<?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>1794-6190</journal-id>
<journal-title><![CDATA[Earth Sciences Research Journal]]></journal-title>
<abbrev-journal-title><![CDATA[Earth Sci. Res. J.]]></abbrev-journal-title>
<issn>1794-6190</issn>
<publisher>
<publisher-name><![CDATA[Universidad Nacional de Colombia]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S1794-61902005000200007</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[USING THE KARHUNEN-LOÈVE TRANSFORM TO SUPPRESS GROUND ROLL IN SEISMIC DATA]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Gómez Londoño]]></surname>
<given-names><![CDATA[Ernesto]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Castillo López]]></surname>
<given-names><![CDATA[Luís]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Thaís de Souza]]></surname>
<given-names><![CDATA[Kazmierczak]]></given-names>
</name>
<xref ref-type="aff" rid="A02"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Ingeominas  ]]></institution>
<addr-line><![CDATA[ ]]></addr-line>
</aff>
<aff id="A02">
<institution><![CDATA[,Universidade Federal do Rio Grande do Sul  ]]></institution>
<addr-line><![CDATA[ ]]></addr-line>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>12</month>
<year>2005</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>12</month>
<year>2005</year>
</pub-date>
<volume>9</volume>
<numero>2</numero>
<fpage>139</fpage>
<lpage>147</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_arttext&amp;pid=S1794-61902005000200007&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_abstract&amp;pid=S1794-61902005000200007&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_pdf&amp;pid=S1794-61902005000200007&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="es"><p><![CDATA[En este estudio se implementó y modificó el Algoritmo de Sacchi (2002), basado en la Transformada Karhunen - Loève (K-L), como una técnica para la supresión de Ground Roll , mostrando que aunque la amplitud del Ground Roll es mayor que la amplitud de la señal al usar la Transformada K-L se tiene éxito en suprimirlo sin causar distorsión en las señales de reflexión, obteniendo mejores resultados frente a técnicas convencionales de remoción: f-k, Paso Alto y Pasa Banda. La Transformada K-L ha sido utilizada en el campo de la detección y procesamiento de imágenes ( Levy and Linderbaurn , 2000), en el reconocimiento de caras, iris y huellas dactilares como factores biométricos de identidad. Una sección sísmica es una imagen del subsuelo por tanto esta transformada puede ser usada en el procesamiento sísmico, porque remueve partes correlacionadas espacialmente y proveyendo una imagen clara y coherente.El algoritmo se aplicó a registros generados con Martillo, Thumper y fuentes explosivas. Se hizo un procesamiento convencional hasta el apilado, remplazando los filtros por le uso de la transformada K-L. Los resultados muestran que la Transformada K-L hace una mejor recuperación de la amplitud de los reflectores, eliminando refracciones que causan eventos someros irreales e incrementando la coherencia lateral de los eventos sísmicos, facilitando la interpretación geológica .]]></p></abstract>
<abstract abstract-type="short" xml:lang="en"><p><![CDATA[The Sacchi's algorithm (2002) based on the Karhunen-Loève (K-L) Transform was modified and implemented to suppress Ground Roll without distortion of the reflection signals, it provided better results than conventional techniques for noise removal like f-k, High-Pass and Band Pass Filters. The K-L Transform is well known in other fields as image processing (Levy and Linderbaurn , 2000), face, iris and fingerprint identification. A seismic section is an image of subsurface where the K-L can be useful in seismic processing because spatially uncorrelated signals can be removed providing a clear and coherent image. The algorithm was applied to seismic data generated with hammer, thumper and explosive sources. Conventional processing flows were used, but one replaced filters with K-L Transform, providing stacked sections. The K-L Transform recovers better the reflector amplitudes when compared with others filters, also it removes refractions that cause unreal shallow events and increases the lateral coherence of seismic events showing a more interpretable geology .]]></p></abstract>
