<?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">OJER</journal-id><journal-title-group><journal-title>Open Journal of Earthquake Research</journal-title></journal-title-group><issn pub-type="epub">2169-9623</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojer.2014.34014</article-id><article-id pub-id-type="publisher-id">OJER-51807</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Earth&amp;Environmental Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  Crustal Stresses and Seismodynamic Characteristics in the Upper Crust
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>fuk</surname><given-names>Aydın</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Atatürk University, Oltu Faculty of Earth Sciences, Mining Engineering, Erzurum, Turkey</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>uaydin@atauni.edu.tr</email></corresp></author-notes><pub-date pub-type="epub"><day>26</day><month>11</month><year>2014</year></pub-date><volume>03</volume><issue>04</issue><fpage>143</fpage><lpage>151</lpage><history><date date-type="received"><day>15</day>	<month>September</month>	<year>2014</year></date><date date-type="rev-recd"><day>17</day>	<month>October</month>	<year>2014</year>	</date><date date-type="accepted"><day>12</day>	<month>November</month>	<year>2014</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><html>
 <head></head>
 
  In this paper an approach to estimate near-surface seismodynamic features by using distance- amplitude reduction with geotectonic characteristics of the upper crust in the Eastern Anatolia is discussed. The data set used in this study consists of 287 regional earthquakes in the magnitude range of 3.0 - 6.1, epicentral distances between 15 km and 202 km and their focal depths reaching up to 13 km. The entire study area is divided into three tectonic blocks according to the distribu-tions of the earthquakes and the location of the fault segment. The estimated quality factor 
  <strong><em>Q</em></strong>
  <sub><strong><em>P-S</em></strong></sub>  values for the three regions ranged from 28.6 to 65, highlighting the regional differences in the seismodynamics of the crust. In Eastern Anatolia, the relatively low average quality factor values (
  <strong><em>Q</em></strong>
  <sub><strong><em>P</em></strong></sub>: 37, 
  <strong><em>Q<sub>S</sub></em></strong>: 55) show average (0.217) and average values ( 
  <img alt="" src="Edit_e106ef4e-9e77-4efb-b947-ece77ce4c6ec.bmp" />
  <strong><em><sub>P</sub></em></strong>: 0.0166, 
  <img alt="" src="Edit_42f2ecef-dbdf-4be8-8430-a33a9f712b18.bmp" />
  <sub><strong><em>S</em></strong></sub>: 0.017). The lowest 
  <strong><em>Q<sub>S </sub>/<strong><em>Q</em></strong><sub><strong><em>P</em></strong></sub></em></strong>  value 1.39 and the highest 
  <strong><em>V<sub>P</sub></em></strong>
  <strong><em><sub> </sub>/V<sub><strong><em>S</em></strong></sub></em></strong>  value 1.65 are found at the Mus station. The highest Poisson’s ratio  
  <img alt="" src="Edit_2f796e68-f7ce-4bd9-ab5a-479575336bf0.bmp" /> and lowest absorption coefficient  
  <img alt="" src="Edit_06d03918-b793-4164-ae18-33c8e223e75b.bmp" /> were found in the Mus area. The variation in 
  <strong><em>Q</em></strong> ,  
  <img style="width:14px;height:15px;" alt="" src="Edit_ca02878b-7504-41b3-9bfa-b53a3b385acf.bmp" width="8" height="16" /> and  
  <img alt="" src="Edit_3dc281e7-daca-43da-b508-46ec9a05fa63.bmp" />indicates that the northern part (Erc and Kem region) of East Anatolia appears to be more active and heterogeneous compared with the southern part (Mus region) of East Anatolia.
 
</html></p></abstract><kwd-group><kwd>Body Wave</kwd><kwd> Seismodynamic Parameters</kwd><kwd> Seismotectonics</kwd><kwd> Upper Crust</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Amplitude reduction is generally frequency-dependent and, more importantly, attenuation characteristics can reveal unique information about lithology, physical state and the degree of rock saturation [<xref ref-type="bibr" rid="scirp.51807-ref1">1</xref>] . Although some authors suggest that near-surface <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x20.png" xlink:type="simple"/></inline-formula> may be frequency-dependent [<xref ref-type="bibr" rid="scirp.51807-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51807-ref3">3</xref>] following the laboratory results [<xref ref-type="bibr" rid="scirp.51807-ref4">4</xref>] and different work [<xref ref-type="bibr" rid="scirp.51807-ref5">5</xref>] that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x21.png" xlink:type="simple"/></inline-formula> is independent of frequency, allowing determination of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x22.png" xlink:type="simple"/></inline-formula> as a function of depth based on the amplitude attenuation of Rayleigh-wave data. The quality factor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x23.png" xlink:type="simple"/></inline-formula> is a function of depth, which is directly related to the material damping ratio [<xref ref-type="bibr" rid="scirp.51807-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.51807-ref7">7</xref>] . It is of fundamental interest in earthquake engineering, [<xref ref-type="bibr" rid="scirp.51807-ref8">8</xref>] geotechnical engineering, ground-water, and environmental studies, as well as in oil exploration and earthquake seismology. The study [<xref ref-type="bibr" rid="scirp.51807-ref9">9</xref>] also indicates that at surface pressure most dry rocks have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x24.png" xlink:type="simple"/></inline-formula>. The Eastern Anatolia fault system is examined using the epicentre distance-amplitude reduction relations model and the work focuses on the seismic body wave’s absorption which reflects the seismotectonic and seismodynamic features belonging to the lithosphere. Regional attenuation changes in body waves can be an indicator to determine the seismotectonic properties of the inner crust. These seismodynamic properties must be known in order to fully understand crustal deformation in the earth. From this information I aim to relate crustal inelasticity with the seismotectonic patterns in the inner crust of Eastern Anatolia.</p><p>There are numerous mechanisms contributing to attenuation and some conditions can affect the attenuation pattern significantly [<xref ref-type="bibr" rid="scirp.51807-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.51807-ref10">10</xref>] . The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x25.png" xlink:type="simple"/></inline-formula> attribute will only detect a lateral variation in lithology if the geological anomaly can be detected in the actual sections [<xref ref-type="bibr" rid="scirp.51807-ref11">11</xref>] . The variability of the near-surface properties is caused by changes in porosity, permeability, fractures, fluids, compaction, diagenesis and metamorphism [<xref ref-type="bibr" rid="scirp.51807-ref12">12</xref>] . The motivation behind <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x26.png" xlink:type="simple"/></inline-formula> analysis is that the P-wave to S-wave velocity ratio is an effective indicator of lithology and/or fractures, cracks and pore space [<xref ref-type="bibr" rid="scirp.51807-ref13">13</xref>] . Poorly consolidated or fractured material will also exhibit high <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x27.png" xlink:type="simple"/></inline-formula> values. In addition, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x28.png" xlink:type="simple"/></inline-formula>analysis can yield estimates of Poisson’s ratio [<xref ref-type="bibr" rid="scirp.51807-ref11">11</xref>] . Poisson’s ratio (or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x29.png" xlink:type="simple"/></inline-formula>) is a key parameter in studying the petrologic properties of crustal rocks [<xref ref-type="bibr" rid="scirp.51807-ref14">14</xref>] and can provide tighter constraints on the crustal composition than either P or S wave velocity alone [<xref ref-type="bibr" rid="scirp.51807-ref15">15</xref>] . It is suggested that seismic energy dissipation could become anisotropic as a result of the application of a uniaxial stress [<xref ref-type="bibr" rid="scirp.51807-ref16">16</xref>] .