posted on 2025-02-25, 03:29authored byHyeongtaek Lim, Xinzheng Yang, Christopher B. Larsen, Kathryn Ledbetter, Marija R. Zoric, Sumana L. Raj, Gaurav Kumar, Natalia Powers-Riggs, Matthias C. Hoffmann, Matthieu Chollet, Leland B. Gee, Tim B. van Driel, Roberto Alonso-Mori, Victoria Kabanova, Abdullah Kahraman, Philip J. M. Johnson, Claudio Cirelli, Camila Bacellar, Kelly J. Gaffney, Xiaosong Li, Amy A. Cordones
Highly covalent Ni bis(dithiolene) and related complexes
provide
an ideal platform for investigating the effects of metal–ligand
orbital hybridization on excited state character and dynamics. In
particular, we focus on the ligand field excited states that dominate
the photophysics of first-row transition metal complexes. We investigate
if they can be significantly delocalized off the metal center, possibly
yielding photochemical reactivity more similar to charge transfer
excited states than metal-centered ligand field excited states. Here,
[Ni(mpo)2] (mpo = 2-mercaptopyridine-N-oxide) provides a representative example for the larger chemical
class and is an active electro- and photocatalyst for proton reduction.
A detailed characterization of the excited state electronic structure,
dynamics, and photochemistry of [Ni(mpo)2] is presented
based on ultrafast transient X-ray absorption spectroscopy at the
Ni and S 1s core absorption K-edges. By comparing the ultrafast Ni
K-edge absorption to ab initio calculations, we identify an excited
state relaxation mechanism where an initial ligand-to-metal charge
transfer excitation results in both excited state electron transfer
(generating a catalytically relevant reduced photoproduct [Ni(mpo)2]−) and relaxation to a pseudotetrahedral
triplet ligand field excited state. From the ultrafast S K-edge absorption,
the ligand field excited state is found to be highly delocalized onto
the thiolate ligands, and a tetrahedral structural distortion is shown
to substantially influence the degree of delocalization. The results
identify a significant structural coordinate to target when aiming
to control the excited state covalency in square planar complexes.