<kwd-group>
<kwd lng="es"><![CDATA[Amplitud]]></kwd>
<kwd lng="es"><![CDATA[coherencia]]></kwd>
<kwd lng="es"><![CDATA[filtro]]></kwd>
<kwd lng="es"><![CDATA[Onda de Tierra]]></kwd>
<kwd lng="es"><![CDATA[ruido]]></kwd>
<kwd lng="en"><![CDATA[Amplitude]]></kwd>
<kwd lng="en"><![CDATA[coherent]]></kwd>
<kwd lng="en"><![CDATA[filter]]></kwd>
<kwd lng="en"><![CDATA[Ground Roll]]></kwd>
<kwd lng="en"><![CDATA[noise]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[  <font size="2" face="verdana">     <p align="center"><b>USING THE KARHUNEN-LO&Egrave;VE TRANSFORM TO SUPPRESS GROUND ROLL IN SEISMIC DATA</b></p>     <p>Ernesto G&oacute;mez Londo&ntilde;o<sup>1</sup>, Lu&iacute;s Castillo L&oacute;pez<sup>2</sup>  and Tha&iacute;s de Souza Kazmierczak<sup>2</sup></p>     <p><sup>1</sup> Ingeominas Bogot&aacute;, Recursos del Subsuelo, e-mail: <a href="mailto:egomez@ingeominas.gov.co">egomez@ingeominas.gov.co</a>    <br> <sup>2</sup> Universidade Federal do Rio Grande do Sul - Brazil.e-mail: <a href="mailto:luis.castillo@ufrgs.br">luis.castillo@ufrgs.br</a>; e-mail: <a href="mailto:thais.kazmierczak@ufrgs.br">thais.kazmierczak@ufrgs.br</a></p> <hr size="1">     <p><b>RESUMEN</b></p>     <p>En este estudio se implement&oacute; y modific&oacute; el Algoritmo de Sacchi (2002), basado en la Transformada Karhunen-Lo&egrave;ve (K-L), como una t&eacute;cnica para la supresi&oacute;n de Ground Roll, mostrando que aunque la amplitud del Ground Roll es mayor que la amplitud de la se&ntilde;al al usar la Transformada K-L se tiene &eacute;xito en suprimirlo sin causar distorsi&oacute;n en las se&ntilde;ales de reflexi&oacute;n, obteniendo mejores resultados frente a t&eacute;cnicas convencionales de remoci&oacute;n: f-k, Paso Alto y Pasa Banda. La Transformada K-L ha sido utilizada en el campo de la detecci&oacute;n y procesamiento de im&aacute;genes (Levy and Linderbaurn, 2000), en el reconocimiento de caras, iris y huellas dactilares como factores biom&eacute;tricos de identidad. Una secci&oacute;n s&iacute;smica es una imagen del subsuelo por tanto esta transformada puede ser usada en el procesamiento s&iacute;smico, porque remueve partes correlacionadas espacialmente y proveyendo una imagen clara y coherente.El algoritmo se aplic&oacute; a registros generados con Martillo, Thumper y fuentes explosivas. Se hizo un procesamiento convencional hasta el apilado, remplazando los filtros por le uso de la transformada K-L. Los resultados muestran que la Transformada K-L hace una mejor recuperaci&oacute;n de la amplitud de los reflectores, eliminando refracciones que causan eventos someros irreales e incrementando la coherencia lateral de los eventos s&iacute;smicos, facilitando la interpretaci&oacute;n geol&oacute;gica.</p>     <p> <b>Palabras clave</b>: Amplitud, coherencia, filtro, Onda de Tierra, ruido.</p> <hr size="1">     <p><b>ABSTRACT</b></p>     <p>The Sacchi&rsquo;s algorithm (2002) based on the Karhunen-Lo&egrave;ve (K-L) Transform was modified and implemented    to suppress Ground Roll without distortion of the reflection signals, it provided better results than conventional techniques for noise removal like f-k, High-Pass and Band Pass Filters. The K-L Transform is well known in other fields as image processing (Levy and Linderbaurn, 2000), face, iris and fingerprint identification. A seismic section is an image of subsurface where the K-L can be useful in seismic processing    because spatially uncorrelated signals can be removed providing a clear and coherent image. The algorithm    was applied to seismic data generated with hammer, thumper and explosive sources. Conventional processing flows were used, but one replaced filters with K-L Transform, providing stacked sections. The K-L Transform recovers better the reflector amplitudes when compared with others filters, also it removes refractions that cause unreal shallow events and increases the lateral coherence of seismic events showing a more interpretable geology.</p>     ]]></body>