</p></sec><sec id="s2"><title>2. Tectonics of Eastern Anatolia</title><p>The north-south intercontinental collision between Arabia and Eurasia since the middle-late Miocene [<xref ref-type="bibr" rid="scirp.51807-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.51807-ref18">18</xref>] and the initiation of the back-arc extension in the Aegean Sea since the late Oligocene [<xref ref-type="bibr" rid="scirp.51807-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.51807-ref20">20</xref>] are the boundary conditions allowing the westward mass transfer of Anatolia, which is usually considered to be a rigid plate bordered by the North Anatolian Fault (NAF) and the East Anatolian Fault (EAF), which meet at Karliova. The high elevations of East Anatolia should not be related to the intercontinental convergence between the Arabian and Eurasian plates, but to mantle up welling, leading to lithospheric thinning and recent extension [<xref ref-type="bibr" rid="scirp.51807-ref21">21</xref>] . The most important tectonic feature is symbolized by high and young topography in the seismically active zone along the Zagros-Bitlis suture resulting from the collision of the Arabian plate with Eurasia (<xref ref-type="fig" rid="fig1">Figure 1</xref>) [<xref ref-type="bibr" rid="scirp.51807-ref22">22</xref>] .</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Map showing the study area (rectangle) and the three seismic stations (filled triangles) used in this study. Stations show blue filled triangles, Erzurum (ERZ), Erzincan (ERC), Palu (PALU) and Muş (MUS). NAFZ-North Anatolian Fault Zone; MOFZ-Malatya Ovacık Fault Zone; EAFZ-East Anatolian Fault Zone; NEAFZ-North East Anatolian Fault. Orange dotted line show major fold and thrust belt BZSZ-Bitlis-Zagros structure zone</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x30.png"/></fig><p>Eastern Anatolia is seismically active and is dissected by numerous seismogenic faults, predominantly in a strike-slip motion. The study areas are characterized by both the North Anatolian Fault Zone and the East Anatolian Fault Zone (<xref ref-type="fig" rid="fig1">Figure 1</xref>). Eastern Anatolia has been affected by several strong earthquakes (December 26, 1939 MS = 7.9, and in 1992, MS = 6.8, Erzincan earthquakes, 13 September, 1924, MS = 6.8 Pasinler (Erzurum) earthquake, 30 October 1983 MS = 5.2, Horasan-Narman, and 23 October 2011 MS = 7.1 Van earthquake). In particular the December 26, 1939 Erzincan quake was the most destructive in Turkey, during which Erzincan and the vicinity affected lost as much as half of its population.</p></sec><sec id="s3"><title>3. Data</title><p>The analyzed events occurred along the three selected active seismic areas encompassing three different geological and seismotectonics contexts and are associated with various types of tectonic mechanisms in the Eastern Anatolia region. The digital events data utilized for seismodynamic properties was recorded during 2006-2010 at the regional seismograph network of three seismic stations by the Earthquake Research Centre, Atat&#252;rk University, Erzurum. The Ercstation is situated on a sedimentation fan in the vicinity of high tectonic and seismic activity. The Kemstation is situated at alluvial basin near recent tectonic and moderate seismic activity, and the Musstation is on a thick alluvial layer away from tectonic and seismic activities at high altitude (<xref ref-type="table" rid="table1">Table 1</xref>). All stations are equipped with CMG-3TD broadband seismographs with a dynamic range of 96 dB and a sampling rate of 100 samples per second. The data detection is based on magnitude, epicentre distance and hypocentre depths. The selected data set consists of 287 vertical recorded waveforms of 141 events with a focal depth between 1.4 km and 12.8 km, epicentre distance between 15 km and 202 km, magnitude ranging between 3 and 6.1 (<xref ref-type="fig" rid="fig2">Figure 2</xref>).</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Map of the simplified tectonics and distribution of the epicentral locations of 202 earthquakes used in this study (black filled circles), seismic stations and cities (red filled triangles)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x31.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The parameters of the seismic stations used in this study</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Station</th><th align="center" valign="middle" >Lat˚</th><th align="center" valign="middle" >Long˚</th><th align="center" valign="middle" >Altitudes</th><th align="center" valign="middle" >Lithology of the Station</th></tr></thead><tr><td align="center" valign="middle" >Kemaliye (Kem)</td><td align="center" valign="middle" >39.2667</td><td align="center" valign="middle" >38.5139</td><td align="center" valign="middle" >1000</td><td align="center" valign="middle" >Alivual Basin</td></tr><tr><td align="center" valign="middle" >Erzincan (Erc)</td><td align="center" valign="middle" >39.7587</td><td align="center" valign="middle" >39.5059</td><td align="center" valign="middle" >1200</td><td align="center" valign="middle" >Sedimentation Fan</td></tr><tr><td align="center" valign="middle" >Mus (Mus)</td><td align="center" valign="middle" >38.7416</td><td align="center" valign="middle" >41.4991</td><td align="center" valign="middle" >1322</td><td align="center" valign="middle" >Alluvial Fan</td></tr></tbody></table></table-wrap><p>The epicentres corrections were made because of the differing distances. Studies of seismic wave attenuation in Eastern Anatolia have been limited due to a limited number of available seismic stations. Other seismic station data is not of sufficient quality for this type of work. Personally, I preferred the vertical <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula> wave amplitudes for this study due to the fact that they can be observed clearly in the vertical component in the inner crust. In order to remove the effect of the magnitudes on the amplitudes, the magnitude normalisation process has been performed for a reference value<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula>, 0. The maximum amplitude values, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula> arrival time have been obtained with the scream software (<xref ref-type="fig" rid="fig3">Figure 3</xref>). In general, the quality factor and Poisson’s ratio is computed without considering the regional seismic velocity differences. In order to eliminate this unfavourable situation vertical <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x37.