{"id":3162,"date":"2024-09-25T07:33:09","date_gmt":"2024-09-25T14:33:09","guid":{"rendered":"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/?page_id=3162"},"modified":"2024-09-25T07:37:49","modified_gmt":"2024-09-25T14:37:49","slug":"crustal-seismic-anisotropy-under-the-lander","status":"publish","type":"page","link":"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/crustal-seismic-anisotropy-under-the-lander\/","title":{"rendered":"Crustal Seismic Anisotropy Under the Lander"},"content":{"rendered":"<p style=\"font-weight: 400;\">With postdoctoral researcher Dr. Jiaqi Li, we modeled SH wave travel times and found that the SH-wave speed in the top 8 km of the crust under the lander is systematically lower than the vertically polarized shear (SV) wave speed previously obtained from receiver functions (e.g. Knapmeyer-Endrun et al., 2021). We interpreted this difference in wave speed with the wave direction of polarization as the <strong>signature of seismic anisotropy under the lander<\/strong>.<\/p>\n<figure id=\"attachment_3167\" aria-describedby=\"caption-attachment-3167\" style=\"width: 2560px\" class=\"wp-caption aligncenter\"><img fetchpriority=\"high\" decoding=\"async\" class=\"wp-image-3167 size-full\" src=\"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-content\/uploads\/2024\/09\/1-s2.0-S0012821X22002904-gr005_lrg-scaled.jpg\" alt=\"S-wave speed models for Layer 1.\" width=\"2560\" height=\"756\" srcset=\"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-content\/uploads\/2024\/09\/1-s2.0-S0012821X22002904-gr005_lrg-scaled.jpg 2560w, https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-content\/uploads\/2024\/09\/1-s2.0-S0012821X22002904-gr005_lrg-300x89.jpg 300w, https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-content\/uploads\/2024\/09\/1-s2.0-S0012821X22002904-gr005_lrg-1024x303.jpg 1024w, https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-content\/uploads\/2024\/09\/1-s2.0-S0012821X22002904-gr005_lrg-2000x591.jpg 2000w\" sizes=\"(max-width: 2560px) 100vw, 2560px\" \/><figcaption id=\"caption-attachment-3167\" class=\"wp-caption-text\">S-wave speed models for Layer 1. (a) The average cross-correlation map for the SH-wave reflections. The black and grey curves mark the acceptable model regions with loose and strict thresholds, respectively. (b) Colored dots represent the 20,000 models from the receiver functions study (Knapmeyer-Endrun et al., 2021) for the 2-layer crustal case. Color indicates the number of models at each grid point. (c) Same as (b) for the 3-layer crustal case.<\/figcaption><\/figure>\n<p style=\"font-weight: 400;\">Seismic anisotropy in the crust is usually attributed to the layering of material with contrasting elastic properties, such as the presence and preferred alignment of melt pockets or the distribution of fluid-filled cracks, microcracks, or preferentially oriented pore spaces. Through modeling, we showed that <strong>dry or liquid-filled cracks\/fractures and igneous intrusions can reproduce the observed amplitude and sign <\/strong>(i.e. an anisotropy coefficient \ud835\udf09=(\ud835\udc49<sub>\ud835\udc46\ud835\udc3b<\/sub>\/\ud835\udc49<sub>\ud835\udc46\ud835\udc49<\/sub>)<sup>2<\/sup>\u00a0between 0.7 and 0.9)<strong>, giving new insight on the structure of the crust under the lander<\/strong>.<\/p>\n<p style=\"font-weight: 400;\">Li, J.,<strong>\u00a0Beghein, C.,<\/strong>\u00a0Wookey, J., Davis, P., Lognonn\u00e9, P., Schimmel, M., Stutzmann, E., Golombek, M., Montagner, J.-P., and Banerdt, W. (2022), Evidence for Crustal Seismic Anisotropy at the InSight Lander Site,\u00a0<em>Earth Planet. Sc. Lett.,\u00a0<\/em><strong>593<\/strong>, 117654, doi:\u00a010.1016\/j.epsl.2022.117654.<\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>With postdoctoral researcher Dr. Jiaqi Li, we modeled SH wave travel times and found that the SH-wave speed in the top 8 km of the crust under the lander is systematically lower than the vertically polarized shear (SV) wave speed previously obtained from receiver functions (e.g. Knapmeyer-Endrun et al., 2021). We interpreted this difference in &hellip; <\/p>\n<p class=\"link-more\"><a href=\"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/crustal-seismic-anisotropy-under-the-lander\/\" class=\"more-link\">Read more<span class=\"screen-reader-text\"> &#8220;Crustal Seismic Anisotropy Under the Lander&#8221;<\/span><\/a><\/p>\n","protected":false},"author":2,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"inspiro_hide_title":false,"footnotes":""},"class_list":["post-3162","page","type-page","status-publish","hentry"],"jetpack_sharing_enabled":true,"featured_media_urls":[],"_links":{"self":[{"href":"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-json\/wp\/v2\/pages\/3162","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-json\/wp\/v2\/comments?post=3162"}],"version-history":[{"count":4,"href":"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-json\/wp\/v2\/pages\/3162\/revisions"}],"predecessor-version":[{"id":3168,"href":"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-json\/wp\/v2\/pages\/3162\/revisions\/3168"}],"wp:attachment":[{"href":"https:\/\/faculty.epss.ucla.edu\/~cbeghein\/wp-json\/wp\/v2\/media?parent=3162"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}