Loading…

Evidence for partial melting and alkali-rich fluids in the crust from a 3-D electrical resistivity model in the vicinity of the Coqen region, western Lhasa terrane, Tibetan Plateau

Both low resistivity zones and low velocity zones are distributed in the middle-lower crust of the western Lhasa terrane, Tibetan Plateau, China. Some estimates from electrical resistivity data suggest large volume fractions of silicate melts that are difficult to reconcile with seismic velocity dat...

Full description

Saved in:
Bibliographic Details
Published in:Earth and planetary science letters 2023-10, Vol.619, p.118316, Article 118316
Main Authors: Sheng, Yue, Jin, Sheng, Comeau, Matthew J., Hou, Zengqian, Becken, Michael, Dong, Hao, Zhang, Letian, Wei, Wenbo, Ye, Gaofeng
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by cdi_FETCH-LOGICAL-a367t-a1bb51229f99dcc0577eb2c943e9bdd1fd794297f51d85f6258d94f256ef71a13
cites cdi_FETCH-LOGICAL-a367t-a1bb51229f99dcc0577eb2c943e9bdd1fd794297f51d85f6258d94f256ef71a13
container_end_page
container_issue
container_start_page 118316
container_title Earth and planetary science letters
container_volume 619
creator Sheng, Yue
Jin, Sheng
Comeau, Matthew J.
Hou, Zengqian
Becken, Michael
Dong, Hao
Zhang, Letian
Wei, Wenbo
Ye, Gaofeng
description Both low resistivity zones and low velocity zones are distributed in the middle-lower crust of the western Lhasa terrane, Tibetan Plateau, China. Some estimates from electrical resistivity data suggest large volume fractions of silicate melts that are difficult to reconcile with seismic velocity data that prefer lower volumes. A second conductive phase, such as saline fluids, that drastically reduces the conductivity but does not significantly affect the seismic velocity because of its low volume may be able to explain these differences. In this study, a 3-D model of the electrical resistivity structure is generated on a profile along longitude 85°E from a latitude of 29°N to 32.5°N. Based on experimental measurement of melts and alkali-rich fluids (e.g., H2O-NaCl), we estimate the volume fraction of each phase that is required to explain the conductive anomalies observed in the geophysical model. The model reveals that the maximum bulk conductivity of the mid-lower crust in the south (1.52 S/m) is much higher than the conductivity of the mid-lower crust in the north (0.18 S/m) when taking 31°N as a rough boundary, near Coqen region. We hypothesize that the conductive zones in the south of the Coqen region may result from a silicate melt and alkali-rich fluid (multicomponent) system. In contrast, partial melting alone can explain the conductive zones in the north. The hypothesis can reconcile the predictions from electrical resistivity data and seismic data, and it corresponds well with zircon Hf isotope data. For example, a combination such as the presence of
doi_str_mv 10.1016/j.epsl.2023.118316
format article
fullrecord <record><control><sourceid>elsevier_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1016_j_epsl_2023_118316</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S0012821X23003291</els_id><sourcerecordid>S0012821X23003291</sourcerecordid><originalsourceid>FETCH-LOGICAL-a367t-a1bb51229f99dcc0577eb2c943e9bdd1fd794297f51d85f6258d94f256ef71a13</originalsourceid><addsrcrecordid>eNp9kNtuEzEQhi0EEqH0BXo1D9ANtjd7sMQNCuUgRaIXReqd5bXHzQTHG2wnVd-rD8guKbdczUH_Nxp9jF0JvhRctB92SzzksJRc1ksh-lq0r9hC1H1TcVHfv2YLzoWseinu37J3Oe84523TqgV7vjmRw2gR_JjgYFIhE2CPoVB8ABMdmPDLBKoS2S34cCSXgSKULYJNx1zAp3EPBurqM2BAW6bgdCFhplzoROUJ9qPD8A86kaU4b0f_d16PvzFO8Qca4zU8Yi6YImy2JhuY2mQiXsMdDVhMhNtgCprje_bGm5Dx8qVesJ9fbu7W36rNj6_f1582lanbrlRGDEMjpFReKWctb7oOB2nVqkY1OCe869RKqs43wvWNb2XTO7XysmnRd8KI-oLJ812bxpwTen1ItDfpSQuuZ-96p2fvevauz94n6OMZwumzE2HS2dJs2FGa9Gg30v_wP1h2j4s</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Evidence for partial melting and alkali-rich fluids in the crust from a 3-D electrical resistivity