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x38.png" xlink:type="simple"/></inline-formula> wave velocities for each region have been estimated (<xref ref-type="fig" rid="fig3">Figure 3</xref> and <xref ref-type="table" rid="table2">Table 2</xref>). These <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x39.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x40.png" xlink:type="simple"/></inline-formula> wave velocities are used to determine the attenuation coefficient and Poisson’s ratio. The seismodynamic properties of the Earth’s crust beneath three selected research areas in Eastern Anatolia were examined using a method based on the decrease of body wave amplitude in time. The three station and the epicentral locations of the earthquakes are presented in the <xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref>. All raw data was filtered using the Butterworth filter for 1 Hz. I used <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x41.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x42.png" xlink:type="simple"/></inline-formula> amplitude normalisation methods for reference values<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x43.png" xlink:type="simple"/></inline-formula>, so as to correct the effects of the magnitudes. The maximum amplitudes were used to calculate the attenuation coefficient. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x44.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x45.png" xlink:type="simple"/></inline-formula> local amplitudes are used to determine the attenuation coefficients (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x46.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x47.png" xlink:type="simple"/></inline-formula>) of the three different tectonics area in Eastern Anatolia.</p></sec><sec id="s4"><title>4. Methods</title><p>By contrast to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x48.png" xlink:type="simple"/></inline-formula> (and consequently also to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x49.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x50.png" xlink:type="simple"/></inline-formula>), the “effective attenuation” parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x51.png" xlink:type="simple"/></inline-formula> in eq. denotes the frequency-dependent effects of the intrinsic attenuation and scattering on random, small-scale heterogeneities, i.e., for Rayleigh- or Mie-type scattering [<xref ref-type="bibr" rid="scirp.51807-ref23">23</xref>] .</p><disp-formula id="scirp.51807-formula100"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2740053x52.png"  xlink:type="simple"/></disp-formula><p>Further, by making, the seismic wave amplitude rate is a parameter that reflects the seismodynamic features of media. The logarithmic decrement, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x53.png" xlink:type="simple"/></inline-formula>is defined as follows [<xref ref-type="bibr" rid="scirp.51807-ref24">24</xref>] . The usual assumption that the spectral site responses <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x54.png" xlink:type="simple"/></inline-formula> are similar or that they can be corrected to a common spectrum [<xref ref-type="bibr" rid="scirp.51807-ref25">25</xref>] , the effects of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x55.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x56.png" xlink:type="simple"/></inline-formula> can be removed by constructing time-lag normalized spectral ratios at different observation times (and/or receiver positions):</p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The plots of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x60.png" xlink:type="simple"/></inline-formula> (km) and t (sn) are used to estimate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x61.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x62.png" xlink:type="simple"/></inline-formula> wave velocity values for the stations in: (a) Kemaliye; (b) Erzincan; and (c) Mus.</title></caption><fig id ="fig3_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x57.png"/></fig><fig id ="fig3_2"><label> (c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x58.png"/></fig><fig id ="fig3_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x59.png"/></fig></fig-group><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x63.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x64.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x65.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x66.png" xlink:type="simple"/></inline-formula> values for Kem, Erc, and Mus stations</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Stat.</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x67.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x68.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x69.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x70.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x71.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x72.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x73.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><sub><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x74.png" xlink:type="simple"/></inline-formula> </sub></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x75.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x76.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >Event</th></tr></thead><tr><td align="center" valign="middle" >Kem</td><td align="center" valign="middle" >6.30</td><td align="center" valign="middle" >3.58</td><td align="center" valign="middle" >1.759</td><td align="center" valign="middle" >0.0214</td><td align="center" valign="middle" >0.0202</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >61</td><td align="center" valign="middle" >41</td><td align="center" valign="middle" >1.48</td><td align="center" valign="middle" >0.229</td><td align="center" valign="middle" >99</td></tr><tr><td align="center" valign="middle" >Erc</td><td align="center" valign="middle" >6.25</td><td align="center" valign="middle" >3.65</td><td align="center" valign="middle" >1.712</td><td align="center" valign="middle" >0.0187</td><td align="center" valign="middle" >0.0176</td><td align="center" valign="middle" >1.06</td><td align="center" valign="middle" >40</td><td align="center" valign="middle" >29</td><td align="center" valign="middle" >1.39</td><td align="center" valign="middle" >0.209</td><td align="center" valign="middle" >95</td></tr><tr><td align="center" valign="middle" >Mus</td><td align="center" valign="middle" >6.61</td><td align="center" valign="middle" >3.74</td><td align="center" valign="middle" >1.767</td><td align="center" valign="middle" >0.0130</td><td align="center" valign="middle" >0.0120</td><td align="center" valign="middle" >1.08</td><td align="center" valign="middle" >65</td><td align="center" valign="middle" >40</td><td align="center" valign="middle" >1.65</td><td align="center" valign="middle" >0.232</td><td align="center" valign="middle" >93</td></tr><tr><td align="center" valign="middle" >Avar.