正Electrical and electromagnetic method Wang et al.present an anomalous principal component decomposition method based on the Stratton-Chu integral.The airwaves and sea layers can be separated from the anomalous field,eliminating the airwave effect.The method is implemented in integral transform form,making it a robust processing method,is particularly effective for removing the effect of the entire sea layer. 相似文献
The mechanism of the disruption, both lithospheric thinning and oceanization of the commonly accepted long‐term‐stable Archaean craton, is still an open question. The available models, all imply a bottom to top process. With the construction of a 1660‐km‐long transect across the eastern North China Craton (NCC), we demonstrate that both the P‐wave velocity and density in the lowermost crust beneath the central section are significantly higher than in the corresponding parts of the south and north sections on the transect. These features are interpreted as geophysical signature of lower crustal underplating, which supplies sufficiently high gravitational potential energy to trigger lateral flow of the lower crust. This magma underplating‐triggered bilateral lower crust flow may facilitate the lithospheric thinning by means of asthenosphere upwelling and decompression melting, which infill the gap produced by the lower crust flow. The underplating‐triggered lower crustal flow can provide an alternative mechanism to explain the NCC lithosphere disruption, which highlights the crustal feedback to Archaean lithosphere disruption, from top to bottom. 相似文献
Synchrotron-based in situ angle-dispersive X-ray diffraction experiments were conducted on a natural uvite-dominated tourmaline sample by using an external-heating diamond anvil cell at simultaneously high pressures and temperatures up to 18 GPa and 723 K, respectively. The angle-dispersive X-ray diffraction data reveal no indication of a structural phase transition over the P–T range of the current experiment in this study. The pressure–volume–temperature data were fitted by the high-temperature Birch–Murnaghan equation of state. Isothermal bulk modulus of K0 = 96.6 (9) GPa, pressure derivative of the bulk modulus of \(K_{0}^{\prime } = 12.5 \;(4)\), thermal expansion coefficient of α0 = 4.39 (27) × 10?5 K?1 and temperature derivative of the bulk modulus (?K/?T)P = ?0.009 (6) GPa K?1 were obtained. The axial thermoelastic properties were also obtained with Ka0 = 139 (2) GPa, \(K_{a0}^{\prime }\) = 11.5 (7) and αa0 = 1.00 (11) × 10?5 K?1 for the a-axis, and Kc0 = 59 (1) GPa, \(K_{c0}^{\prime }\) = 11.4 (5) and αc0 = 2.41 (24) × 10?5 K?1 for the c-axis. Both of axial compression and thermal expansion exhibit large anisotropic behavior. Thermoelastic parameters of tourmaline in this study were also compared with that of the other two ring silicates of beryl and cordierite. 相似文献