<body><![CDATA[<p><b>Key words</b>: Amplitude, coherent, filter, Ground Roll, noise.</p> <hr size="1">     <p><b>INTRODUCTION</b></p>     <p>The Ground Roll is (Scales and Snider, 1998) generated in shallow layers and is a typical Rayleigh wave. It is characterized by low velocity and frequency and high amplitude, being considered a coherent noise in seismic exploration (D'Agosto et al., 2002). The KL algorithm transforms the seismic data in a reasonable number of independent eigen functions that represents the most important signal characteristics. It has been considered a very advisable tool in the processing and analysis of reflection data (Al-Yahya, 1991).The conventional filtering techniques: f-k, High-Pass and BandPass are applied in the frequency domain but in the case of Ground Roll amplitude stronger than reflection signals, f-k filters cause serious distortion of the signal (Karsh and Bayrak, 2004). High Pass filter is based on the low frequency of the Ground Roll, with the disadvantage that also eliminates the low-frequency content of reflection signals. Band pass filter depends on the amount of overlaps between the noise and the signal, therefore when the frequency bands concentrated the energy in each band without overlap, the signal/noise ratio will not change (Yilmaz, 1987).The K-L Transform separates the Ground roll from the reflector signal, permitting to subtract it from seismic data. Its application to real data showed that the Ground Roll suppression increased lateral coherence of seismic events in a stacked section.</p>     <p><b>THEORETICAL BACKGROUND</b></p>     <p>The surface waves in the raw register in <a href="#fig1">figure 1</a> travel with velocities ranging from 100 to 1000 m/s and with frequencies around 10 Hertz and lower than those of reflections and refractions. Note how the near surface effects distort travel time curve at the right flank of reflection &quot;A&quot;.</p>     <p>    <center><a name="fig1"></a><img src="img/revistas/esrj/v9n2/v9n2a07fig1.gif"></center></p>     <p><b>The Karhunen-Lo&egrave;ve Transform</b></p>     <p>It makes a principal component analysis that is a mathematical way of determining that linear transformation  of a sample of points in L-dimensional space which exhibits the properties of the sample most clearly along the coordinate axes. Along the new axes, the sample variance are extremes and uncorrelated, see <a href="#fig2">figure 2</a>. Using a cutoff on the spread along each axis, a sample may be reduced in its dimensionality. This way it can be used to transform independent coordinates into significant and independent ones.</p>     <p>    ]]></body>
<body><![CDATA[<center><a name="fig2"></a><img src="img/revistas/esrj/v9n2/v9n2a07fig2.gif"></center></p>     <p><b>K-L Transform Implementation</b></p>     <p>The seismic traces xi(t) correspond to the rows of the named data matrix x<sub>n*m</sub> , n is the number of traces in the gather and m the number of gathers. The zero-lag covariance matrix  is (Jones and Levy, 1987):</p>     <p>    <center><img src="img/revistas/esrj/v9n2/v9n2a07img1.gif"></center></p>     <p>This expression can be decomposed as</p>     <p>    <center><img src="img/revistas/esrj/v9n2/v9n2a07img2.gif"></center></p> </font>    <p><font size="2" face="verdana">In equation 2 the columns of the matrix V<sub>n*p</sub> are the eigenvectors and A<sub>n*n</sub> is a diagonal matrix with the eigen values on the diagonal. These eigen values are ordered in descending sequence along the principal diagonal of the matrix A<sub>n*n</sub> , V<sup>t</sup><sub>*np</sub> is the corresponding transpose matrix. The principal component of the data can be written by:</font></p> <font size="2" face="verdana">    <p>    ]]></body>
