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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Earth Sci.</journal-id>
<journal-title>Frontiers in Earth Science</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Earth Sci.</abbrev-journal-title>
<issn pub-type="epub">2296-6463</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">887632</article-id>
<article-id pub-id-type="doi">10.3389/feart.2022.887632</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Earth Science</subject>
<subj-group>
<subject>Mini Review</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Late Permian to Late Triassic Large Igneous Provinces: Timing, Eruptive Style and Paleoenvironmental Perturbations</article-title>
<alt-title alt-title-type="left-running-head">Boscaini et al.</alt-title>
<alt-title alt-title-type="right-running-head">Triassic Large Igneous Provinces</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Boscaini</surname>
<given-names>Andrea</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1703282/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Callegaro</surname>
<given-names>Sara</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1359532/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Sun</surname>
<given-names>Yadong</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Marzoli</surname>
<given-names>Andrea</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/131437/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Dipartimento di Geoscienze</institution>, <institution>Universit&#xe0; di Padova</institution>, <addr-line>Padova</addr-line>, <country>Italy</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Centre for Earth Evolution and Dynamics</institution>, <institution>University of Oslo</institution>, <addr-line>Oslo</addr-line>, <country>Norway</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>GeoZentrum Nordbayern, Universit&#xe4;t Erlangen-Nurnberg</institution>, <addr-line>Erlangen</addr-line>, <country>Germany</country>
</aff>
<aff id="aff4">
<sup>4</sup>
<institution>Dipartimento Territorio e Sistemi Agro-Forestali</institution>, <institution>Universit&#xe0; di Padova</institution>, <addr-line>Legnaro</addr-line>, <country>Italy</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/268636/overview">Hossein Azizi</ext-link>, University of Kurdistan, Iran</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1707777/overview">Federico Lucci</ext-link>, University of Bari Aldo Moro, Italy</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1707376/overview">Orhan Karsli</ext-link>, Karadeniz Technical University, Turkey</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Andrea Marzoli, <email>andrea.marzoli@unipd.it</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Petrology, a section of the journal Frontiers in Earth Science</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>12</day>
<month>04</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>10</volume>
<elocation-id>887632</elocation-id>
<history>
<date date-type="received">
<day>01</day>
<month>03</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>23</day>
<month>03</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Boscaini, Callegaro, Sun and Marzoli.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Boscaini, Callegaro, Sun and Marzoli</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>The emplacement of the Siberian Traps, the Central Atlantic Magmatic Province (CAMP) and the Wrangellia have been linked to the end-Permian, the end-Triassic mass extinctions, and to the Carnian Pluvial Episode (CPE), respectively. Exploring the timing, eruptive styles, and volatile degassing of these Large Igneous Provinces (LIPs) is crucial to understand their causal link to the catastrophic environmental crises that punctuated the Triassic. In this study we review the main characteristics of these LIPs, emphasizing common features and differences, and discussing aspects that are still in debate. Estimates of CO<sub>2</sub> budgets and emissions from the three LIPs are based on the Nb content of little evolved basalts and highlight that early Siberian Traps and CAMP and high-Ti Wrangellia volcanics were quite CO<sub>2</sub>-rich. On the contrary, other volcanics from the three LIPs probably emitted relatively low amounts of CO<sub>2</sub>, which reinforces the possibility that thermogenic reactions between sills and sediments were additional fundamental suppliers of climate-modifying gases.</p>