model in the vicinity of the Coqen region, western Lhasa terrane, Tibetan Plateau</title><source>ScienceDirect Freedom Collection 2022-2024</source><creator>Sheng, Yue ; Jin, Sheng ; Comeau, Matthew J. ; Hou, Zengqian ; Becken, Michael ; Dong, Hao ; Zhang, Letian ; Wei, Wenbo ; Ye, Gaofeng</creator><creatorcontrib>Sheng, Yue ; Jin, Sheng ; Comeau, Matthew J. ; Hou, Zengqian ; Becken, Michael ; Dong, Hao ; Zhang, Letian ; Wei, Wenbo ; Ye, Gaofeng</creatorcontrib><description>Both low resistivity zones and low velocity zones are distributed in the middle-lower crust of the western Lhasa terrane, Tibetan Plateau, China. Some estimates from electrical resistivity data suggest large volume fractions of silicate melts that are difficult to reconcile with seismic velocity data that prefer lower volumes. A second conductive phase, such as saline fluids, that drastically reduces the conductivity but does not significantly affect the seismic velocity because of its low volume may be able to explain these differences. In this study, a 3-D model of the electrical resistivity structure is generated on a profile along longitude 85°E from a latitude of 29°N to 32.5°N. Based on experimental measurement of melts and alkali-rich fluids (e.g., H2O-NaCl), we estimate the volume fraction of each phase that is required to explain the conductive anomalies observed in the geophysical model. The model reveals that the maximum bulk conductivity of the mid-lower crust in the south (1.52 S/m) is much higher than the conductivity of the mid-lower crust in the north (0.18 S/m) when taking 31°N as a rough boundary, near Coqen region. We hypothesize that the conductive zones in the south of the Coqen region may result from a silicate melt and alkali-rich fluid (multicomponent) system. In contrast, partial melting alone can explain the conductive zones in the north. The hypothesis can reconcile the predictions from electrical resistivity data and seismic data, and it corresponds well with zircon Hf isotope data. For example, a combination such as the presence of &lt;1% NaCl-bearing aqueous fluids in addition to 5-10% partial melt can reconcile electrical conductivity data and seismic data. We propose that the contributions from partial melt or saline fluids are controlled by the distinct tectonic dynamics in each region. Furthermore, the model compatible with the idea that the Indian lower crust subducted northwards beneath the Lhasa terrane and may not extend far beyond the Indus-Yarlung Zangbo suture (approximately 30-31°N). The widespread distribution and interconnection of crustal conductors at different depths is consistent with the lateral migration of materials. However, both geophysical data sets agree that some anomalies are discontinuous along the profile. Furthermore, the low-angle subducted Indian Plate with no obvious tearing feature and a low volume of melts may have contributed to the absence of long, continuous, N-S-trending normal faults in this region. •A 3-D conductivity model from a denser MT dataset combining new and old data•Significant conductive feature requires partial melting and alkali-rich fluids•High conductance peaks associated with low-velocity zones in mid-upper crust•The results can reconcile the differences from MT, seismic, and geochemical data•The geophysical anomaly connectivity has important tectonic implications</description><identifier>ISSN: 0012-821X</identifier><identifier>EISSN: 1385-013X</identifier><identifier>DOI: 10.1016/j.epsl.2023.118316</identifier><language>eng</language><publisher>Elsevier B.V</publisher><subject>alkali-rich fluid ; electrical conductivity ; Indian Plate ; Lhasa terrane ; melt fraction</subject><ispartof>Earth and planetary science letters, 2023-10, Vol.619, p.118316, Article 118316</ispartof><rights>2023 The Author(s)</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a367t-a1bb51229f99dcc0577eb2c943e9bdd1fd794297f51d85f6258d94f256ef71a13</citedby><cites>FETCH-LOGICAL-a367t-a1bb51229f99dcc0577eb2c943e9bdd1fd794297f51d85f6258d94f256ef71a13</cites><orcidid>0000-0002-1517-6290 ; 0000-0003-0807-7240 ; 0000-0002-7574-8692</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Sheng, Yue</creatorcontrib><creatorcontrib>Jin, Sheng</creatorcontrib><creatorcontrib>Comeau, Matthew J.