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Submeridional boundary zone in Asia : Seismicity, lithosphere structure, and the distribution of convective flows in the upper mantle. / Bushenkova, N. A.; Kuchay, O. A.; Chervov, V. V.

In: Geodynamics and Tectonophysics, Vol. 9, No. 3, 01.01.2018, p. 1007-1023.

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Bushenkova NA, Kuchay OA, Chervov VV. Submeridional boundary zone in Asia: Seismicity, lithosphere structure, and the distribution of convective flows in the upper mantle. Geodynamics and Tectonophysics. 2018 Jan 1;9(3):1007-1023. doi: 10.5800/GT-2018-9-3-0381

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Bushenkova, N. A. ; Kuchay, O. A. ; Chervov, V. V. / Submeridional boundary zone in Asia : Seismicity, lithosphere structure, and the distribution of convective flows in the upper mantle. In: Geodynamics and Tectonophysics. 2018 ; Vol. 9, No. 3. pp. 1007-1023.

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@article{e263717b0eed461d9b1c94cdc2b93b77,
title = "Submeridional boundary zone in Asia: Seismicity, lithosphere structure, and the distribution of convective flows in the upper mantle",
abstract = "The study is focused on the submeridional transregional boundary that stretches as a wide band along 105°E in Central Asia. In modern seismic models, it is traceable to a depth of ~600 km. In the continental area to the west of this boundary, seismic activity is increased. Following the study of the origin of the transregional boundary zone, it becomes possible to assess its contribution to the current geodynamic processes in Asia. This article presents a comprehensive analysis based on comparison of the available data with the results obtained in our study using independent methods. The distribution of earthquakes was analyzed by depth. We revealed a correlation between the characteristics of seismotectonic deformation (STD) reconstructed from earthquake focal mechanisms, the structure of P‐velocity anomalies, and the distribution of convection flows in the upper mantle. The pattern of seismic velocity anomalies in the upper mantle was investigated on the basis of the data from the ISC catalogue for the period of 1964-2011. The modeling was carried out for two regional tomographic schemes, using the first arrivals of P‐waves from [Koulakov et al., 2002] and PP‐phases from [Bushenkova et al., 2002], with the subsequent summation with weight coefficients depending on the distribution of the input data in each scheme. A similar approach was applied in [Koulakov, Bushenkova, 2010] for the territory of Siberia; however, that model only partially covered the submeridional transregional boundary zone and was based on fewer ISC data (until 2001). The parameters of the combined model were used to estimate variations in the lithosphere thickness, which can significantly influence the structure of convection flows in the upper mantle [Chervov et al., 2014; Bushenkova et al., 2014, 2016]. The thickness variations were taken into account when setting boundary conditions in the numerical modeling of thermal convection, which followed the algorithm described in [Chervov, Chernykh, 2014]. The STD field was reconstructed from the earthquake focal mechanisms (M≥4.6) which occurred in Central Asia in 1976-2017. The analysis shows that the zone, wherein the seismic regime changes, correlates with the band wherein the STD principal axes are turning, the submeridional high/low velocity elongated boundary in the seismotomographic model, as well as with the submeridionally elongated descending convective flow in the upper mantle. Shortening of the STD principal axes is observed in the submeridional direction in the western part and in the sublatitudinal direction in the eastern part of the study area. The directions of the principal axes turn in the 93-105°E zone. It is thus probable that the submeridionally elongated descending convective flow in the upper mantle of this region, which results from the superposition of the lithosphere thickness heterogeneities, is a barrier to propagation of seismically manifested active geodynamic processes caused by lithospheric plates collision.",
keywords = ": continental seismicity, Central Asia, Lithosphere structure, Submeridional boundary zone, Thermal convection in the upper mantle, VELOCITY, lithosphere structure, STRONG EARTHQUAKES, ACTIVE TECTONICS, STRUCTURE BENEATH, submeridional boundary zone, CRUSTAL MOVEMENTS, FOCAL MECHANISMS, CONTINENT, thermal convection in the upper mantle, continental seismicity, TECTONIC STRESSES, RECENT GEODYNAMICS, MONGOLIA",
author = "Bushenkova, {N. A.} and Kuchay, {O. A.} and Chervov, {V. V.}",
year = "2018",
month = jan,
day = "1",
doi = "10.5800/GT-2018-9-3-0381",
language = "English",
volume = "9",
pages = "1007--1023",
journal = "Geodynamics and Tectonophysics",
issn = "2078-502X",
publisher = "Institute of the Earth's Crust",
number = "3",

}

RIS

TY - JOUR

T1 - Submeridional boundary zone in Asia

T2 - Seismicity, lithosphere structure, and the distribution of convective flows in the upper mantle

AU - Bushenkova, N. A.

AU - Kuchay, O. A.

AU - Chervov, V. V.

