6 research outputs found

    Nanosized {Pd<sub>4</sub>(μ<sub>4</sub>‑C)}Pd<sub>32</sub>(CO)<sub>28</sub>(PMe<sub>3</sub>)<sub>14</sub> Containing Tetrahedrally Deformed Pd<sub>4</sub> Cage with Encapsulated Carbide Atom: Formal Substitution of Geometrically Analogous Interior Au<sub>4</sub> Entity in Isostructural Au<sub>4</sub>Pd<sub>32</sub>(CO)<sub>28</sub>(PMe<sub>3</sub>)<sub>14</sub> by Electronically Equivalent Pd<sub>4</sub>(μ<sub>4</sub>‑C) and Computational/Catalytic Implications

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    This first homopalladium carbido cluster, {Pd<sub>4</sub>(μ<sub>4</sub>-C)}­Pd<sub>32</sub>(CO)<sub>28</sub>(PMe<sub>3</sub>)<sub>14</sub> (<b>1</b>), was isolated (3–7% yields) from an ultimately simplified procedurethe reaction of CHCl<sub>3</sub> under N<sub>2</sub> with either Pd<sub>8</sub>(CO)<sub>8</sub>­(PMe<sub>3</sub>)<sub>7</sub> or Pd<sub>10</sub>(CO)<sub>12</sub>­(PMe<sub>3</sub>)<sub>6</sub> at room temperature. Charge-coupled device (CCD) X-ray diffraction data at 100 K for <b>1</b>·2.5 C<sub>6</sub>H<sub>14</sub> (<b>1a</b>) and <b>1</b>·3 CHCl<sub>3</sub> (<b>1b</b>) produced closely related molecular parameters for <b>1</b>. This {Pd<sub>4</sub>C}­Pd<sub>32</sub> cluster (<b>1</b>) possesses a highly unusual tetracoordinated carbide atom that causes a major distortion of a central regular Pd<sub>4</sub> tetrahedron into a new symmetry type of encapsulated Pd<sub>4</sub> cage of pseudo-<i>D</i><sub>2</sub> (222) symmetry. Mean Pd–Pd distances for the three pairs of opposite twofold-equivalent Pd–Pd tetrahedral-like edges for <b>1a</b> are 2.71, 2.96, and 3.59 Å; the mean of the four Pd–C distances [range, 1.87(2)–1.94(2) Å] is 1.91 Å. An astonishing molecular feature is that this {Pd<sub>4</sub>C}­Pd<sub>32</sub> cluster (<b>1</b>) is an isostructural and electronically equivalent analogue of the nanosized Au<sub>4</sub>Pd<sub>32</sub>(CO)<sub>28</sub>­(PMe<sub>3</sub>)<sub>14</sub> (<b>2</b>). Cluster <b>2</b>, likewise a pseudo-<i>D</i><sub>2</sub> molecule, contains a geometrically analogous tetrahedrally deformed interior Au<sub>4</sub> entity encapsulated within an identical Pd<sub>32</sub>(CO)<sub>28</sub>(PMe<sub>3</sub>)<sub>14</sub> shell; mean distances for the three corresponding symmetry-equivalent pairs of slightly smaller opposite tetrahedral-distorted Au–Au edges are 2.64, 2.90, and 3.51 Å. A computational study by both a natural population analysis (NPA) and an atoms-in-molecules (AIM) method performed on model analogues {Pd<sub>4</sub>C}­Pd<sub>32</sub>­(CO)<sub>28</sub>(PH<sub>3</sub>)<sub>14</sub> (<b>1-mod</b>) and Au<sub>4</sub>Pd<sub>32</sub>­(CO)<sub>28</sub>(PH<sub>3</sub>)<sub>14</sub> (<b>2-mod</b>) suggested that the negatively charged Au<sub>4</sub> entity in <b>2-mod</b> may be described as two weakly interacting electron-pair Au<sub>2</sub> intradimers. In contrast, an NPA of the {Pd<sub>4</sub>C} entity in <b>1-mod</b> revealed that two similarly oriented identical Pd<sub>2</sub> intradimers of 2.71 Å are primarily stabilized by Pd–C bonding with a negatively charged carbide atom. The isostructural stabilizations of <b>1</b> and <b>2</b> are then attributed to the similar sizes, shapes, and overall negative charge distributions of the electronically equivalent interior {Pd<sub>4</sub>C} and Au<sub>4</sub> entities. This resulting remarkable structural/electronic equivalency between <b>1</b> and <b>2</b> is consistent with the greatly improved performances of commercial palladium catalysts for vinyl acetate synthesis by gold-atom incorporation to suppress carbonization of the Pd atoms, namely, that the extra Au 6s<sup>1</sup> valence electron of each added Au atom provides an effective “negative charge protection” against electron-donating carbon atoms forming Pd carbido species such as {Pd<sub>4</sub>C}

