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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">1117797</article-id>
<article-id pub-id-type="doi">10.3389/feart.2023.1117797</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>Gas-bearing prediction of deep reservoir based on DNN embeddings</article-title>
<alt-title alt-title-type="left-running-head">Ma 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.2023.1117797">10.3389/feart.2023.1117797</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Ma</surname>
<given-names>Shuying</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="aff" rid="aff3">
<sup>3</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/2097436/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Cao</surname>
<given-names>Junxing</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1494631/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Liu</surname>
<given-names>Zhege</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<xref ref-type="aff" rid="aff5">
<sup>5</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Jiang</surname>
<given-names>Xudong</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Su</surname>
<given-names>Zhaodong</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Xue</surname>
<given-names>Ya-juan</given-names>
</name>
<xref ref-type="aff" rid="aff4">
<sup>4</sup>
</xref>
<xref ref-type="aff" rid="aff5">
<sup>5</sup>
</xref>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>State Key Laboratory of Oil and Gas Reservoir Geology and Exploitation, Chengdu University of Technology</institution>, <addr-line>Chengdu</addr-line>, <addr-line>Sichuan</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>School of Network &#x26; Communication Engineering, Chengdu Technological University</institution>, <addr-line>Chengdu</addr-line>, <country>China</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>College of Geophysics, Chengdu University of Technology</institution>, <addr-line>Chengdu</addr-line>, <addr-line>Sichuan</addr-line>, <country>China</country>
</aff>
<aff id="aff4">
<sup>4</sup>
<institution>Sichuan Provincial Key University Laboratory of Meteorological Information and Signal Processing, Chengdu University of Information Technology</institution>, <addr-line>Chengdu</addr-line>, <country>China</country>
</aff>
<aff id="aff5">
<sup>5</sup>
<institution>College of Communication Engineering, Chengdu University of Information Technology</institution>, <addr-line>Chengdu</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/1423308/overview">Paolo Capuano</ext-link>, University of Salerno, Italy</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/1917817/overview">Wenchao Chen</ext-link>, Xi&#x2019;an Jiaotong University, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/905057/overview">Baehyun Min</ext-link>, Ewha Womans University, Republic of Korea</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Junxing Cao, <email>caojx@cdut.edu.cn</email>
</corresp>
</author-notes>
<pub-date pub-type="epub">
<day>19</day>
<month>04</month>
<year>2023</year>
</pub-date>
<pub-date pub-type="collection">
<year>2023</year>
</pub-date>
<volume>11</volume>
<elocation-id>1117797</elocation-id>
<history>
<date date-type="received">
<day>06</day>
<month>12</month>
<year>2022</year>
</date>
<date date-type="accepted">
<day>03</day>
<month>04</month>
<year>2023</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2023 Ma, Cao, Liu, Jiang, Su and Xue.</copyright-statement>
<copyright-year>2023</copyright-year>
<copyright-holder>Ma, Cao, Liu, Jiang, Su and Xue</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 extraction of gas-bearing information from the deeply underground reservoir is extremely difficult due to the weak seismic response and complicated gas distribution characteristics. To predict gas-bearing reservoirs efficiently, we developed a deep neural network (DNN) embedding-based gas-bearing prediction scheme. First, the cepstrum coefficient that is sensitive to hydrocarbons is computed using the raw seismic data. A DNN model inspired by the x-vector in speech recognition is designed, comprising the long short-term memory (LSTM) networks and two fully connected (FC) networks, stacked from the bottom to the top layer. Then, the cepstrum features are fed into the DNN for training and testing, and DNN embedding is extracted from the top layers after optimized network parameters are determined. Finally, the gas-bearing probability of the reservoir is predicted by calculating the cosine distance between pairs of DNN embeddings. When applied to synthetic seismic data, the proposed method offers greater than 90% accuracy at SNR &#x3e; 3&#xa0;dB. Besides, the predicted result applied in deep carbonate reservoirs in China&#x2019;s Sichuan Basin is in basic agreement with the actual situation, demonstrating the certain feasibility of the proposed scheme.</p>
</abstract>
<kwd-group>
<kwd>gas-bearing prediction</kwd>
<kwd>DNN embedding</kwd>
<kwd>TDNN</kwd>
<kwd>LSTM</kwd>
<kwd>cepstrum</kwd>
<kwd>deep reservoirs</kwd>
</kwd-group>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-at-acceptance</meta-name>
<meta-value>Solid Earth Geophysics</meta-value>
</custom-meta>
