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81.
A novel method of synthesizing seismic wave using wavelet reconstruction is proposed and compared with the traditional method of using theory of Fourier transform. By adjusting the frequency band energy and taking it as criterion, the formula of synthesizing seismic wave is deduced. Using the design parameters specified in Chinese Seismic Design Code for buildings, seismic waves are synthesized. Moreover, the method of selecting wavelet bases in synthesizing seismic wave and the influence of the damping ratio on synthesizing results are analyzed. The results show that the synthesis seismic waves using wavelet bases can represent the characteristics of the seismic wave as well as the ground characteristic period, and have good time-frequency non-stationary. 相似文献
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西扬子大陆区泥盆系因有丰富的矿产资源一直为地学界所关注.在泥盆纪盆地演化中,地质事件与成矿关系极为密切.盆地沉积类型有台地型和海槽型两种.台地型泥盆系在沉积建造、生物群落、地质事件及沉积矿产等多方面均能与中、下扬子区相对比,故归属南方区扬子型泥盆系;海槽型泥盆系与台地型泥盆系在时空上均紧密衔接,但成矿作用有明显差别.海槽型泥盆系多产出层控型金和多金属矿床,台地型则以沉积矿床为主. 相似文献
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高峰100号矿体硫、铅同位素特征 总被引:1,自引:0,他引:1
李蘅 《矿物岩石地球化学通报》2001,20(4):334-336
10 0号矿体的成矿物理化学环境为 :成矿温度 30 0± 30℃ ;成矿压力为 84.2× 10 5Pa ;LogfO2 =- 30 .4~- 35 .6 ,LogfCO2 =- 2 .5 5~ +0 .36 ,LogfS2 =- 8.3~ - 11.0 ,pH =4.2~ 4.9。同位素的分析结果 :硫化物的硫同位素为 6 4‰~ 12 .3‰ ,δ3 4 SΣS 值为 6 6~ 13 8;2 0 6Pb 2 0 4Pb值为 17 4 91~ 18 96 0 ,2 0 7Pb 2 0 4Pb值为 15 5 39~15 940 ,2 0 8Pb 2 0 4Pb值为 37 95 7~ 39 4 90。表明 10 0号矿体的硫源是混合硫 ,铅源是两种异常铅混合的结果。 相似文献
87.
T. L. Lim J. J. Quenby M. K. Reuss E. Keppler H. Kunow B. Heber R. J. Forsyth 《Annales Geophysicae》1996,14(4):400-410
During November 1992, a series of forward and reverse shocks passed the ULYSSES spacecraft. Spectral and anisotropy measurements are reported for protons and alpha particles between 0.28 and 6 MeV observed by the Energetic Particle Composition Experiment, data recorded by the Magnetometer Experiment and the high-energy (2.7-300 MeV) proton data from the Kiel Electron Telescope. An analysis of energetic particle, plasma and magnetometer data from ULYSSES has allowed a unique study of the corresponding arrival of fare particles, particles within a corotating interaction region and particles transported with a coronal mass ejection. We present an analysis of these data in terms of possible diffusive shock acceleration but conclude that this is likely to be incompatible with the short transit time of the particles. Shock drift acceleration of particles with energies 0.3 MeV/nucleon or solar acceleration followed by particle trapping behind the shock front are alternative possibilities. 相似文献
88.
拉张状态下方解石组构多星环带到,递进变形状态下才可能出现点极密.因为当分解剪应力达最大值时,含有众多方解石颗粒的岩石中,形成e双晶滑动最有利的方位不可能是唯一的,而是不同方位的滑动系在三维空间中的组合,并且e双晶极点和光轴各自构成古钟型。由于系同一应力作用下的产物,二钟型体的顶角大小不同,但彼此共轴,均平行主任应力方向,属共轴叠钟体。该叠钟体记录了岩石变形时的应力状态,未再变形之前,该组构为初始组构。岩石的递进变形过程,实际是初始组构的递进变形过程,最后形成定型组构.岩石递进变形的全过程,就是初始组构到定型组构的全过程. 相似文献
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90.
G. V. Gibbs D. F. Cox T. D. Crawford M. B. Boisen Jr M. Lim 《Physics and Chemistry of Minerals》2002,29(5):307-318
The electron localization function, η, evaluated for first-principles geometry optimized model structures generated for quartz and coesite, reveals that the oxide anions are coordinated by two hemispherically shaped η-isosurfaces located along each of the SiO bond vectors comprising the SiOSi angles. With one exception, they are also coordinated by larger banana-shaped isosurfaces oriented perpendicular to the plane centered in the vicinity of the apex of each angle. The hemispherical isosurfaces, ascribed to domains of localized bond-pair electrons, are centered ~0.70 Å along the bond vectors from the oxide anions and the banana-shaped isosurfaces, ascribed to domains of localized nonbonding lone-pair electrons, are centered ~0.60 Å from the apex of the angle. The oxide anion comprising the straight SiOSi angle in coesite is the one exception in that the banana-shaped isosurface is missing; however, it is coordinated by two hemispherically shaped isosurfaces that lie along the bond vectors. In the case of a first-principles model structure generated for stishovite, the oxide anion is coordinated by five hemispherically shaped η-isosurfaces, one located along each of the three SiO bond vectors (ascribed to domains of bonding-electron pairs) that are linked to the anion with the remaining two (ascribed to domains of nonbonding-electron pairs) located on opposite sides of the plane defined by three vectors, each isosurface at a distance of ~0.5 Å from the anion. The distribution of the five isosurfaces is in a one-to-one correspondence with the distribution of the maxima displayed by experimental Δρ and theoretical ??2ρ maps. Isosurface η maps calculated for quartz and the (HO) 3 SiOSi(OH) 3 molecule also exhibit maxima that correspond with the (3,?3) maxima displayed by distributions of ??2ρ. Deformation maps observed for the SiOSi bridges for the silica polymorphs and a number of silicates are similar to that calculated for the molecule but, for the majority, the maxima ascribed to lone-pair features are absent. The domains of localized nonbonding-electron pair coordinating the oxide anions of quartz and coesite provide a basis for explaining the flexibility and the wide range of the SiOSi angles exhibited by the silica polymorphs with four-coordinate Si. They also provide a basis for explaining why the SiO bond length in coesite decreases with increasing angle. As found in studies of the interactions of solute molecules with a solvent, a mapping of η-isosurfaces for geometry-optimized silicates is expected to become a powerful tool for deducing potential sites of electrophilic attack and reactivity for Earth materials. The positions of the features ascribed to the lone pairs in coesite correspond with the positions of the H atoms recently reported for an H-doped coesite crystal. 相似文献