“…Note that we have defined the complex combination of X m by (φ 1 , φ 2 ) = (X 1 + iX 2 , X 3 + iX 4 ), and that the fermions are expressed as 6D Weyl spinors, which have 4 complex components. As in the previous paper [16], we do not use the SU(2) Majorana convention, for we prefer unconstrained fermions for the loop calculations. The subscripts on the spinors θ + , θ − denote the positive and negative 6D chiralities, respectively (γθ ± = ±θ ± , where γ = γ 0 γ 1 .…”