scholarly journals High resolution upper mantle discontinuity images across the Pacific Ocean from SS precursors using local slant stack filters

2015 ◽  
Vol 202 (1) ◽  
pp. 175-189 ◽  
Author(s):  
Zhao Zheng ◽  
Sergi Ventosa ◽  
Barbara Romanowicz
1963 ◽  
Vol 53 (1) ◽  
pp. 151-165
Author(s):  
Tetsuo A. Santô ◽  
Markus Båth

Abstract The dispersion of Rayleigh waves along a great number of Pacific paths has been studied by means of records from Pasadena, California, U. S. A., and Huancayo, Peru. Combining these measurements with previous ones based on records at Tsukuba, Hongkong, Honolulu and Suva, it was found that the central part of the Pacific Ocean exhibits the most oceanic structure, with exception for the Hawaiian Islands. In the south-eastern Pacific Ocean an area could be delineated with a new type of dispersion characteristics, not found in any other part of the Pacific. This area agrees closely with the Easter Island Ridge system, and exhibits unusually thin crust and low upper-mantle velocities as well as exceptionally high heat flow.


Science ◽  
1974 ◽  
Vol 186 (4159) ◽  
pp. 141-143 ◽  
Author(s):  
A. R. Leeds ◽  
L. Knopoff ◽  
E. G. Kausel

2000 ◽  
Vol 105 (B4) ◽  
pp. 8229-8242 ◽  
Author(s):  
Scott L. Neal ◽  
Randall L. Mackie ◽  
Jimmy C. Larsen ◽  
Adam Schultz

1993 ◽  
Vol 20 (8) ◽  
pp. 663-666 ◽  
Author(s):  
Martine Bussy ◽  
Jean-Paul Montagner ◽  
Barbara Romanowicz

1968 ◽  
Vol 5 (4) ◽  
pp. 1067-1078 ◽  
Author(s):  
N. A. Beliayevsky ◽  
A. A. Borisov ◽  
I. S. Volvovsky ◽  
Yu. K. Schukin

Transcontinental sections of the earth's crust and Upper Mantle from the Kuril Islands to the Carpathians, and along other principal directions, in all about 15 000 km long, show the following features:(1) The depth of an asthenosphere horizon agrees well with the position of a high-conductivity layer in the Upper Mantle.(2) Hypocenters of earthquakes are located in fault zones. In the zone of the Kuril Island arc, they plunge into the Upper Mantle to depths of hundreds of kilometers, dipping towards the continent.(3) Boundary velocities along the Mohorovičić discontinuity are not dependent on its depth, for they are always in the range 8.0–8.2 km/s; velocities within the crust are correlated with the depths of layers; in the roots of high mountains a layer of 7.5–7.8 km/s has been distinguished near the base of the crust.(3) The crustal thickness in folded areas is in a certain accordance with the altitude of the surface of the earth's solid cover, with Bouguer anomalies and amplitudes of neotectonic movements. It varies from 8 km in margin areas of the Pacific Ocean basin to 60 km in the Tien Shan. Average crustal thicknesses within the platforms are in the region of 40 km, increasing to 50 km in the southern outlying areas of the East-European platform and to 46 km in areas of recent tectonic activity within the Turanian and Siberian Platforms.(4) In deep depressions, internal and outlying seas, the crustal thickness is reduced, and 'granite' layer (6.0–6.5 km/s) is absent. Mesozoic formations of the Far East and adjacent zones of transition from the Pacific Ocean to the continent are distinguished by reduced thicknesses. In Alpine formations the 'basalt' layer dominates over the 'granite' layer.(5) Subhorizontal crustal stratification complicated by deep faults has been found everywhere. Plicate geosynclinal folding is not reflected in deep crustal structures.(6) Temperature of the platform folded basement is mainly related to thickness and composition of the sediments.The transcontinental sections provide a clearer idea of the relationship between anomalous geophysical fields and deep and shallow crustal structures than is given in corresponding maps.


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