Excited state non-adiabatic dynamics of the smallest polyene, trans 1,3-butadiene. I. Time-resolved photoelectron-photoion coincidence spectroscopy

Andrey E Boguslavskiy; Oliver Schalk; Niklas Gador; William J Glover; Toshifumi Mori; Thomas Schultz; Michael S Schuurman; Todd J Martínez; Albert Stolow

doi:10.1063/1.5016452

Excited state non-adiabatic dynamics of the smallest polyene, trans 1,3-butadiene. I. Time-resolved photoelectron-photoion coincidence spectroscopy

J Chem Phys. 2018 Apr 28;148(16):164302. doi: 10.1063/1.5016452.

Authors

Andrey E Boguslavskiy¹, Oliver Schalk¹, Niklas Gador¹, William J Glover², Toshifumi Mori², Thomas Schultz³, Michael S Schuurman¹, Todd J Martínez², Albert Stolow¹

Affiliations

¹ National Research Council Canada, 100 Sussex Drive, Ottawa, Ontario K1A 0R6, Canada.
² Department of Chemistry and PULSE Institute, Stanford University, Stanford, California 94305, USA.
³ Ulsan National Institute of Science and Technology, Ulju-gun, Ulsan 44919, South Korea.

PMID: 29716221
DOI: 10.1063/1.5016452

Abstract

The ultrafast excited state dynamics of the smallest polyene, trans-1,3-butadiene, were studied by femtosecond time-resolved photoelectron-photoion coincidence (TRPEPICO) spectroscopy. The evolution of the excited state wavepacket, created by pumping the bright ¹B_u (ππ*) electronic state at its origin of 216 nm, is projected via one- and two-photon ionization at 267 nm onto several ionization continua. The results are interpreted in terms of Koopmans' correlations and Franck-Condon factors for the excited and cationic states involved. The known predissociative character of the cation excited states is utilized to assign photoelectron bands to specific continua using TRPEPICO spectroscopy. This permits us to report the direct observation of the famously elusive S₁(2¹A_g) dark electronic state during the internal conversion of trans 1,3-butadiene. Our phenomenological analysis permits the spectroscopic determination of several important time constants. We report the overall decay lifetimes of the 1¹B_u and 2¹A_g states and observe the re-appearance of the hot ground state molecule. We argue that the apparent dephasing time of the S₂(1¹B_u) state, which leads to the extreme breadth of the absorption spectrum, is principally due to large amplitude torsional motion on the ¹B_u surface in conjunction with strong non-adiabatic couplings via conical intersections, whereupon nuclear wavepacket revivals to the initial Franck-Condon region become effectively impossible. In Paper II [W. J. Glover et al., J. Chem. Phys. 148, 164303 (2018)], ab initio multiple spawning is used for on-the-fly computations of the excited state non-adiabatic wavepacket dynamics and their associated TRPEPICO observables, allowing for direct comparisons of experiment with theory.