10 research outputs found

    A Twelve-Coordinated Iodide in a Cuboctahedral Silver(I) Skeleton

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    Three new halide-centered octanuclear silver­(I) complexes, [Ag<sub>8</sub>(X)­{S<sub>2</sub>P­(CH<sub>2</sub>CH<sub>2</sub>Ph)<sub>2</sub>}<sub>6</sub>]­(PF<sub>6</sub>), X = F<sup>–</sup>, <b>1</b>; Cl<sup>–</sup>, <b>2</b>; Br<sup>–</sup>, <b>3</b>; were prepared in the presence of the corresponding halide anions with silver­(I) salts and dithiophosphinate ligands. Structure analyses displayed that a Ag<sub>8</sub> cubic core can be modulated by the size effect of the central halide; however, an iodide-centered Ag<sub>8</sub> cluster was not found under similar reaction conditions. Interestingly, a luminescent dodecanuclear silver­(I) cluster, [Ag<sub>12</sub>(μ<sub>12</sub>-I)­(μ<sub>3</sub>-I)<sub>4</sub>{S<sub>2</sub>P­(CH<sub>2</sub>CH<sub>2</sub>Ph)<sub>2</sub>}<sub>6</sub>]­(I), <b>4</b>; was then synthesized. The structure of <b>4</b> contains a novel μ<sub>12</sub>-I at the center of a cuboctahedral silver­(I) atom cage, which is further stabilized by four additional μ<sub>3</sub>-I and six dithiophosphinate ligands. To the best of our knowledge, the μ<sub>12</sub>-I revealed in <b>4</b> is the highest coordination number for a halide ion authenticated by both experimental and computational studies. Previously, the μ<sub>12</sub>-I was only observed in [PyH]­[{TpMo­(μ<sub>3</sub>-S)<sub>4</sub>Cu<sub>3</sub>}<sub>4</sub>(μ<sub>12</sub>-I)]. The synthetic details, spectroscopic studies including multinuclear NMR and ESI-MS, structure elucidations by single crystal X-ray diffraction, and photoluminescence of <b>4</b> are reported herein

    Neutron Diffraction Studies of a Four-Coordinated Hydride in Near Square-Planar Geometry

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    The structure of a nanospheric polyhydrido copper cluster, [Cu<sub>20</sub>(H)<sub>11</sub>{S<sub>2</sub>P­(O<sup><i>i</i></sup>Pr)<sub>2</sub>}<sub>9</sub>], was determined by single-crystal neutron diffraction. The Cu<sub>20</sub> cluster consists of an elongated triangular orthobicupola constructed from 18 Cu atoms that encapsulate a [Cu<sub>2</sub>H<sub>5</sub>]<sup>3–</sup> ion with an exceptionally short Cu–Cu distance. The 11 hydrides in the cluster display three different coordination modes to the Cu atoms: six μ<sub>3</sub>-hydrides in a pyramidal geometry, two μ<sub>4</sub>-hydrides in a tetrahedral cavity, and three μ<sub>4</sub>-hydrides in an unprecedented near square-planar geometry. The neutron data set was collected for 7 days on a small crystal with dimensions of 0.20 mm × 0.50 mm × 0.65 mm using the Spallation Neutron Source TOPAZ single-crystal time-of-flight Laue diffractometer at Oak Ridge National Laboratory. The final <i>R</i>-factor was 8.63% for 16,014 reflections

    Neutron Diffraction Studies of a Four-Coordinated Hydride in Near Square-Planar Geometry

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    The structure of a nanospheric polyhydrido copper cluster, [Cu<sub>20</sub>(H)<sub>11</sub>{S<sub>2</sub>P­(O<sup><i>i</i></sup>Pr)<sub>2</sub>}<sub>9</sub>], was determined by single-crystal neutron diffraction. The Cu<sub>20</sub> cluster consists of an elongated triangular orthobicupola constructed from 18 Cu atoms that encapsulate a [Cu<sub>2</sub>H<sub>5</sub>]<sup>3–</sup> ion with an exceptionally short Cu–Cu distance. The 11 hydrides in the cluster display three different coordination modes to the Cu atoms: six μ<sub>3</sub>-hydrides in a pyramidal geometry, two μ<sub>4</sub>-hydrides in a tetrahedral cavity, and three μ<sub>4</sub>-hydrides in an unprecedented near square-planar geometry. The neutron data set was collected for 7 days on a small crystal with dimensions of 0.20 mm × 0.50 mm × 0.65 mm using the Spallation Neutron Source TOPAZ single-crystal time-of-flight Laue diffractometer at Oak Ridge National Laboratory. The final <i>R</i>-factor was 8.63% for 16,014 reflections

