1982
DOI: 10.1007/bf01197981
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The determination of nitrogen in zirconium by charged-particle activation analysis

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Cited by 5 publications
(2 citation statements)
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“…In the case of 11 C, irradiation below the threshold energy ensures complete elimination of 15 O, elimination is only partial because a beam energy >16 MeV is required for a higher yield of 13 N. However, if activity counting is performed after a sufficiently long decay time, the significantly shorter half-life of 15 O compared with 13 N ensures adequate elimination of the interference. Another pure positronic emitter, 18 F, has its production threshold energy very close to 13 N, but owing to a significantly longer halflife, it has a significantly lower production rate. Moreover, fluorine in biological materials is usually present at much lower levels than nitrogen.…”
Section: Resultsmentioning
confidence: 99%
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“…In the case of 11 C, irradiation below the threshold energy ensures complete elimination of 15 O, elimination is only partial because a beam energy >16 MeV is required for a higher yield of 13 N. However, if activity counting is performed after a sufficiently long decay time, the significantly shorter half-life of 15 O compared with 13 N ensures adequate elimination of the interference. Another pure positronic emitter, 18 F, has its production threshold energy very close to 13 N, but owing to a significantly longer halflife, it has a significantly lower production rate. Moreover, fluorine in biological materials is usually present at much lower levels than nitrogen.…”
Section: Resultsmentioning
confidence: 99%
“…Prompt γ ‐ray neutron activation analysis utilizing the reaction 14 N(n, γ ) 15 N has often been used . Although another possibility is activation with charged particles . Photon activation analysis, in the present work used in an instrumental mode (IPAA), was one of the first nuclear radioanalytical methods used for nitrogen assay .…”
Section: Introductionmentioning
confidence: 97%