</custom-meta-wrap>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>The targets for oil and gas exploration continue to develop to greater depths as the conventional technology for exploration in the petroleum industry advances. Deeply underground reservoirs are covered by massive thick sediments that have minimal physical differences from surrounding rocks, low porosity, strong non-homogeneity, and poor seismic response, making the distribution of oil and gas complicated. Traditional methods used to detect gas-bearing properties in reserves include the &#x201c;bright spot&#x201d; method (<xref ref-type="bibr" rid="B9">Hammond, 1974</xref>), AVO analysis (<xref ref-type="bibr" rid="B10">Hampson, 1991</xref>), and low-frequency shadowing (<xref ref-type="bibr" rid="B23">Taner et al., 1979</xref>). These methods are effective in specific scenarios (<xref ref-type="bibr" rid="B2">Cao et al., 2022</xref>), for example, bright spot technology is mainly useful in shallow unconsolidated clastic reservoirs, while AVO analysis technology is suitable for formations with a relatively simple and gentle structure. Low-frequency shadowing is mainly applied to lithologies that are already known. However, these traditional techniques are difficult to effectively quantify the complex and non-linear connection between seismic response and gas-bearing properties in deeply buried reservoirs.</p>
<p>Recently data-driven deep learning methods are widely used in geophysics for first-to-wave pickup (<xref ref-type="bibr" rid="B14">Liao et al., 2020</xref>; <xref ref-type="bibr" rid="B18">Qu et al., 2021</xref>), seismic data denoising (<xref ref-type="bibr" rid="B26">Wang and Chen, 2019</xref>; <xref ref-type="bibr" rid="B15">Liu et al., 2020</xref>; <xref ref-type="bibr" rid="B13">Liu et al., 2022</xref>), and seismic facies recognition (<xref ref-type="bibr" rid="B25">Tschannen et al., 2020</xref>; <xref ref-type="bibr" rid="B16">Liu et al., 2021</xref>). Due to the advantage of automatically characterizing complex multivariate non-linear relationships, DNN is also used for acquiring reservoir gas-bearing properties. For example, a deep neural network (DNN) model with several hidden layers (<xref ref-type="bibr" rid="B31">Yang et al., 2021</xref>; <xref ref-type="bibr" rid="B32">Zhang et al., 2022</xref>) is built for gas-bearing prediction by leveraging the capability of DNN to handle an end-to-end task. The convolution neural network (CNN), one of the most promising DNN approaches for geophysics issues, has been trained for extracting oil and gas properties (<xref ref-type="bibr" rid="B22">Song et al., 2022</xref>). The characteristics of the reservoir are reflected in the comparison with the surrounding rock layers above and below it. However, these methods primarily concentrate on learning the gas-bearing information of the target layer, and the contextual relationship between the seismic waveforms is not given the same level of attention.</p>
<p>Although there have been many deep learning methods applied to the processing and interpretation of seismic data, few studies have focused on hydrocarbon detection. This article presents an innovative experiment that uses neural networks to quantitatively identify the gas-bearing information in seismic records based on the similarities between seismic and acoustic data. The similarities are manifested in two aspects (<xref ref-type="bibr" rid="B29">Xie et al., 2017</xref>). First, seismic primary waves and acoustic waves can be considered as the same kind of wave since their propagation in the elastic medium follows the same physical laws. In addition, both can be characterized by convolutional models. The seismic record can be seen as a convolution of stratigraphic reflection coefficients and waves, and the acoustic record can be regarded as the convolution of the vocal cord excitation and the vocal tract. Therefore, speech feature parameters can be integrated into seismic data processing. For example, cepstrum is applied to the computation for thin beds thickness (<xref ref-type="bibr" rid="B8">Hall, 2006</xref>) and gas-bearing detection (<xref ref-type="bibr" rid="B24">Tian and Cao, 2011</xref>; <xref ref-type="bibr" rid="B30">Xue et al., 2016</xref>), and the Linear Prediction cepstral Coefficient (LPCC) is utilized for seismic facies analysis (<xref ref-type="bibr" rid="B28">Xie et al., 2016</xref>). With the demand for improving speaker recognition technology, the novel speech characteristics generated by DNN have grown increasingly prominent. Especially, the x-vector, namely, DNN embedding, captures accurately the vocal information of speakers by translating arbitrary-length inputs into fixed-length embeddings, making it effective for short-time records (<xref ref-type="bibr" rid="B20">Snyder et al., 2017</xref>; <xref ref-type="bibr" rid="B21">Snyder et al., 2018</xref>). Therefore, this article utilizes DNN embedding to predict gas-bearing reservoirs due to its outstanding feature extraction ability for short seismic responses.</p>
<p>Facing the problems of weak seismic response and thin thickness of deep buried reservoirs, we have improved and modified the DNN model prediction method. First of all, for data preparation, we obtained datasets tailored to seismic data characteristics. And the cepstrum is employed as the DNN input since it has been shown sensitive to the response of the gas-bearing layer (<xref ref-type="bibr" rid="B3">Cao et al., 2011</xref>; <xref ref-type="bibr" rid="B4">Cao et al., 2019</xref>). Secondly, in terms of the DNN model, it employed long short-term memory (LSTM) networks as the bottom layer to contextualize feature learning and the two FC layer as the primary top layer for embedding extraction. Thirdly, to visualize the gas-bearing distribution, the backend of the model outputs DNN embedding pairs&#x2019; similarity using cosine distance. Evaluations based on both synthetic and actual seismic records from China&#x2019;s Sichuan Basin demonstrate that our method has significant advantages over traditional SVM-based approach (<xref ref-type="bibr" rid="B24">Tian and Cao, 2011</xref>).</p>
