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The long-range non-additive three-body dispersion interaction coefficients$Z_{111}$, $Z_{112}$, $Z_{113}$, and $Z_{122}$ are computed for many atomiccombinations using standard expressions. The atoms considered include hydrogen,the rare gases, the alkali atoms (up to Rb) and the alkaline-earth atoms (up toSr). The term $Z_{111}$, arising from three mutual dipole interactions is knownas the Axilrod-Teller-Muto coefficient or the DDD (dipole-dipole-dipole)coefficient. Similarly, the terms $Z_{112}$, $Z_{113}$, and $Z_{122}$ arisefrom the mutual combinations of dipole (1), quadrupole (2), and octupole (3)interactions between atoms and they are sometimes known, respectively, as DDQ,DDO, and DQQ coefficients. Results for the four $Z$ coefficients are given forthe homonuclear trimers, for the trimers involving two like-rare-gas atoms, andfor the trimers with all combinations of the H, He, Li atoms. An exhaustivecompilation of all coefficients between all possible atomic combinations ispresented as supplementary data.

The long-range non-additive three-body dispersion interactions for the rare gases, alkali and alkaline-earth atoms