An overview of the crustal structure of the Tibetan plateau after 35 years of deep seismic soundings

2011 ◽  
Vol 40 (4) ◽  
pp. 977-989 ◽  
Author(s):  
Zhongjie Zhang ◽  
Yangfan Deng ◽  
Jiwen Teng ◽  
Chunyong Wang ◽  
Rui Gao ◽  
...  
1977 ◽  
Vol 67 (3) ◽  
pp. 735-750
Author(s):  
Kin-Yip Chun ◽  
Toshikatsu Yoshii

abstract Group velocities of fundamental-mode Rayleigh and Love waves are analyzed to construct a crustal structure of the Tibetan Plateau. A moving window analysis is employed to compute group velocities in a wide period range of 7 to 100 sec for 17 individual paths. The crustal models derived from these dispersion data indicate that under the Tibetan Plateau the total crustal thickness is about 70 km and that the crustal velocities are generally low. The low velocities are most probably caused by high temperatures. A low-velocity zone located at an intermediate depth within the crust appears to be strongly demanded by the observed dispersion data. The main features of the proposed crustal structure will place stringent constraints on future tectonic models of the Tibetan Plateau which is generally regarded as a region of active deformation due to the continent-continent collision between India and Asia.


2006 ◽  
Vol 241 (3-4) ◽  
pp. 804-814 ◽  
Author(s):  
Jungmeng Zhao ◽  
Walter D. Mooney ◽  
Xiankang Zhang ◽  
Zhichun Li ◽  
Zhijun Jin ◽  
...  

2006 ◽  
Vol 420 (1-2) ◽  
pp. 253-266 ◽  
Author(s):  
Mingjun Liu ◽  
Walter D. Mooney ◽  
Songlin Li ◽  
Nihal Okaya ◽  
Shane Detweiler

1995 ◽  
Vol 85 (6) ◽  
pp. 1531-1540 ◽  
Author(s):  
Lupei Zhu ◽  
Thomas J. Owens ◽  
George E. Randall

Abstract We investigate lateral variations in crustal structure across the northern boundary of the Tibetan Plateau using the receiver functions at three broadband stations deployed during the 1991-1992 Tibet PASSCAL experiment. The first 5 sec of the receiver functions vary systematically with backazimuth: the radial receiver functions are symmetric across the N-S axis while the tangential receiver functions are antisymmetric across this axis. This symmetry can be modeled by E-W striking dipping interfaces in the upper-middle crust. The strike direction is consistent with the E-W trend of surface geology. Modeling a P-to-S converted phase in the receiver functions at each station suggests that there is a mid-crustal low-velocity layer with its upper boundary dipping 20° to 30° to the south. In addition, a shallow northward-dipping interface is responsible for the “double-peaked” direct P arrivals in the radial receiver functions and large tangential motions at one of the stations. The low-velocity layer, together with other geological and seismological observations, suggests that there is a hot, possibly partial melt zone in the middle crust of northern Tibet. Alternately, dipping velocity interfaces might be associated with some buried thrust faults in the upper crust that accommodated crust shortening during the plateau formation.


2013 ◽  
Vol 24 (4-1) ◽  
pp. 505 ◽  
Author(s):  
Hansheng Wang ◽  
Longwei Xiang ◽  
Patrick Wu ◽  
Holger Steffen ◽  
Lulu Jia ◽  
...  

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