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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Phys.</journal-id>
<journal-title>Frontiers in Physics</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Phys.</abbrev-journal-title>
<issn pub-type="epub">2296-424X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">839699</article-id>
<article-id pub-id-type="doi">10.3389/fphy.2022.839699</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physics</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Characteristic Sequence Analysis of Giant Panda Voiceprint</article-title>
<alt-title alt-title-type="left-running-head">Hu et&#x20;al.</alt-title>
<alt-title alt-title-type="right-running-head">Panda Voiceprint Sequence Analysis</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Hu</surname>
<given-names>Shaoxiang</given-names>
</name>
<xref ref-type="aff" rid="aff1">
<sup>1</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1605422/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Liao</surname>
<given-names>Zhiwu</given-names>
</name>
<xref ref-type="aff" rid="aff2">
<sup>2</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1534941/overview"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Hou</surname>
<given-names>Rong</given-names>
</name>
<xref ref-type="aff" rid="aff3">
<sup>3</sup>
</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1443676/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Chen</surname>
<given-names>Peng</given-names>
</name>
<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/1586645/overview"/>
</contrib>
</contrib-group>
<aff id="aff1">
<sup>1</sup>
<institution>School of Automation Engineering</institution>, <institution>University of Electronic Science and Technology of China</institution>, <addr-line>Chengdu</addr-line>, <country>China</country>
</aff>
<aff id="aff2">
<sup>2</sup>
<institution>School of Computer Science</institution>, <institution>Sichuan Normal University</institution>, <addr-line>Chengdu</addr-line>, <country>China</country>
</aff>
<aff id="aff3">
<sup>3</sup>
<institution>Chengdu Research Base of Giant Panda Breeding</institution>, <institution>Sichuan Key Laboratory of Conservation Biology for Endangered Wildlife</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/838750/overview">Ming Li</ext-link>, Zhejiang University, 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/1607253/overview">Jianwei Yang</ext-link>, Nanjing University of Information Science and Technology, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/426391/overview">Junyu He</ext-link>, Zhejiang University, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Peng Chen, <email>capricorncp@163.com</email>
</corresp>
<fn fn-type="other">
<p>This article was submitted to Interdisciplinary Physics, a section of the journal Frontiers in Physics</p>
</fn>
</author-notes>
<pub-date pub-type="epub">
<day>21</day>
<month>02</month>
<year>2022</year>
</pub-date>
<pub-date pub-type="collection">
<year>2022</year>
</pub-date>
<volume>10</volume>
<elocation-id>839699</elocation-id>
<history>
<date date-type="received">
<day>20</day>
<month>12</month>
<year>2021</year>
</date>
<date date-type="accepted">
<day>14</day>
<month>01</month>
<year>2022</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2022 Hu, Liao, Hou and Chen.</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Hu, Liao, Hou and Chen</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&#x20;terms.</p>
</license>
</permissions>
<abstract>
<p>By analyzing the voiceprint characteristics of giant panda&#x2019;s voice, this study proposes a giant panda individual recognition method based on the characteristics of the composite Mel composite frequency cepstral coefficient (CMFCC) and proves that the characteristic sequence of the CMFCC has long-range dependent characteristics. First, the MFCC (Mel composite frequency cepstral coefficient) with a low frequency resolution is obtained by the Mel filter bank; then, the inverse Mel frequency cepstral coefficient (IMFCC) features of giant panda calls are extracted. The CMFCC characteristic sequence of giant panda voice composed of the MFCC and IMFCC improves the resolution of high- and low-frequency resolution characteristics of giant panda voice. Finally, the first-order difference characteristic parameters of the MFCC are integrated to obtain the difference characteristics between frames. Through experiments, the improvement of the system recognition effect is verified, and the recognition accuracy meets the theoretical expectation.</p>
