2006
DOI: 10.1016/j.cplett.2006.03.043
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Structure and energetics of LiF chains as a model for low dimensional alkali halide nanocrystals

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Cited by 9 publications
(8 citation statements)
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“…They can also be helpful in the interpretation of experiments by providing details of the geometrical configurations and of the electronic density distribution. The structure of LiF chains 15 and of LiF clusters have been analyzed theoretically at different levels, [16][17][18][19][20][21] e.g., ab initio calculations using the Hartree-Fock method, 18,19 a perturbed ion model, 20 and density functional theory (DFT). 12,21 In particular, the three-atom member structure, (LiF)Li + , was predicted to be linear.…”
Section: Introductionmentioning
confidence: 99%
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“…They can also be helpful in the interpretation of experiments by providing details of the geometrical configurations and of the electronic density distribution. The structure of LiF chains 15 and of LiF clusters have been analyzed theoretically at different levels, [16][17][18][19][20][21] e.g., ab initio calculations using the Hartree-Fock method, 18,19 a perturbed ion model, 20 and density functional theory (DFT). 12,21 In particular, the three-atom member structure, (LiF)Li + , was predicted to be linear.…”
Section: Introductionmentioning
confidence: 99%
“…They can also be helpful in the interpretation of experiments by providing details of the geometrical configurations and of the electronic density distribution. The structure of LiF chains and of LiF clusters have been analyzed theoretically at different levels, e.g., ab initio calculations using the Hartree−Fock method, , a perturbed ion model, and density functional theory (DFT). , In particular, the three-atom member structure, (LiF)Li + , was predicted to be linear. , Aguado et al have found that the magic numbers for all alkali halides are n = 4, 6, and 9 independently of the specific ground-state geometry . Yokoyama et al and Haketa et al, using DFT calculations, proposed several structures for the (LiF) n Li 0 and (LiF) n Li + clusters, n = 1−4, and remarked that (LiF)Li 0 stability is achieved either for the F nucleus in between the two Li nuclei or in one extremity of the molecule, while for larger structures ( n > 2) the odd electron is always localized.…”
Section: Introductionmentioning
confidence: 99%
“…Subsequent computational studies ,, investigated the growth and stability of different isomers of LiF clusters by sequential stacking of cubic or ring building blocks leading to the formation of cuboid and ringlike structures. LiF growth mode using a chain building block has also been attempted leading to the formation of low-dimensional nanocrystals . It is worth noting that bulk LiF crystalizes in the cubic NaCl type structure with a lattice parameter of 4.03 Å, leading to the speculation that a cuboid growth mode might be the most favorable.…”
Section: Introductionmentioning
confidence: 99%
“…LiF growth mode using a chain building block has also been attempted leading to the formation of low-dimensional nanocrystals. 11 It is worth noting that bulk LiF crystalizes in the cubic NaCl type structure with a lattice parameter of 4.03 Å, leading to the speculation that a cuboid growth mode might be the most favorable. Interestingly, most of the previous investigations agreed that neutral isomers of Li n F n clusters prefer the ringlike growth mode with rare emergence of the cuboid structures at specific cluster sizes.…”
Section: Introductionmentioning
confidence: 99%
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