25 research outputs found

    Infrared Spectroscopy of [M(CO<sub>2</sub>)<sub><i>n</i></sub>]<sup>+</sup> (M = Ca, Sr, and Ba; <i>n</i> = 1ā€“4) in the Gas Phase: Solvation-Induced Electron Transfer and Activation of CO<sub>2</sub>

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    Cationic complexes of heavy alkaline earth metal and carbon dioxide [M(CO2)n]+ (M = Ca, Sr, and Ba) are produced by a laser vaporization-supersonic expansion ion source in the gas phase and are studied by infrared photodissociation spectroscopy in conjunction with quantum chemistry calculations. For the n = 1 complexes, the metalā€“ligand binding arises primarily from the electrostatic interaction with the CO2 ligand bound to the metal (+I) center in an end-on Ī·1-O fashion. The more highly coordinated complexes [M(CO2)n]+ with n ā‰„ 2 are characterized to involve a [M2+(CO2ā€“)] core ion with the CO2ā€“ ligand bound to the metal (+II) center in a bidentate Ī·2-O, O manner. The activation of CO2 in forming a bent CO2ā€“ moiety occurs via solvation-induced metal cation-ligand electron transfer reactions. Bonding analyses reveal that the attractive forces between M2+ and CO2ā€“ in the core cation come mainly from electrostatic attraction, but the contribution of covalent orbital interactions should not be underestimated. The atomic orbitals of metal dications that are engaged in the orbital interactions are ns and (n ā€“ 1)d orbitals

    Reactions of Vanadium Dioxide Molecules with Acetylene: Infrared Spectra of VO<sub>2</sub>(Ī·<sup>2</sup>ā€‘C<sub>2</sub>H<sub>2</sub>)<sub><i>x</i></sub> (<i>x</i> = 1, 2) and OV(OH)CCH in Solid Neon

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    Reactions of vanadium dioxide molecules with acetylene have been studied by matrix isolation infrared spectroscopy. Reaction intermediates and products are identified on the basis of isotopic substitutions as well as density functional frequency calculations. Ground state vanadium dioxide molecule reacts with acetylene in forming the side-on-bonded VO<sub>2</sub>(Ī·<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>) and VO<sub>2</sub>(Ī·<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>)<sub>2</sub> complexes spontaneously on annealing in solid neon. The VO<sub>2</sub>(Ī·<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>) complex is characterized to have a <sup>2</sup>B<sub>2</sub> ground state with <i>C</i><sub>2<i>v</i></sub> symmetry, whereas the VO<sub>2</sub>(Ī·<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>)<sub>2</sub> complex has a <sup>2</sup>A ground state with <i>C</i><sub>2</sub> symmetry. The VO<sub>2</sub>(Ī·<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>) and VO<sub>2</sub>(Ī·<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>)<sub>2</sub> complexes are photosensitive. The VO<sub>2</sub>(Ī·<sup>2</sup>-C<sub>2</sub>H<sub>2</sub>) complex rearranges to the OVĀ­(OH)Ā­CCH molecule upon UVā€“vis light excitation

    Infrared Photodissociation Spectroscopy and Density Functional Theory Study of Carbon Suboxide Complexes [M(CO)<sub>4</sub>(C<sub>3</sub>O<sub>2</sub>)]<sup>+</sup> (M = Fe, Co, Ni)

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    Infrared photodissociation spectra are measured for mass-selected cation complexes with a chemical formula [MC<sub>7</sub>O<sub>6</sub>]<sup>+</sup> (M = Fe, Co, Ni) formed via pulsed laser evaporation of metal target in expansions of helium gas seeded by CO. The geometries of the complexes are determined by comparison of the experimental spectra with the simulated spectra from density functional calculations. All of these complexes are identified to have [MĀ­(CO)<sub>4</sub>(C<sub>3</sub>O<sub>2</sub>)]<sup>+</sup> structures involving a carbon suboxide ligand, which binds the metal center in an Ī·<sup>1</sup> fashion. The antisymmetric CO stretching vibration of C<sub>3</sub>O<sub>2</sub> is slightly red-shifted upon coordination. The donorā€“acceptor bonding interactions between C<sub>3</sub>O<sub>2</sub> and the metal centers are analyzed using the EDA-NOCV method. The results show that M ā† C<sub>3</sub>O<sub>2</sub> Ļƒ donation is stronger than the M ā†’ C<sub>3</sub>O<sub>2</sub> Ļ€ back-donation in these cation complexes

