<?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">OJS</journal-id><journal-title-group><journal-title>Open Journal of Statistics</journal-title></journal-title-group><issn pub-type="epub">2161-718X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojs.2015.57071</article-id><article-id pub-id-type="publisher-id">OJS-62028</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  On Inversion of Continuous Wavelet Transform
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>intao</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xiaoqing</surname><given-names>Su</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Guocheng</surname><given-names>Wang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>State Key Laboratory of Geodesy and Earth’s Dynamics, Institute of Geodesy and Geophysics,
Chinese Academy of Sciences, Wuhan, China</addr-line></aff><aff id="aff2"><addr-line>Shandong University of Technology, Zibo, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>llt@whigg.ac.cn(IL)</email>;<email>sxq_azj@163.com(XS)</email>;<email>guocheng96@whigg.ac.cn(GW)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>11</day><month>12</month><year>2015</year></pub-date><volume>05</volume><issue>07</issue><fpage>714</fpage><lpage>720</lpage><history><date date-type="received"><day>14</day>	<month>September</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>15</month>	<year>December</year>	</date><date date-type="accepted"><day>18</day>	<month>December</month>	<year>2015</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>
 
 
   This study deduces a general inversion of continuous wavelet transform (CWT) with timescale being real rather than positive. In conventional CWT inversion, wavelet’s dual is assumed to be a reconstruction wavelet or a localized function. This study finds that wavelet’s dual can be a harmonic which is not local. This finding leads to new CWT inversion formulas. It also justifies the concept of normal wavelet transform which is useful in time-frequency analysis and time-frequency filtering. This study also proves a law for CWT inversion: either wavelet or its dual must integrate to zero. 
 
</p></abstract><kwd-group><kwd>Continuous Wavelet Transform</kwd><kwd> Wavelet’s Dual</kwd><kwd> Inversion</kwd><kwd> Normal Wavelet Transform</kwd><kwd> Time-Frequency Filtering</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Continuous wavelet transform (CWT) [<xref ref-type="bibr" rid="scirp.62028-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.62028-ref6">6</xref>] has been well known and widely applied for many years. In convention, CWT is defined with the timescale being positive. However, in practice, both positive and negative timescales are important for the CWT. For example, in earth’s polar motion [<xref ref-type="bibr" rid="scirp.62028-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.62028-ref8">8</xref>] , there are both prograde and retrograde annual wobbles. If one wants to use the CWT to analyze the annual wobbles, he should use a CWT defined with the timescale being real rather than positive.</p><p>CWT inversion has found few applications. The reason lies in that wavelet’s dual is assumed to be a reconstruction wavelet in conventional CWT inversion [<xref ref-type="bibr" rid="scirp.62028-ref6">6</xref>] . In fact, it is difficult for a CWT inversion using a reconstruction wavelet to obtain the admissibility constant. What will happen if wavelet’s dual is not a reconstruction wavelet or a localized function? This study tries to answer this question.</p><p>There has been a general inversion for linear time-frequency transform [<xref ref-type="bibr" rid="scirp.62028-ref9">9</xref>] . This inversion implies the inversion of CWT and the definition of wavelet’s dual. It is expressed as following theorem.</p><p>Deconvolution Theorem. For a time signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x6.png" xlink:type="simple"/></inline-formula>, its time-frequency transform</p><disp-formula id="scirp.62028-formula859"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x7.png"  xlink:type="simple"/></disp-formula><p>can be inverted by</p><disp-formula id="scirp.62028-formula860"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x8.png"  xlink:type="simple"/></disp-formula><p>if</p><disp-formula id="scirp.62028-formula861"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x9.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x10.png" xlink:type="simple"/></inline-formula> denotes time and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x11.png" xlink:type="simple"/></inline-formula> denotes frequency, overline “-” means conjugate operator, hat “^” means Fourier transform operator, for instances, the Fourier transform of kernel <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x12.