10 research outputs found

    Nature of oxygen at rocksalt and spinel oxide surfaces

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    The chemical environment of oxygen in cobalt-containing metal oxides with compositions M xM′( x – 1) O and M xM′(3x – 1) O4 (M,M′ = Mn,Ni,Co) has been studied by Auger, x-ray and ultraviolet photoelectron, and high resolution electron energy loss spectroscopies. While there is a single type of lattice oxygen in the bulk structure of simple rocksalt and spinel oxides, the nature of oxygen at the surface of the spinel oxides is considerably more complex. Photoemission from core oxygen states in these materials often shows multiple peaks and satellite structure which have been attributed to a range of intrinsic and extrinsic oxygen states. All of these 3d transition metal oxides show a single, intense O 1s core photoemission peak at approximately 529.6 eV. In the spinel materials, a second state at 531.2 eV is also observed and is shown to be intrinsic to the spinel surface and not a result of hydroxylation or other surface contaminant. Similar photoemission features in Fe3O4 were previously attributed to final state effects; however, the nature of the multiple final states remains to be elucidated

    Effect of the surface structure on the departure from stoichiometry of Co

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    The surface of an oxide may have a composition different from that of the bulk. A method of calculation of the composition of a powder from the surface structure is presented. It is applied to a Co3O4 sample for which data on composition are deduced from gravimetry, neutron scattering and magnetic susceptibility measurements. It is found that at most 20 % of the excess of oxygen above stoichimetry has to be attributed to cation vacancies, the rest being due to the surface. Charges are counted by the same method, showing that surface oxygen are almost exclusively O-

    Horizontal single-walled carbon nanotubes on MgO(110) and MgO(001) substrates

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    International audienceHorizontal single-walled carbon nanotubes (SWNT) on MgO(110) and MgO(001) single-crystal substrates were synthesized in a temperature range of 830-910 degrees C by chemical vapor deposition using Co catalyst particles. SWNTs grow preferentially along the directions of the two MgO surface planes. For synthesis at 830 degrees C, the distribution of the radial breathing mode (RBM) frequencies of SWNTs grown on MgO(110) is centered at 142 and 168 cm (1), attributed to semi-conducting SWNTs. For the same synthesis time, the RBM distribution of SWNTs grown on MgO(001) is significantly broader. This difference would be due to the larger surface energy of MgO(110) which reduces the probability of coalescence between Co particles

    A brain atlas of axonal and synaptic delays based on modelling of cortico-cortical evoked potentials.

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    Epilepsy presurgical investigation may include focal intracortical single-pulse electrical stimulations with depth electrodes, which induce cortico-cortical evoked potentials at distant sites because of white matter connectivity. Cortico-cortical evoked potentials provide a unique window on functional brain networks because they contain sufficient information to infer dynamical properties of large-scale brain connectivity, such as preferred directionality and propagation latencies. Here, we developed a biologically informed modelling approach to estimate the neural physiological parameters of brain functional networks from the cortico-cortical evoked potentials recorded in a large multicentric database. Specifically, we considered each cortico-cortical evoked potential as the output of a transient stimulus entering the stimulated region, which directly propagated to the recording region. Both regions were modelled as coupled neural mass models, the parameters of which were estimated from the first cortico-cortical evoked potential component, occurring before 80 ms, using dynamic causal modelling and Bayesian model inversion. This methodology was applied to the data of 780 patients with epilepsy from the F-TRACT database, providing a total of 34 354 bipolar stimulations and 774 445 cortico-cortical evoked potentials. The cortical mapping of the local excitatory and inhibitory synaptic time constants and of the axonal conduction delays between cortical regions was obtained at the population level using anatomy-based averaging procedures, based on the Lausanne2008 and the HCP-MMP1 parcellation schemes, containing 130 and 360 parcels, respectively. To rule out brain maturation effects, a separate analysis was performed for older (>15 years) and younger patients (<15 years). In the group of older subjects, we found that the cortico-cortical axonal conduction delays between parcels were globally short (median = 10.2 ms) and only 16% were larger than 20 ms. This was associated to a median velocity of 3.9 m/s. Although a general lengthening of these delays with the distance between the stimulating and recording contacts was observed across the cortex, some regions were less affected by this rule, such as the insula for which almost all efferent and afferent connections were faster than 10 ms. Synaptic time constants were found to be shorter in the sensorimotor, medial occipital and latero-temporal regions, than in other cortical areas. Finally, we found that axonal conduction delays were significantly larger in the group of subjects younger than 15 years, which corroborates that brain maturation increases the speed of brain dynamics. To our knowledge, this study is the first to provide a local estimation of axonal conduction delays and synaptic time constants across the whole human cortex in vivo, based on intracerebral electrophysiological recordings
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