<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OJER</journal-id><journal-title-group><journal-title>Open Journal of Earthquake Research</journal-title></journal-title-group><issn pub-type="epub">2169-9623</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojer.2022.114006</article-id><article-id pub-id-type="publisher-id">OJER-121465</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Earth&amp;Environmental Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  High-Precision Structural Map of Southeast Cameroon Using Phase Filters on Potential Gravimetric Data
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Nzeuga</surname><given-names>Alain Rodrigue</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Bisse</surname><given-names>Salomon Bertrant</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Amaya</surname><given-names>Adama</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kenfack</surname><given-names>Fokem Alpha Baster</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ngah</surname><given-names>Christian Gislain Leonel</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ndjounguep</surname><given-names>Juscar</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Nanfa</surname><given-names>Tefak Fatoumata Maelle</given-names></name><xref ref-type="aff" rid="aff5"><sup>5</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ngoumou</surname><given-names>Paul Claude</given-names></name><xref ref-type="aff" rid="aff6"><sup>6</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Assembe</surname><given-names>Stéphane Patrick</given-names></name><xref ref-type="aff" rid="aff7"><sup>7</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Pokam</surname><given-names>Kengni Serge Hugues</given-names></name><xref ref-type="aff" rid="aff7"><sup>7</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Department of Mining Geology, School of Geology and Mining Engineering, University of Ngaoundere, Meiganga, Cameroon</addr-line></aff><aff id="aff2"><addr-line>Department of Geological Mapping and Geomatic, School of Geology and Mining Engineering, University of Ngaoundere, Meiganga, Cameroon</addr-line></aff><aff id="aff5"><addr-line>Institute of Mining and Geological Research, Ministry of Scientific Research, Yaounde, Cameroon</addr-line></aff><aff id="aff4"><addr-line>Postgraduate School of Science Technology and Geosciences, University of Yaounde I, Yaounde, Cameroon</addr-line></aff><aff id="aff7"><addr-line>Department of Physics, Faculty of Science, University of Bamenda, Bambili, Cameroon</addr-line></aff><aff id="aff6"><addr-line>Department of Geophysics, School of Geology and Mining Engineering, University of Ngaoundere, Meiganga, Cameroon</addr-line></aff><aff id="aff1"><addr-line>Department of Petroleum Gas and Exploration, School of Geology and Mining Engineering, University of Ngaoundere, Meiganga, Cameroon</addr-line></aff><pub-date pub-type="epub"><day>07</day><month>11</month><year>2022</year></pub-date><volume>11</volume><issue>04</issue><fpage>89</fpage><lpage>107</lpage><history><date date-type="received"><day>12,</day>	<month>June</month>	<year>2022</year></date><date date-type="rev-recd"><day>22,</day>	<month>November</month>	<year>2022</year>	</date><date date-type="accepted"><day>25,</day>	<month>November</month>	<year>2022</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The south-east of Cameroon encompasses a wide variety of geological struc
  tures among which we can cite the Congo Craton (CC), the Sanaga Fault
   
  (SF), the Yaound&#233; Domain, the Panafrican belt, the Protozoic series and the Dja complex. The presence of all these structures justifies the great tectonic activity to which this area was subject 
  from
   the rupture of Pangea to the creation of the different plates that exist today. In this work, we will bring out a high
  -
  resolution 
  structural map of the study area by applying the qualitative analysis
   
  of the phase filters on 200,900 points of gravimetric data obtained from the combination of the XGM2016 and ETOPO1 models. Then, with these same data, we will bring out another structural map with 
  the 
  maxima method called Multi
  -
  Scale Horizontal Derivative of Vertical Derivative (MSHDVD) 
  which will be compared to the first in order to show the limits of the MSHDVD 
  method. To do this, we will first use the extension method to highlight the map 
  of residual anomalies, then a combination of derivative, gradient and phase
   filters to highlight the geological structures responsible for fracturing in this area. Phase filters have the advantage that they make it possible to highlight all the geological edges responsible for the fracturing without taking into account the depth, while the MSHDVD method highlights the existing geological contacts (edges) at depths well defined by the examiner. The structural map obtained with the MSHDVD method shows that the major structural direction in this zone is W-E while that obtained from the interpretation of the phase filters is more precise and shows that the major structural direction in this area would be N-S and this result would be in perfect agreement with the tectonics of East Cameroon.
