2013
DOI: 10.1002/qua.24399
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Unpaired electrons at the second‐order reduced density matrix level: Covalent bonding, and coulomb and fermi correlations in closed shell systems

Abstract: The usual one‐electron populations in atomic orbitals of closed shell systems are split into unpaired and paired at the (spin‐dependent) second‐order reduced density matrix level. The unpaired electron in an orbital is defined as the “simultaneous occurrence of an electron and an electron hole of opposite spins in the same spatial orbital,” which for simplicity is called “electropon.” The electropon population in a given orbital reveals whether and to what degree the Coulomb correlations, and hence, the chemic… Show more

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Cited by 10 publications
(35 citation statements)
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“…As a result, 2nd‐quantized expressions (22) and (23) allow an important generalization of conventional ( Γ (1) ‐based) NPA to the analogous Natural Poly‐Electron Population Analysis (NPEPA) . The latter builds on Moffitt's theorem and allows the probabilities of more complex ne/nh excitation patterns to be evaluated for wave functions of uncorrelated or correlated form, as described in the following sections.…”
Section: Nbo Picture Of Single‐electron Excitations In 2nd‐quantizationmentioning
confidence: 99%
“…As a result, 2nd‐quantized expressions (22) and (23) allow an important generalization of conventional ( Γ (1) ‐based) NPA to the analogous Natural Poly‐Electron Population Analysis (NPEPA) . The latter builds on Moffitt's theorem and allows the probabilities of more complex ne/nh excitation patterns to be evaluated for wave functions of uncorrelated or correlated form, as described in the following sections.…”
Section: Nbo Picture Of Single‐electron Excitations In 2nd‐quantizationmentioning
confidence: 99%
“…The main scope of the investigation of unpaired electron distribution is to describe the occupancy of local regions of space of a molecular system by single (α‐ or β‐spin) electrons. This quantity is of broad interest, concerning reaction mechanisms, the design of materials having magnetic properties, and some biochemical topics.…”
Section: Introductionmentioning
confidence: 99%
“…It is possible to overcome these difficulties by introducing an analogous quantity directly from the 2‐RDM (instead of the product of two 1‐RDMs). In this framework, in a recent work, the conventional one‐electron population, normalnλα, in an atomic orbital (AO) φλ is split into two component parts: nλα =normalP1:1(λ;λ¯)+normalP2;0(λλ¯;0) where P 2;0 ( λ λtrue¯;0) is a two‐electron (and zero‐hole) quantity, representing the number of electron pairs belonging to φλ, and P 1;1 ( λ; λtrue¯) is an one‐electron‐one‐hole quantity (α‐spin electron in spin‐orbital λ, and β‐spin hole in λtrue¯). This splitting is shown schematically in Figure for the case of a radical.…”
Section: Introductionmentioning
confidence: 99%
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