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@ARTICLE{Uddin:1042400,
author = {Uddin, M. Shuza and Spahn, Ingo and Basunia, M. Shamsuzzoha
and Voyles, Andrew S. and Spellerberg, Stefan and Hussain,
Mazhar and Sudár, Sándor and Bernstein, Lee A. and
Neumaier, Bernd and Qaim, Syed M.},
title = {{A}n overview of production routes of the non-standard
positron emitter 86g{Y} with emphasis on a comparative
analysis of the 86{S}r(p,n)- and 86{S}r(d,2n)-reactions},
journal = {Radiochimica acta},
volume = {113},
number = {5},
issn = {0033-8230},
address = {Berlin},
publisher = {De Gruyter},
reportid = {FZJ-2025-02554},
pages = {345 - 351},
year = {2025},
abstract = {A very brief overview of the hitherto investigated
production routes of 86gY is given, and a comparative
analysis of its production via the two low-energy reactions,
namely (p,n) and (d,2n) on $96.4\%$ enriched 86Sr as target
material, is presented. Based on our recent cross- section
measurements, the calculated yields of 86gY via the two
reactions were compared, and the levels of co-produced
isotopic impurities were estimated. At low-energy medical
cyclotrons (Ep < 20 MeV; Ed <10 MeV) the use of the (p, n)
reaction is superior, both in terms of the yield of 86gY and
the levels of radionuclidic impurities. At medium-sized
cyclotrons, on the other hand, the (d, 2n) reaction leads to
higher yield of 86gY, but the level of radionuclidic
impurities is also higher. The method of choice for
production of 86gY thus remains the (p,n) reaction on
enriched 86Sr.},
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:001442433300001},
doi = {10.1515/ract-2024-0375},
url = {https://juser.fz-juelich.de/record/1042400},
}