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O16(p,γ)F17 Reaction and the C and O Isotopic Ratios in Red Giant Branch Stars

D. Robb1, P. McGlynn2, M. Aliotta1, C. Ananna3,4,*, F. Barile5,6, L. Barbieri1, D. Bemmerer7, A. Best3,4, R. Biasissi8,9 et al. (LUNA Collaboration)

R. Biasissi8,9, A. Boeltzig7, R. Bonnell1, C. Broggini9, C. G. Bruno1, A. Caciolli8,9, M. Campostrini10, F. Casaburo11,12, F. Cavanna13, G. F. Ciani6, T. Chillery14, P. Colombetti15,13, A. Compagnucci1, P. Corvisiero11,12, L. Csedreki16, T. Davinson1, R. Depalo17,18,†, A. Di Leva3,4, Z. Elekes16, F. Ferraro14, A. Formicola19, Zs. Fülöp16, G. Gervino15,13, R. M. Gesuè20,14, G. Gosta17,18, Gy. Gyürky16, A. Guglielmetti17,18, C. Gustavino21, C. Hebborn22, G. Imbriani3,4, M. Junker14, M. Lugaro23, J. Marsh1, E. Masha7, R. Menegazzo9, D. Mercogliano3,4, V. Paticchio6, D. Piatti8,9, P. Prati11,12, D. Rapagnani3,4, V. Rigato10, M. Rossi12, R. Sariyal13, R. S. Sidhu1,‡, J. Skowronski8,9, O. Straniero24,19, T. Szücs16, S. Turkat8,9,§, M. Vagnoni25,19, and S. Zavatarelli12 (LUNA Collaboration)

  • 1SUPA, School of Physics and Astronomy, University of Edinburgh, EH9 3FD Edinburgh, United Kingdom
  • 2Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA
  • 3Università degli Studi di Napoli “Federico II,” 80125 Naples, Italy
  • 4Istituto Nazionale di Fisica Nucleare, Sezione di Napoli, 80125 Naples, Italy
  • 5Università degli Studi di Bari “A. Moro,” 70125 Bari, Italy
  • 6Istituto Nazionale di Fisica Nucleare, Sezione di Bari, 70125 Bari, Italy
  • 7Helmholtz-Zentrum Dresden-Rossendorf, 01328 Dresden, Germany
  • 8Dipartimento di Fisica, Università degli Studi di Padova, 35131 Padova, Italy
  • 9Istituto Nazionale di Fisica Nucleare, Sezione di Padova, 35131 Padova, Italy
  • 10Laboratori Nazionali di Legnaro, 35020 Legnaro, Italy
  • 11Università degli Studi di Genova, 16146 Genova, Italy
  • 12Istituto Nazionale di Fisica Nucleare, Sezione di Genova, 16146 Genova, Italy
  • 13Istituto Nazionale di Fisica Nucleare, Sezione di Torino, 10125 Torino, Italy
  • 14Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Gran Sasso, 67100 Assergi, Italy
  • 15Dipartimento di Fisica, Università degli Studi di Torino, 10125 Torino, Italy
  • 16HUN-REN Institute for Nuclear Research (ATOMKI), PO Box 51, H-4001 Debrecen, Hungary
  • 17Università degli Studi di Milano, 20133 Milano, Italy
  • 18Istituto Nazionale di Fisica Nucleare, Sezione di Milano, 20133 Milano, Italy
  • 19Istituto Nazionale di Fisica Nucleare, Sezione di Roma, Piazzale A. Moro 2, 00185 Roma, Italy
  • 20Gran Sasso Science Institute, 67100 L’Aquila, Italy
  • 21Istituto Nazionale di Fisica Nucleare, Sezione di Roma, 00185 Roma, Italy
  • 22CNRS - IJCLab, 91405 Orsay, France
  • 23Konkoly Observatory, Research Centre for Astronomy and Earth Sciences (HUN-REN CSFK), 1121 Budapest, Hungary
  • 24Istituto Nazionale di Astrofisica, Osservatorio Astronomico d’Abruzzo, Via Mentore Maggini, 64100 Teramo, Italy
  • 25Università degli Studi della Campania “Luigi Vanvitelli,” 81100 Caserta, Italy

  • *Present address: Università del Salento, 73100 Lecce, Italy.
  • †Contact author: rosanna.depalo@unimi.it
  • ‡Present address: University of Surrey, Guildford GU2 7XH, United Kingdom.
  • §Present address: Technische Universität Dresden, 01069 Dresden, Germany.

Phys. Rev. Lett. 137, 162701 – Published 14 October, 2026

DOI: https://doi.org/10.1103/tclf-b44m

Abstract

The O16:O17 isotopic ratio is a widely used tracer of nucleosynthesis and mixing processes in red giant stars. Its value depends on the rates of the proton-capture reactions responsible for the production and destruction of O16 and O17 among which the O16(p,γ)F17 reaction plays a central role, as it involves both isotopes. This work reports on a new measurement of the O16(p,γ)F17 cross section carried out at the Laboratory for Underground Nuclear Astrophysics (LUNA) over a center-of-mass energy range of 200–380 keV, a region previously unexplored by experimental studies. Two complementary techniques were employed: prompt gamma-ray detection and activation. The results obtained with the two techniques are consistent within experimental uncertainties. From the measured cross sections and existing literature data, we evaluate a new thermonuclear reaction rate, which is then used to demonstrate how simultaneous measurements of stellar carbon and oxygen isotopic ratios constrain the initial mass and the extent of the mixing events in red giant branch stars. In particular, we demonstrate how the C12:C13 abundance ratio is primarily sensitive to the temperature Tmax attained during mixing, whereas the O16:O17 abundance ratio is highly sensitive to the initial stellar mass Mi. Therefore, simultaneous measurements of these isotopic ratios can disentangle and place stringent constraints on Mi and Tmax, and the remaining uncertainty is now dominated by stellar abundance measurements rather than nuclear-physics inputs.

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