Your browser doesn't support javascript.
loading
First Direct Measurement Constraining the
Browne, J; Chipps, K A; Schmidt, Konrad; Schatz, H; Ahn, S; Pain, S D; Montes, F; Ong, W J; Greife, U; Allen, J; Bardayan, D W; Blackmon, J C; Blankstein, D; Cha, S; Chae, K Y; Febbraro, M; Hall, M R; Jones, K L; Kontos, A; Meisel, Z; O'Malley, P D; Schmitt, K T; Smith, K; Smith, M S; Thompson, P; Toomey, R; Vostinar, M; Walter, D.
Afiliação
  • Browne J; Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824.
  • Chipps KA; Joint Institute for Nuclear Astrophysics (JINA-CEE), Michigan State University, East Lansing, Michigan 48824.
  • Schmidt K; Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831.
  • Schatz H; Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996.
  • Ahn S; Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824.
  • Pain SD; Joint Institute for Nuclear Astrophysics (JINA-CEE), Michigan State University, East Lansing, Michigan 48824.
  • Montes F; Institute of Radiation Physics, Helmholtz-Zentrum Dresden-Rossendorf, Bautzner Landstrasse 400, 01328 Dresden, Germany.
  • Ong WJ; Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824.
  • Greife U; Joint Institute for Nuclear Astrophysics (JINA-CEE), Michigan State University, East Lansing, Michigan 48824.
  • Allen J; Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824.
  • Bardayan DW; Joint Institute for Nuclear Astrophysics (JINA-CEE), Michigan State University, East Lansing, Michigan 48824.
  • Blackmon JC; Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831.
  • Blankstein D; Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996.
  • Cha S; Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824.
  • Chae KY; Joint Institute for Nuclear Astrophysics (JINA-CEE), Michigan State University, East Lansing, Michigan 48824.
  • Febbraro M; Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824.
  • Hall MR; Joint Institute for Nuclear Astrophysics (JINA-CEE), Michigan State University, East Lansing, Michigan 48824.
  • Jones KL; Physics Department, Colorado School of Mines, Golden, Colorado 80401.
  • Kontos A; Department of Physics and Astronomy, University of Notre Dame, Notre Dame, Indiana 46556.
  • Meisel Z; Joint Institute for Nuclear Astrophysics (JINA-CEE), Michigan State University, East Lansing, Michigan 48824.
  • O'Malley PD; Department of Physics and Astronomy, University of Notre Dame, Notre Dame, Indiana 46556.
  • Schmitt KT; Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803.
  • Smith K; Department of Physics and Astronomy, University of Notre Dame, Notre Dame, Indiana 46556.
  • Smith MS; Department of Physics, Sungkyunkwan University, Suwon 16419, Korea.
  • Thompson P; Department of Physics, Sungkyunkwan University, Suwon 16419, Korea.
  • Toomey R; Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831.
  • Vostinar M; Department of Physics and Astronomy, University of Notre Dame, Notre Dame, Indiana 46556.
  • Walter D; Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996.
Phys Rev Lett ; 130(21): 212701, 2023 May 26.
Article em En | MEDLINE | ID: mdl-37295108
ABSTRACT
The rate of the final step in the astrophysical αp process, the ^{34}Ar(α,p)^{37}K reaction, suffers from large uncertainties due to a lack of experimental data, despite having a considerable impact on the observable light curves of x-ray bursts and the composition of the ashes of hydrogen and helium burning on accreting neutron stars. We present the first direct measurement constraining the ^{34}Ar(α,p)^{37}K reaction cross section, using the Jet Experiments in Nuclear Structure and Astrophysics gas jet target. The combined cross section for the ^{34}Ar,Cl(α,p)^{37}K,Ar reaction is found to agree well with Hauser-Feshbach predictions. The ^{34}Ar(α,2p)^{36}Ar cross section, which can be exclusively attributed to the ^{34}Ar beam component, also agrees to within the typical uncertainties quoted for statistical models. This indicates the applicability of the statistical model for predicting astrophysical (α,p) reaction rates in this part of the αp process, in contrast to earlier findings from indirect reaction studies indicating orders-of-magnitude discrepancies. This removes a significant uncertainty in models of hydrogen and helium burning on accreting neutron stars.
Assuntos

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Assunto principal: Hélio / Hidrogênio Tipo de estudo: Prognostic_studies / Risk_factors_studies Idioma: En Revista: Phys Rev Lett Ano de publicação: 2023 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Assunto principal: Hélio / Hidrogênio Tipo de estudo: Prognostic_studies / Risk_factors_studies Idioma: En Revista: Phys Rev Lett Ano de publicação: 2023 Tipo de documento: Article