“…(2) If one starts with an odd spectral triple (A, H, D), i,e. without the grading operator, then one can construct an even spectral triple (A, H = H ⊗C 2 , D, γ) using any two 2×2 Pauli spin matrices such that Ω • D (A) ∼ = Ω • D (A) as dgas (Lemma 2.7 in [5]). Therefore, when working with Dirac dga, one can w.l.o.g.…”