25 research outputs found

    {Sn<sub>9</sub>[Si(SiMe<sub>3</sub>)<sub>3</sub>]<sub>2</sub>}<sup>2ā€‘</sup>: A Metalloid Tin Cluster Compound With a Sn<sub>9</sub> Core of Oxidation State Zero

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    The disproportionation reaction of the subvalent metastable halide SnCl proved to be a powerful synthetic method for the synthesis of metalloid cluster compounds of tin. Now we present the synthesis and structural characterization of the anionic metalloid cluster compound [Sn<sub>9</sub>[SiĀ­(SiMe<sub>3</sub>)<sub>3</sub>]<sub>2</sub>]<sup>2ā€‘</sup> <b>3</b> where the oxidation state of the tin atoms is zero. Quantum chemical calculations as well as MoĢˆssbauer spectroscopic investigations show that three different kinds of tin atoms are present within the cluster core. Compound <b>3</b> is highly reactive as shown by NMR investigations, thus being a good starting material for further ongoing research on the reactivity of such partly shielded metalloid cluster compounds

    {Sn<sub>9</sub>[Si(SiMe<sub>3</sub>)<sub>3</sub>]<sub>2</sub>}<sup>2ā€‘</sup>: A Metalloid Tin Cluster Compound With a Sn<sub>9</sub> Core of Oxidation State Zero

    No full text
    The disproportionation reaction of the subvalent metastable halide SnCl proved to be a powerful synthetic method for the synthesis of metalloid cluster compounds of tin. Now we present the synthesis and structural characterization of the anionic metalloid cluster compound [Sn<sub>9</sub>[SiĀ­(SiMe<sub>3</sub>)<sub>3</sub>]<sub>2</sub>]<sup>2ā€‘</sup> <b>3</b> where the oxidation state of the tin atoms is zero. Quantum chemical calculations as well as MoĢˆssbauer spectroscopic investigations show that three different kinds of tin atoms are present within the cluster core. Compound <b>3</b> is highly reactive as shown by NMR investigations, thus being a good starting material for further ongoing research on the reactivity of such partly shielded metalloid cluster compounds

    {Sn<sub>9</sub>[Si(SiMe<sub>3</sub>)<sub>3</sub>]<sub>2</sub>}<sup>2ā€‘</sup>: A Metalloid Tin Cluster Compound With a Sn<sub>9</sub> Core of Oxidation State Zero

    No full text
    The disproportionation reaction of the subvalent metastable halide SnCl proved to be a powerful synthetic method for the synthesis of metalloid cluster compounds of tin. Now we present the synthesis and structural characterization of the anionic metalloid cluster compound [Sn<sub>9</sub>[SiĀ­(SiMe<sub>3</sub>)<sub>3</sub>]<sub>2</sub>]<sup>2ā€‘</sup> <b>3</b> where the oxidation state of the tin atoms is zero. Quantum chemical calculations as well as MoĢˆssbauer spectroscopic investigations show that three different kinds of tin atoms are present within the cluster core. Compound <b>3</b> is highly reactive as shown by NMR investigations, thus being a good starting material for further ongoing research on the reactivity of such partly shielded metalloid cluster compounds

    Structure and Bonding of Bi<sub>4</sub>Ir: A Difficult-to-Access Bismuth Iridide with a Unique Framework Structure

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    Crystals of Bi<sub>4</sub>Ir, a new intermetallic compound, were obtained by the reaction of an iridium-containing intermetallic precursor with liquid bismuth. X-ray diffraction on a single crystal revealed a rhombohedral structure [<i>R</i>3Ģ…<i>m</i>, <i>a</i> = 2656.7(2) pm, and <i>c</i> = 701.6(4) pm]. Bi<sub>4</sub>Ir is not isostructural to Bi<sub>4</sub>Rh but combines motifs of the metastable superconductor Bi<sub>14</sub>Rh<sub>3</sub> with those found in the weak topological insulator Bi<sub>14</sub>Rh<sub>3</sub>I<sub>9</sub>. The two crystallographically independent iridium sites in Bi<sub>4</sub>Ir have square-prismatic and skewed-square-antiprismatic bismuth coordination with Biā€“Ir distances of 283ā€“287 pm. By sharing common edges, the two types of [IrBi<sub>8</sub>] units constitute a complex three-dimensional network of rings and helices. The bonding in the heterometallic framework is dominated by pairwise Biā€“Ir interactions. In addition, three-center bonds are found in the bismuth triangles formed by adjacent [IrBi<sub>8</sub>] polyhedra. Density functional theory based band-structure calculations suggest metallic properties

