<?xml version="1.0" encoding="ISO-8859-1"?><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">
<front>
<journal-meta>
<journal-id>0016-7169</journal-id>
<journal-title><![CDATA[Geofísica internacional]]></journal-title>
<abbrev-journal-title><![CDATA[Geofís. Intl]]></abbrev-journal-title>
<issn>0016-7169</issn>
<publisher>
<publisher-name><![CDATA[Universidad Nacional Autónoma de México, Instituto de Geofísica]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S0016-71692014000100006</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Reducing wind noise in seismic data using Non-negative Matrix Factorization: an application to Villarrica volcano, Chile]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Cabras]]></surname>
<given-names><![CDATA[Giuseppe]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Carniel]]></surname>
<given-names><![CDATA[Roberto]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
<xref ref-type="aff" rid="A03"/>
<xref ref-type="aff" rid="A04"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Jones]]></surname>
<given-names><![CDATA[Joshua P.]]></given-names>
</name>
<xref ref-type="aff" rid="A05"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Takeo]]></surname>
<given-names><![CDATA[Minoru]]></given-names>
</name>
<xref ref-type="aff" rid="A06"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universitá degli Studi di Udine Via delle Scienze Dipartimento di Chimica, Fisica e Ambiente ]]></institution>
<addr-line><![CDATA[Udine ]]></addr-line>
<country>Italy</country>
</aff>
<aff id="A02">
<institution><![CDATA[,Universitá degli Studi di Udine Via delle Scienze Dipartimento di Ingegneria Civile e Architettura Laboratorio di misure e trattamento dei segnali]]></institution>
<addr-line><![CDATA[Udine ]]></addr-line>
<country>Italy</country>
</aff>
<aff id="A03">
<institution><![CDATA[,University of Tokyo Earthquake Research Institute ]]></institution>
<addr-line><![CDATA[Tokyo ]]></addr-line>
<country>Japan</country>
</aff>
<aff id="A04">
<institution><![CDATA[,University of Information Technologies Mechanics and Optics Kronverksky Prospect Int. Syst. Lab. National Research Geognosis Proj.]]></institution>
<addr-line><![CDATA[St. Petersburg ]]></addr-line>
<country>Russia</country>
</aff>
<aff id="A05">
<institution><![CDATA[,CCIS University of Alberta Department of Physics Geognosis Proj]]></institution>
<addr-line><![CDATA[Edmonton ]]></addr-line>
<country>Canada</country>
</aff>
<aff id="A06">
<institution><![CDATA[,University of Tokyo Earthquake Research Institute ]]></institution>
<addr-line><![CDATA[Tokyo ]]></addr-line>
<country>Japan</country>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>03</month>
<year>2014</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>03</month>
<year>2014</year>
</pub-date>
<volume>53</volume>
<numero>1</numero>
<fpage>77</fpage>
<lpage>85</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_arttext&amp;pid=S0016-71692014000100006&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_abstract&amp;pid=S0016-71692014000100006&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.mx/scielo.php?script=sci_pdf&amp;pid=S0016-71692014000100006&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="es"><p><![CDATA[La separación de distintas fuentes existentes en una sola señal sísmica es un problema interesante y al mismo tiempo difícil. En este trabajo presentamos un método semi-ciego para la separación de un solo canal sísmico para mejorar la parte de señal de origen volcánico. En este método, el esquema de descomposición de las fuentes se basa en una factorización en matrices dispersas y non-negativas (Non-negative Matrix Factorization, NMF) de la representación tiempo-frecuencia del único canal sísmico vertical. Como caso de estudio se presenta una aplicación a partir de datos sísmicos registrados en el volcán Villarrica, Chile, uno de los más activos de los Andes meridionales. Los datos analizados están fuertemente contaminados por el ruido del viento y el procedimiento propuesto se utiliza para separar un componente de origen volcánico de otro de origen meteorológico.]]></p></abstract>
