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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">894353</article-id>
<article-id pub-id-type="doi">10.3389/feart.2022.894353</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Earth Science</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>The Multiple Metamorphism of Mafic Granulites From the East Hebei Terrane, North China Craton: Insights Into the Transition of Tectonic Regimes</article-title>
<alt-title alt-title-type="left-running-head">Liu et al.</alt-title>
<alt-title alt-title-type="right-running-head">Multiple Metamorphism in East Hebei</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Liu</surname>
<given-names>Ting</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1511823/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Wei</surname>
<given-names>Chunjing</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/149846/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Yang</surname>
<given-names>Chuan</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Li</surname>
<given-names>Zhuang</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1748935/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>College of Earth Sciences</institution>, <institution>Chengdu University of Technology</institution>, <addr-line>Chengdu</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>MOE Key Laboratory of Orogenic Belts and Crustal Evolution</institution>, <institution>School of Earth and Space Sciences</institution>, <institution>Peking University</institution>, <addr-line>Beijing</addr-line>, <country>China</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>China Transport Telecommunications and Information Center</institution>, <addr-line>Beijing</addr-line>, <country>China</country>
</aff>
<aff id="aff4">
<sup>4</sup>
<institution>College of Geosciences</institution>, <institution>China University of Petroleum (Beijing)</institution>, <addr-line>Beijing</addr-line>, <country>China</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/144151/overview">Yi Chen</ext-link>, Institute of Geology and Geophysics (CAS), China</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/1718928/overview">Fran&#xe7;ois Camille</ext-link>, Commission for the Geological Map of the World, France</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1631115/overview">Shujuan Jiao</ext-link>, Institute of Geology and Geophysics (CAS), China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Ting Liu, <email>liuting3624@pku.edu.cn</email>; Chuan Yang, <email>yangchuan@pku.edu.cn</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>10</day>
<month>05</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>10</volume>
<elocation-id>894353</elocation-id>
<history>
<date date-type="received">
<day>11</day>
<month>03</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>07</day>
<month>04</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Liu, Wei, Yang and Li.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Liu, Wei, Yang and Li</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 East Hebei terrane from the North China Craton preserves the dome&#x2013;and&#x2013;keel structures, which was transected by a later linear belt in the north margin. Mafic granulites from the linear belt and domes record two groups of metamorphic ages at Neoarchean and Paleoproterozoic, but their accurate metamorphic peak conditions and paths have not been well addressed. Three samples of mafic granulites, including two-pyroxene granulite (JD15120), garnet-bearing two-pyroxene granulite (YC8-43), and garnet clinopyroxene granulite (JD1546), were documented for detailed metamorphic studies. Two-episode metamorphism can be recognized. The first-episode recovered from JD15120 and YC8-43 is represented by peak assemblage of medium-grained clinopyroxene, orthopyroxene, amphibole, plagioclase, and ilmenite, which yields ultrahigh temperature (UHT) conditions of 940&#x2013;960&#xb0;C at 7.5&#x2013;8.5&#xa0;kbar and 950&#x2013;990&#xb0;C at 8&#xa0;kbar, respectively, constrained by contours of the maximum anorthite (<italic>X</italic>
<sub>An</sub>) in plagioclase cores. The post-peak evolution is dominated by cooling with decompression, constrained mostly from the measured core-to-rim decreasing <italic>X</italic>
<sub>An</sub> in plagioclase. By contrast, the second-episode overprinting is recognized in all samples, but exhibits varying textures. In garnet-bearing samples (YC8-43 and JD1546), the overprinting assemblages are characterized by poikilitic garnet that occurs either as coronae around the first-episode pyroxenes, forming &#x201c;red-eye socket&#x201d; textures, or as grains in equilibrium with tiny-grained clinopyroxene, plagioclase, amphibole, rutile, and quartz, forming high-pressure (HP) granulite assemblages. These HP granulite assemblages show peak conditions of &#x223c;12 kbar/860&#xb0;C and &#x223c;12.6&#xa0;kbar/835&#xb0;C, constrained by contours of the maximum grossular (<italic>X</italic>
<sub>Grs</sub>) in garnet cores and the minimum <italic>X</italic>
<sub>An</sub> in plagioclase cores. The post-peak evolution is dominated by isothermal decompression, constrained from the outward decreasing <italic>X</italic>
<sub>Grs</sub> in garnet and increasing <italic>X</italic>
<sub>An</sub> in plagioclase. LA-ICP-MS U-Pb zircon dating on JD15120 and JD1546 suggests two metamorphic ages of &#x223c;2.49&#xa0;Ga and &#x223c;1.78&#xa0;Ga, being considered to be correlated with the UHT and HP granulite metamorphism, respectively. Tectonically, the late Neoarchean UHT granulite metamorphism may correlate a vertical sagduction regime, whereas the late Paleoproterozoic HP granulite metamorphism is favored to register the continental collision in the northern margin of the North China Craton. This study may have indications for the Neoarchean&#x2013;Paleoproterozoic tectonic transition of the craton.</p>
</abstract>
<kwd-group>
<kwd>Archean supracrustal rocks</kwd>
<kwd>Ultra-high temperature granulite</kwd>
<kwd>High-pressure granulite</kwd>
<kwd>Pseudosection</kwd>
<kwd>East Hebei terrane</kwd>
<kwd>North China Craton</kwd>
</kwd-group>
<contract-num rid="cn001">42102062 42030304</contract-num>
<contract-sponsor id="cn001">National Natural Science Foundation of China<named-content content-type="fundref-id">10.13039/501100001809</named-content>
</contract-sponsor>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>As a window into the lower continental crust, granulites normally record pressure&#x2013;temperature (<italic>P&#x2013;T</italic>) conditions and <italic>P&#x2013;T</italic> paths being indicative to tectonic models (<xref ref-type="bibr" rid="B25">Harley 1989</xref>, <xref ref-type="bibr" rid="B26">Harley 1998</xref>). Their secular change in apparent thermal gradients is also suggestive for revealing different heat flow and rheology in distinct tectonics (<xref ref-type="bibr" rid="B5">Brown and Johnson 2018</xref>). In the Archean terranes, almost half of the granulites are ultrahigh temperature (UHT) type with high d<italic>T</italic>/d<italic>P</italic> of &#x3e;22&#xb0;C/km (<xref ref-type="bibr" rid="B6">Brown 2007</xref>; <xref ref-type="bibr" rid="B5">Brown and Johnson 2018</xref>), representing extreme thermal conditions related to the coupling between crust, sub-crustal lithosphere, and asthenospheric mantle on a regional scale (<xref ref-type="bibr" rid="B23">Harley 2004</xref>; <xref ref-type="bibr" rid="B24">Harley 2008</xref>; <xref ref-type="bibr" rid="B36">Kelsey and Hand 2015</xref>), whereas the high-pressure (HP) granulites with intermediate d<italic>T</italic>/d<italic>P</italic> of 22&#x2013;11&#xb0;C/km became dominant after the Archean Eon (<xref ref-type="bibr" rid="B5">Brown and Johnson 2018</xref>), being normally considered as the sign for subduction or collision processes in plate tectonics (<xref ref-type="bibr" rid="B63">O&#x27;Brien and R&#xf6;tzler 2003</xref>).</p>
<p>Archean cratons, although featured with thick and depleted lithospheric mantle and relatively stable from subsequent tectonism (<xref ref-type="bibr" rid="B35">Jordan 1978</xref>), can have transformation of the cratonic structures and development of multiple metamorphism in response to later reworking events (e.g., <xref ref-type="bibr" rid="B85">Weber 1984</xref>; <xref ref-type="bibr" rid="B59">Mahan et al., 2008</xref>; <xref ref-type="bibr" rid="B66">Perchuk et al., 2008</xref>). For example, the Pikwitonei granulite domain in the Superior Craton, one of the largest Neoarchean high-grade terranes worldwide, was recovered to have undergone multiple metamorphism, involving normal UHT granulite-facies metamorphism with an anticlockwise <italic>P&#x2013;T</italic> path at Neoarchean, and overprinting greenschist to amphibolite-facies metamorphism with local migmatization at Hudsonian. These distinct metamorphic processes suggest different tectonic settings involving magmatic underplating (<xref ref-type="bibr" rid="B60">Mezger et al., 1990</xref>) or overthrusting during crustal thickening (<xref ref-type="bibr" rid="B1">Arima and Barnett 1984</xref>) for the first-episode metamorphism, and collision between the Superior Craton and the Churchill Province to form the Thompson belt for the second-episode metamorphism (<xref ref-type="bibr" rid="B85">Weber 1984</xref>). Therefore, detailed metamorphic studies on Archean cratons can give insights into the tectonic evolution of the early Earth.</p>
<p>The North China Craton (NCC) consists of four Archean blocks including Ordos, Yinshan, Longgang, and Langrim blocks, and three Paleoproterozoic orogenic belts among them (<xref ref-type="bibr" rid="B112">Zhao et al., 2005</xref>). These Archean blocks were revealed to record Neoarchean granulite-facies metamorphism with anticlockwise <italic>P&#x2013;T</italic> paths, featured with &#x201c;red-eye socket&#x201d; texture in mafic granulites (<xref ref-type="bibr" rid="B114">Zhao et al., 1999</xref>; <xref ref-type="bibr" rid="B112">Zhao et al., 2005</xref>; <xref ref-type="bibr" rid="B40">Kwan et al., 2016</xref>). However, recent studies on mafic granulites from the East Hebei terrane, part of the Longgang block, suggest that some Archean terranes may be subjected to two episodes of granulite-facies metamorphism at late Neoarchean (2.53&#x2013;2.47&#xa0;Ga) and late Paleoproterozoic (1.85&#x2013;1.80&#xa0;Ga), respectively (<xref ref-type="bibr" rid="B14">Duan et al., 2015</xref>; <xref ref-type="bibr" rid="B99">Yang and Wei 2017b</xref>; <xref ref-type="bibr" rid="B56">Lu and Wei 2020</xref>). The first-episode Neoarchean granulite-facies metamorphism is featured with two-pyroxene granulites, and is argued to have peak conditions of normal UHT granulite facies of 8.0&#x2013;11.0&#xa0;kbar/756&#x2013;940&#xb0;C using conventional geothermobarometers (<xref ref-type="bibr" rid="B28">He and Ye 1992</xref>; <xref ref-type="bibr" rid="B8">Chen and Li 1996</xref>; <xref ref-type="bibr" rid="B114">Zhao et al., 1999</xref>; <xref ref-type="bibr" rid="B40">Kwan et al., 2016</xref>; <xref ref-type="bibr" rid="B100">Yang and Wei 2017a</xref>), or 9.0&#x2013;10.0&#xa0;kbar/950&#x2013;1,070&#xb0;C using rare earth elements (REE)-based geothermometers (<xref ref-type="bibr" rid="B100">Yang and Wei 2017a</xref>). On account of that conventional Fe&#x2013;Mg exchange geothermometers are more likely to record lower temperatures than the peak of granulites as a result of the fast diffusion during cooling (e.g., <xref ref-type="bibr" rid="B17">Frost and Chacko 1989</xref>; <xref ref-type="bibr" rid="B65">Pattison et al., 2003</xref>), and the REE-based geothermobarometers generally have large uncertainties (<xref ref-type="bibr" rid="B100">Yang and Wei 2017a</xref>), the peak conditions for the two-pyroxene granulites remain uncertain. The second-episode Paleoproterozoic metamorphism was first recognized in mafic dykes, characterized by HP granulite-facies assemblages, which record <italic>P</italic>&#x2013;<italic>T</italic> conditions of 11&#x2013;12&#xa0;kbar/790&#x2013;810&#xb0;C with clockwise <italic>P</italic>&#x2013;<italic>T</italic> paths at &#x223c;1.82&#xa0;Ga (<xref ref-type="bibr" rid="B14">Duan et al., 2015</xref>). Similar overprinting assemblages were also observed in Neoarchean mafic granulites, which exhibit peak <italic>P</italic>&#x2013;<italic>T</italic> conditions of 12.5&#x2013;12.8&#xa0;kbar/880&#x2013;900&#xb0;C, metamorphic zircon ages of 1.83&#x2013;1.81&#xa0;Ga, and garnet-whole rock Lu&#x2013;Hf isochron ages of 1.77&#x2013;1.79&#xa0;Ga (<xref ref-type="bibr" rid="B100">Yang and Wei 2017a</xref>; <xref ref-type="bibr" rid="B99">Yang and Wei 2017b</xref>; <xref ref-type="bibr" rid="B56">Lu and Wei 2020</xref>). However, <xref ref-type="bibr" rid="B83">Wang et al. (2018)</xref> argued that the HP granulite metamorphism may have occurred at early Paleoproterozoic (&#x223c;2.46&#xa0;Ga), which was followed by heating and decompression to form two-pyroxene granulites. Thus, detailed petrological and geochronological studies on both two-pyroxene and HP granulites need to be further conducted to document their metamorphic evolution.</p>
<p>In this article, representative mafic granulites that have been studied using major element- and REE-based geothermobarometers in <xref ref-type="bibr" rid="B100">Yang and Wei (2017a)</xref>, were selected for constraining their metamorphic <italic>P</italic>&#x2013;<italic>T</italic> conditions and paths on the basis of the pseudosections calculated using THERMOCALC. Zircon U&#x2013;Pb dating was also carried out for defining the metamorphic ages.</p>
</sec>