</td><td align="center" valign="middle" >6.38</td><td align="center" valign="middle" >3.65</td><td align="center" valign="middle" >1.74</td><td align="center" valign="middle" >0.0177</td><td align="center" valign="middle" >0.0166</td><td align="center" valign="middle" >1.06</td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >37</td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >0.223</td><td align="center" valign="middle" >287</td></tr></tbody></table></table-wrap><disp-formula id="scirp.51807-formula101"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2740053x77.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x78.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x79.png" xlink:type="simple"/></inline-formula> are spectral amplitudes at different depths. In this description, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x80.png" xlink:type="simple"/></inline-formula>represents the uncompensated geometrical spreading, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x81.png" xlink:type="simple"/></inline-formula> is the attenuation, which turned out to be frequency-independent in all data examples considered so far. The spectral ratio Equation (2) allows inversion for the three types of attenuation parameters. The properties of elastic crustal attenuation describe the loss of seismic energy in the crust to internal pressure, such as the absorption by fluids in compressional and strain or friction along seismotectonic boundaries. It is denoted by a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x82.png" xlink:type="simple"/></inline-formula> value, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x83.png" xlink:type="simple"/></inline-formula>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x84.png" xlink:type="simple"/></inline-formula> being the energy and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x85.png" xlink:type="simple"/></inline-formula>—the energy dissipation during a one wave cycle [<xref ref-type="bibr" rid="scirp.51807-ref26">26</xref>] .</p><disp-formula id="scirp.51807-formula102"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2740053x86.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x87.png" xlink:type="simple"/></inline-formula> is angular frequency, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x88.png" xlink:type="simple"/></inline-formula>is the quality factor, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x89.png" xlink:type="simple"/></inline-formula>is the epicentre distance, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x90.png" xlink:type="simple"/></inline-formula> is the peak strain energy lost in the cycles. For propagating waves, the parameter that truly exists and is directly measurable is the spatial attenuation coefficient [<xref ref-type="bibr" rid="scirp.51807-ref27">27</xref>] . In the literature the attenuation coefficient at 1 Hz is given as:</p><disp-formula id="scirp.51807-formula103"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2740053x91.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51807-formula104"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2740053x92.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51807-formula105"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2740053x93.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51807-formula106"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2740053x94.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x95.png" xlink:type="simple"/></inline-formula> is the amplitude at any distance from the source, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x96.png" xlink:type="simple"/></inline-formula>is distance, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x97.png" xlink:type="simple"/></inline-formula>is the initial or reference amplitude, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x98.png" xlink:type="simple"/></inline-formula>is the attenuation coefficient, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x99.png" xlink:type="simple"/></inline-formula> is the epicentre distance. The normalized maximum amplitude of the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x100.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x101.png" xlink:type="simple"/></inline-formula> wave vertical components were used in order to compute the absorption calculations (<xref ref-type="fig" rid="fig4">Figure 4</xref>). The seismic quality factor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x102.png" xlink:type="simple"/></inline-formula> and the attenuation coefficient <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x103.png" xlink:type="simple"/></inline-formula> are strongly affected by the tectonic pattern of the crust in any region [<xref ref-type="bibr" rid="scirp.51807-ref28">28</xref>] . Active tectonic regions are associated with low <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x104.png" xlink:type="simple"/></inline-formula> values [<xref ref-type="bibr" rid="scirp.51807-ref29">29</xref>] -[<xref ref-type="bibr" rid="scirp.51807-ref31">31</xref>] .</p><p>The quality factor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x105.png" xlink:type="simple"/></inline-formula> is defined as the energy loss per unit cycle due to inelasticity [<xref ref-type="bibr" rid="scirp.51807-ref24">24</xref>] . <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x106.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x107.png" xlink:type="simple"/></inline-formula> values are energy and amplitude respectively, which are lost in each energy cycle. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x108.png" xlink:type="simple"/></inline-formula>can be written as:</p><disp-formula id="scirp.51807-formula107"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-2740053x109.png"  xlink:type="simple"/></disp-formula><p>where, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x110.png" xlink:type="simple"/></inline-formula>is 1 Hz frequency, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x111.png" xlink:type="simple"/></inline-formula>is the absorption coefficient, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x112.png" xlink:type="simple"/></inline-formula>is the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x113.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x114.png" xlink:type="simple"/></inline-formula> wave velocity, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x115.png" xlink:type="simple"/></inline-formula> are the quality factors that can be easily computed by Equation (8). The relationship of</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x116.png" xlink:type="simple"/></inline-formula>is used to determine the elastic parameter of Poisson’s ratio <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x117.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.51807-ref32">32</xref>] . By definition, Poisson’s ratio is the ratio of radial contraction to axial elongation. Its value in common rock type’s ranges from 0.20 to 0.35. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x118.