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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">960358</article-id>
<article-id pub-id-type="doi">10.3389/feart.2022.960358</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>Reworking of ancient tectonic amalgamation belt beneath the central north of North China Craton revealed by dense seismic observations</article-title>
<alt-title alt-title-type="left-running-head">Zhou et al.</alt-title>
<alt-title alt-title-type="right-running-head">
<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3389/feart.2022.960358">10.3389/feart.2022.960358</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Zhou</surname>
<given-names>Qiming</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1844439/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Shen</surname>
<given-names>Xuzhang</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/1634405/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Huang</surname>
<given-names>He</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Cheng</surname>
<given-names>Siyuan</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Zhang</surname>
<given-names>Jian</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>Guangdong Provincial Key Lab of Geodynamics and Geohazards</institution>, <institution>School of Earth Science and Engineering</institution>, <institution>Sun Yat-Sen University</institution>, <addr-line>Zhuhai</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>Southern Marine Science and Engineering Guangdong Laboratory (Zhuhai)</institution>, <addr-line>Zhuhai</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/1447663/overview">Zhuqi Zhang</ext-link>, China Earthquake Administration, 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/1855356/overview">Yuanze Zhou</ext-link>, University of Chinese Academy of Sciences, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1862010/overview">Xiaobo Tian</ext-link>, Institute of Geology and Geophysics (CAS), China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/872303/overview">Zengxi Ge</ext-link>, Peking University, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Xuzhang Shen, <email>shenxzh5@mail.sysu.edu.cn</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Structural Geology and Tectonics, a section of the journal Frontiers in Earth Science</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>23</day>
<month>08</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>10</volume>
<elocation-id>960358</elocation-id>
<history>
<date date-type="received">
<day>02</day>
<month>06</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>20</day>
<month>07</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Zhou, Shen, Huang, Cheng and Zhang.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Zhou, Shen, Huang, Cheng and Zhang</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 North China Craton (NCC) is one of the oldest cratons in the world, and its internal tectonic belt is often used to investigate the earth&#x2019;s tectonic evolution events. During the late Mesozoic and Cenozoic, the western Pacific subduction zone caused the restructuring of NCC by damaging the craton beneath eastern NCC, resulting in the distinct lateral differences between western and eastern NCC, which ultimately formed the current NCC. Furthermore, the subsequent tectonic events activated the ancient tectonic weak zones, and their traces are imprinted in the deep earth. Here, we investigated the crust structures with a high-density seismic array beneath the splice position of the eastern margin of the Khondalite Belt and the northern part of the central orogenic belt in NCC. The array included 140 short-period seismographs spaced at 2&#x2013;3&#xa0;km intervals, which recorded teleseismic three-component waveforms over a one-month period. P-wave receiver functions calculated from 25 teleseismic events provided an image of the crustal structure. The weak Moho and Moho offset under the study area are visible in the migration image of receiver functions. The geological investigations and the rock outcrops were combined to establish the strong coupling relationship between the present surface fault-depression system and deep structures. The deep material circulation, which governs the surface extension of the basin-range structure, is controlled by the deep material circulation which is ultimately derived from the continuous subduction of the western Pacific. The study&#x2019;s findings indicate that the ancient amalgamative belt might have transformed into a weak zone easily susceptible to modification by plate tectonic movements.</p>