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.62028-formula862"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x13.png"  xlink:type="simple"/></disp-formula><p>and Fourier transform of kernel’s dual <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x14.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.62028-formula863"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x15.png"  xlink:type="simple"/></disp-formula><p>and constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x16.png" xlink:type="simple"/></inline-formula> is called admissibility constant.</p><p>The name of this theorem comes from the fact that it gives the general way to inverting frequency-indexed convolutions. It is noted that the linear time-frequency transform (1) is a set of frequency-indexed convolutions. According to the deconvolution theorem, we will give a general inversion of CWT with timescale being real. This inversion gives an explicit definition of wavelet’s dual. The inversion implies a law: either wavelet or wavelet’s dual must integrate to zero. Also according to the inversion, we find that wavelet’s dual can be a harmonic besides a wavelet. Thus new CWT inversion formulas are obtained. The new formulas suggest the concept of normal wavelet transform, which is useful in time-frequency analysis and time-frequency filtering.</p></sec><sec id="s2"><title>2. Inversion of CWT and Dual of Wavelet</title><p>For a time signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x17.png" xlink:type="simple"/></inline-formula>, its CWT is defined as</p><disp-formula id="scirp.62028-formula864"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x18.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x19.png" xlink:type="simple"/></inline-formula> is a wavelet, a denotes timescale, b denotes time and “||” means absolute operator. It is important to note that the timescale a can be negative. For example, the timescale of a retrograde (i.e. clock-wise) harmonic movement on a complex plane is negative. Also note that the CWT is written in L<sup>1</sup>-norm rather than L<sup>2</sup>-norm. It has been proved that only L<sup>1</sup>-norm CWT spectrum is unbiased in detecting frequency [<xref ref-type="bibr" rid="scirp.62028-ref9">9</xref>] .</p><p>CWT (6) is composed of timescale-indexed convolutions. It can be regarded as a special time-frequency transform. Then, there is a CWT inversion corollary.</p><p>Inversion Corollary. For a time signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x20.png" xlink:type="simple"/></inline-formula>, its CWT (6) can be inverted by</p><disp-formula id="scirp.62028-formula865"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x21.png"  xlink:type="simple"/></disp-formula><p>if</p><disp-formula id="scirp.62028-formula866"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x22.png"  xlink:type="simple"/></disp-formula><p>satisfies</p><disp-formula id="scirp.62028-formula867"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x23.png"  xlink:type="simple"/></disp-formula><p>Proof. CWT (6) is a special time-frequency transform (1) with</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x24.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x25.png" xlink:type="simple"/></inline-formula> (10)</p><p>and</p><disp-formula id="scirp.62028-formula868"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x26.png"  xlink:type="simple"/></disp-formula><p>Letting</p><disp-formula id="scirp.62028-formula869"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x27.png"  xlink:type="simple"/></disp-formula><p>Then</p><disp-formula id="scirp.62028-formula870"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x28.png"  xlink:type="simple"/></disp-formula><p>According to the deconvolution theorem, this inversion corollary is proved.</p><p>This inversion corollary gives a general way to inverting CWT. Relation (8) and (9) establish an explicit definition for wavelet’s dual. This means that a function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x29.png" xlink:type="simple"/></inline-formula> simply satisfying relation (8) and (9) is called a dual of wavelet<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x30.png" xlink:type="simple"/></inline-formula>. Consider that the integration in (8), if existing, is naturally a constant. Such definition is very explicit, because relations (8) and (9) explicate how to obtain a dual of wavelet. Furthermore, in inversion (7), the timescale a spans over entire real field rather than half real field.</p></sec><sec id="s3"><title>3. A CWT Inversion Law</title><p>Observing the relation (8), one can find that it is necessary for the wavelet and its dual of CWT (6) to satisfy</p><disp-formula id="scirp.62028-formula871"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x31.png"  xlink:type="simple"/></disp-formula><p>To make (14) true, there must be that either</p><disp-formula id="scirp.62028-formula872"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x32.png"  xlink:type="simple"/></disp-formula><p>or</p><disp-formula id="scirp.62028-formula873"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x33.png"  xlink:type="simple"/></disp-formula><p>Thus, there is a CWT inversion law.