    Infrared Spectra and Structures of the Neutral and Charged CrCO<sub>2</sub> and Cr(CO<sub>2</sub>)<sub>2</sub> Isomers in Solid Neon

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    The reactions from codeposition of laser-ablated chromium atoms with carbon dioxide in excess neon are studied by infrared absorption spectroscopy. The species formed are identified by the effects of isotopic substitution on their infrared spectra. Density functional calculations are performed to support the spectral assignments and to interpret the geometric and electronic structures of the experimentally observed species. Besides the previously reported insertion products OCrCO and O<sub>2</sub>CrĀ­(CO)<sub>2</sub>, the one-to-one CrĀ­(CO<sub>2</sub>) complex and the one-to-two CrĀ­(CO<sub>2</sub>)<sub>2</sub> complex as well as the CrOCrCO and OCCrCO<sub>3</sub> complexes are also formed. The CrĀ­(CO<sub>2</sub>) complex is characterized to be side-on Ī·<sup>2</sup>-C,O-coordinated. The CrĀ­(CO<sub>2</sub>)<sub>2</sub> complex is identified to involve a side-on Ī·<sup>2</sup>-C,O-coordinated CO<sub>2</sub> and an end-on Ī·<sup>1</sup>-O-coordinated CO<sub>2</sub>. OCCrCO<sub>3</sub> is a carbonate carbonyl complex predicted to have a planar structure with a Ī·<sup>2</sup>-O,O-coordinated carbonate ligand. The CrOCrCO complex is predicted to be linear with a high-spin ground state. Besides the neutral molecules, charged species are also produced. The CrĀ­(CO<sub>2</sub>)<sup>+</sup> and CrĀ­(CO<sub>2</sub>)<sub>2</sub><sup>+</sup> cation complexes are characterized to have linear end-on Ī·<sup>1</sup>-O-coordinated structures with blue-shifted antisymmetric CO<sub>2</sub> stretching vibrational frequencies. The OCrCO<sup>ā€“</sup> anion is bent with the Crā€“O and CO stretching frequencies red-shifted from those of OCrCO neutral molecule

    Infrared Photodissociation Spectroscopic and Theoretical Study of Heteronuclear Transition Metal Carbonyl Cluster Cations in the Gas Phase

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    Heteronuclear transition metal carbonyl cluster cations FeMĀ­(CO)<sub>8</sub><sup>+</sup> (M = Co, Ni and Cu) and MCuĀ­(CO)<sub>7</sub><sup>+</sup> (M = Co and Ni) are produced via a laser vaporization supersonic cluster ion source in the gas phase, which are each mass-selected and studied by infrared photodissociation spectroscopy in the carbonyl stretching frequency region. Their geometric and electronic structures are established by comparison of the experimental spectra with those derived from density functional theoretical calculations. The FeMĀ­(CO)<sub>8</sub><sup>+</sup> (M = Co, Ni, Cu) complexes are determined to have eclipsed (CO)<sub>5</sub>Feā€“MĀ­(CO)<sub>3</sub><sup>+</sup> structures, and the MCuĀ­(CO)<sub>7</sub><sup>+</sup> (M = Co, Ni) ions are characterized to have staggered (CO)<sub>4</sub>Mā€“CuĀ­(CO)<sub>3</sub><sup>+</sup> structures. Natural bonding orbital analysis indicates that the positive charge is mainly distributed on the MĀ­(CO)<sub>3</sub> fragment. The metalā€“metal interaction involves an Ļƒ-type (OC)<sub>4,5</sub>Mā†’MĀ­(CO)<sub>3</sub><sup>+</sup> dative bonding

    Isocyanate Formation from Reactions of Early Lanthanide Metal Atoms with NO and CO in Solid Argon

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    The reactions of early lanthanide metal atoms (Ce, Pr, and Nd) with carbon monoxide and nitric oxide mixtures are studied by infrared absorption spectroscopy in solid argon. The reaction intermediates and products are identified via isotopic substitution as well as theoretical frequency calculations. The results show that the reactions proceed with the initial formation of inserted NLnO molecules, which subsequently react with CO to form the NLnOĀ­(CO) complexes on annealing. The NLnOĀ­(CO) complexes further isomerize to the more stable isocyanate OLnNCO species under UV light excitation