</abstract>
<kwd-group>
<kwd>North China Craton</kwd>
<kwd>dense seismic observations</kwd>
<kwd>receiver function</kwd>
<kwd>weak zone</kwd>
<kwd>reworking</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Several tectonic events in the North China Craton (NCC) since the Archean have been documented, and the available geological evidence explains the various phases of NCC. Three major tectonic events that occurred during the late Paleoproterozoic were reported by many scholars (<xref ref-type="bibr" rid="B11">Kusky et al., 2016</xref>; Li <xref ref-type="bibr" rid="B14">S et al., 2015</xref>; <xref ref-type="bibr" rid="B43">Zhai and Santosh, 2011</xref>; <xref ref-type="bibr" rid="B47">Zhao et al., 2005</xref>, <xref ref-type="bibr" rid="B46">2012</xref>, <xref ref-type="bibr" rid="B49">2013</xref>). The western NCC (WNCC) was formed by the amalgamation of the Yinshan block and the Ordos block at &#x223c;1.95&#xa0;Ga, while the eastern NCC (ENCC) was formed by the collision between Longgang and Nangrim blocks at &#x223c;1.90Ga. Furthermore, WNCC and ENCC amalgamated as a result of a tectonic event at &#x223c;1.85Ga to form the uniform basement of NCC along a central orogenic belt (Trans-North China Craton, TNCO) (<xref ref-type="bibr" rid="B48">Zhao et al., 2001</xref>; <xref ref-type="bibr" rid="B47">2005</xref>). The NCC remained stable for a long time until the significant Mesozoic lithospheric thinning. Numerous ancient tectonic structures have been transformed due to the collision between India and Eurasia plates and the subduction of the Pacific plate, which resulted in the elevation of the Tibetan Plateau (<xref ref-type="bibr" rid="B53">Zhu et al., 2011</xref>; <xref ref-type="bibr" rid="B54">2012</xref>). This indicates the vulnerability of the amalgamation belts to the subsequent tectonic disturbances. This Paleoproterozoic evolution process has also resulted in a unique tectonic background at the boundary between the eastern side of the Khondalite belt and the northern part of TNCO (<xref ref-type="fig" rid="F1">Figure 1A</xref>). The central tectonic belt and Khondalite rock belt are connected along the Huai&#x2019;an-Zhangjiakou area in Hebei province, China. The Shanxi&#x2013;Hebei&#x2013;Inner Mongolia basin tectonic belt, comprising a series of parallel Holocene faults and basins, characterizes the current surface structures and activities that are relatively distinctive (<xref ref-type="fig" rid="F1">Figure 1B</xref>&#x26;c).The tectonic environment in the area is responsible for the relatively high tectonic activity (<xref ref-type="bibr" rid="B16">Li Z et al., 2015</xref>), as evidenced by the earthquake with ML &#x3d; 6.2 triggered in Zhangbei in 1998 (<xref ref-type="bibr" rid="B41">Yang et al., 2002</xref>). The potential of this area for the occurrence of strong earthquakes is also evidenced by the GNSS observation data (<xref ref-type="bibr" rid="B40">Wu et al., 2021</xref>). The Huai&#x2019;an-Zhangjiakou is a highly significant area of TNCO due to the area&#x2019;s paleotectonic and neotectonic activities. From northwest to southeast, the area comprises Yinshan block, Khondalite series, Huai&#x2019;an complex, and Hengshan complex which are the subdivisions of metamorphic outburst classification (<xref ref-type="bibr" rid="B32">Wang et al., 2016</xref>). The temperature and pressure environment at a depth of 35&#x2013;40&#xa0;km at the bottom of the Paleoarchean lower crust is evidenced by the high pressure in the mafic granulites. The subduction&#x2013;collision&#x2013;exhumation events of Paleoproterozoic orogenic tectonic development transported these high-pressure granulites and eclogites into the core crust (<xref ref-type="bibr" rid="B44">Zhang et al., 2019</xref>).Geophysical methods can effectively understand the current deep structures and the tectonic processes. Several scholars have reported the strong concordance of surface topographic changes in the area and the E-W variations in the crustal and lithospheric structures (e.g., <xref ref-type="bibr" rid="B4">Chen, 2010</xref>; <xref ref-type="bibr" rid="B6">Cheng et al., 2013</xref>; <xref ref-type="bibr" rid="B37">Wei et al., 2015</xref>; <xref ref-type="bibr" rid="B51">Zheng et al., 2017</xref>). NCC and several other cratons in the world have restructured as a result of subduction (<xref ref-type="bibr" rid="B55">Zhu et al., 2021</xref>), and the pre-existing structures in the lithosphere primarily control such continental reconfiguration. However, deep imaging results of satisfactory scales in this local area are still lacking. In this context, the reconfiguration of the ancient tectonic amalgamation belt was investigated by procuring the higher precision imaging results of deep structures. For this purpose, a short-period array was deployed in the Huai&#x2019;an-Zhangjiakou area to apply the receiver function method for exploring deep structures. The present tectonic activity explained the activation of the ancient tectonic structures based on the imaging results.