 
</p></abstract><kwd-group><kwd>Gravimetry</kwd><kwd> Potential Field Data</kwd><kwd> Edge Detection</kwd><kwd> Structural Mapping</kwd><kwd> Southeast Cameroon</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Located in southeastern Cameroon, the study area (<xref ref-type="fig" rid="fig1">Figure 1</xref>) is between latitudes 1˚ and 5˚N and longitudes 12˚ and 17˚E. It covers an area of 246,469 km<sup>2</sup> and extends over three Central African countries, namely Gabon, Congo and the Central African Republic. Potential data provide information about sources inside the Earth on a different scale [<xref ref-type="bibr" rid="scirp.121465-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref2">2</xref>]. Determining the residual gravity field amounts to enhance the signal of the total anomaly field by isolating them from the effects of ambient noise and shallow sources [<xref ref-type="bibr" rid="scirp.121465-ref3">3</xref>]. There are cases where quite large anomalies are hidden in the regional field and this is usually because the source is larger than the study area or is located at great depth. Variations in the mid to high frequencies of the gravity anomaly spectrum could reflect the influence of lithospheric structures with changes in density and topographic relief [<xref ref-type="bibr" rid="scirp.121465-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref8">8</xref>]. Thus, a regional/residual separation of the gravity field would be an essential numerical step in the interpretation of gravity data [<xref ref-type="bibr" rid="scirp.121465-ref9">9</xref>]. In the past, this issue has been addressed with a straightforward graphical approach [<xref ref-type="bibr" rid="scirp.121465-ref10">10</xref>] either by empirically selecting data points representative of a regional gravity field [<xref ref-type="bibr" rid="scirp.121465-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref12">12</xref>] or by using various mathematical tools to obtain a regional gravity field [<xref ref-type="bibr" rid="scirp.121465-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref16">16</xref>].</p><p>Despite numerous methods that have been developed and applied for this purpose, probably four methods among them are the most commonly used. The one that will be applied in this work includes the separation method that we used. This category is based on the analysis of the power spectra of gravity fields in order to differentiate between regional and residual gravity fields attributed to sources at different depths [<xref ref-type="bibr" rid="scirp.121465-ref17">17</xref>]. This procedure involves the application of the Fourier transform and gravity data filtering. The wavelength components can then be investigated for gravity fields, while selecting parameters for a separating regional and residual gravity field [<xref ref-type="bibr" rid="scirp.121465-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref20">20</xref>].</p><p>Several gravimetric and seismological studies have been carried out in this region, including the work of [<xref ref-type="bibr" rid="scirp.121465-ref21">21</xref>] - [<xref ref-type="bibr" rid="scirp.121465-ref27">27</xref>]. The main objectives were the determination</p><p>of the depth of the Moho and the structural study. However, the previous structural studies were based on the method of maxima and the objective of our work for the future would be to apply the phase filters to bring out a high-resolution structural map of the south-east of Cameroon.</p><p>The use of 200,900 measurement points from the recent XGM2016 model and the regional/residual separation of the Bouguer anomaly map by the extension method could increase the signature gravity anomalies [<xref ref-type="bibr" rid="scirp.121465-ref28">28</xref>]. The use of the locations of the maxima method [<xref ref-type="bibr" rid="scirp.121465-ref29">29</xref>] and filters such as vertical derivatives, horizontal gradient amplitude [<xref ref-type="bibr" rid="scirp.121465-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref31">31</xref>], total gradient amplitude [<xref ref-type="bibr" rid="scirp.121465-ref32">32</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref33">33</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref34">34</xref>], tilt angle [<xref ref-type="bibr" rid="scirp.121465-ref35">35</xref>] and horizontal gradient amplitude of tilt angle [<xref ref-type="bibr" rid="scirp.121465-ref36">36</xref>] can help in identification and determination of source edges and their positions.