<?xml version="1.0" encoding="UTF-8"?>
<collection xmlns="http://www.loc.gov/MARC21/slim">
 <record>
  <leader>     caa a22        4500</leader>
  <controlfield tag="001">445387548</controlfield>
  <controlfield tag="003">CHVBK</controlfield>
  <controlfield tag="005">20180317143036.0</controlfield>
  <controlfield tag="007">cr unu---uuuuu</controlfield>
  <controlfield tag="008">170323e20110201xx      s     000 0 eng  </controlfield>
  <datafield tag="024" ind1="7" ind2="0">
   <subfield code="a">10.1007/s10714-010-1011-7</subfield>
   <subfield code="2">doi</subfield>
  </datafield>
  <datafield tag="035" ind1=" " ind2=" ">
   <subfield code="a">(NATIONALLICENCE)springer-10.1007/s10714-010-1011-7</subfield>
  </datafield>
  <datafield tag="245" ind1="0" ind2="0">
   <subfield code="a">Improving the sensitivity of future GW observatories in the 1-10Hz band: Newtonian and seismic noise</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[M. Beker, G. Cella, R. DeSalvo, M. Doets, H. Grote, J. Harms, E. Hennes, V. Mandic, D. Rabeling, J. van den Brand, C. van Leeuwen]</subfield>
  </datafield>
  <datafield tag="520" ind1="3" ind2=" ">
   <subfield code="a">The next generation gravitational wave interferometric detectors will likely be underground detectors to extend the GW detection frequency band to frequencies below the Newtonian noise limit. Newtonian noise originates from the continuous motion of the Earth's crust driven by human activity, tidal stresses and seismic motion, and from mass density fluctuations in the atmosphere. It is calculated that on Earth's surface, on a typical day, it will exceed the expected GW signals at frequencies below 10Hz. The noise will decrease underground by an unknown amount. It is important to investigate and to quantify this expected reduction and its effect on the sensitivity of future detectors, to plan for further improvement strategies. We report about some of these aspects. Analytical models can be used in the simplest scenarios to get a better qualitative and semi-quantitative understanding. As more complete modeling can be done numerically, we will discuss also some results obtained with a finite-element-based modeling tool. The method is verified by comparing its results with the results of analytic calculations for surface detectors. A key point about noise models is their initial parameters and conditions, which require detailed information about seismic motion in a real scenario. We will describe an effort to characterize the seismic activity at the Homestake mine which is currently in progress. This activity is specifically aimed to provide informations and to explore the site as a possible candidate for an underground observatory. Although the only compelling reason to put the interferometer underground is to reduce the Newtonian noise, we expect that the more stable underground environment will have a more general positive impact on the sensitivity. We will end this report with some considerations about seismic and suspension noise.</subfield>
  </datafield>
  <datafield tag="540" ind1=" " ind2=" ">
   <subfield code="a">The Author(s), 2010</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Gravitational waves</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Noises</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Beker</subfield>
   <subfield code="D">M.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Cella</subfield>
   <subfield code="D">G.</subfield>
   <subfield code="u">Istituto Nazionale di Fisica Nucleare sez. Pisa, Largo B. Pontecorvo 3, 56127, Pisa, Italy</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">DeSalvo</subfield>
   <subfield code="D">R.</subfield>
   <subfield code="u">LIGO Laboratories, California Institute of Technology, 91125, Pasadena, CA, USA</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Doets</subfield>
   <subfield code="D">M.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Grote</subfield>
   <subfield code="D">H.</subfield>
   <subfield code="u">Max-Planck-Institute for Gravitational Research (Albert Einstein Institute), Hannover, Germany</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Harms</subfield>
   <subfield code="D">J.</subfield>
   <subfield code="u">University of Minnesota, 55455, Minneapolis, MN, USA</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Hennes</subfield>
   <subfield code="D">E.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Mandic</subfield>
