46 research outputs found
DMP for Age distribuition Austria vs. Vienna
DMP from DMP online for the Data Stewardship project</p
Age distribution Austria vs. Vienna
The Figures produced from the Data Stewardship Project.</p
Age distribution Austria vs. Vienna DMP from RDMO
Age distribution Austria vs. Vienna DMP from RDMO, second DMP as comparison to the first.</p
Trinuclear Ruthenium Macrocycles: Toward Supramolecular Water Oxidation Catalysis in Pure Water
The incorporation of a Ru(bda)(bda
= 2,2′-bipyridine-6,6′-dicarboxylate)
water oxidation catalyst into a trinuclear metallosupramolecular macrocycle
leads to increased stability and activity compared to the mononuclear
reference system. To overcome solubility problems of such large structures
in water and the need for large amounts of organic cosolvents, new
macrocyclic water oxidation catalysts with improved water solubility
become desirable. With triethylene glycol side chains, the required
amount of acetonitrile as a cosolvent was halved, whereas the application
of charged ammonium side chains allowed catalysis in pure water. The
catalytic activity was found to be comparable to the parent compound.
Kinetic experiments were performed to explain the rate differences
between those new derivatives and showed that Coulombic repulsion
between the charged side chains and Ce<sup>IV</sup> leads to slower
oxidation processes
C–Br Activation of Aryl Bromides at Ni<sup>0</sup>(NHC)<sub>2</sub>: Stoichiometric Reactions, Catalytic Application in Suzuki–Miyaura Cross-Coupling, and Catalyst Degradation
Complex [Ni<sub>2</sub>(<sup><i>i</i></sup>Pr<sub>2</sub>Im)<sub>4</sub>(COD)] (<b>1</b>) (<sup><i>i</i></sup>Pr<sub>2</sub>Im = 1,3-diisopropylimidazolin-2-ylidene) is a very
efficient catalyst for the Suzuki–Miyaura cross-coupling reaction
of 4-bromotoluene with phenylboronic acid and also mediates the Ullmann-type
homo-cross-coupling reaction of bromobenzene with a moderate efficiency.
Stoichiometric reactions of complex <b>1</b> with aryl bromides
(ArBr) at room temperature lead to mixtures of aryl bromo complexes
of the type <i>trans</i>-[Ni(<sup><i>i</i></sup>Pr<sub>2</sub>Im)<sub>2</sub>(Br)(Ar)] and the bis(bromo) complex <i>trans</i>-[Ni(<sup><i>i</i></sup>Pr<sub>2</sub>Im)<sub>2</sub>(Br)<sub>2</sub>] <b>2</b>. The complexes <i>trans</i>-[Ni(<sup><i>i</i></sup>Pr<sub>2</sub>Im)<sub>2</sub>(Br)(Ar)]
(for Ar = Ph <b>3</b>, 4-MeC<sub>6</sub>H<sub>4</sub> <b>4</b>, 4-Me(O)CC<sub>6</sub>H<sub>4</sub> <b>5</b>, 4-MeOC<sub>6</sub>H<sub>4</sub> <b>6</b>, 4-MeSC<sub>6</sub>H<sub>4</sub> <b>7</b>, 4-Me<sub>2</sub>NC<sub>6</sub>H<sub>4</sub> <b>8</b>, 2-C<sub>5</sub>NH<sub>4</sub> <b>9</b>) can be selectively
synthesized by working at low temperatures and using a high dilution
of the starting materials. A major deactivation pathway for <i>trans</i>-[Ni(<sup><i>i</i></sup>Pr<sub>2</sub>Im)<sub>2</sub>(Br)(Ar)] was identified in the presence of aryl bromides.
