“…In this paper, we are only considering parameterizations of the form U ijk ≡ U i U j U k for i, j, k = 1, 2, 3 in which i, j, and k are all different. Other parameterizations exist [33,34] including those using the same rotation axis twice (U iji ) [35], three of the Gell-Mann matrices parameterizing the generators of SU(3) [36][37][38][39], four complex phases [40], the exponential of a complex matrix [41], or five rotations and a complex phase [42]. 2 If one wanted to include the Majorana phases in the parameterization for U , the symmetric parameterization [43,44] is advantageous over the PDG method of including the Majorana phases, and it simplifies to the PDG parameterization in the context neutrino oscillations.…”