<sec id="s2">
<title>2 Geological Setting</title>
<p>The NCC can be normally divided into Eastern and Western Blocks (e.g., <xref ref-type="bibr" rid="B113">Zhao et al., 1998</xref>; <xref ref-type="bibr" rid="B112">Zhao et al., 2005</xref>; <xref ref-type="bibr" rid="B111">Zhao et al., 2012</xref>; <xref ref-type="fig" rid="F1">Figure 1A</xref>). It is suggested that the Western Block formed at &#x223c;1.95&#xa0;Ga by the collision between the Yinshan and Ordos Blocks along the Khondalite Belt, whereas the Eastern Block formed at &#x223c;1.90&#xa0;Ga when the Longgang and Langrim blocks collided along the Jiao&#x2013;Liao&#x2013;Ji Belt (e.g., <xref ref-type="bibr" rid="B113">Zhao et al., 1998</xref>; <xref ref-type="bibr" rid="B112">Zhao et al., 2005</xref>; <xref ref-type="bibr" rid="B111">Zhao et al., 2012</xref>). The time of the final amalgamation between Western and Eastern Blocks along the Trans-North China Orogen (TNCO) is controversial: one view suggests that it occurred at &#x223c;1.85&#xa0;Ga (<xref ref-type="bibr" rid="B113">Zhao et al., 1998</xref>; <xref ref-type="bibr" rid="B112">Zhao et al., 2005</xref>; <xref ref-type="bibr" rid="B111">Zhao et al., 2012</xref>), whereas another view favors an older collision age of &#x223c;1.95&#xa0;Ga (<xref ref-type="bibr" rid="B71">Qian et al., 2013</xref>; <xref ref-type="bibr" rid="B70">Qian et al., 2015</xref>; <xref ref-type="bibr" rid="B69">Qian and Wei 2016</xref>), and interprets the age of &#x223c;1.85&#xa0;Ga to represent a separated orogenic event occurred along the northern margin of the NCC (<xref ref-type="bibr" rid="B86">Wei 2018</xref>; <xref ref-type="bibr" rid="B72">Qian et al., 2019</xref>). In addition, accretionary and collisional tectonics were also proposed for the NCC, including 2.6&#x2013;2.5&#xa0;Ga Atlantic-type passive margin on the western side of the Eastern Block, the &#x223c;2.5&#xa0;Ga collision between the arc/accretionary prism and the Eastern Block, &#x223c;2.43&#xa0;Ga amalgamation of Western Block and Eastern Block along the Central Orogenic Belt (COB, approximate TNCO), and the 2.3&#x2013;1.9&#xa0;Ga collision along the Inner Mongolia-North Hebei Orogenic Belt (IMNHO) at the north margin of the NCC (<xref ref-type="bibr" rid="B39">Kusky et al., 2016</xref>).</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>
<bold>(A)</bold> Tectonic subdivision of the North China craton (modified after <xref ref-type="bibr" rid="B112">Zhao et al., 2005</xref>; <xref ref-type="bibr" rid="B111">Zhao et al., 2012</xref>). <bold>(B)</bold> Geological map of the East Hebei terrane (modified after <xref ref-type="bibr" rid="B94">Wu et al., 1998</xref>; <xref ref-type="bibr" rid="B86">Wei 2018</xref>) with sample locations. GR-granulite; AM-amphibolite; GS-greenschist.</p>
</caption>
<graphic xlink:href="feart-10-894353-g001.tif"/>
</fig>
<p>The early Precambrian East Hebei terrane, located in the northwestern of the Longgang Block, can be divided into six litho&#x2013;tectonic units (<xref ref-type="fig" rid="F1">Figure 1B</xref>) including the Taipingzhai ovoid-structural domain (I), Qian&#x2019;an gneiss dome (II), Badaohe gneiss dome (III), Lulong&#x2013;Shuangshanzi supracrustal belt (IV), Anziling gneiss dome (V) and Saheqiao linear-structural belt (VI), following <xref ref-type="bibr" rid="B94">Wu et al. (1998)</xref> and <xref ref-type="bibr" rid="B86">Wei (2018)</xref>. There is near-vertical normal shear in the Shuangshanzi shear zone between the Anziling dome and the Lulong&#x2013;Shuangshanzi supracrustal belt formed due to the upwelling of the dome with respect to the down-slipping of the belt (<xref ref-type="bibr" rid="B48">Liu et al., 2017</xref>; <xref ref-type="bibr" rid="B110">Zhao et al., 2021</xref>). Therefore, the terrane well preserves Archean unique dome&#x2013;and&#x2013;keel structure although later deformation marked by numerous NE-to NEE-striking shear zones in the Saheqiao linear-structural belt occurred (<xref ref-type="bibr" rid="B55">Liu and Yang 1994</xref>; <xref ref-type="bibr" rid="B39">Kusky et al., 2016</xref>; <xref ref-type="bibr" rid="B110">Zhao et al., 2021</xref>). As show at <xref ref-type="fig" rid="F1">Figure 1B</xref>, the East Hebei terrane mainly consists of Neoarchean TTG gneisses, charnockites, potassic granites, and supracrustal rocks. The TTG gneisses and charnockites show magmatic ages of mostly 2.56&#x2013;2.48&#xa0;Ga with a peak at &#x223c;2.52&#xa0;Ga (<xref ref-type="bibr" rid="B49">Liu et al., 1990</xref>; <xref ref-type="bibr" rid="B95">Wu and Geng 1991</xref>; <xref ref-type="bibr" rid="B19">Geng et al., 2006</xref>; <xref ref-type="bibr" rid="B101">Yang et al., 2008</xref>; <xref ref-type="bibr" rid="B62">Nutman et al., 2011</xref>; <xref ref-type="bibr" rid="B22">Guo et al., 2013</xref>; <xref ref-type="bibr" rid="B3">Bai et al., 2014</xref>; <xref ref-type="bibr" rid="B2">Bai et al., 2015</xref>; <xref ref-type="bibr" rid="B103">Yang et al., 2016a</xref>; <xref ref-type="bibr" rid="B102">Yang et al., 2016b</xref>), except for a few intrusions in the western margin of Qian&#x2019;an gneiss dome that have older ages of 3.28&#x2013;2.94&#xa0;Ma (<xref ref-type="bibr" rid="B62">Nutman et al., 2011</xref>; <xref ref-type="bibr" rid="B77">Sun et al., 2016</xref>). They were subjected to amphibolite-to granulite-facies metamorphism at 2.53&#x2013;2.47&#xa0;Ga (<xref ref-type="bibr" rid="B19">Geng et al., 2006</xref>; <xref ref-type="bibr" rid="B101">Yang et al., 2008</xref>; <xref ref-type="bibr" rid="B62">Nutman et al., 2011</xref>; <xref ref-type="bibr" rid="B3">Bai et al., 2014</xref>; <xref ref-type="bibr" rid="B2">Bai et al., 2015</xref>). The supracrustal rocks, mainly comprising metasedimentary and metabasic rocks with a few banded iron formation and ultramafic interlayers (<xref ref-type="bibr" rid="B19">Geng et al., 2006</xref>; <xref ref-type="bibr" rid="B67">Polat et al., 2006</xref>), commonly occur as rafts within or as belts between TTG gneiss domes (<xref ref-type="bibr" rid="B86">Wei 2018</xref>). Most of the metasedimentary rocks share similar protolith deposition ages of 2.53&#x2013;2.50&#xa0;Ga (<xref ref-type="bibr" rid="B81">Wan et al., 2015</xref>; <xref ref-type="bibr" rid="B77">Sun et al., 2016</xref>; <xref ref-type="bibr" rid="B15">Duan et al., 2017</xref>; <xref ref-type="bibr" rid="B57">Lu et al., 2017</xref>; <xref ref-type="bibr" rid="B54">Liu and Wei 2020</xref>), except for fuchsite-bearing quartzite that outcropped at Caozhuang and Luanxian areas having deposition age of &#x3e;3.5&#xa0;Ga (<xref ref-type="bibr" rid="B49">Liu et al., 1990</xref>; <xref ref-type="bibr" rid="B62">Nutman et al., 2011</xref>; <xref ref-type="bibr" rid="B11">Chu et al., 2016</xref>). The metabasic rocks were mostly dated to have protolith magmatic ages of 2.61&#x2013;2.52&#xa0;Ga with a few at &#x223c;2.90&#xa0;Ga (<xref ref-type="bibr" rid="B106">Zhang et al., 2012</xref>; <xref ref-type="bibr" rid="B22">Guo et al., 2013</xref>; <xref ref-type="bibr" rid="B18">Fu et al., 2016</xref>; <xref ref-type="bibr" rid="B47">Liou et al., 2017</xref>). Ultramafic rocks, mostly including serpentinized peridotite, picritic amphibolites, and pyroxenite, are argued to be komatiites (<xref ref-type="bibr" rid="B109">Zhang et al., 1980</xref>), intra-oceanic suprasubduction zone ophiolitic rocks (<xref ref-type="bibr" rid="B67">Polat et al., 2006</xref>), or remnants of an enriched mantle plume (<xref ref-type="bibr" rid="B84">Wang et al., 2019</xref>). These supracrustal rocks were normally dated to have two groups of metamorphic ages at 2.53&#x2013;2.47&#xa0;Ga and 1.85&#x2013;1.80&#xa0;Ga as have mentioned in introduction (e.g., <xref ref-type="bibr" rid="B99">Yang and Wei 2017b</xref>; <xref ref-type="bibr" rid="B56">Lu and Wei 2020</xref>). The former episode of metamorphism is widely recorded in the whole East Hebei terrane, corresponding to amphibolite-to greenschist-facies metamorphic conditions in Lulong&#x2013;Shuangshanzi supracrustal belt (<xref ref-type="bibr" rid="B68">Qi et al., 1999</xref>; <xref ref-type="bibr" rid="B22">Guo et al., 2013</xref>), amphibolite-facies condition of 10&#x2013;11&#xa0;kbar/780&#x2013;800&#xb0;C with clockwise <italic>P&#x2013;T</italic> path in the Caozhuang area (<xref ref-type="bibr" rid="B51">Liu et al., 2020</xref>), and the granulite-facies (9.6&#x2013;10.3&#xa0;kbar/860&#x2013;900&#xb0;C) to UHT (9&#x2013;10&#xa0;kbar/&#x3e;1,000&#xb0;C) peak conditions with anticlockwise <italic>P</italic>&#x2013;<italic>T</italic> paths in the western margin of Qian&#x2019;an gneiss dome, Taipingzhai ovoid-structural domain and Saheqiao linear-structural belt (<xref ref-type="bibr" rid="B40">Kwan et al., 2016</xref>; <xref ref-type="bibr" rid="B100">Yang and Wei 2017a</xref>; <xref ref-type="bibr" rid="B15">Duan et al., 2017</xref>; <xref ref-type="bibr" rid="B57">Lu et al., 2017</xref>; <xref ref-type="bibr" rid="B53">Liu and Wei 2018</xref>; <xref ref-type="bibr" rid="B56">Lu and Wei 2020</xref>; <xref ref-type="bibr" rid="B52">Liu et al., 2021</xref>). By contrast, the second-episode metamorphism is locally recognized in the northern part of the terrane, mostly in the Saheqiao linear-structural belt and the Taipingzhai ovoid-structural domain, and dominated by HP granulite-facies metamorphism as have been mentioned in introduction (<xref ref-type="bibr" rid="B15">Duan et al., 2017</xref>; <xref ref-type="bibr" rid="B100">Yang and Wei 2017a</xref>; <xref ref-type="bibr" rid="B56">Lu and Wei 2020</xref>). In addition, there are mafic dykes crosscutting the foliation of Archean TTG gneisses and supracrustal rocks in the Saheqiao linear-structural belt and the Taipingzhai ovoid-structural domain (<xref ref-type="bibr" rid="B9">Chen 1990</xref>; <xref ref-type="bibr" rid="B76">Song 1990</xref>), and proposed to have experienced HP granulite-facies metamorphism in the later overprinting metamorphism (<xref ref-type="bibr" rid="B14">Duan et al., 2015</xref>).</p>
<p>In this study, mafic granulites were collected from the Malanyu, Saheqiao, and Taipingzhai areas. The sample locations are shown on <xref ref-type="fig" rid="F1">Figure 1B</xref>. These granulites occur as rafts with clear or blurry boundaries within TTG rocks (<xref ref-type="fig" rid="F2">Figures 2A,B</xref>). Most of them have weak or penetrative foliations (<xref ref-type="fig" rid="F2">Figure 2C</xref>) and are heterogeneous with the diverse distributions of leucosomes (<xref ref-type="fig" rid="F2">Figure 2D</xref>).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Field occurrence of mafic granulites. <bold>(A,B)</bold> Mafic granulites occurring as rafts or enclaves with clear or blurry boundaries within TTG rocks. <bold>(C)</bold> Mafic granulites with penetrative foliation. <bold>(D)</bold> Heterogeneous mafic granulites with diverse distributions of leucosomes.</p>
</caption>
<graphic xlink:href="feart-10-894353-g002.tif"/>
</fig>
</sec>
<sec id="s3">
<title>3 Petrological Analyses</title>
<sec id="s3-1">
<title>3.1 Bulk-Rock Compositions</title>
<p>Among the selected samples, two-pyroxene granulite (JD15120) was collected from the Taipingzhai ovoid-structural domain, while the garnet-bearing two-pyroxene granulite (YC8-43) and clinopyroxene granulite (JD1546) were from the Saheqiao and Malanyu areas, respectively, in the Saheqiao linear-structural belt (<xref ref-type="fig" rid="F1">Figure 1B</xref>; <xref ref-type="bibr" rid="B100">Yang and Wei 2017a</xref>). Their bulk-rock compositions, being analyzed using a Leeman Prodigy inductively coupled the plasma-optical emission spectroscopy (ICP&#x2013;OES) system with high-dispersion Echelle optics at China University of Geoscience (Beijing), are presented in <xref ref-type="table" rid="T1">Table 1</xref>. The three samples share similar compositions with SiO<sub>2</sub> of 47.41&#x2013;48.76&#xa0;wt%, MgO of 6.86&#x2013;7.90&#xa0;wt%, total Fe<sub>2</sub>O<sub>3</sub> of 12.56&#x2013;16.01&#xa0;wt%, CaO of 10.68&#x2013;12.64&#xa0;wt%, and Mg<sup>&#x23;</sup> of 46&#x2013;52.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Bulk-rock compositions of samples in this study.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left" rowspan="2">Sample</th>
<th align="center" rowspan="2">Type</th>
<th colspan="11" align="center">ICP-OES whole rock composition (wt%)</th>
</tr>
<tr>
<th align="center">SiO<sub>2</sub>
</th>
<th align="center">TiO<sub>2</sub>
</th>
<th align="center">Al<sub>2</sub>O<sub>3</sub>
</th>
<th align="center">TFe<sub>2</sub>O<sub>3</sub>
</th>
<th align="center">MnO</th>
<th align="center">MgO</th>
<th align="center">CaO</th>
<th align="center">Na<sub>2</sub>O</th>
<th align="center">K<sub>2</sub>O</th>
<th align="center">P<sub>2</sub>O<sub>5</sub>
</th>
<th align="center">LOI</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">JD15120</td>
<td align="left">Two-pyroxene granulite</td>
<td align="left">48.76</td>
<td align="left">0.76</td>
<td align="left">14.06</td>
<td align="left">12.56</td>
<td align="left">0.20</td>
<td align="left">7.90</td>
<td align="left">10.68</td>
<td align="left">2.88</td>
<td align="left">0.90</td>
<td align="left">0.11</td>
<td align="left">0.47</td>
</tr>
<tr>
<td align="left">YC8-43</td>
<td align="left">Garnet two-pyroxene granulite</td>
<td align="left">47.74</td>
<td align="left">0.92</td>
<td align="left">13.41</td>
<td align="left">14.14</td>
<td align="left">0.23</td>
<td align="left">7.51</td>
<td align="left">12.64</td>
<td align="left">2.05</td>
<td align="left">0.25</td>
<td align="left">0.08</td>
<td align="left">0.22</td>
</tr>
<tr>
<td align="left">JD1546</td>
<td align="left">Garnet clinopyroxene granulite</td>