</abstract>
<kwd-group>
<kwd>MFCC</kwd>
<kwd>long-range dependent</kwd>
<kwd>individual recognition</kwd>
<kwd>voiceprint</kwd>
<kwd>Gaussian mixture model</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Voiceprint is a collection of various common acoustic feature maps. It is a sound feature measured by special acoustic instruments. The core of voiceprint recognition is to extract its unique speech features from the collected speech information. The feature template is formed after recognition training. During recognition, the speech used is matched with the data in the template library, and the score is calculated to judge the speaker&#x2019;s identity [<xref ref-type="bibr" rid="B1">1</xref>]. Since 1930, there has been a basic research study on speaker recognition [<xref ref-type="bibr" rid="B2">2</xref>]. In 1962, the term &#x201c;voiceprint&#x201d; officially appeared as a sound texture feature [<xref ref-type="bibr" rid="B3">3</xref>]. After that, S. Pruzansky proposed a matching method based on probability value estimation and correlation calculation [<xref ref-type="bibr" rid="B4">4</xref>]. At the same time, the focus of recognition has become to select and extract the corresponding feature recognition parameters. Since 1970, voiceprint features such as the short-term average energy feature, linear prediction cepstral coefficient LPC (linear prediction coefficient), and Mel frequency cepstral coefficients MFCC (Mel frequency cepstral coefficients) have emerged. At the same time, some methods have also been used to extract feature parameters by using cepstral coefficients or introducing first- and second-order dynamic differences [<xref ref-type="bibr" rid="B5">5</xref>]. After the 1980s, characteristic parameters such as time domain decomposition, frequency domain decomposition, and wavelet packet node energy also gradually appeared and were widely used [<xref ref-type="bibr" rid="B6">6</xref>]. Jinxi Guo et&#x20;al. studied the recognition system in the noise environment [<xref ref-type="bibr" rid="B7">7</xref>] and made some achievements and progress.</p>
<p>Voiceprint feature is a key link in human voiceprint recognition technology and related applications. Considering the similarity of the way of sound production between giant pandas and humans, as well as the universality and wide application of voiceprint recognition technology, the voice of giant pandas can be analyzed and studied. At present, there is no case of research on individual recognition of giant pandas based on voiceprint features, especially because of the precious voice data of giant pandas, and the giant pandas and their call waveforms are shown in <xref ref-type="fig" rid="F1">Figure&#x20;1</xref>.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Giant panda and its sound waveform.</p>
</caption>
<graphic xlink:href="fphy-10-839699-g001.tif"/>
</fig>
<p>Voiceprint feature extraction algorithms mainly include the following [<xref ref-type="bibr" rid="B5">5</xref>]: the strong representation ability of the speech signal, good recognition effect, good self-specificity and feature exclusivity, simple operation, and convenient calculation.</p>
<p>In 2021, Li Ming proposed the mmfGn (modified multifractional Gaussian noise) theorem of long-range dependence (LRD) and short-range dependence and used the time-varying Hurst parameter to describe the time-varying sea level of LRD [<xref ref-type="bibr" rid="B8">8</xref>]. A new generalized fractional Gaussian noise (gfGn) is introduced. The study uses gfGn to model the actual traffic trace exhibition. The gfGn model is more accurate than the traditional fractional Gaussian noise (fGn) traffic modeling&#x20;[<xref ref-type="bibr" rid="B9">9</xref>].</p>
