“…In explosive astrophysical scenarios such as novae and X-ray bursts, when temperatures are T 9 ≥ 0.1, it is possible to bypass the β-decay of the waiting points in the HCNO cycle, such as the nuclei 14 O and 15 O, by α capture reactions leading directly to the αp-process and the rp-process [1]. The two breakout paths from the HCNO cycle are the reaction sequences 14 O(α,p) 17 F(p,γ) 18 Ne(α,p) and 15 O(α,γ) 19 Ne(p,γ) shown in Fig.…”