553 research outputs found

    Intrinsic Josephson Effects in the Magnetic Superconductor RuSr2GdCu2O8

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    We have measured interlayer current transport in small sized RuSr2GdCu2O8 single crystals. We find a clear intrinsic Josephson effect showing that the material acts as a natural superconductor-insulator-ferromagnet-insulator-superconductor superlattice. So far, we detected no unconventional behavior due to the magnetism of the RuO2 layers.Comment: 4 pages, 5 figures, to appear in Phys. Rev. Let

    Quantum Quasi-Monte Carlo algorithm for out-of-equilibrium Green functions at long times

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    We extend the recently developed Quantum Quasi-Monte Carlo (QQMC) approach to obtain the full frequency dependence of Green functions in a single calculation. QQMC is a general approach for calculating high-order perturbative expansions in power of the electron-electron interaction strength. In contrast to conventional Markov chain Monte Carlo sampling, QQMC uses low-discrepancy sequences for a more uniform sampling of the multi-dimensional integrals involved and can potentially outperform Monte Carlo by several orders of magnitudes. A core concept of QQMC is the a priori construction of a "model function" that approximates the integrand and is used to optimize the sampling distribution. In this paper, we show that the model function concept extends to a kernel approach for the computation of Green functions. We illustrate the approach on the Anderson impurity model and show that the scaling of the error with the number of integrand evaluations NN is 1/N0.86\sim 1/N^{0.86} in the best cases, and comparable to Monte Carlo scaling 1/N0.5\sim 1/N^{0.5} in the worst cases. We find a systematic improvement over Monte Carlo sampling by at least two orders of magnitude while using a basic form of model function. Finally, we compare QQMC results with calculations performed with the Fork Tensor Product State (FTPS) method, a recently developed tensor network approach for solving impurity problems. Applying a simple Pad\'e approximant for the series resummation, we find that QQMC matches the FTPS results beyond the perturbative regime.Comment: 18 pages, 11 figure

    Direct determination of spin orbit interaction coefficients and realization of the persistent spin helix symmetry

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    The spin orbit interaction plays a crucial role in diverse fields of condensed matter, including the investigation of Majorana fermions, topological insulators, quantum information and spintronics. In III V zinc blende semiconductor heterostructures, two types of spin orbit interaction, Rashba and Dresselhaus act on the electron spin as effective magnetic fields with different directions. They are characterized by coefficients alpha and beta, respectively. When alpha is equal to beta, the so called persistent spin helix symmetry is realized. In this condition, invariance with respect to spin rotations is achieved even in the presence of the spin orbit interaction, implying strongly enhanced spin lifetimes for spatially periodic spin modes. Existing methods to evaluate alpha/beta require fitting analyses that often include ambiguity in the parameters used. Here, we experimentally demonstrate a simple and fitting parameter free technique to determine alpha/beta and to deduce the absolute values of alpha and beta. The method is based on the detection of the effective magnetic field direction and the strength induced by the two spin orbit interactions. Moreover, we observe the persistent spin helix symmetry by gate tuning.Comment: 34 pages with 7 figures including supplementary information. appears in Nature Nanotechnology (2014) Published online 13 July 201

    Out-of-Plane Magnetic Anisotropy in Ordered Ensembles of Fey_yN Nanocrystals Embedded in GaN