<td align="left">47.41</td>
<td align="left">0.87</td>
<td align="left">12.02</td>
<td align="left">16.01</td>
<td align="left">0.21</td>
<td align="left">6.86</td>
<td align="left">11.60</td>
<td align="left">2.19</td>
<td align="left">0.81</td>
<td align="left">0.14</td>
<td align="left">1.21</td>
</tr>
<tr>
<td colspan="13" align="center">
<bold>Normalized molar proportions used for phase equilibria modeling (mole %)</bold>
</td>
</tr>
<tr>
<td align="left">
<bold>Sample</bold>
</td>
<td align="center">
<bold>Figure</bold>
</td>
<td align="left">
<bold>H<sub>2</sub>O</bold>
</td>
<td align="left">
<bold>SiO<sub>2</sub>
</bold>
</td>
<td align="left">
<bold>Al<sub>2</sub>O<sub>3</sub>
</bold>
</td>
<td align="left">
<bold>CaO</bold>
</td>
<td align="left">
<bold>MgO</bold>
</td>
<td align="left">
<bold>FeO</bold>
</td>
<td align="left">
<bold>K<sub>2</sub>O</bold>
</td>
<td align="left">
<bold>Na<sub>2</sub>O</bold>
</td>
<td align="left">
<bold>TiO<sub>2</sub>
</bold>
</td>
<td align="left">
<bold>O</bold>
</td>
<td align="left">
<bold>Mg<sup>&#x23;</sup>
</bold>
</td>
</tr>
<tr>
<td align="left">JD15120</td>
<td align="left">
<xref ref-type="fig" rid="F6">Figure 6A</xref>
</td>
<td align="left">2.51</td>
<td align="left">48.65</td>
<td align="left">8.45</td>
<td align="left">10.84</td>
<td align="left">12.16</td>
<td align="left">12.16</td>
<td align="left">0.69</td>
<td align="left">2.79</td>
<td align="left">0.85</td>
<td align="left">0.91</td>
<td align="left">50</td>
</tr>
<tr>
<td align="left">YC8-43</td>
<td align="left">
<xref ref-type="fig" rid="F7">Figure 7A</xref>
</td>
<td align="left">0.70</td>
<td align="left">50.36</td>
<td align="left">8.51</td>
<td align="left">13.20</td>
<td align="left">12.05</td>
<td align="left">11.22</td>
<td align="left">0.18</td>
<td align="left">2.10</td>
<td align="left">0.68</td>
<td align="left">1.00</td>
<td align="left">52</td>
</tr>
<tr>
<td align="left">YC8-43 (overprinting)</td>
<td align="left">
<xref ref-type="fig" rid="F7">Figure 7B</xref>
</td>
<td align="left">0.95</td>
<td align="left">50.50</td>
<td align="left">7.93</td>
<td align="left">12.11</td>
<td align="left">10.33</td>
<td align="left">14.09</td>
<td align="left">0.20</td>
<td align="left">1.56</td>
<td align="left">0.84</td>
<td align="left">1.48</td>
<td align="left">42</td>
</tr>
<tr>
<td align="left">JD1546</td>
<td align="left">
<xref ref-type="fig" rid="F8">Figure 8</xref>
</td>
<td align="left">1.20</td>
<td align="left">50.23</td>
<td align="left">8.14</td>
<td align="left">13.22</td>
<td align="left">11.15</td>
<td align="left">12.84</td>
<td align="left">0.18</td>
<td align="left">1.64</td>
<td align="left">0.70</td>
<td align="left">0.70</td>
<td align="left">46</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>Wt%, major element oxides in weight percent; LOI, loss on ignition; mole %, major element oxides in mole percent; Mg<sup>&#x23;</sup> &#x3d; MgO/(MgO &#x2b; FeO).</p>
</fn>
</table-wrap-foot>
</table-wrap>
</sec>
<sec id="s3-2">
<title>3.2 Petrography and Mineral Compositions</title>
<p>Mineral compositions were analyzed at the Laboratory of Orogenic Belt and Crustal Evolution of Peking University, China, using a JXA-8100 electron microprobe analyzer (EPM; JEOL). The analyses were conducted under operating conditions of 15&#xa0;KV accelerating voltage and 10&#xa0;nA probe current with a beam diameter of 2&#xa0;&#x3bc;m. Natural and synthetic minerals of the SPI Company were used for standardization. Representative mineral analyses are listed in <xref ref-type="table" rid="T2">Tables 2</xref>, <xref ref-type="table" rid="T3">3</xref>. Photomicrographs are shown in <xref ref-type="fig" rid="F3">Figures 3</xref>, <xref ref-type="fig" rid="F4">4</xref>.</p>
<table-wrap id="T2" position="float">
<label>TABLE 2</label>
<caption>
<p>Selected microprobe analyses for sample JD15120.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Mineral</th>
<th align="center">Cpx-1</th>
<th align="center">Opx-1</th>
<th align="center">Amp-1</th>
<th align="center">Pl-1-c</th>
<th align="center">Pl-1-r</th>
<th align="center">Cpx-2</th>
<th align="center">Opx-2</th>
<th align="center">Amp-2</th>
<th align="center">Pl-2</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">SiO<sub>2</sub>
</td>
<td align="center">52.25</td>
<td align="center">51.63</td>
<td align="char" char=".">42.13</td>
<td align="center">59.06</td>
<td align="center">60.03</td>
<td align="center">52.19</td>
<td align="center">50.97</td>
<td align="char" char=".">41.67</td>
<td align="center">59.05</td>
</tr>
<tr>
<td align="left">TiO<sub>2</sub>
</td>
<td align="center">0.08</td>
<td align="center">&#x2013;</td>
<td align="char" char=".">1.59</td>
<td align="center">0.03</td>
<td align="center">0.02</td>
<td align="center">0.14</td>
<td align="center">0.06</td>
<td align="char" char=".">1.22</td>
<td align="center">0.04</td>
</tr>
<tr>
<td align="left">Al<sub>2</sub>O<sub>3</sub>
</td>
<td align="center">2.21</td>
<td align="center">1.28</td>
<td align="char" char=".">11.81</td>
<td align="center">25.03</td>
<td align="center">24.95</td>
<td align="center">2.02</td>
<td align="center">1.40</td>
<td align="char" char=".">12.33</td>
<td align="center">24.55</td>
</tr>
<tr>
<td align="left">Cr<sub>2</sub>O<sub>3</sub>
</td>
<td align="center">&#x2013;</td>
<td align="center">0.02</td>
<td align="char" char=".">0.03</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.03</td>
<td align="char" char=".">0.04</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">Fe2O3</td>
<td align="center">0.47</td>
<td align="center">1.15</td>
<td align="char" char=".">1.53</td>
<td align="center">0.18</td>
<td align="center">0.40</td>
<td align="center">1.88</td>
<td align="center">0.79</td>
<td align="char" char=".">3.57</td>
<td align="center">1.86</td>
</tr>
<tr>
<td align="left">FeO</td>
<td align="center">9.75</td>
<td align="center">25.06</td>
<td align="char" char=".">12.98</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">7.28</td>
<td align="center">25.34</td>
<td align="char" char=".">11.74</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">MnO</td>
<td align="center">0.82</td>
<td align="center">2.45</td>
<td align="char" char=".">0.23</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.35</td>
<td align="center">1.22</td>
<td align="char" char=".">0.21</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">MgO</td>
<td align="center">12.28</td>
<td align="center">18.77</td>
<td align="char" char=".">11.16</td>
<td align="center">&#x2013;</td>
<td align="center">0.03</td>
<td align="center">13.08</td>
<td align="center">18.99</td>
<td align="char" char=".">11.09</td>
<td align="center">0.10</td>
</tr>
<tr>
<td align="left">CaO</td>
<td align="center">21.43</td>
<td align="center">0.46</td>
<td align="char" char=".">11.52</td>
<td align="center">8.03</td>
<td align="center">7.30</td>
<td align="center">22.65</td>
<td align="center">0.31</td>
<td align="char" char=".">10.83</td>
<td align="center">7.10</td>
</tr>
<tr>
<td align="left">Na<sub>2</sub>O</td>
<td align="center">0.56</td>
<td align="center">0.03</td>
<td align="char" char=".">1.56</td>
<td align="center">6.71</td>
<td align="center">7.17</td>
<td align="center">0.54</td>
<td align="center">0.04</td>
<td align="char" char=".">1.38</td>
<td align="center">6.96</td>
</tr>
<tr>
<td align="left">K<sub>2</sub>O</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="char" char=".">1.45</td>
<td align="center">0.31</td>
<td align="center">0.33</td>
<td align="center">0.02</td>
<td align="center">&#x2013;</td>
<td align="char" char=".">1.53</td>
<td align="center">0.29</td>
</tr>
<tr>
<td align="left">Total</td>
<td align="center">99.81</td>
<td align="center">100.75</td>
<td align="char" char=".">95.84</td>
<td align="center">99.35</td>
<td align="center">100.24</td>
<td align="center">99.97</td>
<td align="center">99.07</td>
<td align="char" char=".">95.25</td>
<td align="center">99.95</td>
</tr>
<tr>
<td align="left">O</td>
<td align="center">6</td>
<td align="center">6</td>
<td align="char" char=".">23</td>
<td align="center">8</td>
<td align="center">8</td>
<td align="center">6</td>
<td align="center">6</td>
<td align="char" char=".">23</td>
<td align="center">8</td>
</tr>
<tr>
<td align="left">Si</td>
<td align="center">1.963</td>
<td align="center">1.956</td>
<td align="char" char=".">6.385</td>
<td align="center">2.655</td>
<td align="center">2.672</td>
<td align="center">1.945</td>
<td align="center">1.956</td>
<td align="char" char=".">6.326</td>
<td align="center">2.649</td>
</tr>
<tr>
<td align="left">Ti</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="char" char=".">0.181</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.004</td>
<td align="center">0.002</td>
<td align="char" char=".">0.139</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">Al</td>
<td align="center">0.098</td>
<td align="center">0.057</td>
<td align="char" char=".">2.110</td>
<td align="center">1.327</td>
<td align="center">1.310</td>
<td align="center">0.089</td>
<td align="center">0.063</td>
<td align="char" char=".">2.207</td>
<td align="center">1.298</td>
</tr>
<tr>
<td align="left">Cr</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="char" char=".">0.004</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="char" char=".">0.005</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">Fe<sup>3&#x2b;</sup>
</td>
<td align="center">0.013</td>
<td align="center">0.033</td>
<td align="char" char=".">0.175</td>
<td align="center">0.006</td>
<td align="center">0.013</td>
<td align="center">0.053</td>
<td align="center">0.023</td>
<td align="char" char=".">0.408</td>
<td align="center">0.063</td>
</tr>
<tr>
<td align="left">Fe<sup>2&#x2b;</sup>
</td>
<td align="center">0.306</td>
<td align="center">0.794</td>
<td align="char" char=".">1.645</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.227</td>
<td align="center">0.813</td>
<td align="char" char=".">1.490</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">Mn</td>
<td align="center">0.026</td>
<td align="center">0.079</td>
<td align="char" char=".">0.030</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.011</td>
<td align="center">0.040</td>
<td align="char" char=".">0.027</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">Mg</td>
<td align="center">0.688</td>
<td align="center">1.060</td>
<td align="char" char=".">2.521</td>
<td align="center">&#x2013;</td>
<td align="center">0.002</td>
<td align="center">0.727</td>
<td align="center">1.086</td>
<td align="char" char=".">2.509</td>
<td align="center">0.007</td>
</tr>
<tr>
<td align="left">Ca</td>
<td align="center">0.863</td>
<td align="center">0.019</td>
<td align="char" char=".">1.871</td>
<td align="center">0.387</td>
<td align="center">0.348</td>
<td align="center">0.905</td>
<td align="center">0.013</td>
<td align="char" char=".">1.762</td>
<td align="center">0.341</td>
</tr>
<tr>
<td align="left">Na</td>
<td align="center">0.041</td>
<td align="center">0.002</td>
<td align="char" char=".">0.458</td>
<td align="center">0.585</td>
<td align="center">0.619</td>
<td align="center">0.039</td>
<td align="center">0.003</td>
<td align="char" char=".">0.406</td>
<td align="center">0.605</td>
</tr>
<tr>
<td align="left">K</td>
<td align="center">0.000</td>
<td align="center">0.000</td>
<td align="char" char=".">0.280</td>
<td align="center">0.018</td>
<td align="center">0.019</td>
<td align="center">0.001</td>
<td align="center">0.000</td>
<td align="char" char=".">0.296</td>
<td align="center">0.017</td>
</tr>
<tr>
<td align="left">
<italic>X</italic>(phase)</td>
<td align="center">0.69</td>
<td align="center">0.57</td>
<td align="char" char=".">0.61</td>
<td align="center">0.39</td>
<td align="center">0.35</td>
<td align="center">0.76</td>
<td align="center">0.57</td>
<td align="char" char=".">0.63</td>
<td align="center">0.35</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>
<italic>X</italic>(Cpx) &#x3d; <italic>X</italic>(Opx) &#x3d; <italic>X</italic>(Amp) &#x3d; Mg/(Fe<sup>2&#x2b;</sup>&#x2b;Mg); <italic>X</italic>(Pl) &#x3d; <italic>X</italic>
<sub>An</sub> &#x3d; Ca/(Ca &#x2b; Na &#x2b; K); -c, grain core; -r, grain rim. &#x201c;&#x2013;&#x201d; means that the content is below the detection limit. The mineral formulas were calculated with the program AX (Holland; <ext-link ext-link-type="uri" xlink:href="http://www.esc.cam.ac.uk/astaff/holland/ax.html">http://www.esc.cam.ac.uk/astaff/holland/ax.html</ext-link>).</p>
</fn>
</table-wrap-foot>
</table-wrap>
<table-wrap id="T3" position="float">
<label>TABLE 3</label>
<caption>
<p>Selected microprobe analyses for samples YC8-43 and JD1546.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left" rowspan="2">Mineral</th>
<th colspan="10" align="center">YC8-43</th>
<th colspan="6" align="center">JD1546</th>
</tr>
<tr>
<th align="center">Cpx-1</th>
<th align="center">Opx</th>
<th align="center">Amp</th>
<th align="center">Pl-1-c</th>
<th align="center">Pl-1-r</th>
<th align="center">Cpx-2</th>
<th align="center">Grt-c</th>
<th align="center">Grt-r</th>
<th align="center">Pl-2-c</th>
<th align="center">Pl-2-r</th>
<th align="center">Cpx</th>
<th align="center">Grt-c</th>
<th align="center">Grt-r</th>
<th align="center">Amp</th>
<th align="center">Pl-c</th>
<th align="center">Pl-r</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">SiO<sub>2</sub>
</td>
<td align="center">51.01</td>
<td align="center">51.29</td>
<td align="char" char=".">41.59</td>
<td align="center">54.31</td>
<td align="center">57.23</td>
<td align="center">52.05</td>
<td align="center">36.83</td>
<td align="center">38.72</td>