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Geological background and the station map. <bold>(A)</bold> Integration of the North China Craton and the position of the profile (<xref ref-type="bibr" rid="B46">Zhao et al., 2012</xref>) and teleseismic events and station distribution. Red circles represent the events recorded, and the black triangle represents the center of the array; <bold>(B)</bold> spatial relationship between the topography, stations, Cenozoic fault distribution, and dense seismic array in the study area; <bold>(C)</bold> plane relationship between platform array and faults. The fault names are: F1-Huai&#x2019;an&#x2013;Wanquan Basin northern margin fault; F2-Zhangjiakou fault; F3-Tianzhen&#x2013;Yanggao basin northern margin fault; F4-Huai&#x2019;an Basin southern margin fault; F5-Yangyuan basin northern margin fault; F6-Liulengshan basin northern margin fault; F7-Yuguang basin southern margin fault; F9-Sunzhuangzi&#x2013;Wulonggou fault; and F10-Xuanhua Basin southern margin fault.</p>
</caption>
<graphic xlink:href="feart-10-960358-g001.tif"/>
</fig>
</sec>
<sec id="s2">
<title>2 Method and data</title>
<sec id="s2-1">
<title>2.1 Method</title>
<p>The receiver function is a reliable seismological method widely applied for the detection of discontinuities in the crust and upper mantle. This approach extracts the signatures of the structure under the station by the deconvolution of the R and Z directions of seismic wave records. The depth of the discontinuities, the crustal thickness, and the average velocity ratio of the crust can be estimated by analyzing the time and amplitude of the P-to-S wave of the crust or upper mantle discontinuities. This method is also used for the development of broadband seismology (<xref ref-type="bibr" rid="B12">Langston, 1979</xref>; <xref ref-type="bibr" rid="B42">Yuan et al., 1997</xref>; <xref ref-type="bibr" rid="B52">Zhu and Kanamori, 2000</xref>) and understanding the crustal and upper mantle structure globally and regionally with a multitude of intriguing conclusions. However, the distance between stations in broadband seismic array observation is generally more than 10&#xa0;km, with longer periods of observation, typically several years, due to the constraints of observation cost and environment, which also limits its implementation. Apart from this, the spatial resolution is also limited due to the minimum distance of such stations&#x2019; separation. However, this method has been successfully applied recently in dense array observation data for a shorter time period. In petroleum exploration, a dense array of stations are established flexibly and quickly at several hundred meters apart by the operation of low-cost and simple nodal seismographs. After a short period of continuous observation (1&#x2013;2 months), suitable teleseismic earthquakes can be identified for high-resolution crustal structure imaging. Several studies have been successfully carried out globally on the investigation of short-period dense array observation data. For example, a series of innovative research studies have been performed in Long Beach (e.g., <xref ref-type="bibr" rid="B18">Lin et al., 2013</xref>; <xref ref-type="bibr" rid="B2">Bowden et al., 2015</xref>; <xref ref-type="bibr" rid="B1">Bianco et al., 2019</xref>), a representative study area where a shallow magma chamber was imaged under the Wudalianchi volcanic field using highly dense arrays (<xref ref-type="bibr" rid="B15">Li et al., 2016</xref>). Similarly, <xref ref-type="bibr" rid="B33">Wang et al. (2019)</xref> imaged the fault damage zone of the San Jacinto Fault near Anza using a dense array of ambient noise tomography. The unprecedented details of the growing crustal structure along various boundaries of the Tibetan Plateau were unveiled by a series of short-period dense arrays (e.g., <xref ref-type="bibr" rid="B20">Liu X et al., 2017</xref>; <xref ref-type="bibr" rid="B23">Shen et al., 2020</xref>, <xref ref-type="bibr" rid="B24">2022</xref>; <xref ref-type="bibr" rid="B28">Tian et al., 2021</xref>). Furthermore, the existence of Paleoproterozoic residual subduction in the craton margin was revealed by deploying a high-density seismic array across the boundary between the Yinshan block and the Ordos block (the Khondalite belt) (<xref ref-type="bibr" rid="B31">Wan et al., 2020</xref>).</p>
