“…Furthermore, we already note in lemma 3.4, that ρ * (C 2 ) acts on each irreducible component as a scalar multiple of identity with the same eigenvalue. Finally, to prove our holonomy criterion, we only have to examine the eigenvalues of ρ * (C 4 ) on the irreducible components of the spin representation of K. Those eigenvalues may be computed with the help of a formula given in [CGH00]. Denoting by (e 1 , e 2 , e 3 , e 4 ) the standard basis of R 4 , the root system of F 4 is the set of elements x = 4 i=1 x i e i with integer or half-integer coordinates in R 4 such that x 2 = 1 or 2, [Hum72], [BMP85].…”