<p>In 2021, Junyu used the Bayesian maximum entropy (BME) method to represent the internal spatiotemporal dependence of sea surface chlorophyll concentration (SSCC) distribution [<xref ref-type="bibr" rid="B10">10</xref>]. The Hurst index value of chlorophyll on the ocean surface ranges from 0.6757 to 0.8431. A high Hurst index value represents strong LRD, which may be a common phenomenon of daily sea surface chlorophyll&#x20;[<xref ref-type="bibr" rid="B11">11</xref>].</p>
<p>This study focuses on the analysis and optimization of the Mel frequency cepstral coefficient of giant panda voice, discusses the long-range&#x2013;dependent characteristics of feature sequence, analyzes the voiceprint feature sequence suitable for the giant panda individual recognition system, and realizes the individual recognition algorithm based on the giant panda voiceprint.</p>
</sec>
<sec id="s2">
<title>2 Mel Frequency Cepstral Coefficients</title>
<p>Mel frequency cepstral coefficients (MFCCs) are voiceprint features extracted by combining the auditory perception characteristics of human ears with the generation mechanism of speech [<xref ref-type="bibr" rid="B12">12</xref>]. The sensitivity of the human ear to sound is not linear, but it changes with the change in frequency. It is more sensitive to low-frequency sound than high-frequency sound. According to the perceptual characteristics of the human auditory system, the Mel cepstral coefficient is widely used in voiceprint recognition.</p>
<sec id="s2-1">
<title>2.1 Mel Frequency Cepstral Coefficients of Giant Panda</title>
<p>The frequency corresponding to the MFCC is the Mel frequency, which is recorded as <inline-formula id="inf1">
<mml:math id="m1">
<mml:mrow>
<mml:msub>
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<mml:mi>l</mml:mi>
</mml:mrow>
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</inline-formula>, and its functional correspondence with frequency <inline-formula id="inf2">
<mml:math id="m2">
<mml:mi>f</mml:mi>
</mml:math>
</inline-formula> is as follows:<disp-formula id="e2_1">
<mml:math id="m3">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mrow>
<mml:mi>m</mml:mi>
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<mml:mi>l</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>2595</mml:mn>
<mml:mo>&#xd7;</mml:mo>
<mml:mi mathvariant="normal">lo</mml:mi>
<mml:msub>
<mml:mi mathvariant="normal">g</mml:mi>
<mml:mrow>
<mml:mn>10</mml:mn>
</mml:mrow>
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<mml:mrow>
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<mml:mrow>
<mml:mn>700</mml:mn>
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</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(2.1)</label>
</disp-formula>
</p>
<p>The following is the extraction process of the Mel frequency cepstral coefficient:<list list-type="simple">
<list-item>
<p>1) First, the original speech signal <inline-formula id="inf3">
<mml:math id="m4">
<mml:mrow>
<mml:mi>s</mml:mi>
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</inline-formula> is sampled at the sampling frequency of 44.1&#xa0;KHz and quantized in the 16bit mode, and then, the background noise and high-frequency noise are eliminated by using a bandpass filter. Finally, the time domain signal <inline-formula id="inf4">
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</inline-formula> is obtained by using a pre emphasis technology to compensate the high-frequency loss of sound. Then, it is transformed by formula <xref ref-type="disp-formula" rid="e2_2">Eq. 2.2</xref> to obtain the corresponding linear spectrum <inline-formula id="inf5">
<mml:math id="m6">
<mml:mrow>
<mml:mi>X</mml:mi>
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</inline-formula>, where <inline-formula id="inf6">
<mml:math id="m7">
<mml:mi>k</mml:mi>
</mml:math>
</inline-formula> is the time domain frequency corresponding to each point of the original speech signal.</p>
</list-item>
</list>
<disp-formula id="e2_2">
<mml:math id="m8">
<mml:mrow>
<mml:mi>X</mml:mi>
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<mml:mstyle displaystyle="true">
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<label>(2.2)</label>
