Along-axis variation in crustal thickness at the ultraslow spreading Southwest Indian Ridge (50°E) from a wide-angle seismic experiment

The Southwest Indian Ridge (SWIR) is characterized by an ultraslow spreading rate, thin crust, and extensive outcrops of serpentinized peridotite. Previous studies have used geochemical and geophysical data to suggest the presence of a thicker crust at the central and shallowest portions of the SWIR...

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Main Authors: Niu, Xiongwei (Author), Ruan, Aiguo (Author), Li, Jiabiao (Author), Minshull, T.A (Author), Sauter, Daniel (Author), Wu, Zhenli (Author), Qiu, Xuelin (Author), Zhao, Minghui (Author), Chen, Y. John (Author), Singh, Satish (Author)
Format: Article
Language:English
Published: 2015-02.
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042 |a dc 
100 1 0 |a Niu, Xiongwei  |e author 
700 1 0 |a Ruan, Aiguo  |e author 
700 1 0 |a Li, Jiabiao  |e author 
700 1 0 |a Minshull, T.A.  |e author 
700 1 0 |a Sauter, Daniel  |e author 
700 1 0 |a Wu, Zhenli  |e author 
700 1 0 |a Qiu, Xuelin  |e author 
700 1 0 |a Zhao, Minghui  |e author 
700 1 0 |a Chen, Y. John  |e author 
700 1 0 |a Singh, Satish  |e author 
245 0 0 |a Along-axis variation in crustal thickness at the ultraslow spreading Southwest Indian Ridge (50°E) from a wide-angle seismic experiment 
260 |c 2015-02. 
856 |z Get fulltext  |u https://eprints.soton.ac.uk/374553/1/Niu_et_al-2015-Geochemistry%252C_Geophysics%252C_Geosystems.pdf 
520 |a The Southwest Indian Ridge (SWIR) is characterized by an ultraslow spreading rate, thin crust, and extensive outcrops of serpentinized peridotite. Previous studies have used geochemical and geophysical data to suggest the presence of a thicker crust at the central and shallowest portions of the SWIR, from the Prince Edward (35°30?E) to the Gallieni (52°20?E) fracture zones. Here we present a new analysis of wide-angle seismic data along the ridge 49°17?E-50°49?E. Our main conclusions are as follows: (1) we find an oceanic layer 2 of roughly constant thickness and steep velocity gradient, underlain by a layer 3 with variable thickness and low velocity gradient; (2) the crustal thickness varies from ?5 km beneath nontransform discontinuities (NTDs) up to ?10 km beneath a segment center; (3) the melt supply is focused in segment centers despite a small NTD between adjacent segments; (4) the presence of a normal upper mantle velocity indicates that no serpentinization occurs beneath this thick crust. Our observation of thick crust at an ultraslow spreading ridge adds further complexity to relationships between crustal thickness and spreading rate, and supports previous suggestions that the extent of mantle melting is not a simple function of spreading rate, and that mantle temperature or chemistry (or both) must vary significantly along axis. 
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