    Ferrocene-Functionalized Cu(I)/Ag(I) Dithiocarbamate Clusters

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    A series of compounds, namely, [Cu<sub>8</sub>(μ<sub>4</sub>-H)­{S<sub>2</sub>CN­MeCH<sub>2</sub>Fc}<sub>6</sub>]­(PF<sub>6</sub>) (<b>1</b>), [Cu<sub>7</sub>(μ<sub>4</sub>-H) {S<sub>2</sub>CN<sup><i>i</i></sup>PrCH<sub>2</sub>Fc}<sub>6</sub>] (<b>2</b>), [Cu<sub>3</sub>{S<sub>2</sub>CN­(Bz) (CH<sub>2</sub>Fc)}<sub>2</sub>(dppf)<sub>2</sub>]­(PF<sub>6</sub>) (<b>3</b>), and [Ag<sub>2</sub>{S<sub>2</sub>CNMe­(CH<sub>2</sub>Fc)}<sub>2</sub>(PPh<sub>3</sub>)<sub>2</sub>] (<b>4</b>) (dppf = 1,1′-bis­(diphenylphosphino)­ferrocene), supported by multiferrocene assemblies, were synthesized. All the compounds were characterized by <sup>1</sup>H NMR, Fourier transform infrared, elemental analysis, and electrospray ionization mass spectrometry techniques. Single-crystal X-ray structural analysis revealed that <b>1</b> is a monocationic octanuclear Cu<sup>I</sup> cluster and that <b>2</b> is a neutral heptanuclear Cu<sup>I</sup> cluster with tetracapped tetrahedral (<b>1</b>) and tricapped tetrahedral (<b>2</b>) geometries entrapped with an interstitial hydride, anchored by six ferrocene units at the periphery of the core. Compounds <b>3</b> and <b>4</b> comprise trimetallic Cu<sup>I</sup> and dimetallic Ag<sup>I</sup> cores enfolded by four and two ferrocene moieties. Interestingly both chelating and bridging modes of binding are observed for dppf ligand in <b>3</b>. Further the formation and isolation of polyhydrido copper clusters [Cu<sub>28</sub>H<sub>15</sub>{S<sub>2</sub>CN<sup><i>i</i></sup>PrCH<sub>2</sub>Fc}<sub>12</sub>]­(PF<sub>6</sub>) (<b>5</b>) and [Cu<sub>28</sub>H<sub>15</sub>{S<sub>2</sub>CN<sup><i>n</i></sup>Bu<sub>2</sub>}<sub>12</sub>]­(PF<sub>6</sub>) (<b>7</b>), stabilized by bulky ferrocenyl and <i>n</i>-butyl dithiocarbamate ligands, was demonstrated. They are readily identified by <sup>2</sup>H NMR studies on their deuterium analogues, [Cu<sub>28</sub>D<sub>15</sub>{S<sub>2</sub>CN<sup><i>i</i></sup>PrCH<sub>2</sub>Fc}<sub>12</sub>]­(PF<sub>6</sub>) (<b>6</b>) and [Cu<sub>28</sub>D<sub>15</sub>{S<sub>2</sub>CN<sup><i>n</i></sup>Bu<sub>2</sub>}<sub>12</sub>]­(PF<sub>6</sub>) (<b>8</b>). Though the structure details as well as spectroscopic characterizations of <b>5</b> are yet to be investigated, the compound <b>7</b> is fully characterized by variety of spectroscopy including single-crystal X-ray diffraction. The cyclic voltammetry studies for compounds <b>1</b>, <b>2</b>, and <b>4</b> display irreversible redox peaks for Fe<sup>2+</sup>/Fe<sup>3+</sup> couple wherein the reduction peaks are not well-resolved due to some adsorption of the complex onto the electrode surface

    A Nanospheric Polyhydrido Copper Cluster of Elongated Triangular Orthobicupola Array: Liberation of H<sub>2</sub> from Solar Energy