<body><![CDATA[<center><img src="img/revistas/esrj/v9n2/v9n2a07img3.gif"></center></p>     <p>If we form the matrix M&rsquo;<sub>p*m</sub> by selecting the upper m rows of the matrix M<sub>p*m</sub>, m is related with the order of the filter or principal row number, placing zeros in the remaining n-m rows, n is related with the Cut of the Filter, the Ground roll is assumed to be represented by the matrix product between the eigenvectors matrix V<sub>n*p</sub> and the matrix M&rsquo;<sub>p*m</sub>, that include the principal components in agreement with the following expression:</p>     <p>    <center><img src="img/revistas/esrj/v9n2/v9n2a07img4.gif"></center></p>     <p>Finally, the Ground roll X&rsquo;<sub>n*m</sub> is subtracted from the data matrix X<sub>n*m</sub>, obtaining the gather without Ground roll</p>     <p>    <center><img src="img/revistas/esrj/v9n2/v9n2a07img5.gif"></center></p>     <p>Xo is a <sub>n*m</sub> matrix that represents the filtered seismic  gather.As mentioned before x<sub>n*m</sub> is the input data matrix and X&rsquo;<sub>n*m</sub> is a matrix that represents the Ground roll extracted from the input data.</p>     <p><b>RESULTS</b></p>     <p>The capacity of KL Algorithm to suppress Ground Roll at gather level is evaluated using shot gathers with dispersive waves of high amplitude, obtained from shallow and dip seismic surveys using 3 types of source were used: hammer, dynamite and thumper.</p>     ]]></body>
<body><![CDATA[<p><b>Hammer</b></p>     <p>The 102.data seismic gather (<a href="#fig3">figure 3</a>) is a record corresponding to the UN-01 Seismic Line. Note in the red square like the Ground Roll diminishes before (left) and after (right) KL Algorithm application; the gather is much less noisy in the first 100 ms, with Order of the Filter: 2 and Cut of the Filter: 1.<a href="#fig4">Figure 4</a> shows the interactive spectral analysis for Seismic Record No 12 of UN-01, before on top and after on bottom the application of the K-L Transform. The K-L Filtering gives good results because it compresses more the amplitude spectrum. Additionally, the maximum amplitude of the raw power spectrum with the K-L is lower into the red circle (10000) compared with one of the same gather without this filter in the black circle (4,5 e + 07), indicating high amplitude concentrations in the spectrum; corresponding to the Ground Roll suppressed with K-L. The record with K-L displays seismic events with coherence and continuity.</p>     <p>    <center><a name="fig3"></a><img src="img/revistas/esrj/v9n2/v9n2a07fig3.gif"></center></p>     <p>    <center><a name="fig4"></a><img src="img/revistas/esrj/v9n2/v9n2a07fig4.gif"></center></p>     <p><b>Explosive Source</b></p>     <p>The shot gather in <a href="#fig5">Figure 5</a>, was generated using dynamite, it displays hyperbolic moveout, coherent    noise masking the reflection signals. The analyses with f-k, High-Pass and the KL Filters gave the better results for the last one.The Band-Pass filter is used where the seismic trace contains low-frequency noise, such as Ground Roll and high-frequency ambient noise. The seismic reflection  energy usually is confined to a bandwidth between 10 to 70 Hertz, with dominant frequency of 15 Hz.Comparison between Band-Pass [15-30-55-70] (<a href="#fig6">Figure 6</a>), and KL Filter gave a better result for the KL, the Ground Roll cone has been suppressed and the lateral coherence of deeper seismic events increased.</p>     <p>    <center><a name="fig5"></a><img src="img/revistas/esrj/v9n2/v9n2a07fig5.gif"></center></p>     ]]></body>
<body><![CDATA[<p>    <center><a name="fig6"></a><img src="img/revistas/esrj/v9n2/v9n2a07fig6.gif"></center></p>     <p><b>Thumper</b></p>     <p><a href="#fig7">Figure 7</a> shows an example, of the shot gather 481 with high content of Ground Roll. The Seismic  Line RM-01, was acquired using a thumper source. A substantial increasing in the lateral coherence of the seismic events below the 200 ms is remarked.<a href="#fig8">Figure 8</a> shows the amplitude spectrum of the shot gather 481 before and after the KL filter application, a significant reduction of the high amplitude corresponding to Ground Roll is seen.