</sec>
<sec sec-type="materials|methods" id="s2">
<title>2 Materials and methods</title>
<p>Since acoustic waves and seismic waves share certain similarities described above, it is theoretically possible to apply speaker recognition technology to identify certain geological bodies, such as gas-bearing reservoirs. Speaker recognition identifies the speaker by acquiring common features in numerous utterances. Similarly, when common characteristics in seismic records are extracted for gas-bearing prediction, the gas-bearing reservoir corresponds to the speaker, and the seismic records correspond to the acoustic records. Nonetheless, these two records differ, and the technique cannot be transferred directly. Based on the characteristics of the seismic data, the proposed scheme displayed in <xref ref-type="fig" rid="F1">Figure 1</xref> is designed for seismic records.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Workflow of gas-bearing prediction for the deep reservoir based on DNN Embeddings.</p>
</caption>
<graphic xlink:href="feart-11-1117797-g001.tif"/>
</fig>
<sec id="s2-1">
<title>2.1 Data preparation</title>
<p>When preparing the dataset, the difference in attenuation, repeatability, and frequency of seismic data must be taken into consideration (<xref ref-type="bibr" rid="B3">Cao et al., 2011</xref>; <xref ref-type="bibr" rid="B4">Cao et al., 2019</xref>).</p>
<sec id="s2-1-1">
<title>2.1.1 Attenuation</title>
<p>The speaker is the source of speech records, and there is no attenuation as time passes. While the source of seismic records is the reflection or dispersion of the seismic source signal, which is a secondary source and decays with increasing recording time. Therefore, amplitude-preserving processing is necessary (<xref ref-type="bibr" rid="B7">Gao et al., 2022</xref>) to remove the effects of spherical diffusion and inelastic attenuation.</p>
</sec>
<sec id="s2-1-2">
<title>2.1.2 Repeatability</title>
<p>The &#x201c;voiceprint&#x201d; characteristic is repeated in a single utterance for acoustic records, and a single speaker can give numerous bits of utterances. Seismic records are continuous and redundant (<xref ref-type="bibr" rid="B5">Col&#xe9;ou et al., 2003</xref>). The continuity means that the geological condition over a certain spatial range is similar, which is the foundation of tectonic and stratigraphic interpretation. The redundancy exists in some spreading information of wavefront propagation that occurs in both longitudinal and lateral directions. To sum up, seismic records within a certain lateral and longitudinal range can be approximately regarded as the response of a similar reservoir.</p>
</sec>
<sec id="s2-1-3">
<title>2.1.3 Short-time smoothness</title>
<p>Speech recognition decomposes acoustic records into frames, and each frame can be regarded as a smooth signal. The frequency of seismic records is much lower than the frequency of acoustic records, so the seismic response can only be considered smooth when the time window is narrow. Since the characteristics of the reservoir are reflected in the comparison with the surrounding rock above and below it, the window can be expanded within a reasonable range.</p>
</sec>
</sec>
<sec id="s2-2">
<title>2.2 Pre-processing</title>
<p>Before extracting the features from the raw seismic records, pre-processing needs to be implemented. Pre-processing consists of pre-emphasis, framing, and windowing operations. Except for important parameter values which are specially set according to our practical experience, the process is consistent with speech signal processing (<xref ref-type="bibr" rid="B17">Muda et al., 2010</xref>).</p>
</sec>
<sec id="s2-3">
<title>2.3 Feature extraction</title>
<p>The cepstrum feature is selected as the input feature for DNN to extract stratigraphic response features by taking into account the following factors. Firstly, the cepstrum feature is sensitive to gas-bearing characteristics in hydrocarbon prediction (<xref ref-type="bibr" rid="B3">Cao et al., 2011</xref>; <xref ref-type="bibr" rid="B4">Cao et al., 2019</xref>). Then, the cepstrum has a simple derivation process compared with the widely used Mel Frequency Cepstral Coefficient (MFCC) and the FilterBank (FBank) (<xref ref-type="bibr" rid="B33">Zheng et al., 2001</xref>; <xref ref-type="bibr" rid="B27">Wang et al., 2014</xref>) in speech recognition, which is represented in <xref ref-type="fig" rid="F2">Figure 2</xref>. Moreover, the cepstrum also can simplify the relation between seismic wavelet and stratigraphic reflection coefficients which will be demonstrated below.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>The extraction process of MFCC, FBank, and Cepstrum features.</p>
</caption>
<graphic xlink:href="feart-11-1117797-g002.tif"/>
</fig>
<p>The cepstrum is the real component of the Inverse Discrete Fourier transform (IDFT) for a time domain sequence&#x2019;s logarithmic amplitude spectrum, which is a homomorphic transform. Assume that <inline-formula id="inf1">
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<mml:mn>0,1,2</mml:mn>
<mml:mo>,</mml:mo>
<mml:mo>&#x2026;</mml:mo>
<mml:mo>,</mml:mo>
<mml:mi>N</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:math>
</inline-formula> is the discrete sampling of the analog frequency.</p>
