Abstract:A global cross-section of the Earth parallel to the tectonic equator (TE) path, the great circle representing the equator of net lithosphere rotation, shows a difference in shear wave velocities between the western and eastern flanks of the three major oceanic rift basins. The lowvelocity layer in the upper asthenosphere, at a depth range of 120 to 200 km, is assumed to represent the decoupling between the lithosphere and the underlying mantle. Along the TE-perturbed (TE-pert) path, a ubiquitous LVZ, about 1,0… Show more
“…Plate growth rate is due to the difference between VA and VB. The plate separation increases at the half spreading rate hS = (VA−VB)/2, Vr being always faster than hS. Thickness of the oceanic lithosphere, estimated from geophysical data and confirmed with HP‐HT experimental results on mantle assemblages, is 100 km westwards far from the ridge and 80 km eastwards, and between 20 to 40 km depth at the ridge axis (Chalot‐Prat et al, 2010, 2013; Falloon, Danyushevsky, et al, 2007; Falloon, Green, & Danyushevsky, 2007; Green et al, 2014; Green & Falloon, 2015; Panza & Romanelli, 2014). Experimental results (Green & Falloon, 2015) demonstrate that MORB (Mid‐Oceanic Ridge Basalts) parental melts segregate from residual peridotite between 55 and 45 km depth (down to 65 km; up to 30 km) below the LAB (Lithosphere‐Asthenosphere Boundary) of the thinned lithosphere area.…”
Section: Correlations Between Shallow and Deep Lithospheric Processes...supporting
“…Plate growth rate is due to the difference between VA and VB. The plate separation increases at the half spreading rate hS = (VA−VB)/2, Vr being always faster than hS. Thickness of the oceanic lithosphere, estimated from geophysical data and confirmed with HP‐HT experimental results on mantle assemblages, is 100 km westwards far from the ridge and 80 km eastwards, and between 20 to 40 km depth at the ridge axis (Chalot‐Prat et al, 2010, 2013; Falloon, Danyushevsky, et al, 2007; Falloon, Green, & Danyushevsky, 2007; Green et al, 2014; Green & Falloon, 2015; Panza & Romanelli, 2014). Experimental results (Green & Falloon, 2015) demonstrate that MORB (Mid‐Oceanic Ridge Basalts) parental melts segregate from residual peridotite between 55 and 45 km depth (down to 65 km; up to 30 km) below the LAB (Lithosphere‐Asthenosphere Boundary) of the thinned lithosphere area.…”
Section: Correlations Between Shallow and Deep Lithospheric Processes...supporting
“…Moreover, seismic images from Panza and Romanelli (2014) show an asymmetric shape of the LVZ, thicker and more elongated westward (2/3 in volume) than eastward (1/3 in volume) of ridge axis in all oceans. This spectacular and permanent asymmetry of the LVZ shape raises the question not only of the origin of partial melting, but also of its much greater development below the western part of the oceans.…”
Section: Upper Asthenospherementioning
confidence: 96%
“…From the top to the bottom of this layer, seismic waves gradually increase their speed with respect to the LVZ. Vs is much higher than in the upper asthenosphere and more or less similar to that of the lithosphere (Panza and Romanelli 2014). Its mineralogical and chemical composition is inferred from experimental petrology on MORB genesis (Green et al, 2014;Green, 2015), being the N-MORB mantle source located below 230 km.…”
Section: Lower Asthenospherementioning
confidence: 97%
“…As shown by Doglioni et al (2003), observations on the bathymetry of ridge flanks (shallower eastward) of Pacific and Atlantic oceans and on variable rates of oceanic spreading (Muller et al, 1997;Mallows and Searle, 2012) contradict the concept of full symmetry. Panza et al (2010) and Panza and Romanelli (2014) provided evidence for asymmetry in both shear wave velocity and thickness within mantle lithosphere and asthenosphere when comparing the two sides of most spreading ridges. In general, the old (>60 Ma) western lithospheric plates have a faster shear wave velocity and are thicker (≈100 km versus ≈80 km in the eastern flank).…”
Section: Asymmetry On Both Sides Of Oceanic Spreading Axis and Prelimmentioning
confidence: 99%
“…In general, the old (>60 Ma) western lithospheric plates have a faster shear wave velocity and are thicker (≈100 km versus ≈80 km in the eastern flank). Seismic tomography (Thybo, 2006;Panza et al, 2010;Schmerr, 2012;Panza and Romanelli, 2014) provides robust evidence of an asymmetric LVZ at depths from about 80-100 km down to 180-225 km. The average Vs within the western LVZ is slower than the eastern one.…”
Section: Asymmetry On Both Sides Of Oceanic Spreading Axis and Prelimmentioning
Combining geophysical, petrological and structural data on oceanic mantle lithosphere, underlying asthenosphere and oceanic basalts, an alternative oceanic plate spreading model is proposed in the framework of the westward migration of oceanic spreading ridges relative to the underlying asthenosphere. This model suggests that evolution of both the composition and internal structure of oceanic plates and underlying upper mantle strongly depends at all scales on plate kinematics. We show that the asymmetric features of lithospheric plates and underlying upper asthenosphere on both sides of oceanic spreading ridges, as shown by geophysical data (seismic velocities, density, thickness, and plate geometry), reflect somewhat different mantle compositions, themselves related to various mantle differentiation processes (incipient to high partial melting degree, percolation/reaction and refertilisation) at different depths (down to 300 km) below and laterally to the ridge axis. The fundamental difference between western and eastern plates is linked to the westward ridge migration inducing continuing mantle refertilisation of the western plate by percolation-reaction with ascending melts, whereas the eastern plate preserves a barely refertilized harzburgitic residue. Plate thickness on both sides of the ridge is controlled both by cooling of the asthenospheric residue and by the instability of pargasitic amphibole producing a sharp depression of the water-undersaturated solidus, its intersection with the geotherm at ~90 km, and incipient melt production right underneath the lithosphere-asthenosphere boundary (LAB). Thus the intersection of the geotherm with the waterundersaturated lherzolite solidus explains the existence of a low-velocity zone (LVZ). As oceanic lithosphere is moving westward relative to asthenospheric mantle, this partially molten upper asthenosphere facilitates the decoupling between lower asthenosphere and lithosphere. Thereby the westward drift of the lithosphere is necessarily slowed down, top to down, inducing a progressive decoupling within the mantle lithosphere itself. This intra-mantle decoupling could be at the origin of asymmetric detachment faults allowing mantle exhumation along slow-spreading ridges. Taking into account the asymmetric features of the LVZ, migration of incipient melt fractions and upwelling paths from the lower asthenosphere through the upper asthenosphere are oblique, upward and eastward. MORB are sourced from an eastward and oblique, near-adiabatic mantle upwelling from the lower asthenosphere. This unidirectional mantle transfer is induced by isostatic suction of the migrating spreading ridge.
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