</sec>
<sec id="s2-2">
<title>2.2 High dense seismic array and data source</title>
<p>From August 2020 to September 2020, we deployed approximately 230-km-long seismic profiles with 140 short-period seismometers, crossing the ancient tectonic boundary and rift system from south to north in our study area (<xref ref-type="fig" rid="F1">Figure 1</xref> b and c). EPS seismometers with a flat velocity response ranging from 0.2 to 200&#xa0;Hz were kept nearly 1&#x2013;3&#xa0;km apart, and the observations were performed continuously for nearly one month with a sampling rate of 100 samples/s. The teleseismic waveform records of Ms &#x3e; 5.5 with distinct P-wave signal onsets were carefully identified within an epicentral distance range of 30&#xb0;&#x2013;95&#xb0; (<xref ref-type="fig" rid="F1">Figure 1D</xref>). The earthquake catalog was obtained from the global United States Geological Survey (USGS) (<ext-link ext-link-type="uri" xlink:href="http://neic.usgs.gov/neis/epic/epic_global.html">http://neic.usgs.gov/neis/epic/epic_global.html</ext-link>), and the event waveforms with obvious P-wave onset signals are shown in <xref ref-type="fig" rid="F2">Figure 2</xref>.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Observed teleseismic waveforms of R and Z components (after 0.02&#x2013;2 Hz bandpass filtering).</p>
</caption>
<graphic xlink:href="feart-10-960358-g002.tif"/>
</fig>
</sec>
<sec id="s2-3">
<title>2.3 Data processing procedure</title>
<p>Each seismic event&#x2019;s theoretical p-wave arrival time was calculated based on the IASP91 model (<xref ref-type="bibr" rid="B10">Kennett and Engdahl, 1991</xref>). The seismic data between 20&#xa0;s before and 80&#xa0;s after the P-wave were collected after calibrating the P-wave arrival. Furthermore, the mean, the linear trend, and other filtering processes were removed to check the waveform quality. The original ENZ component data were rotated to the RTZ component per the circle path. The waveforms with relatively clear recorded events were deconvoluted with different Gaussian filters to obtain the receiver functions and subsequently selected the clear receiver functions of the PmS seismic phase (<xref ref-type="bibr" rid="B17">Ligorr&#xed;a and Ammon, 1999</xref>). A Gaussian filter of 5 with an approximate pulse width of 0.75&#xa0;s was used to maintain the detailed information in receiver function traces. Also, the receiver functions with a Gaussian filter of 2 (1.18&#xa0;s pulse width), 5 (0.75&#xa0;s pulse width), and 10 (0.53&#xa0;s pulse width) were calculated to test the stability of signal characteristics (<xref ref-type="fig" rid="F3">Figure 3</xref>). The crustal structure under the station was obtained by stacking in accordance with the transition point of projection and subsequently selected 560 high-quality receiver functions. The influence of other interfaces at different epicentral distances was reduced by correcting the time of receiver functions with P-to-S moveout correction by setting a reference distance of 65&#xb0; and a focal length of 20&#xa0;km. Thus, the receiver functions may be configured to display the undulations of the Moho or the interfacial features of the crust. The profiles of stacking receiver functions after P-to-S moveout correction during different periods along the longitude of PmS pierce points, calculated based on the IASP91 model, are shown in <xref ref-type="fig" rid="F3">Figure 3</xref>.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Stacking profile of receiver functions with different Gaussian filter factors (alp). Alp &#x3d; 2 (1.18&#xa0;s pulse width), 5 (0.75&#xa0;s pulse width), and 10 (0.53&#xa0;s pulse width) were used to compare the signal stability.</p>
</caption>
<graphic xlink:href="feart-10-960358-g003.tif"/>
</fig>
