248 research outputs found

    (S)-6-Methyl-∊-caprolactone

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    The chiral title compound, C7H12O2, a lactone derivative, features a seven-membered ring that adopts a chair conformation. The crystal structure is stabilized by weak C—H⋯O inter­actions occurring in the (100) plane. The absolute configuration was assigned on the basis of the enantioselective synthesis

    (4aS,5R,7R,8S,8aR)-8-(1,3-Dioxolan-2-yl)-7,8-dimethyl-5-(1-methyl­ethen­yl)perhydro­naphthalen-2-one

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    In the chiral title compound, C18H28O3, the two six-membered rings of the perhydronaphthalenone adopt a rigid chair–chair conformation and the five-membered dioxolanyl ring adopts an envelope conformation. The crystal structure is stabilized only by weak inter­actions

    Quantum paramagnetism in a non-Kramers rare-earth oxide: Monoclinic Pr2Ti2O7\rm Pr_2Ti_2O_7

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    Little is so far known about the magnetism of the A2B2O7\rm A_2B_2O_7 monoclinic layered perovskites that replace the spin-ice supporting pyrochlore structure for rA/rB>1.78r_A/r_B>1.78. We show that high quality monoclinic Pr2_2Ti2_2O7_7 single crystals with a three-dimensional network of non-Kramers Pr3+^{3+} ions that interact through edge-sharing super-exchange interactions, form a singlet ground state quantum paramagnet that does not undergo any magnetic phase transitions down to at least 1.8 K. The chemical phase stability, structure, and magnetic properties of the layered perovskite Pr2_2Ti2_2O7_7 were investigated using x-ray diffraction, transmission electron microscopy, and magnetization measurements. Synthesis of polycrystalline samples with the nominal compositions of Pr2_2Ti2+x_{2+x}O7_7 (0.16x0.16-0.16 \leq x \leq 0.16) showed that deviations from the Pr2_2Ti2_2O7_7 stoichiometry lead to secondary phases of related, structures including the perovskite phase Pr2/3_{2/3}TiO3_3 and the orthorhombic phases Pr4_4Ti9_9O24_{24} and Pr2_2TiO5_5. No indications of site disordering (stuffing and anti-stuffing) or vacancy defects were observed in the Pr2_2Ti2_2O7_7 majority phase. A procedure for growth of high-structural-quality, stoichiometric single crystals of Pr2_2Ti2_2O7_7 by the traveling solvent floating zone (TSFZ) method is reported. Thermo-magnetic measurements of single-crystalline Pr2_2Ti2_2O7_7 reveal an isolated singlet ground state that we associate with the low symmetry crystal electric field environments that split the 2J+1=92J+1=9-fold degenerate spin-orbital multiplets of the four differently coordinated Pr3+^{3+} ions into 36 isolated singlets resulting in an anisotropic temperature independent van-Vleck susceptibility at low TT. A small isotropic Curie term is associated with 0.96(2)\% non-interacting Pr4+^{4+} impurities.Comment: 18 pages, 7 figures, 6 table

    Ruthenium-Locked Helical Chirality: A Barrier of Inversion and Formation of an Asymmetric Macrocycle

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    Upon coordination to metal centers, tetradentate ligands based on the 6,6'-bis(2 ''-aminopyridyl)-2,2'-bipyridine (bapbpy) structure form helical chiral complexes due to the steric clash between the terminal pyridines of the ligand. For octahedral ruthenium(II) complexes, the two additional axial ligands bound to the metal center, when different, generate diastereotopic aromatic protons that can be distinguished by NMR. Based on these geometrical features, the inversion barrier of helical [Ru-II(L)(RR'SO)Cl](+) complexes, where L is a sterically hindered bapbpy derivative and RR'SO is a chiral or achiral sulfoxide ligand, was studied by variable-temperature H-1 NMR The coalescence energies for the inversion of the helical chirality of [Ru(bapbpy)(DMSO)(Cl)]Cl and [Ru(bapbpy)(MTSO)(Cl)]Cl (where MTSO is (R)-methyl p-tolylsulfoxide) were found to be 43 and 44 kJ/mol, respectively. By contrast, in [Ru(biqbpy)(DMSO)(Cl)]Cl (biqbpy = 6,6'-bis(aminoquinolyl)-2,2'-bipyridine increased strain caused by the larger terminal quinoline groups resulted in a coalescence temperature higher than 376 K, which pointed to an absence of helical chirality inversion at room temperature. Further increasing the steric strain by introducing methoxy groups ortho to the nitrogen atoms of the terminal pyridyl groups in bapbpy resulted in the serendipitous discovery of a ring-closing reaction that took place upon trying to make [Ru(OMe-bapbpy)(DMSO)Cl](+) (OMe-bapbpy = 6,6'-bis(6-methoxy-aminopyridyl)2,2'-bipyridine). This reaction generated, in excellent yields, a chiral complex [Ru(L '')(DMSO)Cl]Cl, where L '' is an asymmetric tetrapyridyl macrocycle. This unexpected transformation appears to be specific to ruthenium(II) as macrocyclization did not occur upon coordination of the same ligand to palladium(II) or rhodium(III).Macromolecular Biochemistr

