@article{781a0d45bd714cbf80d49e4275a17cf5,
title = "Mapping Crustal Shear Wave Velocity Structure and Radial Anisotropy Beneath West Antarctica Using Seismic Ambient Noise",
abstract = "Using 8- to 25-s-period Rayleigh and Love wave phase velocity dispersion data extracted from seismic ambient noise, we (i) model the 3-D shear wave velocity structure of the West Antarctic crust and (ii) map variations in crustal radial anisotropy. Enhanced regional resolution is offered by the UK Antarctic Seismic Network. In the West Antarctic Rift System (WARS), a ridge of crust ∼26–30 km thick extending south from Marie Byrd Land separates domains of more extended crust (∼22 km thick) in the Ross and Amundsen Sea Embayments, suggesting along-strike variability in the Cenozoic evolution of the WARS. The southern margin of the WARS is defined along the southern Transantarctic Mountains and Haag-Ellsworth Whitmore Mountains (HEW) block by a sharp crustal thickness gradient. Crust ∼35–40 km is modeled beneath the Haag Nunataks-Ellsworth Mountains, decreasing to ∼30–32 km thick beneath the Whitmore Mountains, reflecting distinct structural domains within the composite HEW block. Our analysis suggests that the lower crust and potentially the middle crust is positively radially anisotropic (VSH>VSV) across West Antarctica. The strongest anisotropic signature is observed in the HEW block, emphasizing its unique provenance among West Antarctica's crustal units, and conceivably reflects a ∼13-km-thick metasedimentary succession atop Precambrian metamorphic basement. Positive radial anisotropy in the WARS crust is consistent with observations in extensional settings and likely reflects the lattice-preferred orientation of minerals such as mica and amphibole by extensional deformation. Our observations support a contention that anisotropy may be ubiquitous in the continental crust.",
author = "O'Donnell, {J. P.} and Brisbourne, {A. M.} and Stuart, {G. W.} and Dunham, {C. K.} and Y. Yang and Nield, {G. A.} and Whitehouse, {P. L.} and Nyblade, {A. A.} and Wiens, {D. A.} and S. Anandakrishnan and Aster, {R. C.} and Huerta, {A. D.} and Lloyd, {A. J.} and T. Wilson and Winberry, {J. P.}",
note = "Funding Information: We thank all BAS camp staff, field guides, and air unit personnel for the logistical support of the UKANET seismic and GNSS networks. We similarly acknowledge all field teams and camp staff associated with the POLENET‐ANET project and thank Kenn Borek Air and the New York Air Guard for flight support. J. P. O. D., C. K. D., G. A. N., and P. L. W. are supported by the Natural Environment Research Council (Grants NE/L006065/1, NE/L006294/1, and NE/K009958/1). POLENET‐ANET is supported by the National Science Foundation Office of Polar Programs (Grants 0632230, 0632239, 0652322, 0632335, 0632136, 0632209, and 0632185). UKANET seismic instrumentation was provided and supported by SEIS‐UK. POLENET‐ANET seismic instrumentation was provided and supported by the Incorporated Research Institutions for Seismology (IRIS) through the PASSCAL Instrument Center. The UKANET ( www.ukanet.wixsite.com/ukanet ; network code 1D; https://doi.org/10.7914/SN/1D_2016 ) data will be accessible through the IRIS Data Management Center ( http://www.iris.edu/mda ) from January 2021. POLENET‐ANET (network code YT), ASAIN (network code AI), GSN (network code IU), and SEPA (network code XB) seismic data can be accessed through the IRIS DMC. The facilities of the IRIS Consortium are supported by the NSF under cooperative Agreement EAR‐1063471, the NSF Office of Polar Programs, and the DOE National Nuclear Security Administration. Figures were created using the Generic Mapping Tools (GMT) software (Wessel & Smith, ) with color maps from Kovesi ( ) and Crameri ( ). The phase and shear wave velocity models developed here can be accessed at the UK Polar Data Centre, https://doi.org/10.5285/b5ffac8a-9846-4f86-9a71-3ce992a18148 . We thank Simone Pilia and an anonymous reviewer for reviews. Funding Information: We thank all BAS camp staff, field guides, and air unit personnel for the logistical support of the UKANET seismic and GNSS networks. We similarly acknowledge all field teams and camp staff associated with the POLENET-ANET project and thank Kenn Borek Air and the New York Air Guard for flight support. J. P. O. D., C. K. D., G. A. N., and P. L. W. are supported by the Natural Environment Research Council (Grants NE/L006065/1, NE/L006294/1, and NE/K009958/1). POLENET-ANET is supported by the National Science Foundation Office of Polar Programs (Grants 0632230, 0632239, 0652322, 0632335, 0632136, 0632209, and 0632185). UKANET seismic instrumentation was provided and supported by SEIS-UK. POLENET-ANET seismic instrumentation was provided and supported by the Incorporated Research Institutions for Seismology (IRIS) through the PASSCAL Instrument Center. The UKANET (www.ukanet.wixsite.com/ukanet; network code 1D; https://doi.org/10.7914/SN/1D_2016) data will be accessible through the IRIS Data Management Center (http://www.iris.edu/mda) from January 2021. POLENET-ANET (network code YT), ASAIN (network code AI), GSN (network code IU), and SEPA (network code XB) seismic data can be accessed through the IRIS DMC. The facilities of the IRIS Consortium are supported by the NSF under cooperative Agreement EAR-1063471, the NSF Office of Polar Programs, and the DOE National Nuclear Security Administration. Figures were created using the Generic Mapping Tools (GMT) software (Wessel & Smith,) with color maps from Kovesi () and Crameri (). The phase and shear wave velocity models developed here can be accessed at the UK Polar Data Centre, https://doi.org/10.5285/b5ffac8a-9846-4f86-9a71-3ce992a18148. We thank Simone Pilia and an anonymous reviewer for reviews. Publisher Copyright: {\textcopyright}2019. American Geophysical Union. All Rights Reserved.",
year = "2019",
month = nov,
day = "1",
doi = "10.1029/2019GC008459",
language = "English (US)",
volume = "20",
pages = "5014--5037",
journal = "Geochemistry, Geophysics, Geosystems",
issn = "1525-2027",
publisher = "American Geophysical Union",
number = "11",
}