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@ARTICLE{FarwickzumHagen:825422,
      author       = {Farwick zum Hagen, Ferdinand H. and Zimmermann, Domenik M.
                      and Silva, Caio C. and Schlueter, Christoph and Atodiresei,
                      Nicolae and Jolie, Wouter and Martínez-Galera, Antonio J.
                      and Dombrowski, Daniela and Schröder, Ulrike A. and Will,
                      Moritz and Lazić, Predrag and Caciuc, Vasile and Blügel,
                      Stefan and Lee, Tien-Lin and Michely, Thomas and Busse,
                      Carsten},
      title        = {{S}tructure and {G}rowth of {H}exagonal {B}oron {N}itride
                      on {I}r(111)},
      journal      = {ACS nano},
      volume       = {10},
      number       = {12},
      issn         = {1936-086X},
      address      = {Washington, DC},
      publisher    = {Soc.},
      reportid     = {FZJ-2016-07885},
      pages        = {11012–11026},
      year         = {2016},
      abstract     = {Using the X-ray standing wave method, scanning tunneling
                      microscopy, low energy electron diffraction, and density
                      functional theory, we precisely determine the lateral and
                      vertical structure of hexagonal boron nitride on Ir(111).
                      The moiré superstructure leads to a periodic arrangement of
                      strongly chemisorbed valleys in an otherwise rather flat,
                      weakly physisorbed plane. The best commensurate
                      approximation of the moiré unit cell is (12 × 12) boron
                      nitride cells resting on (11 × 11) substrate cells, which
                      is at variance with several earlier studies. We uncover the
                      existence of two fundamentally different mechanisms of layer
                      formation for hexagonal boron nitride, namely, nucleation
                      and growth as opposed to network formation without
                      nucleation. The different pathways are linked to different
                      distributions of rotational domains, and the latter enables
                      selection of a single orientation only.},
      cin          = {IAS-1 / PGI-1 / JARA-FIT / JARA-HPC},
      ddc          = {540},
      cid          = {I:(DE-Juel1)IAS-1-20090406 / I:(DE-Juel1)PGI-1-20110106 /
                      $I:(DE-82)080009_20140620$ / $I:(DE-82)080012_20140620$},
      pnm          = {142 - Controlling Spin-Based Phenomena (POF3-142) / 143 -
                      Controlling Configuration-Based Phenomena (POF3-143)},
      pid          = {G:(DE-HGF)POF3-142 / G:(DE-HGF)POF3-143},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000391079700045},
      doi          = {10.1021/acsnano.6b05819},
      url          = {https://juser.fz-juelich.de/record/825422},
}