Cold Neutron-Deuteron Capture and Wigner-SU(4) Symmetry
arXiv:2210.15650 · doi:10.1103/PhysRevC.108.044001
Abstract
We calculate the cold neutron-deuteron () capture cross section, , to next-to-next-to leading order (NNLO) using the model-independent approach of pionless effective field theory (EFT()). At leading order we find mb, while the experimental result is 0.508(15) mb [Jurney, Bendt and Browne in Phys. Rev. C 25, 2810 (1982)] for a laboratory neutron velocity of 2200 m/s. At next-to-leading-order (NLO), we show that is sensitive to the low energy constant (LEC), , of the two-nucleon isovector current appearing at NLO. A fit of at NLO to the triton magnetic moment yields a NLO prediction of mb, where the error comes from propagating the error from the fit. At next-to-next-to-leading-order (NNLO), we find that a new three-nucleon magnetic moment counterterm is required for renormalization group invariance of both and the triton magnetic moment. Fitting the NNLO correction to (denoted ) to cold neutron-proton capture () yields a NNLO prediction of mb, where the error comes from propagating the error from the fit. We also study different fittings of and to , , and/or the triton magnetic moment. For example, fitting simultaneously to , , and the triton magnetic moment at NLO, and fitting simultaneously to and at NNLO, yields mb and mb, respectively, where errors are naively estimated from EFT() power counting. In addition, we discuss how Wigner-SU(4) symmetry may alter the naive EFT() expansion of .
arXiv comment61 pages, 10 figures, version published in PRC. Some typos and errors in numerical results are fixed compared to the previous version
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