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Theoretical Ionization Energies and Geometries for Ni sub n (4 < = n < = 9)
Ionization energies for Ni clusters with four to nine atoms have been calculated and compared to recent experiments. Two different models have been tried, both of them relying on a clear identification of 3d derived and 4s,4p derived orbitals. In the first model, used previously for Cu clusters, all...
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Published in: | Journal of physical chemistry (1952) 1992-04, Vol.96 (9), p.3633-3640 |
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container_issue | 9 |
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container_title | Journal of physical chemistry (1952) |
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creator | Nygren, M A Siegbahn, P E M Wahlgren, U Akeby, H |
description | Ionization energies for Ni clusters with four to nine atoms have been calculated and compared to recent experiments. Two different models have been tried, both of them relying on a clear identification of 3d derived and 4s,4p derived orbitals. In the first model, used previously for Cu clusters, all metal atoms are described as effective one-electron systems and a 4s,4p electron is ionized. In the second model, 3d ionization is considered by describing one metal atom at the all-electron level. It is shown that the second model is required to explain the absence of odd--even oscillations in the experimental ionization measurements. It is also argued that the fact that the outermost ionization sometimes occurs from a 3d orbital is not in conflict with a model where the 3d orbitals only make small contributions to the binding of the cluster. The calculations show, in agreement with experiment, that the Ni sub 6 cluster is the only one of the investigated clusters which has an ionization energy > 6.2 eV and which is thus out of reach for the laser source used in the experiments. |
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Two different models have been tried, both of them relying on a clear identification of 3d derived and 4s,4p derived orbitals. In the first model, used previously for Cu clusters, all metal atoms are described as effective one-electron systems and a 4s,4p electron is ionized. In the second model, 3d ionization is considered by describing one metal atom at the all-electron level. It is shown that the second model is required to explain the absence of odd--even oscillations in the experimental ionization measurements. It is also argued that the fact that the outermost ionization sometimes occurs from a 3d orbital is not in conflict with a model where the 3d orbitals only make small contributions to the binding of the cluster. The calculations show, in agreement with experiment, that the Ni sub 6 cluster is the only one of the investigated clusters which has an ionization energy > 6.2 eV and which is thus out of reach for the laser source used in the experiments.</description><identifier>ISSN: 0022-3654</identifier><language>eng</language><ispartof>Journal of physical chemistry (1952), 1992-04, Vol.96 (9), p.3633-3640</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784</link.rule.ids></links><search><creatorcontrib>Nygren, M A</creatorcontrib><creatorcontrib>Siegbahn, P E M</creatorcontrib><creatorcontrib>Wahlgren, U</creatorcontrib><creatorcontrib>Akeby, H</creatorcontrib><title>Theoretical Ionization Energies and Geometries for Ni sub n (4 < = n < = 9)</title><title>Journal of physical chemistry (1952)</title><description>Ionization energies for Ni clusters with four to nine atoms have been calculated and compared to recent experiments. Two different models have been tried, both of them relying on a clear identification of 3d derived and 4s,4p derived orbitals. In the first model, used previously for Cu clusters, all metal atoms are described as effective one-electron systems and a 4s,4p electron is ionized. In the second model, 3d ionization is considered by describing one metal atom at the all-electron level. It is shown that the second model is required to explain the absence of odd--even oscillations in the experimental ionization measurements. It is also argued that the fact that the outermost ionization sometimes occurs from a 3d orbital is not in conflict with a model where the 3d orbitals only make small contributions to the binding of the cluster. 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Two different models have been tried, both of them relying on a clear identification of 3d derived and 4s,4p derived orbitals. In the first model, used previously for Cu clusters, all metal atoms are described as effective one-electron systems and a 4s,4p electron is ionized. In the second model, 3d ionization is considered by describing one metal atom at the all-electron level. It is shown that the second model is required to explain the absence of odd--even oscillations in the experimental ionization measurements. It is also argued that the fact that the outermost ionization sometimes occurs from a 3d orbital is not in conflict with a model where the 3d orbitals only make small contributions to the binding of the cluster. The calculations show, in agreement with experiment, that the Ni sub 6 cluster is the only one of the investigated clusters which has an ionization energy > 6.2 eV and which is thus out of reach for the laser source used in the experiments.</abstract></addata></record> |
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title | Theoretical Ionization Energies and Geometries for Ni sub n (4 < = n < = 9) |
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