2015
DOI: 10.1016/j.physletb.2015.10.073
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The first science result with the JENSA gas-jet target: Confirmation and study of a strong subthreshold F18(p,α)

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Cited by 26 publications
(50 citation statements)
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“…A Γ p of 7.3±0.6 eV was extracted from proton transfer data [10], however, the population of the 330 keV resonance could have been contaminated by nearby states. 19 Ne studies by Laird et al [17] and Bardayan et al [18], respectively, found discrepancies in the spin and parity assignments for levels close to the proton threshold in 19 Ne. This may have ramifications for the 18 F(p,γ) 19 Ne reaction rate at nova temperatures; the new spin and parity assignments differ from those published previously, leading to changes in the interference effects with stronger, higher lying states, hence altering the capture cross section.…”
Section: Thementioning
confidence: 95%
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“…A Γ p of 7.3±0.6 eV was extracted from proton transfer data [10], however, the population of the 330 keV resonance could have been contaminated by nearby states. 19 Ne studies by Laird et al [17] and Bardayan et al [18], respectively, found discrepancies in the spin and parity assignments for levels close to the proton threshold in 19 Ne. This may have ramifications for the 18 F(p,γ) 19 Ne reaction rate at nova temperatures; the new spin and parity assignments differ from those published previously, leading to changes in the interference effects with stronger, higher lying states, hence altering the capture cross section.…”
Section: Thementioning
confidence: 95%
“…Hence there is significant interest in radioisotopes thought to be abundantly produced in such events, in the hope that their decay signatures can be directly observed. One radioisotope of interest is 18 F, as its positron annihilation, following β + decay, is thought to be the major source of 511 keV line emission γ-rays after nova outbursts [3]. This is due to the fact that the relatively long half life of 18 F (t 1/2 =110 mins) results in a significant number of positrons being emitted shortly after the expanding nova envelope becomes transparent to γ-rays, whilst its halflife is short enough that its absolute decay rate remains high.…”
Section: A Classical Novaementioning
confidence: 99%
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