</p><p>In this work, we will use the Bouguer anomaly data to separate field components. Then we will apply the first-order derivation, the Horizontal Gradient (HG), the Analytical Signal (AS), the Tilt Angle (TDR) and the horizontal gradient of the tilt angle (HG<sub>TDR</sub>) filters to highlight the different contacts. Finally, we will compare the geological contacts obtained from the combination of TDR and HG<sub>TDR</sub> maps with those obtained by the multi-scale horizontal derivative of the vertical derivative method to bring out a new tectono-structural map of the region and show the limitations of the MSHDVD method.</p></sec><sec id="s2"><title>2. Geological Setting</title><p>The geology of the southeast Cameroon as represented in <xref ref-type="fig" rid="fig2">Figure 2</xref> is very complex and encompasses structures of a varied nature. It is characterised by a dentritic hydrograhic network that emphasizes a variety of tectonic features such as the Ntem complex, (a part of Congo Craton), the Yaounde domain, the Sanaga fault (SF), the Prot&#233;rozoic series and the Dja complex. All these structures have already been the subject of several studies with different methods by several authors working in the field of geology. The geology of the study area could generally be divided into the Precambrian basement and Archean structure [<xref ref-type="bibr" rid="scirp.121465-ref37">37</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref38">38</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref39">39</xref>]. These two major geological features are associated with the Oubanguides Belt, formed during the Atlantic opening from the continental collision of the Archean Congo and West African Cratons in Africa together with the S&#227;o Francisco Craton in South America [<xref ref-type="bibr" rid="scirp.121465-ref36">36</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref40">40</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref41">41</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref42">42</xref>], during which NE-SW, E-W to ESE-WNW, NW-SE and N-S main lineaments were formed and the crust rejuvenated at the NW edge of the Congo Craton [<xref ref-type="bibr" rid="scirp.121465-ref43">43</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref44">44</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref45">45</xref>].</p><p>The Congo Craton is one of the largest cratonic blocks in Africa with an area of about 5.7 million Km<sup>2</sup> with a diameter of ~2500 Km [<xref ref-type="bibr" rid="scirp.121465-ref46">46</xref>]. Cameroon shares with the neighbouring contries the northern edge of the largest African Craton called the Congo Craton [<xref ref-type="bibr" rid="scirp.121465-ref47">47</xref>]. The Ntem Complex located in the southern part of Cameroon is mainly composed by early Proterozoic syenites and constitutes the northern edge of the Archean Congo Craton domain [<xref ref-type="bibr" rid="scirp.121465-ref41">41</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref48">48</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref49">49</xref>]. It has been first influenced by the Liberian orogeny marked by various folds and brittle structures [<xref ref-type="bibr" rid="scirp.121465-ref50">50</xref>] with an Archaean magnetism rocks with some reworked material that formed in early Proterozoic times [<xref ref-type="bibr" rid="scirp.121465-ref51">51</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref52">52</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref53">53</xref>].</p><p>The Yaounde domain is a huge nappe thrusted southward onto the Congo Craton. It comprises low to high grade garnet bearing shale, gneisses and orthogneisses transformed under a medium to high pressure metamorphism reaching the granulite facies [<xref ref-type="bibr" rid="scirp.121465-ref39">39</xref>]. In the Yaounde domain, [<xref ref-type="bibr" rid="scirp.121465-ref54">54</xref>] showed that the tectonic caused by overall dextral transgressions due to alternating E-W to NW-SE contractions and N-S to NE-SW orogenic-parallel extensions generated N or S foliation penetration associated with ENE-WSW stretching lineation and a N-S to NE-SW folding. However, the tectonic evolution of the southern Cameroon is still debated regarding the collision system, the strike-slip direction and the history of the complexity of its geodynamics.