</p><p>Inversion Law. In CWT inversion, either wavelet or its dual must integrate to zero.</p><p>This law applies to any CWT inversion and can never be violated. Such law breaks the traditional zero-integration requirement on wavelet. The zero-integration requirement on wavelet is made in the case that the dual of the wavelet is exactly the wavelet itself. Such case is very special. As shown by the inversion corollary, a CWT with its wavelet being unevenly undulant is still possible to be inverted.</p></sec><sec id="s4"><title>4. CWT Inversion with Wavelet’s Dual Being a Harmonic</title><p>Making a CWT inversion is equivalent to finding a dual of wavelet. In tradition, wavelet’s dual is assumed to be a reconstruction wavelet or a localized function [<xref ref-type="bibr" rid="scirp.62028-ref6">6</xref>] . It is interesting to find that wavelet’s dual can be a harmonic which is not local. Letting</p><disp-formula id="scirp.62028-formula874"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x34.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x35.png" xlink:type="simple"/></inline-formula> is a nonzero real, the admissibility constant becomes</p><disp-formula id="scirp.62028-formula875"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x36.png"  xlink:type="simple"/></disp-formula><p>This means, for a time signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x37.png" xlink:type="simple"/></inline-formula>, its CWT (6) can be inverted by</p><disp-formula id="scirp.62028-formula876"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x38.png"  xlink:type="simple"/></disp-formula><p>Particularly, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x39.png" xlink:type="simple"/></inline-formula>, inversion (19) is simply</p><disp-formula id="scirp.62028-formula877"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x40.png"  xlink:type="simple"/></disp-formula><p>Inversion (20) has been found by Liu and Hsu 2012. It plays a main role in the concept of normal wavelet transform [<xref ref-type="bibr" rid="scirp.62028-ref9">9</xref>] . Here, for the first time, inversion (19) is found. It means that a CWT can be inverted by dilating and translating a harmonic! The important reason lies in inversion (19) is that a harmonic is evenly undulant no matter the wavelet is evenly undulant or not. Inversion (19) shows that the dual of a wavelet is not unique. For a wavelet, the number of its duals is innumerous. For a CWT, its inversion can be of innumerous forms.</p><p>In inversion (19), there is requirement for the wavelet is that</p><disp-formula id="scirp.62028-formula878"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x41.png"  xlink:type="simple"/></disp-formula><p>This requirement can be easily to meet by letting</p><disp-formula id="scirp.62028-formula879"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x42.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x43.png" xlink:type="simple"/></inline-formula> is a window. Also note that wavelet (22) is usually inadmissible.</p></sec><sec id="s5"><title>5. Normal Wavelet Transform</title><p>For time signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x44.png" xlink:type="simple"/></inline-formula>, its CWT (6) is called a normal wavelet transform if the wavelet is defined as</p><disp-formula id="scirp.62028-formula880"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x45.png"  xlink:type="simple"/></disp-formula><p>where window <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x46.png" xlink:type="simple"/></inline-formula> satisfies</p><p>1) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x47.png" xlink:type="simple"/></inline-formula> (24)</p><p>and</p><p>2) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x48.png" xlink:type="simple"/></inline-formula> (25)</p><p>where “ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x50.png" xlink:type="simple"/></inline-formula> “ means “if and only if”. As a special CWT, the normal wavelet transform is useful in time-fre- quency analysis and time-frequency-filtering.</p><sec id="s5_1"><title>5.1. Time-Frequency Analysis</title><p>If applying a normal wavelet transform to a harmonic</p><disp-formula id="scirp.62028-formula881"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x51.png"  xlink:type="simple"/></disp-formula><p>It is easy to observe that</p><p>1) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x52.png" xlink:type="simple"/></inline-formula> (27)</p><p>2) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x53.png" xlink:type="simple"/></inline-formula> (28)</p><p>Relations (27) and (28) assure that the normal wavelet transform is accurate and useful in time-frequency analysis. At first, Relation (27) means that the normal wavelet transform can exactly (i.e. without bias) detect the immediate (i.e. local) frequency of a harmonic. Secondly, relation (28) means that the normal wavelet transform can exactly detect the immediate amplitude and phase of a harmonic. It is important to note that, relation (27) does not hold if the CWT (6) is not defined in L<sup>1</sup>-norm. Different from the S-transform [<xref ref-type="bibr" rid="scirp.62028-ref10">10</xref>] as well as General S-transform [<xref ref-type="bibr" rid="scirp.62028-ref11">11</xref>] , the normal wavelet transform can detect the immediate rather than initial phase of a harmonic. Similar to S-transform as well as General S-transform, the normal wavelet transform can do time frequency filtering.