</disp-formula>
<list list-type="simple">
<list-item>
<p>2) The Mel frequency filter bank composed of a group of triangular filters is used to filter the linear spectrum to obtain the Mel spectrum, and then, its logarithmic energy is calculated to obtain the logarithmic energy <inline-formula id="inf7">
<mml:math id="m9">
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</list-item>
</list>
</p>
<p>A group of triangular bandpass filter combinations constitute Mel filter banks, where, <inline-formula id="inf8">
<mml:math id="m10">
<mml:mrow>
<mml:mn>0</mml:mn>
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</inline-formula> is the total number of triangular filters in Mel filter banks. The center frequency of these filters is <inline-formula id="inf10">
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</inline-formula>. Considering the logarithmic conversion relationship between the Mel frequency and ordinary frequency, it can be seen that the center spectrum of each filter with an equal interval linear distribution in the Mel frequency is dense in the low-frequency band and sparse in the high-frequency band. The schematic diagram of the Mel frequency filter bank is shown in <xref ref-type="fig" rid="F2">Figure&#x20;2</xref>.</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Mel scale filter&#x20;bank.</p>
</caption>
<graphic xlink:href="fphy-10-839699-g002.tif"/>
</fig>
<p>The transfer function of each bandpass filter is as follows:<disp-formula id="e2_3">
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</mml:mrow>
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</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(2.3)</label>
</disp-formula>
</p>
<p>The formula for obtaining the logarithmic spectrum <inline-formula id="inf11">
<mml:math id="m14">
<mml:mrow>
<mml:mi>S</mml:mi>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mi>m</mml:mi>
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</inline-formula> is as follows:<disp-formula id="e2_4">
<mml:math id="m15">
<mml:mrow>
<mml:mi>S</mml:mi>
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<mml:mo>(</mml:mo>
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</mml:mrow>
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<mml:mrow>
<mml:mo>(</mml:mo>
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<mml:munderover>
<mml:mstyle displaystyle="true">
<mml:mo>&#x2211;</mml:mo>
</mml:mstyle>
<mml:mrow>
<mml:mi>k</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>0</mml:mn>
</mml:mrow>
<mml:mrow>
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<mml:mo>&#x2212;</mml:mo>
<mml:mn>1</mml:mn>
</mml:mrow>
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<mml:mtext>&#x7c;</mml:mtext>
<mml:mi>X</mml:mi>
<mml:mrow>
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<mml:mi>k</mml:mi>
<mml:mo>)</mml:mo>
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<label>(2.4)</label>
</disp-formula>
<list list-type="simple">
<list-item>
<p>3) By substituting the above logarithmic energy into the discrete cosine transform (DCT), the Mel cepstral parameters <inline-formula id="inf12">
<mml:math id="m16">
<mml:mrow>
<mml:mi>C</mml:mi>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mi>n</mml:mi>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula> of order L can be obtained, as shown in <xref ref-type="disp-formula" rid="e2_5">Eq. 2.5</xref>, where L is the order of MFCC coefficients, usually is 12&#x2013;16, and <italic>M</italic> is the number of Mel filters.</p>
</list-item>
</list>
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<mml:math id="m17">
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</mml:mrow>
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</mml:mrow>
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</mml:mrow>
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<label>(2.5)</label>
</disp-formula>
</p>
<p>
<xref ref-type="fig" rid="F3">Figure&#x20;3</xref> is a 12-order MFCC characteristic diagram of a giant panda voice, in which the <italic>X</italic>-axis represents the order of the MFCC coefficient, the <italic>Y</italic>-axis represents the number of frames of voice, and the <italic>Z</italic>-axis represents the corresponding cepstral parameter&#x20;value.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>12th order MFCC characteristic diagram.</p>