<td align="center">61.24</td>
<td align="center">59.09</td>
<td align="center">51.99</td>
<td align="center">38.36</td>
<td align="center">37.69</td>
<td align="char" char=".">42.23</td>
<td align="center">61.60</td>
<td align="center">60.03</td>
</tr>
<tr>
<td align="left">TiO<sub>2</sub>
</td>
<td align="center">0.22</td>
<td align="center">0.03</td>
<td align="char" char=".">2.29</td>
<td align="center">0.06</td>
<td align="center">&#x2013;</td>
<td align="center">0.20</td>
<td align="center">&#x2013;</td>
<td align="center">0.09</td>
<td align="center">0.07</td>
<td align="center">0.05</td>
<td align="center">0.25</td>
<td align="center">0.06</td>
<td align="center">0.10</td>
<td align="char" char=".">2.07</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">Al<sub>2</sub>O<sub>3</sub>
</td>
<td align="center">3.21</td>
<td align="center">2.33</td>
<td align="char" char=".">12.61</td>
<td align="center">29.59</td>
<td align="center">27.46</td>
<td align="center">2.72</td>
<td align="center">20.43</td>
<td align="center">20.09</td>
<td align="center">24.35</td>
<td align="center">25.03</td>
<td align="center">3.63</td>
<td align="center">20.30</td>
<td align="center">20.32</td>
<td align="char" char=".">12.42</td>
<td align="center">24.42</td>
<td align="center">25.73</td>
</tr>
<tr>
<td align="left">Cr<sub>2</sub>O<sub>3</sub>
</td>
<td align="center">&#x2013;</td>
<td align="center">0.02</td>
<td align="char" char=".">0.03</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.17</td>
<td align="center">&#x2013;</td>
<td align="center">0.06</td>
<td align="center">0.04</td>
<td align="center">0.04</td>
<td align="center">0.04</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="char" char=".">0.02</td>
<td align="center">0.04</td>
<td align="center">0.03</td>
</tr>
<tr>
<td align="left">Fe2O3</td>
<td align="center">2.89</td>
<td align="center">1.75</td>
<td align="char" char=".">1.89</td>
<td align="center">0.17</td>
<td align="center">0.14</td>
<td align="center">1.52</td>
<td align="center">4.72</td>
<td align="center">0.84</td>
<td align="center">0.09</td>
<td align="center">0.39</td>
<td align="center">1.71</td>
<td align="center">2.17</td>
<td align="center">3.00</td>
<td align="char" char=".">2.10</td>
<td align="center">0.09</td>
<td align="center">0.16</td>
</tr>
<tr>
<td align="left">FeO</td>
<td align="center">9.07</td>
<td align="center">23.34</td>
<td align="char" char=".">13.32</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">8.06</td>
<td align="center">21.02</td>
<td align="center">25.47</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">9.67</td>
<td align="center">23.29</td>
<td align="center">23.91</td>
<td align="char" char=".">13.50</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">MnO</td>
<td align="center">0.26</td>
<td align="center">1.08</td>
<td align="char" char=".">0.04</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.17</td>
<td align="center">1.12</td>
<td align="center">1.23</td>
<td align="center">&#x2013;</td>
<td align="center">0.05</td>
<td align="center">0.09</td>
<td align="center">1.21</td>
<td align="center">1.26</td>
<td align="char" char=".">0.09</td>
<td align="center">0.04</td>
<td align="center">0.03</td>
</tr>
<tr>
<td align="left">MgO</td>
<td align="center">12.24</td>
<td align="center">20.26</td>
<td align="char" char=".">11.22</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">12.34</td>
<td align="center">5.45</td>
<td align="center">5.81</td>
<td align="center">0.02</td>
<td align="center">0.05</td>
<td align="center">11.83</td>
<td align="center">5.11</td>
<td align="center">5.73</td>
<td align="char" char=".">11.11</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">CaO</td>
<td align="center">20.41</td>
<td align="center">0.56</td>
<td align="char" char=".">11.58</td>
<td align="center">12.03</td>
<td align="center">9.58</td>
<td align="center">21.90</td>
<td align="center">9.50</td>
<td align="center">7.22</td>
<td align="center">5.97</td>
<td align="center">6.96</td>
<td align="center">20.82</td>
<td align="center">9.47</td>
<td align="center">7.35</td>
<td align="char" char=".">11.47</td>
<td align="center">5.79</td>
<td align="center">7.05</td>
</tr>
<tr>
<td align="left">Na<sub>2</sub>O</td>
<td align="center">0.84</td>
<td align="center">0.02</td>
<td align="char" char=".">1.69</td>
<td align="center">4.64</td>
<td align="center">6.04</td>
<td align="center">0.89</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">8.44</td>
<td align="center">7.61</td>
<td align="center">1.05</td>
<td align="center">0.03</td>
<td align="center">0.06</td>
<td align="char" char=".">1.61</td>
<td align="center">8.47</td>
<td align="center">7.43</td>
</tr>
<tr>
<td align="left">K<sub>2</sub>O</td>
<td align="center">0.00</td>
<td align="center">0.00</td>
<td align="char" char=".">1.71</td>
<td align="center">0.24</td>
<td align="center">0.27</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.02</td>
<td align="center">0.25</td>
<td align="center">0.27</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.02</td>
<td align="char" char=".">1.72</td>
<td align="center">0.30</td>
<td align="center">0.21</td>
</tr>
<tr>
<td align="left">Total</td>
<td align="center">99.86</td>
<td align="center">100.50</td>
<td align="char" char=".">97.78</td>
<td align="center">101.04</td>
<td align="center">100.74</td>
<td align="center">99.87</td>
<td align="center">98.61</td>
<td align="center">99.46</td>
<td align="center">100.47</td>
<td align="center">99.54</td>
<td align="center">100.91</td>
<td align="center">99.79</td>
<td align="center">99.14</td>
<td align="char" char=".">98.13</td>
<td align="center">100.77</td>
<td align="center">100.67</td>
</tr>
<tr>
<td align="left">O</td>
<td align="center">6</td>
<td align="center">6</td>
<td align="char" char=".">23</td>
<td align="center">8</td>
<td align="center">8</td>
<td align="center">6</td>
<td align="center">12</td>
<td align="center">12</td>
<td align="center">8</td>
<td align="center">8</td>
<td align="center">6</td>
<td align="center">12</td>
<td align="center">12</td>
<td align="char" char=".">23</td>
<td align="center">8</td>
<td align="center">8</td>
</tr>
<tr>
<td align="left">Si</td>
<td align="center">1.913</td>
<td align="center">1.924</td>
<td align="char" char=".">6.206</td>
<td align="center">2.430</td>
<td align="center">2.551</td>
<td align="center">1.943</td>
<td align="center">2.909</td>
<td align="center">3.040</td>
<td align="center">2.713</td>
<td align="center">2.654</td>
<td align="center">1.927</td>
<td align="center">3.000</td>
<td align="center">2.968</td>
<td align="char" char=".">6.274</td>
<td align="center">2.720</td>
<td align="center">2.658</td>
</tr>
<tr>
<td align="left">Ti</td>
<td align="center">0.006</td>
<td align="center">&#x2013;</td>
<td align="char" char=".">0.257</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.006</td>
<td align="center">&#x2013;</td>
<td align="center">0.005</td>
<td align="center">0.002</td>
<td align="center">0.002</td>
<td align="center">0.007</td>
<td align="center">0.004</td>
<td align="center">0.006</td>
<td align="char" char=".">0.231</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">Al</td>
<td align="center">0.142</td>
<td align="center">0.103</td>
<td align="char" char=".">2.218</td>
<td align="center">1.561</td>
<td align="center">1.443</td>
<td align="center">0.120</td>
<td align="center">1.902</td>
<td align="center">1.859</td>
<td align="center">1.272</td>
<td align="center">1.325</td>
<td align="center">0.159</td>
<td align="center">1.871</td>
<td align="center">1.886</td>
<td align="char" char=".">2.175</td>
<td align="center">1.271</td>
<td align="center">1.343</td>
</tr>
<tr>
<td align="left">Cr</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="char" char=".">0.004</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.005</td>
<td align="center">&#x2013;</td>
<td align="center">0.004</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="char" char=".">0.002</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">Fe<sup>3&#x2b;</sup>
</td>
<td align="center">0.081</td>
<td align="center">0.049</td>
<td align="char" char=".">0.212</td>
<td align="center">0.006</td>
<td align="center">0.005</td>
<td align="center">0.042</td>
<td align="center">0.279</td>
<td align="center">0.049</td>
<td align="center">0.003</td>
<td align="center">0.013</td>
<td align="center">0.048</td>
<td align="center">0.128</td>
<td align="center">0.178</td>
<td align="char" char=".">0.235</td>
<td align="center">0.003</td>
<td align="center">0.005</td>
</tr>
<tr>
<td align="left">Fe<sup>2&#x2b;</sup>
</td>
<td align="center">0.284</td>
<td align="center">0.732</td>
<td align="char" char=".">1.662</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.252</td>
<td align="center">1.389</td>
<td align="center">1.672</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.300</td>
<td align="center">1.523</td>
<td align="center">1.575</td>
<td align="char" char=".">1.677</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">Mn</td>
<td align="center">0.008</td>
<td align="center">0.034</td>
<td align="char" char=".">0.005</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.005</td>
<td align="center">0.075</td>
<td align="center">0.082</td>
<td align="center">&#x2013;</td>
<td align="center">0.002</td>
<td align="center">0.003</td>
<td align="center">0.080</td>
<td align="center">0.084</td>
<td align="char" char=".">0.011</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">Mg</td>
<td align="center">0.684</td>
<td align="center">1.132</td>
<td align="char" char=".">2.495</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.687</td>
<td align="center">0.641</td>
<td align="center">0.680</td>
<td align="center">0.001</td>
<td align="center">0.003</td>
<td align="center">0.653</td>
<td align="center">0.596</td>
<td align="center">0.672</td>
<td align="char" char=".">2.460</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
</tr>
<tr>
<td align="left">Ca</td>
<td align="center">0.820</td>
<td align="center">0.023</td>
<td align="char" char=".">1.852</td>
<td align="center">0.577</td>
<td align="center">0.457</td>
<td align="center">0.876</td>
<td align="center">0.804</td>
<td align="center">0.607</td>
<td align="center">0.283</td>
<td align="center">0.335</td>
<td align="center">0.827</td>
<td align="center">0.793</td>
<td align="center">0.620</td>
<td align="char" char=".">1.826</td>
<td align="center">0.274</td>
<td align="center">0.334</td>
</tr>
<tr>
<td align="left">Na</td>
<td align="center">0.061</td>
<td align="center">0.002</td>
<td align="char" char=".">0.489</td>
<td align="center">0.403</td>
<td align="center">0.522</td>
<td align="center">0.064</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.725</td>
<td align="center">0.663</td>
<td align="center">0.075</td>
<td align="center">0.005</td>
<td align="center">0.009</td>
<td align="char" char=".">0.464</td>
<td align="center">0.725</td>
<td align="center">0.638</td>
</tr>
<tr>
<td align="left">K</td>
<td align="center">0.000</td>
<td align="center">0.000</td>
<td align="char" char=".">0.326</td>
<td align="center">0.014</td>
<td align="center">0.015</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.002</td>
<td align="center">0.014</td>
<td align="center">0.015</td>
<td align="center">&#x2013;</td>
<td align="center">&#x2013;</td>
<td align="center">0.002</td>
<td align="char" char=".">0.326</td>
<td align="center">0.017</td>
<td align="center">0.012</td>
</tr>
<tr>
<td align="left">
<italic>X</italic>(phase)</td>
<td align="center">0.71</td>
<td align="center">0.61</td>
<td align="char" char=".">0.60</td>
<td align="center">0.58</td>
<td align="center">0.46</td>
<td align="center">0.73</td>
<td align="center">0.22</td>
<td align="center">0.22</td>
<td align="center">0.28</td>
<td align="center">0.33</td>
<td align="center">0.69</td>
<td align="center">0.20</td>
<td align="center">0.23</td>
<td align="char" char=".">0.59</td>
<td align="center">0.27</td>
<td align="center">0.34</td>
</tr>
<tr>
<td align="left">
<italic>Y</italic>(phase)</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="center">0.28</td>
<td align="center">0.20</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
<td align="center">0.27</td>
<td align="center">0.21</td>
<td align="left"/>
<td align="left"/>
<td align="left"/>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>
<p>
<italic>X</italic>(Grt) &#x3d; <italic>X</italic>
<sub>Py</sub> &#x3d; Mg/(Fe<sup>2&#x2b;</sup>&#x2b;Mg &#x2b; Ca &#x2b; Mn); <italic>Y</italic>(Grt) &#x3d; <italic>X</italic>
<sub>Grs</sub> &#x3d; Ca/(Fe<sup>2&#x2b;</sup>&#x2b;Mg &#x2b; Ca &#x2b; Mn); others are as in <xref ref-type="table" rid="T2">Table 2</xref>.</p>
</fn>
</table-wrap-foot>
</table-wrap>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Photomicrographs of sample JD15120. <bold>(A,B)</bold> Coexistence of medium-grained Cpx-1, Opx-1, Pl-1, Amp-1, and ilmenite. <bold>(C,D)</bold> Vermicular minerals of Cpx-2, Opx-2, Amp-2, Pl-2, and quartz along the margin of Amp-1 and Pl-1.</p>
</caption>
<graphic xlink:href="feart-10-894353-g003.tif"/>
</fig>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Photomicrographs of samples YC8-43 and JD1546: <bold>(A)</bold> Large-scale photograph showing mineral relations that medium-grained orthopyroxene, Cpx-1, Pl-1, and amphibole are overprinted by fine-grained garnet, Cpx-2, Pl-2, and quartz in YC8-43; <bold>(B,C)</bold> poikilitic garnet with worm-like quartz inclusions occurring with fine-grained Cpx-2 and Pl-2 around medium-grained Cpx-1 and orthopyroxene in YC8-43; <bold>(D)</bold> garnet occurring as &#x201c;red-eye pocket&#x201d; separating Cpx-1 from Pl-1 in YC8-43; and <bold>(E,F)</bold> photomicrographs of the sample JD1546 showing the coexistence of fine-grained garnet, clinopyroxene, amphibole, and plagioclase with minor amounts of quartz and biotite.</p>