<abstract abstract-type="short" xml:lang="en"><p><![CDATA[Single channel source separation of seismic signals is an appealing but difficult problem. In this paper, we introduce a semi-blind single-channel seismic source separation method to enhance the components of volcanic origin. In this method, the source decomposition scheme is addressed as a Sparse Non-negative Matrix Factorization (NMF) of the time-frequency representation of the single vertical seismic channel. As a case study we present an application using seismic data recorded at Villarrica volcano, Chile, one of the most active in the southern Andes. The analysed dataset is strongly contaminated by wind noise and the procedure is used to separate a component of volcanic origin from another of meteorological origin.]]></p></abstract>
<kwd-group>
<kwd lng="es"><![CDATA[Tremor volcánico]]></kwd>
<kwd lng="es"><![CDATA[NMF]]></kwd>
<kwd lng="es"><![CDATA[Villarrica]]></kwd>
<kwd lng="es"><![CDATA[reducción del ruido del viento]]></kwd>
<kwd lng="en"><![CDATA[volcanic tremor]]></kwd>
<kwd lng="en"><![CDATA[NMF]]></kwd>
<kwd lng="en"><![CDATA[Villarrica]]></kwd>
<kwd lng="en"><![CDATA[wind noise reduction]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[  	    <p align="justify"><font face="verdana" size="4">Original paper</font></p>     <p align="justify">&nbsp;</p>     <p align="center"><font face="verdana" size="4"><b>Reducing wind noise in seismic data using Non&#45;negative Matrix Factorization: an application to Villarrica volcano, Chile</b></font></p>     <p align="center">&nbsp;</p>  	    <p align="center"><font face="verdana" size="2"><b>Giuseppe Cabras<sup>1</sup>*, Roberto Carniel<sup>2,3,4</sup>, Joshua P. Jones<sup>5</sup> and Minoru Takeo<sup>3</sup></b></font></p>     <p align="center">&nbsp;</p>      <p align="justify"><font face="verdana" size="2"><sup><i>1</i></sup><i> Dipartimento di Chimica, Fisica e Ambiente Universit&aacute; degli Studi di Udine Via delle Scienze, 206, Udine, Italy.</i> *Corresponding authors: <a href="mailto:giuseppe.cabras@uniud.it">giuseppe.cabras@uniud.it</a></font></p>     <p align="justify"><font face="verdana" size="2"><sup><i>2</i></sup><i> Laboratorio di misure e trattamento dei segnali Dipartimento di Ingegneria Civile e Architettura Universit&aacute; degli Studi di Udine Via delle Scienze, 206 Udine, Italy</i>.</font></p>     <p align="justify"><font face="verdana" size="2"><sup><i>3</i></sup><i> Earthquake Research Institute University of Tokyo Tokyo, Japan.</i> E&#45;mail: <a href="mailto:roberto.carniel@uniud.it">roberto.carniel@uniud.it</a></font></p>     ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2"><sup><i>4</i></sup><i> Geognosis Proj., Int. Syst. Lab. National Research University of Information Technologies Mechanics and Optics Kronverksky Prospect, 49 St. Petersburg 197101, Russia.</i></font></p>     <p align="justify"><font face="verdana" size="2"><sup><i>5</i></sup><i> Department. of Physics &#45; CCIS University of Alberta, Edmonton AB T6G 2E1 Canada.</i> E&#45;mail: <a href="mailto:jpjones@ualberta.ca">jpjones@ualberta.ca</a></font></p>     <p align="justify"><font face="verdana" size="2"><sup><i>6</i></sup><i> Earthquake Research Institute University of Tokyo Tokyo, Japan.</i> E&#45;mail: <a href="mailto:takeo@eri.u&#45;tokyo.ac.jp">takeo@eri.u&#45;tokyo.ac.jp</a></font></p>     <p align="justify">&nbsp;</p>     <p align="justify"><font face="verdana" size="2">Received: January 17, 2013.     <br>   Accepted: April 05, 2013.     <br>   Published on line: December 11, 2013.</font></p>     <p align="justify">&nbsp;</p>     <p align="justify"><font face="verdana" size="2"><b>Resumen</b></font></p>  	    <p align="justify"><font face="verdana" size="2">La separaci&oacute;n de distintas fuentes existentes en una sola se&ntilde;al s&iacute;smica es un problema interesante y al mismo tiempo dif&iacute;cil. En este trabajo presentamos un m&eacute;todo semi&#45;ciego para la separaci&oacute;n de un solo canal s&iacute;smico para mejorar la parte de se&ntilde;al de origen volc&aacute;nico. En este m&eacute;todo, el esquema de descomposici&oacute;n de las fuentes se basa en una factorizaci&oacute;n en matrices dispersas y non&#45;negativas (Non&#45;negative Matrix Factorization, NMF) de la representaci&oacute;n tiempo&#45;frecuencia del &uacute;nico canal s&iacute;smico vertical. Como caso de estudio se presenta una aplicaci&oacute;n a partir de datos s&iacute;smicos registrados en el volc&aacute;n Villarrica, Chile, uno de los m&aacute;s activos de los Andes meridionales. Los datos analizados est&aacute;n fuertemente contaminados por el ruido del viento y el procedimiento propuesto se utiliza para separar un componente de origen volc&aacute;nico de otro de origen meteorol&oacute;gico.