</caption>
<graphic xlink:href="fphy-10-839699-g003.tif"/>
</fig>
</sec>
<sec id="s2-2">
<title>2.2&#x20;First-Order Differential Mel Frequency Cepstral Coefficients of Giant Panda Sound</title>
<p>The standard MFCC parameters reflect the static characteristics within each frame of speech, while the difference of the MFCC reflects the dynamic characteristics. The Furui experiment shows that adding dynamic characteristics to the features can greatly improve the system performance [<xref ref-type="bibr" rid="B13">13</xref>]. The introduction of differential features has a wide range of applications and good results in the field of human voice recognition. Therefore, this method is also first used in the processing of giant panda&#x20;voice.</p>
<p>After obtaining the MFCC parameters, use <xref ref-type="disp-formula" rid="e2_5">Eq. 2.5</xref> to extract the MFCC first-order differential parameter <inline-formula id="inf13">
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<mml:mi mathvariant="normal">&#x394;</mml:mi>
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</mml:mrow>
</mml:math>
</inline-formula>.<disp-formula id="e2_6">
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</mml:mrow>
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<mml:mtr>
<mml:mtd>
<mml:msub>
<mml:mi>C</mml:mi>
<mml:mi>t</mml:mi>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:msub>
<mml:mi>C</mml:mi>
<mml:mrow>
<mml:mi>t</mml:mi>
<mml:mo>&#x2b;</mml:mo>
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</mml:mrow>
</mml:msub>
<mml:mo>&#xa0;</mml:mo>
<mml:mo>&#xa0;</mml:mo>
<mml:mi>t</mml:mi>
<mml:mo>&#x2265;</mml:mo>
<mml:mi>T</mml:mi>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>&#x398;</mml:mi>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
<mml:mo>&#xa0;</mml:mo>
</mml:mrow>
</mml:math>
<label>(2.6)</label>
</disp-formula>where <inline-formula id="inf14">
<mml:math id="m20">
<mml:mrow>
<mml:msub>
<mml:mi>D</mml:mi>
<mml:mi>t</mml:mi>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula> represents <italic>t</italic>-th &#x394;MFCC, <inline-formula id="inf15">
<mml:math id="m21">
<mml:mi>T</mml:mi>
</mml:math>
</inline-formula> is the order of the cepstral coefficient, <inline-formula id="inf16">
<mml:math id="m22">
<mml:mi>&#x398;</mml:mi>
</mml:math>
</inline-formula> is the time difference of the first derivative, and the values of 1 and 2 represent the first cepstral coefficient&#x20;[<xref ref-type="bibr" rid="B14">14</xref>].</p>
<p>
<xref ref-type="fig" rid="F4">Figure&#x20;4</xref> shows the characteristics of the MFCC of order 12 and &#x394;MFCC of order 12 of the same giant panda&#x20;voice.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>12th order MFCC and its &#x394;MFCC characteristic diagram. <bold>(A)</bold> MFCC characteristic diagram and <bold>(B)</bold> &#x394;MFCC characteristic.</p>
</caption>
<graphic xlink:href="fphy-10-839699-g004.tif"/>
</fig>
</sec>
</sec>
<sec id="s3">
<title>3 Compound Mel Frequency Cepstral Coefficient of Giant Panda Sound</title>
<sec id="s3-1">
<title>3.1 The Inverse Mel Frequency Cepstral Coefficient</title>
<p>The IMFCC feature can compensate the high-frequency information and improve the system recognition rate through its integration with the traditional MFCC. The structure of the IMFCC filter bank is shown in <xref ref-type="fig" rid="F5">Figure&#x20;5</xref>.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Inverted Mel filter&#x20;bank.</p>
</caption>
<graphic xlink:href="fphy-10-839699-g005.tif"/>
</fig>
<p>Corresponding to the Mel domain of the traditional filter structure, we call this domain as the inverted Mel domain, which is recorded as IMEL, and the corresponding frequency is recorded as <inline-formula id="inf17">
<mml:math id="m23">
<mml:mrow>
<mml:msub>
<mml:mi>F</mml:mi>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mi>m</mml:mi>
<mml:mi>e</mml:mi>
<mml:mi>l</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:math>
