Abstract

Using the spectral-element method, we explored the effect of topography of upper-mantle discontinuities on the traveltimes of SS precursors recorded on transverse component seismograms. The latter are routinely used to infer the topography of mantle transition zone discontinuities. The step from precursory traveltimes to topographic changes is mainly done using linearised ray theory, or sometimes using finite-frequency kernels. We simulated exact seismograms in 1-D and 3-D elastic models of the mantle. In a second simulation, we added topography to the discontinuities. We compared the waveforms obtained with and without topography by cross correlation of the SS precursors. Since we did not add noise, the precursors are visible in individual seismograms without the need of stacking. The resulting time anomalies were then converted into topographic variations and compared to the original topographic models. Based on the correlation between initial and inferred models, and provided that ray coverage is good, we found that linearised ray theory gives a relatively good idea on the location of the uplifts and depressions of the discontinuities. It seriously underestimates the amplitude of the topographic variations by a factor ranging between 2 and 7. Real data depend on the 3-D elastic structure and the topography. All studies to date correct for the 3-D elastic effects assuming that the traveltimes can be linearly decomposed into a structure and a discontinuity part. We found a strong non-linearity in this decomposition which cannot be modelled without a fully non-linear inversion for elastic structure and discontinuities simultaneously.

Highlights

  • The nature of the mantle transition zone (MTZ) discontinuities is still not fully understood, despite their potential importance for understanding the mineralogical and geodynamic state of the mantle, for example, Morgan & Shearer (1993)

  • Other studies have used receiver functions to analyse Ps and Sp conversions to determine the topography of the MTZ discontinuities using regional and global data, (e.g. Paulssen 1988; Shearer 1991; Chevrot et al 1999; Tonegawa et al 2005; Lawrence & Shearer 2006; Andrews & Deuss 2008; Tauzin et al 2008; Eagar et al 2010; Tauzin et al 2013)

  • We investigate for the first time the reliability of linearised ray theory for converting SS precursors into depths of MTZ discontinuities

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Summary

Introduction

The nature of the mantle transition zone (MTZ) discontinuities is still not fully understood, despite their potential importance for understanding the mineralogical and geodynamic state of the mantle, for example, Morgan & Shearer (1993). Shearer 1991; Shearer & Masters 1992; Shearer 1993; Vasco et al 1995; Estabrook & Kind 1996; Flanagan & Shearer 1998, 1999; Shearer et al 1999; Shearer 2000; Gu & Dziewonski 2002; Deuss & Woodhouse 2002; Gu et al 2003; Schmerr & Garnero 2006, 2007; Deuss 2007, 2009; Lawrence & Shearer 2008; Houser et al 2008; Thomas & Billen 2009; Lessing et al 2014) These data are attractive because their main sensitivity is concentrated near their bounce points (or midpoints), which are halfway between source and receiver, for a source at the surface. The receiver function method is predominantly sensitive to structure beneath the recording station; it can provide detailed maps of topography of the ‘410’ and ‘660’ mainly in continental regions

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