</abstract>
<kwd-group>
<kwd>triassic</kwd>
<kwd>siberian traps</kwd>
<kwd>central atlantic magmatic province (CAMP)</kwd>
<kwd>carnian crisis</kwd>
<kwd>wrangellia LIP</kwd>
<kwd>large igneous province</kwd>
<kwd>mass extinction</kwd>
</kwd-group>
<contract-sponsor id="cn001">Ministero Dell&#x27;Universit&#xe0; e Della Ricerca<named-content content-type="fundref-id">10.13039/501100021856</named-content>
</contract-sponsor>
</article-meta>
</front>
<body>
<sec id="s1">
<title>Introduction</title>
<p>The Triassic was a crucial period for shaping the modern world, in terms of the evolution of both the biosphere and the geosphere. While successful faunas and floras spread over Pangea, in the Panthalassa and Tethys oceans, the Triassic biosphere was devastated by two extreme extinctions at its dawn (ca. 252&#xa0;Ma) and its end (ca. 201&#xa0;Ma) and by a combined extinction and significant radiation episode at ca. 232&#xa0;Ma, during the Carnian (e.g., <xref ref-type="bibr" rid="B73">Tanner et al., 2004</xref>; <xref ref-type="bibr" rid="B69">Song et al., 2013</xref>; <xref ref-type="bibr" rid="B3">Bernardi et al., 2018</xref>; <xref ref-type="bibr" rid="B20">Dal Corso et al., 2020</xref>, <xref ref-type="bibr" rid="B21">2022</xref>; <xref ref-type="bibr" rid="B76">Wignall and Atkinson 2020</xref>). The three main biocrises coincided with the emplacement of three Large Igneous Provinces (LIPs), namely, the Siberian Traps, the Central Atlantic Magmatic Province (CAMP), and the Wrangellia (<xref ref-type="fig" rid="F1">Figure 1</xref>). In this article, we review the main features of these LIPs, with a focus on their timing, emplacement styles, and CO<sub>2</sub> budgets. This is followed by an in-depth discussion of their critical roles in the Triassic environmental crises.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Simplified sketches of <bold>(A)</bold> the Siberian Traps (modified after <xref ref-type="bibr" rid="B71">Svensen et al., 2018</xref>) <bold>(B)</bold> the Wrangellia (modified after <xref ref-type="bibr" rid="B44">Lassiter et al., 1995</xref>), and <bold>(C)</bold> the CAMP (modified after <xref ref-type="bibr" rid="B17">Capriolo et al., 2020</xref>). <bold>(C)</bold> Coloured lines represent the geographic distribution of the six geochemical groups of the CAMP magmas identified by <xref ref-type="bibr" rid="B49">Marzoli et al. (2018)</xref>: P&#x3d;Prevalent, HTi&#x3d;high-Ti, T&#x3d;Tiourjdal, R&#x3d;Recurrent, C&#x3d;Carolina, H&#x3d;Holyoke.</p>
</caption>
<graphic xlink:href="feart-10-887632-g001.tif"/>
</fig>
</sec>
<sec id="s2">
<title>Continental Large Igneous Provinces: The Siberian Traps and the CAMP</title>
<p>High-precision geochronology proves that the main activity of the Siberian Traps and the CAMP (main pulses at 252.3&#x2013;251.4&#xa0;Ma and 201.6&#x2013;201.0&#xa0;Ma, respectively; for the Siberian Traps: <xref ref-type="bibr" rid="B40">Kamo et al., 2003</xref>; <xref ref-type="bibr" rid="B9">Burgess and Bowring, 2015</xref>; <xref ref-type="bibr" rid="B11">Burgess et al., 2017</xref>; <xref ref-type="bibr" rid="B1">Augland et al., 2019</xref>; for the CAMP: <xref ref-type="bibr" rid="B6">Blackburn et al., 2013</xref>; <xref ref-type="bibr" rid="B24">Davies et al., 2017</xref>, <xref ref-type="bibr" rid="B23">2021</xref>; <xref ref-type="bibr" rid="B48">Marzoli et al., 2019</xref>) spanned the end-Permian and end-Triassic extinction intervals, respectively (251.94&#x2013;251.88&#xa0;Ma and 201.51&#x2013;201.36&#xa0;Ma; <xref ref-type="bibr" rid="B61">Schoene et al., 2010</xref>; <xref ref-type="bibr" rid="B10">Burgess et al., 2014</xref>; <xref ref-type="bibr" rid="B77">Wotzlaw et al., 2014</xref>). The pulsed nature of these LIPs was inferred from magnetostratigraphy and biostratigraphy (e.g., <xref ref-type="bibr" rid="B42">Knight et al., 2004</xref>; <xref ref-type="bibr" rid="B54">Panfili et al., 2019</xref>; <xref ref-type="bibr" rid="B45">Latyshev et al., 2020</xref>), yielding eruption rates possibly two orders of magnitude greater than the most voluminous present-day eruptions, such as those at Hawai&#x2019;i (e.g., <xref ref-type="bibr" rid="B55">Patrick et al., 2020</xref>). The Siberian Traps and the CAMP are among the most voluminous known LIPs (both ca. 3 &#xb1; 1 million km<sup>3</sup>; <xref ref-type="bibr" rid="B60">Saunders and Reichow, 2009</xref>; <xref