Abstract:The structure of iron pentacarbonyl, Fe(CO)(5), was reinvestigated by gas-phase electron diffraction using an experimental rotational constant available from the literature as a constraint on the structural parameters. The study utilized a B3LYP/6-311+G(d) ab initio quadratic force field, scaled to fit observed infrared wavenumbers, from which were calculated corrections for the effects of vibrational averaging on distances and certain other quantities useful for the structural analysis. The results confirm th… Show more
“…Isolated M(CO) 5 compounds have 18 normal vibrational modes, but only the m 10 and m 6 carbonyl stretching modes, which represent the asymmetric in-plane equatorial carbonyl stretch and asymmetric axial carbonyl stretch, respectively, are IR active in the region near 2000 cm À1 [32][33][34][35][36][37][38][39][40]. However, when IPC forms a complex with a single solvent molecule, the totally symmetric m 1 vibrational mode becomes IR active due to the induced break in D 3h symmetry.…”
“…Isolated M(CO) 5 compounds have 18 normal vibrational modes, but only the m 10 and m 6 carbonyl stretching modes, which represent the asymmetric in-plane equatorial carbonyl stretch and asymmetric axial carbonyl stretch, respectively, are IR active in the region near 2000 cm À1 [32][33][34][35][36][37][38][39][40]. However, when IPC forms a complex with a single solvent molecule, the totally symmetric m 1 vibrational mode becomes IR active due to the induced break in D 3h symmetry.…”
“…51 More recently, in vaporphase, Fe͑CO͒ 5 has seen use as an ingredient in the production of carbon nanotubes. 52 Consequently, the structure of this molecule has been examined both theoretically 33,35,53 and experimentally, 54 and results are compared with findings from this study in Table V. From these studies, a minor discrepancy 53 occurs between experiment and theory over the relative sizes of the planar and axial Fe-C distances.…”
Describing materials properties and behavior over increasing scales of dimension and complexity requires an optimal balance of completeness and accuracy in solving the local density equations. In this study, the convergence properties of a set of schemes that aim to achieve increasing accuracy are systematically examined according to the hierarchical approximations upon which they are based. Specifically, the Harris density functional ͑HDF͒ and related schemes that express the total energy in terms of atomic densities and limited self-consistency are compared within a single consistent framework. Convergence of the HDF energy relative to input density is first tested by carrying out calculations within the non-self-consistent atom fragment and self-consistent atom fragment ͑SCAF͒ approximations and then by supplementing the SCAF density by increasing numbers of partial waves about each atomic site using the self-consistent partial wave ͑SCPW͒ method. The construct of the SCPW method, that solves the local density equations with controlled precision according to the number of partial waves in the site density expansions, enables this study. The rapid convergence of structural properties with an increasing number of partial waves on each site, sometimes even with only L = 0 partial waves, provides additional justification for HDF-based tight-binding and molecular dynamics methods where the interatomic potentials are obtained from the superposition of atomiclike densities. The convergence of ground state structural properties is demonstrated by application to the set of molecules: carbon monoxide, water, orthosilicic acid ͑H 4 SiO 4 ͒, formamide ͑HCONH 2 ͒, iron pentacarbonyl ͓Fe͑CO͒ 5 ͔, and dimanganese decacarbonyl ͓Mn 2 ͑CO͒ 10 ͔.
“…Experimental FeACO bond lengths are rather well reproduced by the CCSD calculation ( Table 1). [46] In the solid state, however, axial and equatorial FeACO bond lengths were found to be 1.811(2) Å and 1.803(2) Å , respectively. This conclusion, however, is at variance with the gas phase electron diffraction study performed by Hedberg and coworkers.…”
Section: Main Features Of the Computational Scheme For Obtaining The mentioning
confidence: 92%
“…[40][41][42][43] Computed and experimental FeACO bond distances [44] are recorded in Table 1. [46] The authors determined bond lengths of 1.810 Å and 1.842 Å for the axial and equatorial FeACO bonds, respectively. The axial FeACO bonds in Fe(CO) 5 should be slightly longer than the equatorial FeACO bonds.…”
Section: Main Features Of the Computational Scheme For Obtaining The mentioning
A nonstandard computational scheme has been applied to calculate Fe(CO)(5) with the aim to illustrate the operation of the Dewar-Chatt-Duncanson model by computation. A full configuration interaction (CI) calculation in an active space has been performed. The active space is built from naturally localized molecular orbitals (NLMOs) localized in bond regions or forming lone pairs. For selecting this active space, Weinhold's perturbation theory formulated in the natural bond orbital (NBO) space has been applied. Bonding, lone pair, and antibond NBOs exhibiting large interaction energies serve to define the active space. The actually applied active space, however, comprises NLMOs that are close in shape to the NBOs indicated by perturbation theory. Thus, a CI calculation with localized orbitals has been performed meeting the classical reasoning of chemists that is often based on local bonding concepts. The computational scheme yields the Lewis structure for Fe(CO)(5) whose energy is identical to the Hartree-Fock energy. The Lewis energy comprises CO → Fe σ-electron transfer (ET) and CO ← Fe electron back donation (BD). This Lewis energy gets lowered by localized correlation energy contributions caused by ET processes where electrons are back donated from the Fe d-lone pairs into the CO ligands. Thus, electron correlation within the selected active space is dominated by electron BD. Energies and electron populations of the NBOs support the notion that electrons are preferentially back donated into the equatorial CO ligands. Weights of local Slater determinants, determining the correlation energy, also point to a predominant BD into the equatorial CO ligands. Correlation energy increments resulting from electron BD into single antibond orbitals of the CO ligands have been calculated. These energy quantities also demonstrate that BD into the equatorial CO ligands is more energy lowering than BD into the axial CO ligands.
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