</font></p>  	    ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2"><b>Palabras clave:</b> Tremor volc&aacute;nico, NMF, Villarrica, reducci&oacute;n del ruido del viento.</font></p>     <p align="justify">&nbsp;</p>      <p align="justify"><font face="verdana" size="2"><b>Abstract</b></font></p>  	    <p align="justify"><font face="verdana" size="2">Single channel source separation of seismic signals is an appealing but difficult problem. In this paper, we introduce a semi&#45;blind single&#45;channel seismic source separation method to enhance the components of volcanic origin. In this method, the source decomposition scheme is addressed as a Sparse Non&#45;negative Matrix Factorization (NMF) of the time&#45;frequency representation of the single vertical seismic channel. As a case study we present an application using seismic data recorded at Villarrica volcano, Chile, one of the most active in the southern Andes. The analysed dataset is strongly contaminated by wind noise and the procedure is used to separate a component of volcanic origin from another of meteorological origin.</font></p>  	    <p align="justify"><font face="verdana" size="2"><b>Key words:</b> volcanic tremor, NMF, Villarrica, wind noise reduction.</font></p>  	    <p align="justify">&nbsp;</p>     <p align="justify"><font face="verdana" size="2"><b>Introduction</b></font></p>  	    <p align="justify"><font face="verdana" size="2">Villarrica volcano (Chile), located in the southern Andes (39.42&deg; S, 71.93&deg; W) has more than 60 important historical eruptions (Casertano, 1963). As other volcanoes of basic composition (Behncke <i>et al.,</i> 2003; Behncke, 2009), Villarrica can not only produce effusive and moderate explosivity activity, but also pyroclastic flows that represent the most dangerous scenario (Moreno, 1998). It is currently characterized by the presence of a small (30&#45;40 m wide) summit lava lake which produces a persistent volcanic tremor and discrete events associated to strombolian activity (Ortiz <i>et al,</i> 2003; T&aacute;rraga <i>et al,</i> 2008). In November 2004 we installed an L22 three&#45;component geophone (f<sub>0</sub> = 2.0 Hz) approximately 800 m from the summit crater. The seismometer recorded continuously for a period of 10 days, between November 8, 2004 and November 17, 2004.</font></p>  	    <p align="justify"><font face="verdana" size="2">Noise often affects records of volcanic tremor or ambient ground&#45;motion recordings used e.g. for HVSR estimates of seismic site amplification. Benson <i>et al.</i> (2007) introduce several methods to reduce the effects of local, non&#45;stationary noise sources, earthquakes and instrumental irregularities on ambient noise. Lambert <i>et al.</i> (2011) propose four methodologies focused on the removal of the effects of anthropogenic noise. In this work, we apply an innovative wind noise reduction procedure to the tremor recorded at Villarrica, based on Non&#45;negative Matrix Factorization with Sparse Coding (Hoyer, 2002) and on the construction of a wind noise dictionary which is estimated from the available seismic recording itself. The presented procedure can be extended to the filtering of wind noise in other volcanic geophysical time series, such as the ones recorded by infrasonic sensors (Ichihara <i>et al.,</i> 2012).</font></p> 	    <p align="justify">&nbsp;</p>      ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2"><b>A two training step strategy to Single&#45;Sensor Seismic Analysis</b></font></p>  	    <p align="justify"><font face="verdana" size="2">In this paper, we extend the Non&#45;negative Matrix Factorization (NMF) and Sparse Coding (SC) procedure introduced in (Cabras <i>et al.,</i> 2012), where the basic idea is that we can obtain a meaningful part&#45;based factor decomposition (Lee &amp; Seung, 1999) from a single&#45;channel time series imposing only the constraints of non&#45;negativity and sparseness of the data. For a general discussion on NMF and SC, see Cichocki <i>et al.</i> (2009). As we will describe in detail below, the main contribution with respect to the original procedure (Cabras <i>et al.,</i> 2012) lies in the training stage, where we learn two sets of basis components in two steps directly from the available dataset: in the first training step we learn an approximate volcanic&#45;set basis components (or preliminary volcanic&#45;set dictionary), <img src="/img/revistas/geoint/v53n1/a6i1.jpg">, selecting a non windy data&#45;set for training; in the second training step we learn the wind&#45;set basis components (or noise&#45;set dictionary), <i>D<sub>n</sub>,</i> selecting a windy data&#45;set for training. The separation stage remains the same of (Cabras <i>et al.,</i> 2012), providing a fixed wind&#45;set basis components, <i>D<sub>n</sub></i> to the constrained sparse NMF learning loop.