166 research outputs found

    Quasiparticle contribution to heat carriers relaxation time in DyBa2_2Cu3_3O7−x_{7-x} from heat diffusivity measurements

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    It is shown that the controversy on phonons or electrons being the most influenced heat carriers below the critical temperature of high-Tc_c superconductors can be resolved. Electrical and thermal properties of the same DyBa2_2Cu3_3O7−x_{7-x} monodomain have been measured for two highly different oxygenation levels. While the oxygenated sample DyBa2_2Cu3_3O7_{7} has very good superconducting properties (Tc=90T_c=90 K), the DyBa2_2Cu3_3O6.3_{6.3} sample exhibits an insulator behavior. A careful comparison between measurements of the {\bf thermal diffusivity} of both samples allows us to extract the electronic contribution. This contribution to the relaxation time of heat carriers is shown to be large below TcT_c and more sensitive to the superconducting state than the phonon contribution.Comment: 13 pages, 6 figure

    Interface barriers at the interfaces of polar GaAs(111) faces with Al2O3

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    Internal photoemission measurements of barriers for electrons at interfaces between GaAs(111) and atomic-layer deposited Al2O3 indicate that changing the GaAs polar crystal face orientation from the Ga-terminated (111)A to the As-terminated (111)B has no effect on the barrier height and remains the same as at the non-polar GaAs(100)/Al2O3 interface. Moreover, the presence of native oxide on GaAs(111) or passivation of this surface with sulphur also have no measurable influence on the GaAs(111)/Al2O3 barrier. These results suggest that the orientation and composition-sensitive surface dipoles conventionally observed at GaAs surfaces are effectively compensated at GaAs/oxide interfaces. (C) 2012 American Institute of Physics. (http://dx.doi.org/10.1063/1.3698461

    Les facteurs prédictifs de morbimortalité chez les patients sous ballon de contre pulsion intra-aortique en chirurgie cardiaque

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    Le ballon de contre pulsion intra-aortique (BCPIA) est fréquemment utilisé en chirurgie cardiaque, comme moyen d'assistance circulatoire en cas de bas débit cardiaque. Il est d'intérêt clinique de déterminer les facteurs pronostiques chez les patients porteurs d'un BCPIA en chirurgie cardiaque, et qui restent un sujet rarement élucidé dans la littérature. L'objectif de notre travail est de déterminer les facteurs prédictifs de morbimortalitéchez les patients sous ballon de contre pulsion intraortique en périopératoire d'une chirurgie cardiaque. Il s'agit d'une étude rétrospective portant sur l'ensemble des patients opérés en chirurgie cardiaque sous circulation extracorporelle, et ayant bénéficiés de la mise en place d'un ballon de contre pulsion intra-aortique en périopératoire, au service de chirurgie cardiovasculaire de l'Hôpital Militaire Mohamed V de Rabat, entrele mois de janvier 2005 et le mois d'aout 20014. Soixante dix patients ont été inclus dans notre étude. En analyse univariée l'âge, la dyspnée de stade III et IV, l'insuffisance cardiaque, la présence d'un infarctus du myocarde, d'une coronaropathie mono et bitronculaire, les anomalies du doppler de trons supra-aortique et du membre inférieur, le caractère urgent de la chirurgie, la durée de la circulation extracorporelle, l'instabilité hémodynamique postopératoire, le saignement et l'insuffisance rénale postopératoire étaient statistiquement associés à une mortalité postopératoire élevée. La dyskinésie préopératoire et la sortie de circulation extracorporelle sous drogues étaient associées à une morbidité globale élevée. En analyse multi variée, seule l'âge, constituait un facteur de risque indépendant de mortalité dans notre série avec un Odds Ratio (OR): 1,89 ; un Intervalle de Confiance (IC) 95% de (1,52-4,97) et un p =0,045. Au terme de notre étude, le taux de mortalité était de 48,57% et de morbidité globale était de 87,1%. Il nous parait donc nécessaire pour diminuer l'incidence de cette morbimortalité dans notre population, d'agir sur les facteurs que nous jugeons modifiables tels l'amélioration de la fonction cardiaque préopératoire, l'optimisation de la fonction rénale, la réduction de la durée de CEC et le contrôle du saignement

    Estimation of the charge carrier localization length from Gaussian fluctuations in the magneto-thermopower of La_{0.6}Y_{0.1}Ca_{0.3}MnO_3

