Abstract
The encapsulation of a water molecule within two open-cage [59]fullerenones with 18-membered-ring ( 1) or 19-membered-ring orifices ( 2) is studied by DFT with empirical dispersion terms. The equilibrium structure of each H 2O@[59]fullerenone and the transition-state structure for the water molecule leaving the cage are optimised and the counterpoise-corrected binding energy and barrier height are calculated. While the H 2O binding energies in H 2O@ 1 and H 2O@ 2 are almost equal, the barrier for H 2O leaving the cage is much higher for 1 (108 kJ mol −1) than for 2 (46 kJ mol −1). A water molecule can enter the cage-opened fullerenone 2 almost barrierless, whereas this barrier is 63 kJ mol −1 in 1.
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