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@ARTICLE{Barashenkov:59102,
      author       = {Barashenkov, I. V. and Woodford, S.R. and Zemlyanaya, E.
                      V.},
      title        = {{I}nteractions of parametrically driven dark solitons. {I}.
                      {N}éel-{N}éel and {B}loch-{B}loch interactions},
      journal      = {Physical review / E},
      volume       = {75},
      number       = {2},
      issn         = {1539-3755},
      address      = {College Park, Md.},
      publisher    = {APS},
      reportid     = {PreJuSER-59102},
      pages        = {026604},
      year         = {2007},
      note         = {Record converted from VDB: 12.11.2012},
      abstract     = {We study interactions between the dark solitons of the
                      parametrically driven nonlinear Schrodinger equation, Eq.
                      (1). When the driving strength, h, is below root
                      gamma(2)+1/9, two well-separated Neel walls may repel or
                      attract. They repel if their initial separation 2z(0) is
                      larger than the distance 2z(u) between the constituents in
                      the unstable stationary complex of two walls. They attract
                      and annihilate if 2z(0) is smaller than 2z(u). Two Neel
                      walls with h lying between root gamma(2)+1/9 and a threshold
                      driving strength h(sn) attract for 2z(0)< 2z(u) and evolve
                      into a stable stationary bound state for 2z(0)> 2z(u).
                      Finally, the Neel walls with h greater than h(sn) attract
                      and annihilate-irrespective of their initial separation. Two
                      Bloch walls of opposite chiralities attract, while Bloch
                      walls of like chiralities repel-except near the critical
                      driving strength, where the difference between the
                      like-handed and oppositely handed walls becomes negligible.
                      In this limit, similarly handed walls at large separations
                      repel while those placed at shorter distances may start
                      moving in the same direction or transmute into an oppositely
                      handed pair and attract. The collision of two Bloch walls or
                      two nondissipative Neel walls typically produces a quiescent
                      or moving breather.},
      keywords     = {J (WoSType)},
      cin          = {IFF-1},
      ddc          = {530},
      cid          = {I:(DE-Juel1)VDB781},
      pnm          = {Kondensierte Materie},
      pid          = {G:(DE-Juel1)FUEK414},
      shelfmark    = {Physics, Fluids $\&$ Plasmas / Physics, Mathematical},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000244532000049},
      doi          = {10.1103/PhysRevE.75.026604},
      url          = {https://juser.fz-juelich.de/record/59102},
}