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 in | Astrophysics and space science Vol. 370; no. 8; p. 81 |
---|---|
Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Dordrecht
Springer Netherlands
01.08.2025
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
ISSN | 0004-640X 1572-946X |
DOI | 10.1007/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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Cites_doi | 10.1103/RevModPhys.81.1773 10.1016/S0550-3213(98)00440-4 10.1016/j.nuclphysa.2008.09.014 10.1103/PhysRevD.76.033005 10.1007/s10509-023-04252-9 10.1088/0004-637X/743/1/24 10.1016/j.newast.2022.101971 10.1103/PhysRevC.82.034609 10.1103/RevModPhys.83.195 10.1103/PhysRevLett.102.062503 10.1016/S0375-9474(99)00298-5 10.1103/PhysRevLett.97.122502 10.1016/S0375-9474(02)00597-3 10.1140/epja/i2006-09-006-5 10.1016/0375-9474(90)90271-M 10.1016/j.nima.2008.07.082 10.1016/j.nuclphysa.2008.06.003 10.1016/S0375-9474(99)00030-5 |
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References | R. Higa (4476_CR12) 2008; 809 D.B. Kaplan (4476_CR13) 1998; 534 E.G. Adelberger (4476_CR1) 2011; 83 F. Ajzenberg-Selove (4476_CR2) 1990; 506 M. Khoddam (4476_CR15) 2023; 100 C. Angulo (4476_CR3) 1999; 656 J.-W. Chen (4476_CR5) 1999; 653 E. Hernandez (4476_CR11) 2007; 76 P. Navratil (4476_CR16) 2010; 82 S. Pastore (4476_CR18) 2008; 78 A. Coc (4476_CR6) 2014; 744 D.R. Tilley (4476_CR21) 2002; 708 W. Nörtershäuser (4476_CR17) 2009; 102 A.M. Serenelli (4476_CR20) 2011; 743 D. Bemmerer (4476_CR4) 2006; 97 M. Khoddam (4476_CR14) 2023; 368 E. Epelbaum (4476_CR9) 2009; 81 H. Costantini (4476_CR7) 2008; 814 H. Sadeghi (4476_CR19) 2025; 370 A. Di Leva (4476_CR8) 2008; 595 H.-W. Hammer (4476_CR10) 2006; 28 |
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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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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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