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    An unprecedented air-stable, nanospheric polyhydrido copper cluster, [Cu<sub>20</sub>H<sub>11</sub>(S<sub>2</sub>P­(O<sup>i</sup>Pr)<sub>2</sub>)<sub>9</sub>] (<b>1</b><sub><b>H</b></sub>), which is the first example of an elongated triangular orthobicupola array of Cu atoms having <i>C</i><sub>3<i>h</i></sub> symmetry, was synthesized and characterized. Its composition was primarily determined by electrospray ionization mass spectrometry, and it was fully characterized by <sup>1</sup>H, <sup>2</sup>H, and <sup>31</sup>P NMR spectroscopy and single-crystal X-ray diffraction (XRD). The structure of complex <b>1</b><sub><b>H</b></sub> can be expressed in terms of a trigonal-bipyramidal [Cu<sub>2</sub>H<sub>5</sub>]<sup>3–</sup> unit anchored within an elongated triangular orthobicupola containing 18 Cu atoms, which is further stabilized by 18 S atoms from nine dithiophosphate ligands and six capping hydrides. The positions of the 11 hydrides revealed by low temperature XRD were supported by a density functional theory investigation on the simplified model [Cu<sub>20</sub>H<sub>11</sub>(S<sub>2</sub>PH<sub>2</sub>)<sub>9</sub>] with <i>C</i><sub>3<i>h</i></sub> symmetry. <b>1</b><sub><b>H</b></sub> is capable of releasing H<sub>2</sub> gas upon irradiation with sunlight, under mild thermal conditions (65 °C), or in the presence of acids at room temperature

    A Nanospheric Polyhydrido Copper Cluster of Elongated Triangular Orthobicupola Array: Liberation of H<sub>2</sub> from Solar Energy

    No full text
    An unprecedented air-stable, nanospheric polyhydrido copper cluster, [Cu<sub>20</sub>H<sub>11</sub>(S<sub>2</sub>P­(O<sup>i</sup>Pr)<sub>2</sub>)<sub>9</sub>] (<b>1</b><sub><b>H</b></sub>), which is the first example of an elongated triangular orthobicupola array of Cu atoms having <i>C</i><sub>3<i>h</i></sub> symmetry, was synthesized and characterized. Its composition was primarily determined by electrospray ionization mass spectrometry, and it was fully characterized by <sup>1</sup>H, <sup>2</sup>H, and <sup>31</sup>P NMR spectroscopy and single-crystal X-ray diffraction (XRD). The structure of complex <b>1</b><sub><b>H</b></sub> can be expressed in terms of a trigonal-bipyramidal [Cu<sub>2</sub>H<sub>5</sub>]<sup>3–</sup> unit anchored within an elongated triangular orthobicupola containing 18 Cu atoms, which is further stabilized by 18 S atoms from nine dithiophosphate ligands and six capping hydrides. The positions of the 11 hydrides revealed by low temperature XRD were supported by a density functional theory investigation on the simplified model [Cu<sub>20</sub>H<sub>11</sub>(S<sub>2</sub>PH<sub>2</sub>)<sub>9</sub>] with <i>C</i><sub>3<i>h</i></sub> symmetry. <b>1</b><sub><b>H</b></sub> is capable of releasing H<sub>2</sub> gas upon irradiation with sunlight, under mild thermal conditions (65 °C), or in the presence of acids at room temperature

    Anion Encapsulation and Geometric Changes in Hepta- and Hexanuclear Copper(I) Dichalcogeno Clusters: A Theoretical and Experimental Investigation

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    Whereas stable octanuclear clusters of the type M<sup>I</sup><sub>8</sub>(E<sup>∩</sup>E)<sub>6</sub> (M = Cu, Ag; E<sup>∩</sup>E = dithio or diseleno ligand) are known for being able to encapsulate a hydride or main-group anion under some circumstances, only the related hydride-containing heptanuclear [M<sup>I</sup>]<sub>7</sub>(H)­(E<sup>∩</sup>E)<sub>6</sub> and empty hexanuclear [M<sup>I</sup>]<sub>6</sub>(E<sup>∩</sup>E)<sub>6</sub> species have been characterized so far. In this paper we investigate by the means of theoretical calculations and experiments the viability of empty and anion-centered clusters of the type [Cu<sup>I</sup>]<sub>7</sub>(X)­(E<sup>∩</sup>E)<sub>6</sub> and [Cu<sup>I</sup>]<sub>6</sub>(X)­(E<sup>∩</sup>E)<sub>6</sub> (X = vacancy, H or a main-group atom). The theoretical prediction for the existence of anion-containing heptanuclear species, the shape of which is modulated by the anion nature and size, have been fully confirmed by the synthesis and characterization of [Cu<sub>7</sub>(X)­{S<sub>2</sub>P­(O<sup>i</sup>Pr)<sub>2</sub>}<sub>6</sub>] (X = H, Br). This consistency between experiment and theory allows us to predict the stability and shape-modulated structure of a whole series of [Cu<sup>I</sup>]<sub>7</sub>(X)­(E<sup>∩</sup>E)<sub>6</sub> (X = vacancy, H, O, S, halogen) and [Cu<sup>I</sup>]<sub>6</sub>(X)­(E<sup>∩</sup>E)<sub>6</sub> (X = H, halogen) clusters