    Coordination and Solvation of the Au<sup>+</sup> Cation: Infrared Photodissociation Spectroscopy of Mass-Selected Au(H<sub>2</sub>O)<sub><i>n</i></sub><sup>+</sup> (<i>n</i> = 1ā€“8) Complexes

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    Gold cationā€“water complexes with attached argon atoms are produced via a laser vaporization supersonic cluster source. The [AuĀ­(H<sub>2</sub>O)<sub><i>n</i></sub>Ar<sub><i>x</i></sub>]<sup>+</sup> (<i>n</i> = 1ā€“8; <i>x</i> = 1 or 2) complexes are each mass selected and studied by infrared photodissociation spectroscopy in the OH stretching frequency region to explore the coordination and solvation structures of the Au<sup>+</sup> cation. Density functional calculations have been performed, and the calculated vibrational spectra are compared to the experimental spectra to identify the gas-phase structures of the AuĀ­(H<sub>2</sub>O)<sub><i>n</i></sub><sup>+</sup> complexes. Confirming previous theoretical predications, the first coordination shell of the Au<sup>+</sup> cation contains two water molecules forming a linear Oā€“Au<sup>+</sup>ā€“O arrangement; subsequent water molecules bind to the two H<sub>2</sub>O ligands of the AuĀ­(H<sub>2</sub>O)<sub>2</sub><sup>+</sup> core ion via hydrogen bond forming of the second hydration shell, which is complete at <i>n</i> = 6. For the complexes with <i>n</i> ā‰¤ 7, the experimental spectrum can in general be assigned to the predicted global minimum structure. However, the spectrum suggests that two or more conformers coexist for the <i>n</i> = 8 complex, indicating that the identification of a single global minimum becomes less important upon increasing the number of solvating water molecules

    Infrared Photodissociation Spectroscopy of Heterodinuclear Ironā€“Zinc and Cobaltā€“Zinc Carbonyl Cation Complexes

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    Feā€“Zn and Coā€“Zn heteronuclear carbonyl cation complexes are produced via a laser vaporization supersonic cluster source in the gas phase. The dinuclear FeZnĀ­(CO)<sub>5</sub><sup>+</sup> and CoZnĀ­(CO)<sub>7</sub><sup>+</sup> cation complexes are observed to be the most intense heterodinuclear carbonyl cation species in the mass spectra. The infrared spectra are obtained via mass selection and infrared photodissociation spectroscopy in the carbonyl stretching frequency region. Their geometric and electronic structures are assigned with the support of density functional calculations. The FeZnĀ­(CO)<sub>5</sub><sup>+</sup> complex is determined to have a (OC)<sub>5</sub>Feā€“Zn structure with a Feā€“Zn half bond. The CoZnĀ­(CO)<sub>7</sub><sup>+</sup> ion is established to have a staggered (OC)<sub>4</sub>Coā€“ZnĀ­(CO)<sub>3</sub> structure involving a Coā€“Zn Ļƒ single bond

    Carbon Dioxide Activation by Scandium Atoms and Scandium Monoxide Molecules: Formation and Spectroscopic Characterization of ScCO<sub>3</sub> and OCScCO<sub>3</sub> in Solid Neon

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    The reactions of carbon dioxide with scandium monoxide molecules and scandium atoms are investigated using matrix isolation infrared spectroscopy in solid neon. The species formed are identified by the effects of isotopic substitution on their infrared spectra as well as density functional calculations. The results show that the ground state ScO molecule reacts with carbon dioxide to form the carbonate complex ScCO<sub>3</sub> spontaneously on annealing. The ground state Sc atom reacts with two carbon dioxide molecules to give the carbonate carbonyl complex OCScCO<sub>3</sub> via the previously reported OScCO insertion intermediate on annealing. The observation of these spontaneous reactions is consistent with theoretical predictions that both the Sc + 2CO<sub>2</sub> ā†’ OCScCO<sub>3</sub> and ScO + CO<sub>2</sub> ā†’ ScCO<sub>3</sub> reactions are thermodynamically exothermic and are kinetically facile, requiring little or no activation energy
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