% 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{Bouaziz:811714,
      author       = {Bouaziz, Juba and Lounis, Samir and Blügel, Stefan and
                      Ishida, Hiroshi},
      title        = {{M}icroscopic theory of the residual surface resistivity of
                      {R}ashba electrons},
      journal      = {Physical review / B},
      volume       = {94},
      number       = {4},
      issn         = {2469-9950},
      address      = {College Park, Md.},
      publisher    = {APS},
      reportid     = {FZJ-2016-04098},
      pages        = {045433},
      year         = {2016},
      abstract     = {A microscopic expression of the residual electrical
                      resistivity tensor is derived in linear response theory for
                      Rashba electrons scattering at a magnetic impurity with
                      cylindrical or noncylindrical potential. The behavior of the
                      longitudinal and transversal residual resistivity is
                      obtained analytically and computed for an Fe impurity at the
                      Au(111) surface. We studied the evolution of the resistivity
                      tensor elements as a function of the Rashba spin-orbit
                      strength and the magnetization direction of the impurity. We
                      found that the absolute values of longitudinal resistivity
                      reduce with increasing spin-orbit strength of the substrate
                      and that the scattering of the conduction electrons at
                      magnetic impurities with magnetic moments pointing in
                      directions not perpendicular to the surface plane produce a
                      planar Hall effect and an anisotropic magnetoresistance even
                      if the impurity carries no spin-orbit interaction.
                      Functional forms are provided describing the anisotropy of
                      the planar Hall effect and the anisotropic magnetoresistance
                      with respect to the direction of the impurity moment. In the
                      limit of no spin-orbit interaction and a nonmagnetic
                      impurity of cylindrical symmetry, the expression of the
                      residual resistivity of a two-dimensional electron gas has
                      the same simplicity and form as for the three-dimensional
                      electron gas [J. Friedel, J. Nuovo. Cim. 7, 287 (1958)] and
                      can also be expressed in terms of scattering phase shifts},
      cin          = {IAS-1 / PGI-1 / JARA-FIT / JARA-HPC},
      ddc          = {530},
      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:000381484900003},
      doi          = {10.1103/PhysRevB.94.045433},
      url          = {https://juser.fz-juelich.de/record/811714},
}