“…Calculations show that the Ti-terminated surface of STO favors the production of propene (DE a,propene = 145 kJ mol À1 , DE a,acetone = 155 kJ mol À1 )a nd the Sr-terminated surface favors the production of acetone (DE a,propene = 235 kJ mol À1 , DE a,acetone = 149 kJ mol À1 ), which agrees well with our experimental observations. Apparent activation energies were calculated by fitting the Arrhenius equation to kinetic data (see Figure S13 and Table S4) collected under differential conditions (conversion 13 %) [21] and used to compare reactivity data at the same temperature for the five samples:T iO 2 -disk 400 8 8C ,S rO 400 8 8C , STO ðHNO 3 Þ,400 8 8C ,S TO 400 8 8C ,a nd STO 550 8 8C .A pparent activation energies for acetone production on surface-Sr-rich STO (STO 550 8 8C ;1 63 kJ mol À1 )a nd for propene production on as urface-Ti-rich STO sample (STO ðHNO 3 Þ,400 8 8C ;1 30 kJ mol À1 ) showed general agreement with the magnitude of the DFTcalculated activation energies for the RDS,n amely,1 49 and 145 kJ mol À1 ,r espectively.A lthough the good agreement between our DFT barriers of the rate-limiting steps and the experimental apparent activation energies sheds light on the reaction mechanisms at the two different terminations, ap roper reaction kinetic analysis is warranted in the future to firmly establish arelationship between the DFT-predicted mechanism and the experimental kinetic data. Theu niquet unabilityo fr eaction selectivityt hrough induceds urfacet erminationso fS TO is evidentf romacomparison with theindividualsingleoxides.…”