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Combined Gravimetric-Seismic Moho Model of Tibet

Baranov, Alexey, Bagherbandi, Mohammad, and Tenzer, Robert, 2018. Combined Gravimetric-Seismic Moho Model of Tibet. Geosciences, 8(12):461, doi:10.3390/geosciences8120461.

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@ARTICLE{2018Geosc...8..461B,
       author = {{Baranov}, Alexey and {Bagherbandi}, Mohammad and {Tenzer}, Robert},
        title = "{Combined Gravimetric-Seismic Moho Model of Tibet}",
      journal = {Geosciences},
     keywords = {Moho, satellite gravity missions, seismic data, terrain model, Tibet},
         year = 2018,
        month = dec,
       volume = {8},
       number = {12},
          eid = {461},
        pages = {461},
     abstract = "{Substantial progress has been achieved over the last four decades to
        better understand a deep structure in the Himalayas and Tibet.
        Nevertheless, the remoteness of this part of the world still
        considerably limits the use of seismic data. A possible way to
        overcome this practical restriction partially is to use products
        from the Earth's satellite observation systems. Global
        topographic data are provided by the Shuttle Radar Topography
        Mission (SRTM). Global gravitational models have been derived
        from observables delivered by the gravity-dedicated satellite
        missions, such as the Gravity Recovery and Climate Experiment
        (GRACE) and the Gravity field and steady-state Ocean Circulation
        Explorer (GOCE). Optimally, the topographic and gravity data
        should be combined with available results from tomographic
        surveys to interpret the lithospheric structure, including also
        a Moho relief. In this study, we use seismic, gravity, and
        topographic data to estimate the Moho depth under orogenic
        structures of the Himalayas and Tibet. The combined Moho model
        is computed based on solving the Vening Meinesz-Moritz (VMM)
        inverse problem of isostasy, while incorporating seismic data to
        constrain the gravimetric solution. The result of the combined
        gravimetric-seismic data analysis exhibits an anticipated more
        detailed structure of the Moho geometry when compared to the
        solution obtained merely from seismic data. This is especially
        evident over regions with sparse seismic data coverage. The
        newly-determined combined Moho model of Tibet shows a typical
        contrast between a thick crustal structure of orogenic
        formations compared to a thinner crust of continental basins.
        The Moho depth under most of the Himalayas and the Tibetan
        Plateau is typically within 60-70 km. The maximum Moho deepening
        of \raisebox{-0.5ex}\textasciitilde76 km occurs to the south of
        the Bangong-Nujiang suture under the Lhasa terrane. Local maxima
        of the Moho depth to \raisebox{-0.5ex}\textasciitilde74 km are
        also found beneath Taksha at the Karakoram fault. This Moho
        pattern generally agrees with the findings from existing
        gravimetric and seismic studies, but some inconsistencies are
        also identified and discussed in this study.}",
          doi = {10.3390/geosciences8120461},
       adsurl = {https://ui.adsabs.harvard.edu/abs/2018Geosc...8..461B},
      adsnote = {Provided by the SAO/NASA Astrophysics Data System}
}

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