Abstract

Lattice QCD calculations of two-nucleon systems are used to isolate the short-distance two-body electromagnetic contributions to the radiative capture process np→dγnp \to dγ, and the photo-disintegration processes γ(∗)d→npγ^{(\ast)} d \to np. In nuclear potential models, such contributions are described by phenomenological meson-exchange currents, while in the present work, they are determined directly from the quark and gluon interactions of QCD. Calculations of neutron-proton energy levels in multiple background magnetic fields are performed at two values of the quark masses, corresponding to pion masses of mπ∼450m_π\sim 450 and 806 MeV, and are combined with pionless nuclear effective field theory to determine these low-energy inelastic processes. Extrapolating to the physical pion mass, a cross section of σlqcd(np→dγ)=332.4(+5.4−4.7) mbσ^{lqcd}(np\to dγ)=332.4({\tiny \begin{array}{l}+5.4 \\ - 4.7\end{array}})\ mb is obtained at an incident neutron speed of v=2,200 m/sv=2,200\ m/s, consistent with the experimental value of σexpt(np→dγ)=334.2(0.5) mbσ^{expt}(np \to dγ) = 334.2(0.5)\ mb.

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