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41.
Therelationshipsbetwenearthquakesandpositionsofthesunandmoon(Ⅱ)——Sometemporalcharacteristicsoftheaftershocksequencesofstronge... 相似文献
42.
Researchonpredictionofthefolowingnotice┐ableshocksofearthquakesequencesPU-XIONGLIU(刘蒲雄),XIU-QICHEN(陈修启),XIAO-JIANLU(吕晓健)andD... 相似文献
43.
Considerations on the global seismic sequences: the second and the third largest aftershocks 总被引:1,自引:0,他引:1
Theodoros M. Tsapanos 《Geophysical Journal International》1992,111(3):630-636
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通过对邢台及邻区永年台应力的计算和对余震、余震频度关系的分析,表明邢台强烈地震发生后,震中区应力稍小于外区应力;应力的变化和余震频度、强余震关系较明显. 相似文献
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The aim of this work is to quantitatively set up a simple hypothesis for occurrence of earthquakes conditioned by prior events, on the basis of a previously existing model and the use of recent instrumental observations. A simple procedure is presented in order to determine the conditional probability of pairs of events (foreshock-mainshock, mainshock-aftershock) with short time and space separation. The first event of a pair should not be an aftershock, i.e., it must not be related to a stronger previous event. The Italian earthquake catalog of the Istituto Nazionale di Geofisica (ING) (1975–1995, M 3.4), the earthquake catalog of the Japan Meteorological Agency (JMA) (1983–1994, M 3.0) and that of the National Observatory of Athens (NOA) (1982–1994, M 3.8) were analyzed. The number of observed pairs depends on several parameters: the size of the space-time quiescence volume defining nonaftershocks, the inter event time, the minimum magnitude of the two events, and the spatial dimension of the alarm volume after the first event. The Akaike information criterion has been adopted to assess the optimum set of space-time parameters used in the definition of the pairs, assuming that the occurrence rate of subsequent events may be modeled by two Poisson processes with different rates: the higher rate refers to the space-time volume defined by the alarms and the lower one simulates earthquakes that occur in the nonalarm space-time volume. On the basis of the tests carried out on the seismic catalog of Italy, the occurrence rate of M 3.8 earthquakes followed by a M 3.8 mainshock within 10 km and 10 days (validity) is 0.459. We have observed, for all three catalogs, that the occurrence rate density for the second event of a couple (mainshock or aftershock) of magnitude M2 subsequent to a nonaftershock of magnitude M1 in the time range T can be modeled by the following relationship: (T, M2) = 10a + b(M1 - M2) with b varying from 0.74 (Japan) to 1.09 (Greece). The decrease of the occurrence rate in time for a mainshock after a foreshock or for large aftershocks after a mainshock, for all three databases, obeys the Omori's law with p changing from 0.94 (Italy) to 2.0 (Greece). 相似文献
47.
Statistical features of aftershock distribution size for moderate and large earthquakes in Chinese mainland 总被引:1,自引:0,他引:1
Based on data of earthquake sequences with MS≥5.0 in Chinese mainland from 1970 to 2004,for different se-quence types and different rupture modes of the main shock,the relationship between aftershock distribution size Rand the magnitude of the main shock M0 has been studied statistically.Considering the rupture mode of the mainshock,we give the quantitative statistical relationships between R and M0 under 95%confidence level for differentsequence types.Qualitatively,lgR,the logarithm of the aftershock distribution size,is positively correlative to theM0,but the data distribution is dispersed.Viewing from different sequence types,the correlation between R and M0is very weak for isolated earthquake type(IET)sequence,R distributes in the range from 5 to 60 km;For main-shock-aftershock type(MAT),lgR is positively correlative to M0;For multiple main shock type(MMT),the core-lation between lgR and M0 is not very obvious when M0≤6.2 and R distributes in the range from 5 to 70 km,whileit shows a linear correlation when M0≥6.3.The statistical results also show that the occupational ratios of differentsequence types for strike-slip and oblique slip are almost the same.But for dip-slip(mostly are thrust mechanisms),the ratio of MAT is higher than that of IET and MMT.Comparing with previous results,it indicates that,when M0is large enough,R is mainly determined by M0 and there is almost no relationship with the rupture mode of themain shock. 相似文献
48.
Using the ground motion attenuation relation, we calculated and compared the effective peak acceleration (EPA) generated by main shocks and their strong aftershocks of 21 earthquake sequences with MS≥7 occurred in Chinese mainland and offing of China during 1966~2002. The result shows that EPA of strong aftershocks usually exceed that of main shock for 76.2% earthquake sequences and EPA of more than 50% strong aftershocks are greatly lar-ger than that of main shocks in large area, which suggests that it is necessary to take damage produced by strong aftershock into account in the probabilistic seismic hazard analysis and the seismic design. 相似文献
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50.
依据1970年以来记录相对完备的MSge;5.0地震序列资料,统计研究了中国大陆余震分布尺度与序列最大地震震级M0及最大地震破裂形式之间的关系. 在95%置信概率下,考虑主震破裂形式, 分序列类型给出了余震分布尺度与M0之间的统计关系. 定性而言,余震分布尺度的对数lgR与M0正相关, 但数据分布较为离散. 分类型来看, 孤立型序列余震分布尺度与M0之间统计相关程度低, 余震分布尺度介于5~60 km之间; 主余型序列lgR与M0正相关; 多震型序列当M0le;6.2时lgR与M0之间相关性不显著,余震分布尺度介于5~70 km之间, 当M0ge;6.3时lgR与M0线性相关. 统计结果还表明, 走滑近走滑及斜滑型主震所导致序列类型比例之间没有显著差异,而倾滑近倾滑型主震(主要为逆断型破裂)所导致的主余型序列所占比例较高, 孤立型及多震型序列所占比例则相对较低. 对比研究显示, 当M0较高时,余震分布尺度主要取决于主震大小而与主震破裂形式关系不明显. 相似文献