The paper is based on relations between a ternary symmetric form defining the SO ( 3 ) geometry in dimension five and Cartanâs works on isoparametric hypersurfaces in spheres. As observed by Bryant such a ternary form exists only in dimensions n k = 3 k + 2 , where k = 1 , 2 , 4 , 8 . In these dimensions it reduces the orthogonal group to the subgroups H k â SO ( n k ) , with H 1 = SO ( 3 ) , H 2 = SU ( 3 ) , H 4 = Sp ( 3 ) and H 8 = F 4 . This enables studies of special Riemannian geometries with structure groups H k in dimensions n k . The necessary and sufficient conditions for the H k geometries to admit the characteristic connection are given. As an illustration nontrivial examples of SU ( 3 ) geometries in dimension 8 admitting characteristic connection are provided. Among them are the examples having nonvanishing torsion and satisfying Einstein equations with respect to either the Levi-Civita or the characteristic connections. The torsionless models for the H k geometries have the respective symmetry groups G 1 = SU ( 3 ) , G 2 = SU ( 3 ) Ă SU ( 3 ) , G 3 = SU ( 6 ) and G 4 = E 6 . The groups H k and G k constitute a part of the âmagic squareâ for Lie groups. The âmagic squareâ Lie groups suggest studies of ten other classes of special Riemannian geometries. Apart from the two exceptional cases, they have the structure groups U ( 3 ) , S ( U ( 3 ) Ă U ( 3 ) ) , U ( 6 ) , E 6 Ă SO ( 2 ) , Sp ( 3 ) Ă SU ( 2 ) , SU ( 6 ) Ă SU ( 2 ) , SO ( 12 ) Ă SU ( 2 ) and E 7 Ă SU ( 2 ) and should be considered in respective dimensions 12, 18, 30, 54, 28, 40, 64 and 112. The two âexceptionalâ cases are: SU ( 2 ) Ă SU ( 2 ) geometries in dimension 8 and SO ( 10 ) Ă SO ( 2 ) geometries in dimension 32. The case of SU ( 2 ) Ă SU ( 2 ) geometry in dimension 8 is examined closer. We determine the tensor that reduces SO ( 8 ) to SU ( 2 ) Ă SU ( 2 ) leaving the more detailed studies of the geometries based on the magic square ideas to the forthcoming paper.