For stars with 0.8 M⊙ ≤ M ≤ 8.0 M⊙, nucleosynthesis enters its final phase during the asymptotic giant branch (AGB) stage. During this evolutionary period, grain condensation occurs in the stellar atmosphere, and the star experiences significant mass loss. The production of presolar grains can often be attributed to this unique stellar environment. A subset of presolar oxide grains features dramatic 18O depletion that cannot be explained by the standard AGB star burning stages and dredge-up models. An extra mixing process, referred to as cool bottom processing (CBP), was proposed for low-mass AGB stars. The 18O depletion observed within certain stellar environments and within presolar grain samples may result from the 18O+p processes du...
The O17(p,γ)F18 and O17(p,α)N14 reactions have a profound influence on hydrogen-burning nucleosynthe...
Background: Shell hydrogen burning during the asymptotic giant branch (AGB) phase through the oxygen...
The 18O(p, α)15N reaction is of primary importance to pin down the uncertainties, due to nuclear phy...
For 0.8 Mȯ ≤ M ≤ 8.0 Mȯ stars, the final phase of nucleosynthesis occurs during the asymptotic giant...
At the Laboratory for Experimental Nuclear Astrophysics (LENA), two rare oxygen isotope proton captu...
The 16O(p,gamma)17F reaction rate is revisited with special emphasis on the stellar temperature rang...
The 17;18O(p,α)14;15N nuclear reactions play an important role in several astrophysical scenarios, ...
In recent years, the Trojan Horse Method (THM) has been used to investigate the low-energy cross sec...
The 18O(p,α)15N reaction affects the synthesis of 15N, 18O and 19F isotopes, whose abundances can be...
A self-consistent calculation of asymptotic giant branch (AGB) evolution was carried out, including ...
Background: Shell hydrogen burning during the asymptotic giant branch (AGB) phase through the oxygen...
The 18O(p, ?)15N reaction is of great importance in several astrophysical scenarios, as it influence...
The 18O(p,\u3b1)15N reaction affects the synthesis of 15N, 18O and 19F isotopes, whose abundances ca...
Many nucleosynthesis and mixing processes of low-mass stars as they evolve from the Main Sequence to...
The O17(p,γ)F18 and O17(p,α)N14 reactions have a profound influence on hydrogen-burning nucleosynthe...
Background: Shell hydrogen burning during the asymptotic giant branch (AGB) phase through the oxygen...
The 18O(p, α)15N reaction is of primary importance to pin down the uncertainties, due to nuclear phy...
For 0.8 Mȯ ≤ M ≤ 8.0 Mȯ stars, the final phase of nucleosynthesis occurs during the asymptotic giant...
At the Laboratory for Experimental Nuclear Astrophysics (LENA), two rare oxygen isotope proton captu...
The 16O(p,gamma)17F reaction rate is revisited with special emphasis on the stellar temperature rang...
The 17;18O(p,α)14;15N nuclear reactions play an important role in several astrophysical scenarios, ...
In recent years, the Trojan Horse Method (THM) has been used to investigate the low-energy cross sec...
The 18O(p,α)15N reaction affects the synthesis of 15N, 18O and 19F isotopes, whose abundances can be...
A self-consistent calculation of asymptotic giant branch (AGB) evolution was carried out, including ...
Background: Shell hydrogen burning during the asymptotic giant branch (AGB) phase through the oxygen...
The 18O(p, ?)15N reaction is of great importance in several astrophysical scenarios, as it influence...
The 18O(p,\u3b1)15N reaction affects the synthesis of 15N, 18O and 19F isotopes, whose abundances ca...
Many nucleosynthesis and mixing processes of low-mass stars as they evolve from the Main Sequence to...
The O17(p,γ)F18 and O17(p,α)N14 reactions have a profound influence on hydrogen-burning nucleosynthe...
Background: Shell hydrogen burning during the asymptotic giant branch (AGB) phase through the oxygen...
The 18O(p, α)15N reaction is of primary importance to pin down the uncertainties, due to nuclear phy...