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Isoscalar M1 and E2 Amplitudes in n+p -> d+gamma

2 Pith papers cite this work. Polarity classification is still indexing.

2 Pith papers citing it
abstract

The low energy radiative capture process n+p -> d+gamma provides a sensitive probe of the two-nucleon system. The cross section for this process is dominated by the isovector M1 amplitude for capture from the 1S0 channel via the isovector magnetic moment of the nucleon. In this work we use effective field theory to compute the isoscalar M1 and isoscalar E2 amplitudes that are strongly suppressed for cold neutron capture. The actual value of the isoscalar E2 amplitude is expected to be within 15% of the value computed in this work. In contrast, due to the vanishing contribution of the one-body operator at leading order and next-to-leading order, the isoscalar M1 amplitude is estimated to have a large uncertainty. We discuss in detail the deuteron quadrupole form factor and SD mixing.

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nucl-th 2

years

2026 2

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UNVERDICTED 2

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representative citing papers

Coulomb Corrections to Three-Nucleon Moments

nucl-th · 2026-05-18 · unverdicted · novelty 4.0

Pionless EFT calculations find unexpectedly small O(alpha) Coulomb corrections to three-nucleon magnetic moments and GT matrix elements, yielding a fitted prediction for the proton-proton fusion reduced matrix element of 2.776(331).

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Showing 2 of 2 citing papers.

  • Coulomb Corrections to Three-Nucleon Moments nucl-th · 2026-05-18 · unverdicted · none · ref 6 · internal anchor

    Pionless EFT calculations find unexpectedly small O(alpha) Coulomb corrections to three-nucleon magnetic moments and GT matrix elements, yielding a fitted prediction for the proton-proton fusion reduced matrix element of 2.776(331).

  • Coulomb Effects and Wigner-SU(4) Symmetry in He-3 Charge and Magnetic Properties nucl-th · 2026-04-28 · unverdicted · none · ref 16

    Non-perturbative Coulomb corrections in LO pionless EFT give a 0.85(3) MeV He-3/H-3 binding split, 0.043(2) fm charge-radius shift, 0.036(2) fm magnetic-radius shift, and -0.0041(1) μ_N moment shift.