</p>     <p>    <center><a name="fig7"></a><img src="img/revistas/esrj/v9n2/v9n2a07fig7.gif"></center></p>     <p>    <center><a name="fig8"></a><img src="img/revistas/esrj/v9n2/v9n2a07fig8.gif"></center></p>     <p><b>Shallow Survey</b></p>     <p>The 2D seismic data was acquired in October-2004 with a split spread configuration in the campus of the National University of Colombia, with a Geode seismic recorder with 24 channels for high resolution acquisition, the source consist in a hammer (8 kg) and geophones with vertical component. The processing of the UN-01 Seismic Line provided stacked sections shown in <a href="#fig9">Figure 9</a>, on top conventional and on bottom with K-L. The section on bottom presents better results, increases lateral coherence and gives a clearer image. On the other hand, the KL suppresses unreal shallow events (indicated by the arrow), due to refractions that are observed with the conventional processing.</p>     ]]></body>
<body><![CDATA[<p>    <center><a name="fig9"></a><img src="img/revistas/esrj/v9n2/v9n2a07fig9.gif"></center></p>     <p><b>Deep Survey</b></p>     <p>This 2D data was acquired using a thumper in split spread configuration at Southern of the Middle Magdalena Valley, involving tertiary sediments from the Gualanday Group.The stacked section in RM-01 in Figure 10 was obtained with conventional processing on bottom and with application of the K-L Transform on top. The top image presents a great rank of amplitude (-3 to 3) compared with the conventional stacked on bottom (-2 to 2) as observed into the red circles; indicating a better amplitude recovering in reflectors with K-L use, although the processing sequence did not include fx Decon. Besides the KL shows coherence and it does not present the whitening effect due to the conventional processing flow (<a href="#fig10">Figure 10</a>. Red square, bottom). By the other hand, high dips (black arrow), are observed in conventional process image which are not true because the direction of seismic line was N-S, parallels to the beds strikes of the tertiary sediments with very smooth dips; in consequence they must be horizontals in the seismic section, as it is observed in the K-L image in agreement with the subsurface geology.</p>     <p>    <center><a name="fig10"></a><img src="img/revsitas/esrj/v9n2/v9n2a07fi10.gif"></center></p>     <p><b>CONCLUSIONS</b></p>     <p>The Algorithm Karhunen-Lo&egrave;ve is computationally economic and efficient to filter seismic data, providing    coherent information of subsurface image.The interactive spectral analysis showed more concentrations    of high amplitude due to the Ground Roll, and it verifies that K-L Algorithm suppresses the Ground Roll waves. Also it is verified than the amplitude    of the Ground Roll is stronger than the reflection  signals. By using K-L Algorithm to extract the Ground Roll it suggests a form to suppress Ground Roll, without distorting the reflection signals.Additionally, using K-L filter increases the lateral coherence of seismic events, in comparison with the three conventional methods of suppression: Filters  f - k, High-Pass and Band- Pass. The algorithm was tested with raw gather containing Ground Roll (high amplitude) obtained from shallow and depth seismic land surveys with different source (hammer,  dynamite and thumper. A lateral coherence increase is observed in stacked sections. The K-L use recovers the amplitude of the deep reflectors furnishing a resultant section more approximated to real geology.</p>     <p><b>REFERENCES</b></p>     <!-- ref --><p>&bull; Al-Husseini, M., Glover J. and Barley B., 1981. Dispersion Patterns of the Ground Roll in Eastern Saudi Arabia, Geophysics, Vol 46, p. 121-137.&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000072&pid=S1794-6190200500020000700001&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p>&bull; Al-Yahya, K.M., 1991. Application of the Partial Karhunen-Lo&egrave;ve Transform to Suppress Random Noise in Seismic Sections: Geophys. Prosp., 39, p. 77-93.