<?xml version="1.0" encoding="UTF-8"?>
<collection xmlns="http://www.loc.gov/MARC21/slim">
 <record>
  <leader>     caa a22        4500</leader>
  <controlfield tag="001">463224590</controlfield>
  <controlfield tag="003">CHVBK</controlfield>
  <controlfield tag="005">20180405153223.0</controlfield>
  <controlfield tag="007">cr unu---uuuuu</controlfield>
  <controlfield tag="008">170326e20070401xx      s     000 0 eng  </controlfield>
  <datafield tag="024" ind1="7" ind2="0">
   <subfield code="a">10.1007/s10853-006-1212-3</subfield>
   <subfield code="2">doi</subfield>
  </datafield>
  <datafield tag="035" ind1=" " ind2=" ">
   <subfield code="a">(NATIONALLICENCE)springer-10.1007/s10853-006-1212-3</subfield>
  </datafield>
  <datafield tag="245" ind1="0" ind2="0">
   <subfield code="a">Quantitative analysis for kinetics of reactive diffusion in the Fe-Cr system</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[M. Kajihara, T. Yamashina]</subfield>
  </datafield>
  <datafield tag="520" ind1="3" ind2=" ">
   <subfield code="a">In the binary Fe-Cr system, the γ phase with the face-centered cubic structure becomes a stable intermediate phase sandwiched between the Fe-rich α1 and Cr-rich α2 phases with the body-centered cubic structure in the temperature range between T=1,119 and 1,185K. Within this temperature range, the reactive diffusion between the α1 and α2 phases was experimentally observed by Nishizawa and Chiba (Nishizawa and Chiba (1970) J Jap Inst Met 34:629). In their experiment, Fe/Cr diffusion couples were annealed at T=1,123-1,163K for up to 600h. Although the γ phase should be formed due to annealing, it was not recognized in any annealed diffusion couples. The mathematical model reported in a previous study (2004 Acta Mater 52:1193) was used to analyze their experimental results theoretically. In order to provide the boundary conditions for the analysis, the phase diagram in the Fe-Cr system was computed by a CALPHAD technique. The analysis indicates that the γ phase is actually produced at the interface but its thickness is less than 1μm even after annealing at T=1,163K for 600h. Thus, the γ phase is practically invisible under their experimental conditions. The analysis provides the experimental conditions for the γ phase to grow to observable thicknesses.</subfield>
  </datafield>
  <datafield tag="540" ind1=" " ind2=" ">
   <subfield code="a">Springer Science+Business Media, LLC, 2006</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Kajihara</subfield>
   <subfield code="D">M.</subfield>
   <subfield code="u">Department of Materials Science and Engineering, Tokyo Institute of Technology, 226-8502, Midori-ku, Yokohama, Japan</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Yamashina</subfield>
   <subfield code="D">T.</subfield>
   <subfield code="u">Graduate School, Tokyo Institute of Technology, 226-8502, Midori-ku, Yokohama, Japan</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="773" ind1="0" ind2=" ">
   <subfield code="t">Journal of Materials Science</subfield>
   <subfield code="d">Kluwer Academic Publishers-Plenum Publishers; http://www.springer-ny.com</subfield>
   <subfield code="g">42/7(2007-04-01), 2432-2442</subfield>
   <subfield code="x">0022-2461</subfield>
   <subfield code="q">42:7&lt;2432</subfield>
   <subfield code="1">2007</subfield>
   <subfield code="2">42</subfield>
   <subfield code="o">10853</subfield>
  </datafield>
  <datafield tag="856" ind1="4" ind2="0">
   <subfield code="u">https://doi.org/10.1007/s10853-006-1212-3</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/s10853-006-1212-3</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">Kajihara</subfield>
   <subfield code="D">M.</subfield>
   <subfield code="u">Department of Materials Science and Engineering, Tokyo Institute of Technology, 226-8502, Midori-ku, Yokohama, Japan</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">Yamashina</subfield>
   <subfield code="D">T.</subfield>
   <subfield code="u">Graduate School, Tokyo Institute of Technology, 226-8502, Midori-ku, Yokohama, Japan</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">Journal of Materials Science</subfield>
   <subfield code="d">Kluwer Academic Publishers-Plenum Publishers; http://www.springer-ny.com</subfield>
   <subfield code="g">42/7(2007-04-01), 2432-2442</subfield>
   <subfield code="x">0022-2461</subfield>
   <subfield code="q">42:7&lt;2432</subfield>
   <subfield code="1">2007</subfield>
   <subfield code="2">42</subfield>
   <subfield code="o">10853</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>
