Direct measurement of the 15N(p,gamma)16O total cross section at novae energies
arXiv:0902.0783 · doi:10.1088/0954-3899/36/4/045202
Abstract
The 15N(p,gamma)16O reaction controls the passage of nucleosynthetic material from the first to the second carbon-nitrogen-oxygen (CNO) cycle. A direct measurement of the total 15N(p,gamma)16O cross section at energies corresponding to hydrogen burning in novae is presented here. Data have been taken at 90-230 keV center-of-mass energy using a windowless gas target filled with nitrogen of natural isotopic composition and a bismuth germanate summing detector. The cross section is found to be a factor two lower than previously believed.
LUNA collaboration; accepted by J. Phys. G
References in corpus (6)
- Activation measurement of the 3He(alpha,gamma)7Be cross section at low energy
- First measurement of the 14N(p,gamma)15O cross section down to 70 keV
- Precision study of ground state capture in the 14N(p,gamma)15O reaction
- Ultra-sensitive in-beam gamma-ray spectroscopy for nuclear astrophysics at LUNA
- Feasibility of low energy radiative capture experiments at the LUNA underground accelerator facility
- Measurement of 25Mg(p; gamma)26Al resonance strengths via gamma spectrometry
Cited by in corpus (11)
- The 12C(a,g)16O reaction and its implications for stellar helium burning
- LUNA: Status and Prospects
- The Future of Solar Neutrinos
- The 14N(p,gamma)15O reaction studied with a composite germanium detector
- An actively vetoed Clover gamma-detector for nuclear astrophysics at LUNA
- Constraining the S factor of 15N(p,g)16O at Astrophysical Energies
- Exploring Stars in Underground Laboratories: Challenges and Solutions
- Solar fusion III: New data and theory for hydrogen-burning stars
- Study of the neutron and proton capture reactions 10,11b(n, g), 11b(p, g), 14c(p, g), and 15n(p, g) at thermal and astrophysical energies
- Cosmic-ray induced background intercomparison with actively shielded HPGe detectors at underground locations
- Radiative proton capture on within effective field theory