</font></p>      <p align="justify"><font face="verdana" size="2">We can state an NMF problem as follows: given a non&#45;negative data matrix <b>X</b>&#8712;<img src="/img/revistas/geoint/v53n1/a6i2.jpg">(with <i>x<sub>&#402;t</sub></i> &#8805; 0 or equivalently <i>X &#8805; 0)</i> and a reduced rank <i>K (K</i> &#8804; <i>min(F,T)),</i> find two non&#45;negative matrices <b>D</b>&#8712;<img src="/img/revistas/geoint/v53n1/a6i3.jpg">, called dictionary or basis components and <b>H</b>&#8712;<img src="/img/revistas/geoint/v53n1/a6i4.jpg">, called sparse code or weights, which factorize <i>X</i> as well as possible, that is:</font></p>      <p align="center"><img src="/img/revistas/geoint/v53n1/a6e1.jpg"></p>      <p align="justify"><font face="verdana" size="2">where <b>E</b>&#8712;<img src="/img/revistas/geoint/v53n1/a6i2.jpg">represents the approximation error to minimize. The meaning of dictionary matrix <i>D,</i> sparse code matrix <i>H</i> and rank <i>K</i> depends on the specific application and signal representation. To estimate the parameters of NMF, (i.e. the factor matrices <i>D</i> and <i>H),</i> we need to minimize the measure of similarity (or cost function C) between the data matrix <i>X</i> and the estimated model matrix <i><img src="/img/revistas/geoint/v53n1/a6i5.jpg">;</i> the simplest and widely used measure is the squared Euclidean distance (or Frobenius norm):</font></p>      <p align="center"><img src="/img/revistas/geoint/v53n1/a6e2.jpg"></p>      <p align="justify"><font face="verdana" size="2">where &#955; ia a non&#45;negative regularization parameter that controls the tradeoff between sparseness and reconstruction error and &#124;&#124; <i>H &#124;&#124;<sub>1</sub></i> is an <img src="/img/revistas/geoint/v53n1/a6i6.jpg"> norm regularization function proposed in Hoyer (2002).</font></p>      <p align="justify"><font face="verdana" size="2">Cabras <i>et al.</i> (2012) adopted the single channel enhancement model originally developed for processing audio records (Cabras <i>et al.,</i> 2010) to separate a "high convective", relatively transient, seismic source of interest from a "low convective", relatively continuous, "noise" in a single&#45;sensor seismic time series recorded at Erta 'Ale volcano (Harris <i>et al,</i> 2005). Erta 'Ale is characterized by the presence of a permanent lava lake that produces, in a similar way to Villarrica, at least part of a continuous volcanic tremor (Jones <i>et al.,</i> 2006), which is really characterized by a superposition of different independent sources (Jones <i>et al.,</i> 2012). In the Erta 'Ale case study, we learned the basis components of the noise <i>n(t),</i> denoted by D<sub>n</sub>, in a single step training stage, because in our data&#45;set we have segments of pure "low convective noise" for training.</font></p>  	    <p align="justify"><font face="verdana" size="2">In the present case study of Villarrica volcano, this strategy is not directly applicable. In fact, our data&#45;set is characterized by a relatively continuous "volcanic tremor", our source of interest, immersed in a relatively transient "wind" noise that we want to suppress. Wind components change rapidly in time and wind gusts can show very high energy, with comparable or greater energy than the volcanic tremor background, which is always present. This implies that we have no samples of pure "wind" noise for training. Both tremor and wind are non&#45;stationary broad&#45;band sources, with overlapping components in time and frequency as in the daily data&#45;set shown in <a href="/img/revistas/geoint/v53n1/a6f1.jpg" target="_blank">Figure 1</a>. Focusing our attention to power spectral density of a windy day and a few hours of tremor signal registration without wind present, we recognize that most of the energy overlaps in the low frequency range, while high frequency range is dominated by wind components, as depicted in <a href="#f2">Figure 2</a>. Our final task is to reduce wind noise in single&#45;channel volcanic seismic recordings by means of a classical refiltering technique as suppression rule, such as a Wiener one (see <a href="/img/revistas/geoint/v53n1/a6f3.jpg" target="_blank">Figure 3</a>).