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    The magneto-thermoelectric power (TEP) ΔS(T,H)\Delta S(T,H) of perovskite type manganise oxide La0.6Y0.1Ca0.3MnO3La_{0.6}Y_{0.1}Ca_{0.3}MnO_3 is found to exhibit a sharp peak at some temperature T∗=170KT^{*}=170K. By approximating the true shape of the measured magneto-TEP in the vicinity of T∗T^{*} by a linear triangle of the form ΔS(T,H)≃Sp(H)±B±(H)(T∗−T)\Delta S(T,H)\simeq S_p(H)\pm B^{\pm}(H)(T^{*}-T), we observe that B−(H)≃2B+(H)B ^{-}(H)\simeq 2B ^{+}(H). We adopt the electron localization scenario and introduce a Ginzburg-Landau (GL) type theory which incorporates the two concurrent phase transitions, viz., the paramagnetic-ferromagnetic transition at the Curie point TCT_C and the "metal-insulator" (M-I) transition at TMIT_{MI}. The latter is characterized by the divergence of the field-dependent charge carrier localization length ξ(T,H)\xi (T,H) at some characteristic field H0H_0. Calculating the average and fluctuation contributions to the total magnetization and the transport entropy related magneto-TEP ΔS(T,H)\Delta S(T,H) within the GL theory, we obtain a simple relationship between T∗T^{*} and the above two critical temperatures (TCT_{C} and TMIT_{MI}). The observed slope ratio B−(H)/B+(H)B ^{-}(H)/B ^{+}(H) is found to be governed by the competition between the electron-spin exchange JSJS and the induced magnetic energy MsH0M_sH_0. The comparison of our data with the model predictions produce TC=195KT_{C}=195K, JS=40meVJS=40meV, M0=0.4MsM_0=0.4M_s, ξ0=10A˚\xi_0=10\AA, and ne/ni=2/3n_e/n_i=2/3 for the estimates of the Curie temperature, the exchange coupling constant, the critical magnetization, the localization length, and the free-to-localized carrier number density ratio, respectively.Comment: 6 pages (REVTEX), 2 PS figures (epsf.sty); submitted to Phys.Rev.

    Two band gap field-dependent thermal conductivity of MgB2MgB_2

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    The thermal conductivity κ(H,T)\kappa (H,T) of the new superconductor MgB2MgB_2 was studied as a function of the temperature and a magnetic field. No anomaly in the thermal conductivity κ(H,T)\kappa (H,T) is observed around the superconducting transition in absence or presence of magnetic fields up to 14 Tesla; upon that field the superconductivity of MgB2MgB_2 persisted. The thermal conductivity in zero-field shows a TT-linear increase up to 50K. The thermal conductivity is found to increase with increasing field at high fields. We interpret the findings as if there are two subsystems of quasiparticles with different field-dependent characters in a two (LL and SS)-band superconductor reacting differently with the vortex structure. The unusual enhancement of κ(H,T)\kappa (H ,T) at low temperature but higher than a (Hc2S≃3TH_{c2S}\simeq 3T) critical field is interpreted as a result of the overlap of the low energy states outside the vortex cores in the SS-band.Comment: 6 pages,3 figure

    Thermal conductivity in B- and C- phase of UPt_3

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    Although the superconductivity in UPt_3 is one of the most well studied, there are still lingering questions about the nodal directions in the B and C phase in the presence of a magnetic field. Limiting ourselves to the low temperature regime (T<<Delta(0)), we study the magnetothermal conductivity with in semiclassical approximation using Volovik's approach. The angular dependence of the magnetothermal conductivity for an arbitrary field direction should clarify the nodal structure in UPt_3.Comment: 4 pages, 5 figure

    Group-IV graphene- and graphane-like nanosheets

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    We performed a first principles investigation on the structural and electronic properties of group-IV (C, SiC, Si, Ge, and Sn) graphene-like sheets in flat and buckled configurations and the respective hydrogenated or fluorinated graphane-like ones. The analysis on the energetics, associated with the formation of those structures, showed that fluorinated graphane-like sheets are very stable, and should be easily synthesized in laboratory. We also studied the changes on the properties of the graphene-like sheets, as result of hydrogenation or fluorination. The interatomic distances in those graphane-like sheets are consistent with the respective crystalline ones, a property that may facilitate integration of those sheets within three-dimensional nanodevices
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