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@ARTICLE{Gonzalez:280646,
      author       = {Gonzalez, Jesus and Jähnert, Kevin and Speer, Kerstin and
                      Liu, Limeng and Räthel, Jan and Knapp, Michael and
                      Ehrenberg, Helmut and Bram, Martin and Guillon, Olivier},
      title        = {{E}ffect of {I}nternal {C}urrent {F}low {D}uring the
                      {S}intering of {Z}irconium {D}iboride by {F}ield {A}ssisted
                      {S}intering {T}echnology},
      journal      = {Journal of the American Ceramic Society},
      volume       = {99},
      number       = {1},
      issn         = {0002-7820},
      address      = {Oxford [u.a.]},
      publisher    = {Wiley-Blackwell},
      reportid     = {FZJ-2016-00411},
      pages        = {35 - 42},
      year         = {2016},
      abstract     = {Effect of electric current on sintering behavior and
                      microstructure evolution of zirconium diboride (ZrB2) was
                      investigated using three different configurations of Field
                      Assisted Sintering Technology/Spark Plasma Sintering. The
                      current flow through the ZrB2 compact was controlled by
                      modifying the interface between the graphite punches and the
                      electrical conductive powder. Boron nitride discs, graphite
                      foils or direct contact with the graphite punches were the
                      three different interfaces used in order to deflect, conduct
                      or promote, respectively, the current during the sintering
                      process of the electrically conductive ZrB2 ceramics. The
                      current flow during the sintering process triggered the
                      elimination/reduction in B2O3, leading to faster diffusion
                      rates at high temperatures and limiting the formation of B4C
                      secondary phase. This allows to control the final density,
                      grain size (from 19.6 to 43.2 μm) and secondary phase
                      formation (from 5.95 to 11.61 $vol\%)$ as well as the
                      electrical resistivity (from 7.7 to 9.4 μΩ·cm) of the
                      specimens.},
      cin          = {IEK-1 / JARA-ENERGY},
      ddc          = {660},
      cid          = {I:(DE-Juel1)IEK-1-20101013 / $I:(DE-82)080011_20140620$},
      pnm          = {899 - ohne Topic (POF3-899)},
      pid          = {G:(DE-HGF)POF3-899},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000368076800007},
      doi          = {10.1111/jace.13931},
      url          = {https://juser.fz-juelich.de/record/280646},
}