Coherent Vibrational Wavepacket Dynamics in Platinum(II) Dimers and Their Implications
journal contributionposted on 27.04.2018, 00:00 by Pyosang Kim, Matthew S. Kelley, Arnab Chakraborty, Nolan L. Wong, Richard P. Van Duyne, George C. Schatz, Felix N. Castellano, Lin X. Chen
Vibrational coherence in the metal–metal-to-ligand-charge transfer (MMLCT) excited state of cyclometalated platinum dimers with a pseudo C2 symmetry was investigated where two nearly degenerate transitions from the highest occupied molecular orbital (metal–metal σ* orbital) to higher energy ligand π* orbitals could be simultaneously induced. We observed oscillatory features in femtosecond degenerate transient absorption (TA) signals from complexes [(ppy)Pt(μ-tBu2pz)]2 (1) and anti-[(ppy)Pt(μ-pyt)]2 (2), which are attributed to coherent nuclear motions that modulate the HOMO (antibonding σ*) energy level, and hence, the energy for the MMLCT transition. The characteristics of such coherent nuclear motions, such as the oscillatory frequency and the dephasing time, differ between 1 and 2 and are explained by mainly two structural factors that could influence the vibrational coherence: the Pt–Pt distance (2.97 Å for 1 vs 2.85 Å for 2) and molecular shape (1 in an “A” frame vs 2 in an “H” frame). Because the electronic coupling between the two Pt atoms determines the energy splitting of the bonding σ and antibonding σ* orbital, the Pt–Pt stretching mode coupled to the MMLCT transition changes the inter Pt distance from that of the ground state. Interestingly, while 1 shows a single Pt–Pt stretching frequency of 120 cm–1 in the MMLCT state, 2 exhibits multiple downshifted frequencies (80 and 105 cm–1) in the MMLCT state along with a shorter vibrational dephasing time than 1. Based on the ground state optimized structures and Raman calculations, the changes evident in the vibrational wavepacket dynamics in 2 are closely correlated with the “H” framed geometry in 2 compared to the “A” frame in 1, leading to the sharp increase in π–π interaction between ppy ligands. Although the TA experiments do not directly reveal the ultrafast intersystem crossing (ISC) because of a strong coherent spike at early time scales, the dependence of the vibrational wavepacket dynamics on molecular geometry can be understood based on previously proposed potential energy surfaces as a function of Pt–Pt distance, suggesting that the interaction between the cyclometalating ligands can be a key factor in determining the Pt–Pt shortening and the related energy relaxation dynamics in the Pt(II) dimers. Further experiments using femtosecond broadband TA and X-ray scattering spectroscopy are planned to investigate directly the ISC and Pt–Pt contraction to support the relationship between ground state molecular geometry and photoinduced structural changes in the Pt(II) dimers.
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energy relaxation dynamicsvibrational dephasing timeMMLCT transition changesvibrational wavepacket dynamicscyclometalated platinum dimersPtC 2 symmetryground state optimized structuresImplications Vibrational coherenceHOMOISCCoherent Vibrational Wavepacket Dynamicsground statefemtosecond broadband TAMMLCT state1 vs 2.85 Å