Abstract:We present pseudo-potential calculations of geometrical structures of stable isomers of LiAr n clusters with both an electronic ground state and excited states of the lithium atom. The Li atom is perturbed by argon atoms in LiAr n clusters. Its electronic structure obtained as the eigenfunctions of a single-electron operator describing the electron in the field of a Li ? Ar n core, the Li ? and Ar atoms are replaced by pseudo-potentials. These pseudo-potentials include core-polarization operators to account fo… Show more
“…The isomers of low energy that were found in the present work are shown in Figure 1. Their structure is similar to that reported for LiAr n 23 and NaAr n 22 clusters. Except for the lowest isomer of KAr 10 , K is indeed located at the surface of a close-pack Ar cluster.…”
Section: ■ Results and Discussionsupporting
confidence: 85%
“…The electron problem thus reduces in alkali-rare clusters to that of a single electron (the valence electron of the alkali atom) and can be treated very simply at the Hartree–Fock level. This methodology, which we call the one-electron model, was recently applied to simulate the absorption spectrum of Li and Na in small argon clusters. , …”
Section: Introductionmentioning
confidence: 99%
“…This methodology, which we call the one-electron model, was recently applied to simulate the absorption spectrum of Li and Na in small argon clusters. 22,23 The present work associates the one-electron model to an MC exploration of the ground-state phase space to simulate the absorption spectrum of a single potassium atom bound to a few argon atoms. These spectra, used as a tool to explore local structures about the K atom and the onset of large-amplitude motions in KAr n (n = 1−10) clusters, are simulated at cluster temperatures between 2 and 25 K.…”
Photoabsorption spectra of KArn (n = 1-10) are simulated at temperatures ranging between 5 and 25 K. The calculations associate a Monte Carlo (MC) method to sample cluster geometries at temperature T, with a one-electron ab initio model to calculate the ground-state and excited-state energies of the cluster. The latter model replaces the K(+) core electrons and all the electrons of the Ar atoms by appropriate pseudopotentials, complemented by core polarization potentials. It also provides the necessary oscillator strengths to simulate the spectra. Global optimization by basin-hopping is used in combination with MC simulation at low temperature (5 K) to identify the most stable isomer and remarkable isomers of ground-state KArn clusters, which are stable with respect to deformations of the order of those expected with Zero Point Energy motions. The absorption spectra calculated for each of these isomers at 5 K suggest that absorption spectroscopy can probe sensitively the local environment of K atom: surface location of K with respect to a close-packed Ar moiety, number of Ar atom in close vicinity, and local symmetry about K. Simulation at increasing temperatures, up to the evaporation limit of K out of the cluster, shows the onset of large amplitude motions above 20 K, when the K atom experiences a variety of local environments.
“…The isomers of low energy that were found in the present work are shown in Figure 1. Their structure is similar to that reported for LiAr n 23 and NaAr n 22 clusters. Except for the lowest isomer of KAr 10 , K is indeed located at the surface of a close-pack Ar cluster.…”
Section: ■ Results and Discussionsupporting
confidence: 85%
“…The electron problem thus reduces in alkali-rare clusters to that of a single electron (the valence electron of the alkali atom) and can be treated very simply at the Hartree–Fock level. This methodology, which we call the one-electron model, was recently applied to simulate the absorption spectrum of Li and Na in small argon clusters. , …”
Section: Introductionmentioning
confidence: 99%
“…This methodology, which we call the one-electron model, was recently applied to simulate the absorption spectrum of Li and Na in small argon clusters. 22,23 The present work associates the one-electron model to an MC exploration of the ground-state phase space to simulate the absorption spectrum of a single potassium atom bound to a few argon atoms. These spectra, used as a tool to explore local structures about the K atom and the onset of large-amplitude motions in KAr n (n = 1−10) clusters, are simulated at cluster temperatures between 2 and 25 K.…”
Photoabsorption spectra of KArn (n = 1-10) are simulated at temperatures ranging between 5 and 25 K. The calculations associate a Monte Carlo (MC) method to sample cluster geometries at temperature T, with a one-electron ab initio model to calculate the ground-state and excited-state energies of the cluster. The latter model replaces the K(+) core electrons and all the electrons of the Ar atoms by appropriate pseudopotentials, complemented by core polarization potentials. It also provides the necessary oscillator strengths to simulate the spectra. Global optimization by basin-hopping is used in combination with MC simulation at low temperature (5 K) to identify the most stable isomer and remarkable isomers of ground-state KArn clusters, which are stable with respect to deformations of the order of those expected with Zero Point Energy motions. The absorption spectra calculated for each of these isomers at 5 K suggest that absorption spectroscopy can probe sensitively the local environment of K atom: surface location of K with respect to a close-packed Ar moiety, number of Ar atom in close vicinity, and local symmetry about K. Simulation at increasing temperatures, up to the evaporation limit of K out of the cluster, shows the onset of large amplitude motions above 20 K, when the K atom experiences a variety of local environments.
“…Then, we achieved one and two-electron calculations of the electronic states of the Sr + Kr and SrKr molecules, respectively. For the SrKr diatomic molecules, we employed a full Configurations Interaction (full-CI) employing the CIPSI algorithm, (Configuration Interaction by Perturbation of a multi-configuration wave function Selected Iteratively) [59][60][61][62][63].…”
Section: Methodsmentioning
confidence: 99%
“…The hamiltonian for the Sr + Kr and SrKr molecular systems is described by the following equation [61,62]:…”
A computational study of the electronic structure of the SrKr and Sr+Kr molecular systems is presented in this paper. The computational scheme is based on the Full Configuration Interaction (FCI) method and semi-empirical pseudo-potential approach of the atomic core Sr2+ with Gaussian-type-orbital (GTO) basis sets. We have calculated the potential energy surfaces (PESs), spectroscopic parameters, electric dipole moments, and the vibrational levels' spacing for the electronic states of the SrKr molecule and its Sr+Kr ion. The accuracy of the current spectroscopic results is discussed by comparing them tothe available experimental and theoretical data. It is interesting to note that the relevant data of the Sr+Kr molecular ion show significant shapes in the higher 2Σ+ electric states, which allows us to check the intense transition in electric dipole moment and to carry out a diabatic investigation in the future.
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