<?xml version="1.0" encoding="UTF-8"?>
<collection xmlns="http://www.loc.gov/MARC21/slim">
 <record>
  <leader>     caa a22        4500</leader>
  <controlfield tag="001">397504608</controlfield>
  <controlfield tag="003">CHVBK</controlfield>
  <controlfield tag="005">20180308164541.0</controlfield>
  <controlfield tag="007">cr unu---uuuuu</controlfield>
  <controlfield tag="008">161202e19950501xx      s     000 0 eng  </controlfield>
  <datafield tag="024" ind1="7" ind2="0">
   <subfield code="a">10.1093/oxfordjournals.rpd.a082652</subfield>
   <subfield code="2">doi</subfield>
  </datafield>
  <datafield tag="024" ind1="7" ind2="0">
   <subfield code="a">0144-8420</subfield>
   <subfield code="2">pii</subfield>
  </datafield>
  <datafield tag="035" ind1=" " ind2=" ">
   <subfield code="a">(NATIONALLICENCE)oxford-10.1093/oxfordjournals.rpd.a082652</subfield>
  </datafield>
  <datafield tag="245" ind1="0" ind2="0">
   <subfield code="a">Determination of the Neutron Angular Response Using a Single Etched Track Detector</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[K. Turek, J. Bednár, E. Piesch]</subfield>
  </datafield>
  <datafield tag="520" ind1="3" ind2=" ">
   <subfield code="a">A method for the determination of the neutron angular response as a function of incident angle is described using only one exposure of a single bent plastic detector strip in a half cylindrical geometry. After etching, the detector surface is scanned along the centre line in parallel narrow fields. On the basis of the equation derived from the irradiation geometry the distance of each field can be correlated to the angle of neutron incidence a. Thus, the track density values correspond to all angles from O o to 90 o. The application of the least square fit method provides: (a) correction in case of an inaccurate irradiation geometry, (b) the proper 'source-detector' distance correction of the neutron fluence, and (c) a method for estimating the angular response as a function of angle a of neutron incidence using the simple empirical equation p (a)=a+b X cos (2a+p).</subfield>
  </datafield>
  <datafield tag="540" ind1=" " ind2=" ">
   <subfield code="a">Radiation Protection Dosimetry</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Turek</subfield>
   <subfield code="D">K.</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Bednár</subfield>
   <subfield code="D">J.</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Piesch</subfield>
   <subfield code="D">E.</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="773" ind1="0" ind2=" ">
   <subfield code="t">Radiation Protection Dosimetry</subfield>
   <subfield code="d">Oxford University Press</subfield>
   <subfield code="g">59/3(1995-05-01), 205-211</subfield>
   <subfield code="x">0144-8420</subfield>
   <subfield code="q">59:3&lt;205</subfield>
   <subfield code="1">1995</subfield>
   <subfield code="2">59</subfield>
   <subfield code="o">rpd</subfield>
  </datafield>
  <datafield tag="856" ind1="4" ind2="0">
   <subfield code="u">https://doi.org/10.1093/oxfordjournals.rpd.a082652</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/10.1093/oxfordjournals.rpd.a082652</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">Turek</subfield>
   <subfield code="D">K.</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">Bednár</subfield>
   <subfield code="D">J.</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">Piesch</subfield>
   <subfield code="D">E.</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">Radiation Protection Dosimetry</subfield>
   <subfield code="d">Oxford University Press</subfield>
   <subfield code="g">59/3(1995-05-01), 205-211</subfield>
   <subfield code="x">0144-8420</subfield>
   <subfield code="q">59:3&lt;205</subfield>
   <subfield code="1">1995</subfield>
   <subfield code="2">59</subfield>
   <subfield code="o">rpd</subfield>
  </datafield>
  <datafield tag="900" ind1=" " ind2="7">
   <subfield code="a">Metadata rights reserved</subfield>
   <subfield code="b">CC BY-NC-4.0</subfield>
   <subfield code="u">http://creativecommons.org/licenses/by-nc/4.0</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-oxford</subfield>
  </datafield>
 </record>
</collection>