ref-type="bibr" rid="B49">Marzoli et al., 2018</xref>), although a precise estimate of the original and preserved magma volume remains challenging. Large parts of the Siberian Traps are intrusive, subaerial, and huge volumes of volcanics were likely removed by erosion. The best-studied part of the province is on the Siberian Craton, at a paleolatitude of ca. 50&#x2013;60&#xb0;N, over an area of ca. 2.5 million km<sup>2</sup> (<xref ref-type="fig" rid="F1">Figure 1A</xref>). The CAMP was emplaced over 10 million km<sup>2</sup> straddling the equator, and has been similarly partly eroded away, as demonstrated by the sparsely preserved lava piles (<xref ref-type="fig" rid="F1">Figure 1C</xref>).</p>
<p>The first emplacement stage of the Siberian Traps started shortly before 252.24 &#xb1; 0.12&#xa0;Ma with initial pyroclastic eruptions followed by effusive activity emplaced in ca 0.30&#xa0;Ma. From 251.91 &#xb1; 0.07&#xa0;Ma, the extrusive activity waned and shifted to dominantly intrusive for ca. 0.40&#xa0;Ma, building the vast network of sills in the Tunguska Basin. These tholeiitic magmas were produced by shallower and extensive melting of a mixed peridotitic-pyroxenitic mantle (<xref ref-type="bibr" rid="B68">Sobolev et al., 2011</xref>; <xref ref-type="bibr" rid="B15">Callegaro et al., 2021</xref>). Renewed extrusive activity is recognized from 251.48 &#xb1; 0.09&#xa0;Ma, marking the beginning of the third phase of the Siberian Traps. During this phase, tholeiitic extrusive and intrusive activities were accompanied by mafic to felsic alkaline intrusions in Maymecha-Kotuy and Taimyr areas (<xref ref-type="bibr" rid="B29">Elkins-Tanton et al., 2007</xref>; <xref ref-type="bibr" rid="B67">Sobolev et al., 2009</xref>; <xref ref-type="bibr" rid="B1">Augland et al., 2019</xref>). Alkaline melts were produced from a deep (5.5&#xa0;GPa) and volatile-rich (carbonated) mantle source (<xref ref-type="bibr" rid="B29">Elkins-Tanton et al., 2007</xref>). The youngest sill dated in Tunguska (251.35 &#xb1; 0.09&#xa0;Ma; <xref ref-type="bibr" rid="B9">Burgess and Bowring, 2015</xref>), and the Guli carbonatitic complex in the Maymecha-Kotuy region (250.20 &#xb1; 0.30&#xa0;Ma; <xref ref-type="bibr" rid="B40">Kamo et al., 2003</xref>) represent the youngest known Siberian Traps products.</p>
<p>The beginning of the second (intrusive) phase is considered as the deadly subinterval of the Siberian Traps (<xref ref-type="bibr" rid="B11">Burgess et al., 2017</xref>), since it coincides with the beginning of the extinction horizon at Meishan (251.94 &#xb1; 0.04&#xa0;Ma; <xref ref-type="bibr" rid="B10">Burgess et al., 2014</xref>), Dongpan and Penglaitan (251.94 &#xb1; 0.03&#xa0;Ma and 251.98 &#xb1; 0.03&#xa0;Ma; <xref ref-type="bibr" rid="B2">Baresel et al., 2017</xref>), China. Even if these tholeiitic magmas were probably volatile poor (<xref ref-type="bibr" rid="B64">Sibik et al., 2015</xref>), the interaction between the sills and the sedimentary host-rocks (i.e., evaporites, carbonates, marlstones, and coal) likely produced large amounts of thermogenic carbon, sulfur and halocarbon species (<xref ref-type="bibr" rid="B71">Svensen et al., 2018</xref>; <xref ref-type="bibr" rid="B15">Callegaro et al., 2021</xref>; <xref ref-type="bibr" rid="B65">Sibik et al., 2021</xref>).</p>
<p>The end of the Triassic witnessed the emplacement of the CAMP mainly between 201.64 &#xb1; 0.03&#xa0;Ma and 201.36 &#xb1; 0.02&#xa0;Ma (<xref ref-type="bibr" rid="B6">Blackburn et al., 2013</xref>; <xref ref-type="bibr" rid="B24">Davies et al., 2017</xref>, <xref ref-type="bibr" rid="B23">2021</xref>; <xref ref-type="bibr" rid="B48">Marzoli et al., 2019</xref>), coincident with the main end-Triassic extinction interval (201.51 &#xb1; 0.15 to 201.36 &#xb1; 0.15&#xa0;Ma; <xref ref-type="bibr" rid="B61">Schoene et al., 2010</xref>; <xref ref-type="bibr" rid="B77">Wotzlaw et al., 2014</xref>). Basaltic magmas erupted as short-lived pulses (<xref ref-type="bibr" rid="B42">Knight et al., 2004</xref>; <xref ref-type="bibr" rid="B48">Marzoli et al., 2019</xref>) during this magmatic phase have been shown to be rich in CO<sub>2</sub> and SO<sub>2</sub> (<xref ref-type="bibr" rid="B12">Callegaro et al., 2014a</xref>; <xref ref-type="bibr" rid="B17">Capriolo et al., 2020</xref>) and possibly triggered the dramatic increase in CO<sub>2</sub>, the rise of temperature and the climatic perturbations heralding the end of the Triassic (<xref ref-type="bibr" rid="B43">Landwehrs et al., 2020</xref>; <xref ref-type="bibr" rid="B46">Lindstr&#xf6;m et al., 2021</xref>; <xref ref-type="bibr" rid="B18">Capriolo et al., 2022</xref>). Later erupted magmas, for example, in North America and Africa (Holyoke and Recurrent groups; <xref ref-type="bibr" rid="B6">Blackburn et al., 2013</xref>; <xref ref-type="bibr" rid="B49">Marzoli et al., 2018</xref>, <xref ref-type="bibr" rid="B48">2019</xref>) appear to be less voluminous and possibly had limited environmental effects.</p>
