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@ARTICLE{Muoz:819431,
      author       = {Muñoz, A. and Monge, M. A. and Savoini, B. and Pareja, R.
                      and Radulescu, A.},
      title        = {{SANS} characterization of particle dispersions in {W}-{T}i
                      and {W}-{V} alloys},
      journal      = {International journal of refractory metals $\&$ hard
                      materials},
      volume       = {61},
      issn         = {0263-4368},
      address      = {Amsterdam [u.a.]},
      publisher    = {Elsevier Science},
      reportid     = {FZJ-2016-05095},
      pages        = {173 - 178},
      year         = {2016},
      abstract     = {SEM analyses of W-Ti and W-V alloys produced by a powder
                      metallurgy route have revealed the presence of Ti or V pools
                      with different sizes and shapes. The larger pools have sizes
                      between ~ 0.3 and several microns and are embedded between
                      the matrix grains. The smaller Ti-rich (V-rich) particles,
                      with sizes below ~ 0.3 μm, are spherical and are dispersed
                      inside the matrix grains. The characteristics of the second
                      phase nanoparticles have been studied using the SANS
                      technique. The scattering curves have been analyzed in terms
                      of a polydisperse particle system following the Beaucage
                      approach, and the maximum entropy method to obtain the
                      particle size distributions. Beaucage analyses suggest the
                      presence of two particle populations, characterized by radii
                      of gyration from 50 to 80 Å (population I) and between 650
                      and 760 Å (population II). The volume distribution obtained
                      by the maximum entropy approach reveals a prominent peak
                      with particle diameter of 60 Å and ~ 70 Å for the W-Ti and
                      W-V alloys, respectively. Secondary peaks in the size range
                      100–300 Å could be associated with the particle
                      population with the larger radius of gyration.},
      cin          = {JCNS (München) ; Jülich Centre for Neutron Science JCNS
                      (München) ; JCNS-FRM-II / Neutronenstreuung ; JCNS-1},
      ddc          = {670},
      cid          = {I:(DE-Juel1)JCNS-FRM-II-20110218 /
                      I:(DE-Juel1)JCNS-1-20110106},
      pnm          = {6G15 - FRM II / MLZ (POF3-6G15) / 6G4 - Jülich Centre for
                      Neutron Research (JCNS) (POF3-623)},
      pid          = {G:(DE-HGF)POF3-6G15 / G:(DE-HGF)POF3-6G4},
      experiment   = {EXP:(DE-MLZ)KWS2-20140101},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000388048300023},
      doi          = {10.1016/j.ijrmhm.2016.09.009},
      url          = {https://juser.fz-juelich.de/record/819431},
}