% 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:906022,
author = {Uddin, M. Shuza and Qaim, Syed M. and Scholten, Bernhard
and Basunia, M. Shamsuzzoha and Bernstein, Lee A. and Spahn,
Ingo and Neumaier, Bernd},
title = {{P}ositron {E}mission {I}ntensity in the {D}ecay of 86g{Y}
for {U}se in {D}osimetry {S}tudies},
journal = {Molecules},
volume = {27},
number = {3},
issn = {1420-3049},
address = {Basel},
publisher = {MDPI},
reportid = {FZJ-2022-01187},
pages = {768 -},
year = {2022},
abstract = {The β+-emitting radionuclide 86gY (t1/2 = 14.7 h) forms a
matched-pair with the β−-emitting therapeutic
radionuclide 90Y (t1/2 = 2.7 d) for theranostic application
in medicine. This approach demands a precise knowledge of
the positron emission probability of the PET nuclide which
was until recently rather uncertain for 86gY. In this work,
an 86gY source of high radionuclidic purity was prepared and
a direct measurement of the positron emission intensity per
100 decay of the parent (hereafter “positron emission
intensity”) was performed using high-resolution HPGe
detector γ-ray spectroscopy. The electron capture intensity
was also determined as an additional check by measuring the
Kα and Kβ X-rays of energies 14.1 and 15.8 keV,
respectively, using a low energy HPGe detector. From those
measurements, normalized values of 27.2 ± $2.0\%$ for
β+-emission and 72.8 ± $2.0\%$ for EC were obtained. These
results are in excellent agreement with values recently
reported in the literature based on a detailed decay scheme
study.},
cin = {INM-5},
ddc = {540},
cid = {I:(DE-Juel1)INM-5-20090406},
pnm = {5253 - Neuroimaging (POF4-525)},
pid = {G:(DE-HGF)POF4-5253},
typ = {PUB:(DE-HGF)16},
pubmed = {35164033},
UT = {WOS:000760507600001},
doi = {10.3390/molecules27030768},
url = {https://juser.fz-juelich.de/record/906022},
}