Crustal structure of the Southwest Indian Ridge at the Atlantis II Fracture Zone

Citation
Mr. Muller et al., Crustal structure of the Southwest Indian Ridge at the Atlantis II Fracture Zone, J GEO R-SOL, 105(B11), 2000, pp. 25809-25828
Citations number
69
Categorie Soggetti
Earth Sciences
Journal title
JOURNAL OF GEOPHYSICAL RESEARCH-SOLID EARTH
ISSN journal
21699313 → ACNP
Volume
105
Issue
B11
Year of publication
2000
Pages
25809 - 25828
Database
ISI
SICI code
0148-0227(20001110)105:B11<25809:CSOTSI>2.0.ZU;2-U
Abstract
The Southwest Indian Ridge is a slow spreading end-member of the mid-ocean ridge system. The deepest borehole penetrating the lower oceanic crust, Oce an Drilling Program hole 735B, lies on the eastern transverse ridge of the Atlantis II Fracture Zone at 57 degreesE. A wide-angle seismic survey in th e vicinity of the borehole reveals a crustal structure that is highly heter ogeneous. To the east of Atlantis Bank, on which hole 735B is located, the crust consists of a 2-2.5 km thick high-velocity-gradient oceanic layer 2 a nd a 1-2 km thick low-velocity-gradient layer 3. The transform valley has a 2.5-3 km thick crust with anomalously low velocities interpreted to consis t largely of highly serpentinized mantle rocks. The seismically defined cru st is thickest beneath the borehole, where layer 2 is thinner and the lower crust is inferred to contain 2-3 km of partially serpentinized mantle. The seismic velocity models are consistent with gravity data which show weak r esidual mantle Bouguer anomalies because the regions of thinner crust have lower crustal densities. Stress variations deduced from mass balances betwe en the transform valley floor and the adjacent transverse ridges are much l arger than the likely threshold for lithospheric failure and therefore indi cate that the relief is supported dynamically. The variation of crustal thi ckness with spreading rate defined by data from the Southwest Indian Ridge and elsewhere is consistent with models of melt generation in which the upw elling mantle is cooled by conductive heat loss at very slow spreading rate s? resulting in reduced melt generation under the spreading axis. Large seg ment-scale variations in crustal thickness suggest subcrustal along-axis mi gration of melt toward segment centers.