“…In Figure , the central basis vectors ( x̂ , ŷ , ẑ ), if rotated along the z axis by ϕ and then along the y axis by θ i , can be transformed into the local ones ( x̂ i , ŷ i , ẑ i ): ( x̂ i , ŷ i , ẑ i ) = ( x̂ , ŷ , ẑ ) R z (ϕ) R y (θ i ). Hence, the transmitted light field can be related with the incident one by transformation , bold-italicẼ o u t = R z ( ϕ ) R y ( θ t ) T R y − 1 ( θ i ) R z − 1 ( ϕ ) bold-italicẼ i n = M bold-italicẼ i n Here R y (θ) and R z (ϕ) denote unitary rotations around the y axis by θ and the z axis by ϕ, respectively R y ( θ ) = [ true cos θ 0 sin θ 0 1 0 − sin θ 0 cos θ ] , goodbreak0em0.25em R …”