“…Therefore, the energy degeneracy between the − K and + K valleys is removed so that the valley polarized state is realized in the conduction band of Li@2H-TiTe 2 rather than in the frequently reported valence band of other ferrovalley materials. Remarkably, the valley polarization with a fully clean energy window reaches as sizable as 160 meV, which is larger than or comparable to that reported in monolayers VSe 2 (78.2 meV), 11 FeClBr (188 meV), 14 LaH 2 (137 meV), 15 Cr 2 COF MXene (291/379 meV), 16 CeI 2 (208 meV), 17 2H-RuCl 2 (240 meV), 18 CrHfN 2 Cl 2 (55 meV), 19 RuClX (X = F, Br) (194/226 meV), 20 Fe(OH) 2 (67 meV), 21 VSSe (85 meV), 29 and VClBr (70 meV). 30 It is noteworthy that the valley polarization of the conduction band will be reversed when the magnetization points to the − z direction, as shown in Fig.…”