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@ARTICLE{Cermak:189293,
      author       = {Cermak, Petr and Prokeš, Karel and Ouladdiaf, Bachir and
                      Boehm, Martin and Kratochvílová, Marie and Javorský,
                      Pavel},
      title        = {{M}agnetic structures in the magnetic phase diagram of
                      {H}o$_2${R}h{I}n$_8$},
      journal      = {Physical review / B},
      volume       = {91},
      number       = {14},
      issn         = {1098-0121},
      address      = {College Park, Md.},
      publisher    = {APS},
      reportid     = {FZJ-2015-02471},
      pages        = {144404},
      year         = {2015},
      abstract     = {The magnetic phase diagram of the tetragonal Ho2RhIn8
                      compound has similar features to many related systems,
                      revealing a zero magnetic field AF1 and a field-induced AF2
                      phases. Details of the magnetic order in the AF2 phase were
                      not reported yet for any of the related compounds. In
                      addition, only the Ho2RhIn8 phase diagram contains a small
                      region of the incommensurate zero-field AF3 phase. We have
                      performed a number of neutron diffraction experiments on
                      single crystals of Ho2RhIn8 using several diffractometers
                      including experiments in both horizontal and vertical
                      magnetic fields up to 4 T. We present details of the
                      magnetic structures in all magnetic phases of the rich phase
                      diagram of Ho2RhIn8. The Ho magnetic moments point along the
                      tetragonal c axis in every phase. The ground-state AF1 phase
                      is characterized by propagation vector k=(1/2,0,0). The more
                      complex ferrimagnetic AF2 phase is described by four
                      propagation vectors
                      k0=(0,0,0),k1=(1/2,0,0),k2=(0,1/2,1/2),k3=(1/2,1/2,1/2). The
                      magnetic structure in the AF3 phase is incommensurate with
                      kAF3=(0.5,δ,0). Our results are consistent with theoretical
                      calculations based on crystal field theory.},
      cin          = {JCNS (München) ; Jülich Centre for Neutron Science JCNS
                      (München) ; JCNS-FRM-II / JCNS-2},
      ddc          = {530},
      cid          = {I:(DE-Juel1)JCNS-FRM-II-20110218 /
                      I:(DE-Juel1)JCNS-2-20110106},
      pnm          = {524 - Controlling Collective States (POF3-524) / 6212 -
                      Quantum Condensed Matter: Magnetism, Superconductivity
                      (POF3-621) / 6G15 - FRM II / MLZ (POF3-6G15) / 6G4 - Jülich
                      Centre for Neutron Research (JCNS) (POF3-623)},
      pid          = {G:(DE-HGF)POF3-524 / G:(DE-HGF)POF3-6212 /
                      G:(DE-HGF)POF3-6G15 / G:(DE-HGF)POF3-6G4},
      experiment   = {EXP:(DE-MLZ)External-20140101},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000352255600003},
      doi          = {10.1103/PhysRevB.91.144404},
      url          = {https://juser.fz-juelich.de/record/189293},
}