</p></sec><sec id="s3"><title>3. Origin of Data</title><p>The gravity data used in this work are the combination of the XGM2016 global gravitational model used to generate the free-air gravity anomaly and the ETOPO1 topographic and bathymetric datasets [<xref ref-type="bibr" rid="scirp.121465-ref56">56</xref>] used to compute the topographic and bathymetric gravity corrections. To get the Bouguer anomalies data, we applied these gravity corrections to the free-air gravity anomaly. The experimental Gravity Field Model XGM2016, parameterized as a spherical harmonic series up to degree and order 719, was computed as a precursor study for the upcoming combined Earth Gravitational Model 2020 (EGM2020). The combination methodoly of XGM2016 is the same as its predecessor model GOCOO5c [<xref ref-type="bibr" rid="scirp.121465-ref57">57</xref>]. The main difference between XGM2016 and GOCOO5c models is that XGM2016 is supported by an improved terrestrial data set of gravity anomaly area-means provided by the United States National Geospatial-Intelligence Agency (NGA). These differences result from including additional information of satellite data that contribute to the improved ground data in these regions. XGM2016 also yields a smoother Mean Dynamic Topography with significantly reduced artifacts, which has the benefit of enhanced information with respect to ocean area modelling.</p></sec><sec id="s4"><title>4. Methodologies</title><p>Many filtering operations are necessary and should be applied on the Bouguer anomaly map to bring out the lineaments necessary to plot a geological model of the subsoil and highlighting the intrusions of igneous bodies in the study area located in Cameroon. The separation by extension method of Bouguer anomalies is first summarized. Then the first order derivative filters followed by the horizontal gradient, the analytical signal, and the tilt angle and its horizontal gradient will be used to plot the edge contacts of the study area. Finally, we will used the Blakely and Simpson method [<xref ref-type="bibr" rid="scirp.121465-ref29">29</xref>] to apply the multi-scale horizontal derivative of the vertical derivative to also plot the edge geological contacts of the same study area and then compare the two methods and the corresponding structural maps.</p><sec id="s4_1"><title>4.1. Regional/Residual Separation</title><p>The extension method is the regional/residual separation method used here. It consists in determining of a suitable altitude for upward continuation after applied the Fourier transform, in the goal to obtain the optimum regional anomaly map for the study area by applying the Zeng method [<xref ref-type="bibr" rid="scirp.121465-ref58">58</xref>]. The maxima calculated at each altitude of upward continuation are then counted and plotted in <xref ref-type="fig" rid="fig3">Figure 3</xref>. The altitude where the maxima become zero corresponds to the altitude where the regional anomaly map is optimum [<xref ref-type="bibr" rid="scirp.121465-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref59">59</xref>]. Thus the map extended to 30 Km corresponds to the regional anomalies map of the study area.</p></sec><sec id="s4_2"><title>4.2. Derivative Filters</title><p>Let us consider that the total gravimetric intensity data is represented as ΔG, caused by the distribution of density sources beneath the surface. We can apply the derivative filters when the gravity fields of several sources interfere in the goal to determine the contact location of the sources [<xref ref-type="bibr" rid="scirp.121465-ref60">60</xref>]. This is due to the vertical derivative being able to isolate the gravity effects of individual sources better than the Bouguer anomaly because of it’s no applying in the frequency domain which generally enhances data errors, depending on the signal/noise ratio [<xref ref-type="bibr" rid="scirp.121465-ref61">61</xref>]. The vertical derivative also has the advantage to operate the calculation at several heights using a stable operator like an upward continuation [<xref ref-type="bibr" rid="scirp.121465-ref18">18</xref>].