2006
DOI: 10.1063/1.2137691
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Accurate ab initio potential for the Na+⋯I• complex

Abstract: High-level ab initio calculations employing the multireference configuration interaction and coupled clusters methods with a correlation-consistent sequence of basis sets have been used to obtain accurate potential energy curves for the complex of the sodium cation with the iodine atom. Potential curves for the first two electronic Lambda-S states have very different characters: the potential for the 2pi state has a well depth of approximately 10 kcal/mol, while the 2sigma state is essentially unbound. This di… Show more

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Cited by 8 publications
(11 citation statements)
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“…The experimental values of μ CN and Q are 0.5738 a.u . and 2.536 a.u., respectively. Therefore μ CN Q > 0 and the eigenstates | v ± 〉 at θ = 0 are given as |vΓ3=|j=32 m=32Γ3,|vΓ4=|j=32 m=32Γ4, |v+Γ3=|j=32 m=12Γ3,|v+Γ4=|j=32 m=12Γ4. …”
Section: Resultsmentioning
confidence: 97%
See 1 more Smart Citation
“…The experimental values of μ CN and Q are 0.5738 a.u . and 2.536 a.u., respectively. Therefore μ CN Q > 0 and the eigenstates | v ± 〉 at θ = 0 are given as |vΓ3=|j=32 m=32Γ3,|vΓ4=|j=32 m=32Γ4, |v+Γ3=|j=32 m=12Γ3,|v+Γ4=|j=32 m=12Γ4. …”
Section: Resultsmentioning
confidence: 97%
“…The electrostatic dipole–quadrupole interaction has a time‐reversal symmetry, and the doubly degeneracy is a consequence of Kramers degeneracy for the odd number of electrons on I atom. We obtained the model PECs by substituting the experimental values for μ CN and Q in eq. and compare their functional behaviors with our PECs calculated by COSOCI method in Figures a and 5b.…”
Section: Resultsmentioning
confidence: 99%
“…The SO mixing of the 1 1 E and 2 1 A 1 states of the excited complex gives rise to three SO states, labeled I, II, and III (X is used for the ground state of the I − (CH 3 CN) complex, which is essentially the 1 1 A 1 state); the first two states correlate with the 2 P 3/2 limit of the free iodine atom, whereas the third one correlates with the 2 P 1/2 limit. 81,82 For a complex with cylindrical symmetry, such as Na + We now turn our attention to more quantitative aspects of the photoionization and photoexcitation of I − (CH 3 CN). As we have demonstrated previously, 86 ab initio (MP2) calculations predict binding energies for the binary halide−acetonitrile clusters in excellent agreement with experimental data.…”
Section: Photoexcitation and Photoionization Ofmentioning
confidence: 99%
“…The potential energy curves for the 1 2 E and 1 2 A 1 states of I • (CH 3 CN) have substantially different well depths due to the nonspherical distribution of the electron density of the iodine atom, giving rise to a nonzero quadrupole moment and relatively large differences in the polarizability along different axes. 82 In the lower 1 2 E state, the interaction between acetonitrile and the iodine atom (located on the methyl group side) is relatively strong, with a potential well of ∼50 meV (∼1.2 kcal/mol) at a C−I distance of ∼4 Å (Figure 3). The well depth for the 1 2 A 1 state is only 23 meV (∼0.5 kcal/ mol), and the potential energy minimum is located at a shorter acetonitrile−iodine distance, with r(C−I) = 3.8 Å.…”
Section: Photoexcitation and Photoionization Ofmentioning
confidence: 99%
“…Among these, NaI might be the most thoroughly investigated molecule from both experimental 1-7 and theoretical [8][9][10][11][12][13][14][15][16] points of view. It has been established for diatomic alkali halides that the covalent and ionic potential energy curves ͑PECs͒ cross at an avoided crossing ͑AC͒ point and the covalent and ionic PECs are repulsive and strongly bound, respectively, when the internuclear distance is relatively small.…”
Section: Introductionmentioning
confidence: 99%