PY - 2018/1/1

Y1 - 2018/1/1

N2 - The study is focused on the submeridional transregional boundary that stretches as a wide band along 105°E in Central Asia. In modern seismic models, it is traceable to a depth of ~600 km. In the continental area to the west of this boundary, seismic activity is increased. Following the study of the origin of the transregional boundary zone, it becomes possible to assess its contribution to the current geodynamic processes in Asia. This article presents a comprehensive analysis based on comparison of the available data with the results obtained in our study using independent methods. The distribution of earthquakes was analyzed by depth. We revealed a correlation between the characteristics of seismotectonic deformation (STD) reconstructed from earthquake focal mechanisms, the structure of P‐velocity anomalies, and the distribution of convection flows in the upper mantle. The pattern of seismic velocity anomalies in the upper mantle was investigated on the basis of the data from the ISC catalogue for the period of 1964-2011. The modeling was carried out for two regional tomographic schemes, using the first arrivals of P‐waves from [Koulakov et al., 2002] and PP‐phases from [Bushenkova et al., 2002], with the subsequent summation with weight coefficients depending on the distribution of the input data in each scheme. A similar approach was applied in [Koulakov, Bushenkova, 2010] for the territory of Siberia; however, that model only partially covered the submeridional transregional boundary zone and was based on fewer ISC data (until 2001). The parameters of the combined model were used to estimate variations in the lithosphere thickness, which can significantly influence the structure of convection flows in the upper mantle [Chervov et al., 2014; Bushenkova et al., 2014, 2016]. The thickness variations were taken into account when setting boundary conditions in the numerical modeling of thermal convection, which followed the algorithm described in [Chervov, Chernykh, 2014]. The STD field was reconstructed from the earthquake focal mechanisms (M≥4.6) which occurred in Central Asia in 1976-2017. The analysis shows that the zone, wherein the seismic regime changes, correlates with the band wherein the STD principal axes are turning, the submeridional high/low velocity elongated boundary in the seismotomographic model, as well as with the submeridionally elongated descending convective flow in the upper mantle. Shortening of the STD principal axes is observed in the submeridional direction in the western part and in the sublatitudinal direction in the eastern part of the study area. The directions of the principal axes turn in the 93-105°E zone. It is thus probable that the submeridionally elongated descending convective flow in the upper mantle of this region, which results from the superposition of the lithosphere thickness heterogeneities, is a barrier to propagation of seismically manifested active geodynamic processes caused by lithospheric plates collision.

AB - The study is focused on the submeridional transregional boundary that stretches as a wide band along 105°E in Central Asia. In modern seismic models, it is traceable to a depth of ~600 km. In the continental area to the west of this boundary, seismic activity is increased. Following the study of the origin of the transregional boundary zone, it becomes possible to assess its contribution to the current geodynamic processes in Asia. This article presents a comprehensive analysis based on comparison of the available data with the results obtained in our study using independent methods. The distribution of earthquakes was analyzed by depth. We revealed a correlation between the characteristics of seismotectonic deformation (STD) reconstructed from earthquake focal mechanisms, the structure of P‐velocity anomalies, and the distribution of convection flows in the upper mantle. The pattern of seismic velocity anomalies in the upper mantle was investigated on the basis of the data from the ISC catalogue for the period of 1964-2011. The modeling was carried out for two regional tomographic schemes, using the first arrivals of P‐waves from [Koulakov et al., 2002] and PP‐phases from [Bushenkova et al., 2002], with the subsequent summation with weight coefficients depending on the distribution of the input data in each scheme. A similar approach was applied in [Koulakov, Bushenkova, 2010] for the territory of Siberia; however, that model only partially covered the submeridional transregional boundary zone and was based on fewer ISC data (until 2001). The parameters of the combined model were used to estimate variations in the lithosphere thickness, which can significantly influence the structure of convection flows in the upper mantle [Chervov et al., 2014; Bushenkova et al., 2014, 2016]. The thickness variations were taken into account when setting boundary conditions in the numerical modeling of thermal convection, which followed the algorithm described in [Chervov, Chernykh, 2014]. The STD field was reconstructed from the earthquake focal mechanisms (M≥4.6) which occurred in Central Asia in 1976-2017. The analysis shows that the zone, wherein the seismic regime changes, correlates with the band wherein the STD principal axes are turning, the submeridional high/low velocity elongated boundary in the seismotomographic model, as well as with the submeridionally elongated descending convective flow in the upper mantle. Shortening of the STD principal axes is observed in the submeridional direction in the western part and in the sublatitudinal direction in the eastern part of the study area. The directions of the principal axes turn in the 93-105°E zone. It is thus probable that the submeridionally elongated descending convective flow in the upper mantle of this region, which results from the superposition of the lithosphere thickness heterogeneities, is a barrier to propagation of seismically manifested active geodynamic processes caused by lithospheric plates collision.

KW - : continental seismicity

KW - Central Asia

KW - Lithosphere structure

KW - Submeridional boundary zone

KW - Thermal convection in the upper mantle

KW - VELOCITY

KW - lithosphere structure

KW - STRONG EARTHQUAKES

KW - ACTIVE TECTONICS

KW - STRUCTURE BENEATH

KW - submeridional boundary zone

KW - CRUSTAL MOVEMENTS

KW - FOCAL MECHANISMS

KW - CONTINENT

KW - thermal convection in the upper mantle

KW - continental seismicity

KW - TECTONIC STRESSES

KW - RECENT GEODYNAMICS

KW - MONGOLIA

UR - http://www.scopus.com/inward/record.url?scp=85055639845&partnerID=8YFLogxK

U2 - 10.5800/GT-2018-9-3-0381

DO - 10.5800/GT-2018-9-3-0381

M3 - Article

AN - SCOPUS:85055639845

VL - 9

SP - 1007

EP - 1023

JO - Geodynamics and Tectonophysics

JF - Geodynamics and Tectonophysics

SN - 2078-502X

IS - 3

ER -

ID: 17246692