</caption>
<graphic xlink:href="feart-10-894353-g004.tif"/>
</fig>
<p>Sample JD15120 is a two-pyroxene granulite with a weak foliation, comprising mostly clinopyroxene (25&#xa0;vol%), orthopyroxene (15&#xa0;vol%), amphibole (27&#xa0;vol%), plagioclase (30&#xa0;vol%), and minor amounts of biotite, quartz, and ilmenite. It shows overall equigranular texture, where the fine-to medium-grained (0.2&#x2013;1.0&#xa0;mm across) clinopyroxene, orthopyroxene, amphibole, and plagioclase directly contact with each other (hereafter Cpx-1, Opx-1, Amp-1, and Pl-1, respectively) (<xref ref-type="fig" rid="F3">Figures 3A,B</xref>). Amp-1 can also occur surrounding or replacing clinopyroxene at rims, suggesting later growth (<xref ref-type="fig" rid="F3">Figure 3B</xref>). Occasionally, there are vermiform minerals of &#x3c;0.1&#xa0;mm, including clinopyroxene, orthopyroxene, amphibole, and plagioclase (hereafter Cpx-2, Opx-2, Amp-2, and Pl-2 respectively), occurring as coronae around Amp-1 or along the boundary between Amp-1 and Pl-1 (<xref ref-type="fig" rid="F3">Figures 3C,D</xref>). Clinopyroxene (Cpx-1 and Cpx-2) shows similar diopsidic compositions with En [ &#x3d; Mg/(Ca &#x2b; Mg &#x2b; Fe<sup>2&#x2b;</sup>)] of 0.36&#x2013;0.39, Fs [ &#x3d; Fe<sup>2&#x2b;</sup>/(Ca &#x2b; Mg &#x2b; Fe<sup>2&#x2b;</sup>)] of 0.12&#x2013;0.16, Wo [ &#x3d; Ca/(Ca &#x2b; Mg &#x2b; Fe<sup>2&#x2b;</sup>)] of 0.46&#x2013;0.49, and <italic>X</italic>
<sub>Mg</sub> [ &#x3d; Mg/(Mg &#x2b; Fe<sup>2&#x2b;</sup>)] of 0.68&#x2013;0.76 (<xref ref-type="bibr" rid="B61">Morimoto 1988</xref>), but Cpx-1 occasionally has exsolution lamellae of ilmenite in the core. Orthopyroxene (both Opx-1 and Opx-2) has composition of hypersthene with En of 0.52&#x2013;0.57, Fs of 0.42&#x2013;0.47, Wo of &#x223c;0.01, and <italic>X</italic>
<sub>Mg</sub> of 0.52&#x2013;0.67 (<xref ref-type="bibr" rid="B61">Morimoto 1988</xref>). Amphibole (Amp-1 and Amp-2) has similar composition of pargasite involving K<sub>2</sub>O of 1.45&#x2013;1.82&#xa0;wt%, Ca<sub>B</sub> &#x3d; 1.76&#x2013;1.89, (Na &#x2b; K)<sub>A</sub> &#x3d; 0.56&#x2013;0.73, Si &#x3d; 6.29&#x2013;6.39, and <italic>X</italic>
<sub>Mg</sub> &#x3d; 0.52&#x2013;0.63 (<xref ref-type="bibr" rid="B42">Leake et al., 2003</xref>), but higher Ti of 0.18&#x2013;0.28&#xa0;p. f.u. in Amp-1 and lower Ti of 0.10&#x2013;0.14&#xa0;p. f.u. in Amp-2. Plagioclase commonly has cuspate boundaries. Pl-1 has chemical zonation with a constant <italic>X</italic>
<sub>An</sub> &#x3d; Ca/(Ca &#x2b; Na &#x2b; K)] of 0.39&#x2013;0.41 in the core but outward decreasing to 0.34&#x2013;0.36 in the rim (<xref ref-type="fig" rid="F5">Figure 5A</xref>), while Pl-2 shows slightly lower <italic>X</italic>
<sub>An</sub> of 0.35&#x2013;0.39. A few biotite flakes occur around Amp-1 or Cpx-1, suggesting their later growth. Additionally, ilmenite occurs as anhedral grains, and minor amounts of quartz exhibit as irregular shapes coexisting with the rim of Pl-1, or as vermiform grains in coronae. On the basis of the mineral relations and compositions, two generations of assemblage can be inferred for the sample. The first generation comprises the fine-to-medium-grained minerals that include the peak and final stages. The peak assemblage is featured with the coexistence of Cpx-1, Opx-1, Amp-1, Pl-1, and ilmenite, while the final assemblage is characterized by the re-growth of Amp-1 and Pl-1 and the emergence of biotite and quartz. The second generation of assemblage consists of the vermiform minerals of Cpx-2, Opx-2, Amp-2, Pl-2, and Qz in the coronae mostly around Amp-1.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Composition zoning profiles for plagioclase in JD15120 <bold>(A)</bold>, YC8-43 <bold>(B)</bold>, and JD1546 <bold>(C)</bold>, and for garnet in YC8-43 <bold>(D)</bold> and JD1546 <bold>(E)</bold>.</p>
</caption>
<graphic xlink:href="feart-10-894353-g005.tif"/>
</fig>
<p>Sample YC8-43 is a garnet-bearing two-pyroxene granulite, comprising clinopyroxene (20&#xa0;vol%), orthopyroxene (17&#xa0;vol%), garnet (15&#xa0;vol%), amphibole (15&#xa0;vol%), plagioclase (30&#xa0;vol%), ilmenite (3&#xa0;vol%), and minor amounts of quartz, biotite, and rutile (<xref ref-type="fig" rid="F4">Figures 4A&#x2013;D</xref>). Clinopyroxene occur either as subhedral to anhedral grains of 0.3&#x2013;1.2&#xa0;mm in contact with orthopyroxene (hereafter Cpx-1), or as irregular grains of &#x3c;0.2&#xa0;mm coexisting with garnet (hereafter Cpx-2). Both of the two types have similar diopsidic compositions with En of 0.36&#x2013;0.38, Fs of 0.14&#x2013;0.17, Wo of 0.46&#x2013;0.48, and <italic>X</italic>
<sub>Mg</sub> of 0.67&#x2013;0.73 (<xref ref-type="bibr" rid="B61">Morimoto 1988</xref>). Orthopyroxene shows as anhedral grains of 0.3&#x2013;1.8&#xa0;mm and has hypersthene compositions, containing En of 0.60&#x2013;0.63, Fs of 0.37&#x2013;0.39, Wo of &#x223c;0.01, and <italic>X</italic>
<sub>Mg</sub> of 0.61&#x2013;0.63 (<xref ref-type="bibr" rid="B61">Morimoto 1988</xref>). Plagioclase is subdivided into tabular grains of 0.3&#x2013;1.5&#xa0;mm in diameter (Pl-1) or irregular grains of &#x3c;0.3&#xa0;mm (Pl-2). Pl-1 mostly contacts to Cpx-1, orthopyroxene and amphibole, but occasionally be separated from pyroxenes by garnet (<xref ref-type="fig" rid="F4">Figures 4C,D</xref>). It exhibits core-to-rim zoning with <italic>X</italic>
<sub>An</sub> decreasing from 0.56 to 0.59 in the core to 0.38&#x2013;0.47 in the rim (<xref ref-type="fig" rid="F5">Figure 5B</xref>). Pl-2 occurs with garnet and Cpx-2, exhibiting core to rim zoning with increasing <italic>X</italic>
<sub>An</sub> from 0.28 to 0.34 (<xref ref-type="fig" rid="F5">Figure 5B</xref>). Garnet is 0.2&#x2013;0.5&#xa0;mm poikilitic grains with numerous quartz inclusions (<xref ref-type="fig" rid="F4">Figures 4B&#x2013;D</xref>). It occurs alone or with Cpx-2 surrounding Cpx-1 and/or orthopyroxene, forming &#x201c;red-eye socket&#x201d; textures to separate Cpx-1 and orthopyroxene from Pl-1 (<xref ref-type="fig" rid="F4">Figures 4C,D</xref>; <xref ref-type="bibr" rid="B87">Wei et al., 2014</xref>). It has almost constant <italic>X</italic>
<sub>Py</sub> [&#x3d; Mg/(Ca &#x2b; Mg &#x2b; Fe<sup>2&#x2b;</sup>&#x2b;Mn), defined accordingly for other components] mostly of 0.21&#x2013;0.23 (with a maximum of 0.25) and <italic>X</italic>
<sub>Sps</sub> of &#x223c;0.03, but shows core-to-rim increasing <italic>X</italic>
<sub>Alm</sub> (0.48&#x2192;0.56) and decreasing <italic>X</italic>
<sub>Grs</sub> (0.28&#x2192;0.20) (<xref ref-type="fig" rid="F5">Figure 5D</xref>). Amphibole is mostly anhedral grains with sizes of 0.2&#x2013;0.8&#xa0;mm directly contacting to pyroxenes, or irregular shapes surrounding Cpx-1, showing later growth. It has pargasite compositions (<xref ref-type="bibr" rid="B42">Leake et al., 2003</xref>) involving K<sub>2</sub>O of 1.53&#x2013;1.71&#xa0;wt%, Ca<sub>B</sub> &#x3d; 1.83&#x2013;1.85, (Na &#x2b; K)<sub>A</sub> &#x3d; 0.60&#x2013;0.73, Si &#x3d; 6.21&#x2013;6.37, Ti &#x3d; 0.24&#x2013;0.26&#xa0;p. f.u. and <italic>X</italic>
<sub>Mg</sub> &#x3d; 0.55&#x2013;0.60 (<xref ref-type="bibr" rid="B100">Yang and Wei 2017a</xref>). Biotite occurs around amphibole, indicating their later growth. Ilmenite is irregular grains among minerals or as rounded grains within Cpx-1. It can also be included in garnet. Minor amounts of rutile occur as inclusions in garnet. Quartz occurs as interstitial grains among minerals, or as vermicular inclusions in garnet. Based on petrological observations and mineral compositions, two generations of mineral assemblage can be inferred. The first generation is recognized to involve final and peak stages. The peak stage is marked by the coexistence of Cpx-1, orthopyroxene, Pl-1, amphibole, and ilmenite, while the final is featured with the growth of biotite and quartz. The second generation is characterized by the coexistence of poikilitic garnet, Cpx-2, Pl-2, quartz, and rutile.</p>
<p>Sample JD1546 is a garnet-clinopyroxene granulite, consisting of clinopyroxene (30&#xa0;vol%), garnet (23&#xa0;vol%), amphibole (17&#xa0;vol%), plagioclase (28&#xa0;vol%), ilmenite (2&#xa0;vol%), and minor amounts of quartz and biotite (<xref ref-type="fig" rid="F4">Figures 4E,F</xref>). The sample has an equigranular texture with grain sizes mostly of 0.1&#x2013;0.5&#xa0;mm, except for a few larger-sized clinopyroxene grains of 1.0&#x2013;1.5&#xa0;mm. Clinopyroxene has diopsidic compositions with En of 0.37&#x2013;0.40, Fs of 0.12&#x2013;0.17, Wo of 0.43&#x2013;0.50, and <italic>X</italic>
<sub>Mg</sub> of 0.69&#x2013;0.77 (<xref ref-type="bibr" rid="B61">Morimoto 1988</xref>). Plagioclase is anhedral, and exhibits core-to-rim zoning with increasing <italic>X</italic>
<sub>An</sub> from 0.27 to 0.35 (<xref ref-type="fig" rid="F5">Figure 5C</xref>). Garnet occurs normally with clinopyroxene or as &#x201c;red-eye socket&#x201d; textures around clinopyroxene. It exhibits core-to-rim decreasing <italic>X</italic>
<sub>Grs</sub> of 0.27&#x2192;0.21 and increasing <italic>X</italic>
<sub>Alm</sub> of 0.50&#x2192;0.55, but contains almost constant <italic>X</italic>
<sub>Py</sub> of 0.20&#x2013;0.23 and <italic>X</italic>
<sub>Sps</sub> of &#x223c;0.03 (<xref ref-type="fig" rid="F5">Figure 5E</xref>). Amphibole is mostly irregular grains with cuspate boundaries, and has pargasite compositions with K<sub>2</sub>O of 1.72&#x2013;1.92&#xa0;wt%, Ca<sub>B</sub> &#x3d; 1.78&#x2013;1.83, (Na &#x2b; K)<sub>A</sub> &#x3d; 0.63&#x2013;0.68, Si &#x3d; 6.16&#x2013;6.27, Ti &#x3d; 0.20&#x2013;0.23&#xa0;p. f.u., and <italic>X</italic>
<sub>Mg</sub> &#x3d; 0.59&#x2013;0.63 (<xref ref-type="bibr" rid="B42">Leake et al., 2003</xref>). Minor amounts of biotite display as irregular flakes or sticks around amphibole or clinopyroxene, suggesting their later formation. Quartz mostly occurs as interstitial grains among other minerals. Ilmenite and rutile occur as irregular grains or as inclusions in garnet. Based on the aforementioned textural relations, the peak assemblage is inferred to involve clinopyroxene, garnet, amphibole, plagioclase, and rutile, and the later growth of amphibole and biotite may represent the post-peak evolution. Presence of the larger-sized clinopyroxene might represent the relicts from an earlier metamorphism.</p>
</sec>
</sec>
<sec id="s4">
<title>4 Metamorphic <italic>P&#x2013;T</italic> Conditions</title>
<p>Pseudosection modeling for these samples was conducted using THERMOCALC 3.50 and the internally consistent thermodynamic dataset of <xref ref-type="bibr" rid="B30">Holland and Powell (2011)</xref> update (ds62) in the system NCKFMASHTO (Na<sub>2</sub>O&#x2013;CaO&#x2013;K<sub>2</sub>O&#x2013;FeO&#x2013;MgO&#x2013;Al<sub>2</sub>O<sub>3</sub>&#x2013;SiO<sub>2</sub>&#x2013;H<sub>2</sub>O&#x2013;TiO<sub>2</sub>&#x2013;Fe<sub>2</sub>O<sub>3</sub>). Mixing models are those presented for garnet, orthopyroxene, and biotite (<xref ref-type="bibr" rid="B88">White et al., 2014</xref>), melt, clinopyroxene, and amphibole (<xref ref-type="bibr" rid="B20">Green et al., 2016</xref>), plagioclase (<xref ref-type="bibr" rid="B31">Holland and Powell 2003</xref>), and ilmenite (<xref ref-type="bibr" rid="B89">White et al., 2000</xref>). Among these models, amphibole model &#x201c;hb&#x201d; and clinopyroxene model &#x201c;aug&#x201d; were used because they are suit for clinoamphibole including pargasite, and for high-temperature clinopyroxene, respectively. As JD15120 and JD1546 are overall homogeneous, the analyzed bulk-rock compositions were used for the phase equilibria modeling. Whereas for YC8-43, the first generation of assemblages was modeled using the analyzed composition, and the second generation of assemblages was calculated based on an effective composition, generated on the basis of mass balance by integrating modal abundance and compositions of relevant minerals together (<xref ref-type="bibr" rid="B7">Carson et al., 1999</xref>). The H<sub>2</sub>O contents and O (Fe<sub>2</sub>O<sub>3</sub>) values used in the modeling was defined using <italic>T</italic>&#x2013;<italic>M</italic> (H<sub>2</sub>O) and <italic>T</italic>&#x2013;<italic>M</italic>(O) diagrams (e.g., <xref ref-type="bibr" rid="B38">Korhonen et al., 2011</xref>; <xref ref-type="bibr" rid="B37">Korhonen et al., 2012</xref>). Compositions used for modeling are presented in <xref ref-type="table" rid="T1">Table 1</xref>.</p>
<sec id="s4-1">
<title>4.1 Sample JD15120</title>
<p>The <italic>P&#x2013;T</italic> pseudosection for sample JD15120 was drawn within a <italic>P&#x2013;T</italic> range of 4&#x2013;10&#xa0;kbar and 700&#x2013;1,100&#xb0;C (<xref ref-type="fig" rid="F6">Figure 6A</xref>), contoured with isopleths of <italic>X</italic>
<sub>An</sub> in plagioclase and Ti in amphibole. The fluid-absent solidus occurs at temperatures of 830&#x2013;900&#xb0;C. The inferred peak assemblage involving medium-grained Cpx-1, Opx-1, Pl-1, Amph-1, and ilmenite is constrained under a large <italic>P&#x2013;T</italic> condition of &#x3c;8.5&#xa0;kbar/900&#x2013;1,010&#xb0;C, limited by the garnet-in curve on the high-<italic>P</italic> limit, and biotite-in and orthopyroxene-out curves on the low- and high-<italic>T</italic> limits. The maximum <italic>X</italic>
