% 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{Uddin:824580,
      author       = {Uddin, M. S. and Sudár, S. and Spahn, I. and Shariff, M.
                      A. and Qaim, S. M.},
      title        = {{E}xcitation function of the {N}i $^{60}$ ( p , γ ) {C}u
                      $^{61}$ reaction from threshold to 16 {M}e{V}},
      journal      = {Physical review / C},
      volume       = {93},
      number       = {4},
      issn         = {2469-9985},
      address      = {Woodbury, NY},
      publisher    = {Inst.},
      reportid     = {FZJ-2016-07150},
      pages        = {044606},
      year         = {2016},
      abstract     = {Excitation function of the reaction Ni60(p,γ)Cu61 was
                      measured via the activation technique in the energy range of
                      1.3-16.0 MeV using a low-energy accelerator and a small
                      cyclotron. The results are comparable to those previously
                      obtained via prompt γ counting. In addition excitation
                      functions of the more common competing Ni60(p,n)Cu60 and
                      Ni60(p,α)Co57 reactions were also measured. Theoretical
                      calculations on proton-induced reactions on Ni60 were
                      performed using the nuclear model code talys. The results
                      suggest that near the threshold of the reaction the compound
                      nucleus mechanism dominates. Thereafter the contribution of
                      direct interactions becomes rather strong, especially
                      between 4 and 6 MeV, i.e., just below the threshold of the
                      Ni60(p,n)Cu60 reaction. The cross section at the maximum of
                      the excitation function of each of the three reactions,
                      namely, Ni60(p,γ)Cu61,Ni60(p,n)Cu60, and Ni60(p,α)Co57,
                      amounts to 2, 320, and 85 mb, respectively. The (p,n)
                      reaction is thus the most commonly occurring process, and
                      the (p,γ) reaction is the weakest, possibly due to higher
                      probability of particle emission than γ-ray emission from
                      the highly excited intermediate nucleus Cu61 formed in the
                      interaction of a proton with the target nucleus Ni60.},
      cin          = {INM-5},
      ddc          = {530},
      cid          = {I:(DE-Juel1)INM-5-20090406},
      pnm          = {573 - Neuroimaging (POF3-573)},
      pid          = {G:(DE-HGF)POF3-573},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000373770300007},
      doi          = {10.1103/PhysRevC.93.044606},
      url          = {https://juser.fz-juelich.de/record/824580},
}