</p></sec><sec id="s5_2"><title>5.2. Time-Frequency Filtering</title><p>According to (20), the normal wavelet transform can be inverted simply by</p><disp-formula id="scirp.62028-formula882"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x54.png"  xlink:type="simple"/></disp-formula><p>because</p><disp-formula id="scirp.62028-formula883"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x55.png"  xlink:type="simple"/></disp-formula><p>This inversion suggests that</p><disp-formula id="scirp.62028-formula884"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x56.png"  xlink:type="simple"/></disp-formula><p>where S is some time-frequency area and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x57.png" xlink:type="simple"/></inline-formula> denotes the filtered signal. (31) is the basic formula for time-frequency filtering by using the normal wavelet transform.</p><p>We here provide a numeric example of time-frequency analysis and time-frequency filtering by using the normal wavelet transform. A test time signal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x58.png" xlink:type="simple"/></inline-formula> is constructed (<xref ref-type="fig" rid="fig1">Figure 1</xref>). It is composed of three intermittent harmonic sub-signals and some noises. We apply a normal wavelet transform to this signal by letting</p><disp-formula id="scirp.62028-formula885"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-1240569x59.png"  xlink:type="simple"/></disp-formula><p>The normal wavelet transform spectrum is obtained (<xref ref-type="fig" rid="fig2">Figure 2</xref>). One can observe that there are clearly three significant sub-signal in the original signal. According to the spectrum significance, three time-frequency areas can be determined. Then, according to (31), one can recover the three sub-signals in time domain (<xref ref-type="fig" rid="fig3">Figure 3</xref>). The recovered sub-signals are well fitted to its original counterparts, which shows the good time-frequency filtering function of the normal wavelet transform.</p></sec></sec><sec id="s6"><title>6. Conclusion</title><p>According to deconvolution theorem, this study explicates the way to inverting continuous wavelet transform (CWT) and the definition of wavelet’s dual. We prove that, in CWT inversion, either wavelet or its dual must integrate to zero. This study shows that wavelet’s dual can be a harmonic, which leads to new CWT inversion for-</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Test time signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x61.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-1240569x60.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Normal wavelet spectrum of the test time signal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x63.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-1240569x64.png" xlink:type="simple"/></inline-formula> (the white closed lines denote three significant time-frequency areas)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-1240569x62.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Three sub-signals (blue) and their corresponding recovered sub-signals (red) (a, b, and c)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-1240569x65.png"/></fig><p>mulas. One of the formulas justifies the concept of normal wavelet transform, which is useful in time-frequency analysis and time-frequency filtering.</p></sec><sec id="s7"><title>Acknowledgements</title><p>We thank the Editor and the referee for their comments. This study is supported by NSFC 41074050 and by 2011YQ120045 of Ministry of Science and Technology of the People’s Republic of China.</p></sec><sec id="s8"><title>Cite this paper</title><p>LintaoLiu,XiaoqingSu,GuochengWang, (2015) On Inversion of Continuous Wavelet Transform. Open Journal of Statistics,05,714-720. doi: 10.4236/ojs.2015.57071</p></sec></body><back><ref-list><title>References</title><ref id="scirp.62028-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">http://scienceworld.wolfram.com/biography/Zweig.html</mixed-citation></ref><ref id="scirp.62028-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Goupillaud, P., Grossman, A. and Morlet, J. 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