2016
DOI: 10.1021/acs.jpcc.6b07845
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Unraveling the Apparent Dimerization Tendency in Small Mon Clusters with n = 3–10

Abstract: The geometric, electronic, and magnetic properties of Mo n clusters, with n = 3−10, are investigated from a computational point of view. Calculations are carried out using gradient-corrected density functional theory, a small core pseudopotential to represent inner electrons, and a tripleζ basis set to describe the 4s, 4p, 4d, and 5s valence atomic orbitals. The geometries of the ground states for every cluster size are distorted versions of the familiar structures adopted by transition metal aggregates. Both … Show more

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Cited by 7 publications
(2 citation statements)
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References 16 publications
(25 reference statements)
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“…The distorted trigonal bipyramid (DTB) conformation of Mo 5 in singlet is the most stable structure and this is consistent with the previous predictions and the application of small core pseudopotential in predicting small Mo clusters was proposed in those works. 37,38 The energy of triplet DTB Mo 5 is only 3.70 kcal/mol higher than that of the singlet state. The most stable structure of Ni 5 [square pyramid (SP)] is different from that predicted by B3LYP 39 while similar to the one with GGA functionals.…”
Section: Resultsmentioning
confidence: 96%
“…The distorted trigonal bipyramid (DTB) conformation of Mo 5 in singlet is the most stable structure and this is consistent with the previous predictions and the application of small core pseudopotential in predicting small Mo clusters was proposed in those works. 37,38 The energy of triplet DTB Mo 5 is only 3.70 kcal/mol higher than that of the singlet state. The most stable structure of Ni 5 [square pyramid (SP)] is different from that predicted by B3LYP 39 while similar to the one with GGA functionals.…”
Section: Resultsmentioning
confidence: 96%
“…La cuarta columna consigna el número entero de átomos de Co que entran dentro de dicho rango, y la ultima columna contiene las estequiometrías resultantes. Partiendo de las estructuras obtenidas en el capítulo anterior y de estructuras bien conocidas para clústers puros de Mo [65,71], se calcularon los isómeros de menor energía para cada tamaño. Para generar las geometrías de partida se tomaron los isómeros de menor energía de cada tamaño para las geometrías originales, reemplazando cada posición no equivalente con átomos de Co, generando todas las permutaciones posibles, hasta llegar a la estequeometria deseada.…”
Section: Clústers De Mo Y Counclassified