<p>Furthermore, the receiver functions on the temporal domain were converted into the spatial domain along the ray path and P-to-S conversion arrivals by the common conversion point (CCP) stacking method (<xref ref-type="bibr" rid="B42">Yuan et al., 1997</xref>). For migration purposes, the crust and upper mantle within 75&#xa0;km depth were divided into 0.5&#xa0;km segments in both the horizontal and vertical directions, and subsequently, the quality of migration images was improved by staking the receiver functions with the pierce points along the ray path using the IASP91 model to generate the final migration images ultimately. The migration images obtained along the profiles from receiver functions with the Gaussian filter of 5 are shown in <xref ref-type="fig" rid="F4">Figure 4D</xref>.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>Topography, receiver function, and migration image. <bold>(A)</bold> Topographic elevation of the survey line, <bold>(B)</bold> topography and geomorphology of the study area and the distribution plan of the station, and <bold>(C)</bold> profile under the survey line superimposed by the receiving function. <bold>(D)</bold> CCP result. F1-Huai&#x2019;an&#x2013;Wanquan Basin northern margin fault; F2-Zhangjiakou fault; F3-Tianzhen&#x2013;Yanggao basin northern margin fault; F4-Huai&#x2019;an Basin southern margin fault; F5-Yangyuan basin northern margin fault; F6-Liulengshan basin northern margin fault; F7-Yuguang basin southern margin fault; F9-Sunzhuangzi&#x2013;Wulonggou fault; F10-Xuanhua Basin southern margin fault.</p>
</caption>
<graphic xlink:href="feart-10-960358-g004.tif"/>
</fig>
</sec>
</sec>
<sec id="s3">
<title>3 Results</title>
<p>The reliable signals in the receiver functions are stable with variations in time and alp. A smaller alp factor provides the Moho basic and smoothed interface data, while a larger alp factor provides more crustal information (<xref ref-type="bibr" rid="B36">Wei et al., 2016</xref>). Even though the signal of the Moho is about 5&#xa0;s (depth of approximately 40&#xa0;km), it has a distinct segmented pattern from south to north. The profile is subdivided into three characteristic segments based on the shape of the Moho signal: (&#x2160;) 39&#xb0;N&#x2013;39.8&#xb0;N (south of F7), where the Moho is clear and continuous in the staking profile, gradually descending from south to north; (&#x2161;) 39.8&#xb0;N&#x2013;40.7&#xb0;N (between F7 and F1), where the morphology is complex with weak continuity, exhibiting no single layer; and (&#x2162;) 40.7&#xb0;N&#x2013;42&#xb0;N (north of F1), where the Moho is relatively stable and flat. In addition, some relatively stable negative signals shallower than 25&#xa0;km depth observed in the range of 36.7&#xb0;N&#x2013;41.5&#xb0;N may represent a low-velocity zone (LVZ) within the crust. A comparative analysis of topographic elevation, surface structure, receiver function results, and CCP results are shown in <xref ref-type="fig" rid="F4">Figure 4</xref>. Based on the CCP results, the Moho exhibits a uniform pattern. However, the Moho in region &#x2160; is curved downward, while that in region &#x2161; is relatively complex and that in region &#x2162; is relatively flat. The LVZ is mainly concentrated in region &#x2161; and is discontinuous. The complex features of the Moho represent a series of surfaces closely related to structural features and deep structures and are visible below the densely constructed basin ridges.</p>
</sec>
<sec id="s4">
<title>4 Discussion</title>
<p>NCC is regarded as the most severely damaged craton on earth (<xref ref-type="bibr" rid="B3">Carlson et al., 2005</xref>; <xref ref-type="bibr" rid="B53">Zhu et al., 2011</xref>). The tectonic belts around cratons are relatively mechanically weak zones compared to the cratons and are primary sites of intense heating and strain localization (<xref ref-type="bibr" rid="B8">Hu et al., 2018</xref>; <xref ref-type="bibr" rid="B19">Liu et al., 2021</xref>). Based on the imaging results, the average depth of the Moho beneath the profile is 40&#xa0;km. A comparative study was carried out on the basic crustal conditions under the adjacent regions in North China by the receiver function method and by using the broadband seismograph data (<xref ref-type="bibr" rid="B50">Zheng et al., 2007</xref>; <xref ref-type="bibr" rid="B5">Chen, 2009</xref>; <xref ref-type="bibr" rid="B26">Tang et al., 2010</xref>; <xref ref-type="bibr" rid="B22">Lou et al., 2017</xref>; <xref ref-type="bibr" rid="B25">Si et al., 2017</xref>; <xref ref-type="bibr" rid="B38">Wei et al., 2020</xref>; <xref ref-type="bibr" rid="B57">Zuo et al., 2020</xref>), which are comparable with crustal thickness obtained by the measured receiver functions. The imaging results of the Moho obtained from region &#x2160; and region &#x2162; are comparable to the results from the western Khondalite belt (<xref ref-type="bibr" rid="B31">Wan et al., 2020</xref>). Moreover, the results of wide-angle reflection and refraction profile data of deep seismic sounding indicate the existence of a deep crust-scale fault zone extending to the Moho beneath the Zhangjiakou area, as well as the presence of LVZ within the crust (<xref ref-type="bibr" rid="B56">Zhu et al., 1999</xref>), which may suggest the presence of intense magmatic activity.</p>