<sub>An</sub> of 0.39&#x2013;0.41 in the core of Pl-1 is plotted in the peak field and constrains a precise peak condition of 7.5&#x2013;8.5&#xa0;kbar/940&#x2013;960&#xb0;C with a temperature uncertainty of &#x223c;6&#xb0;C (two-sigma level) calculated using THERMOCALC. It needs to be mentioned that this uncertainty should be considered as a minimum because it is propagated from the uncertainty on the enthalpy alone and does not include other sources of uncertainty. The post-peak decompressional cooling is driven by the reaction Cpx &#x2b; Ilm &#x2b; Liq &#x3d; Opx &#x2b; Pl &#x2b; Amp &#x2b; Bt, responsible for later growth of biotite and Amp-1, and also the outward decreasing <italic>X</italic>
<sub>An</sub> in Pl-1. The measured maximum Ti of 0.28 in Amp-1 is plotted in the biotite-present field, yielding temperatures of &#x3e;910&#xb0;C, whereas the lower Ti values were plotted in the sub-solidus fields. However, the observed final assemblage marked by the presence of quartz does not occur in <xref ref-type="fig" rid="F6">Figure 6A</xref>, probably because the residual melts that produced the final assemblage were locally segregated and not completely equilibrated with other minerals. Therefore, we calculated a <italic>T&#x2013;M</italic> (melt) pseudosection at 7&#xa0;kbar by adding more melts in the final mineral assemblage on <xref ref-type="fig" rid="F6">Figure 6A</xref>. As shown in <xref ref-type="fig" rid="F6">Figure 6B</xref>, the fluid-absent solidus occurs at lower temperatures as the melt modes increase, and the quartz-present final assemblage appears at &#x223c;810&#xb0;C on the solidus with the melt modes of 10&#x2013;20&#xa0;mol%. This field is well consistent with the measured <italic>X</italic>
<sub>An</sub> of 0.34&#x2013;0.36 in the rim of Pl-1. Moreover, the measured lower Ti values in amphibole can also plot in the suprasolidus fields. Therefore, a post-peak decompressional cooling process from the peak condition of 7.5&#x2013;8.5&#xa0;kbar/940&#x2013;960&#xb0;C to the final condition of &#x223c;7&#xa0;kbar/&#x223c;810&#xb0;C can be well constrained for JD15120.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>
<bold>(A)</bold> <italic>P&#x2013;T</italic> pseudosection with proposed <italic>P&#x2013;T</italic> path for sample JD15120 in the system NCKFMASHTO. Mineral abbreviations follow <xref ref-type="bibr" rid="B90">Whitney and Evans (2010)</xref>. Composition used for modeling the <italic>P&#x2013;T</italic> pseudosection is listed in <xref ref-type="table" rid="T1">Table 1</xref>. <bold>(B)</bold> <italic>T&#x2013;M</italic> (melt) diagram at 7&#xa0;kbar. The melt composition was defined at 7&#xa0;kbar and 904&#xb0;C in <xref ref-type="fig" rid="F6">Figure 6A</xref>, and the composition at <italic>M</italic> (melt) &#x3d; 0 equals to the composition for <xref ref-type="fig" rid="F6">Figure 6A</xref>.</p>
</caption>
<graphic xlink:href="feart-10-894353-g006.tif"/>
</fig>
</sec>
<sec id="s4-2">
<title>4.2 Sample YC8-43</title>
<p>The <italic>P&#x2013;T</italic> pseudosection for the first-generation of assemblages in YC8-43 was drawn within a <italic>P&#x2013;T</italic> range of 4&#x2013;10&#xa0;kbar and 750&#x2013;1,000&#xb0;C (<xref ref-type="fig" rid="F7">Figure 7A</xref>), contoured with isopleths of <italic>X</italic>
<sub>An</sub> in plagioclase and Ti in amphibole. The fluid-absent solidus occurs at temperatures of 860&#x2013;890&#xb0;C. The observed peak assemblage involving medium-grained Cpx-1, orthopyroxene, Pl-1, amphibole, and ilmenite is constrained under a large <italic>P&#x2013;T</italic> condition of &#x3c;8&#xa0;kbar/870&#x2013;1,000&#xb0;C, limited by the garnet-in curve on the high-<italic>P</italic> limit, and the liquid-out and amphibole-out curves on the low- and high-<italic>T</italic> limits. The measured maximum <italic>X</italic>
<sub>An</sub> of 0.59&#x2013;0.56 in the core of Pl-1 is plotted in the peak assemblage field, and yields a peak temperature of 950&#x2013;990&#xb0;C at 8&#xa0;kbar with the uncertainty of &#x223c;6&#xb0;C (two-sigma level). The post-peak decompression cooling is dominated by the reaction of Cpx &#x2b; Ilm &#x2b; Liq &#x3d; Opx &#x2b; Pl &#x2b; Amp, being responsible for the observed re-growth of amphibole and the core-to-rim decreasing <italic>X</italic>
<sub>An</sub> in Pl-1. The measured Ti of 0.24&#x2013;0.26 in amphibole is consistent with the cooling evolution. Similar to JD15120, the quartz-present final assemblage and the measured <italic>X</italic>
<sub>An</sub> of 0.38&#x2013;0.47 in the rim of Pl-1 do not occur in the pseudosection, as a result of local segregation of residual melts. This can be solved using an alternative pseudosection as in <xref ref-type="fig" rid="F6">Figure 6B</xref>.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>
<italic>P&#x2013;T</italic> pseudosection with the proposed <italic>P&#x2013;T</italic> path for the first-episode metamorphism <bold>(A)</bold> and second-episode metamorphism <bold>(B)</bold> in the sample YC8-43. Others are same as <xref ref-type="fig" rid="F6">Figure 6A</xref>.</p>
</caption>
<graphic xlink:href="feart-10-894353-g007.tif"/>
</fig>
<p>The second-generation of assemblages is modeled over a <italic>P&#x2013;T</italic> range of 7&#x2013;13&#xa0;kbar and 800&#x2013;900&#xb0;C (<xref ref-type="fig" rid="F7">Figure 7B</xref>), countered with the isopleths of <italic>X</italic>
<sub>Grs</sub> in garnet and <italic>X</italic>
<sub>An</sub> in plagioclase. The inferred peak assemblage including garnet, Cpx-2, Pl-2, amphibole, quartz, and rutile occurs within a large <italic>P&#x2013;T</italic> of &#x3e;11&#xa0;kbar/810&#x2013;880&#xb0;C, constrained by the rutile-out curve in the low-<italic>P</italic> limit, and the liquid-out and amphibole-out curves in the low- and high-<italic>T</italic> limits. The measured maximum <italic>X</italic>
<sub>Grs</sub> of 0.28 in the garnet core and the minimum <italic>X</italic>
<sub>An</sub> of 0.28 in the Pl-2 core yield a precise peak condition of &#x223c;12&#xa0;kbar/860&#xb0;C within the peak assemblage field with uncertainties of &#x223c;1.6 kbar and &#x223c;22&#xb0;C (two-sigma level). The post-peak decompression is dominated by the reaction of Grt &#x2b; Cpx &#x2b; Qz &#x2b; Liq &#x3d; Amp &#x2b; Pl, responsible for the formation of outward increasing <italic>X</italic>
<sub>An</sub> in Pl-2 but decreasing <italic>X</italic>
<sub>Grs</sub> in garnet.</p>
</sec>
<sec id="s4-3">
<title>4.3 Sample JD1546</title>
<p>The <italic>P&#x2013;T</italic> pseudosection for the sample JD1546 was calculated within a <italic>P&#x2013;T</italic> range of 7&#x2013;14&#xa0;kbar and 750&#x2013;950&#xb0;C (<xref ref-type="fig" rid="F8">Figure 8</xref>), contoured with isopleths of <italic>X</italic>
<sub>Py</sub> and <italic>X</italic>
<sub>Grs</sub> in garnet and <italic>X</italic>
<sub>An</sub> in plagioclase. The observed peak assemblage involving garnet, clinopyroxene, amphibole, plagioclase, and rutile is constrained under a <italic>P&#x2013;T</italic> condition of &#x3e;10.5&#xa0;kbar/820&#x2013;870&#xb0;C, constrained by the rutile-out curve on the low-<italic>P</italic> limit, and the K-feldspar-in and amphibole-out curves on the low- and high-<italic>T</italic> limits. The measured maximum <italic>X</italic>
<sub>Grs</sub> of 0.27 in the core of garnet and the minimum <italic>X</italic>
<sub>An</sub> of 0.27 in the core of plagioclase are plotted to yield a precise peak condition at &#x223c;12.6&#xa0;kbar and &#x223c;835&#xb0;C in the peak assemblage field with uncertainties of &#x223c;0.6&#xa0;kbar and &#x223c;20&#xb0;C (two-sigma level). This is almost consistent with the temperature defined by the measured maximum <italic>X</italic>
<sub>Py</sub> of 0.23 in garnet. The post-peak decompression is dominated by the reaction of Grt &#x2b; Cpx &#x2b; Qz &#x2b; Liq &#x3d; Amp &#x2b; Pl &#xb1; Bt, in accordance with the outward increasing <italic>X</italic>
<sub>An</sub> in plagioclase but decreasing <italic>X</italic>
<sub>Grs</sub> in garnet, and also responsible for the later growth of amphibole and biotite.</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>
<italic>P&#x2013;T</italic> pseudosection with the proposed <italic>P&#x2013;T</italic> path for the sample JD1546. Others are same as <xref ref-type="fig" rid="F6">Figure 6A</xref>.</p>
</caption>
<graphic xlink:href="feart-10-894353-g008.tif"/>
</fig>
</sec>
</sec>
<sec id="s5">
<title>5 Zircon Dating</title>
<p>Zircon grains from the samples JD15120 (two-pyroxene granulite) and JD1546 (garnet clinopyroxene granulite) were separated by conventional heavy liquid and magnetic separation followed by hand-picking under a binocular microscope. Selected grains were mounted in an epoxy resin, polished down to expose the grain centers, photographed in transmitted and reflected light, and imaged using cathode luminescence (CL). CL imaging was conducted at Peking University on a FEI PHILIPS XL30 SFEG SEM with 2-min scanning time under the condition of 15&#xa0;kV and 120&#xa0;&#x3bc;A. The zircon LA&#x2013;ICP&#x2013;MS U&#x2013;Pb isotopic analyses were performed at Peking University using an Agilent 7500c ICP-MS system connected with a 193&#xa0;nm ArF excimer laser system (COMPexPro 102) with the automatic positioning system. Zircon 91,500 was used as the standard and the standard silicate glass NIST was used to optimize the machine (<xref ref-type="bibr" rid="B91">Wiedenbeck et al., 1995</xref>; <xref ref-type="bibr" rid="B92">Wiedenbeck et al., 2004</xref>). The concentration of U, Th, and Pb elements were calibrated using <sup>29</sup>Si as an internal calibrant and NIST 610 as an external reference standard. <sup>207</sup>Pb/<sup>206</sup>Pb, <sup>206</sup>Pb/<sup>238</sup>U, and <sup>207</sup>Pb/<sup>235</sup>U ratios and apparent ages were calculated using the GLITTER 4.4 (<xref ref-type="bibr" rid="B79">Van Achterbergh et al., 2001</xref>; <xref ref-type="bibr" rid="B21">Griffin 2008</xref>). The age calculations and plotting of concordia diagrams were carried out using ISOPLOT 3.0 (<xref ref-type="bibr" rid="B58">Ludwig 2003</xref>). Analyses described as &#x201c;concordant&#x201d; refer to &#x3c;10% discordance. The results are presented in <xref ref-type="sec" rid="s13">Supplementary Tables S1, S2</xref>.</p>
<p>Zircon grains in the sample JD15120 are mostly oval or round in shape and have sizes of 30&#x2013;150&#xa0;&#x3bc;m with length/width ratios of 1:1&#x2013;2:1 (<xref ref-type="fig" rid="F9">Figure 9A</xref>). Two groups can be recognized based on their appearances on CL images. Group-1 grains are mostly dim in their luminescence and have a sector, patchy, or fir-tree zones. Group-2 zircons have clear core&#x2013;rim structures, where the grain cores show similar features with the group-1 zircons, and the rims, mostly 3&#x2013;20&#xa0;&#x3bc;m across, are gray in color and have structureless zones. We have conducted only 25 analyses on 25 group-1 grains or group-2 zircon cores, as the rims of group-2 zircons are much smaller than the diameter of the beam spot. The results yield apparent <sup>207</sup>Pb/<sup>206</sup>Pb ages from 2529 &#xb1; 31 to 2447 &#xb1; 53&#xa0;Ma. Most of the analyses were plotted on or close to the concordia curve in <xref ref-type="fig" rid="F9">Figure 9B</xref> and define an upper intersect age of 2490 &#xb1; 19&#xa0;Ma (MSWD &#x3d; 0.21), with a weighted mean age of 2488 &#xb1; 10&#xa0;Ma (MSWD &#x3d; 0.38). These zircons were analyzed to have the Th/U ratios of mostly 0.11&#x2013;1.49, with only one outlier of 3.18. They show left inclined REE patterns with high (Lu/Gd)<sub>N</sub> of 25.97&#x2013;100.00, and exhibit positive Ce anomalies (Ce/Ce<sup>&#x2a;</sup> &#x3d; 11.95&#x2013;101.29), and mostly negative Eu anomalies (Eu/Eu<sup>&#x2a;</sup> &#x3d; 0.20&#x2013;1.00) (<xref ref-type="fig" rid="F9">Figure 9C</xref>). They are considered to grow from metamorphic melts (<xref ref-type="bibr" rid="B74">Rubatto 2002</xref>; <xref ref-type="bibr" rid="B82">Wan et al., 2011</xref>).</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>
<bold>(A)</bold> Cathodoluminescence (CL) images of selected zircons from the sample JD15120. Solid circles show the inner positions of LA&#x2013;ICP&#x2013;MS analytical sites with their identification numbers as in <xref ref-type="sec" rid="s13">Supplementary Table S1</xref>. <bold>(B)</bold> U&#x2013;Pb isotopic age distributions of analyzed zircons. <bold>(C)</bold> Chondrite-normalized REE patterns (<xref ref-type="bibr" rid="B78">Sun and McDonough 1989</xref>).</p>
</caption>
<graphic xlink:href="feart-10-894353-g009.tif"/>
</fig>
