Enantio-conversion with the help of electromagnetic fields is an essential issue due to the chiralitydependence of many chemical, biological, and pharmaceutical processes. Here, we propose a method for this issue based on a five-level double-∆ model of chiral molecules. By utilizing the breaking of left-right symmetry in the two ∆-type sub-structures, we can establish the chiral-state-selective excitation with one chiral ground state being excited to an achiral excited state and the other one being undisturbed. In the meanwhile, the achiral excited state will relax to the two chiral ground states. The two effects simultaneously acting on the chiral mixtures can convert molecules of different chiralities to the ones of the same chirality, i.e., the enantio-conversion via optical pumping. With typical parameters in gas-phase experiments, we numerically show that highly efficient enantioconversion can be achieved. Our method works in the appearance of decoherences and without the precise control of pulse-durations (pulse-areas) and/or pulse-shapes. These advantages offer it promising features in promoting the future exploring of enantio-conversion.
I. INTRODUCTIONRecently, the inner-state enantio-purification [1-19], spatial enantio-separation [20-30], and enantiodiscrimination [31][32][33][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49] have become essential issues, since the vast majority of chemical [50], biological [51][52][53], and pharmaceutical [54-57] processes essentially depend on molecular chirality. For these purposes, the (electronic, vibrational, and/or rotational) inner states of chiral molecules are manipulated with the help of electromagnetic fields. Moreover, precisely manipulating the rotational populations of chiral molecules has opened new avenues to study parity violation [58,59].The inner-state enantio-purification includes the enantio-specific state transfer [1-12] and the enantioconversion [13][14][15][16][17][18][19]. It aims to enhance the population excess of one chirality over the other in an inner state in chiral mixtures. The achieved inner-state enantiomeric excess characterizes the efficiency of the inner-state enantiopurification. The enantio-specific state transfer [1][2][3][4][5][6][7][8][9][10][11][12] achieves the enhancement of inner-state enantiomeric excess without changing the chiralities of molecules. The enantio-conversion [13][14][15][16][17][18][19] is more ambitious, since it aims to convert molecules of different chiralities to the ones of the same chirality.Most proposals of the inner-state enantiopurification [1-19] are based on few-level models with left-right symmetry-breaking ∆-type (sub-) structures (e.g. the three-level ∆ type model [1][2][3][4][5][6][7][8][9][10][11][12][13] and the four-level double-∆ [14-19] model). In these models, the chirality-dependency results from the sign difference between the products of the three electric-dipole transition