In the present work, the energy relaxation process in doped solid matrices is studied. The photoexcitation of NO molecule to its first electronic Rydberg state, being trapped in argon, neon and parahydrogen (pH2) cryogenic solids, is considered. Classical molecular dynamics (MD) simulations were used by applying a quantum correction for the temperature using anharmonic approach. Potential energy surfaces (PESs) recently performed for the NO–Ne, NO–Ar and NO–H2 systems have been used, with the aim to describe the dynamical response of the solid matrices upon NO photoexcitation. MD simulations partially reproduced the experimental results. In the case of the NO–Ne system, the results totally agree with a previous work. These are the first res...
Molecular orbital theory and calculations are used to describe the ultraviolet singlet excited state...
We report new global potential energy surfaces (PESs) for the D-0 and D-1 states of NO3. The PESs ar...
We report new accurate ab initio potential energy surfaces (PESs) for the ground (X˜2A1) and fi...
New time and energy resolved data on vibrationally relaxed and unrelaxed emissions from the valence ...
Fluorescence (phosphorescence) excitation spectra as well as luminescence spectra and decay times we...
A model assuming simple analytical forms for potential curves and coupling matrix elements is used t...
Electronic and vibrational relaxation of NO in Ar, Kr and Xe matrices has been studied using excitat...
The rebinding of NO to myoglobin after photolysis is studied using the 'reactive molecular dynamics'...
In the present work we studied the immediate medium response to the excitation to the $A(3s\sigma)$...
Electronic and vibrational relaxationsof NO in Ar, Kr, and Xe matrixes were studied using excitation...
SIGLECopy held by FIZ Karlsruhe; available from UB/TIB Hannover / FIZ - Fachinformationszzentrum Kar...
Mol.-dynamics simulations of structural relaxation in electronically excited NO-doped solid neon are...
We study the ultrafast dynamics of structural relaxation induced by the Rydberg excitation of an NO ...
Several new progressions consisting of broadbands have been observed in the absorption spectra of NO...
The photoion excitation spectrum of NO has been measured in the 9.26-13.8 eV region using synchrotro...
Molecular orbital theory and calculations are used to describe the ultraviolet singlet excited state...
We report new global potential energy surfaces (PESs) for the D-0 and D-1 states of NO3. The PESs ar...
We report new accurate ab initio potential energy surfaces (PESs) for the ground (X˜2A1) and fi...
New time and energy resolved data on vibrationally relaxed and unrelaxed emissions from the valence ...
Fluorescence (phosphorescence) excitation spectra as well as luminescence spectra and decay times we...
A model assuming simple analytical forms for potential curves and coupling matrix elements is used t...
Electronic and vibrational relaxation of NO in Ar, Kr and Xe matrices has been studied using excitat...
The rebinding of NO to myoglobin after photolysis is studied using the 'reactive molecular dynamics'...
In the present work we studied the immediate medium response to the excitation to the $A(3s\sigma)$...
Electronic and vibrational relaxationsof NO in Ar, Kr, and Xe matrixes were studied using excitation...
SIGLECopy held by FIZ Karlsruhe; available from UB/TIB Hannover / FIZ - Fachinformationszzentrum Kar...
Mol.-dynamics simulations of structural relaxation in electronically excited NO-doped solid neon are...
We study the ultrafast dynamics of structural relaxation induced by the Rydberg excitation of an NO ...
Several new progressions consisting of broadbands have been observed in the absorption spectra of NO...
The photoion excitation spectrum of NO has been measured in the 9.26-13.8 eV region using synchrotro...
Molecular orbital theory and calculations are used to describe the ultraviolet singlet excited state...
We report new global potential energy surfaces (PESs) for the D-0 and D-1 states of NO3. The PESs ar...
We report new accurate ab initio potential energy surfaces (PESs) for the ground (X˜2A1) and fi...