2021
DOI: 10.1016/j.nds.2021.11.002
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Nuclear Data Sheets for A=64

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Cited by 11 publications
(3 citation statements)
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“…The decay data have conventionally received more attention with regard to their standardisation, and detailed evaluated mass decay chains are available for the above-mentioned five radionuclides (Junde et al, 2005;Nichols et al, 2012;Browne and Tuli, 2013;Zuber and Singh, 2015;Singh and Chen, 2021). The data given in Table 1 are all standardised, especially the halflives, the γ-ray energies and their intensities, as well as the β + (β -) energies and their intensities.…”
Section: Standardised Decay Data: Discrepancies and Deficienciesmentioning
confidence: 99%
“…The decay data have conventionally received more attention with regard to their standardisation, and detailed evaluated mass decay chains are available for the above-mentioned five radionuclides (Junde et al, 2005;Nichols et al, 2012;Browne and Tuli, 2013;Zuber and Singh, 2015;Singh and Chen, 2021). The data given in Table 1 are all standardised, especially the halflives, the γ-ray energies and their intensities, as well as the β + (β -) energies and their intensities.…”
Section: Standardised Decay Data: Discrepancies and Deficienciesmentioning
confidence: 99%
“…This radioisotope presents a complex decay scheme, which includes electron capture, beta minus, and positron emissions. The low-energy positrons emitted (17.49%, max 0.653 MeV, mean 0.278 MeV) are excellent for positron emission tomography imaging, especially due to a spatial resolution similar to fluorine-18, as determined by comparable average free travel distance of positrons (0.70 mm in the case of copper-64 and 0.69 mm in the case of fluorine-18) [ 1 , 2 ]. The lack of abundant gamma emissions (only 0.47%, 1.346 MeV) is also an advantage since they can cause interferences that impact the image quality, as in the case of other non-pure positron emitters such as bromine-76, yttrium-86, rubidium-82, and iodine-124 [ 3 ].…”
Section: Introductionmentioning
confidence: 99%
“…The β − emission (38.48%, max 0.579 MeV, mean 0.190 MeV) offers the possibility for targeted radionuclide therapy with a highly localised dose, in situ visualised by the means of β + (PET). Additionally, the electron capture events determine the emission of Auger electrons (Auger L 0.84 keV, 58.0% and Auger K 6.54 keV, 22.62%) which increases the radiotoxicity of the radioisotope when delivered inside the targeted cells, in particular when the emitting radioisotope is trapped in the cell nucleus [ 1 , 4 ].…”
Section: Introductionmentioning
confidence: 99%