Precision calculation of $^3$He$(α,γ)^7$Be for solar physics

We calculate the cross section for radiative capture $^3$He$(α,γ)^7$Be at next-to-next-to-leading order (NNLO). At this order of perturbation, momentum dependent two-body currents make their first appearance. We provide a model-independent construction of these currents from gauge and Galilean invariance, where the general framework for constructing higher-order two-body currents in low-energy effective field theories becomes evident. The $^3$He$(α,γ)^7$Be astrophysical S-factor $S_{34}(0)= 0.564^{+0.17}_{-0.015}$ keV b is obtained from a Bayesian analysis at NNLO, with an additional nominal theoretical uncertainty $\pm0.017$ keV b of 3%.

Publication Details

Journal
ArXiv.org
Published
2025-09-29
Primary Topic
Polysaccharides Composition and Applications
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article
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article

Precision calculation of $^3$He$(α,γ)^7$Be for solar physics

ArXiv.org
Polysaccharides Composition and Applications
article

Precision calculation of $^3$He$(α,γ)^7$Be for solar physics

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Abstract

We calculate the cross section for radiative capture $^3$He$(α,γ)^7$Be at next-to-next-to-leading order (NNLO). At this order of perturbation, momentum dependent two-body currents make their first appearance. We provide a model-independent construction of these currents from gauge and Galilean invariance, where the general framework for constructing higher-order two-body currents in low-energy effective field theories becomes evident. The $^3$He$(α,γ)^7$Be astrophysical S-factor $S_{34}(0)= 0.564^{+0.17}_{-0.015}$ keV b is obtained from a Bayesian analysis at NNLO, with an additional nominal theoretical uncertainty $\pm0.017$ keV b of 3%.

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Polysaccharides Composition and Applications
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Precision calculation of $^3$He$(α,γ)^7$Be for solar physics · ArXiv.org (2025) | TGRS Research Map | TGRS