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@ARTICLE{Fenske:255498,
      author       = {Fenske, Jochen and Lott, Dieter and Tartakovskaya, Elena V.
                      and Lee, Hwachol and LeClair, Patrick R. and Mankey, Gary J.
                      and Schmidt, Wolfgang and Schmalzl, Karin and Klose, Frank
                      and Schreyer, Andreas},
      title        = {{M}agnetic order and phase transitions in {F}e $_{50}$ {P}t
                      $_{50– x}$ {R}h $_{x}$},
      journal      = {Journal of applied crystallography},
      volume       = {48},
      number       = {4},
      issn         = {1600-5767},
      address      = {Copenhagen},
      publisher    = {Munksgaard},
      reportid     = {FZJ-2015-05660},
      pages        = {1142 - 1158},
      year         = {2015},
      abstract     = {Polarized and unpolarized neutron diffraction techniques
                      have been applied to study the temperature-dependent
                      magnetic and structural properties of four 200 nm-thick
                      Fe50Pt50-xRhx films with x = 5, x = 10, x = 17.5 and x = 25.
                      Similar to the bulk system, an antiferromagnetic to
                      ferromagnetic transition can be found in the films with
                      decreasing Rh concentration. The application of structure
                      factor calculations enables one to determine the microscopic
                      magnetic configuration of the different films as a function
                      of temperature and Rh concentration. The developed models
                      indicate a magnetic transition from a dominant
                      antiferromagnetic order in the out-of-plane direction to a
                      dominant ferromagnetic order in the in-plane direction with
                      decreasing Rh concentration. The different magnetic
                      configurations can theoretically be described by a
                      phenomenological model which includes a two-ion and a
                      one-ion interaction Hamiltonian term with different
                      temperature dependencies of the anisotropy constants.},
      cin          = {JCNS-2 / PGI-4 / JARA-FIT / JCNS-ILL},
      ddc          = {540},
      cid          = {I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
                      $I:(DE-82)080009_20140620$ / I:(DE-Juel1)JCNS-ILL-20110128},
      pnm          = {144 - Controlling Collective States (POF3-144) / 524 -
                      Controlling Collective States (POF3-524) / 6212 - Quantum
                      Condensed Matter: Magnetism, Superconductivity (POF3-621) /
                      6213 - Materials and Processes for Energy and Transport
                      Technologies (POF3-621) / 6G4 - Jülich Centre for Neutron
                      Research (JCNS) (POF3-623)},
      pid          = {G:(DE-HGF)POF3-144 / G:(DE-HGF)POF3-524 /
                      G:(DE-HGF)POF3-6212 / G:(DE-HGF)POF3-6213 /
                      G:(DE-HGF)POF3-6G4},
      experiment   = {EXP:(DE-Juel1)ILL-IN12-20150421},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000358791900018},
      doi          = {10.1107/S1600576715011462},
      url          = {https://juser.fz-juelich.de/record/255498},
}