&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000073&pid=S1794-6190200500020000700002&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p>&bull; DAgosto, C., Marfurt, K. and Steven, J., 2002. Modeling and Removal of Ground Roll from Horizontal Component of C-Waves. SEG.&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000074&pid=S1794-6190200500020000700003&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p><font size="2" face="verdana">&bull; Jones, I. F., and Levy, S., 1987. Signal - to - Noise Enhancement in Multichannel Seismic Data Processing: Geophys. Prosp., 35, p. 12-32.</font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000075&pid=S1794-6190200500020000700004&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p><font size="2" face="verdana">&bull; Karsh, H. and Bayrak, Y., 2004. Using the Wiener - Levinson Algorithm to Suppress Ground Roll. Journal of Applied Geophysics 55, p 187-197.</font>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000076&pid=S1794-6190200500020000700005&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p>&bull; Levy, A. and Linderbaurn, M., 2000. Sequential Karhunen-Lo&egrave;ve Basis Extraction and its Application to Images, IEEE Transactions on Image Processing, Vol 9, No 8, p. 1371-1374.&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000077&pid=S1794-6190200500020000700006&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p>&bull; Nesvijski, E. G., 2000. On a Possibility of Rayleigh Transformed Sub-Surface Waves Propagation. Center of Technology, Federal University of Santa Maria, Brasil.&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000078&pid=S1794-6190200500020000700007&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p>&bull; Sacchi, M.D., 2002. Karhunen - Lo&egrave;ve (KL) Filtering of Seismic Data Algorithm. Signal Analysis and Imaging Group (SAIG), Department of Physics, Alberta University.&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000079&pid=S1794-6190200500020000700008&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p>&bull; Scales, J. and Snider, R., 1998. &iquest;What is Noise?: Geophysics, Vol 63, p. 1122-1124.&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000080&pid=S1794-6190200500020000700009&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p>&bull; Yilmaz, O., 1987. Seismic Data Processing: Society of Exploration Geophysicists, Tulsa, p. 9-79.&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000081&pid=S1794-6190200500020000700010&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --><!-- ref --><p>&bull; Zywicki, D., 1999. Traditional Seismic Surface Wave Tests. Georgia Tech Research Institute (GTRI), p. 11.34.&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=000082&pid=S1794-6190200500020000700011&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> ]]></body><back>
<ref-list>
<ref id="B1">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Al- Husseini]]></surname>
<given-names><![CDATA[M]]></given-names>
</name>
<name>
<surname><![CDATA[Glover]]></surname>
<given-names><![CDATA[J]]></given-names>
</name>
<name>
<surname><![CDATA[Barley]]></surname>
<given-names><![CDATA[B]]></given-names>
</name>
</person-group>
<article-title xml:lang="en"><![CDATA[Dispersion Patterns of the Ground Roll in Eastern Saudi Arabia]]></article-title>
<source><![CDATA[Geophysics]]></source>
<year>1981</year>
<volume>46</volume>
<page-range>121-137</page-range></nlm-citation>
</ref>
<ref id="B2">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[K.M.]]></surname>
<given-names><![CDATA[Al- Yahya]]></given-names>
</name>
</person-group>
<article-title xml:lang="fr"><![CDATA[Application of the Partial Karhunen-Loève Transform to Suppress Random Noise in Seismic Sections]]></article-title>
<source><![CDATA[Geophys . Prosp]]></source>
<year>1991</year>
<volume>39</volume>
<page-range>77-93</page-range></nlm-citation>
</ref>
<ref id="B3">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[DAgosto]]></surname>
<given-names><![CDATA[C]]></given-names>
</name>
<name>
<surname><![CDATA[Marfurt]]></surname>
<given-names><![CDATA[K]]></given-names>
