Probing Earths deep interior using mantle discontinuities Arwen
Probing Earth’s deep interior using mantle discontinuities Arwen Deuss University of Cambridge, UK also: Jennifer Andrews, Kit Chambers, Simon Redfern, John Woodhouse
Global tomography Velocity heterogeneity in the Earth: Ritsema, van Heijst & Woodhouse (1999) * thermal in origin? * also chemical/compositional heterogeneity? * lithosphere/asthenosphere boundary? * what happens in the transition zone? * where do slabs go?
Mantle discontinuities mineral physics seismology Seismology (Deuss & Woodhouse, GRL, 2002)
History Number of papers per depth, since 1959
Questions (1) what is the nature of the Lehmann discontinuity at 220 km depth? (2) what happens in the transition zone and how much thermal vs. chemical heterogeneity? (3) are there discontinuities in the lower mantle?
Data: 7018 traces * 6. 0 < Mw < 7. 0 * 100 < distance < 160 * depth < 75 km
Global data coverage SS-wave bounce points
Complete data set * synthetics for PREM: discontinuities at 220, 400 and 670 km depth *complete data set: discontinuities at 410, 520 and 660 km depth
Robustness of reflections Stack for North America 220 410 520 660 800 1050 1150 (Deuss & Woodhouse, GRL, 2002)
Robustness of reflections Stack for Indonesia 220 410 520 660 1050 1150 (Deuss & Woodhouse, GRL, 2002)
Reflections per depth * clear reflections from transition zone discontinuities at 410 and 660 km depth * additional discontinuities in upper and lower mantle at 220, 260, 310 and 800 km depth (Deuss & Woodhouse, GRL 2002)
Questions (1) what is the nature of the Lehmann discontinuity at 220 km depth? (2) what happens in the transition zone and how much thermal vs. chemical heterogeneity? (3) are there discontinuities in the lower mantle?
Upper mantle reflectors (Deuss & Woodhouse, GRL, 2002)
Mantle discontinuities - Mineral physics Seismological observations (Deuss & Woodhouse, EPSL, 2004) Clapeyron Slopes
Mineral physical mechanisms Phase transitions: * Coesite –Stishovite, 250 -300 km depth, d. P/d. T=2. 5 -3. 1 * Orthoenstatite – High clinoenstatite, 250 -300 km depth, d. P/d. T=1. 4 Change in deformation mechanism: * Dislocation-diffusion creep dry: 340 -380 km depth, d. P/d. T=-2. 4 wet: 240 -280 km depth, d. P/d. T=-2. 4 Karato (1993)
Questions (1) what is the nature of the Lehmann discontinuity at 220 km depth? (2) what happens in the transition zone and how much thermal vs. chemical heterogeneity? (3) are there discontinuities in the lower mantle?
Transition zone structure
410 km topography (Chambers, Deuss & Woodhouse, EPSL, 2005)
520 -km discontinuity Observations Splitting of 520 -km discontinuity * more complicated than just olivine * garnet phase change? trace elements? (Deuss & Woodhouse, Science, 2001)
Splitting observations 520 km discontinuity * no correlation with tectonic features
Phase transitions: 520 km discontinuity Pyrolite phase diagram a b g * high Fe-content: no b-g transition * wet conditions: b-g much sharper * low Ca-content: no gt-Ca. Pv transition
WKBJ synthetics Two reflectors can indeed be observed!
Regional stacks Transition zone SS precursors: * 410 and 660 km visible in all PP precursors: * 410 km always visible * 660 km visible in some regions
660 -km discontinuity Observations Clear reflections from 660 km depth in PP precursors (Deuss et al. , Science, 2006)
660 -km discontinuity Observations Long period: single peaks Short period: double peaks
Mineral physics: 660 km discontinuity For pyrolite mantle composition (after Hirose, 2001)
Seismic amplitudes Variations in amplitudes are consistent with the pyrolite model (using Weidner & Wang, 1998)
Questions (1) what is the nature of the Lehmann discontinuity at 220 km depth? (2) what happens in the transition zone and how much thermal vs. chemical heterogeneity? (3) are there discontinuities in the lower mantle?
Lower mantle Data * reflections around 800 km and 1000 -1200 km
Lower mantle 800 -900 km * in different regions, both continental and oceanic
Lower mantle 1000 -1200 km * mainly in subduction zone areas related to slabs?
Lower mantle – Mineral physics Phase transitions * stishovite -> Ca. Cl 2 -type (in Si. O 2) * (Mg, Fe)Si. O 3 perovskite, orthorhombic -> cubic phase Others * change in chemical composition? * change in deformation mechanism? free silica? unlikely!
What next? Fresnel zones Dahlen, 2003
Conclusions * comparison of seismic observations of mantle discontinuities with mineral physics implies significant amount of chemical heterogeneity * important implications for mantle flow * we need to expand to other data types and implement new techniques (such as finite frequency kernels) to further understand the level of heterogeneity
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