<p>Zircons in the sample JD1546 are mostly rounded with size range within 20&#x2013;150&#xa0;&#x3bc;m and length/width ratios of 1:1&#x2013;2:1 (<xref ref-type="fig" rid="F10">Figure 10A</xref>). They can be subdivided into three groups based on their appearances on CL images. The group-1 zircons are mostly bright in their luminescence and have blurred oscillatory or sector zones. The group-2 accounts for the majority of zircons, and the grains are significantly coarse with sizes of mostly &#x3e;80&#xa0;&#x3bc;m and have clear core&#x2013;rim structures. The grain cores are mostly dim in luminescence and have patchy or sector zones, while the rims are 5&#x2013;30&#xa0;&#x3bc;m wide with gray luminescence and structureless zones. The group-3 is rare and small with sizes of &#x3c;40&#xa0;&#x3bc;m, featured with dark or gray luminescence and structureless zones. Five analyses were obtained on five group-1 zircons with apparent <sup>207</sup>Pb/<sup>206</sup>Pb ages from 2522 &#xb1; 22 to 2607 &#xb1; 20&#xa0;Ma (<xref ref-type="fig" rid="F10">Figure 10B</xref>). These zircons show the Th/U ratios of 0.35&#x2013;0.49 and exhibit left inclined REE patterns with (Lu/Gd)<sub>N</sub> of 17.24&#x2013;32.22, positive Ce anomalies (Ce/Ce<sup>&#x2a;</sup> &#x3d; 9.95&#x2013;17.33), and negative Eu anomalies (Eu/Eu<sup>&#x2a;</sup> &#x3d; 0.20&#x2013;0.67) on the chondrite-normalized REE patterns (<xref ref-type="fig" rid="F10">Figure 10C</xref>). They are considered to be captured zircons of mafic magma. Twenty-seven analyses were conducted on 27 group-2 zircon cores and yielded apparent <sup>207</sup>Pb/<sup>206</sup>Pb ages ranging from 2465 &#xb1; 9 to 2526 &#xb1; 11&#xa0;Ma. These results were plotted on or close to the concordia curve in <xref ref-type="fig" rid="F10">Figure 10B</xref> and defined an upper intersect age of 2494 &#xb1; 18&#xa0;Ma (MSWD &#x3d; 0.18), with a weighted mean age of 2494 &#xb1; 5&#xa0;Ma (MSWD &#x3d; 1.5). These zircons have the Th/U ratios of mostly 0.24&#x2013;0.38 with an outlier of 0.13. On the chondrite-normalized REE patterns, they display left inclined REE patterns with (Lu/Gd)<sub>N</sub> of 10.45&#x2013;131.68, positive Ce anomalies (Ce/Ce<sup>&#x2a;</sup> &#x3d; 2.04&#x2013;29.25), and positive or negative Eu anomalies (Eu/Eu<sup>&#x2a;</sup> &#x3d; 0.28&#x2013;2.12) (<xref ref-type="fig" rid="F10">Figure 10C</xref>). These zircons were considered to have a metamorphic origin (<xref ref-type="bibr" rid="B13">Corfu et al., 2003</xref>). The group-2 zircon rims are smaller than the beam diameter and cannot be analyzed. Only two analyses were obtained on two group-3 zircons. One grain (&#x23;12) has apparent <sup>207</sup>Pb/<sup>206</sup>Pb age of 1784 &#xb1; 20&#xa0;Ma (<xref ref-type="fig" rid="F10">Figure 10B</xref>). It has a low Th/U ratio of 0.07 than other zircons and displays significantly low total REE values, flat HREE pattern with (Lu/Gd)<sub>N</sub> of 21.34, positive Ce anomalies (Ce/Ce<sup>&#x2a;</sup> &#x3d; 5.77), and negative Eu anomalies (Eu/Eu<sup>&#x2a;</sup> &#x3d; 0.81) (<xref ref-type="fig" rid="F10">Figure 10C</xref>). It is considered to be metamorphic zircons that coexist with garnet (<xref ref-type="bibr" rid="B74">Rubatto 2002</xref>). The other grain (&#x23;7) has an apparent <sup>207</sup>Pb/<sup>206</sup>Pb age of 1922 &#xb1; 26&#xa0;Ma (<xref ref-type="fig" rid="F10">Figure 10B</xref>) and the Th/U ratio of 0.30. As it has a flat HREE pattern situated between the REE patterns of group-2 zircon cores and &#x23;12 zircon (<xref ref-type="fig" rid="F10">Figure 10C</xref>); we considered that its result would be a mixture of two ages.</p>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>
<bold>(A)</bold> Cathodoluminescence (CL) images of selected zircons from the sample JD1546. Solid circles show the inner positions of LA&#x2013;ICP&#x2013;MS analytical sites with their identification numbers as in <xref ref-type="sec" rid="s13">Supplementary Table S2</xref>. <bold>(B)</bold> U&#x2013;Pb isotopic age distributions of analyzed zircons. <bold>(C)</bold> Chondrite-normalized REE patterns (<xref ref-type="bibr" rid="B78">Sun and McDonough 1989</xref>).</p>
</caption>
<graphic xlink:href="feart-10-894353-g010.tif"/>
</fig>
</sec>
<sec id="s6">
<title>6 Discussion</title>
<sec id="s6-1">
<title>6.1 Metamorphic Evolution of Mafic Granulites</title>
<p>Based on the petrological observations and phase equilibria modeling, two-episode metamorphism can be referred from mafic granulites including the fist-episode UHT metamorphism and the later overprinting metamorphism.</p>
<sec id="s6-1-1">
<title>6.1.1 The First-Episode Ultrahigh Temperature Metamorphism</title>
<p>The first-episode metamorphism is inferred in the samples JD15120 and YC8-43, suggesting a <italic>P&#x2013;T</italic> path involving UHT peak conditions and post-peak decompressional cooling under normal granulite-facies conditions. The peak assemblage in both samples is inferred to consist of fine-to-medium-grained clinopyroxene, orthopyroxene, amphibole, plagioclase, and ilmenite. The peak conditions were constrained to be 940&#x2013;960&#xb0;C at 7.5&#x2013;8.5&#xa0;kbar for the sample JD15120 and 950&#x2013;990&#xb0;C at 8&#xa0;kbar for the sample YC8-43, on the basis of the stability of the peak assemblages in <italic>P&#x2013;T</italic> pseudosections and contours of the measured maximum <italic>X</italic>
<sub>An</sub> in the core of plagioclase (<xref ref-type="fig" rid="F6">Figures 6A</xref>, <xref ref-type="fig" rid="F7">7A</xref>). The post-peak evolution is inferred to be dominated by cooling with decompression, which is supported by the later growth of amphibole and biotite, the measured core-to-rim decreasing <italic>X</italic>
<sub>An</sub> in plagioclase (<xref ref-type="fig" rid="F5">Figures 5A,B</xref>), and the measured Ti in amphibole (<xref ref-type="fig" rid="F6">Figures 6A</xref>, <xref ref-type="fig" rid="F7">7A</xref>). For both of the samples, the observed quartz- and biotite-present final assemblages may represent local segregation of residual melts, and thus, record lower-temperature solidi (&#x223c;810&#xb0;C/7&#xa0;kbar for JD15120 in <xref ref-type="fig" rid="F6">Figure 6B</xref>) than those modeled in the <italic>P&#x2013;T</italic> pseudosections in <xref ref-type="fig" rid="F6">Figures 6A</xref>, <xref ref-type="fig" rid="F7">7A</xref>. The peak UHT conditions are consistent with the REE-based geothermometric results of 948&#x2013;1,031&#xb0;C from <xref ref-type="bibr" rid="B100">Yang and Wei (2017a)</xref>, which are much higher than conventional Cpx&#x2013;Opx Fe&#x2013;Mg exchange geothermometric results of 756&#x2013;940&#xb0;C (<xref ref-type="bibr" rid="B28">He and Ye 1992</xref>; <xref ref-type="bibr" rid="B8">Chen and Li 1996</xref>; <xref ref-type="bibr" rid="B114">Zhao et al., 1999</xref>; <xref ref-type="bibr" rid="B100">Yang and Wei 2017a</xref>). These suggest that both the <italic>X</italic>
<sub>An</sub> in plagioclase cores and REEs in pyroxenes have high potential for recording the peak temperatures for UHT granulites (<xref ref-type="bibr" rid="B10">Cherniak and Dimanov 2010</xref>; <xref ref-type="bibr" rid="B44">Liang et al., 2013</xref>; <xref ref-type="bibr" rid="B43">Li and Wei 2016</xref>). However, conventional Fe&#x2013;Mg exchange geothermometers are most likely to record the closure of Fe&#x2013;Mg diffusion between minerals, with temperatures even lower than the solidus recorded by the quartz-present final assemblages.</p>
<p>Similar UHT peak conditions with post-peak cooling and decompression processes to normal granulite-facies were recovered in mafic and pelitic or greywacke granulites from the East Hebei terrane (<xref ref-type="bibr" rid="B15">Duan et al., 2017</xref>; <xref ref-type="bibr" rid="B53">Liu and Wei 2018</xref>; <xref ref-type="bibr" rid="B54">Liu and Wei 2020</xref>; <xref ref-type="bibr" rid="B52">Liu et al., 2021</xref>; <xref ref-type="fig" rid="F11">Figure 11</xref>). In these granulites, pre-peak up-<italic>P</italic> processes can be inferred on the basis of 1) high-<italic>X</italic>
<sub>An</sub> plagioclase, spinel, or cordierite inclusions in garnet from pelitic granulites (<xref ref-type="bibr" rid="B15">Duan et al., 2017</xref>; <xref ref-type="bibr" rid="B54">Liu and Wei 2020</xref>; <xref ref-type="bibr" rid="B52">Liu et al., 2021</xref>), 2) orthopyroxene giving way to garnet in greywacke granulites (<xref ref-type="bibr" rid="B54">Liu and Wei 2020</xref>), and 3) rounded magnetite&#x2013;ilmenite inclusions in clinopyroxene from mafic granulites (<xref ref-type="bibr" rid="B53">Liu and Wei 2018</xref>), suggesting anticlockwise <italic>P&#x2013;T</italic> paths (<xref ref-type="fig" rid="F11">Figure 11</xref>).</p>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>Summarized <italic>P&#x2013;T</italic> conditions and paths for granulites from the East Hebei terrane. Thick arrows represent <italic>P&#x2013;T</italic> paths under peak <italic>P&#x2013;T</italic> conditions in this study. The <italic>P&#x2013;T</italic> paths from literatures are D15, from <xref ref-type="bibr" rid="B14">Duan et al. (2015)</xref>; D17, from <xref ref-type="bibr" rid="B15">Duan et al. (2017)</xref>; YW17, from <xref ref-type="bibr" rid="B100">Yang and Wei (2017a)</xref>; W18, from <xref ref-type="bibr" rid="B83">Wang et al. (2018)</xref>; LW18, from <xref ref-type="bibr" rid="B53">Liu and Wei (2018)</xref>; LW20-G, path of meta-greywacke rock from <xref ref-type="bibr" rid="B54">Liu and Wei (2020)</xref>; L20, from <xref ref-type="bibr" rid="B56">Lu and Wei (2020)</xref>; and L21, from <xref ref-type="bibr" rid="B52">Liu et al. (2021)</xref>. Mineral stabilities: Amp-out (WW) and Amp-out (SD) lines from the experiments of <xref ref-type="bibr" rid="B96">Wyllie and Wolf (1993)</xref> and <xref ref-type="bibr" rid="B75">Sen and Dunn (1994)</xref>; Grt-in (WW) line is after <xref ref-type="bibr" rid="B96">Wyllie and Wolf (1993)</xref>. The wet solidus of mafic rocks is after <xref ref-type="bibr" rid="B41">Lambert and Wyllie (1972)</xref> and the dry solidus of granodiorite is cited from <xref ref-type="bibr" rid="B73">Robertson and Wyllie (1971)</xref>. The transition lines of Al<sub>2</sub>SiO<sub>5</sub> are calculated by THERMOCALC. The abbreviations: NG&#x2014;&#x2018;normal&#x2019; granulite; UHTG&#x2014;ultrahigh-temperature granulite; EHPG&#x2014;eclogite-high-pressure granulite.</p>
</caption>
<graphic xlink:href="feart-10-894353-g011.tif"/>
</fig>
</sec>
<sec id="s6-1-2">
<title>6.1.2 The Overprinting Metamorphism</title>
<p>The overprinting metamorphism is recognized in all of the mafic granulites, but exhibits varying textures. In the sample JD15120 from the Taipingzhai ovoid-structural domain, the overprinting assemblages comprise tiny-grained clinopyroxene, orthopyroxene, plagioclase, amphibole, and quartz that occurred as vermicular coronae between medium-grained amphibole and plagioclase. In the sample YC8-43 from the central Saheqiao linear-structural belt, poikilitic garnet occurs as coronae or &#x201c;red-eye sockets,&#x201d; or aggregates with tiny-grained clinopyroxene, plagioclase, amphibole, rutile, and quartz around the previous two-pyroxenes. Whereas in the sample JD1546 that from the west Saheqiao linear-structural belt, poikilitic garnet-bearing overprinting assemblages have completely replaced the previous UHT assemblages except for a few relicts of medium-grained clinopyroxene. The garnet-bearing assemblages are modeled to have peak <italic>P&#x2013;T</italic> conditions of &#x223c;12&#xa0;kbar/860&#xb0;C for YC8-43 and &#x223c;12.6 kbar/835&#xb0;C for JD1546, based on the stability of the peak assemblages in the <italic>P&#x2013;T</italic> pseudosections, and the isopleths of the maximum <italic>X</italic>
<sub>Grs</sub> in garnet cores and the minimum <italic>X</italic>
<sub>An</sub> in plagioclase cores (<xref ref-type="fig" rid="F7">Figures 7B</xref>, <xref ref-type="fig" rid="F8">8</xref>). The peak <italic>P&#x2013;T</italic> conditions are consistent with the results of 10&#x2013;14&#xa0;kbar/800&#x2013;875&#xb0;C calculated using REE- and major elements-based geothermobarometers (<xref ref-type="bibr" rid="B100">Yang and Wei 2017a</xref>). Similar HP granulite peak conditions of 9&#x2013;11 kbar/&#x223c;800&#xb0;C and 12.5&#x2013;12.8&#xa0;kbar/880&#x2013;900&#xb0;C are also recovered in mafic granulites from the Malanyu and Beidazhangzi areas in the Saheqiao linear-structural belt (<xref ref-type="bibr" rid="B83">Wang et al., 2018</xref>; <xref ref-type="bibr" rid="B56">Lu and Wei 2020</xref>). Moreover, the overprinting assemblages in pelitic granulites from the Taipingzhai domain were also constrained to show peak conditions of 10&#x2013;12&#xa0;kbar/830&#x2013;880&#xb0;C, based on the high <italic>X</italic>
<sub>Grs</sub> of re-grown garnet (<xref ref-type="bibr" rid="B15">Duan et al., 2017</xref>). The post-peak decompression processes are inferred on the basis of the outward decreasing <italic>X</italic>
<sub>Grs</sub> in garnet and increasing <italic>X</italic>
<sub>An</sub> in plagioclase in this study and also in other supracrustal rocks (<xref ref-type="bibr" rid="B56">Lu and Wei 2020</xref>) and mafic dykes (<xref ref-type="bibr" rid="B14">Duan et al., 2015</xref>). In these research works, there are a few coarse-grained plagioclase grains recording a core-to-mantle decreasing <italic>X</italic>
<sub>An</sub> before the outward increasing <italic>X</italic>
<sub>An</sub> in the rim, being considered to suggest prograde up-<italic>T</italic> and <italic>P</italic> processes and clockwise <italic>P&#x2013;T</italic> paths (<xref ref-type="fig" rid="F11">Figure 11</xref>).</p>
</sec>
</sec>
<sec id="s6-2">
<title>6.2 Significance of Zircon Ages</title>
<p>Most metamorphic zircons from the samples JD15120 and JD1546 yielded ages of 2488 &#xb1; 10&#xa0;Ma (MSWD &#x3d; 0.38) and 2494 &#xb1; 5&#xa0;Ma (MSWD &#x3d; 1.5), respectively, which are considered to be related with the early-episode UHT metamorphism. This is because that 1) the zircons with the older ages are mostly large in size, round in shape, and have high Th/U ratios, showing the features of zircons that grew from metamorphic melts (<xref ref-type="bibr" rid="B74">Rubatto 2002</xref>; <xref ref-type="bibr" rid="B82">Wan et al., 2011</xref>); and 2) they display left-inclined REE patterns with high (Lu/Gd)<sub>N</sub> values, suggesting that no garnet was involved with the zircon growth (<xref ref-type="bibr" rid="B74">Rubatto 2002</xref>). These features are consistent with the recovered <italic>P&#x2013;T</italic> evolution of the early-episode UHT metamorphism. Moreover, the metamorphic ages are in accordance with the Neoarchean metamorphic ages of 2.55&#x2013;2.46&#xa0;Ga with a peak at &#x223c;2.50&#xa0;Ga from supracrustal rocks in the East Hebei terrane (e.g., <xref ref-type="bibr" rid="B62">Nutman et al., 2011</xref>) and even in other terranes of the NCC (e.g., <xref ref-type="bibr" rid="B32">Huang et al., 2020</xref>).</p>