</font></p> 	    <p align="center"><a name="f2"></a><img src="/img/revistas/geoint/v53n1/a6f2.jpg"></p>      ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">As in the Erta 'Ale case (Cabras <i>et al.,</i> 2012), we aim to estimate the undesired components, or interference, <i>n(t)</i> and the source of interest, or target, <i>s(t)</i> directly from the observable data mix in the time domain, with minimal <i>a priori</i> knowledge. A common technique to manipulate a time&#45;varying observed signal consists in transforming it into a time&#45;frequency representation. Assuming that saturation effects are absent in the mixed observable <i>x(t):</i></font></p>  	    <p align="center"><img src="/img/revistas/geoint/v53n1/a6e3.jpg"></p>      <p align="justify"><font face="verdana" size="2">and assuming that <i>s(t)</i> and <i>n(t)</i> are uncorrelated, we can extend linearity in the power spectral domain and transform the data into a non&#45;negative representation suitable for NMF scheme:</font></p>  	    <p align="center"><img src="/img/revistas/geoint/v53n1/a6e4.jpg"></p>      <p align="justify"><font face="verdana" size="2">where the observable signal <i>x(t)</i> and the sources <i>s(t)</i> and <i>n(t)</i> are transformed into a complex time&#45;frequency representation <i>X</i>(<i>f,t</i>), <i>X<sub>s</sub>(f, t)</i> and <i>X<sub>n</sub>(f, t)</i> respectively. The most commonly used time&#45;frequency representation is the Short&#45;Time Fourier Transform (STFT) which transforms a discrete time signal into a complex spectrogram.</font></p>     <p align="justify"><font face="verdana" size="2">In the following a more general element&#45;wise exponentiated STFT was adopted:</font></p>  	    <p align="center"><img src="/img/revistas/geoint/v53n1/a6e5.jpg"></p>      <p align="justify"><font face="verdana" size="2">where <i>&#946;</i> is an important parameter to NMF performance, not only in audio application as shown in Schmidt <i>et al.</i> (2007), but also on seismic time&#45;frequency signal representation.</font></p>  	    <p align="justify"><font face="verdana" size="2">In a time&#45;frequency representation, the <i>k</i> columns of the dictionary matrix D in Eq. 1 constitute the characteristic frequency components of the spectrogram amplitude, while the <i>k</i> rows of the sparse code matrix H contains the weights of corresponding components of the dictionary matrix used in each time frame of the spectrogram amplitude.</font></p>  	    <p align="justify"><font face="verdana" size="2">Assuming the additivity of sources, the dictionary of the mixed signal of Eq. 1 can be seen as the horizontal concatenation of the individual source dictionaries. Moreover, the sparse code of the mixed signal can be seen as the vertical concatenation of the individual source sparse codes:</font></p>  	    ]]></body>
<body><![CDATA[<p align="center"><img src="/img/revistas/geoint/v53n1/a6e6.jpg"></p>     <p align="justify"><font face="verdana" size="2">where all matrices are non&#45;negative.</font></p>     <p align="justify"><font face="verdana" size="2">In order to estimate the magnitude of true sources <i>X<sub>s</sub></i> and <i>X<sub>n</sub></i>, we use a constrained sparse NMF (NMF*) to compute the dictionary of the target source <i>D<sub>s</sub></i> and the sparse code of both sources <i>H<sub>s</sub></i> and <i>H<sub>n</sub></i> assuming the dictionary <i>D<sub>n</sub></i> known <i>a priori</i> (Cabras <i>et al,</i> 2010). Finally we estimate the spectrogram of tremor source as:</font></p>  	    <p align="center"><img src="/img/revistas/geoint/v53n1/a6e7.jpg"></p>      <p align="justify"><font face="verdana" size="2">and the spectrogram of the wind noise as:</font></p>  	    <p align="center"><img src="/img/revistas/geoint/v53n1/a6e8.jpg"></p>     <p align="justify"><font face="verdana" size="2">Three strategies can be adopted to learn dictionaries <i>D<sub>s</sub></i> and <i>D<sub>n</sub></i> depending on available mixed and unmixed training data, characterizing the following enhancement models:</font></p>     <p align="justify"><font face="verdana" size="2">a)&nbsp;Precompute all dictionaries <i>(D<sub>s</sub></i> and <i>D<sub>n</sub></i> or in general <i>D<sub>1</sub>, D<sub>2</sub>,</i> <i>...,</i> D<sub>N</sub>) in non&#45;overlapping time&#45;series (Sources Training, ST enhancement model);</font></p>     <p align="justify"><font face="verdana" size="2">b)&nbsp;Precompute background noise dictionary <i>(D<sub>n</sub>)</i> when non&#45;overlapped to target and learn target dictionary <i>(D<sub>s</sub>)</i> from mixed recording (Background Training and Foreground Learning, BT/FL enhancement model);</font></p>     <p align="justify"><font face="verdana" size="2">Preliminary precompute background target dictionary (<i>D'<sub>s</sub></i>) when non&#45;overlapped to foreground noise, learn foreground noise dictionary <i>(D<sub>n</sub>)</i> from mixed recording, learn background target dictionary <i>(D<sub>s</sub>)</i> from mixed recording (Foreground Training and Background Learning, FT/BL enhancement model).