The 3He(α, γ)7Be reaction in effective field theory

We present a theoretical analysis of the 3 He( α , γ ) 7 Be radiative capture reaction, using pionless effective field theory (EFT) at the leading order. What sets our approach apart is the unique combination of direct capture mechanisms and resonant processes that involve the 7 / 2 − excited state...

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Published inAstrophysics and space science Vol. 370; no. 8; p. 81
Main Authors Sadeghi, Hossein, Khoddam, Maryam
Format Journal Article
LanguageEnglish
Published Dordrecht Springer Netherlands 01.08.2025
Springer Nature B.V
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ISSN0004-640X
1572-946X
DOI10.1007/s10509-025-04476-x

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Abstract We present a theoretical analysis of the 3 He( α , γ ) 7 Be radiative capture reaction, using pionless effective field theory (EFT) at the leading order. What sets our approach apart is the unique combination of direct capture mechanisms and resonant processes that involve the 7 / 2 − excited state of 7 Be at 429 keV. By rigorously examining electromagnetic multipole transitions, we’ve managed to achieve a theoretical uncertainty of just 4.1% for the astrophysical S-factor. Our calculated value of S ( 0 ) = 0.511 ± 0.021  keV ⋅ b aligns impressively with the recommended experimental value of 0.529 ± 0.018  keV ⋅ b. At the temperatures found in the solar core ( T 9 = 0.015 ), our reaction rate of ( 9.2 ± 0.4 ) × 10 3  cm 3  mol − 1  s − 1 helps to clear up some long-standing discrepancies in stellar models. Interestingly, our multipole decomposition shows a surprising persistence of M1 contributions (35.2% at resonance) that goes beyond what typical single-particle models would predict, underscoring the significance of two-body currents. The theoretical uncertainties we encountered are mainly due to EFT truncation errors (2.8%) and variations in low-energy constants (2.1%). These findings have direct implications for solar neutrino flux predictions and calculations of primordial lithium abundance.
AbstractList We present a theoretical analysis of the 3 He( α , γ ) 7 Be radiative capture reaction, using pionless effective field theory (EFT) at the leading order. What sets our approach apart is the unique combination of direct capture mechanisms and resonant processes that involve the 7 / 2 − excited state of 7 Be at 429 keV. By rigorously examining electromagnetic multipole transitions, we’ve managed to achieve a theoretical uncertainty of just 4.1% for the astrophysical S-factor. Our calculated value of S ( 0 ) = 0.511 ± 0.021  keV ⋅ b aligns impressively with the recommended experimental value of 0.529 ± 0.018  keV ⋅ b. At the temperatures found in the solar core ( T 9 = 0.015 ), our reaction rate of ( 9.2 ± 0.4 ) × 10 3  cm 3  mol − 1  s − 1 helps to clear up some long-standing discrepancies in stellar models. Interestingly, our multipole decomposition shows a surprising persistence of M1 contributions (35.2% at resonance) that goes beyond what typical single-particle models would predict, underscoring the significance of two-body currents. The theoretical uncertainties we encountered are mainly due to EFT truncation errors (2.8%) and variations in low-energy constants (2.1%). These findings have direct implications for solar neutrino flux predictions and calculations of primordial lithium abundance.
We present a theoretical analysis of the 3He(α, γ)7Be radiative capture reaction, using pionless effective field theory (EFT) at the leading order. What sets our approach apart is the unique combination of direct capture mechanisms and resonant processes that involve the 7/2− excited state of 7Be at 429 keV. By rigorously examining electromagnetic multipole transitions, we’ve managed to achieve a theoretical uncertainty of just 4.1% for the astrophysical S-factor. Our calculated value of S(0)=0.511±0.021 keV⋅b aligns impressively with the recommended experimental value of 0.529±0.018 keV⋅b. At the temperatures found in the solar core (T9=0.015), our reaction rate of (9.2±0.4)×103 cm3 mol−1 s−1 helps to clear up some long-standing discrepancies in stellar models. Interestingly, our multipole decomposition shows a surprising persistence of M1 contributions (35.2% at resonance) that goes beyond what typical single-particle models would predict, underscoring the significance of two-body currents. The theoretical uncertainties we encountered are mainly due to EFT truncation errors (2.8%) and variations in low-energy constants (2.1%). These findings have direct implications for solar neutrino flux predictions and calculations of primordial lithium abundance.
ArticleNumber 81
Author Khoddam, Maryam
Sadeghi, Hossein
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  email: M-Khoddam@Postdoct.araku.ac.ir
  organization: Department of Physics, Faculty of Sciences, Arak University
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Snippet We present a theoretical analysis of the 3 He( α , γ ) 7 Be radiative capture reaction, using pionless effective field theory (EFT) at the leading order. What...
We present a theoretical analysis of the 3He(α, γ)7Be radiative capture reaction, using pionless effective field theory (EFT) at the leading order. What sets...
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StartPage 81
SubjectTerms Accuracy
Astrobiology
Astronomy
Astrophysics
Astrophysics and Astroparticles
Beryllium
Beryllium 7
Cosmology
Energy
Field theory
Lithium
Multipoles
Neutrinos
Nuclear physics
Observations and Techniques
Physics
Physics and Astronomy
Solar core
Solar neutrinos
Space Exploration and Astronautics
Space Sciences (including Extraterrestrial Physics
Stellar models
Theoretical analysis
Truncation errors
Uncertainty
Title The 3He(α, γ)7Be reaction in effective field theory
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