<p>Similar to the Siberian Traps, CAMP magmas are mainly preserved as large sills intruding Paleozoic terrestrial sediments in South America and North-western Africa, and Triassic terrestrial sediments in North America and Europe (<xref ref-type="bibr" rid="B49">Marzoli et al., 2018</xref> and references therein). The CAMP basalts mobilized large amounts of organic carbon and possibly halogens from evaporitic deposits (<xref ref-type="bibr" rid="B36">Heimdal et al., 2018</xref>, <xref ref-type="bibr" rid="B35">2019</xref>; <xref ref-type="bibr" rid="B16">Capriolo et al., 2021</xref>). Available geochronological data indicate that some CAMP intrusions are older than the preserved (and dated) erupted basalts (<xref ref-type="bibr" rid="B24">Davies et al., 2017</xref>). However, the intrusion of sills in Amazonia and north-western Africa seems to be relatively prolonged from ca. 201.53 &#xb1; 0.07&#xa0;Ma to ca. 201.35 &#xb1; 0.03&#xa0;Ma (<xref ref-type="bibr" rid="B24">Davies et al., 2017</xref>, <xref ref-type="bibr" rid="B23">2021</xref>), i.e., spanning the entire end-Triassic extinction interval (<xref ref-type="bibr" rid="B61">Schoene et al., 2010</xref>). However, it is still unclear whether CAMP intrusions occurred in pulses, thus emitting thermogenic volatiles at high rates, and playing a catastrophic role in the end-Triassic crisis.</p>
<p>Unlike the Siberian Traps, CAMP magmas are relatively uniform in composition, mainly being tholeiitic basalts. Whether such relatively high degree mantle melts originated from the deep or shallow mantle is still disputed (e.g., <xref ref-type="bibr" rid="B59">Ruiz-Martinez et al., 2012</xref>; <xref ref-type="bibr" rid="B74">Tegner et al., 2019</xref>; <xref ref-type="bibr" rid="B7">Boscaini et al., 2022</xref>). CAMP basalts lack geochemical signatures of a mantle plume originating from the deep mantle but show a subduction signature, which is best interpreted as reflecting the presence of recycled subducted continental rocks (sediments, mainly; <xref ref-type="bibr" rid="B13">Callegaro et al., 2013</xref>; <xref ref-type="bibr" rid="B52">Merle et al., 2014</xref>; <xref ref-type="bibr" rid="B63">Shellnutt et al., 2018</xref>; <xref ref-type="bibr" rid="B48">Marzoli et al., 2019</xref>). The absence of alkaline mafic rocks or carbonatites in the CAMP calls against a significant contribution from particularly CO<sub>2</sub>-rich metasomatized mantle portions. In contrast to the Siberian Traps, evidence for explosive volcanic activity is rare for the CAMP, whose lavas are mostly compound pahoehoe flows (e.g., <xref ref-type="bibr" rid="B28">El Hacimi et al., 2011</xref>) and therefore occurred as fissure eruptions like the historical Laki eruption in Iceland.</p>
<sec id="s2-1">
<title>Oceanic Large Igneous Province: The Wrangellia</title>
<p>The Wrangellia LIP presently crops out along the north-western margin of North America (<xref ref-type="fig" rid="F1">Figure 1B</xref>). It represents one of the best-preserved accreted oceanic plateaus on Earth, which contrast starkly with continental LIPs in terms of mantle processes, emplacement style and, possibly, environmental implications (<xref ref-type="bibr" rid="B41">Kerr, 2005</xref>).</p>
<p>The origin of the Wrangellia tholeiitic basalts has been attributed to deep mantle processes (i.e., mantle plume; <xref ref-type="bibr" rid="B56">Richards et al., 1991</xref>; <xref ref-type="bibr" rid="B44">Lassiter et al., 1995</xref>; <xref ref-type="bibr" rid="B31">Greene et al., 2009a</xref>; <xref ref-type="bibr" rid="B33">Greene et al., 2009b</xref>; <xref ref-type="bibr" rid="B62">Shellnutt et al., 2021</xref>). The early emplaced low-Ti basalts (0.4&#x2013;1.2 TiO<sub>2</sub> wt%) were probably sourced from partial melting of a rising mantle plume and show a significant contribution from the subduction-modified lithospheric mantle (<xref ref-type="bibr" rid="B31">Greene et al., 2009a</xref>; <xref ref-type="bibr" rid="B33">Greene et al., 2009b</xref>). Conversely, the later high-Ti basalts (1.4&#x2013;2.4 TiO<sub>2</sub> wt%) were sourced chiefly from the mantle plume (<xref ref-type="bibr" rid="B31">Greene et al., 2009a</xref>; <xref ref-type="bibr" rid="B33">Greene et al., 2009b</xref>).</p>
