1976
DOI: 10.1088/0305-4616/2/5/009
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Internal bremsstrahlung spectral shapes of45Ca and3aS

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Cited by 8 publications
(1 citation statement)
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“…Although there is a sufficient difference between the β energies emitted by 3 H (E av = 5.7 keV, E max = 18.6 keV) and 45 Ca (E av = 77 keV, E max = 252 keV), the internal bremsstrahlung effect of the 45 Ca spectra (Babu et al, 1976) emitted in the β-decay may lead to sufficient tailing of the peak. This may lead to fictitious peak area measurement in the 3 H window and hence lead to inaccurate results, especially for higher activity concentrations of 45 Ca compared to 3 H. So for better quantification of radionuclides in the dual-label mode, it is crucial to verify the effect of 45 Ca in the 3 H regions, especially with increasing quench.…”
Section: Discussionmentioning
confidence: 99%
“…Although there is a sufficient difference between the β energies emitted by 3 H (E av = 5.7 keV, E max = 18.6 keV) and 45 Ca (E av = 77 keV, E max = 252 keV), the internal bremsstrahlung effect of the 45 Ca spectra (Babu et al, 1976) emitted in the β-decay may lead to sufficient tailing of the peak. This may lead to fictitious peak area measurement in the 3 H window and hence lead to inaccurate results, especially for higher activity concentrations of 45 Ca compared to 3 H. So for better quantification of radionuclides in the dual-label mode, it is crucial to verify the effect of 45 Ca in the 3 H regions, especially with increasing quench.…”
Section: Discussionmentioning
confidence: 99%