</p><p>Basically, we can write horizontal and vertical first-order derivatives as:</p><p>∂ Δ G ∂ x = Δ G i + 1 , j − Δ G i − 1 , j 2 Δ x (1)</p><p>∂ Δ G ∂ y = Δ G i , j + 1 − Δ G i , j − 1 2 Δ y (2)</p><p>∂ Δ G ∂ z = F − 1 { | k | F ( Δ G ) } (3)</p><p>where, Δx and Δy are sample intervals, i and j represent the measurements of ΔG, F and F<sup>−1</sup> are defined as the Fourier transform and inverse Fourier transform and |k| is the radial wavenumber.</p><p>To calculate the Horizontal Gradient Amplitude (HGA) [<xref ref-type="bibr" rid="scirp.121465-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref31">31</xref>] and the Analytic Signal Amplitude (ASA) [<xref ref-type="bibr" rid="scirp.121465-ref32">32</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref33">33</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref34">34</xref>], we can combine these quantities as follows:</p><p>HGA = ( ∂ Δ G ∂ x ) 2 + ( ∂ Δ G ∂ y ) 2 (4)</p><p>ASA = ( ∂ Δ G ∂ x ) 2 + ( ∂ Δ G ∂ y ) 2 + ( ∂ Δ G ∂ z ) 2 (5)</p><p>These filters are efficient to isolate boundaries since maximum value usually is located above the source, especially when symmetry is present [<xref ref-type="bibr" rid="scirp.121465-ref62">62</xref>] [<xref ref-type="bibr" rid="scirp.121465-ref63">63</xref>].</p></sec><sec id="s4_3"><title>4.3. Phase Filters</title><p>The Tilt Angle (TDR) is one of the most phase filters used today to highlight geological information. The tilt derivative and its total horizontal derivative are useful for mapping shallow basement structures and mineral exploration targets [<xref ref-type="bibr" rid="scirp.121465-ref35">35</xref>]. They proposed an interesting approach known as tilt angle (tilt filter). They used the ratio of the vertical derivative to the absolute amplitude of the horizontal gradient when applied to potential data in order to define the tilt angle as follows:</p><p>TDR = tan − 1 [ ∂ Δ G ∂ z ( ∂ Δ G ∂ x ) 2 + ( ∂ Δ G ∂ y ) 2 ] (6)</p><p>The horizontal gradient of tilt angle (HG<sub>TDR</sub>) was developed by many researchers like [<xref ref-type="bibr" rid="scirp.121465-ref64">64</xref>] and [<xref ref-type="bibr" rid="scirp.121465-ref65">65</xref>] to improve the results of the tilt angle method. It is given by:</p><p>HG TDR = ( ∂ TDR ∂ x ) 2 + ( ∂ TDR ∂ y ) 2 (7)</p></sec><sec id="s4_4"><title>4.4. Determination of Edge Contacts Using Phase Filters</title><p>For determination of precise edges, the TDR and HG<sub>TDR</sub> are well indicated but the HG<sub>TDR</sub> is more precise than the TDR because it detects very faint edges better than it. [<xref ref-type="bibr" rid="scirp.121465-ref36">36</xref>] shows that the TDR is a good approach to equalize disparate signals, but it is not primarily an edge detection filter because it uses its zero contours to detect the source edges. The edge of HG<sub>TDR</sub> will be plotted using the Blakely and Simpson method and then, the map of zero contours of TDR and the one of HG<sub>TDR</sub> will be used to plot the corresponding structural map of the study area.</p></sec><sec id="s4_5"><title>4.5. Determination of Edge Contacts Using the Multi-Scale Horizontal Derivative of Vertical Derivative Method</title><p>The upward continuation of the gravity field at increasing heights has the particularity of highlighting the gravity effect of deeper sources. To determine the geological contacts, it is important to know that the highest upward continuation corresponds to the gravity response of the deepest part of the contact. When the contact is located vertically to the source, the maxima of the total horizontal gradient of the upward continuation fields are located at the same position and when the maxima systematically shift in a horizontal direction, the dip direction of the contact should be identified [<xref ref-type="bibr" rid="scirp.121465-ref60">60</xref>].</p><p>That method involves the following steps:</p><p>&#173; Calculating the first-order vertical derivative for upward continued gravity field at different heights, called here the multi-scale vertical derivative;</p><p>&#173; Determining the maxima of the horizontal gradient of the multi-scale vertical derivative;</p><p>&#173; Superposing the maps obtained for different continuation heights.