</creatorcontrib><creatorcontrib>Hou, Zengqian</creatorcontrib><creatorcontrib>Becken, Michael</creatorcontrib><creatorcontrib>Dong, Hao</creatorcontrib><creatorcontrib>Zhang, Letian</creatorcontrib><creatorcontrib>Wei, Wenbo</creatorcontrib><creatorcontrib>Ye, Gaofeng</creatorcontrib><title>Evidence for partial melting and alkali-rich fluids in the crust from a 3-D electrical resistivity model in the vicinity of the Coqen region, western Lhasa terrane, Tibetan Plateau</title><title>Earth and planetary science letters</title><description>Both low resistivity zones and low velocity zones are distributed in the middle-lower crust of the western Lhasa terrane, Tibetan Plateau, China. Some estimates from electrical resistivity data suggest large volume fractions of silicate melts that are difficult to reconcile with seismic velocity data that prefer lower volumes. A second conductive phase, such as saline fluids, that drastically reduces the conductivity but does not significantly affect the seismic velocity because of its low volume may be able to explain these differences. In this study, a 3-D model of the electrical resistivity structure is generated on a profile along longitude 85°E from a latitude of 29°N to 32.5°N. Based on experimental measurement of melts and alkali-rich fluids (e.g., H2O-NaCl), we estimate the volume fraction of each phase that is required to explain the conductive anomalies observed in the geophysical model. The model reveals that the maximum bulk conductivity of the mid-lower crust in the south (1.52 S/m) is much higher than the conductivity of the mid-lower crust in the north (0.18 S/m) when taking 31°N as a rough boundary, near Coqen region. We hypothesize that the conductive zones in the south of the Coqen region may result from a silicate melt and alkali-rich fluid (multicomponent) system. In contrast, partial melting alone can explain the conductive zones in the north. The hypothesis can reconcile the predictions from electrical resistivity data and seismic data, and it corresponds well with zircon Hf isotope data. For example, a combination such as the presence of &lt;1% NaCl-bearing aqueous fluids in addition to 5-10% partial melt can reconcile electrical conductivity data and seismic data. We propose that the contributions from partial melt or saline fluids are controlled by the distinct tectonic dynamics in each region. Furthermore, the model compatible with the idea that the Indian lower crust subducted northwards beneath the Lhasa terrane and may not extend far beyond the Indus-Yarlung Zangbo suture (approximately 30-31°N). The widespread distribution and interconnection of crustal conductors at different depths is consistent with the lateral migration of materials. However, both geophysical data sets agree that some anomalies are discontinuous along the profile. Furthermore, the low-angle subducted Indian Plate with no obvious tearing feature and a low volume of melts may have contributed to the absence of long, continuous, N-S-trending normal faults in this region. •A 3-D conductivity model from a denser MT dataset combining new and old data•Significant conductive feature requires partial melting and alkali-rich fluids•High conductance peaks associated with low-velocity zones in mid-upper crust•The results can reconcile the differences from MT, seismic, and geochemical data•The geophysical anomaly connectivity has important tectonic implications</description><subject>alkali-rich fluid</subject><subject>electrical conductivity</subject><subject>Indian Plate</subject><subject>Lhasa