    Synthesis and Crystal Structure Determination of Ag<sub>9</sub>FeS<sub>4.1</sub>Te<sub>1.9</sub>, the First Example of an Iron Containing Argyrodite

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    Ag<sub>9</sub>FeS<sub>4.1</sub>Te<sub>1.9</sub> was prepared by solid state synthesis from stoichiometric amounts of the elements at 873 K. The compound forms gray crystals which are stable against air and moisture. The crystal structure was determined by X-ray diffraction from selected single crystals. Ag<sub>9</sub>FeS<sub>4.1</sub>Te<sub>1.9</sub> crystallizes in the space group <i>F</i>4Ģ…3<i>m</i>, <i>a</i> = 11.0415(7) ƅ, <i>V</i> = 1346.1(1) ƅ<sup>3</sup>, and <i>Z</i> = 4 (powder data at 293 K). The compound shows a reversible phase transition upon cooling to the space group <i>P</i>2<sub>1</sub>3, <i>a</i> = 11.0213(1) ƅ, <i>V</i> = 1338.75(2) ƅ<sup>3</sup>, and <i>Z</i> = 4 (single crystal data at 200 K). The title compound is the first example of an iron containing argyrodite-type material with Fe<sup>3+</sup> located in tetrahedral sites. Silver atoms are disordered at room temperature which was taken into account by nonharmonic refinement of the silver positions. The refinement converged to <i>R</i><sub>1</sub> = 3.51% and <i>wR</i><sub>2</sub> = 10.66% for the room temperature measurement and to <i>R</i><sub>1</sub> = 1.55% and <i>wR</i><sub>2</sub>= 5.23% for the 200 K data set (all data). Impedance measurements were performed in the temperature range from 323 to 473 K. Ionic conductivity values are 1.81 Ɨ 10<sup>ā€“2</sup> S cm<sup>ā€“1</sup> at 323 K and 1.41 Ɨ 10<sup>ā€“1</sup> S cm<sup>ā€“1</sup> at 468 K. The activation energy is 0.19 eV from 323 to 423 K and 0.06 eV from 393 to 473 K. DTA measurements reveal congruent melting at 907 K. A phase transition temperature of 232 K with an enthalpy of 7.9 kJ/mol was determined by DSC measurements. <sup>57</sup>Fe MoĢˆssbauer spectra show one signal at 298 K and a doublet at 78 K, indicating Fe<sup>3+</sup> and structural distortions upon cooling the samples. Hyperfine field splitting of iron is observed at 5 K. Measurements of the molar susceptibility revealed that the compound is paramagnetic down to a NeĢel temperature of <i>T</i><sub>N</sub> = 22.1(5) K. Antiferromagnetic ordering is observed at lower temperatures

    Ferrocenyl-Functionalized Sn/Se and Sn/Te Complexes: Synthesis, Reactivity, Optical, and Electronic Properties

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    An adamantane-shaped, ferrocenyl-substituted tin selenide complex, [(FcSn)<sub>4</sub>Se<sub>6</sub>] (<b>1</b>; Fc = ferrocenyl), and a ferrocenyl-substituted tin telluride five-membered ring, [(Fc<sub>2</sub>Sn)<sub>3</sub>Te<sub>2</sub>] (<b>2</b>), were obtained upon treatment of FcSnCl<sub>3</sub> with K<sub>2</sub>E (E = Se, Te). Complex <b>1</b> further reacts with Na<sub>2</sub>SĀ·9H<sub>2</sub>O and [CuĀ­(PPh<sub>3</sub>)<sub>3</sub>Cl] to form a ternary complex, [(CuPPh<sub>3</sub>)<sub>6</sub>(S/Se)<sub>6</sub>(SnFc)<sub>2</sub>] (<b>3</b>). We discuss structures, optical and electrochemical properties as well as MoĢˆssbauer spectra

    Polynitroxides from Alkoxyamine Monomers: Structural and Kinetic Investigations by Solid State NMR

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    A novel synthetic route toward polyĀ­(4-methacryloyloxy-2,2,6,6-tetramethylpiperidine-<i>N</i>-oxyl) (PTMA) is described. The polymerization of alkoxyamine-based monomers by atom transfer radical polymerization (ATRP) was investigated, as the polyalkoxyamine serves as the precursor for PTMA. The polydispersity indices (PDIs) and the kinetic data of the polymerization indicate a controlled reaction. The oxidative Cā€“O bond cleavages of the polyalkoxyamine lead to PTMA. This transformation occurs with excellent yields, and it is possible to transfer the narrow PDIs of the prepolymer to PTMA. The material is characterized in detail using cyclic voltammetry in solution and magnetic susceptibility measurements as well as multinuclear solid state NMR and EPR spectroscopies. The conversion of the precursor polymer to the polynitroxide can be conveniently monitored by <sup>1</sup>H and <sup>19</sup>F magic-angle spinning (MAS) as well as <sup>13</sup>CĀ­{<sup>1</sup>H} cross-polarization (CP)-MAS NMR. In addition, the intermolecular interaction of the nitroxide side chain units in the polymer at high conversion can be detected and monitored by the observation of pronounced low-frequency shifts