<p>As an oceanic plateau, the magmatic products of the Wrangellia are considerably different from those of continental LIPs like the Siberian Traps and the CAMP and include tholeiitic submarine and subaerial flows. Few sills beneath and interbedded with the lavas are also present. A total volume of at least 1 million km<sup>3</sup> was estimated for the entire LIP (<xref ref-type="bibr" rid="B32">Greene et al., 2010</xref>). Pillow lavas at the base of the volcanic succession are ubiquitous over the entire province. However, they form thinner sequences (&#x223c;500 vs. &#x223c;2,500&#xa0;m) and are highly vesicular in Alaska and Yukon compared to south-western Canada (Vancouver Island), suggesting a southward deepening of the emplacement depth (<xref ref-type="bibr" rid="B32">Greene et al., 2010</xref>). This is consistent with subaerial pahoehoe lavas being relatively more abundant in Alaska and Yukon, where they pile up to 3,500&#xa0;m (<xref ref-type="bibr" rid="B32">Greene et al., 2010</xref>).</p>
<p>The age of the Wrangellia is poorly constrained. A maximum time span of ca. 2&#xa0;Ma has been inferred from magnetostratigraphic studies (<xref ref-type="bibr" rid="B32">Greene et al., 2010</xref> and references therein). Valuable constraints are offered by biostratigraphy. <italic>Daonella</italic>-bearing shales unconformably underlie the lowest basalts of the volcanic sequence. <italic>Daonella</italic> would indicate a maximum Ladinian age (<xref ref-type="bibr" rid="B66">Smith and MacKevet, 1970</xref>; <xref ref-type="bibr" rid="B8">Brack et al., 2005</xref>), but <italic>Daonella</italic> is also known from younger Triassic strata (e.g., <xref ref-type="bibr" rid="B30">F&#xfc;rsich and Wendt, 1977</xref>). The termination of Wrangellia volcanism was marked by the establishment of stable carbonate production on top of volcanic successions and was geographically diachronous. On Vancouver Island, the uppermost basalts of the Karmutsen Formation are interbedded with sediments bearing ammonoids and bivalve <italic>Halobia</italic> of the Tuvalian 1 <italic>dilleri</italic> Zone (Upper Carnian; <xref ref-type="bibr" rid="B19">Carlisle and Susuki, 1974</xref>). On Haida Gwaii (Queen Charlotte Islands), the volcanic sequence is overlain by the carbonate-dominated Kunga Group that yields conodonts and ammonoids of the Tuvalian 2-3 <italic>welleri</italic> Zone (<xref ref-type="bibr" rid="B27">Desrochers and Orchard, 1991</xref>). In south-western Yukon, the volcanism continued to at least the early Norian, evidenced by conodonts recovered from interbedded limestones in the Nikolai Formation (<xref ref-type="bibr" rid="B38">Israel et al., 2006</xref>). Ar/Ar and U-Pb ages for the Wrangellia magmatic rocks span between 232 and 226&#xa0;Ma (<xref ref-type="bibr" rid="B32">Greene et al., 2010</xref> and references therein). However, samples selected for Ar/Ar dating showed widespread alteration leading to large age uncertainties (up to 11&#xa0;Ma), disturbed spectra, and excess argon. Zircons and baddeleyite selected for U-Pb dating were not chemically abraded, likely yielding ages younger than the actual crystallization ages.</p>
<p>The lack of high precision radioisotopic ages for the Wrangellia precludes the possibility to constrain the onset of magmatism, and to distinguish different pulses in the volcanic activity, in turn hindering reconstruction of rates of volcanic or thermogenic gas discharges. This is crucial as the Wrangellia has been tentatively linked to a period of significant climate changes and biological turnover during the Late Triassic, known as CPE (<xref ref-type="bibr" rid="B20">Dal Corso et al., 2020</xref>). The finding of four negative carbon isotope excursions (NCIEs) correlated with Hg spikes in sedimentary strata across the CPE suggest a volcanic origin for this event (<xref ref-type="bibr" rid="B22">Dal Corso et al., 2018</xref>, <xref ref-type="bibr" rid="B20">2020</xref>; <xref ref-type="bibr" rid="B47">Lu et al., 2021</xref>; <xref ref-type="bibr" rid="B50">Mazaheri-Johari et al., 2021</xref>). The