    Nanosized {Pd<sub>4</sub>(μ<sub>4</sub>‑C)}Pd<sub>32</sub>(CO)<sub>28</sub>(PMe<sub>3</sub>)<sub>14</sub> Containing Tetrahedrally Deformed Pd<sub>4</sub> Cage with Encapsulated Carbide Atom: Formal Substitution of Geometrically Analogous Interior Au<sub>4</sub> Entity in Isostructural Au<sub>4</sub>Pd<sub>32</sub>(CO)<sub>28</sub>(PMe<sub>3</sub>)<sub>14</sub> by Electronically Equivalent Pd<sub>4</sub>(μ<sub>4</sub>‑C) and Computational/Catalytic Implications

    No full text
    This first homopalladium carbido cluster, {Pd<sub>4</sub>(μ<sub>4</sub>-C)}­Pd<sub>32</sub>(CO)<sub>28</sub>(PMe<sub>3</sub>)<sub>14</sub> (<b>1</b>), was isolated (3–7% yields) from an ultimately simplified procedurethe reaction of CHCl<sub>3</sub> under N<sub>2</sub> with either Pd<sub>8</sub>(CO)<sub>8</sub>­(PMe<sub>3</sub>)<sub>7</sub> or Pd<sub>10</sub>(CO)<sub>12</sub>­(PMe<sub>3</sub>)<sub>6</sub> at room temperature. Charge-coupled device (CCD) X-ray diffraction data at 100 K for <b>1</b>·2.5 C<sub>6</sub>H<sub>14</sub> (<b>1a</b>) and <b>1</b>·3 CHCl<sub>3</sub> (<b>1b</b>) produced closely related molecular parameters for <b>1</b>. This {Pd<sub>4</sub>C}­Pd<sub>32</sub> cluster (<b>1</b>) possesses a highly unusual tetracoordinated carbide atom that causes a major distortion of a central regular Pd<sub>4</sub> tetrahedron into a new symmetry type of encapsulated Pd<sub>4</sub> cage of pseudo-<i>D</i><sub>2</sub> (222) symmetry. Mean Pd–Pd distances for the three pairs of opposite twofold-equivalent Pd–Pd tetrahedral-like edges for <b>1a</b> are 2.71, 2.96, and 3.59 Å; the mean of the four Pd–C distances [range, 1.87(2)–1.94(2) Å] is 1.91 Å. An astonishing molecular feature is that this {Pd<sub>4</sub>C}­Pd<sub>32</sub> cluster (<b>1</b>) is an isostructural and electronically equivalent analogue of the nanosized Au<sub>4</sub>Pd<sub>32</sub>(CO)<sub>28</sub>­(PMe<sub>3</sub>)<sub>14</sub> (<b>2</b>). Cluster <b>2</b>, likewise a pseudo-<i>D</i><sub>2</sub> molecule, contains a geometrically analogous tetrahedrally deformed interior Au<sub>4</sub> entity encapsulated within an identical Pd<sub>32</sub>(CO)<sub>28</sub>(PMe<sub>3</sub>)<sub>14</sub> shell; mean distances for the three corresponding symmetry-equivalent pairs of slightly smaller opposite tetrahedral-distorted Au–Au edges are 2.64, 2.90, and 3.51 Å. A computational study by both a natural population analysis (NPA) and an atoms-in-molecules (AIM) method performed on model analogues {Pd<sub>4</sub>C}­Pd<sub>32</sub>­(CO)<sub>28</sub>(PH<sub>3</sub>)<sub>14</sub> (<b>1-mod</b>) and Au<sub>4</sub>Pd<sub>32</sub>­(CO)<sub>28</sub>(PH<sub>3</sub>)<sub>14</sub> (<b>2-mod</b>) suggested that the negatively charged Au<sub>4</sub> entity in <b>2-mod</b> may be described as two weakly interacting electron-pair Au<sub>2</sub> intradimers. In contrast, an NPA of the {Pd<sub>4</sub>C} entity in <b>1-mod</b> revealed that two similarly oriented identical Pd<sub>2</sub> intradimers of 2.71 Å are primarily stabilized by Pd–C bonding with a negatively charged carbide atom. The isostructural stabilizations of <b>1</b> and <b>2</b> are then attributed to the similar sizes, shapes, and overall negative charge distributions of the electronically equivalent interior {Pd<sub>4</sub>C} and Au<sub>4</sub> entities. This resulting remarkable structural/electronic equivalency between <b>1</b> and <b>2</b> is consistent with the greatly improved performances of commercial palladium catalysts for vinyl acetate synthesis by gold-atom incorporation to suppress carbonization of the Pd atoms, namely, that the extra Au 6s<sup>1</sup> valence electron of each added Au atom provides an effective “negative charge protection” against electron-donating carbon atoms forming Pd carbido species such as {Pd<sub>4</sub>C}