<p>The discrete seismic signal is expressed as the following equation based on the seismic record convolutional model.<disp-formula id="e2">
<mml:math id="m13">
<mml:mrow>
<mml:mi>s</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>w</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x2217;</mml:mo>
<mml:mi>r</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(2)</label>
</disp-formula>
</p>
<p>In <xref ref-type="disp-formula" rid="e2">Formula 2</xref>, <inline-formula id="inf12">
<mml:math id="m14">
<mml:mrow>
<mml:mi>r</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula> is the stratigraphic reflection coefficient, <inline-formula id="inf13">
<mml:math id="m15">
<mml:mrow>
<mml:mi>w</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>n</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula> is the seismic wavelet, which is typically the Ricker wavelet, and <inline-formula id="inf14">
<mml:math id="m16">
<mml:mrow>
<mml:mo>&#x2a;</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> is the convolution operation. According to <xref ref-type="disp-formula" rid="e1">Formula 1</xref>, the cepstrum domain parameters of the seismic record can be computed as follows.<disp-formula id="e3">
<mml:math id="m17">
<mml:mrow>
<mml:mi>R</mml:mi>
<mml:mi>e</mml:mi>
<mml:mrow>
<mml:mfenced open="[" close="]" separators="|">
<mml:mrow>
<mml:msup>
<mml:mi>F</mml:mi>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msup>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi mathvariant="italic">log</mml:mi>
<mml:mrow>
<mml:mfenced open="|" close="|" separators="|">
<mml:mrow>
<mml:mi>S</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>R</mml:mi>
<mml:mi>e</mml:mi>
<mml:mrow>
<mml:mfenced open="[" close="]" separators="|">
<mml:mrow>
<mml:msup>
<mml:mi>F</mml:mi>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msup>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi mathvariant="italic">log</mml:mi>
<mml:mrow>
<mml:mfenced open="|" close="|" separators="|">
<mml:mrow>
<mml:mi>W</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x2b;</mml:mo>
<mml:mi>R</mml:mi>
<mml:mi>e</mml:mi>
<mml:mrow>
<mml:mfenced open="[" close="]" separators="|">
<mml:mrow>
<mml:msup>
<mml:mi>F</mml:mi>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msup>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi mathvariant="italic">log</mml:mi>
<mml:mrow>
<mml:mfenced open="|" close="|" separators="|">
<mml:mrow>
<mml:mi>R</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(3)</label>
</disp-formula>
</p>
<p>In <xref ref-type="disp-formula" rid="e3">Formula 3</xref>, <inline-formula id="inf15">
<mml:math id="m18">
<mml:mrow>
<mml:mi>S</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>,</mml:mo>
<mml:mi>W</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula> and <inline-formula id="inf16">
<mml:math id="m19">
<mml:mrow>
<mml:mi>R</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>k</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula> are the spectrum of seismic record, seismic wavelet, and reflection coefficients, respectively. In the cepstrum domain, the correlation between seismic wavelet and reflection coefficient becomes simple, i.e., the convolutional relationship in the time domain becomes a sum of two in the cepstrum. Before input to DNN, the energy, mean, and variance of the cepstrum are added to the first three dimensions of each frame feature to enhance the dimensionality of the feature parameters.</p>
</sec>
<sec id="s2-4">
<title>2.4 Training DNN model</title>
<p>The DNN architecture is comparable to the network architecture in the Kaldi Voxceleb recipe (<xref ref-type="bibr" rid="B12">Kumar et al., 2020</xref>), which consists of the frame-level layer, segment-level layer, and softmax layer as shown in <xref ref-type="fig" rid="F3">Figure 3</xref>. The first frame-level layers in Kaldi consist of time-delay neural networks (TDNN) with a context and are utilized for learning repetitive features in multiple frames. In this paper, we suggest switching from TDNN to LSTM networks, because that LSTM can automatically learn long-term relationships between sequences and have a similar time-delay function. And then, the segment-level layer gathers information from the context to recognize the segment characteristics of seismic records, among which, a statistical pooling layer combines the mean and standard deviation from the output of frame 5, and two fully connected (FC) layers can be utilized to extract embedding after the training is completed. The number of hidden layer nodes is reduced according to the length of the frame there because of the smaller size of seismic data. The top softmax layer outputs the maximum posterior probability for each reservoir type and it is no longer required once the DNN training is complete. In addition, each layer has a batch normalization (BN) layer and a rectified linear units (ReLUs) activation function to enhance DNN performance.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>The DNN architecture of the proposed scheme.</p>
</caption>
<graphic xlink:href="feart-11-1117797-g003.tif"/>
</fig>
</sec>
<sec id="s2-5">
<title>2.5 Scoring prediction</title>
<p>The front of our proposed method is used for extracting seismic embeddings. Once the DNN model has been trained, two FC layers produce the embeddings, which are the representations of the seismic records. The output of segment 1 is Embedding a (EMa), which is immediately output on the statistics layer, while the output of segment 2 is Embedding b (EMb), which is extracted from the FC layer after the ReLUs layer.</p>
