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
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 MoĢssbauer
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
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 MoĢssbauer
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
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 MoĢssbauer
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
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 BiāIr
distances of 283ā287 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 BiāIr 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
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) Ć
, <i>V</i> = 1346.1(1) Ć
<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) Ć
, <i>V</i> = 1338.75(2) Ć
<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 Ć 10<sup>ā2</sup> S cm<sup>ā1</sup> at 323 K and 1.41 Ć 10<sup>ā1</sup> S cm<sup>ā1</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
MoĢssbauer 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 NeĢel 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
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 MoĢssbauer
spectra
Polynitroxides from Alkoxyamine Monomers: Structural and Kinetic Investigations by Solid State NMR
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 CāO 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>āTm<sup>3+</sup>āYb<sup>3+</sup> FluorideāPhosphate Glasses
We
report near-infrared to ultraviolet (UV) upconversion emissions in
triply-doped Gd<sup>3+</sup>āTm<sup>3+</sup>āYb<sup>3+</sup> fluorideāphosphate 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 200ā250 nm. The mixed fluorideāphosphate
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
Quantum dots that
efficiently emit white light directly or feature
a ācandle-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
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 ZintlāKlemmāBusmann
electron numberāstructure 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 HOMOāLUMO gap upon
incorporation of Ce<sup>3+</sup> within the semimetal cages