The NN scattering 3S1-3D1 mixing angle at NNLO

Details The NN scattering 3S1-3D1 mixing angle at NNLO The NN scattering 3S1-3D1 mixing angle at NNLO

1999-06-19

arxiv.org/abs/nucl-th/9906056v2

Phys.Rev. C61 (2000) 044005

Physics

Nuclear Physics

Nuclear Theory

17 pages, journal version

Scientific paper

10.1103/PhysRevC.61.044005

The 3S1-3D1 mixing angle for nucleon-nucleon scattering, epsilon_1, is calculated to next-to-next-to-leading order in an effective field theory with perturbative pions. Without pions, the low energy theory fits the observed epsilon_1 well for momenta less than $\sim 50$ MeV. Including pions perturbatively significantly improves the agreement with data for momenta up to $\sim 150$ MeV with one less parameter. Furthermore, for these momenta the accuracy of our calculation is similar to an effective field theory calculation in which the pion is treated non-perturbatively. This gives phenomenological support for a perturbative treatment of pions in low energy two-nucleon processes. We explain why it is necessary to perform spin and isospin traces in d dimensions when regulating divergences with dimensional regularization in higher partial wave amplitudes.

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