</font></p>  	    ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2">A limitation of the Sources Training enhancement model strategy is that each source dictionary <i>D<sub>1</sub>, D<sub>2</sub>,</i> <i>...,</i> <i>D<sub>N</sub>,</i> must be modeled prior to the separation. This approach was followed by Mehmood <i>et al.</i> (2012) in a seismic footstep detection based system to separate the human footstep signatures from the horse footstep spectral signatures. However, the availability of non&#45;overlapping time series for all the different sources rarely applies to natural seismic datasets. Background Training and Foreground Learning is a more realistic strategy when background noise is more stationary than the foreground signal of interest and we can easily recognize enough samples of background noise&#45;only to learn <i>D<sub>n</sub>.</i> Schmidt <i>et al.,</i> (2007) suggest to pre&#45;compute <i>D<sub>n</sub>,</i> an approach followed also by (Cabras <i>et al.,</i> 2012), then learn <i>D<sub>s</sub>(f, m), H<sub>s</sub>(m, t)</i> and <i>H<sub>n</sub>(k, t)</i> with a modified constrained NMF, where <i>m</i> is the number of user defined components of the target source dictionary and <i>k</i> is the number of user defined components of the noise dictionary.</font></p>      <p align="justify"><font face="verdana" size="2">But if we are interested in a Background Source more stationary than the Foreground Noise, it will be probably very difficult to find samples of noise&#45;only components to carry out the training. An alternative approach has then to be followed, where a first training step on background source&#45;only samples is followed by a learning step of noise components which determines the new 2 steps foreground noise training (FT in <a href="/img/revistas/geoint/v53n1/a6f3.jpg" target="_blank">Figure 3</a>) while in Cabras <i>et al.</i> (2012) background noise was trained in one single step, because of noise&#45;only samples availability. The estimation of <i>a priori</i> noise dictionary, <i>D<sub>n</sub>,</i> is modeled by a two step sparse NMF computation, where equations are similar to the equations described in Cabras <i>et al.</i> (2012) but switching the index definitions of "noise" (n) and "source" (s) and shortly reformulated here for clarity. In the first step the sparse NMF algorithm starts with randomly initialized matrix, <i>D'<sub>s</sub></i> and <i>H'<sub>s</sub> </i>and alternates the following updates until convergence:</font></p>      <p align="center"><img src="/img/revistas/geoint/v53n1/a6e9.jpg"></p>     <p align="center"><img src="/img/revistas/geoint/v53n1/a6e10.jpg"></p>     <p align="justify"><font face="verdana" size="2">where <img src="/img/revistas/geoint/v53n1/a6i7.jpg"> operator indicates element&#45;wise multiplication, the fraction line element&#45;wise division between two matrices,<img src="/img/revistas/geoint/v53n1/a6i1.jpg"> is the Euclidean column&#45;wise normalization of the dictionary to prevent joint numerical drifts <i>D'<sub>s</sub></i> in <i>H'<sub>s</sub></i> and (Eggert and K&oacute;rner, 2004), <i><b>1</b></i> is a suitable size square matrix of ones and <i>A</i> is the activity diagonal binary square matrix, explained in more detail in the discussion section. The parameter <i>&#955;<sub>s</sub></i> determines the degree of sparsity in the code matrix. The trained preliminary dictionary of target source <i>D'<sub>s</sub></i> is the <i>a priori</i> knowledge to learn the noise dictionary <i>D<sub>n</sub>,</i> which can be trained directly from selected time sections of the available noisy signal using a constrained sparse <i>NMF</i> (NMF*) model estimation, so that only<i> D<sub>n</sub></i>, <i>H<sub>n</sub></i> and <i>H'<sub>s</sub></i> are estimated, while d' is predefined and left unchanged by the following updating equations until