<p>The back-end in our scheme is scoring prediction based on the embedding similarity. The embedding of the gas reserve is derived from the seismic record adjacent to the gas-bearing well, which is indicated as <inline-formula id="inf17">
<mml:math id="m20">
<mml:mrow>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>M</mml:mi>
<mml:mi>g</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. Similarly, the embedding for a seismic record to be predicted is labeled as <inline-formula id="inf18">
<mml:math id="m21">
<mml:mrow>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>M</mml:mi>
<mml:mi>p</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. The embedding similarity between <inline-formula id="inf19">
<mml:math id="m22">
<mml:mrow>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>M</mml:mi>
<mml:mi>g</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> and <inline-formula id="inf20">
<mml:math id="m23">
<mml:mrow>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>M</mml:mi>
<mml:mi>p</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> represents the gas-bearing probability of the corresponding layer where the seismic records are located. The normalized cosine distance is employed in this research to represent the similarity, which is described by the equation below.<disp-formula id="e4">
<mml:math id="m24">
<mml:mrow>
<mml:mi mathvariant="italic">Cos</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>M</mml:mi>
<mml:mi>g</mml:mi>
</mml:msub>
<mml:mo>,</mml:mo>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>M</mml:mi>
<mml:mi>p</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0.5</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>M</mml:mi>
<mml:mi>g</mml:mi>
</mml:msub>
<mml:mo>&#x2219;</mml:mo>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>M</mml:mi>
<mml:mi>p</mml:mi>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mrow>
<mml:mfenced open="&#x2016;" close="&#x2016;" separators="|">
<mml:mrow>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>M</mml:mi>
<mml:mi>g</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
<mml:mo>&#x2219;</mml:mo>
<mml:mrow>
<mml:mfenced open="&#x2016;" close="&#x2016;" separators="|">
<mml:mrow>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>M</mml:mi>
<mml:mi>p</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:mfrac>
<mml:mo>&#x2b;</mml:mo>
<mml:mn>0.5</mml:mn>
</mml:mrow>
</mml:math>
<label>(4)</label>
</disp-formula>
</p>
</sec>
</sec>
<sec id="s3">
<title>3 The experiment of the geological model</title>
<p>A geological attenuation model was developed to test the effectiveness of gas-bearing prediction with the dispersive viscosity equation (<xref ref-type="bibr" rid="B11">He et al., 2009</xref>). By referring to reservoir logging parameters and geological data in the Sichuan Basin, China, the geological model was designed and its parameters were configured in <xref ref-type="table" rid="T1">Table 1</xref>. In <xref ref-type="fig" rid="F4">Figure 4A</xref>, Layer &#x2462;, &#x2463;, and &#x2464; are the water-bearing reservoir, the gas-bearing reservoir, and the gas-water mixed reservoir, respectively, and they are all 40&#xa0;m thick. The Ricker wavelet with a frequency of 30&#xa0;Hz is employed to imitate seismic records, and the digital sampling frequency is 500&#xa0;Hz. The model is first orthorectified based on the viscous dispersive wave equation, and then the simulated seismic profile was obtained by applying conventional wave equation offset. As a result, the synthetic seismic record is generated as shown in <xref ref-type="fig" rid="F4">Figure 4B</xref>, which is without noise. A particular amount of Gaussian white noise is added to the seismic record to imitate the low signal-to-noise (SNR) environment of the deeply underground reservoir. The SNR of the synthetic seismic record after adding noise ranges from 1&#xa0;dB to 10&#xa0;dB. <xref ref-type="fig" rid="F4">Figures 4C, D</xref> show the synthetic seismic data at SNR &#x3d; 1&#xa0;dB and SNR &#x3d; 10dB, respectively.</p>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Rock properties for the geological model (where, <inline-formula id="inf21">
<mml:math id="m25">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">V</mml:mi>
<mml:mi mathvariant="normal">p</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the primary velocity, <inline-formula id="inf22">
<mml:math id="m26">
<mml:mrow>
<mml:mi mathvariant="normal">&#x3c1;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is the density, <inline-formula id="inf23">
<mml:math id="m27">
<mml:mrow>
<mml:mi mathvariant="normal">&#x3be;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is the dispersion coefficient, <inline-formula id="inf24">
<mml:math id="m28">
<mml:mrow>
<mml:mi mathvariant="normal">&#x3b7;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is the viscosity coefficient, <inline-formula id="inf25">
<mml:math id="m29">
<mml:mrow>
<mml:mi mathvariant="normal">Q</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> is the attenuation coefficient).</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Layer number</th>
<th align="left">
<inline-formula id="inf26">
<mml:math id="m30">
<mml:mrow>
<mml:msub>
<mml:mi mathvariant="normal">V</mml:mi>
<mml:mi mathvariant="normal">p</mml:mi>
</mml:msub>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi mathvariant="normal">m</mml:mi>
<mml:mo>.</mml:mo>
<mml:msup>
<mml:mi mathvariant="normal">s</mml:mi>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula>
</th>
<th align="left">
<inline-formula id="inf27">
<mml:math id="m31">
