2009
DOI: 10.1103/physrevc.80.065802
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E1andE2cross sections of theC12

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Cited by 45 publications
(156 citation statements)
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“…The cross section for the triple-α process is experimentally quite well determined [4]. Our knowledge of the 12 C(α, γ) 16 O reaction under typical helium burning conditions (T 9 ∼ 0.2 or E c.m. ∼ 300 keV), however, is still limited by its small cross section and by the crucial role played by two sub-threshold states in 16 O [5].…”
Section: Introductionmentioning
confidence: 99%
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“…The cross section for the triple-α process is experimentally quite well determined [4]. Our knowledge of the 12 C(α, γ) 16 O reaction under typical helium burning conditions (T 9 ∼ 0.2 or E c.m. ∼ 300 keV), however, is still limited by its small cross section and by the crucial role played by two sub-threshold states in 16 O [5].…”
Section: Introductionmentioning
confidence: 99%
“…Contrary to the triple α reaction which is dominated by the contribution from a resonant state (the so-called Hoyle state) the 12 C(α, γ) 16 O reaction proceeds mainly through two radiative capture modes to the 16 O ground state. One is E1 capture with contributions from the 1 − state at E x =9.585 MeV (E r =2.418 MeV) and the sub-threshold 1 − state at E x =7.117 MeV (E r =-45 keV).…”
Section: Introductionmentioning
confidence: 99%
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