</p></sec></sec><sec id="s5"><title>5. Results</title><sec id="s5_1"><title>5.1. Bouguer Anomaly Map</title><p>The data resulting from the combination of the XGM2016 global gravitational model and ETOPO1 topographic and bathymetric datasets were used to gridded the Bouguer anomalies map with a grid cell size of 5000 m grid space to show the spatial distribution of gravity anomaly. The corresponding map is called the Total Gravity Intensity (TGI). It clearly displays the differences in locations of high gravimetric intensities that reach the peak of −8.5 mGal and low gravimetric intensities that the lowest reached the peak of −112.4 mGal (<xref ref-type="fig" rid="fig4">Figure 4</xref>). The</p><p>signal of this map is affected with many noises due to the effects of regional on the distribution of gravity anomalies and a direct interpretation without eliminating these effects will contain errors. To make it, we need to separate the regional effects from the Bouguer and this will be the subject of the next section.</p></sec><sec id="s5_2"><title>5.2. Regional/Residual Maps</title><p>As explained previously in Section 4, the Bouguer anomalies map extended to 30 Km corresponds to the regional anomalies map (<xref ref-type="fig" rid="fig5">Figure 5</xref>(a)). Now, it we will subtract from the Bouguer anomalies map to get the corresponding residual anomalies map (<xref ref-type="fig" rid="fig5">Figure 5</xref>(b)) representing in <xref ref-type="fig" rid="fig4">Figure 4</xref> and which will be the basis of the various filtering operations that will follow.</p><p>The positive anomalies with peaks reaching 38 mGal observed on the regional anomaly map correspond to Neoproterozoic series made up of post to syn-tectonic granitoids. The average intensity anomalies observed on the residual map are mostly nuggets, sandstones and quartzites of the Dja group. The negative anomalies observed correspond to Mesoarchean gneiss and volcano-clastic sandstones of the Poli group and the conglomerates, quartzites, sedimentary sandstones and volcano-sedimentary sandstones of the Lom group. Finally, we can observe a great correlation between the residual anomalies map and the geological map of the study area. Theses anomalies would be caused by the effects of surface structures present in the study area.</p></sec><sec id="s5_3"><title>5.3. Derivative Filter</title><p>The first-order derivative filters have been applied according to the procedures schematically described in section 4 in the goal to highlight the gravimetric signatures of the study area. The Z-derivative map represented in <xref ref-type="fig" rid="fig6">Figure 6</xref> presents a good distribution of the anomalies with peaks range from −2 Gal to 3 Gal. The positive anomalie observed at point A is more highlighted and could represented the volcano-clastic sandstones of the Poli group as represented on the geological map.</p></sec><sec id="s5_4"><title>5.4. Gradients Filters</title><p>The horizontal (<xref ref-type="fig" rid="fig7">Figure 7</xref>(a)) and total gradient amplitude (<xref ref-type="fig" rid="fig7">Figure 7</xref>(b)) respectively noted HGA and ASA were applied to the residual map in the goal to identify isolated sources, since in most cases the filtered anomaly is entirely positive and the maximum value is located above the source. The gradient maps represented in <xref ref-type="fig" rid="fig7">Figure 7</xref> better represented the anomalies and we can observed that the positive and negative anomalies which were grouped on the Bouguer regional map are isolated and the gradients filters aim to center the gravity anomalies below their geological sources. We can observe a less difference between these two figures in the highlighting of the positives anomalies represented at the northwest part of the study area and this can be explained by the fact that the ASA is more indicated to detect geologic sources and boundaries of the shallowest sources than the HGA, since it adds the vertical derivative in its formulation. These filters are not sufficient for a good interpretation of the anomalies observed in the study area because they are limited to a qualitative interpretation, but furthermore the information that it gives corroborate the one observe on the geological map.