<mml:mrow>
<mml:mi mathvariant="normal">&#x3c1;</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:mi mathvariant="normal">g</mml:mi>
<mml:mo>.</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mi mathvariant="normal">c</mml:mi>
<mml:mi mathvariant="normal">m</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>3</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula>
</th>
<th align="left">
<inline-formula id="inf28">
<mml:math id="m32">
<mml:mrow>
<mml:mi mathvariant="normal">&#x3be;</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> (HZ)</th>
<th align="left">
<inline-formula id="inf29">
<mml:math id="m33">
<mml:mrow>
<mml:mi mathvariant="normal">&#x3b7;</mml:mi>
<mml:mrow>
<mml:mfenced open="(" close=")" separators="|">
<mml:mrow>
<mml:msup>
<mml:mi mathvariant="normal">m</mml:mi>
<mml:mn>2</mml:mn>
</mml:msup>
<mml:mo>.</mml:mo>
<mml:msup>
<mml:mi mathvariant="normal">s</mml:mi>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula>
</th>
<th align="left">
<inline-formula id="inf30">
<mml:math id="m34">
<mml:mrow>
<mml:mi mathvariant="normal">Q</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>
</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">&#x2460;</td>
<td align="left">6,246</td>
<td align="left">2.7290</td>
<td align="left">1</td>
<td align="left">1</td>
<td align="left">200</td>
</tr>
<tr>
<td align="left">&#x2461;</td>
<td align="left">6,109</td>
<td align="left">2.6850</td>
<td align="left">1</td>
<td align="left">1</td>
<td align="left">200</td>
</tr>
<tr>
<td align="left">&#x2462;</td>
<td align="left">6,400</td>
<td align="left">2.7800</td>
<td align="left">30</td>
<td align="left">3</td>
<td align="left">15</td>
</tr>
<tr>
<td align="left">&#x2463;</td>
<td align="left">5,900</td>
<td align="left">2.7280</td>
<td align="left">10</td>
<td align="left">500</td>
<td align="left">5</td>
</tr>
<tr>
<td align="left">&#x2464;</td>
<td align="left">5,950</td>
<td align="left">2.7605</td>
<td align="left">20</td>
<td align="left">200</td>
<td align="left">8</td>
</tr>
<tr>
<td align="left">&#x2465;</td>
<td align="left">6,422</td>
<td align="left">2.7256</td>
<td align="left">1</td>
<td align="left">1</td>
<td align="left">200</td>
</tr>
<tr>
<td align="left">&#x2466;</td>
<td align="left">6,426</td>
<td align="left">2.8364</td>
<td align="left">1</td>
<td align="left">1</td>
<td align="left">200</td>
</tr>
</tbody>
</table>
</table-wrap>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>
<bold>(A)</bold> Geological model. <bold>(B)</bold> The synthetic seismic record without noise. <bold>(C)</bold> The synthetic seismic record with SNR &#x3d; 1&#xa0;dB. <bold>(D)</bold> The synthetic seismic record with SNR &#x3d; 10&#xa0;dB.</p>
</caption>
<graphic xlink:href="feart-11-1117797-g004.tif"/>
</fig>
<p>When preparing the dataset, the seismic records including the stratigraphic response of layers &#x2462;, &#x2463;, and &#x2464; are divided into the seismic response of the water-bearing reservoir, the gas-bearing reservoir, and the gas-water mixed reservoir, respectively. Ten seismic records with stratigraphic responses around layers &#x2462;, &#x2463;, and &#x2464; are eliminated to limit the impact of distinct stratigraphic borders. Among the stratigraphic responses of each type of reservoir, 60% and 10% of the seismic records are selected randomly as training datasets and validation datasets respectively, while the remaining 30% are test datasets. In pre-processing and feature extraction, the parameter values are all adopted by our prior experiment. The pre-emphasis coefficient is 0.93, the frame length is set to 20 milliseconds (ms), and the frameshift is set the half of the frame length. Besides, Hamming window is selected because the cepstrum coefficient calculated from it is relatively stable. Then, the seismic records&#x2019; cepstrum parameters are calculated and fed into the DNN model. The DNN model in Kaldi is primarily written in C&#x2b;&#x2b;, whereas the proposed DNN model is constructed and trained in Pytorch. When training a DNN model, the objective function is a multiclassification cross-entropy function, the optimizer uses Adam (<xref ref-type="bibr" rid="B1">Barakat and Bianchi, 2021</xref>), and the learning strategy is OneCycle (<xref ref-type="bibr" rid="B19">Smith, 2017</xref>). The training process at extremely low SNR (1&#xa0;dB&#x223c;4&#xa0;dB) is represented in <xref ref-type="fig" rid="F5">Figure 5</xref>, while the training results with SNR greater than 4&#xa0;dB are not shown since the accuracy of the training and validation datasets exceeds 98% and the loss is less than 0.1.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>
<bold>(A, B)</bold>Accuracy for training and validation sets. <bold>(C, D)</bold>Loss for training and validation sets.</p>
</caption>
<graphic xlink:href="feart-11-1117797-g005.tif"/>
</fig>
<p>When the training of the DNN model is completed, the parameter values of each DNN layer are fixed. The embedding extracted from the seismic records at the center of layers &#x2462;, &#x2463;, and &#x2464; is regarded as the embedding of reservoirs in which they are located. The cosine distance between the embedding of the seismic record to be predicted and three types of reservoir embedding is calculated respectively, and the reservoir corresponding to the highest cosine distance is the predicted reservoir. When the DNN input features are Cepstrum, MFCC, and FBank, three alternative gas-bearing prediction models are generated. From the result indicated in <xref ref-type="fig" rid="F6">Figures 6A, B</xref>, it can be seen that cepstrum as a feature parameter has a robust advantage over the other two features.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>The predicted error rate of the geological model. <bold>(A)</bold> EMa with different DNN inputs. <bold>(B)</bold> EMb with different DNN inputs. <bold>(C)</bold> EMa with different architectures. <bold>(D)</bold> EMb with different architectures.</p>