</inline-formula>. The relationship with the time domain is as follows:<disp-formula id="e3_1">
<mml:math id="m24">
<mml:mrow>
<mml:msub>
<mml:mi>F</mml:mi>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mi>m</mml:mi>
<mml:mi>e</mml:mi>
<mml:mi>l</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mi>f</mml:mi>
<mml:mo>)</mml:mo>
</mml:mrow>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>219.268</mml:mn>
<mml:mo>&#x2212;</mml:mo>
<mml:mn>2595</mml:mn>
<mml:mi>l</mml:mi>
<mml:mi>o</mml:mi>
<mml:mi>g</mml:mi>
<mml:mn>10</mml:mn>
<mml:mrow>
<mml:mo>(</mml:mo>
<mml:mrow>
<mml:mn>1</mml:mn>
<mml:mo>&#x2b;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:mn>4031.25</mml:mn>
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<mml:mi>f</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>700</mml:mn>
</mml:mrow>
</mml:mfrac>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(3.1)</label>
</disp-formula>
</p>
<p>The inverted filter response becomes<disp-formula id="e3_2">
<mml:math id="m25">
<mml:mrow>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>H</mml:mi>
<mml:mi>i</mml:mi>
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</mml:mrow>
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<mml:mn>1</mml:mn>
</mml:mrow>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:math>
<label>(3.2)</label>
</disp-formula>where <inline-formula id="inf18">
<mml:math id="m26">
<mml:mrow>
<mml:mi>E</mml:mi>
<mml:msub>
<mml:mi>H</mml:mi>
<mml:mi>i</mml:mi>
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<mml:mrow>
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<mml:mi>k</mml:mi>
<mml:mo>)</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:math>
</inline-formula> is the filter response in the MEL domain.</p>
<p>
<xref ref-type="fig" rid="F6">Figure&#x20;6</xref> shows the 12th order MFCC and the 12th order IMFCC characteristic diagram of a giant panda sound, in which the X axis represents the order of the MFCC , the Y axis represents the number of voice frames, and the Z axis represents the corresponding cepstral parameter values.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>12th order characteristic diagram of giant panda sound. <bold>(A)</bold> MFC and <bold>(B)</bold> IMFCC.</p>
</caption>
<graphic xlink:href="fphy-10-839699-g006.tif"/>
</fig>
</sec>
<sec id="s3-2">
<title>3.2 Composite Mel Composite Frequency Cepstral Coefficient</title>
<p>MFCC characteristic parameters are obtained through the Mel filter bank and a series of operations. Accordingly, the characteristic coefficients obtained after a series of operations through the Mel filter bank and composite filter bank of the inverted Mel filter bank are called composite Mel frequency cepstral coefficients, which are recorded as the CMFCC (compound Mel frequency cepstral coefficient).</p>
<p>Therefore, we fuse the 12th order MFCC characteristic diagram and 12th order IMFCC characteristic diagram in <xref ref-type="fig" rid="F7">Figure.7</xref> to obtain the corresponding 24th order CMFCC characteristic parameter diagram, as shown in <xref ref-type="fig" rid="F8">Figure&#x20;8</xref>.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>24th order CMFCC characteristic diagram.</p>
</caption>
<graphic xlink:href="fphy-10-839699-g007.tif"/>
</fig>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>Original sound signal of the giant panda and the CMFCC characteristic sequence. <bold>(A)</bold> Original sound signal of the giant panda, <bold>(B)</bold> the CMFCC characteristic sequence extracted from the&#x20;sound.</p>
</caption>
<graphic xlink:href="fphy-10-839699-g008.tif"/>
</fig>
</sec>
<sec id="s3-3">
<title>3.3 Hurst Exponent of the Composite Mel Composite Frequency Cepstral Coefficient Feature Sequence</title>
<p>Assuming that the sequence composed of CMFCC features satisfies the fractional Brownian motion distribution, we can calculate <bold>
<italic>H</italic>
</bold> according to the following method [<xref ref-type="bibr" rid="B13">13</xref>, <xref ref-type="bibr" rid="B15">15</xref>,&#x20;<xref ref-type="bibr" rid="B16">16</xref>].</p>
