100年来该地区复发强震的危险性很高,未来50年内复发强震的危险性也不能排除。 相似文献
123.
唐山地震的超晚期强余震估计 总被引:1,自引:0,他引:1
根据华北历史地震的重复性和免疫性,认为在唐山周围85km,200年内,对6级地震具有一定的免疫性;在研究了唐山地震序列自身的衰减规律后,认为在今后几十几强余震的最大活动水平为5级,发生6级以上土地震的可能性很小。 相似文献
124.
阐述了如何利用地下水宏观异常作强烈地震的临震预报,详细叙述了利用地下水宏观异常预报地震三要素的方法。 相似文献
125.
中强地震前油井动态异常机理研究 总被引:1,自引:0,他引:1
在分析油井映震特征的基础上,着重对油井动态异常的形成机理进行了研究。认为:映震灵敏井孔的空间分布主要受应力易于集中的构造条件的控制,特别是断层的又汇处、转折端和断裂带,这是与其他流体观测项目的相同之处;在本研究中,首次提出了油井动态前兆异常形成的三种力学过程,即岩土力学过程、水动力学过程和气体动力学过程以及油井特有的二种”放大”作用(变径和气体膨胀)的观点;解释了油井动态震前多为正异常的力学机制。 相似文献
126.
从原始方程出发,应用大气运动的对称反对称性理论,就赤道地区一呈偶极子分布的反对称冷热源对越赤道气流的形成和维持作用进行了定性分析。结果表明,非绝热加热的反对称分布对越赤道气流的影响是通过诱发和维持反对称的气压场分量来实现的。即在热源上空低层形成低压,高层形成高压;在热汇上空形成相反的气压场。这样,在赤道上空高、低层就将形成与相应气压梯度方向一致的越赤道气流 相似文献
127.
A seismic re fraction/wide-angle reflection profile is analysed for the presence of correlated events ('phases'). The correlation problem is formulated in terms of temporally, spatially and frequency-local complex covariances. For robustness, the method concentrates on phase rather than amplitude information. This allows a computationally efficient algorithm that can make allowance for signal correlation length and can model curved wavefronts. A statistical test based on residual phase misfit across the analysed subarray is used to assess the probability that a detected event represents a real correlated signal.
With our chosen analysis parameters and confidence level (over 99.9 per cent). 1222 events were detected in the data. Using simple techniques based on 1-D earth models, detected events are associated with a small number of particular wave types. In this way, we have succeeded in classifying almost 95 per cent of the detected events. Those that remain describe those components of the data that are inconsistent with our simple ray paths in the 1-D assumption and with our prescribed tolerance. These include reverberations, near-surface guided waves and reflected waves from strongly laterally inhomogeneous structures. According to our modelling, about 25 per cent of the detected events are consistent with simple P -wave reflected energy, and these are to a very large extent (over 85 per cent) distinct from all the other wave-type models we have used. A direct mapping of the detected events into the offset-depth domain reveals dear internal and external consistencies among the detections for the various wave types. Estimated earth structure is consistent with models from previous analyses based on much larger data sets.
We have thus succeeded in extracting correlated events from the data and decomposing these, approximately but meaningfully, into distinct classes (ray paths) 相似文献
With our chosen analysis parameters and confidence level (over 99.9 per cent). 1222 events were detected in the data. Using simple techniques based on 1-D earth models, detected events are associated with a small number of particular wave types. In this way, we have succeeded in classifying almost 95 per cent of the detected events. Those that remain describe those components of the data that are inconsistent with our simple ray paths in the 1-D assumption and with our prescribed tolerance. These include reverberations, near-surface guided waves and reflected waves from strongly laterally inhomogeneous structures. According to our modelling, about 25 per cent of the detected events are consistent with simple P -wave reflected energy, and these are to a very large extent (over 85 per cent) distinct from all the other wave-type models we have used. A direct mapping of the detected events into the offset-depth domain reveals dear internal and external consistencies among the detections for the various wave types. Estimated earth structure is consistent with models from previous analyses based on much larger data sets.
We have thus succeeded in extracting correlated events from the data and decomposing these, approximately but meaningfully, into distinct classes (ray paths) 相似文献
128.