</caption>
<graphic xlink:href="feart-11-1117797-g006.tif"/>
</fig>
<p>The bottom layer of the x-vector uses TDNN with context to learn the segment feature in speech recognition. The effective response time of the reservoir in the seismic record is shorter than that of the speech record, and a shorter context should be set. In order to assess the impact of contextual width, we configure the TDNN-based gas-bearing prediction models with three time-delay strategies. These three strategies, labeled as TDNN_311, TDNN_331, and TDNN_333, set the context of frames 1, frame 1&#x223c;2, and frames 1&#x223c;3 to 3 respectively, while the other layers have no delay. TDNN is implemented in the deep learning toolkit Torch by 1d-CNN because TDNN is equivalent to 1d-CNN (<xref ref-type="bibr" rid="B6">Daniel et al., 2018</xref>). Because the process of selecting the optimal combination from the three schemes is somewhat inefficient, we propose to replace TDNN with LSTM. To compare the improvement of the proposed method, we also compare it with previous studies (<xref ref-type="bibr" rid="B24">Tian and Cao, 2011</xref>), in which the absolute value of the difference between 1 and 2-order cepstral coefficients is extracted as the training samples of the support vector machine (SVM) classifier. The predicted error rate of the test samples belonging to the corresponding reserve is calculated based on different architectures respectively, which is shown in <xref ref-type="fig" rid="F6">Figures 6C, D</xref>. The superior performance of LSTM shows that it may automatically learn the long-term relationships among sequences with the use of input gates, forgetting gates, output gates, and internal memory units.</p>
</sec>
<sec id="s4">
<title>4 The experiment of field</title>
<p>The work area is located in the Xiaoquan&#x2013;Xinchang tectonic belt of the western Sichuan exploration area in China, with 150 <inline-formula id="inf31">
<mml:math id="m35">
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<mml:mn>2</mml:mn>
</mml:msup>
</mml:mrow>
</mml:math>
</inline-formula> as shown in <xref ref-type="fig" rid="F7">Figure 7</xref>. This tectonic zone is mainly zonal distribution located in the Longmenshan foreland basin, one of the most important China&#x2019;s natural gas-rich areas. The marine strata of this area dominated by carbonate is buried deep (about 4,000&#xa0;m&#x2013;7,000&#xa0;m) including from Sinian to Middle Triassic. In this area, the Upper Triassic Maan Tang Formation (<inline-formula id="inf32">
<mml:math id="m36">
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</inline-formula>) and the Leikoupo Formation (<inline-formula id="inf33">
<mml:math id="m37">
<mml:mrow>
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<mml:mi>T</mml:mi>
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<mml:mi>l</mml:mi>
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</mml:math>
</inline-formula>) are the target layer due to massive natural gas resources. The thickness of the gas reservoir is thin, which results in minor differences in the physical parameters of the gas-bearing layer and surrounding rocks, and the poor seismic response signal makes exploration with current technologies more difficult. There are three drilled well sites in the field area, and the geological formations of Well A, Well B, and Well C are a water-bearing reservoir, a gas-bearing reservoir, and a gas-water mixed reservoir in the target layer, respectively. When the datasets are generated, the seismic record from the top weathered crust of <inline-formula id="inf34">
<mml:math id="m38">
<mml:mrow>
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</inline-formula> to the bottom of <inline-formula id="inf35">
<mml:math id="m39">
<mml:mrow>
<mml:msub>
<mml:mi>T</mml:mi>
<mml:mn>2</mml:mn>
</mml:msub>
<mml:msub>
<mml:mi>l</mml:mi>
<mml:mn>4</mml:mn>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> (around 150&#xa0;m) is intercepted as the target layer along longitudinal time. Moreover, the seismic data (about 450 records) in the lateral 300&#xa0;m range around Well A, B, and C is chosen. The seismic records close to the three wells are divided into three distinct types of stratigraphic response, namely, the seismic response of the water-bearing layer, the gas-bearing layer, and the gas-water mixed layer. The training and the validation curve are represented in <xref ref-type="fig" rid="F8">Figure 8</xref>.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Structural diagram of the study area <xref ref-type="bibr" rid="B2">Cao et al. (2022)</xref>.</p>
</caption>
<graphic xlink:href="feart-11-1117797-g007.tif"/>
</fig>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>Accuracy and loss based on the field data.</p>
</caption>
<graphic xlink:href="feart-11-1117797-g008.tif"/>
</fig>
