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Home Astronomy research Software Infrastructure: MESA FLASH-X STARLIB MESA-Web starkiller-astro My instruments White dwarf pulsations: 12C(α,γ) & overshooting Probe of 12C(α,γ)16O Impact of 22Ne Impact of ν cooling Variable white dwarfs MC reaction rates Micronovae Novae White dwarf supernova: Stable nickel production Remnant metallicities Colliding white dwarfs Merging white dwarfs Ignition conditions Metallicity effects Central density effects Detonation density Tracer particle burning Subsonic burning fronts Supersonic fronts W7 profiles Massive stars: Pop III with HST/JWST Rotating progenitors 3D evolution to collapse MC reaction rates Pre-SN variations Massive star supernova: Yields of radionuclides 26Al & 60Fe 44Ti, 60Co & 56Ni SN 1987A light curve Constraints on Ni/Fe An r-process Effects of 12C +12C Neutron Stars and Black Holes: Black Hole spectrum Mass Gap with LVK Compact object IMF He burn neutron stars Neutrino Emission: Neutrino emission from stars Identifying the Pre-SN Neutrino HR diagram Pre-SN Beta Processes Pre-SN neutrinos Stars: Hypatia catalog SAGB stars Nugrid Yields I He shell convection BBFH at 40 years γ-rays within 100 Mpc Iron Pseudocarbynes Pre-Solar Grains: C-rich presolar grains SiC Type U/C grains Grains from massive stars Placing the Sun SiC Presolar grains Chemical Evolution: Radionuclides in 2020s Zone models H to Zn Mixing ejecta Thermodynamics, Opacities & Networks Radiative Opacity Skye EOS Helm EOS Five EOSs Equations of State 12C(α,γ)16O Rate Proton-rich NSE Reaction networks Bayesian reaction rates Verification Problems: Validating an astro code Su-Olson Cog8 Mader RMTV Sedov Noh Software Instruments AAS Journals 2025 AAS YouTube 2025 AAS Peer Review Workshops 2025 ASU Energy in Everyday Life 2025 MESA Classroom Other Stuff: Bicycle Adventures Illustrations Presentations Contact: F.X.Timmes my one page vitae, full vitae, research statement, and teaching statement. |
The 12C(α,γ)16O reaction and its implications for stellar helium burning (2017)
The creation of carbon and oxygen in our Universe is one of the forefront questions in nuclear astrophysics. The determination of the abundance of these elements is key to our understanding of both the formation of life on Earth and to the life cycles of stars. While nearly all models of different nucleosynthesis environments are affected by the production of carbon and oxygen, a key ingredient, the precise determination of the reaction rate of $^{12}$C($\alpha , \gamma$)$^{16}$O, has long remained elusive. This is owed to the reaction's inaccessibility, both experimentally and theoretically. Nuclear theory has struggled to calculate this reaction rate because the cross section is produced through different underlying nuclear mechanisms. Isospin selection rules suppress the E1 component of the ground state cross section, creating a unique situation where the E1 and E2 contributions are of nearly equal amplitudes. Experimentally there have also been great challenges. Measurements have been pushed to the limits of state-of-the-art techniques, often developed for just these measurements. The data have been plagued by uncharacterized uncertainties, often the result of the novel measurement techniques that have made the different results challenging to reconcile. However, the situation has markedly improved in recent years, and the desired level of uncertainty 10% may be in sight. In this review article the current understanding of this critical reaction is summarized. The emphasis is placed primarily on the experimental work and interpretation of the reaction data, but discussions of the theory and astrophysics are also pursued. The main goal is to summarize and clarify the current understanding of the reaction and then point the way forward to an improved determination of the reaction rate. |
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