convergence:</font></p>     <p align="center"><img src="/img/revistas/geoint/v53n1/a6e11.jpg"></p>     <p align="center"><img src="/img/revistas/geoint/v53n1/a6e12.jpg"></p>     <p align="center"><img src="/img/revistas/geoint/v53n1/a6e13.jpg"></p>     <p align="justify"><font face="verdana" size="2">The resulting noise dictionary, <i>D<sub>n</sub>,</i> is the <i>a priori</i> estimated information needed by the final Background Learning step (BL) as shown in <a href="/img/revistas/geoint/v53n1/a6f3.jpg" target="_blank">Figure 3</a>. BL is the final Blind Source Separation step (BSS) which assigns the decomposed parts to the source of interest and discards the interference source described in Cabras <i>et al.</i> (2012) with a solution based on a constrained sparse Non&#45;negative Matrix Factorization <i>(NMF)</i> model estimation and <i>prior</i> knowledge on undesired component.</font></p>     <p align="justify">&nbsp;</p>      ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2"><b>A case study: Villarrica wind noise reduction</b></font></p>  	    <p align="justify"><font face="verdana" size="2">For illustrative purposes, we applied our methodology to a seismic dataset recorded at Villarrica volcano.</font></p>  	    <p align="justify"><font face="verdana" size="2"><i>Datasets</i></font></p>  	    <p align="justify"><font face="verdana" size="2">The analyzed dataset consists of 10 full day records of a single L22 short period vertical sensor component (&#402;<sub>0</sub>=2.0 Hz) sampled at 100 Hz. Each record exhibits non stationary high frequency non volcanic signal contamination, presumably determined by strong wind. No additional <i>a priori</i> information, such as a wind gauge, is available. <a href="/img/revistas/geoint/v53n1/a6f1.jpg" target="_blank">Figure 1</a> shows an example of a full day record spectral analysis. The Power Spectrum Density (PSD) of <a href="#f2">Figure 2</a> shows that the wind energy recorded from the vertical sensor component dominate in frequency &gt; 10 Hz, while overlaps with tremor energy in the low frequency range.</font></p>  	    <p align="justify"><font face="verdana" size="2"><i>Parameters</i></font></p>  	    <p align="justify"><font face="verdana" size="2">In order to process the dataset with the NMF algorithm, volcanic recordings are analyzed by an 8192 point Hamming windowed with <i>&#946;</i> = 1/3 exponentiated STFT and 50&#37; overlap (Eq. 4). This heuristic value of <i>&#946;,</i> which corresponds to the cube root compression, is quite important to achieve good NMF data decomposition in terms of SNR, our experimental results confirm that the more common value<i> &#946;=</i> 1 produces worse separation results.</font></p>      <p align="justify"><font face="verdana" size="2">The number of components in the target source dictionary, <i>m,</i> and the number of components in the noise source, <i>k,</i> are very important parameters which depend highly to the true but unknown sources, since all these components concur to model the sources. Using too few components results in a poor model of the sources which show strong evidence only for a limited set of data; conversely, more complex models (i.e. with many components) can always fit the data, but we must avoid implausible over&#45;parameterized models, following the principle of parsimony, i.e. finding the model that most simply accounts for the observed dataset. With our seismic datasets, we get plausible dictionaries with <i>k</i> and <i>m</i> in the range of 32&#45;64 components.</font></p>     <p align="justify"><font face="verdana" size="2">The sparsity regularization parameter enforces sparseness (i.e. simplicity) to learn the preliminary volcanic dictionary and controls the tradeoff between sparseness and reconstruction error. Increasing the sparseness term, the dictionary solution becomes less fragmented, since the decomposition algorithm tends to encode the input matrix using less dictionary components. Good solutions are achieved with <i>&#955;<sub>s</sub></i> = 0.5.</font></p>     <p align="justify"><font face="verdana" size="2">In a similar way, sparseness regularization parameter enforces sparseness to learn the wind noise dictionary <i>D<sub>n</sub></i> <i>,</i> in our experimental datasets; good results were obtained for <i>&#955;<sub>s</sub></i> = 0.5.</font></p>     <p align="justify">&nbsp;</p>      ]]></body>
