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Based on molecular dynamics simulations of the unimolecular dissociation of energetic
C2H4OH radicals, we have discovered a previously unexplored pathway leading to the formation
of water (H2O) + vinyl (CH2CH)
In this work, based on electronic structure calculations and molecular orbital analysis,
a physical explanation is offered for the observed large decrease in ionization energies in
going from hydroxymethyl to hydroxyethyl radical. The project features the computational
effort of an experimental group supported by iOpenShell.

We investigated the highly debated three-body dissociation of sym-triazine to three HCN products, which depends
on the topology of the excited states' potential energy surfaces.
Electronic states of the uracil dimer.
The benzene dimer cation is a model system for ionized π-stacked aromatic molecules,
which are thought to play an important role in charge transfer processes in biological
systems (e.g. DNA). Using the EOM-IP method, we characterize the ten low-lying
excited states of the benzene dimer cation and determine important relaxation
coordinates.
Ionization of liquid water is of great practical interest in the context of
atmospheric and biological chemistry. The removal of an electron leads to cascade
formation of reactive intermediates that can incur cellular damage. Despite several
decades of research, the nature of the initially formed state and its immediate
dynamics are still poorly understood. We pose a very fundamental question: "What does
it mean to ionize water?"
Studies of alkyl and alkyl peroxy radicals to determine their contribution to ozone
formation.
As a part of spectroscopy modeling unit of programs, we develop a code for wavepacket propagation.
To model angular distributions of photoelectrons, we implemented the
calculation of Dyson orbitals using EOM-IP/EA-CCSD.
Equilibrium structure, vibrational frequencies, and ionization energies of the
para-benzyne radical anion are characterized by coupled-cluster and
equation-of-motion methods. Vibronic interactions with the low-lying excited state result
in a flat potential energy surface along the coupling mode and even in lower-symmetry
C2v structures. Additional complications arise due to Hartree-Fock
instabilities and near-instabilities.
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