   <subfield code="D">V.</subfield>
   <subfield code="u">University of Minnesota, 55455, Minneapolis, MN, USA</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Rabeling</subfield>
   <subfield code="D">D.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">van den Brand</subfield>
   <subfield code="D">J.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">van Leeuwen</subfield>
   <subfield code="D">C.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="773" ind1="0" ind2=" ">
   <subfield code="t">General Relativity and Gravitation</subfield>
   <subfield code="d">Springer US; http://www.springer-ny.com</subfield>
   <subfield code="g">43/2(2011-02-01), 623-656</subfield>
   <subfield code="x">0001-7701</subfield>
   <subfield code="q">43:2&lt;623</subfield>
   <subfield code="1">2011</subfield>
   <subfield code="2">43</subfield>
   <subfield code="o">10714</subfield>
  </datafield>
  <datafield tag="856" ind1="4" ind2="0">
   <subfield code="u">https://doi.org/10.1007/s10714-010-1011-7</subfield>
   <subfield code="q">text/html</subfield>
   <subfield code="z">Onlinezugriff via DOI</subfield>
  </datafield>
  <datafield tag="908" ind1=" " ind2=" ">
   <subfield code="D">1</subfield>
   <subfield code="a">research-article</subfield>
   <subfield code="2">jats</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">856</subfield>
   <subfield code="E">40</subfield>
   <subfield code="u">https://doi.org/10.1007/s10714-010-1011-7</subfield>
   <subfield code="q">text/html</subfield>
   <subfield code="z">Onlinezugriff via DOI</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Beker</subfield>
   <subfield code="D">M.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Cella</subfield>
   <subfield code="D">G.</subfield>
   <subfield code="u">Istituto Nazionale di Fisica Nucleare sez. Pisa, Largo B. Pontecorvo 3, 56127, Pisa, Italy</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">DeSalvo</subfield>
   <subfield code="D">R.</subfield>
   <subfield code="u">LIGO Laboratories, California Institute of Technology, 91125, Pasadena, CA, USA</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Doets</subfield>
   <subfield code="D">M.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Grote</subfield>
   <subfield code="D">H.</subfield>
   <subfield code="u">Max-Planck-Institute for Gravitational Research (Albert Einstein Institute), Hannover, Germany</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Harms</subfield>
   <subfield code="D">J.</subfield>
   <subfield code="u">University of Minnesota, 55455, Minneapolis, MN, USA</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Hennes</subfield>
   <subfield code="D">E.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Mandic</subfield>
   <subfield code="D">V.</subfield>
   <subfield code="u">University of Minnesota, 55455, Minneapolis, MN, USA</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Rabeling</subfield>
   <subfield code="D">D.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">van den Brand</subfield>
   <subfield code="D">J.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">van Leeuwen</subfield>
   <subfield code="D">C.</subfield>
   <subfield code="u">Nikhef, National Institute for Subatomic Physics, P. O. Box 41182, 1009 DB, Amsterdam, The Netherlands</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">773</subfield>
   <subfield code="E">0-</subfield>
   <subfield code="t">General Relativity and Gravitation</subfield>
   <subfield code="d">Springer US; http://www.springer-ny.com</subfield>
   <subfield code="g">43/2(2011-02-01), 623-656</subfield>
   <subfield code="x">0001-7701</subfield>
   <subfield code="q">43:2&lt;623</subfield>
   <subfield code="1">2011</subfield>
   <subfield code="2">43</subfield>
   <subfield code="o">10714</subfield>
  </datafield>
  <datafield tag="900" ind1=" " ind2="7">
   <subfield code="a">Metadata rights reserved</subfield>
   <subfield code="b">Springer special CC-BY-NC licence</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="898" ind1=" " ind2=" ">
   <subfield code="a">BK010053</subfield>
   <subfield code="b">XK010053</subfield>
   <subfield code="c">XK010000</subfield>
  </datafield>
  <datafield tag="949" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="F">NATIONALLICENCE</subfield>
   <subfield code="b">NL-springer</subfield>
  </datafield>
 </record>
</collection>
