The Challenge of the So-Called Electron Configurations of the Transition Metals

Quite different meanings are attached by chemists to the words element, atom, orbital, order of orbitals or configurations. This causes conceptual inconsistencies, in particular with respect to the transition‐metal elements and their atoms or ions. The different meanings will here be distinguished c...

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Veröffentlicht in:Chemistry : a European journal 2006-05, Vol.12 (15), p.4101-4114
Hauptverfasser: Wang, S. G., Qiu, Y. X., Fang, H., Schwarz, W. H. E.
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Qiu, Y. X.
Fang, H.
Schwarz, W. H. E.
description Quite different meanings are attached by chemists to the words element, atom, orbital, order of orbitals or configurations. This causes conceptual inconsistencies, in particular with respect to the transition‐metal elements and their atoms or ions. The different meanings will here be distinguished carefully. They are analyzed on the basis of empirical atomic spectral data and quasi‐relativistic density functional calculations. The latter are quite reliable for different average configuration energies of transition‐metal atoms. The so‐called “configurations of the chemical elements”, traditionally displayed in periodic tables, are the dominant configurations of the lowest spin‐orbit levels of the free atoms. They are chemically rather irrelevant. In many‐electron systems the ns and np AOs are significantly below the more hydrogen‐like nd ones. Even (n+1)s is below nd for all light neutral atoms from C onwards, but only up to the first elements of the respective long rows! The most common orbital order in transition‐metal atoms is 3p ≪ 3d < 4s etc. The chemically relevant configuration in group g is always dg instead of dg−2 s2. Conceptually clear reasoning eliminates apparent textbook inconsistencies between simple quantum‐chemical models and the empirical facts. The empirically and theoretically well‐founded Rydberg (n−δl) rule is to be preferred instead of the historical Madelung (n+l) rule with its large number of exceptions. Chemically bound atoms differ from free atoms significantly: Diffuse Rydberg orbitals, for example, (n+1)s, are perturbed away in compounds. The common order of orbitals in bonded transition metal atoms is np≪nd
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G. ; Qiu, Y. X. ; Fang, H. ; Schwarz, W. H. E.</creator><creatorcontrib>Wang, S. G. ; Qiu, Y. X. ; Fang, H. ; Schwarz, W. H. E.</creatorcontrib><description>Quite different meanings are attached by chemists to the words element, atom, orbital, order of orbitals or configurations. This causes conceptual inconsistencies, in particular with respect to the transition‐metal elements and their atoms or ions. The different meanings will here be distinguished carefully. They are analyzed on the basis of empirical atomic spectral data and quasi‐relativistic density functional calculations. The latter are quite reliable for different average configuration energies of transition‐metal atoms. The so‐called “configurations of the chemical elements”, traditionally displayed in periodic tables, are the dominant configurations of the lowest spin‐orbit levels of the free atoms. They are chemically rather irrelevant. In many‐electron systems the ns and np AOs are significantly below the more hydrogen‐like nd ones. Even (n+1)s is below nd for all light neutral atoms from C onwards, but only up to the first elements of the respective long rows! The most common orbital order in transition‐metal atoms is 3p ≪ 3d &lt; 4s etc. The chemically relevant configuration in group g is always dg instead of dg−2 s2. Conceptually clear reasoning eliminates apparent textbook inconsistencies between simple quantum‐chemical models and the empirical facts. The empirically and theoretically well‐founded Rydberg (n−δl) rule is to be preferred instead of the historical Madelung (n+l) rule with its large number of exceptions. Chemically bound atoms differ from free atoms significantly: Diffuse Rydberg orbitals, for example, (n+1)s, are perturbed away in compounds. The common order of orbitals in bonded transition metal atoms is np≪nd&lt;(n+1)s, because nd collapses below (n+1)s at the beginning of the transition‐metal rows. The n+l rule for the order of orbitals in the periodic table should be replaced by the experimental and theoretical correct Rydberg rule n−δ(l). Density functional theory works unexpectedly well for atomic configuration energies.</description><identifier>ISSN: 0947-6539</identifier><identifier>EISSN: 1521-3765</identifier><identifier>DOI: 10.1002/chem.200500945</identifier><identifier>PMID: 16544343</identifier><language>eng</language><publisher>Weinheim: WILEY-VCH Verlag</publisher><subject>Aufbau principle ; density functional calculations ; electron interaction ; electronic configurations ; orbitals ; transition metal atoms</subject><ispartof>Chemistry : a European journal, 2006-05, Vol.12 (15), p.4101-4114</ispartof><rights>Copyright © 2006 WILEY‐VCH Verlag GmbH &amp; Co. 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X.</creatorcontrib><creatorcontrib>Fang, H.</creatorcontrib><creatorcontrib>Schwarz, W. H. E.</creatorcontrib><title>The Challenge of the So-Called Electron Configurations of the Transition Metals</title><title>Chemistry : a European journal</title><addtitle>Chemistry - A European Journal</addtitle><description>Quite different meanings are attached by chemists to the words element, atom, orbital, order of orbitals or configurations. This causes conceptual inconsistencies, in particular with respect to the transition‐metal elements and their atoms or ions. The different meanings will here be distinguished carefully. They are analyzed on the basis of empirical atomic spectral data and quasi‐relativistic density functional calculations. The latter are quite reliable for different average configuration energies of transition‐metal atoms. The so‐called “configurations of the chemical elements”, traditionally displayed in periodic tables, are the dominant configurations of the lowest spin‐orbit levels of the free atoms. They are chemically rather irrelevant. In many‐electron systems the ns and np AOs are significantly below the more hydrogen‐like nd ones. Even (n+1)s is below nd for all light neutral atoms from C onwards, but only up to the first elements of the respective long rows! The most common orbital order in transition‐metal atoms is 3p ≪ 3d &lt; 4s etc. The chemically relevant configuration in group g is always dg instead of dg−2 s2. Conceptually clear reasoning eliminates apparent textbook inconsistencies between simple quantum‐chemical models and the empirical facts. The empirically and theoretically well‐founded Rydberg (n−δl) rule is to be preferred instead of the historical Madelung (n+l) rule with its large number of exceptions. Chemically bound atoms differ from free atoms significantly: Diffuse Rydberg orbitals, for example, (n+1)s, are perturbed away in compounds. The common order of orbitals in bonded transition metal atoms is np≪nd&lt;(n+1)s, because nd collapses below (n+1)s at the beginning of the transition‐metal rows. The n+l rule for the order of orbitals in the periodic table should be replaced by the experimental and theoretical correct Rydberg rule n−δ(l). 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This causes conceptual inconsistencies, in particular with respect to the transition‐metal elements and their atoms or ions. The different meanings will here be distinguished carefully. They are analyzed on the basis of empirical atomic spectral data and quasi‐relativistic density functional calculations. The latter are quite reliable for different average configuration energies of transition‐metal atoms. The so‐called “configurations of the chemical elements”, traditionally displayed in periodic tables, are the dominant configurations of the lowest spin‐orbit levels of the free atoms. They are chemically rather irrelevant. In many‐electron systems the ns and np AOs are significantly below the more hydrogen‐like nd ones. Even (n+1)s is below nd for all light neutral atoms from C onwards, but only up to the first elements of the respective long rows! 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subjects Aufbau principle
density functional calculations
electron interaction
electronic configurations
orbitals
transition metal atoms
title The Challenge of the So-Called Electron Configurations of the Transition Metals
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