</p></sec><sec id="s5_5"><title>5.5. Phase Filters</title><p>The phase filters are not used to determinate the locations of anomalies responsible to the body intrusions as the gradient filters, but are instead used to determinate the edges contacts such as faults. The TDR (<xref ref-type="fig" rid="fig8">Figure 8</xref>(a)) and the HG<sub>TDR</sub> (<xref ref-type="fig" rid="fig8">Figure 8</xref>(b)) filters illustrated in <xref ref-type="fig" rid="fig8">Figure 8</xref> are well indicated for determination of precise edges sources but the HG<sub>TDR</sub> can be more precise than the TDR because it detects very faint edges better than it. As observed in the first order Z-derivative of Bouguer residual anomalies map (<xref ref-type="fig" rid="fig6">Figure 6</xref>), we can observe that</p><p>there is a very great similarity on this one and the map of TDR, and the map of TDR would therefore represent the geological contacts at the origin of these intrusions. The HG<sub>TDR</sub> map isolated contact edges both from shallow and deep structures existing below them because it is the application of a gradient filter on the TDR.</p></sec><sec id="s5_6"><title>5.6. Determination of Structural MapUsing Phase Filters</title><p>[<xref ref-type="bibr" rid="scirp.121465-ref36">36</xref>] shows that the TDR is a good approach to equalize disparate signal but, it is not primarily an edge detection filter because it uses its zero contours to detect the source edges while the HG<sub>TDR</sub> use it maxima to determine the position of the source edge. The zero-contours map of the TDR (<xref ref-type="fig" rid="fig9">Figure 9</xref>(a)) and the source edges map of HG<sub>TDR</sub> (<xref ref-type="fig" rid="fig9">Figure 9</xref>(b)) will be used and analyzed together to draw the structural map responsible to the fracturing in the study area, which will be represented in <xref ref-type="fig" rid="fig1">Figure 1</xref>0(a).</p><p>The rose diagram of the structural direction represented in the map of <xref ref-type="fig" rid="fig1">Figure 1</xref>0(b) shows that the fracturing in this zone was done along 3 main directions namely N-S, W-E and SW-NE and the major direction of fracturing in southeast Cameroon is N-S.</p></sec><sec id="s5_7"><title>5.7. Determination of Structural MapUsing MSHDVD Method</title><p>The detailed methodology for this section has been developed in previous section 4. In this section, using the maxima method, we have identified all the edges contact successively at depths 2, 4, 6, 8 and 10 Km. The map in <xref ref-type="fig" rid="fig1">Figure 1</xref>1(a) represents the contact map at different height and <xref ref-type="fig" rid="fig1">Figure 1</xref>1(b) represents the corresponding structural map.</p><p>The rose diagram of the structural direction drown with MSHVDV method represented in <xref ref-type="fig" rid="fig1">Figure 1</xref>2 shows that the fracturing in the study area was done</p><p>along 4 directions namely N-S, W-E, NW-SE SW-NE and the major direction of fracturing in southeast Cameroon according to MSHDVD methos is W-E.</p></sec></sec><sec id="s6"><title>6. Discussion</title><p>The Bouguer residual anomaly map (<xref ref-type="fig" rid="fig5">Figure 5</xref>(b)) highlights a large positive anomaly located at the north of the study area, a large medium anomaly located to the center to the southeast and many large negative anomalies located both at the west and the southwest. These variations observed on the lithology are due to cross cut by post-metamorphic and post deformation intrusions, both covered by discordant glacial deposits overlain by carbonate formations of the upper Dja series called Mintom Formation and the overthrusting unit including the Yokadouma series overlapping the folded unit [<xref ref-type="bibr" rid="scirp.121465-ref66">66</xref>]. This map presents the distribution of anomalies more precisely than the one of Bouguer and is similar to that one. This resemblance rate to the Bouguer anomaly map justifies the chosen separation method and validates the extension height which is 30 km. finally, we can observed that the repartition of these anomalies in block can not a priori informed on the structural directions.</p><p>The first-order Z-derived map (<xref ref-type="fig" rid="fig6">Figure 6</xref>) enhances the information contained in the residual map. It dissociated the anomalies that were represented in block and shows some positive anomalies that were not visible on the residual map. The gradient maps (<xref ref-type="fig" rid="fig7">Figure 7</xref>) isolate the different sources that were arranged as a block and place the gravity anomalies directly above their sources.