1992
DOI: 10.1016/0168-9002(92)90166-2
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Standardization of 192Ir

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Cited by 15 publications
(5 citation statements)
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“…Hence, this is truly a 4π solid angle method for particles and photons with a very high total efficiency for most nuclides. It is well suited for the standardization of radionuclides with a complex decay [54,66], but also for pure β-and α-decay [17][18][19] and even electron capture [67]. Limitations are the rather high noise level, equivalent to an energy threshold of about 10 keV, and the escape probability of high-energy photons.…”
Section: π Windowless Sandwich Spectrometermentioning
confidence: 99%
“…Hence, this is truly a 4π solid angle method for particles and photons with a very high total efficiency for most nuclides. It is well suited for the standardization of radionuclides with a complex decay [54,66], but also for pure β-and α-decay [17][18][19] and even electron capture [67]. Limitations are the rather high noise level, equivalent to an energy threshold of about 10 keV, and the escape probability of high-energy photons.…”
Section: π Windowless Sandwich Spectrometermentioning
confidence: 99%
“…The most commonly used detector for 4πγ counting is a large well-type NaI(Tl) detector; various dimensions are given in the literature (152.4 mm × 152.4 mm [10], 75 mm × 75 mm [11], 127 mm × 127 mm [12], 152 mm × 127 mm [13]) and also larger crystals have been installed (e.g. 203 mm × 203 mm at the JRC-IRMM).…”
Section: Typical Detection Set-upmentioning
confidence: 99%
“…In those cases, pulses delivered by both detectors are first summed in coincidence before feeding the electronic chain. An existing configuration consists of sandwiching the source between two windowless Cs(Tl) crystals, which offers the possibility to measure particles in coincidence with γ and x rays [10,14].…”
Section: Typical Detection Set-upmentioning
confidence: 99%
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