<p>Only one valid metamorphic age of 1784 &#xb1; 20&#xa0;Ma was obtained from one zircon grain in the sample JD1546, which may correspond to the HP granulite-facies overprinting because that 1) the zircon is small in shape, dark in CL image, and has low Th/U ratio of 0.07, being consistent with zircons that from metamorphic fluid (<xref ref-type="bibr" rid="B74">Rubatto 2002</xref>; <xref ref-type="bibr" rid="B82">Wan et al., 2011</xref>); and 2) it displays the HREE-flat REE pattern with a low (Lu/Gd)<sub>N</sub> value, suggesting its equilibrium with garnet (<xref ref-type="bibr" rid="B74">Rubatto 2002</xref>). This age is consistent with the Lu&#x2013;Hf garnet-whole rock isochron age of 1.77&#x2013;1.79&#xa0;Ga in similar granulites from the Saheqiao linear-structural belt (<xref ref-type="bibr" rid="B99">Yang and Wei 2017b</xref>). It is worthy to mention that the age of the HP granulite-facies overprinting had well dated to occur at 1.81&#x2013;1.82&#xa0;Ga from metabasic dykes (<xref ref-type="bibr" rid="B14">Duan et al., 2015</xref>) and other HP granulites (<xref ref-type="bibr" rid="B99">Yang and Wei 2017b</xref>; <xref ref-type="bibr" rid="B56">Lu and Wei 2020</xref>).</p>
<p>Note that although sample JD1546 is almost completely modified by HP granulite assemblages, its metamorphic zircons are mostly formed during the late Neoarchean UHT metamorphism. This suggests that zircons are more resistant than the major minerals during the lower-temperature overprinting on the higher-temperature UHT granulites. Therefore, it should be careful in linking the metamorphic assemblages with ages, especially for the rocks that have underwent multi-episode metamorphism.</p>
</sec>
<sec id="s6-3">
<title>6.3 Tectonic Implications</title>
<p>Two-episode metamorphism has been inferred in the East Hebei terrane, including the late Neoarchean UHT metamorphism and late Paleoproterozoic HP granulite-facies metamorphism, where the first one is featured with anticlockwise <italic>P&#x2013;T</italic> paths whereas the latter one is marked by clockwise <italic>P&#x2013;T</italic> paths (<xref ref-type="fig" rid="F11">Figure 11</xref>). These two different metamorphic processes may suggest distinct tectonic settings.</p>
<sec id="s6-3-1">
<title>6.3.1 Late Neoarchean Ultrahigh Temperature Metamorphism</title>
<p>The late Neoarchean UHT metamorphism in the East Hebei terrane may attribute from four tectonic models, including amalgamation of microcontinental terranes (e.g., <xref ref-type="bibr" rid="B104">Zhai and Santosh 2011</xref>), subduction&#x2013;collision (e.g., <xref ref-type="bibr" rid="B39">Kusky et al., 2016</xref>; <xref ref-type="bibr" rid="B50">Liu et al., 2018</xref>), plume-related processes (e.g., <xref ref-type="bibr" rid="B114">Zhao et al., 1999</xref>; <xref ref-type="bibr" rid="B19">Geng et al., 2006</xref>), and vertical tectonics (&#x201c;drip tectonics&#x201d; or &#x201c;sagduction&#x201d;; e.g., <xref ref-type="bibr" rid="B15">Duan et al., 2017</xref>; <xref ref-type="bibr" rid="B53">Liu and Wei 2018</xref>,; <xref ref-type="bibr" rid="B54">Liu and Wei 2020</xref>). The Archean vertical tectonism is marked by mantle overturn and crustal delamination in the mantle&#x2013;crust scale and sagduction within the crust (<xref ref-type="bibr" rid="B34">Johnson et al., 2014</xref>; <xref ref-type="bibr" rid="B27">Harris and B&#xe9;dard 2014</xref>; <xref ref-type="bibr" rid="B4">B&#xe9;dard 2018</xref>). A sagduction process, including the diapirism of granitoids and sinking of supracrustal rocks (e.g., <xref ref-type="bibr" rid="B12">Collins et al., 1998</xref>; <xref ref-type="bibr" rid="B80">Van Kranendonk et al., 2004</xref>), is considered to be the most possible mechanism that accounts for the formation of Archean unique dome&#x2013;and&#x2013;keel structures (e.g., <xref ref-type="bibr" rid="B12">Collins et al., 1998</xref>; <xref ref-type="bibr" rid="B46">Lin 2005</xref>; <xref ref-type="bibr" rid="B45">Lin and Beakhouse 2013</xref>; <xref ref-type="bibr" rid="B64">Parmenter et al., 2006</xref>), and the simultaneity between the metamorphism of supracrustal rocks and their ambient TTG magmatic activity (<xref ref-type="bibr" rid="B16">Fran&#xe7;ois et al., 2014</xref>). Thus, a sagduction process is preferred to be responsible for the late Neoarchean UHT metamorphism in the East Hebei terrane, based on the following lines of evidence: 1) the Archean unique dome&#x2013;and&#x2013;keel structures are well preserved (<xref ref-type="fig" rid="F1">Figure 1</xref>), with the Lulong&#x2013;Shuangshanzi supracrustal belt distributed between TTG domes and numerous supracrustal rafts within the domes; 2) the determined metamorphic ages of 2.55&#x2013;2.46&#xa0;Ga with a peak at &#x223c;2.50&#xa0;Ga are coeval with the final pulse of TTG magmatism that ranging from 2.56 to 2.48&#xa0;Ga with a peak at &#x223c;2.52&#xa0;Ga (e.g., <xref ref-type="bibr" rid="B86">Wei 2018</xref>); and 3) near-vertical normal shear formed due to the upwelling of Anziling dome with respect to the down-slipping of the Lulong&#x2013;Shuangshanzi supracrustal belt was inferred based on sub-vertical textures including mineral lineations and &#x201c;S&#x201d;-type folds in the Shuangshanzi shear zone (<xref ref-type="bibr" rid="B48">Liu et al., 2017</xref>; <xref ref-type="bibr" rid="B110">Zhao et al., 2021</xref>). The counterclockwise <italic>P&#x2013;T</italic> path in supracrustal rafts can be interpreted in a sagduction process, where the supracrustal rocks were heated first by the intrusion of high-temperature TTG magmas, or more possibly, the mantle-derived magmas, and then dropped to magmas to reach the peak stage, and finally cooled and uplifted during the doming processes.</p>
</sec>
<sec id="s6-3-2">
<title>6.3.2 Late Paleoproterozoic Metamorphism</title>
<p>The late Paleoproterozoic metamorphism is widely observed in the NCC (e.g., <xref ref-type="bibr" rid="B115">Duan et al., 2015</xref>; <xref ref-type="bibr" rid="B33">Huang et al., 2016</xref>; <xref ref-type="bibr" rid="B99">Yang and Wei 2017b</xref>; <xref ref-type="bibr" rid="B115">Zou et al., 2022</xref>), and its tectonic setting has been controversially debated. The prevalent view suggests a successive collision model among the Archean blocks, forming the Khondalite belt at &#x223c;1.95&#xa0;Ga, the Jiao-Liao-Ji belt at &#x223c;1.90&#xa0;Ga, and the TNCO at &#x223c;1.85&#xa0;Ga (e.g., <xref ref-type="bibr" rid="B112">Zhao et al., 2005</xref>; <xref ref-type="bibr" rid="B111">Zhao et al., 2012</xref>). However, the final amalgamation of the NCC along TNCO is argued to occur at &#x223c;1.95&#xa0;Ga, and the dated age of &#x223c;1.85&#xa0;Ga from granulites is interpreted to be correlated with a separated within-plate orogeny (<xref ref-type="bibr" rid="B86">Wei 2018</xref>; <xref ref-type="bibr" rid="B72">Qian et al., 2019</xref>). Another view contests that there were cold oceanic subduction and collision tectonics occurred in the north margin of the NCC (e.g., <xref ref-type="bibr" rid="B39">Kusky et al., 2016</xref>). The oceanic subduction is limited within 1.92&#x2013;1.85&#xa0;Ga and supported by the eclogite-facies metamorphism in the Chicheng ophiolitic m&#xe9;lange (<xref ref-type="bibr" rid="B108">Zhang Y. Y. et al., 2020</xref>; <xref ref-type="bibr" rid="B107">Zhang et al., 2021</xref>), and eclogite xenoliths with superdeep majorite inclusions in the carbonatite from the boundary between the Khondalite belt and TNCO (<xref ref-type="bibr" rid="B98">Xu et al., 2017</xref>; <xref ref-type="bibr" rid="B97">Xu et al., 2018</xref>), while the collision may occur later at 1.85&#x2013;1.80&#xa0;Ga with the similar spatial distribution of the IMNHO, between the NCC and a missing continent (<xref ref-type="bibr" rid="B39">Kusky et al., 2016</xref>) or the southwestern margin of the Siberia Craton (<xref ref-type="bibr" rid="B93">Wu et al., 2018</xref>).</p>
<p>In this study, late Paleoproterozoic metamorphism was well constrained in the East Hebei terrane, and it becomes weaker from north to south. In the Saheqiao linear-structural belt, HP granulite assemblages are well developed and stronger deformation had mostly removed the Neoarchean fabrics (<xref ref-type="bibr" rid="B100">Yang and Wei 2017a</xref>; <xref ref-type="bibr" rid="B56">Lu and Wei 2020</xref>; this article). In the Taipingzhai ovoid-structural domain, the Archean domal structures are survived, and the overprinting assemblages are limited in pelitic granulites with the regrowth of garnet (<xref ref-type="bibr" rid="B15">Duan et al., 2017</xref>), and in mafic granulites with the formation of vermicular coronae (<xref ref-type="fig" rid="F3">Figures 3C,D</xref>), although good HP granulite assemblages are developed in mafic dykes (<xref ref-type="bibr" rid="B14">Duan et al., 2015</xref>). While in the Qian&#x2019;an gneiss dome, overprinting assemblages were reported from the Caozhuang supracrustal rocks that are characterized by staurolite-bearing assemblages of low-amphibolite facies (<xref ref-type="bibr" rid="B51">Liu et al., 2020</xref>). Thus, the late Paleoproterozoic overprinting metamorphism in the East Hebei terrane suggests a medium <italic>P</italic>/<italic>T</italic> ratio at 1.78&#x2013;1.82&#xa0;Ga (<xref ref-type="bibr" rid="B14">Duan et al., 2015</xref>; <xref ref-type="bibr" rid="B15">Duan et al., 2017</xref>; <xref ref-type="bibr" rid="B99">Yang and Wei 2017b</xref>; <xref ref-type="bibr" rid="B56">Lu and Wei 2020</xref>; this article). This is considered to be correlated with intracontinental deformation that triggered by the oceanic subduction-related continental collision in the northern margin of the NCC. The collision event is also favored by the &#x223c;1.89&#xa0;Ga Barrovian-type metamorphism in the Kondalite belt (<xref ref-type="bibr" rid="B33">Huang et al., 2016</xref>), the &#x223c;1.84&#xa0;Ga HP granulites from the North Liaoning terrane (Duan et al., 2019), the 1.74&#x2013;1.83&#xa0;Ga amphibolite-to-granulite-facies metamorphism in the Miyun complex (<xref ref-type="bibr" rid="B29">He et al., 1993</xref>; <xref ref-type="bibr" rid="B105">Zhang H. C. G. et al., 2020</xref>; <xref ref-type="bibr" rid="B115">Zou et al., 2022</xref>), and the &#x223c;1.85&#xa0;Ga within-plate metamorphism and deformation in the Wutai&#x2013;Hengshan region (<xref ref-type="bibr" rid="B86">Wei 2018</xref>; <xref ref-type="bibr" rid="B72">Qian et al., 2019</xref>).</p>
</sec>
</sec>
</sec>
<sec id="s7">
<title>7 Conclusion</title>
<p>
<list list-type="simple">
<list-item>
<p>(1) Two-episode metamorphism can be recognized in mafic granulites from the East Hebei terrane.</p>
</list-item>
<list-item>
<p>(2) The first-episode metamorphism is recovered under UHT conditions of 940&#x2013;990&#xa0;&#xb0;C at 7.5&#x2013;8.5&#xa0;kbar and post-peak cooling with the decompression process to &#x223c;7&#xa0;kbar/&#x223c;810&#xa0;&#xb0;C.</p>
</list-item>
<list-item>
<p>(3) The second-episode overprinting metamorphism exhibits varying textures in different samples. In garnet-bearing samples, the overprinting assemblages show HP granulite-facies peak conditions of 12&#x2013;12.6&#xa0;kbar/835&#x2013;860&#xb0;C, and post-peak isothermal decompression to &#x223c;9&#xa0;kbar.</p>
</list-item>
<list-item>
<p>(4) Zircon dating suggests two metamorphic ages of &#x223c;2.49&#xa0;Ga and &#x223c;1.78&#xa0;Ga, being considered to be correlated with the UHT and HP granulite metamorphism, respectively.</p>
</list-item>
<list-item>
<p>(5) The late Neoarchean UHT granulite metamorphism with a thermal gradient of &#x223c;33&#xb0;C/km may correlate a vertical sagduction regime, whereas the late Paleoproterozoic HP granulite metamorphism with a thermal gradient of &#x223c;20&#xb0;C/km is favored to register the continental collision in the northern margin of the North China Craton.</p>
</list-item>
</list>
</p>
</sec>
</body>
<back>
<sec id="s8">
<title>Data Availability Statement</title>
<p>The original contributions presented in the study are included in the article/<xref ref-type="sec" rid="s13">Supplementary Material</xref>, further inquiries can be directed to the corresponding authors.</p>
</sec>
<sec id="s9">
<title>Author Contributions</title>
<p>TL calculated the pseudosections, performed the data analyses, and wrote the manuscript. CY and ZL collected the samples and conducted the experiments. CJW developed the project and revised the manuscript. All authors discussed the results and were involved in writing the paper.</p>
</sec>
<sec id="s10">
<title>Funding</title>
<p>This work was financially supported by the National Natural Science Foundation of China (Grant Nos: 42102062, 42030304).</p>
</sec>
<sec sec-type="COI-statement" id="s11">
<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="s12">
<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>
<ack>
<p>We thank the editor Yi Chen for his editorial work, and Dr. Camille Fran&#x00E7;ois and Dr. Shujuan Jiao for their thoughtful and constructive comments, which have greatly improved our manuscript.</p>
</ack>
<sec id="s13">
<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.2022.894353/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/feart.2022.894353/full&#x23;supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="DataSheet1.DOCX" id="SM1" mimetype="application/DOCX" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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