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x119.png" xlink:type="simple"/></inline-formula> local velocities are used to determine the local quality factor<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x120.png" xlink:type="simple"/></inline-formula>, local quality factor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x121.png" xlink:type="simple"/></inline-formula> the regional Poisson’s ratio<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x122.png" xlink:type="simple"/></inline-formula> for three different regions.</p></sec><sec id="s5"><title>5. Results</title><p>The great difference of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x123.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x124.png" xlink:type="simple"/></inline-formula> were found in the Mus region. It may be potentially important for the interpretation of regional variations in attenuation. It is estimated the regional Poisson’s ratio by calculated speeds of the seismic body waves. The highest <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x125.png" xlink:type="simple"/></inline-formula> is found at the Mus station, the Zagros-Bitlis Suture and its vicinity, and the western side of the Mus station and its vicinity. The highest <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x126.png" xlink:type="simple"/></inline-formula> value is observed in the Kem and Mus region while lowest <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x127.png" xlink:type="simple"/></inline-formula> value is observed in the Mus region (<xref ref-type="fig" rid="fig5">Figure 5</xref>). The highest Poisson’s ratio-<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x128.png" xlink:type="simple"/></inline-formula> and lowest absorption coefficient-<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x129.png" xlink:type="simple"/></inline-formula> was found in the Mus area. The lowest <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x130.png" xlink:type="simple"/></inline-formula> and high <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x131.png" xlink:type="simple"/></inline-formula> values were found in the Erc region (<xref ref-type="table" rid="table2">Table 2</xref>).</p><p>Numerous studies have been carried out in different parts of the world in order to determine the attenuation of seismic waves in the crust [<xref ref-type="bibr" rid="scirp.51807-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.51807-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.51807-ref33">33</xref>] -[<xref ref-type="bibr" rid="scirp.51807-ref38">38</xref>] , which determined the attenuation seismic waves in a number of tectonically stable and active areas. In the 1982 found that the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x132.png" xlink:type="simple"/></inline-formula> ratio to be unity for air dry rocks and less than unity for fully saturated rocks [<xref ref-type="bibr" rid="scirp.51807-ref39">39</xref>] . Our result on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x133.png" xlink:type="simple"/></inline-formula> ratio is in the range of 1.39 - 1.65 (<xref ref-type="table" rid="table2">Table 2</xref>)</p><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Plots of the absorption for ln (Ap) and ln (As) versus distance for the stations in: (a) Kem; (b) Erc; and (c) Mus.</title></caption><fig id ="fig4_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x134.png"/></fig><fig id ="fig4_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x135.png"/></fig><fig id ="fig4_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x136.png"/></fig><fig id ="fig4_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x137.png"/></fig><fig id ="fig4_5"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x138.png"/></fig><fig id ="fig4_6"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x139.png"/></fig></fig-group><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Plot of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x141.png" xlink:type="simple"/></inline-formula> value versus<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x142.png" xlink:type="simple"/></inline-formula>. Kem and Mus stations which do not differ significantly from the average value of Poisson’s ratio for the area. Erc stations which differ significantly from the average value for the area</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-2740053x140.png"/></fig><p>and is in good agreement with the results obtained by the laboratory measurement and other experimental results mentioned down. In Eastern Anatolia, the relatively low average <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x143.png" xlink:type="simple"/></inline-formula> values (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x144.png" xlink:type="simple"/></inline-formula>: 37,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x145.png" xlink:type="simple"/></inline-formula>: 55) show average <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x146.png" xlink:type="simple"/></inline-formula> (0.223) and average <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x147.png" xlink:type="simple"/></inline-formula> values (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x148.png" xlink:type="simple"/></inline-formula>: 0.0166,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x149.png" xlink:type="simple"/></inline-formula>: 0.0177) (<xref ref-type="table" rid="table2">Table 2</xref>). In Eastern Anatolia, the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x150.png" xlink:type="simple"/></inline-formula> values are between 1.48 and 1.65. The highest <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x151.png" xlink:type="simple"/></inline-formula> value 1.65 is observed in the Mus region, while the lowest <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x152.png" xlink:type="simple"/></inline-formula> value 1.39 is observed in the Erc region (<xref ref-type="fig" rid="fig3">Figure 3</xref>). This study of results is quite comparable and in relation with tectonic and crustal structure is therefore similar. In this study I attempted to determine these different seismodynamic relationships among the North Anatolian Fault zone, the East Anatolian Fault zone and the Bitlis-Zagros structure in the Eastern Anatolia.</p></sec><sec id="s6"><title>6. Discussion</title><p>The spatial variation of the regional coda quality factor has been utilized in order to obtain a better understanding of tectonics, seismicity, seismic risk analysis and engineering seismology [<xref ref-type="bibr" rid="scirp.51807-ref30">30</xref>] [<xref ref-type="bibr" rid="scirp.51807-ref40">40</xref>] . Seismic waves are attenuated travelling through crust due to Jin the elasticity and heterogeneity of the medium [<xref ref-type="bibr" rid="scirp.51807-ref41">41</xref>] -[<xref ref-type="bibr" rid="scirp.51807-ref44">44</xref>] . The average <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x153.png" xlink:type="simple"/></inline-formula> value calculated for Eastern Anatolia is approximately 37. This is equal to the value computed for the Erzurum region of Eastern Anatolia (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x154.png" xlink:type="simple"/></inline-formula>: 37) [<xref ref-type="bibr" rid="scirp.51807-ref45">45</xref>] and greater than the Oltu region in Eastern Anatolia (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x155.png" xlink:type="simple"/></inline-formula>: 33) [<xref ref-type="bibr" rid="scirp.51807-ref46">46</xref>] . It is calculated S wave attenuation coefficient and quality factor for Eastern Anatolia using the model based on the epicentre distance-amplitude relations [<xref ref-type="bibr" rid="scirp.51807-ref47">47</xref>] . Coda <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x156.