TY - JOUR
T1 - Structural, Spectroscopic, and Dynamic Properties of Li2+(X2 ∑g+) in Interaction with Krypton Atom
AU - Saidi, Samah
AU - Mabrouk, Nesrine
AU - Dhiflaoui, Jamila
AU - Berriche, Hamid
N1 - Publisher Copyright:
© 2023 by the authors.
PY - 2023/7
Y1 - 2023/7
N2 - We report a computational study of the potential energy surface (PES) and vibrational bound states for the ground electronic state of (Formula presented.). The PES was calculated in Jacobi coordinates at the Restricted Coupled Cluster method RCCSD(T) level of calculation and using aug-cc-pVnZ (n = 4 and 5) basis sets. Afterward, this PES is extrapolated to the complete basis set (CBS) limit for correction. The obtained interaction energies were, then, interpolated numerically using the reproducing kernel Hilbert space polynomial (RKHS) approach to produce analytic expressions for the 2D-PES. The analytical PES is used to solve the nuclear Schrodinger equation to determine the bound states’ eigenvalues of (Formula presented.) for a (Formula presented.) = 0 total angular momentum configuration and to understand the effects of orientational anisotropy of the forces and the interplay between the repulsive and attractive interaction within the potential surface. In addition, the radial and angular distributions of some selected bound state levels, which lie below, around, and above the T-shaped 90° barrier well, are calculated and discussed. We note that the radial distributions clearly acquire a more complicated nodal structure and correspond to bending and stretching vibrational motions “mode” of the (Formula presented.) atom along the radial coordinate, and the situation becomes very different at the highest bound states levels with energies higher than the T-shaped 90° barrier well. The shape of the distributions becomes even more complicated, with extended angular distributions and prominent differences between even and odd states.
AB - We report a computational study of the potential energy surface (PES) and vibrational bound states for the ground electronic state of (Formula presented.). The PES was calculated in Jacobi coordinates at the Restricted Coupled Cluster method RCCSD(T) level of calculation and using aug-cc-pVnZ (n = 4 and 5) basis sets. Afterward, this PES is extrapolated to the complete basis set (CBS) limit for correction. The obtained interaction energies were, then, interpolated numerically using the reproducing kernel Hilbert space polynomial (RKHS) approach to produce analytic expressions for the 2D-PES. The analytical PES is used to solve the nuclear Schrodinger equation to determine the bound states’ eigenvalues of (Formula presented.) for a (Formula presented.) = 0 total angular momentum configuration and to understand the effects of orientational anisotropy of the forces and the interplay between the repulsive and attractive interaction within the potential surface. In addition, the radial and angular distributions of some selected bound state levels, which lie below, around, and above the T-shaped 90° barrier well, are calculated and discussed. We note that the radial distributions clearly acquire a more complicated nodal structure and correspond to bending and stretching vibrational motions “mode” of the (Formula presented.) atom along the radial coordinate, and the situation becomes very different at the highest bound states levels with energies higher than the T-shaped 90° barrier well. The shape of the distributions becomes even more complicated, with extended angular distributions and prominent differences between even and odd states.
KW - radial and angular distributions
KW - RCCSD(T) method
KW - RKHS interpolation
KW - vibrational quantum bound states
UR - https://www.scopus.com/pages/publications/85166260075
U2 - 10.3390/molecules28145512
DO - 10.3390/molecules28145512
M3 - Article
AN - SCOPUS:85166260075
SN - 1420-3049
VL - 28
JO - Molecules
JF - Molecules
IS - 14
M1 - 5512
ER -