PaperPanorama

arXiv:1708.04017·v1·Nuclear Theory

Models, measurements, and effective field theory: proton capture on Beryllium-7 at next-to-leading order

Xilin Zhang · Kenneth M. Nollett · Daniel R. Phillips

Abstract

We employ an effective field theory (EFT) that exploits the separation of scales in the p-wave halo nucleus to describe the process up to a center-of-mass energy of 500 keV. The calculation, for which we develop the lagrangian and power counting, is carried out up to next-to-leading order (NLO) in the EFT expansion. The power counting we adopt implies that Coulomb interactions must be included to all orders in . We do this via EFT Feynman diagrams computed in time-ordered perturbation theory, and so recover existing quantum-mechanical technology such as the two-potential formalism for the treatment of the Coulomb-nuclear interference. Meanwhile the strong interactions and the E1 operator are dealt with via EFT expansions in powers of momenta, with a breakdown scale set by the size of the Be core, MeV. Up to NLO the relevant physics in the different channels that enter the radiative capture reaction is encoded in ten different EFT couplings. The result is a model-independent parametrization for the reaction amplitude in the energy regime of interest. To show the connection to previous results we fix the EFT couplings using results from a number of potential model and microscopic calculations in the literature. Each of these models corresponds to a particular point in the space of EFTs. The EFT structure therefore provides a very general way to quantify the model uncertainty in calculations of . We also demonstrate that the only NLO corrections in come from an inelasticity that is practically of NLO size in the energy range of interest, and so the truncation error in our calculation is effectively NLO. We also discuss the relation of our extrapolated to the previous standard evaluation.

Comments: 68 pages, 10 figures, and 4 tables

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