7 research outputs found

    Infrared Photodissociation Spectroscopy of Mass-Selected Heteronuclear Iron–Copper Carbonyl Cluster Anions in the Gas Phase

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    Mass-selected heteronuclear iron–copper carbonyl cluster anions CuFe­(CO)<sub><i>n</i></sub><sup>–</sup> (<i>n</i> = 4–7) are studied by infrared photodissociation spectroscopy in the carbonyl stretching frequency region in the gas phase. The cluster anions are produced via a laser vaporization supersonic cluster ion source. Their geometric structures are determined by comparison of the experimental spectra with those calculated by density functional theory. The experimentally observed CuFe­(CO)<sub><i>n</i></sub><sup>–</sup> (<i>n</i> = 4–7) cluster anions are characterized to have (OC)<sub>4</sub>Fe–Cu­(CO)<sub><i>n</i>−4</sub> structures, each involving a <i>C</i><sub>3<i>v</i></sub> symmetry Fe­(CO)<sub>4</sub><sup>–</sup> building block. Bonding analysis indicates that the Fe–Cu bond in the CuFe­(CO)<sub><i>n</i></sub><sup>–</sup> (<i>n</i> = 4–7) cluster anions is a σ type single bond with the iron center possessing the most favored 18-electron configuration. The results provide important new insight into the structure and bonding of hetronuclear transition metal carbonyl cluster anions

    Infrared Photodissociation Spectroscopy of Mass Selected Homoleptic Copper Carbonyl Cluster Cations in the Gas Phase

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    Infrared spectra of mass-selected homoleptic copper carbonyl cluster cations including dinuclear Cu<sub>2</sub>(CO)<sub>6</sub><sup>+</sup> and Cu<sub>2</sub>(CO)<sub>7</sub><sup>+</sup>, trinuclear Cu<sub>3</sub>(CO)<sub>7</sub><sup>+</sup>, Cu<sub>3</sub>(CO)<sub>8</sub><sup>+</sup>, and Cu<sub>3</sub>(CO)<sub>9</sub><sup>+</sup>, and tetranuclear Cu<sub>4</sub>(CO)<sub>8</sub><sup>+</sup> are measured via infrared photodissociation spectroscopy in the carbonyl stretching frequency region. The structures are established by comparison of the experimental spectra with simulated spectra derived from density functional calculations. The Cu<sub>2</sub>(CO)<sub>6</sub><sup>+</sup> cation is characterized to have an unbridged <i>D</i><sub>3<i>d</i></sub> structure with a Cu–Cu half bond. The Cu<sub>2</sub>(CO)<sub>7</sub><sup>+</sup> cation is determined to be a weakly bound complex involving a Cu<sub>2</sub>(CO)<sub>6</sub><sup>+</sup> core ion. The trinuclear Cu<sub>3</sub>(CO)<sub>7</sub><sup>+</sup> and Cu<sub>3</sub>(CO)<sub>8</sub><sup>+</sup> cluster cations are determined to have triangle Cu<sub>3</sub> core structures with <i>C</i><sub>2</sub> symmetry involving two Cu­(CO)<sub>3</sub> groups and one Cu­(CO)<sub><i>x</i></sub> group (<i>x</i> = 1 or 2). In contrast, the trinuclear Cu<sub>3</sub>(CO)<sub>9</sub><sup>+</sup> cluster cation is determined to have an open chain-like (OC)<sub>3</sub>Cu–Cu­(CO)<sub>3</sub>–Cu­(CO)<sub>3</sub> structure. The tetranuclear Cu<sub>4</sub>(CO)<sub>8</sub><sup>+</sup> cluster cation is characterized to have a tetrahedral Cu<sub>4</sub><sup>+</sup> core structure with all carbonyl groups terminally bonded
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