The effects of lithium doping on the nonlinear optical properties of new electrodes (lithium-doped corannulene) were investigated in detail. Nine dynamically stable geometries of Li n -C 20 H 10 (n=1, 2) are predicted by B3LYP/6-31G (d,p). Among these nine structures, the largest first static hyperpolarizability ( 0 ) is computed to be 15314 au, which is dramatically larger than the 0 value of 74 au for C 20 H 10 , indicating that Li doping plays an important role in elevating the first hyperpolarizability of corannulene. The extensive number of works that have been performed over the past two decades to investigate the nonlinear optical (NLO) properties of novel NLO materials [1][2][3][4][5][6][7] have been devoted to discovering the important/key influencing factors that can lead to dramatic increases in the first hyperpolarizability [8]. The strategies used mainly focused on utilizing molecules that contain extended -electron systems [9] or that can be characterized as planar donor--conjugated bridge-acceptor (D--A) types [10,11] [29]. Corannulene can be thought of as the upper third of a C 60 molecule with the valences of the outermost atoms saturated by H atoms. The molecule resembles a shallow bowl with C 5v symmetry (Figure 1) and the six-membered rings at the periphery lie significantly out of the plane. C 20 H 10 exhibits a number of interesting properties [30,31] and its complexes with ions or atoms, such as alkaline cations or transition metal atoms [32][33][34][35], have been studied both experimentally and theoretically. Following the discussion above, we investigated corannulene molecules with Li doping for the design of novel NLO materials.In the current work, to investigate the effect of Li doping on the NLO properties of corannulene, we predict the structural and electronic properties of Li n -C 20 H 10 (n=1, 2) at the atomic level. It is found that the large hyperpolarizabilities of Li n -C 20 H 10 (n=1, 2) strongly depend upon the concentration and position of the Li atoms.