</name>
<name>
<surname><![CDATA[Steven]]></surname>
<given-names><![CDATA[J]]></given-names>
</name>
</person-group>
<source><![CDATA[Modeling and Removal of Ground Roll from Horizontal Component of C-Waves]]></source>
<year>2002</year>
<publisher-name><![CDATA[SEG]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B4">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Jones]]></surname>
<given-names><![CDATA[I. F]]></given-names>
</name>
<name>
<surname><![CDATA[Levy]]></surname>
<given-names><![CDATA[S]]></given-names>
</name>
</person-group>
<article-title xml:lang="en"><![CDATA[Signal - to - Noise Enhancement in Multichannel Seismic Data Processing]]></article-title>
<source><![CDATA[Geophys . Prosp]]></source>
<year>1987</year>
<volume>35</volume>
<page-range>12-32</page-range></nlm-citation>
</ref>
<ref id="B5">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Karsh]]></surname>
<given-names><![CDATA[H]]></given-names>
</name>
<name>
<surname><![CDATA[Bayrak]]></surname>
<given-names><![CDATA[Y]]></given-names>
</name>
</person-group>
<article-title xml:lang="en"><![CDATA[Using the Wiener - Levinson Algorithm to Suppress Ground Roll]]></article-title>
<source><![CDATA[Journal of Applied Geophysics]]></source>
<year>2004</year>
<volume>55</volume>
<page-range>187-197</page-range></nlm-citation>
</ref>
<ref id="B6">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Levy]]></surname>
<given-names><![CDATA[A]]></given-names>
</name>
<name>
<surname><![CDATA[Linderbaurn]]></surname>
<given-names><![CDATA[M]]></given-names>
</name>
</person-group>
<article-title xml:lang="en"><![CDATA[Sequential Karhunen-Loève Basis Extraction and its Application to Images]]></article-title>
<source><![CDATA[IEEE Transactions on Image Processing]]></source>
<year>2000</year>
<volume>9</volume>
<numero>8</numero>
<issue>8</issue>
<page-range>1371-1374</page-range></nlm-citation>
</ref>
<ref id="B7">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Nesvijski]]></surname>
<given-names><![CDATA[E. G]]></given-names>
</name>
</person-group>
<source><![CDATA[On a Possibility of Rayleigh Transformed Sub-Surface Waves Propagation]]></source>
<year>2000</year>
<publisher-name><![CDATA[Center of TechnologyFederal University of Santa Maria]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B8">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Sacchi]]></surname>
<given-names><![CDATA[M.D]]></given-names>
</name>
</person-group>
<source><![CDATA[Karhunen - Loève (KL) Filtering of Seismic Data Algorithm. Signal Analysis and Imaging Group (SAIG )]]></source>
<year>2002</year>
<publisher-name><![CDATA[Department of Physics, Alberta University]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B9">
<nlm-citation citation-type="journal">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Scales]]></surname>
<given-names><![CDATA[J]]></given-names>
</name>
<name>
<surname><![CDATA[Snider]]></surname>
<given-names><![CDATA[R]]></given-names>
</name>
</person-group>
<article-title xml:lang="en"><![CDATA[¿What is Noise?]]></article-title>
<source><![CDATA[Geophysics]]></source>
<year>1998</year>
<volume>63</volume>
<page-range>1122-1124</page-range></nlm-citation>
</ref>
<ref id="B10">
<nlm-citation citation-type="book">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Yilmaz]]></surname>
<given-names><![CDATA[O]]></given-names>
</name>
</person-group>
<source><![CDATA[Seismic Data Processing]]></source>
<year>1987</year>
<page-range>9-79</page-range><publisher-loc><![CDATA[Tulsa ]]></publisher-loc>
<publisher-name><![CDATA[Society of Exploration Geophysicists]]></publisher-name>
</nlm-citation>
</ref>
<ref id="B11">
<nlm-citation citation-type="">
<person-group person-group-type="author">
<name>
<surname><![CDATA[Zywicki]]></surname>
<given-names><![CDATA[D]]></given-names>
</name>
</person-group>
<source><![CDATA[Traditional Seismic Surface Wave Tests. Georgia Tech Research Institute (GTRI)]]></source>
<year>1999</year>
<page-range>11.34</page-range></nlm-citation>
</ref>
</ref-list>
</back>
</article>