duration of the CPE was inferred to be of ca. 1.2 to 1.7&#xa0;Ma based on magnetostratigraphic, biostratigraphic and cyclostratigraphic studies (<xref ref-type="bibr" rid="B79">Zhang et al., 2015</xref>; <xref ref-type="bibr" rid="B53">Miller et al., 2017</xref>; <xref ref-type="bibr" rid="B3">Bernardi et al., 2018</xref>; <xref ref-type="bibr" rid="B20">Dal Corso et al., 2020</xref>). Accordingly, two tuffaceous claystones intercalated with CPE-related rocks of the Jiyuan Basin (China) were dated at 233.10 &#xb1; 1.30 and 232.90 &#xb1; 2.10&#xa0;Ma (LA-ICP-MS U-Pb zircon ages; <xref ref-type="bibr" rid="B47">Lu et al., 2021</xref>). However, although the ages of the Wrangellia and the CPE partially overlap, their relative timing remains highly debated.</p>
</sec>
</sec>
<sec id="s3">
<title>Discussion and Concluding Remarks</title>
<p>Eruptions of the Siberian Traps, the CAMP, and the Wrangellia LIPs deeply reshaped the Triassic world. In particular, the Siberian Traps and the CAMP emplaced in continental settings as pulsed magmatic events, and both bear strong evidence of interaction between magmas and sedimentary country rocks. A clear difference between these LIPs is shown by the widespread explosive volcanism and abundant alkaline magmatism marking the early and final phases of the Siberian Traps, but unknown for the CAMP. On the other hand, the Wrangellia presents substantial differences as it was emplaced in an oceanic setting, and partially consists of subaqueous lava flows. Due to the lack of high-precision geochronology it is also impossible to clarify whether its magmatic activity was pulsed or continuous.</p>
<p>A recurrent aspect of the Triassic period is that multiple NCIEs were reported worldwide for the end-Permian (e.g., <xref ref-type="bibr" rid="B78">Wu et al., 2021</xref>) and end-Triassic mass extinction intervals (<xref ref-type="bibr" rid="B58">Ruhl et al., 2020</xref>), as well as for the CPE (<xref ref-type="bibr" rid="B70">Sun et al., 2019</xref>; <xref ref-type="bibr" rid="B22">Dal Corso et al., 2018</xref>, <xref ref-type="bibr" rid="B20">2020</xref>). NCIEs would testify for the injection of large quantities of isotopically depleted CO<sub>2</sub> into the atmosphere and oceans. Likely, CO<sub>2</sub> (and other greenhouse and poisonous gases) would have been released either from the erupted magmas (<xref ref-type="bibr" rid="B17">Capriolo et al., 2020</xref>) or from devolatilization of the intruded host-rocks (<xref ref-type="bibr" rid="B72">Svensen et al., 2009</xref>; <xref ref-type="bibr" rid="B16">Capriolo et al., 2021</xref>), implying that LIPs-related magmatism was the main driver for catastrophic environmental changes of the Triassic. Since the magnitude of these global crises is also related to the rates at which volatiles were generated, quantifying the process of magma degassing is crucial. Direct estimates of released CO<sub>2</sub> were obtained from fresh, non-recrystallized melt inclusions (e.g., <xref ref-type="bibr" rid="B67">Sobolev et al., 2009</xref>; <xref ref-type="bibr" rid="B5">Black et al., 2014</xref>; <xref ref-type="bibr" rid="B64">Sibik et al., 2015</xref>; <xref ref-type="bibr" rid="B17">Capriolo et al., 2020</xref>). However, these are few (and potentially not entirely representative) for the Siberian Traps and the CAMP, and completely lacking for the Wrangellia. We therefore adopted here the approach of <xref ref-type="bibr" rid="B57">Rosenthal et al. (2015)</xref> to estimate the initial CO<sub>2</sub> contents of basaltic magmas from their incompatible trace element compositions. In fact, Nb and CO<sub>2</sub> behave similarly during partial mantle melting, both strongly partitioning into the melt phase. However, at shallow depth in the crust, CO<sub>2</sub> is degassed as magma ascends towards the surface (<xref ref-type="bibr" rid="B17">Capriolo et al., 2020</xref>), while Nb remains in the melt. We applied this proxy to whole-rock compositions of the three Triassic LIPs (<xref ref-type="fig" rid="F2">Figure 2</xref>) filtered for basalts with MgO &#x3e;7&#xa0;wt% to consider only those magmas closer to the composition of mantle-derived primitive melts, as suggested by <xref ref-type="bibr" rid="B37">Hernandez Nava et al. (2021)</xref>.