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@ARTICLE{Uddin:1007614,
      author       = {Uddin, M. Shuza and Basunia, M. Shamsuzzoha and Spahn, Ingo
                      and Spellerberg, Stefan and Khan, Rahat and Uddin, M. Mezbah
                      and Bernstein, Lee A. and Neumaier, Bernd and Qaim, Syed M.},
      title        = {{C}ross sections and calculated yields of some
                      radionuclides of yttrium, strontium and rubidium formed in
                      proton-induced reactions on enriched strontium-86:
                      possibility of production of 85g{S}r, 83{R}b and 82m{R}b in
                      no-carrier-added form},
      journal      = {Radiochimica acta},
      volume       = {111},
      number       = {2},
      issn         = {0033-8230},
      address      = {Berlin},
      publisher    = {De Gruyter},
      reportid     = {FZJ-2023-02113},
      pages        = {81 - 90},
      year         = {2023},
      abstract     = {Cross sections of the 86Sr(p,3n)84mY, 86Sr(p,αn)82mRb, and
                      86Sr(p,x)85gSr reactions were measured from their respective
                      thresholds up to 16.2 MeV and from 23.0 to 44.1 MeV at FZJ,
                      and from 14.3 to 24.5 MeV at LBNL, using $96.4\%$ enriched
                      86SrCO3 as target material. Thin targets prepared by
                      sedimentation were irradiated with protons in a
                      stacked-form, and the induced radioactivity was measured by
                      high-resolution γ-ray spectrometry. Nuclear model
                      calculations based on the code TALYS reproduced our
                      experimental cross section data well. From the excitation
                      functions, the integral yields of the above three
                      radionuclides were calculated. The yield of 85gSr via the
                      natSr(n,γ)process was also measured using the TRIGA Mark-II
                      reactor at AERE, Savar. A comparison of the reactor and
                      cyclotron production of carrier-added 85gSr is given. The
                      production possibilities of the three investigated
                      radionuclides in no-carrier-added forms at a 30 MeV
                      cyclotron via new routes are discussed.},
      cin          = {INM-5},
      ddc          = {610},
      cid          = {I:(DE-Juel1)INM-5-20090406},
      pnm          = {5253 - Neuroimaging (POF4-525)},
      pid          = {G:(DE-HGF)POF4-5253},
      typ          = {PUB:(DE-HGF)16},
      UT           = {WOS:000891184000001},
      doi          = {10.1515/ract-2022-0086},
      url          = {https://juser.fz-juelich.de/record/1007614},
}