Abstract

SUMMARYThe mantle transition zone is the region between the globally observed major seismic velocity discontinuities around depths of 410 and 660 km and is important for determining the style of convection and mixing between the upper and the lower mantle. In this study, P-to-S converted waves, or receiver functions, are used to study these discontinuities beneath the Alaskan subduction zone, where the Pacific Plate subducts underneath the North American Plate. Previous tomographic models do not agree on the depth extent of the subducting slab, therefore improved imaging of the Earth structure underneath Alaska is required. We use 27 800 high quality radial receiver functions to make common conversion point stacks. Upper mantle velocity anomalies are accounted for by two recently published regional tomographic S-wave velocity models. Using these two tomographic models, we show that the discontinuity depths within our CCP stacks are highly dependent on the choice of velocity model, between which velocity anomaly magnitudes vary greatly. We design a quantitative test to show whether the anomalies in the velocity models are too strong or too weak, leading to over- or undercorrected discontinuity depths. We also show how this test can be used to rescale the 3-D velocity corrections in order to improve the discontinuity topography maps.After applying the appropriate corrections, we find a localized thicker mantle transition zone and an uplifted 410 discontinuity, which show that the slab has clearly penetrated into the mantle transition zone. Little topography is seen on the 660 discontinuity, indicating that the slab has probably not reached the lower mantle. In the southwest, P410s arrivals have very small amplitudes or no significant arrival at all. This could be caused by water or basalt in the subducting slab, reducing the strength at the 410, or by topography on the 410 discontinuity, preventing coherent stacking. In the southeast of Alaska, a thinner mantle transition zone is observed. This area corresponds to the location of a slab window, and thinning of the mantle transition zone may be caused by hot mantle upwellings.

Highlights

  • The mantle transition zone delineates the upper from the lower mantle, and its characteristic phase transitions both affect and reflect the style of mantle convection

  • The receiver function data set is used to make common conversion point (CCP) stacks to study the topography on the transition zone discontinuities underneath Alaska using PREM, MABPM and JSWLW

  • We will present our results on the MTZ thickness and the topography of the 410 and the 660, for the different velocity models used

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Summary

Introduction

The mantle transition zone delineates the upper from the lower mantle, and its characteristic phase transitions both affect and reflect the style of mantle convection. Subducting plates leave an imprint on the boundaries of the mantle transition zone, the seismic discontinuities at approximately 410 and 660 km depth. By studying these we can constrain the depth extent of subducting slabs. We use receiver functions, which are waves that convert at discontinuities, to image the mantle transition zone to better constrain the Earth structure underneath Alaska. A U.S state, is located on the northwestern edge of the North American plate and along the northern part of the Pacific subduction zone. At the eastern part of the subduction zone lies the Yakutat terrane, a region of unusually thick oceanic crust

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