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<article xsi:noNamespaceSchemaLocation="http://jats.nlm.nih.gov/publishing/1.1/xsd/JATS-journalpublishing1-mathml3.xsd" dtd-version="1.1" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"><front><journal-meta><journal-id journal-id-type="publisher-id">JSE</journal-id><journal-title-group><journal-title>Journal of Seismic Exploration</journal-title></journal-title-group><issn>0963-0651</issn><eissn/><publisher><publisher-name>AccScience Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi"/><article-categories><subj-group subj-group-type="heading"><subject>Article</subject></subj-group></article-categories><title>3D isotropic elastic reverse time migration using signed magnitudes of elastic data components</title><url>https://geophysical-press.com/journal/JSE/articles/152</url><author>WANGWENLONG,A. MCMECHANGEORGE</author><pub-date pub-type="publication-year"><year>2019</year></pub-date><volume>28</volume><issue>3</issue><history><date date-type="pub"><published-time>2019-06-01</published-time></date></history><abstract>Wang, W. and McMechan, G.A., 2019. 3D isotropic elastic reverse time migration using signed magnitudes of elastic data components. Journal of Seismic Exploration, 28: 221-244. Elastic reverse time migration (ERTM) is capable of characterizing subsurface properties more completely than its acoustic counterpart. P- and S-waves coexist in elastic wavefields, and their separation is required before, or as part of, applying the image conditions. Traditional P- and S-wave separation methods based on divergence and curl operators don't preserve the elastic vector information, and the associated polarity reversals of S-wave images are difficult to handle. Thus a preferable workflow for isotropic ERTM should include a vector decomposition of the elastic wavefields and a vector-based image condition that directly uses the signed magnitudes of the decomposed vector wavefields to produce PP and PS images. We propose a new 3D elastic image condition which is a source-normalized crosscorrelation of the signed magnitudes of the decomposed wavefields. The image condition is robust and stable for generating 3D PP and PS images and their corresponding angle domain common-image gathers (ADCIGs) with incident angles calculated from Poynting vectors. Comparisons between the proposed image condition and a vector-based dot-product image condition and show that the proposed image condition generates PP ADCIGs with a wider range of incident angles than existing dot-product image conditions.</abstract><keywords>3D, RTM, elastic, image condition</keywords></article-meta></front><body/><back><ref-list><ref id="B1" content-type="article"><label>1</label><element-citation publication-type="journal"><p>Aki, K. and Richards, P.G., 1980. Quantitative Seismology, Theory and Methods. W.H.Freeman and Co., Sausalito.Aminzadeh, F., Burkhard, N., Nicoletis, L., Rocca, F. and Wyatt, K., 1994. SEG/EAGE_ 3-D modeling project: 2nd update. The Leading Edge, 13: 949-952.Cerveny, V., 2001. Seismic Ray Theory. Cambridge University Press, Cambridge.Chang, W. and McMechan, G.A., 1986. Reverse-time migration of offset verticalseismic profiling data using the excitation-time imaging condition. 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