    High-Yield Synthesis of PPh<sub>3</sub>-Ligated Decanuclear Tl–Pd Cluster, Pd<sub>9</sub>[Tl(acac)](CO)<sub>9</sub>(PPh<sub>3</sub>)<sub>6</sub>: Comparative Analysis of Tl(I)–Pd(0) Bonding Connectivities with Known Tl–Pd Clusters and Resulting Insight Concerning Their Dissimilar Dynamic Solution Behavior

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    The new Tl­(I)–Pd(0) cluster Pd<sub>9</sub>[μ<sub>3/3</sub>-Tl­(acac)]­(μ<sub>2</sub>-CO)<sub>6</sub>(μ<sub>3</sub>-CO)<sub>3</sub>(PPh<sub>3</sub>)<sub>6</sub> (<b>1</b>) was prepared in high yields (over 90%), both by reaction of Pd<sub>10</sub>(CO)<sub>12</sub>(PPh<sub>3</sub>)<sub>6</sub> (<b>4</b>), PPh<sub>3</sub>, and TlPF<sub>6</sub> in THF in the presence of acetylacetone (Hacac) and base (NEt<sub>3</sub>) and by direct reaction of Pd<sub>10</sub>(CO)<sub>12</sub>(PPh<sub>3</sub>)<sub>6</sub> with PPh<sub>3</sub> and Tl­(acac). The composition and molecular structure of <b>1</b> were unambiguously established from 100 K CCD X-ray diffractometry studies of two solvated crystals, <b>1</b>·1.5Hacac·0.5THF (<b>1A</b>) and <b>1</b>·0.3THF (<b>1B</b>), which showed essentially identical geometries for the entire Pd<sub>9</sub>Tl­(CO)<sub>9</sub>P<sub>6</sub> fragment of pseudo-<i>C</i><sub>3<i>v</i></sub> symmetry; its composition is in agreement with X-ray Tl/Pd field-emission microanalysis with a scanning electron microscope for crystals of <b>1B</b>. This cluster can be viewed as a markedl<i></i>y deformed Pd<sub>6</sub> octahedron (oct) with the three Pd­(oct) atoms of one of its eight triangular faces connected both by three edge-bridging wingtip (wt) Pd­(μ<sub>2</sub>-CO)<sub>2</sub>PPh<sub>3</sub> fragments and by a symmetrical capping Tl­(I). Three triply bridging carbonyl ligands asymmetrically cap the lower alternate 3-fold-related triangular faces of the Pd<sub>6</sub> octahedron, and the three other PPh<sub>3</sub> ligands are each coordinated to Pd atoms in the geometrically opposite staggered Pd­(oct)<sub>3</sub> face. The 6s<sup>2</sup>5d<sup>10</sup> Tl­(I) is also equivalently attached to both chelating O atoms of a bidentate acetylacetonate (acac) monoanion. Although the <i>C</i><sub>2</sub> axis of the pseudo-<i>C</i><sub>2<i>v</i></sub> planar Tl­(acac) fragment is approximately parallel to the pseudo-<i>C</i><sub>3</sub> axis of the TlPd<sub>9</sub> core, the orientation of the Tl­(acac) plane relative to the octahedral-based Pd<sub>9</sub> geometry is considerably different for each of the three independent nondisordered molecules of <b>1</b> in <b>1A</b> and <b>1B</b>; these different planar Tl­(acac) orientations may be mainly attributed to anisotropic crystal-packing effects. Coordination of the Tl­(I) atom to the three Pd­(oct) atoms of the Pd<sub>9</sub> core presumably occurs via its so-called “inert” 6s<sup>2</sup> electron pair with resulting three short Tl–Pd­(oct) connectivities of mean distance 2.83 Å; these connectivities together with three longer Tl–Pd­(wt) ones of mean distance 3.15 Å give rise to a (crown-like)­Pd<sub>6</sub> sextuple (μ<sub>3/3</sub>-Tl) coordination mode. Of particular stereochemical interest is a comparison of solution behavior of <b>1</b> with that for the known structurally related analogue, Pd<sub>9</sub>[μ<sub>3</sub>-TlCo­(CO)<sub>3</sub>L]­(μ<sub>2</sub>-CO)<sub>6</sub>(μ<sub>3</sub>-CO)<sub>3</sub>L<sub>6</sub> (<b>2</b>) (with L = PEt<sub>3</sub> instead of PPh<sub>3</sub>). In <b>2</b> the Tl­(I) is alternatively attached to a trigonal-bipyramidal Co­(CO)<sub>3</sub>L monoanion and primarily coordinated to the three inner Pd­(oct) atoms of a similar PR<sub>3</sub>/CO-ligated octahedron; corresponding Tl–Pd­(oct) and Tl–Pd­(wt) mean distances for two independent molecules in <b>2</b> are 2.77 and 3.31 Å, respectively. Variable-temperature <sup>31</sup>P­{<sup>1</sup>H} NMR solution data of <b>1</b> indicate the occurrence of presumed fast wobbling-like motion of the [μ<sub>3/3</sub>-Tl­(acac)] entity about the pseudo-<i>C</i><sub>3</sub> axis of the Pd<sub>9</sub>(μ<sub>2</sub>-CO)<sub>6</sub>(μ<sub>3</sub>-CO)<sub>3</sub>P<sub>6</sub> fragment <i>without Pd–Tl detachment</i> (i.e., the entire cluster of <b>1</b> remains intact). In direct contrast, corresponding temperature-dependent <sup>31</sup>P and <sup>13</sup>C NMR data of <b>2</b> instead are consistent with <i>rapid, reversible dissociation/association of the entire</i> [μ<sub>3</sub>-TlCo­(CO)<sub>3</sub>L] ligand from the analogous Pd<sub>9</sub>(μ<sub>2</sub>-CO)<sub>6</sub>(μ<sub>3</sub>-CO)<sub>3</sub>P<sub>6</sub> fragment of <b>2</b>. This highly dissimilar dynamic solution behavior that points to a stronger Tl­(I) attachment to the Pd<sub>9</sub> core in <b>1</b> than that in <b>2</b> may be attributed from the above crystallographic evidence to greater involvement of the outer three wingtip Pd­(wt) atoms in bonding connectivities to the Tl­(I) in <b>1</b> compared to predominant bonding connectivities of only the three inner Pd­(oct) atoms to the Tl­(I) in <b>2</b>. <sup>1</sup>H NMR solution spectra of <b>1</b> also suggest significant covalent character in the bidentate Tl–O­(acac) bonding in <b>1</b> based upon the observation of H­(acac)–Tl coupling; this premise is consistent with its Tl–O distances of 2.35 Å (av) being ca. 0.2 Å shorter than those of 2.52 Å (av) found in crystalline Tl­(acac), which with no observed H–Tl NMR coupling in solution implies ionicity of its bidentate Tl–O bonding. Both <b>1</b> and <b>2</b> conform to an 86 CVE count expected for an octahedral metal polyhedron based upon the Tl­(I) and each wingtip Pd­(μ<sub>2</sub>-CO)<sub>2</sub>L fragment contributing 2 and 4 CVEs, respectively