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Initial maximum CO<sub>2</sub> budgets obtained from Nb whole-rock concentrations of magmas for the Siberian Traps (circles), the Wrangellia (triangles) and the CAMP (squares). Following <xref ref-type="bibr" rid="B57">Rosenthal et al. (2015)</xref>, we assumed CO<sub>2</sub>/Nb &#x3d; 505 &#xb1; 168, which corresponds to mantle source CO<sub>2</sub> of 75 &#xb1; 25&#xa0;ppm. Data are filtered for MgO &#x3e; 7wt%. Maximum and minimum MgO contents are 22.9&#x2013;7.1&#xa0;wt% (average 10.2&#xa0;wt%) for the Siberian Traps, 17.5&#x2013;7.1&#xa0;wt% (average 9.8&#xa0;wt%) for the Wrangellia, and 16.6&#x2013;7.0&#xa0;wt% (average 8.7&#xa0;wt%) for the CAMP. Data are plotted in ranked order. Siberian Traps: data from GEOROC Database (<ext-link ext-link-type="uri" xlink:href="http://georoc.mpch-mainz.gwdg.de/">http://georoc.mpch-mainz.gwdg.de/</ext-link>); <xref ref-type="bibr" rid="B34">Hawkesworth et al. (1995)</xref>; <xref ref-type="bibr" rid="B67">Sobolev et al. (2009</xref>, <xref ref-type="bibr" rid="B68">2011)</xref>; <xref ref-type="bibr" rid="B64">Sibik et al. (2015)</xref>; <xref ref-type="bibr" rid="B15">Callegaro et al. (2021)</xref>. Wrangellia: data from <xref ref-type="bibr" rid="B31">Greene et al. (2009a)</xref>, <xref ref-type="bibr" rid="B33">Greene et al. (2009b)</xref>, <xref ref-type="bibr" rid="B32">Greene et al. (2010)</xref>. CAMP: data from <xref ref-type="bibr" rid="B25">De Min et al. (2003)</xref>; <xref ref-type="bibr" rid="B39">Jourdan et al. (2003)</xref>; <xref ref-type="bibr" rid="B26">Deckart et al. (2005)</xref>; <xref ref-type="bibr" rid="B75">Verati et al. (2005)</xref>; <xref ref-type="bibr" rid="B51">Merle et al. (2011</xref>, <xref ref-type="bibr" rid="B52">2014)</xref>; <xref ref-type="bibr" rid="B13">Callegaro et al. (2013</xref>, <xref ref-type="bibr" rid="B14">2014b)</xref>; <xref ref-type="bibr" rid="B4">Bertrand et al. (2014)</xref>; <xref ref-type="bibr" rid="B48">Marzoli et al. (2019)</xref>. All data are reported in the <xref ref-type="sec" rid="s8">Supplementary Appendix Table</xref>. CO<sub>2</sub> concentrations measured from melt inclusions (MI) for the Siberian Traps (<xref ref-type="bibr" rid="B5">Black et al., 2014</xref>; <xref ref-type="bibr" rid="B64">Sibik et al., 2015</xref>) are reported for comparison (open circles). Yellow and grey arrows represent CO<sub>2</sub> estimates obtained from trace element (TE) concentrations in melt inclusions following the same approach as whole-rock data. CO<sub>2</sub> concentrations obtained from MI of the Gudchikhinsky Formation (yellow colour; Lower Unit) and of intrusives of the main phase of the Siberian Traps (grey colour; <xref ref-type="bibr" rid="B64">Sibik et al., 2015</xref>) are ca. 0.3&#x2013;0.9&#xa0;wt% and ca. 0&#x2013;0.3&#xa0;wt%, respectively, consistent with the results obtained from whole-rock data. Red arrow represents CO<sub>2</sub> concentrations estimated from gas exsolution bubbles preserved in melt inclusion of CAMP magmas (<xref ref-type="bibr" rid="B17">Capriolo et al., 2020</xref>).</p>
</caption>
<graphic xlink:href="feart-10-887632-g002.tif"/>
</fig>
<p>CO<sub>2</sub> concentrations estimated for magmas of the Siberian Traps are significantly variable within the three magmatic phases previously described (<xref ref-type="fig" rid="F2">Figure 2</xref>). High-Ti lava flows of the Lower Unit and the low-Ti magmas of the Middle-Transitional Unit yielded the highest calculated CO<sub>2</sub> contents (ca. 0.1&#x2013;1.2 and 0.05&#x2013;0.7&#xa0;wt%, respectively; <xref ref-type="fig" rid="F2">Figure 2</xref>). In contrast, lavas of the Upper Unit and correlated intrusions, which characterize the second and more voluminous Siberian main phase, yielded lower CO<sub>2</sub> contents (ca. 0.1&#x2013;0.3&#xa0;wt%; <xref ref-type="fig" rid="F2">Figure 2</xref>). Within CAMP, the earliest erupted basalts from north-western Africa are relatively enriched in CO<sub>2</sub> (0.4&#x2013;0.7&#xa0;wt%), while the slightly later and ubiquitous low-Ti magmas of the Prevalent group (<xref ref-type="bibr" rid="B13">Callegaro et al., 2013</xref>; <xref ref-type="bibr" rid="B52">Merle et al., 2014</xref>; <xref ref-type="bibr" rid="B49">Marzoli et al., 2018</xref>, <xref ref-type="bibr" rid="B48">2019</xref>) yielded slightly lower CO<sub>2</sub> concentrations (ca. 0.1 to 0.5&#xa0;wt%; <xref ref-type="fig" rid="F2">Figure 2</xref>). These results would imply that, for both the Siberian Traps and the CAMP, the highest concentrations of mantle-derived CO<sub>2</sub> were produced from magmas