</p><p>The TDR map (<xref ref-type="fig" rid="fig8">Figure 8</xref>(a)) highlights the different gravimetric domains while the HG<sub>TDR</sub> map (<xref ref-type="fig" rid="fig8">Figure 8</xref>(b)) highlights the different contacts that delimit these different domains. Now, we can observe the main structural directions responsible for the fracturing in the southeast of Cameroon. These directions can be WSW-ENE, W-E and NNW-SSE. The zero contours map (<xref ref-type="fig" rid="fig9">Figure 9</xref>(a)) highlights the various contacts that would be at the origin of the various anomalies while the source edge maps (<xref ref-type="fig" rid="fig9">Figure 9</xref>(b)) justify at these points the presence of the various corresponding anomalies. Thus, we believe that the structural map obtained by phase filters (<xref ref-type="fig" rid="fig1">Figure 1</xref>0(a)) is better suitable for highlighting geological contacts as faults. The corresponding rose diagram (<xref ref-type="fig" rid="fig1">Figure 1</xref>0(b)) shows that the main structural direction of the study area is N-S, followed by W-E and SW-NE. That information would be correct because the fracturing will follow the one of the Sanaga Fault that causes a moving of the crust from these directions.</p><p>The sources edge determined by the MSHDVD method represented in <xref ref-type="fig" rid="fig1">Figure 1</xref>1(a) is not easy to interpret because it determinates the contacts at precise different depths. The structural corresponding map highlights most of the contacts shown on the structural map obtained by phase filters but the main structural directions here are W-E followed by N-S. This information corroborates the previous one, but we note that the methodology used to plot that faults were not very efficient.</p><p>Our results highlight some structures that already existed according to the observations of the geological map, but also highlight new faults.</p></sec><sec id="s7"><title>7. Conclusions</title><p>In this research work, we separated the regional/residual anomalies by the extension method in order to obtain the best map of residual anomalies which was the result of subtraction of the Bouguer map upwards to 30 Km from the Bouguer map. Then we used filters such as HG, AS, TDR and HG<sub>TDR</sub> gradient to enhance the geological information and highlight the geological source edges responsible for these anomalies. Finally, we also used the MSHDVD method to highlight the edge contacts and we observed that this method is not more precise than the first one. The main result of this work is the structural map obtained by the interpretation of phase filters, with the main structural direction known as N-S. This shows the major lineaments of the region and faults of various directions with high precision. These results are comparable to those existing and corroborate the information on the geological map. Also, the large fault network plotted shows that the south-east of Cameroon would be a compression zone due to the strike-slip fault network of the Sanaga, and this fault network justifies the presence of a great mineralization activity which would have led to the formation of minerals of varied nature that exists in the southeast of Cameroon.</p><p>The geological structures observed show that the tectonic activity in this region is still ongoing. However, it would be important to delineate the depths of the structures that form the observed main structures by quantitative analysis, inversion and/or by 2D or 3D modelling. Also, the use of remote sensing data and minerals analysis will make it possible to precisely highlight the mineralogy of the said region with the goal to complete the geological information.</p></sec><sec id="s8"><title>Acknowledgements</title><p>The authors are grateful to the editor of the journal and the two unknown reviewers for detailed and constructive reviews, which significantly improved the original manuscript. All grid files and maps were created using Oasis montaj v8.4.</p></sec><sec id="s9"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s10"><title>Cite this paper</title><p>Rodrigue, N.A., Bertrant, B.S., Adama, A., Baster, K.F.A., Leonel, N.C.G., Juscar, N., Maelle, N.T.F., Claude, N.P., Patrick, A.S. and Hugues, P.K.S. (2022) High-Precision Structural Map of Southeast Cameroon Using Phase Filters on Potential Gravimetric Data. 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