    Isolation and Structural Characterization of a Mackay 55-Metal-Atom Two-Shell Icosahedron of Pseudo‑<i>I</i><sub><i>h</i></sub> Symmetry, Pd<sub>55</sub>L<sub>12</sub>(μ<sub>3</sub>‑CO)<sub>20</sub> (L = PR<sub>3</sub>, R = Isopropyl): Comparative Analysis with Interior Two-Shell Icosahedral Geometries in Capped Three-Shell Pd<sub>145</sub>, Pt-Centered Four-Shell Pd–Pt M<sub>165</sub>, and Four-Shell Au<sub>133</sub> Nanoclusters

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    We present the first successful isolation and crystallographic characterization of a Mackay 55-metal-atom two-shell icosa­hedron, Pd<sub>55</sub>L<sub>12</sub>­(μ<sub>3</sub>-CO)<sub>20</sub> (L = PPr<sup>i</sup><sub>3</sub>) (<b>1</b>). Its two-shell icosa­hedron of pseudo-<i>I</i><sub><i>h</i></sub> symmetry (without isopropyl substituents) enables a structural/bonding comparison with <i>interior</i> 55-metal-atom two-shell icosa­hedral geometries observed within the multi-shell capped 145-metal-atom three-shell Pd<sub>145</sub>­(CO)<sub>72</sub>­(PEt<sub>3</sub>)<sub>30</sub> and 165-metal-atom four-shell Pt-centered (μ<sub>12</sub>-Pt)­Pd<sub>164‑<i>x</i></sub>Pt<sub><i>x</i></sub>­(CO)<sub>72</sub>­(PPh<sub>3</sub>)<sub>20</sub> (<i>x</i> ≈ 7) nanoclusters, and within the recently reported four-shell Au<sub>133</sub>(SC<sub>6</sub>H<sub>4</sub>-<i>p</i>-Bu<sup>t</sup>)<sub>52</sub> nanocluster. DFT calculations carried out on a Pd<sub>55</sub>­(CO)<sub>20</sub>(PH<sub>3</sub>)<sub>12</sub> model analogue, with triisopropyl phosphine substituents replaced by H atoms, revealed a positive +0.84 <i>e</i> charge for the entire Pd<sub>55</sub> core, with a highly positive second-shell Pd<sub>42</sub> surface of +1.93 <i>e</i>
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