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x157.png" xlink:type="simple"/></inline-formula> values are determined between 37 &#177; 14 and 724 &#177; 256 by using 196 earthquakes occurring between 2005-2010 in Eastern Anatolia [<xref ref-type="bibr" rid="scirp.51807-ref48">48</xref>] .</p><p>The different stresses characteristics of Kem, Erc and Mus indicate the different velocity values and deviating seismodynamic values. The region is also the site of very high tectonic activity revealed by several recent high magnitude earthquakes along active faults. The highest attenuation was observed in Mus. It may be caused by certain geological structures. This study indicates that there is a relationship between seismodynamic properties and stress structures in the upper crust of Eastern Anatolia.</p></sec><sec id="s7"><title>7. Conclusion</title><p>Compared to Poisson’s ratios, the compression values can be a better indicator of the content of seismodynamic properties. For the three different regions, the amplitude dependency of average<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x158.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x159.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x160.png" xlink:type="simple"/></inline-formula> values show a range of heterogeneity in the upper crust. The lateral local Poisson’s ratio can be explained by local variations of seismic velocity and different stresses structures. These are related to different seismodynamic and kinematic activities in the inner crust. The lowest <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x161.png" xlink:type="simple"/></inline-formula> and high <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-2740053x162.png" xlink:type="simple"/></inline-formula> values can be explained by tectonic activity, and severe deformation in the Erzincan region. A high Poisson’s ratio and low absorption coefficient was found in the Mus area, which is consistent with the possibility of a partial melt in the upper crust and Bitlis-Zagros structure. Mus and the area around the Karliova Triple Junction fields can be considered to be pressure subduction zones, indicating the presence of greater compressional power at the Zagros-Bitlis Suture zone and its immediate surroundings, by which the structure of the NAF and EAFZ systemsin the north of the Bitlis-Zagros is formed. The variation of the seismodynamic parameter indicates that the seismotectonics and heterogeneity of the lithosphere affect the stress behaviour of the inner crust. The differentiation of seismodynamic properties in different areas is due to the heterogeneities along the inner crust. These differences in attenuation properties are due to actual crustal thickness differences and may be because that the stresses in the region have different patterns.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.51807-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Toks?z, M.N. and Johnson, D.H. (1981) Seismic Wave Attenuation. Society of Exploration Geophysicist. </mixed-citation></ref><ref id="scirp.51807-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Jeng, Y., Tsai, J. and Chen, S. (1999) An Improved Method of Determining Near-Surface Q. Geophysics, 64, 1608- 1617. http://dx.doi.org/10.1190/1.1444665</mixed-citation></ref><ref id="scirp.51807-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Xia, J., Miller, R.D., Park, C.B. and Tian, G. (2002) Determining Q of Near-Surface Materials from Rayleigh Waves. Journal of Applied Geophysics, 51, 121-129. http://dx.doi.org/10.1016/S0926-9851(02)00228-8</mixed-citation></ref><ref id="scirp.51807-ref4"><label>4</label><mixed-citation publication-type="book" xlink:type="simple">Johnston, D.H. and Toks?z, M.N. (1981) Definitions and Terminology. In: Toks?z, M.N. and Johnston, D.H., Eds., Seismic Wave Attenuation, 1-5. </mixed-citation></ref><ref id="scirp.51807-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Mitchell, B.J. (1995) An Elastic Structure and Evolution of the Continental Crust and Upper Mantle from Seismic Surface Wave Attenuation. Reviews of Geophysics, 33, 441-462. http://dx.doi.org/10.1029/95RG02074</mixed-citation></ref><ref id="scirp.51807-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Lai, C.G. and Rix, G.J. (1998) Simultaneous Inversion of Rayleigh Phase Velocity and Attenuation for Near-Surface Site Characterization. Report No. GIT-CEE/GEO-98-2. School of Civil and Environmental Engineering, Georgia Institute of Technology.</mixed-citation></ref><ref id="scirp.51807-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Rix, G.J., Lai, C.D. and Spang Jr., A.W. (2000) In Situ Measurement of Damping Ratio Using Surface Waves. Journal of Geotechnical and Geoenvironmental Engineering, 126, 472-480. Anatolia, Turkey, Soil Dynamics and Earthquake Engineering, 31, 1192-1195.</mixed-citation></ref><ref id="scirp.51807-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Kramer, S.L. (1996) Geotechnical Earthquake Engineering. Prentice Hall, Upper Saddle River.</mixed-citation></ref><ref id="scirp.51807-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Johnston, D.H., Toksoz, M.N. and Timur, A. (1979) Attenuation of Seismic Waves in Dry and Saturated Rocks: I. Mechanics in Geophysics, 44, 691-711. http://dx.doi.org/10.1190/1.1440970</mixed-citation></ref><ref id="scirp.51807-ref10"><label>10</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Aki</surname><given-names> K. </given-names></name>,<etal>et al</etal>. (<year>1985</year>)<article-title>Theory of Earthquake Prediction with Special Reference to Monitoring of the Quality Factor of Lithosphere by the Coda Method</article-title><source> Journal of Earthquake Predict Research</source><volume> 3</volume>,<fpage> 219</fpage>-<lpage>230</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.51807-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Sheriff, R.E. (1991) Encyclopaedia Dictionary of Exploration Geophysics. Society of Exploration Geophysicists, Tulsa.</mixed-citation></ref><ref id="scirp.51807-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Toks?z, M.N., Cheng, C.H. and Timur, A. (1976) Velocities of Seismic Waves in Porous Rocks. Geophysics, 41, 621- 645. http://dx.doi.org/10.1190/1.1440639 </mixed-citation></ref><ref id="scirp.51807-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Tatman, R.H. (1982) VP/VS and Lithology. Geophysics, 47, 336-334. http://dx.doi.org/10.1190/1.1441339</mixed-citation></ref><ref id="scirp.51807-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Christensen, N.I. (1996) Poisson’s Ratio and Crustal Seismology. Journal of Geophysical Research, 101, 3139-3156.  
http://dx.doi.org/10.1029/95JB03446</mixed-citation></ref><ref id="scirp.51807-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Zhao, D., Tani, H. and Mishra, O.P. (2004) Crustal Heterogeneity in the 2000 Western Tottori Earthquake Region: Effect of Fluids from Slab Dehydration. Physics of the Earth and Planetary Interiors, 145, 161-177.  