<p>Numerical experiments demonstrate that inheritance is the primary controlling factor of lithospheric rifting and layer stiffness. The rift styles mostly depend on the inherited weaknesses embedded in the model (<xref ref-type="bibr" rid="B7">Chenin and Beaumont, 2013</xref>). The study area crosses through Yuguang and Wanquan basins from south to north and crosses a series of Holocene normal faults, making the area active. The normal faults are distributed in the east of the western parts, and their characteristic stress conditions are generally in a north&#x2013;south extensional environment. On the other hand, the combined analysis of previous tomographic results using the receiver function shows that the Moho in region &#x2161; is discontinuous (<xref ref-type="fig" rid="F5">Figure 5</xref>). Also, the complex deep structure in region &#x2161; corresponds rather well with the distribution of the faults and basins, implying that the surface topography variation is generally congruent with the deep dynamic processes. Faults 1 and 7 seem to represent two boundaries of the whole fault and basin system, governed by the migration of deep material on both sides. Frequently, the axis of lithosphere extension and continental breakup is parallel to the orogenic belts and suture zones (<xref ref-type="bibr" rid="B30">van Wijk, 2005</xref>). This area is probably related to the weak zone formed by the collage of Yinshan and Ordos blocks, which is evidenced by the combined analysis of the area with the E-W trend of the surface structure.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Tomography profile and receiver functions. The tomography results are combined with the results reported by <xref ref-type="bibr" rid="B27">Tao et al. (2018)</xref>.</p>
</caption>
<graphic xlink:href="feart-10-960358-g005.tif"/>
</fig>
<p>F1-Huai&#x2019;an&#x2013;Wanquan Basin northern margin fault; F4-Huai&#x2019;an Basin southern margin fault; F5-Yangyuan basin northern margin fault; F6-Liulengshan basin northern margin fault; F7-Yuguang basin southern margin fault.</p>
<p>Based on the tomography results, subduction of the western Pacific has extended westward into the central and WNCC toward the Datong volcano (<xref ref-type="bibr" rid="B35">Wei et al., 2012</xref>; <xref ref-type="bibr" rid="B21">Liu Z et al., 2017</xref>; <xref ref-type="bibr" rid="B45">Zhao, 2017</xref>; <xref ref-type="bibr" rid="B13">Lei et al., 2018</xref>), with a large mantle wedge in the middle and upper mantle. The depth profile of the S-wave perturbation velocity along the latitude of 40&#xb0;N is illustrated in <xref ref-type="fig" rid="F6">Figure 6</xref> based on the topography results reported by <xref ref-type="bibr" rid="B27">Tao et al. (2018)</xref>.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>Tomographic profile of the Pacific subduction with latitude &#x3d; 40&#xb0;N (according to <xref ref-type="bibr" rid="B27">Tao et al., 2018</xref>)</p>
</caption>
<graphic xlink:href="feart-10-960358-g006.tif"/>
</fig>
<p>The Pacific plate is deeply subducted toward the west, forming a large mantle wedge, and its influence extends westward, up to a longitude of 110&#xb0;E. The uneven mantle flow in the upper mantle caused by the subducting slab front poses strong action on the upper lithosphere, thereby influencing the tectonic evolution of the crustal and upper mantle structure beneath NC (<xref ref-type="bibr" rid="B29">Tian et al., 2019</xref>). The high calorific value in North China at a depth of &#x223c;100&#xa0;km is also evidenced by the geothermal results reported by <xref ref-type="bibr" rid="B34">Wang and Cheng, (2012)</xref>. The low-velocity anomalies in the crust and upper mantle below the Zhangjiakou area are shown by the local ambient noise (<xref ref-type="bibr" rid="B9">Jiang et al., 2021</xref>). The aforementioned findings show that certain Cenozoic tectonic deformation and fault development in the study area are strongly connected to the internal restructuring of the craton caused by the subduction of the western Pacific plate. The area is tectonically characterized by the western subduction of the Pacific plate and the distinct local restructuring evidenced by the formation of a large mantle wedge. The tomography images from ambient noise also reveal that the crust and upper mantle beneath the Shanxi fault depression belt, Zhangjiakou, and Datong volcanic areas are characterized by low-velocity anomalies associated with a large area of intense Cenozoic magmatic activity in Datong triggered by the upwelling of hot materials from the mantle (<xref ref-type="bibr" rid="B57">Zuo et al., 2020</xref>), and the slow movement of the magma surface causing negative signals.</p>