terrane</subject><subject>melt fraction</subject><issn>0012-821X</issn><issn>1385-013X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNp9kNtuEzEQhi0EEqH0BXo1D9ANtjd7sMQNCuUgRaIXReqd5bXHzQTHG2wnVd-rD8guKbdczUH_Nxp9jF0JvhRctB92SzzksJRc1ksh-lq0r9hC1H1TcVHfv2YLzoWseinu37J3Oe84523TqgV7vjmRw2gR_JjgYFIhE2CPoVB8ABMdmPDLBKoS2S34cCSXgSKULYJNx1zAp3EPBurqM2BAW6bgdCFhplzoROUJ9qPD8A86kaU4b0f_d16PvzFO8Qca4zU8Yi6YImy2JhuY2mQiXsMdDVhMhNtgCprje_bGm5Dx8qVesJ9fbu7W36rNj6_f1582lanbrlRGDEMjpFReKWctb7oOB2nVqkY1OCe869RKqs43wvWNb2XTO7XysmnRd8KI-oLJ812bxpwTen1ItDfpSQuuZ-96p2fvevauz94n6OMZwumzE2HS2dJs2FGa9Gg30v_wP1h2j4s</recordid><startdate>202310</startdate><enddate>202310</enddate><creator>Sheng, Yue</creator><creator>Jin, Sheng</creator><creator>Comeau, Matthew J.</creator><creator>Hou, Zengqian</creator><creator>Becken, Michael</creator><creator>Dong, Hao</creator><creator>Zhang, Letian</creator><creator>Wei, Wenbo</creator><creator>Ye, Gaofeng</creator><general>Elsevier B.V</general><scope>6I.</scope><scope>AAFTH</scope><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-1517-6290</orcidid><orcidid>https://orcid.org/0000-0003-0807-7240</orcidid><orcidid>https://orcid.org/0000-0002-7574-8692</orcidid></search><sort><creationdate>202310</creationdate><title>Evidence for partial melting and alkali-rich fluids in the crust from a 3-D electrical resistivity model in the vicinity of the Coqen region, western Lhasa terrane, Tibetan Plateau</title><author>Sheng, Yue ; Jin, Sheng ; Comeau, Matthew J. ; Hou, Zengqian ; Becken, Michael ; Dong, Hao ; Zhang, Letian ; Wei, Wenbo ; Ye, Gaofeng</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a367t-a1bb51229f99dcc0577eb2c943e9bdd1fd794297f51d85f6258d94f256ef71a13</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>alkali-rich fluid</topic><topic>electrical conductivity</topic><topic>Indian Plate</topic><topic>Lhasa terrane</topic><topic>melt fraction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Sheng, Yue</creatorcontrib><creatorcontrib>Jin, Sheng</creatorcontrib><creatorcontrib>Comeau, Matthew J.</creatorcontrib><creatorcontrib>Hou, Zengqian</creatorcontrib><creatorcontrib>Becken, Michael</creatorcontrib><creatorcontrib>Dong, Hao</creatorcontrib><creatorcontrib>Zhang, Letian</creatorcontrib><creatorcontrib>Wei, Wenbo</creatorcontrib><creatorcontrib>Ye, Gaofeng</creatorcontrib><collection>ScienceDirect Open Access Titles</collection><collection>Elsevier:ScienceDirect:Open Access</collection><collection>CrossRef</collection><jtitle>Earth and planetary science letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sheng, Yue</au><au>Jin, Sheng</au><au>Comeau, Matthew J.</au><au>Hou, Zengqian</au><au>Becken, Michael</au><au>Dong, Hao</au><au>Zhang, Letian</au><au>Wei, Wenbo</au><au>Ye, Gaofeng</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Evidence for partial melting and alkali-rich fluids in the crust from a 3-D electrical resistivity model in the vicinity of the Coqen region, western Lhasa terrane, Tibetan Plateau</atitle><jtitle>Earth and planetary science letters</jtitle><date>2023-10</date><risdate>2023</risdate><volume>619</volume><spage>118316</spage><pages>118316-</pages><artnum>118316</artnum><issn>0012-821X</issn><eissn>1385-013X</eissn><abstract>Both low resistivity zones and low velocity zones are distributed in the middle-lower crust of the western Lhasa terrane, Tibetan Plateau, China. Some estimates from electrical resistivity data suggest large volume fractions of silicate melts that are difficult to reconcile with seismic velocity data that prefer lower volumes. A second conductive phase, such as saline fluids, that drastically reduces the conductivity but does not significantly affect the seismic velocity because of its low volume may be able to explain these differences. In this study, a 3-D model of the electrical resistivity structure is generated on a profile along longitude 85°E from a latitude of 29°N to 32.5°N. Based