<p>Let n be the number of data of CMFCC-modified multifractional Gaussian noise (mmfGn) [<xref ref-type="bibr" rid="B8">8</xref>, <xref ref-type="bibr" rid="B9">9</xref>]. Let <inline-formula id="inf19">
<mml:math id="m27">
<mml:mrow>
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<mml:mi>N</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula> be the length of the neighborhood used for estimating the function parameter. We will estimate <inline-formula id="inf20">
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<mml:mrow>
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</inline-formula> only for <inline-formula id="inf21">
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</mml:mrow>
</mml:math>
</inline-formula>.</p>
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</mml:mrow>
</mml:math>
</inline-formula> to be an integer. Then, our estimator of <inline-formula id="inf23">
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</mml:math>
</inline-formula> is the following:<disp-formula id="e3_3">
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</mml:msqrt>
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<mml:mo>,</mml:mo>
</mml:mrow>
</mml:math>
<label>(3.3)</label>
</disp-formula>where<disp-formula id="e3_4">
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</mml:math>
<label>(3.4)</label>
</disp-formula>
</p>
<p>
<xref ref-type="fig" rid="F8">Figure&#x20;8</xref> shows the original sound signal of giant panda and the CMFCC characteristic sequence. <xref ref-type="fig" rid="F9">Figure&#x20;9</xref> shows the H-index distribution of two CMFCC characteristic sequences of the giant panda sound. In <xref ref-type="fig" rid="F9">Figure&#x20;9A</xref>, the giant panda sound duration time <inline-formula id="inf24">
<mml:math id="m34">
<mml:mrow>
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<mml:mo>&#x3d;</mml:mo>
<mml:mn>2</mml:mn>
<mml:mi>s</mml:mi>
</mml:mrow>
</mml:math>
</inline-formula>, sampling frequency <inline-formula id="inf25">
<mml:math id="m35">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mi>s</mml:mi>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mn>192</mml:mn>
<mml:mi>k</mml:mi>
<mml:mi>H</mml:mi>
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</mml:mrow>
</mml:math>
</inline-formula>, <inline-formula id="inf26">
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<mml:mrow>
<mml:mi>n</mml:mi>
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</mml:mrow>
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</inline-formula>, and <inline-formula id="inf27">
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<mml:mo>&#x3d;</mml:mo>
<mml:mn>512</mml:mn>
</mml:mrow>
</mml:math>
</inline-formula>. In <xref ref-type="fig" rid="F9">Figure&#x20;9B</xref>, the giant panda sound duration <inline-formula id="inf28">
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</mml:mrow>
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</inline-formula>, sampling frequency <inline-formula id="inf29">
<mml:math id="m39">
<mml:mrow>
<mml:msub>
<mml:mi>f</mml:mi>
<mml:mi>s</mml:mi>
</mml:msub>
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</inline-formula>, <inline-formula id="inf30">
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<mml:mrow>
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<mml:mo>&#x3d;</mml:mo>
<mml:mn>512</mml:mn>
</mml:mrow>
</mml:math>
</inline-formula>. The experimental results show that the CMFCC characteristic sequence of the giant panda voice has long-range dependent characteristics.</p>
<fig id="F9" position="float">
<label>FIGURE 9</label>
<caption>
<p>H-index distribution of two CMFCC characteristic sequences of giant panda sound, <bold>(A)</bold> <inline-formula id="inf32">
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</mml:mrow>
</mml:math>
</inline-formula>.</p>
</caption>
<graphic xlink:href="fphy-10-839699-g009.tif"/>
</fig>
</sec>
</sec>
<sec id="s4">
<title>4 Discussion</title>
<p>We applied the CMFCC feature sequence with LRD to giant panda individual recognition. Considering that this feature is the feature information obtained within the speech frame, the &#x25b3;MFCC of the MFCC feature parameter is introduced. The two features of CMFCC and &#x394;MFCC are fused to obtain a new feature parameter.</p>