    Ultraviolet Upconversion Luminescence in a Highly Transparent Triply-Doped Gd<sup>3+</sup>ā€“Tm<sup>3+</sup>ā€“Yb<sup>3+</sup> Fluorideā€“Phosphate Glasses

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    We report near-infrared to ultraviolet (UV) upconversion emissions in triply-doped Gd<sup>3+</sup>ā€“Tm<sup>3+</sup>ā€“Yb<sup>3+</sup> fluorideā€“phosphate glasses. Emission at 310 nm, originated from the Gd<sup>3+</sup>:<sup>6</sup>P<sub>7/2</sub> ā†’ <sup>8</sup>S<sub>7/2</sub> transition, was observed for the first time in glasses. The high-purity glasses prepared exhibit extended transparency in the UV down to 200ā€“250 nm. The mixed fluorideā€“phosphate environment of the rare-earth ions was characterized by means of NMR techniques using scandium as a diamagnetic mimic for the luminescent species, for which the ligand distribution was quantified by <sup>45</sup>ScĀ­{<sup>31</sup>P} rotational echo double-resonance NMR. Both the intensity of the Gd<sup>3+</sup> emission as well as those of the UV emissions at 290, 347, and 363 nm increase with increasing ratio of fluoride to phosphate ligands coordinating to the rare-earth ion

    Solid Solution Quantum Dots with Tunable Dual or Ultrabroadband Emission for LEDs

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    Quantum dots that efficiently emit white light directly or feature a ā€œcandle-likeā€ orange photoluminescence with a high Stokes shift are presented. The key to obtaining these unique emission properties is through controlled annealing of the core Cu-In-Ga-S quantum dots in the presence of zinc ions, thus forming Zn-Cu-In-Ga-S solid solutions with different distributions of the substitution and dopant elements. The as-obtained nanocrystals feature excellent quantum yields of up to 82% with limited or even eliminated reabsorption and a color rendering index of bare particles of up to 88, enabling the production of high-quality white LEDs using a single color converter layer. Furthermore, the color properties can be tuned by changing the experimental conditions as well as by varying the excitation wavelength. The multicomponent luminescence mechanism is discussed in detail based on similar literature reports. White LEDs with unparalleled color quality and competitive luminous efficacies are presented herein

    Doped Semimetal Clusters: Ternary, Intermetalloid Anions [Ln@Sn<sub>7</sub>Bi<sub>7</sub>]<sup>4ā€“</sup> and [Ln@Sn<sub>4</sub>Bi<sub>9</sub>]<sup>4ā€“</sup> (Ln = La, Ce) with Adjustable Magnetic Properties

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    Two K([2.2.2]Ā­crypt) salts of lanthanide-doped semimetal clusters were prepared, both of which contain at the same time two types of ternary intermetalloid anions, [Ln@Sn<sub>7</sub>Bi<sub>7</sub>]<sup>4ā€“</sup> and [Ln@Sn<sub>4</sub>Bi<sub>9</sub>]<sup>4ā€“</sup>, in 0.70:0.30 (Ln = La) or 0.39:0.61 (Ln = Ce) ratios. The cluster shells represent nondeltahedral, fullerane-type arrangements of 14 or 13 main group metal atoms that embed the Ln<sup>3+</sup> cations. The assignment of formal +III oxidation states for the Ln sites was confirmed by means of magnetic measurements that reveal a diamagnetic LaĀ­(III) compound and a paramagnetic CeĀ­(III) analogue. Whereas the cluster anions with a 14-atomic main-group metal cage represent the second examples in addition to a related EuĀ­(II) cluster published just recently, the 13-atomic cages exhibit a yet unprecedented enneahedral topology. In contrast to the larger cages, which accord to the Zintlā€“Klemmā€“Busmann electron numberā€“structure correlation, the smaller clusters require a more profound interpretation of the bonding situation. Quantum chemical investigations served to shed light on these unusual complexes and showed significant narrowing of the HOMOā€“LUMO gap upon incorporation of Ce<sup>3+</sup> within the semimetal cages
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