Noise reduction and detection of weak, coherent signals through phase-weighted stacks 总被引:10,自引:0,他引:10
We present a new tool for efficient incoherent noise reduction for array data employing complex trace analysis. An amplitude-unbiased coherency measure is designed based on the instantaneous phase, which is used to weight the samples of an ordinary, linear stack. The result is called the phase-weighted stack (PWS) and is cleaned from incoherent noise. PWS thus permits detection of weak but coherent arrivals. The method presented can easily be extended to phase-weighted cross-correlations or be applied in the τ p domain. We illustrate and discuss the advantages and disadvantages of PWS in comparison with other coherency measures and present examples. We further show that our non-linear stacking technique enables us to detect a weak lower-mantle P -to- S conversion from a depth of approximately 840 km on array data. Hints of an 840 km discontinuity have been reported; however, such a discontinuity is not yet established due to the lack of further evidence. 相似文献
129.
M. Cocco J. Pacheco S. K. Singh F. Courboulex 《Geophysical Journal International》1997,131(1):135-145
An analysis of the Zihuatanejo, Mexico, earthquake of 1994 December 10 ( M = 6.6), based on teleseismic and near-source data, shows that it was a normal-faulting, intermediate-depth ( H = 50 ± 5 km) event. It was located about 30 km inland, within the subducted Cocos plate. The preferred fault plane has an azimuth of 130°, a dip of 79° and a rake of −86°. The rupture consisted of two subevents which were separated in time by about 2 s, with the second subevent occurring downdip of the first. The measured stress drop was relatively high, requiring a Δσ of about a kilobar to explain the high-frequency level of the near-source spectra. A rough estimate of the thickness of the seismogenic part of the oceanic lithosphere below Zihuatanejo, based on the depth and the rupture extent of this event, is 40 km.
This event and the Oaxaca earthquake of 1931 January 15 ( M = 7.8) are the two significant normal-faulting, intermediate-depth shocks whose epicentres are closest to the coast. Both of these earthquakes were preceded by several large to great shallow, low-angle thrust earthquakes, occurring updip. The observations in other subduction zones show just the opposite: normal-faulting events precede, not succeed, updip, thrust shocks. Indeed, the thrust events, soon after their occurrence, are expected to cause compression in the slab, thus inhibiting the occurrence of normal-faulting events. To explain the occurrence of the Zihuatanejo earthquake, we note that the Cocos plate, after an initial shallow-angle subduction, unbends and becomes subhorizontal. In the region of the unbending, the bottom of the slab is in horizontal extension. We speculate that the large updip seismic slip during shallow, low-angle thrust events increases the buckling of the slab, resulting in an incremental tensional stress at the bottom of the slab and causing normal-faulting earthquakes. This explanation may also hold for the 1931 Oaxaca event. 相似文献
This event and the Oaxaca earthquake of 1931 January 15 ( M = 7.8) are the two significant normal-faulting, intermediate-depth shocks whose epicentres are closest to the coast. Both of these earthquakes were preceded by several large to great shallow, low-angle thrust earthquakes, occurring updip. The observations in other subduction zones show just the opposite: normal-faulting events precede, not succeed, updip, thrust shocks. Indeed, the thrust events, soon after their occurrence, are expected to cause compression in the slab, thus inhibiting the occurrence of normal-faulting events. To explain the occurrence of the Zihuatanejo earthquake, we note that the Cocos plate, after an initial shallow-angle subduction, unbends and becomes subhorizontal. In the region of the unbending, the bottom of the slab is in horizontal extension. We speculate that the large updip seismic slip during shallow, low-angle thrust events increases the buckling of the slab, resulting in an incremental tensional stress at the bottom of the slab and causing normal-faulting earthquakes. This explanation may also hold for the 1931 Oaxaca event. 相似文献
130.
松辽盆地白垩系的密集段及海水进侵的新证 总被引:37,自引:0,他引:37
在总结松辽盆地白恶系层地层特征的基础上,阐述了密集段的地质学和地球物理学标志,经分析,大多数重要反射与密集段相关而并非是层序边界,根据扫描电镜分析结果,在密集段中首次发现了钙质超微化石,为区内白垩纪海水进侵的提供了新的证据,由稳定同位素分析,密集段形成了缺氧,相对可容纳空间最大及水体最深时期。 相似文献