Abstract

The northeastern margin of the Tibetan Plateau, which includes the Qiangtang and Songpan-Ganzi terranes as well as the Kunlun Shan and the Qaidam Basin, continues to deform in response to the ongoing India–Eurasia collision. To test competing hypotheses concerning the mechanisms for this deformation, we assembled a high-quality data set of approximately 14 000 P- and 4000 S-wave arrival times from earthquakes at teleseismic distances from the International Deep Profiling of Tibet and the Himalaya, Phase IV broad-band seismometer deployments. We analyse these arrival times to determine tomographic images of P- and S-wave velocities in the upper mantle beneath this part of the plateau. To account for the effects of major heterogeneity in crustal and uppermost mantle wave velocities in Tibet, we use recent surface wave models to construct a starting model for our teleseismic body wave inversion. We compare the results from our model with those from simpler starting models, and find that while the reduction in residuals and results for deep structure are similar between models, the results for shallow structure are different. Checkerboard tests indicate that features of ∼125 km length scale are reliably imaged throughout the study region. Using synthetic tests, we show that the best recovery is below ∼300 km, and that broad variations in shallow structure can also be recovered. We also find that significant smearing can occur, especially at the edges of the model. We observe a shallow dipping seismically fast structure at depths of ∼140–240 km, which dies out gradually between 33°N and 35°N. Based on the lateral continuity of this structure (from the surface waves) we interpret it as Indian lithosphere. Alternatively, the entire area could be thickened by pure shear, or the northern part could be an underthrust Lhasa Terrane lithospheric slab with only the southern part from India. We see a deep fast wave velocity anomaly (below 300 km), that is consistent with receiver function observations of a thickened transition zone and could be a fragment of oceanic lithosphere. In NE Tibet, it appears to be disconnected from faster wave velocities above (i.e. it is not downwelling or subducting here). Our models corroborate results of previous work which imaged a relatively slow wave velocity region below the Kunlun Shan and northern Songpan-Ganzi Terrane, which is difficult to reconcile with the hypothesis of southward-directed continental subduction at the northern margin. Wave velocities in the shallow mantle beneath the Qaidam Basin are faster than normal, and more so in the east than the west.

Highlights

  • The high (∼5 km) elevation of the Tibetan Plateau is a consequence of the collision between the Indian and Eurasian plates during the closure of the Tethys Ocean

  • We describe the results of an arrival time tomography study of the upper mantle beneath northeast Tibet using recordings of P and S waves from earthquakes at teleseismic distances from the INDEPTH IV array

  • In eastern Tibet, the Lhasa and Qiangtang terranes are separated by the Bangong–Nujiang Suture (BNS), which began as a rift in the Early Ordovician or Carboniferous, and later became a convergent margin

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Summary

Introduction

The high (∼5 km) elevation of the Tibetan Plateau is a consequence of the collision between the Indian and Eurasian plates during the closure of the Tethys Ocean. The evolution of the Tibetan Plateau (Fig. 1) involved numerous collisions, with terranes accreted to Eurasia during the closure of the Tethys Ocean. In eastern Tibet, the Lhasa and Qiangtang terranes are separated by the Bangong–Nujiang Suture (BNS), which began as a rift in the Early Ordovician or Carboniferous, and later became a convergent margin. The Qiangtang and the Songpan-Ganzi terranes are separated by the Jinsha Suture (JS), which was formed by the closure of the Songpan-Ganzi Ocean (Yin & Harrison 2000) in the late Triassic or earliest Jurassic (Dewey et al 1988). Mechie & Kind (2013) note that three studies show the LAB to be at 150–200 km depth underneath northern Lhasa and the Qiangtang (Kumar et al 2006; Zhao et al 2011; Yue et al 2012) One way to estimate the thickness is to look for the lithosphere–asthenosphere boundary (LAB) using negative converters in receiver function studies. Mechie & Kind (2013) note that three studies show the LAB to be at 150–200 km depth underneath northern Lhasa and the Qiangtang (Kumar et al 2006; Zhao et al 2011; Yue et al 2012)

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