This deactivation process includes (i) the formation of <i>trans</i>-[Ni(<sup><i>i</i></sup>Pr<sub>2</sub>Im)<sub>2</sub>(Br)<sub>2</sub>] from <i>trans</i>-[Ni(<sup><i>i</i></sup>Pr<sub>2</sub>Im)<sub>2</sub>(Br)(Ar)] (<b>2</b>) and ArBr
and (ii) the formation of an imidazolium salt of the type 2[<sup><i>i</i></sup>Pr<sub>2</sub>Im-Ar]<sup>+</sup>[NiBr<sub>4</sub>]<sup>2–</sup> from <i>trans</i>-[Ni(<sup><i>i</i></sup>Pr<sub>2</sub>Im)<sub>2</sub>(Br)<sub>2</sub>] (<b>2</b>) and ArBr. The reactions of complex <b>2</b> with
a series of aryl halides at higher temperatures lead to the decomposition
of the bis(carbene) nickel moiety with formation of the imidazolium
salts 2[<sup>i</sup>Pr<sub>2</sub>Im-Ar]<sup>+</sup>[NiBr<sub>2</sub>X<sub>2</sub>]<sup>2–</sup> (for X = I, Ar = Ph <b>10</b> and X = Br, Ar = Ph <b>11</b>, 4-MeC<sub>6</sub>H<sub>4</sub> <b>12</b>, 4-FC<sub>6</sub>H<sub>4</sub> <b>13</b>,
4-OSi(CH<sub>3</sub>)<sub>3</sub>-C<sub>6</sub>H<sub>4</sub> <b>14</b>) in high yields
To be or not to be – nematic liquid crystals from shape-persistent V-shaped nematogens with the ‘magic angle’
<p>The tetrahedral bending angle in V-shaped nematogens was claimed to be the optimum for finding a biaxial nematic liquid crystal phase. The benzo[1,2-b:4,3-b’]dithiophene core, recently successfully applied as a tetrahedral bending unit in mesogens with lateral flexible chains, is here embedded in a scaffold with only terminal chains, which conventionally promotes the formation of nematic phases at low temperature. A series of new mesogens has been successfully prepared, realising hockey-stick, hockey-stick dimer and V-shaped molecular topologies. Only the hockey-stick mesogens assemble in uniaxial nematic phases over a broad temperature range. Single crystal structure analysis of a hockey-stick and V-shaped compound reveal remarkable similarities with the benzodithiophene core wrapped by aliphatic chains. A model explaining the absence of nematic mesophases in the family of V-shaped, shape-persistent mesogens with terminal aliphatic chains is presented and results in the proposal of a new design for biaxial nematogens.</p
Novel Synthesis and Crystal Structure Analysis of <i>rac</i>-β-(Trimethylsilyl)alanine
A new efficient, convenient, and cost-saving multistep synthesis of rac-2-amino-3-(trimethylsilyl)propanoic acid (rac-β-(trimethylsilyl)alanine, rac-4) has been developed, starting from diethyl malonate (total yield 25%). In addition, rac-4 has been structurally characterized by single-crystal X-ray diffraction
Supplementary document for Spatiospectral Characterization of Ultrafast Pulse-Beams by Multiplexed Broadband Ptychography - 5444836.pdf
Supplemental Documen
Complete Monitoring of Coherent and Incoherent Spin Flip Domains in the Recombination of Charge-Separated States of Donor-Iridium Complex-Acceptor Triads
The spin chemistry of photoinduced
charge-separated (CS) states
of three triads comprising one or two triarylamine donors, a cyclometalated
iridium complex sensitizer and a naphthalene diimide (NDI) acceptor,
was investigated by transient absorption spectroscopy in the ns−μs
time regime. Strong magnetic-field effects (MFE) were observed for
two triads with a phenylene bridge between iridium complex sensitizer
and NDI acceptor. For these triads, the lifetimes of the CS states
increased from 0.6 μs at zero field to 40 μs at about
2 T. Substituting the phenylene by a biphenyl bridge causes the lifetime
of the CS state at zero field to increase by more than 2 orders of
magnitude (τ = 79 μs) and the MFE to disappear almost
completely. The kinetic MFE was analyzed in the framework of a generalized
Hayashi–Nagakura scheme describing coherent (S, T<sub>0</sub> ↔ T<sub>±</sub>) as well as incoherent (S, T<sub>0</sub> ⇌ T<sub>±</sub>) processes by a single rate constant <i>k</i><sub>±</sub>. The magnetic-field dependence of <i>k</i><sub>±</sub> of the triads with phenylene bridge spans
2 orders of magnitude and exhibits a biphasic behavior characterized
by a superposition of two Lorentzians. This biphasic MFE is observed
for the first time and is clearly attributable to the coherent (<i>B</i> < 10 mT) and incoherent (10 mT < <i>B</i> < 2 T) domains of spin motion induced by isotropic and anisotropic
hyperfine coupling. The parameters of both domains are well understood
in terms of the structural properties of the two triads, including
the effect of electron hopping in the triad with two donor moieties.
The kinetic model also accounts for the reduction of the MFE on reducing
the rate constant of charge recombination in the triad with the biphenyl
bridge
spatialChirpGif3.gif
Visualization 1 shows propagation of the central five spectral components of the spatially chirped pulse-beam from the prism experiment without the knife-edge. The top row shows the spatial profile of each beamlet as it propagates. The bottom left panel shows the summed intensity of these spectral components which is calculated from the individually propagated beamlets. The two bottom right panels show sagittal and tangential views of the beams colored by their local wavelengths, which are the same as Fig 3.a) and b). Here we are also showing the propagation of the beamlets, which are colored according to wavelength and have sizes proportional to their second moments. Based on these panels we can separately identify the beamlet crossing plane and focal plane of the beams in each direction