<p>There are 20 individual giant pandas. Each individual has 10s sounds, including 4s for training and 6s for testing. The ratio between the number of correctly recognized test sounds and the total number of test sounds is the correct recognition rate. The final result is the average of the recognition rates of the three experiments, as shown in <xref ref-type="fig" rid="F10">Figure&#x20;10</xref> and <xref ref-type="table" rid="T1">Table&#x20;1</xref>.</p>
<fig id="F10" position="float">
<label>FIGURE 10</label>
<caption>
<p>Line chart of the individual recognition rate of the giant&#x20;panda.</p>
</caption>
<graphic xlink:href="fphy-10-839699-g010.tif"/>
</fig>
<table-wrap id="T1" position="float">
<label>TABLE 1</label>
<caption>
<p>Recognition rate of giant panda individual recognition.</p>
</caption>
<table>
<thead valign="top">
<tr>
<th align="left">Order\Type</th>
<th align="center">8</th>
<th align="center">12</th>
<th align="center">16</th>
<th align="center">20</th>
</tr>
</thead>
<tbody valign="top">
<tr>
<td align="left">MFCC</td>
<td align="char" char="(">56.67(68)</td>
<td align="char" char="(">71.67(86)</td>
<td align="char" char="(">79.17(95)</td>
<td align="char" char="(">80.83(97)</td>
</tr>
<tr>
<td align="left">CMFCC</td>
<td align="char" char="(">65(78)</td>
<td align="char" char="(">77.5(93)</td>
<td align="char" char="(">83.33(100)</td>
<td align="char" char="(">85.83(103)</td>
</tr>
<tr>
<td align="left">CMFCC&#x2b;&#x394;MFCC</td>
<td align="char" char="(">67.5(81)</td>
<td align="char" char="(">80.83(97)</td>
<td align="char" char="(">86.67(104)</td>
<td align="char" char="(">88.33(106)</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The order of CMFCC and MFCC features are 8, 12, 16, and 20, respectively, and the order of &#x25b3;MFCC also corresponds to 8, 12, 16, and 20. From <xref ref-type="table" rid="T1">Table&#x20;1</xref>, we can see that the higher the order of features, the higher is the recognition rate, indicating that the correlation of feature sequences is also stronger.</p>
<p>The final individual identification of giant panda is shown in <xref ref-type="table" rid="T1">Table&#x20;1</xref>. <xref ref-type="fig" rid="F10">Figure&#x20;10</xref> is a broken line diagram of three feature recognition results.</p>
<p>It can be seen from <xref ref-type="fig" rid="F10">Figure&#x20;10</xref> and <xref ref-type="table" rid="T1">Table&#x20;1</xref> that the characteristic parameters obtained by flipping the Mel filter bank can improve the resolution of the high-frequency part. Therefore, after using CMFCC features, the recognition rate of giant panda individuals is higher than that under the MFCC. At the same time, this is because the &#x394;MFCC feature considers the difference between frames and improves the feature performance of the CMFCC. Therefore, the recognition rate of the CMFCC and &#x394;MFCC combination feature is better, and the theoretical results are consistent with the experimental expectations.</p>
</sec>
<sec id="s5">
<title>5 Conclusion</title>
<p>This study mainly presents the characteristics of the Mel composite cepstral coefficient of giant panda sound (CMFCC) for individual recognition. It is verified that the CMFCC feature sequence conforms to the distribution characteristics of fractional Brownian motion, which has long-range dependence. This feature sequence makes use of the memory characteristics of the giant panda voice in time and can obtain the characteristics of the giant panda sound in low- and high-frequency resolution at the same time. Through experimental verification, it has the best effect on individual recognition of the giant panda and improves the efficiency of the giant panda. The recognition rate has reached the expected effect of individual recognition of the giant&#x20;panda.</p>
</sec>
</body>
<back>
<sec 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>This research is supported by the Chengdu Research Base of Giant Panda Breeding (Nos. 2020CPB-C09 and CPB2018-01).</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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