10 research outputs found
A Twelve-Coordinated Iodide in a Cuboctahedral Silver(I) Skeleton
Three new halide-centered
octanuclear silverÂ(I) complexes, [Ag<sub>8</sub>(X)Â{S<sub>2</sub>PÂ(CH<sub>2</sub>CH<sub>2</sub>Ph)<sub>2</sub>}<sub>6</sub>]Â(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 silverÂ(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 silverÂ(I) cluster, [Ag<sub>12</sub>(μ<sub>12</sub>-I)Â(μ<sub>3</sub>-I)<sub>4</sub>{S<sub>2</sub>PÂ(CH<sub>2</sub>CH<sub>2</sub>Ph)<sub>2</sub>}<sub>6</sub>]Â(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 silverÂ(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]Â[{TpMoÂ(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
The
structure of a nanospheric polyhydrido copper cluster, [Cu<sub>20</sub>(H)<sub>11</sub>{S<sub>2</sub>PÂ(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
The
structure of a nanospheric polyhydrido copper cluster, [Cu<sub>20</sub>(H)<sub>11</sub>{S<sub>2</sub>PÂ(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
A series
of compounds, namely, [Cu<sub>8</sub>(μ<sub>4</sub>-H)Â{S<sub>2</sub>CNÂMeCH<sub>2</sub>Fc}<sub>6</sub>]Â(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>CNÂ(Bz) (CH<sub>2</sub>Fc)}<sub>2</sub>(dppf)<sub>2</sub>]Â(PF<sub>6</sub>) (<b>3</b>), and [Ag<sub>2</sub>{S<sub>2</sub>CNMeÂ(CH<sub>2</sub>Fc)}<sub>2</sub>(PPh<sub>3</sub>)<sub>2</sub>] (<b>4</b>) (dppf = 1,1′-bisÂ(diphenylphosphino)Âferrocene),
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>]Â(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>]Â(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>]Â(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>]Â(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
An unprecedented
air-stable, nanospheric polyhydrido copper cluster,
[Cu<sub>20</sub>H<sub>11</sub>(S<sub>2</sub>PÂ(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
An unprecedented
air-stable, nanospheric polyhydrido copper cluster,
[Cu<sub>20</sub>H<sub>11</sub>(S<sub>2</sub>PÂ(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
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)Â(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)Â(E<sup>∩</sup>E)<sub>6</sub> and [Cu<sup>I</sup>]<sub>6</sub>(X)Â(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)Â{S<sub>2</sub>PÂ(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)Â(E<sup>∩</sup>E)<sub>6</sub> (X = vacancy, H, O, S, halogen) and [Cu<sup>I</sup>]<sub>6</sub>(X)Â(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
The structure and optical properties of several polynuclear
goldÂ(I)
species, namely, diselenophosphate [AuÂ{μ-Se<sub>2</sub>PÂ(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> [AuÂ{μ-Se<sub>2</sub>PÂ(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
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)Â(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)Â(E<sup>∩</sup>E)<sub>6</sub> and [Cu<sup>I</sup>]<sub>6</sub>(X)Â(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)Â{S<sub>2</sub>PÂ(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)Â(E<sup>∩</sup>E)<sub>6</sub> (X = vacancy, H, O, S, halogen) and [Cu<sup>I</sup>]<sub>6</sub>(X)Â(E<sup>∩</sup>E)<sub>6</sub> (X = H, halogen)
clusters
A μ<sub>9</sub>-Iodide in a Tricapped Trigonal-Prismatic Geometry
Two luminescent, undecanuclear silver complexes [Ag<sub>11</sub>(μ<sub>9</sub>-I)Â(μ<sub>3</sub>-I)<sub>3</sub>{E<sub>2</sub>PÂ(O<sup>i</sup>Pr)<sub>2</sub>}<sub>6</sub>]Â(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