<p>LVZ-low-velocity zone; F1-Huai&#x2019;an&#x2013;Wanquan Basin northern margin fault; F4-Huai&#x2019;an Basin southern margin fault; F5-Yangyuan basin northern margin fault; F6-Liulengshan basin northern margin fault; F7-Yuguang basin southern margin fault.</p>
<p>The results of the receiver function and tomographic imaging were combined to generate a conceptual diagram of the tectonic process of this area, as shown in <xref ref-type="fig" rid="F7">Figure 7</xref>. Since region &#x2161; in <xref ref-type="fig" rid="F3">Figure 3</xref> and <xref ref-type="fig" rid="F4">Figure 4</xref> was relatively weak in the ancient craton collage belt earlier, it is more sensitive to get impacted by the mantle wedge (<xref ref-type="bibr" rid="B57">Zuo et al., 2020</xref>). These weak zones are reactivated by the mantle plume resulting in the upwelling of the Moho as channels, which ultimately restructures the crust. The shallow crust&#x2019;s materials are pushed to move on both sides by the circulatory power of deep materials, resulting in a series of normal faults and grabens on the earth&#x2019;s surface. As a result, region &#x2160; and region &#x2162; may still retain the shape of the ancient Moho without substantial changes.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Sketched model of the interaction between the mantle and crust.</p>
</caption>
<graphic xlink:href="feart-10-960358-g007.tif"/>
</fig>
</sec>
<sec id="s5">
<title>5 Conclusion</title>
<p>In the present study, a short-period dense array is used to generate the receiver function image of two ancient tectonic belt boundaries of NCC. The extensive continental restructuring of the area might have affected the structure and properties of the continental lithosphere and impacted both surface processes and mantle dynamics regionally. For example, the series of nearly parallel E-W basins and lithospheric scale normal faults in the study area demonstrate their relationship with the pre-existing weak zone apart from the signatures representing current tectonic processes. The present study proposed a model illustrating the damage of the ancient weak zone caused by the dynamic processes of western Pacific subduction. The mantle wedge activates the local thermal circulation in the lithosphere to reactivate the weak zone to enter the crust as a channel which forms an extensional environment. This is evidenced by the slowly cooling magma upwelling of LVZ at the bottom of the upper crust in Zhangbei-Huai&#x2019;an and Yangyuan basins.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s6">
<title>Data availability statement</title>
<p>The original contributions presented in the study are included in the article/Supplementary Material; further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s7">
<title>Author contributions</title>
<p>Conception and design of the study: QZ and XS; acquisition of data: QZ and XS; analysis and/or interpretation of the data: QZ, XS, HH, SC, and JZ; drafting the manuscript: QZ and XS; revising the manuscript critically for important intellectual content: QZ.</p>
</sec>
<sec id="s8">
<title>Funding</title>
<p>Some figures are plotted using the Generic Mapping Tools (<xref ref-type="bibr" rid="B39">Wessel et al., 2019</xref>). This study was financially supported by the National Key Research and Development Program of China (2017YFC1500100), the National Natural Science Foundation of China (Grant Nos. 41874052 and 41730212), the Second Tibetan Plateau Scientific Expedition and Research Program (STEP) (2019QZKK0701), the Guangdong Province Introduced Innovative R&#x26;D Team (2016ZT06N331 and 2017ZT07Z066), and the Guangdong Collaborative Innovation Center for Earthquake Prevention and Mitigation (2018B020207011).</p>
</sec>
<sec sec-type="COI-statement" id="s9">
<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="s10">
<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>
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