<p>After training, the seismic embeddings nearest to three wells are generated and used as the reservoir represent in which they are located. The cosine distances are calculated independently by the embeddings of the to-be-predicted seismic records and the embeddings of three reservoirs. Subsequently, the cosine score with the gas reservoir indicates the gas-bearing probability. When the Cepstrum, MFCC, and FBank are selected as input features, it shows the same phenomenon in the geological model that the error rate with Cepstrum is lower than that of the other two feature parameters in <xref ref-type="fig" rid="F9">Figure 9A</xref>. Similarly, <xref ref-type="fig" rid="F9">Figure 9B</xref> shows that LSTM has a moderate performance compared with the three strategies of TDNN and obvious advantages over previous SVM architectures. Further, we list the probabilities of the test samples belonging to each category with the proposed and the previous method in <xref ref-type="fig" rid="F10">Figure 10</xref>. To make the comparison fairer, we normalized each probability using the formula below, where <inline-formula id="inf36">
<mml:math id="m40">
<mml:mrow>
<mml:mi>j</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1,2,3</mml:mn>
</mml:mrow>
</mml:math>
</inline-formula> denote the three categories of reservoirs, respectively, <inline-formula id="inf37">
<mml:math id="m41">
<mml:mrow>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mi>j</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the initial probability, and <inline-formula id="inf38">
<mml:math id="m42">
<mml:mrow>
<mml:msub>
<mml:mover accent="true">
<mml:mi>P</mml:mi>
<mml:mo>&#x2d9;</mml:mo>
</mml:mover>
<mml:mi>j</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> is the normalized probability.<disp-formula id="e5">
<mml:math id="m43">
<mml:mrow>
<mml:msub>
<mml:mover accent="true">
<mml:mi>P</mml:mi>
<mml:mo>&#x2d9;</mml:mo>
</mml:mover>
<mml:mi>j</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mi>j</mml:mi>
</mml:msub>
<mml:mrow>
<mml:mstyle displaystyle="true">
<mml:munderover>
<mml:mo>&#x2211;</mml:mo>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mn>3</mml:mn>
</mml:munderover>
</mml:mstyle>
<mml:msub>
<mml:mi>P</mml:mi>
<mml:mi>i</mml:mi>
</mml:msub>
</mml:mrow>
</mml:mfrac>
<mml:mo>,</mml:mo>
<mml:mi>j</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>1,2,3</mml:mn>
</mml:mrow>
</mml:math>
<label>(5)</label>
</disp-formula>
</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>The predicted error rate of the field. <bold>(A)</bold> With different DNN inputs. <bold>(B)</bold> With different architectures.</p>
</caption>
<graphic xlink:href="feart-11-1117797-g009.tif"/>
</fig>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>
<bold>(A)</bold> The predicted probability based on EMb. <bold>(B)</bold> The predicted probability based on SVM.</p>
</caption>
<graphic xlink:href="feart-11-1117797-g010.tif"/>
</fig>
<p>To visualize the gas-bearing distribution clearly, the proposed approach is applied to the whole work area. In <xref ref-type="fig" rid="F11">Figure 11</xref>, the value of the region predicted as reservoir B is equal to the cosine scoring, whereas the value of the region predicted to be reservoir A and C are set to 0 and 0.5, respectively. The prediction results based on the two embeddings show comparable gas-bearing distribution zones, while the gas-bearing region based on EMb is slightly larger which is consistent with the result in <xref ref-type="fig" rid="F9">Figure 9</xref> that fewer of the gas-bearing test samples are poorly predicted.</p>
<fig id="F11" position="float">
<label>FIGURE 11</label>
<caption>
<p>Predicted gas-bearing probability in the work area. <bold>(A)</bold> Based on EMa. <bold>(B)</bold> Based on EMb.</p>
</caption>
<graphic xlink:href="feart-11-1117797-g011.tif"/>
</fig>
</sec>
<sec sec-type="conclusion" id="s5">
<title>5 Conclusion</title>
<p>To deal with the difficult challenge of gas-bearing prediction in deeply buried reservoirs, this paper proposes an innovative gas-bearing prediction model based on DNN embedding. Motivated by the similarity between seismic data and acoustic data, the DNN model is designed by referring to the structure of the x-vector in speech identification, in which gas-sensitive cepstral parameters are the input, the bottom layers are LSTM networks that can learn the contextual relationship of the seismic waveforms, and the output is a DNN embedding used for similarity scoring. The validity of the proposed method was demonstrated in both generated synthetic seismic records and actual seismic data. The next study is to consider the hyperparametric assessment since the parameters in feature extraction and DNN training are mainly chosen empirically. Furthermore, data augmentation might be explored to improve predictive capabilities because data amount is the fundamental restriction of DNN.</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>All authors listed have made a substantial, direct, and intellectual contribution to the work and approved it for publication.</p>
</sec>
<sec id="s8">
<title>Funding</title>
<p>The authors declare that this study received funding from the project of the SINOPEC Science and Technology Department (Grant No. P20055-6). The funder was not involved in the study design, collection, analysis, interpretation of data, the writing of this article, or the decision to submit it for publication.</p>
<p>This work was supported by the National Natural Science Foundation of China (Grant Nos. 42030812 and 41974160), Chengdu University of Technology Postgraduate Innovative Cultivation Program (Grant No. CDUT2022BJCX009), Technological Development for Sichuan Province (2021ZYD0030), and Natural Science Foundation of Sichuan (No. 2023NSFSC0258).</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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