http://dx.doi.org/10.1016/j.pepi.2004.03.009</mixed-citation></ref><ref id="scirp.51807-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Nur, A. and Simmons, G. (1969) Stress-Induced Velocity Anisotropy in Rocks: An Experimental Study. Journal of Geophysical Research, 74, 6667-6674. http://dx.doi.org/10.1029/JB074i027p06667</mixed-citation></ref><ref id="scirp.51807-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Seng?r, A.M.C. and Yilmaz, Y. (1981) Tethyan Evaluation of Turkey: A Plate Tectonic Approach. Tectonophysics, 75, 181-190, 193-199, 203-241. http://dx.doi.org/10.1016/0040-1951(81)90275-4 </mixed-citation></ref><ref id="scirp.51807-ref18"><label>18</label><mixed-citation publication-type="book" xlink:type="simple">?eng?r, A.M.C., G?rür, N. and Saroglu, F. (1985) Strike-Slip Faulting and Related Basin Formation in Zones of Tectonic Escape: Turkey as a Case Study. In: Biddle, K.T. and Christie-Blick, N., Eds., Strike-Slip Deformation, Basin Formation and Sedimentation, Vol. 37, Society of Economic Paleontologists and Mineralogists Special Publication, 227-264. </mixed-citation></ref><ref id="scirp.51807-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Jolivet, L., Daniel, J.M., Truffert, C. and Goffe, B. (1994) Exhumation of Deep Crustal Metamorphic Rocks and Crustal Extension in Back-Arc Regions. Lithos, 33, 3-30. http://dx.doi.org/10.1016/0024-4937(94)90051-5</mixed-citation></ref><ref id="scirp.51807-ref20"><label>20</label><mixed-citation publication-type="book" xlink:type="simple">Jolivet, L. and Patriat, M. (1999) Ductile Extension and the Formation of the Aegean Sea. In: Durand, B., Jolivet, L., Horvath, F. and Seranne, M., Eds., The Mediterranean Basins: Tertiary Extension within the Alphine Oragen, Vol. 156, Geological Society, Special Publications, London, 427-456.</mixed-citation></ref><ref id="scirp.51807-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Dhondt, D. and Chorowicz, J. (2006) Review of the Neotectonics of the Eastern Turkish—Armenian Plateau by Geomorphic Analysis of Digital Elevation Model Imagery. International Journal of Earth Sciences, 95, 34-49.  
http://dx.doi.org/10.1007/s00531-005-0020-3</mixed-citation></ref><ref id="scirp.51807-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">?eng?r, A. and Kidd, W. (1979) Post-Collisional Tectonics of the Turkish-Iranian Plateau and a Comparison with Tibet. Tectonophysics, 55, 361-376. http://dx.doi.org/10.1016/0040-1951(79)90184-7 </mixed-citation></ref><ref id="scirp.51807-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Morozov, I.B. (2009) Seismological Attenuation Coefficient and the Origins of Apparent Q(f). University of Saskatchewan, Saskatoon, 32.</mixed-citation></ref><ref id="scirp.51807-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Aki, K. and Richards, P.G. (1980) Quantitative Seismology: Theory and Methods. Vol. 1, W. H. Freeman and Co., London.</mixed-citation></ref><ref id="scirp.51807-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">Morozov, I.B., Morozova, E.A., Smithson, S.B. and Solodilov, L.N. (1998) On the Nature of the Teleseismic Pn Phase Observed on the Ultralong-Range Profile “Quartz,” Russia. Bulletin of the Seismological Society of America, 88, 62- 73.</mixed-citation></ref><ref id="scirp.51807-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">Knopoff, L. (1964) Q. Reviews of Geophysics, 2, 625-660. http://dx.doi.org/10.1029/RG002i004p00625</mixed-citation></ref><ref id="scirp.51807-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">Chernov, L.A. (1960) Wave Propagation in a Random Medium. McGraw-Hill, New York, 35-57, 168 p.</mixed-citation></ref><ref id="scirp.51807-ref28"><label>28</label><mixed-citation publication-type="other" xlink:type="simple">Mitchell, B.J. (1995) Anelastic Structure and Evolution of the Continental Crust and Upper Mantle from Seismic Surface Wave Attenuation. Reviews of Geophysics, 33, 441-462. http://dx.doi.org/10.1029/95RG02074</mixed-citation></ref><ref id="scirp.51807-ref29"><label>29</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Mitchell</surname><given-names> B.J. </given-names></name>,<etal>et al</etal>. (<year>1975</year>)<article-title>Regional Rayleigh Wave Attenuation in North America. Journal of Geophysical Research, 80, 4904-4916. Mak, S., Chan, L.S., Chandler, A.M. and Koo, R.C.H. (2004) Coda Q Estimates in the Hong Kong Region</article-title><source> Journal of Asian Earth Science</source><volume> 24</volume>,<fpage> 127</fpage>-<lpage>136</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.51807-ref30"><label>30</label><mixed-citation publication-type="other" xlink:type="simple">Singh, S.K. and Herrmann, R.B. (1983) Regionalization of Crustal Coda Q in the Continental United States. Journal of Geophysical Research, 88, 527-538. http://dx.doi.org/10.1029/JB088iB01p00527</mixed-citation></ref><ref id="scirp.51807-ref31"><label>31</label><mixed-citation publication-type="other" xlink:type="simple">Jin, A. and Aki, K. (1980) Spatial and Temporal Correlation between Coda Q and Seismicity in China. Bulletin of the Seismological Society of America, 78, 741-769.</mixed-citation></ref><ref id="scirp.51807-ref32"><label>32</label><mixed-citation publication-type="other" xlink:type="simple">Utsa, T. (1984) Estimation of Parameters for Recurrence Models of Earthquakes. Bulletin of the Earthquake Research Institute, The University of Tokyo, 59, 53-66.