    Shorter Alkyl Chains Enhance Molecular Diffusion and Electron Transfer Kinetics between Photosensitisers and Catalysts in CO2 -Reducing Photocatalytic Liposomes.

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    Funder: Nederlandse Organisatie voor Wetenschappelijk Onderzoek; Id: http://dx.doi.org/10.13039/501100003246Covalent functionalisation with alkyl tails is a common method for supporting molecular catalysts and photosensitisers onto lipid bilayers, but the influence of the alkyl chain length on the photocatalytic performances of the resulting liposomes is not well understood. In this work, we first prepared a series of rhenium-based CO2 -reduction catalysts [Re(4,4'-(Cn H2n+1 )2 -bpy)(CO)3 Cl] (ReCn ; 4,4'-(Cn H2n+1 )2 -bpy=4,4'-dialkyl-2,2'-bipyridine) and ruthenium-based photosensitisers [Ru(bpy)2 (4,4'-(Cn H2n+1 )2 -bpy)](PF6 )2 (RuCn ) with different alkyl chain lengths (n=0, 9, 12, 15, 17, and 19). We then prepared a series of PEGylated DPPC liposomes containing RuCn and ReCn , hereafter noted Cn , to perform photocatalytic CO2 reduction in the presence of sodium ascorbate. The photocatalytic performance of the Cn liposomes was found to depend on the alkyl tail length, as the turnover number for CO (TON) was inversely correlated to the alkyl chain length, with a more than fivefold higher CO production (TON=14.5) for the C9 liposomes, compared to C19 (TON=2.8). Based on immobilisation efficiency quantification, diffusion kinetics, and time-resolved spectroscopy, we identified the main reason for this trend: two types of membrane-bound RuCn species can be found in the membrane, either deeply buried in the bilayer and diffusing slowly, or less buried with much faster diffusion kinetics. Our data suggest that the higher photocatalytic performance of the C9 system is due to the higher fraction of the more mobile and less buried molecular species, which leads to enhanced electron transfer kinetics between RuC9 and ReC9

    Mechanomyographic Analysis for Muscle Activity Assessment during a Load-Lifting Task

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    International audienceThe purpose of this study was to compare electromyographic (EMG) with mechanomyographic (MMG) recordings during isometric conditions, and during a simulated load-lifting task. Twenty-two males (age: 25.5 ± 5.3 years) first performed maximal voluntary contractions (MVC) and submaximal isometric contractions of upper limb muscles at 25%, 50% and 75% MVC. Participants then executed repetitions of a functional activity simulating a load-lifting task above shoulder level, at 25%, 50% and 75% of their maximum activity (based on MVC). The low-frequency part of the accelerometer signal (<5 Hz) was used to segment the six phases of the motion. EMG and MMG were both recorded during the entire experimental procedure. Root mean square (RMS) and mean power frequency (MPF) were selected as signal extraction features. During isometric contractions, EMG and MMG exhibited similar repeatability scores. They also shared similar RMS vs. force relationship, with RMS increasing to 75% MVC and plateauing to 100%. MPF decreased with increasing force to 75% MVC. In dynamic condition, RMSMMG exhibited higher sensitivity to changes in load than RMSEMG. These results confirm the feasibility of MMG measurements to be used during functional activities outside the laboratory. It opens new perspectives for future applications in sports science, ergonomics and human–machine interface conception
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