2020
DOI: 10.21468/scipostphysproc.3.009
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Clustering in $^{18}$O - absolute determination of branching ratios via high-resolution particle spectroscopy

Abstract: The determination of absolute branching ratios for high-energy states in light nuclei is an important and useful tool for probing the underlying nuclear structure of individual resonances: for example, in establishing the tendency of an excited state towards α-cluster structure. Difficulty arises in measuring these branching ratios due to similarities in available decay channels, such as ( 18 O,n) and ( 18 O,2n), as well as differences in geometric efficiencies due to population of bound excited levels in daug… Show more

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Cited by 3 publications
(10 citation statements)
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“…Just above the n-decay threshold of S n = 8.045 MeV, it is very difficult to distinguish between γ -decay and n-decay events due to the limited kinetic energy available to product 17 O nuclei. As γ -decay becomes suppressed above particle decay thresholds, it is very unlikely to find a significant value of γ/ tot for high-lying excitations, however, the states at 8126(3) MeV, 8219(1) MeV and 8280(1) MeV have been previously determined to γ -decay [16].…”
Section: States Below the N-thresholdmentioning
confidence: 99%
“…Just above the n-decay threshold of S n = 8.045 MeV, it is very difficult to distinguish between γ -decay and n-decay events due to the limited kinetic energy available to product 17 O nuclei. As γ -decay becomes suppressed above particle decay thresholds, it is very unlikely to find a significant value of γ/ tot for high-lying excitations, however, the states at 8126(3) MeV, 8219(1) MeV and 8280(1) MeV have been previously determined to γ -decay [16].…”
Section: States Below the N-thresholdmentioning
confidence: 99%
“…In order to distinguish between these decay channels, a kinematic technique known as a Catania plot (also known as a Romano plot) [16,17,19,26] was employed. A FIG.…”
Section: A Decay Channelsmentioning
confidence: 99%
“…The in-house Monte-Carlo code, Resolution8.1 [19,27,28], was used to generate events for each observed excited state, simulating all available decay paths. Individual decay paths for each state were simulated using 10 7 events in order to determine the expected geometry efficiency of the DSSD array while limiting the associated statistical error.…”
Section: B Monte-carlo Simulationmentioning
confidence: 99%
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