</mixed-citation></ref><ref id="scirp.51807-ref33"><label>33</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Herrmann</surname><given-names> R.B. </given-names></name>,<etal>et al</etal>. (<year>1980</year>)<article-title>Q Estimation Using the Coda of Local Earthquakes</article-title><source> Bulletin of the Seismological Society of America</source><volume> 70</volume>,<fpage> 447</fpage>-<lpage>468</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.51807-ref34"><label>34</label><mixed-citation publication-type="other" xlink:type="simple">Roecker, S.W., Tuckel, B., King, J. and Hatzfeld, D. (1982) Estimations of Q in Central Asia as a Function of Frequency and Depth Using the Coda of Locally Recorder Earthquakes. Bulletin of the Seismological Society of America, 72, 129-149.</mixed-citation></ref><ref id="scirp.51807-ref35"><label>35</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Reha</surname><given-names> S. </given-names></name>,<etal>et al</etal>. (<year>1984</year>)<article-title>Q Determination from Local Earthquakes in South Carolina Plain</article-title><source> Bulletin of the Seismological Society of America</source><volume> 74</volume>,<fpage> 2257</fpage>-<lpage>2268</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.51807-ref36"><label>36</label><mixed-citation publication-type="other" xlink:type="simple">Ak?nc?, A., Taktak, G. and Ergintav, S. (1994) Attenuation of Coda Waves in the Western Anatolia. Physics of the Earth and Planetary Interiors, 87, 155-165. http://dx.doi.org/10.1016/0031-9201(94)90028-0 </mixed-citation></ref><ref id="scirp.51807-ref37"><label>37</label><mixed-citation publication-type="other" xlink:type="simple">Ak?nc?, A. and Eyido?an, H. (1996) Frequency-Dependent Attenuation of S and Coda Waves in Erzincan Region (Turkey). Physics of the Earth and Planetary Interiors, 97, 109-119. http://dx.doi.org/10.1016/0031-9201(96)03155-X </mixed-citation></ref><ref id="scirp.51807-ref38"><label>38</label><mixed-citation publication-type="other" xlink:type="simple">Anderson, D.L. and Given, J.W. (1982) Absorption Band Q Model for the Earth. Journal of Geophysical Research, 87, 3893-3904. http://dx.doi.org/10.1029/JB087iB05p03893</mixed-citation></ref><ref id="scirp.51807-ref39"><label>39</label><mixed-citation publication-type="book" xlink:type="simple">Vassiliou, M., Salvado, C.A. and Tittmann, B.R. (1982) Seismic Attenuation. In: Carmichael, R.S., Ed., CRC Handbook of Physical Properties of Rocks, Vol. 3, CRC Press, Boca Raton.</mixed-citation></ref><ref id="scirp.51807-ref40"><label>40</label><mixed-citation publication-type="other" xlink:type="simple">Jin, A. and Aki, K. (1988) Spatial and Temporal Correlation between Coda Q and Seismicity in China. Bulletin of the Seismological Society of America, 78, 741-769.</mixed-citation></ref><ref id="scirp.51807-ref41"><label>41</label><mixed-citation publication-type="other" xlink:type="simple">Ricker, N. (1953) The Form and Laws of Propagation of Seismic Wavelets. Geophysics, 18, 10-40.  
http://dx.doi.org/10.1190/1.1437843</mixed-citation></ref><ref id="scirp.51807-ref42"><label>42</label><mixed-citation publication-type="other" xlink:type="simple">Futterman, W.I. (1962) Dispersive Body Waves. Journal of Geophysical Research, 67, 5279-5291.  
http://dx.doi.org/10.1029/JZ067i013p05279</mixed-citation></ref><ref id="scirp.51807-ref43"><label>43</label><mixed-citation publication-type="other" xlink:type="simple">White, J.E. (1983) Underground Sound, Application of Seismic Waves. Elsevier Science Publishing Company Inc, Amsterdam, 83-137.</mixed-citation></ref><ref id="scirp.51807-ref44"><label>44</label><mixed-citation publication-type="other" xlink:type="simple">Kneib, G. and Shapiro, S.A. (1995) Viscoacoustic Wave Propagation in 2-D Random Media and Separation of Absorption and Scattering Attenuation. Geophysics, 60, 459-467. http://dx.doi.org/10.1190/1.1443783</mixed-citation></ref><ref id="scirp.51807-ref45"><label>45</label><mixed-citation publication-type="other" xlink:type="simple">Ayd?n, U. and Kadirov, A. (2007) Attenuatin in Eastern Anatolia. ?stanbul üniversitesi Mühendislik Fakültesi, Yerbilimleri Dergisi, C., 20, S,1, s. 35-41. </mixed-citation></ref><ref id="scirp.51807-ref46"><label>46</label><mixed-citation publication-type="other" xlink:type="simple">Ayd?n, U., Acar, A. and Din?er, I. (2006) Estimation of Seismic Wave Absorption Rates near Area Earthquakes in East Anatolia Erzurum ?entre. ?ukurova üniversitesi Fenve Mühendislik Bilimleri Dergisi. C., 15, S. 1, s. 86-96. </mixed-citation></ref><ref id="scirp.51807-ref47"><label>47</label><mixed-citation publication-type="other" xlink:type="simple">Ayd?n, U. and Sahin, S. (2011) Comparison of the Attenuation Properties for Two Different Areas in Eastern Anatolia, Turkey. Soil Dynamics and Earthquake Engineering, 31, 1192-1195. </mixed-citation></ref><ref id="scirp.51807-ref48"><label>48</label><mixed-citation publication-type="other" xlink:type="simple">?ahin, ?. and Ayd?n, U. (2011) Do?u Anadolu’da yüksek frekansl? dalga yay?n?m?. The High Frequency Wave Propagation in East Anatolia, Uluslararas??lmi Pratik Kongresi, Bakü. </mixed-citation></ref></ref-list></back></article>