    Structure and Spectroscopic Properties of Gold(I) Diselenophosph(in)ate Complexes: A Joint Experimental and Theoretical Study

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    The structure and optical properties of several polynuclear gold­(I) species, namely, diselenophosphate [Au­{μ-Se<sub>2</sub>P­(OR)<sub>2</sub>}]<sub>2</sub> complexes (R = <sup><i>i</i></sup>Pr, Et, <sup><i>n</i></sup>Pr) respectively numbered <b>1</b>, <b>2</b>, and <b>3</b> and number <b>4</b> [Au­{μ-Se<sub>2</sub>P­(CH<sub>2</sub>)<sub>2</sub>Ph)<sub>2</sub>}]<sub>2</sub>, exhibiting interesting structural, absorption, and emission properties have been studied. The synthesis, full characterization, and experimental spectroscopic study of <b>3</b> and <b>4</b> have first been carried out, <b>1</b> and <b>2</b> being previously studied. In the solid state, <b>3</b> gives polymers, like <b>1</b> and <b>2</b>, whereas <b>4</b> exists under a dinuclear monomeric form. The absorption and phosphorescence properties of <b>4</b> have been rationalized using DFT and TDDFT computations. In particular, Au–Au bonding seems to appear in its first singlet and triplet states, whereas such a bond does not exist in the ground state. Then, the influence of polymerization through aurophilic bonding on the optical properties of <b>2</b> is investigated (<b>1</b> and <b>3</b> behave as <b>2</b>). It is shown using TDDFT computations that its observed UV–visible excitation spectrum in solution is due to high oligomers and not to monomers or low size oligomers. ESI-MS molecular weight measurements confirm the occurrence of such oligomers of <b>2</b> in solution. An assignment of the observed bands of <b>2</b> is proposed. The transition corresponding to the first excitation band, which is mainly a HOMO to LUMO one, exhibits metal-centered character, i.e., a gold 5d to 6p orbital transition, but concomitantly transfers significant electron density from gold to phosphorus atoms so that it is also a MLCT one

    Anion Encapsulation and Geometric Changes in Hepta- and Hexanuclear Copper(I) Dichalcogeno Clusters: A Theoretical and Experimental Investigation

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    Whereas stable octanuclear clusters of the type M<sup>I</sup><sub>8</sub>(E<sup>∩</sup>E)<sub>6</sub> (M = Cu, Ag; E<sup>∩</sup>E = dithio or diseleno ligand) are known for being able to encapsulate a hydride or main-group anion under some circumstances, only the related hydride-containing heptanuclear [M<sup>I</sup>]<sub>7</sub>(H)­(E<sup>∩</sup>E)<sub>6</sub> and empty hexanuclear [M<sup>I</sup>]<sub>6</sub>(E<sup>∩</sup>E)<sub>6</sub> species have been characterized so far. In this paper we investigate by the means of theoretical calculations and experiments the viability of empty and anion-centered clusters of the type [Cu<sup>I</sup>]<sub>7</sub>(X)­(E<sup>∩</sup>E)<sub>6</sub> and [Cu<sup>I</sup>]<sub>6</sub>(X)­(E<sup>∩</sup>E)<sub>6</sub> (X = vacancy, H or a main-group atom). The theoretical prediction for the existence of anion-containing heptanuclear species, the shape of which is modulated by the anion nature and size, have been fully confirmed by the synthesis and characterization of [Cu<sub>7</sub>(X)­{S<sub>2</sub>P­(O<sup>i</sup>Pr)<sub>2</sub>}<sub>6</sub>] (X = H, Br). This consistency between experiment and theory allows us to predict the stability and shape-modulated structure of a whole series of [Cu<sup>I</sup>]<sub>7</sub>(X)­(E<sup>∩</sup>E)<sub>6</sub> (X = vacancy, H, O, S, halogen) and [Cu<sup>I</sup>]<sub>6</sub>(X)­(E<sup>∩</sup>E)<sub>6</sub> (X = H, halogen) clusters

    A μ<sub>9</sub>-Iodide in a Tricapped Trigonal-Prismatic Geometry

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    Two luminescent, undecanuclear silver complexes [Ag<sub>11</sub>(μ<sub>9</sub>-I)­(μ<sub>3</sub>-I)<sub>3</sub>{E<sub>2</sub>P­(O<sup>i</sup>Pr)<sub>2</sub>}<sub>6</sub>]­(PF<sub>6</sub>) [E = S (yellow), <b>1</b>; Se (orange), <b>2</b>], containing the first μ<sub>9</sub>-iodine inscribed at the center of a pentacapped trigonal-prismatic silver skeleton, were reported
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