<body><![CDATA[<p align="justify"><font face="verdana" size="2"><b>Results and discussion</b></font></p>  	    <p align="justify"><font face="verdana" size="2">In order to estimate the preliminary target dictionary <i>D'<sub>s</sub></i>, we analyze several 1 day records (8.64 Msamples&#64;100Hz sampling frequency) to catch some temporal frames without wind, as at 5 hrs of <a href="/img/revistas/geoint/v53n1/a6f1.jpg" target="_blank">Figure 1</a>, where Power Spectral Density is similar to the red line of <a href="#f2">Figure 2</a>. It is evident that a major requirement for the method to work properly is the availability and the recognition by the user of a time period for which there is only "source" signal, i.e. without wind contamination. This training period should be chosen by careful examination of the spectral content time evolution and/or, if available, using additional data such as datasets from pressure sensors, microphones, infrasound sensors or anemometers. Visual spectrogram screening can be a subjective and an error prone selection activity which must be taken in account and reduced adopting a statistical estimation algorithm, in <a href="/img/revistas/geoint/v53n1/a6f3.jpg" target="_blank">figure 3</a> we call it Statistical Foreground Activity Detector, which detect and flag the active frames (if frame t is active: <i>A<sub>tt</sub> =</i> 1, otherwhise 0), implemented as a time&#45;recursive averaging algorithm based on signal&#45;presence uncertainty, similar to statistical Voice Activity Detector (VAD) used in speech enhancement methods (Cabras <i>et al,</i> 2010). With the selected temporal frames we apply a sparse NMF to preliminary train the tremor dictionary shown in bottom left panel of Figure 4. This pre&#45;estimated source model is then used to estimate the wind noise dictionary applying a sparse NMF* learning algorithm on a strong windy day data&#45;set; the resulting <i>D<sub>n</sub></i> is depicted in the top right panel of <a href="/img/revistas/geoint/v53n1/a6f4.jpg" target="_blank">Figure 4</a>. This is a definitive wind noise dictionary for our data&#45;set and is very important to prevent volcanic tremor components amongs <i>D<sub>n</sub></i> components. The further learning step (BL in <a href="/img/revistas/geoint/v53n1/a6f3.jpg" target="_blank">Figure 3</a>) was applied to all records of the data&#45;set to estimate <i>D<sub>s</sub>, H<sub>s</sub></i> and <i>H<sub>n</sub></i> and estimate the tremor source spectrogram (Eq. 7) and the noise source spectrogram (Eq. 8). <a href="/img/revistas/geoint/v53n1/a6f5.jpg" target="_blank">Figure 5</a> shows the estimated spectrogram sources of a full day recording. The dataset tremor dictionary <i>D<sub>s</sub></i> is shown in the right bottom of <a href="/img/revistas/geoint/v53n1/a6f4.jpg" target="_blank">Figure 4</a>. It is similar to but smoother, depending on more data frames, and it differs greatly from <i>D<sub>n</sub></i> although it points out some frequency superposition.</font></p>      <p align="justify">&nbsp;</p>     <p align="justify"><font face="verdana" size="2"><b>Conclusions</b></font></p>  	    <p align="justify"><font face="verdana" size="2">We have presented an automatic method for wind noise reduction of volcanic tremor based on estimating the noise components dictionary by means of sparse NMF algorithms. The novel idea is to pre&#45;compute a preliminary dictionary model only for the target source and infer the dictionary model of the noise from a suitable representation of a signal mixture. Notwithstanding the obvious drawback that the user must be able to highlight a time period where source signal is not affected by wind (if possible with the help of additional wind&#45;affected sensors), experiments on a real world seismic&#45;only dataset recorded at Villarrica volcano contaminated by strong wind noise show that sparse NMF algorithms and our method are quite effective to reduce wind noise in single channel seismic recordings and can be succesfully used to better investigate the time evolution of tremor spectral content.</font></p>     <p align="justify">&nbsp;</p>      <p align="justify"><font face="verdana" size="2"><b>Acknowledgments</b></font></p>  	    <p align="justify"><font face="verdana" size="2">We are grateful to Dr. Jeff Witter for assistance with location and deinstallation of the seismometer site.</font></p>     <p align="justify">&nbsp;</p>      <p align="justify"><font face="verdana" size="2"><b>Bibliography</b></font></p>  	    ]]></body>
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