International audienceWe propose a new canonical perturbation procedure, based on Van Vleck's theory, for investigating nonadiabatic (i.e., non Born–Oppenheimer) dynamics. The basic idea is to let the unitary transformations depend on the matrix representations of angular momentum operators. The new procedure is applied to a simple model with two 2-dimensional diabatic electronic surfaces coupled by a λq term, which to some extent mimicks the bending and antisymmetric stretching degrees of freedom of NO2 in the ground and first excited electronic states. It is shown that the anharmonicities induced in the lowest surface by the coupling to the excited one are very precisely obtained from the proposed procedure
After photoexcitation, molecules can follow many different paths for electronic relaxation. Of these...
After photoexcitation, molecules can follow many different paths for electronic relaxation. Of these...
We report new accurate ab initio potential energy surfaces (PESs) for the ground (X˜2A1) and fi...
International audienceWe propose a new canonical perturbation procedure, based on Van Vleck's theory...
International audienceWe propose a new canonical procedure for investigating non-Born–Oppenheimer dy...
International audienceThis article proposes an unified presentation of recent results dealing with c...
Canonical Perturbation theory is a powerful tool in the field of molecular physics. It consists of a...
accepted for publication in J. Chem. Phys.We use the effective Hamiltonian that we recently fitted a...
International audienceIn this paper effects of higher order Jahn-Teller coupling terms on the nonadi...
International audienceCanonical perturbation theory (CPT) is a powerful tool in the field of molecul...
Performing molecular dynamics in electronically excited states requires the inclusion of nonadiabati...
The nonadiabatic couplings which arise when two potential energy surfaces of a polyatomic molecule g...
Chemical relaxation phenomena, including photochemistry and electron transfer processes, form a vigo...
A method for computing coupled, diabatic state representations of the lowest electronic states coupl...
Author Institution: Laboratoire de Spectrometrie Physique (CNRS UMR5588), Universite Joseph Fourier ...
After photoexcitation, molecules can follow many different paths for electronic relaxation. Of these...
After photoexcitation, molecules can follow many different paths for electronic relaxation. Of these...
We report new accurate ab initio potential energy surfaces (PESs) for the ground (X˜2A1) and fi...
International audienceWe propose a new canonical perturbation procedure, based on Van Vleck's theory...
International audienceWe propose a new canonical procedure for investigating non-Born–Oppenheimer dy...
International audienceThis article proposes an unified presentation of recent results dealing with c...
Canonical Perturbation theory is a powerful tool in the field of molecular physics. It consists of a...
accepted for publication in J. Chem. Phys.We use the effective Hamiltonian that we recently fitted a...
International audienceIn this paper effects of higher order Jahn-Teller coupling terms on the nonadi...
International audienceCanonical perturbation theory (CPT) is a powerful tool in the field of molecul...
Performing molecular dynamics in electronically excited states requires the inclusion of nonadiabati...
The nonadiabatic couplings which arise when two potential energy surfaces of a polyatomic molecule g...
Chemical relaxation phenomena, including photochemistry and electron transfer processes, form a vigo...
A method for computing coupled, diabatic state representations of the lowest electronic states coupl...
Author Institution: Laboratoire de Spectrometrie Physique (CNRS UMR5588), Universite Joseph Fourier ...
After photoexcitation, molecules can follow many different paths for electronic relaxation. Of these...
After photoexcitation, molecules can follow many different paths for electronic relaxation. Of these...
We report new accurate ab initio potential energy surfaces (PESs) for the ground (X˜2A1) and fi...