% IMPORTANT: The following is UTF-8 encoded.  This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.

@ARTICLE{Biniskos:837531,
      author       = {Biniskos, N. and Raymond, S. and Schmalzl, K. and
                      Schneidewind, A. and Voigt, J. and Georgii, R. and Hering,
                      P. and Persson, J. and Friese, K. and Brückel, T.},
      title        = {{S}pin dynamics of the magnetocaloric compound
                      {M}n{F}e$_{4}$ {S}i$_{3}$},
      journal      = {Physical review / B},
      volume       = {96},
      number       = {10},
      issn         = {2469-9950},
      address      = {Woodbury, NY},
      publisher    = {Inst.},
      reportid     = {FZJ-2017-06419},
      pages        = {104407},
      year         = {2017},
      abstract     = {The magnetic excitation spectrum of the magnetocaloric
                      compound MnFe4Si3 has been investigated by means of
                      polarized and unpolarized inelastic neutron scattering on
                      single crystals. Spectra were collected in the ferromagnetic
                      phase (TC≈305K), as well as in the paramagnetic state, in
                      order to understand the nature of the magnetism in MnFe4Si3.
                      Spin-wave measurements at 1.5 K reveal a strong anisotropy
                      of the magnetic exchange interactions along the (h00) and
                      (00l) reciprocal directions of the hexagonal system, which
                      also manifests itself in the q-dependent linewidths in the
                      paramagnetic state. The correlation lengths indicate a
                      short-range order, while the average linewidth is of the
                      order of kBTC pointing to a behavior typical of many
                      ferromagnets. In addition, the in- and out-of-plane spin
                      fluctuations are found to be isotropic around TC and can be
                      suppressed by a magnetic field of 2 T.},
      cin          = {JCNS-2 / PGI-4 / JARA-FIT / JCNS-ILL / JCNS (München) ;
                      Jülich Centre for Neutron Science JCNS (München) ;
                      JCNS-FRM-II},
      ddc          = {530},
      cid          = {I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
                      $I:(DE-82)080009_20140620$ / I:(DE-Juel1)JCNS-ILL-20110128 /
                      I:(DE-Juel1)JCNS-FRM-II-20110218},
      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 /
                      EXP:(DE-MLZ)PANDA-20140101 / EXP:(DE-MLZ)MIRA-20140101},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000409429300005},
      doi          = {10.1103/PhysRevB.96.104407},
      url          = {https://juser.fz-juelich.de/record/837531},
}