on experimental measurement of melts and alkali-rich fluids (e.g., H2O-NaCl), we estimate the volume fraction of each phase that is required to explain the conductive anomalies observed in the geophysical model. The model reveals that the maximum bulk conductivity of the mid-lower crust in the south (1.52 S/m) is much higher than the conductivity of the mid-lower crust in the north (0.18 S/m) when taking 31°N as a rough boundary, near Coqen region. We hypothesize that the conductive zones in the south of the Coqen region may result from a silicate melt and alkali-rich fluid (multicomponent) system. In contrast, partial melting alone can explain the conductive zones in the north. The hypothesis can reconcile the predictions from electrical resistivity data and seismic data, and it corresponds well with zircon Hf isotope data. For example, a combination such as the presence of &lt;1% NaCl-bearing aqueous fluids in addition to 5-10% partial melt can reconcile electrical conductivity data and seismic data. We propose that the contributions from partial melt or saline fluids are controlled by the distinct tectonic dynamics in each region. Furthermore, the model compatible with the idea that the Indian lower crust subducted northwards beneath the Lhasa terrane and may not extend far beyond the Indus-Yarlung Zangbo suture (approximately 30-31°N). The widespread distribution and interconnection of crustal conductors at different depths is consistent with the lateral migration of materials. However, both geophysical data sets agree that some anomalies are discontinuous along the profile. Furthermore, the low-angle subducted Indian Plate with no obvious tearing feature and a low volume of melts may have contributed to the absence of long, continuous, N-S-trending normal faults in this region. •A 3-D conductivity model from a denser MT dataset combining new and old data•Significant conductive feature requires partial melting and alkali-rich fluids•High conductance peaks associated with low-velocity zones in mid-upper crust•The results can reconcile the differences from MT, seismic, and geochemical data•The geophysical anomaly connectivity has important tectonic implications</abstract><pub>Elsevier B.V</pub><doi>10.1016/j.epsl.2023.118316</doi><orcidid>https://orcid.org/0000-0002-1517-6290</orcidid><orcidid>https://orcid.org/0000-0003-0807-7240</orcidid><orcidid>https://orcid.org/0000-0002-7574-8692</orcidid><oa>free_for_read</oa></addata></record>
fulltext fulltext
identifier ISSN: 0012-821X
ispartof Earth and planetary science letters, 2023-10, Vol.619, p.118316, Article 118316
issn 0012-821X
1385-013X
language eng
recordid cdi_crossref_primary_10_1016_j_epsl_2023_118316
source ScienceDirect Freedom Collection 2022-2024
subjects alkali-rich fluid
electrical conductivity
Indian Plate
Lhasa terrane
melt fraction
title Evidence for partial melting and alkali-rich fluids in the crust from a 3-D electrical resistivity model in the vicinity of the Coqen region, western Lhasa terrane, Tibetan Plateau
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-01T09%3A27%3A25IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-elsevier_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Evidence%20for%20partial%20melting%20and%20alkali-rich%20fluids%20in%20the%20crust%20from%20a%203-D%20electrical%20resistivity%20model%20in%20the%20vicinity%20of%20the%20Coqen%20region,%20western%20Lhasa%20terrane,%20Tibetan%20Plateau&rft.jtitle=Earth%20and%20planetary%20science%20letters&rft.au=Sheng,%20Yue&rft.date=2023-10&rft.volume=619&rft.spage=118316&rft.pages=118316-&rft.artnum=118316&rft.issn=0012-821X&rft.eissn=1385-013X&rft_id=info:doi/10.1016/j.epsl.2023.118316&rft_dat=%3Celsevier_cross%3ES0012821X23003291%3C/elsevier_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-a367t-a1bb51229f99dcc0577eb2c943e9bdd1fd794297f51d85f6258d94f256ef71a13%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true