“…First, it is a simple limit of multi-orbital models such as those used to describe transition metal oxides [9][10][11], graphene's SU(4) spin-valley symmetry [12], and twisted-bilayer graphene [13][14][15][16][17]. Second, the SU(N ) FHM is predicted to display a variety of interesting and exotic phases even in very special limits, such as: the conventional N = 2 FHM, the N = 3 FHM [18][19][20][21][22][23][24][25][26][27], the N = 4 FHM at quarter filling [28,29], even values of N at half-filling [30][31][32][33][34][35][36][37], special N → ∞ limits [38][39][40][41][42], 1D chains [43][44][45][46][47][48][49], and the Heisenberg limit for N = 3, 4, 5 [10,26,[50][51][52][53]…”