of the initial phases. Interestingly, the end-Permian extinction coincides with the initial emplacement of the volatile-poor sills of the Siberian Traps, while the end-Triassic extinction coincides with the effusive activity of the CAMP, whose lavas are relatively CO<sub>2</sub>-rich (<xref ref-type="bibr" rid="B17">Capriolo et al., 2020</xref>). The fact that variable amounts of mantle-derived CO<sub>2</sub> from the magmas produced similar environmental consequences suggests that additional isotopically depleted CO<sub>2</sub> was likely released during the intrusive Siberian Traps activity. In this case, a significant part of the emitted CO<sub>2</sub> (and possibly other gases, e.g., CH<sub>4</sub>, SO<sub>2</sub> and halocarbons) may have been produced thermogenically from the intruded host rocks (e.g., <xref ref-type="bibr" rid="B72">Svensen et al., 2009</xref>, <xref ref-type="bibr" rid="B71">2018</xref>; <xref ref-type="bibr" rid="B16">Capriolo et al., 2021</xref>) highlighting the crucial role of sedimentary basins as additional suppliers of climate-modifying gases. Noteworthy, the early terrestrial onset of the end-Permian extinction seems to suggest that mantle-derived halogens were key environmental impactors during the first phase of the Siberian Traps (<xref ref-type="bibr" rid="B68">Sobolev et al., 2011</xref>; <xref ref-type="bibr" rid="B21">Dal Corso et al., 2022</xref>).</p>
<p>Geochemical data for the Wrangellia are relatively scarce. However, the high-Ti basalts have the highest Nb and thus possibly the highest CO<sub>2</sub> contents (ca. 0.3&#x2013;0.5&#xa0;wt%), while the low-Ti basalts were relatively Nb and thus CO<sub>2</sub>-depleted (&#x2264;0.3&#xa0;wt%). This difference may imply that the overall production of CO<sub>2</sub> increased when magmas were predominantly sourced from the mantle plume source, i.e., with minor or no contribution from the lithospheric mantle.</p>
<p>To summarize, in this study, we reviewed the main features of the Siberian Traps, the Wrangellia and the CAMP LIPs, which impacted the Triassic world. High-precision geochronology strongly links the Siberian Traps and the CAMP to the end-Permian and the end-Triassic mass extinctions, respectively. A similar cause-and-effect scenario between the Wrangellia and the CPE seems plausible based on paleontological, biostratigraphic and geochemical studies. However, further high-precision dating on both lava flows and intrusions is necessary to constrain the onset, evolution, and cessation of this LIP, as well as its emplacement mechanisms.</p>
<p>Using previously published data, we estimated maximum CO<sub>2</sub> contents for magmas of the three Triassic LIPs. Even if these estimates are based on proxy data, our results highlight that the mantle-related CO<sub>2</sub> budgets of the more primitive basalts seem to vary during the overall life cycle of each LIP, suggesting that different mantle sources or melting regimes came into play to produce these exceptionally voluminous volcanic events. These observations stress the fact that each LIP is a unique case-study and building paradigms that apply to all LIPs when discussing their relationship to concurrent Earth crises is not straightforward.</p>
</sec>
</body>
<back>
<sec id="s4">
<title>Author Contributions</title>
<p>AB wrote the review on Wrangellia, compiled data from the literature and produced the figures. SC wrote the review on the Siberian Traps. AM designed the project and wrote the review on the CAMP. YS contributed to the review on Wrangellia.</p>
</sec>
<sec id="s5">
<title>Funding</title>
<p>Financial support was provided by the Italian Ministry of University and Research (PRIN 20178LPCP to AM). SC acknowledges support from the Research Council of Norway (Grant 301096, Young Research Talents).</p>
</sec>
<sec sec-type="COI-statement" id="s6">
<title>Conflict of Interest</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s7">
<title>Publisher&#x2019;s Note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<sec id="s8">
<title>Supplementary Material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/feart.2022.887632/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/feart.2022.887632/full&#x23;supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="Table1.xlsx" id="SM1" mimetype="application/xlsx" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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