Oxynitrides are promising visible-light-responsive photocatalysts,b ut their structures are almost confined with three-dimensional (3D) structures such as perovskites.A phase-pure Li 2 LaTa 2 O 6 Nw ith al ayered perovskite structure was successfully prepared by thermal ammonolysis of al ithium-richo xide precursor.L i 2 LaTa 2 O 6 Ne xhibited high crystallinity and visible-light absorption up to 500 nm. As opposed to well-known 3D oxynitride perovskites,L i 2 LaTa 2 O 6 Ns upported by abinuclear Ru II complex was capable of stably and selectively converting CO 2 into formate under visible light (l > 400 nm). Transient absorption spectroscopyi ndicated that, as compared to 3D oxynitrides,L i 2 LaTa 2 O 6 Np ossesses al ower density of mid-gap states that work as recombination centers of photogenerated electron/hole pairs,b ut ah igher density of reactive electrons,w hichi sr esponsible for the higher photocatalytic performance of this layered oxynitride.Semiconductor materials that can split water into H 2 and O 2 as photocatalysts have been extensively explored and developed.[1] Recently,t he research interest is being expanded to CO 2 reduction, but it is generally very difficult to achieve the reaction because of the lack of active sites for CO 2 reduction on the surface as well as the predominant occurrence of competitive H 2 evolution reaction.[2] Some layered perovskite oxides consisting of Ti 4+ ,N b
5+,a nd Ta 5+ have been regarded as high-potential photocatalysts for water splitting and CO 2 reduction. [3,4] Since most of metal oxide photocatalysts have large band gaps (> 3eV) and are hence inactive under visible light (l > 400 nm), [5] mixed-anion compounds such as oxynitrides have attracted considerable attention as potential visible-lightresponsive photocatalysts toward solar energy conversion. [6,7] While nitrogen-doping into oxides is aconventional and facile