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    Phase-separated semiconductors containing magnetic nanostructures are relevant systems for the realization of high-density recording media. Here, the controlled strain engineering of Gaδ\deltaFeN layers with Fey_yN embedded nanocrystals (NCs) \textit{via} Alx_xGa1x_{1-x}N buffers with different Al concentration 0<xAl<410<x_\mathrm{Al}<41\% is presented. Through the addition of Al to the buffer, the formation of predominantly prolate-shaped ε\varepsilon-Fe3_3N NCs takes place. Already at an Al concentration xAlx_\mathrm{Al}\,\approx\,5\% the structural properties---phase, shape, orientation---as well as the spatial distribution of the embedded NCs are modified in comparison to those grown on a GaN buffer. Although the magnetic easy axis of the cubic γ\gamma'-Gay_yFe4y_{4-y}N nanocrystals in the layer on the xAl=0%x_\mathrm{Al} = 0\% buffer lies in-plane, the easy axis of the ε\varepsilon-Fe3_3N NCs in all samples with Alx_xGa1x_{1-x}N buffers coincides with the [0001][0001] growth direction, leading to a sizeable out-of-plane magnetic anisotropy and opening wide perspectives for perpendicular recording based on nitride-based magnetic nanocrystals.Comment: 29 pages, 10 figures, submitte

    Superconducting properties of RuSr2GdCu2O8 studied by SQUID magnetometry

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    For polycrystalline RuSr2GdCu2O8 (Ru-1212), distinct peaks have been reported in d.c. magnetization in the superconducting state of the sample. Sr2GdRuO6 (Sr-2116), the precursor for the preparation of Ru-1212, shows similar peaks in the same temperature regime. Based on measurements performed on both bulk and powdered samples of Ru-1212 and Sr-2116, we exclude the possibility, that the observed behavior of the magnetization of Ru-1212 is due to Sr-2116 impurities. The effect is related to the superconductivity of Ru-1212, but it is not an intrinsic property of this compound. We provide evidence that the observation of magnetization peaks in the superconducting state of Ru-1212 is due to flux motion generated by the movement of the sample in an inhomogeneous field, during the measurement in the SQUID magnetometer. We propose several tests, that help to decide, whether the features observed in a SQUID magnetization measurement of Ru-1212 represent a property of the compound or not.Comment: 22 pages, 9 figure

    Safety and Efficacy of Dronedarone in the Treatment of Atrial Fibrillation/Flutter

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    Dronedarone is an amiodarone analog but differs structurally from amiodarone in that the iodine moiety was removed and a methane-sulfonyl group was added. These modifications reduced thyroid and other end-organ adverse effects and makes dronedarone less lipophilic, shortening its half-life. Dronedarone has been shown to prevent atrial fibrillation/flutter (AF/AFl) recurrences in several multi-center trials. In addition to its rhythm control properties, dronedarone has rate control properties and slows the ventricular response during AF. Dronedarone is approved in Europe for rhythm and rate control indications. In patients with decompensated heart failure, dronedarone treatment increased mortality and cardiovascular hospitalizations. However, when dronedarone was used in elderly high risk AF/AFl patients excluding such high risk heart failure, cardiovascular hospitalizations were significantly reduced and the drug was approved in the USA for this indication in 2009 by the Food and Drug Administration. Updated guidelines suggest dronedarone as a front-line antiarrhythmic in many patients with AF/Fl but caution that the drug should not be used in patients with advanced heart failure. In addition, the recent results of the PALLAS trial suggest that dronedarone should not be used in the long-term treatment of patients with permanent AF

    Josephson Plasma in RuSr2GdCu2O8

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    Josephson plasma in RuSr2_{2}GdCu2_{2}O8_{8}, Ru1x_{1-x}Sr2_{2}GdCu2+x_{2+x}O8_{8} (x = 0.3), and RuSr2_{2}Eu2x_{2-x}Cex_{x}Cu2_{2}O10_{10} (x = 0.5) compounds is investigated by the sphere resonance method. The Josephson plasma is observed in a low-frequency region (around 8.5 cm1^{-1} at T \ll TcT_{c}) for ferromagnetic RuSr2_{2}GdCu2_{2}O8_{8}, while it increases to 35 cm1^{-1} for non-ferromagnetic Ru1x_{1-x}Sr2_{2}GdCu2+x_{2+x}O8_{8} (x = 0.3), which represents a large reduction in the Josephson coupling at ferromagnetic RuO2_{2} block layers. The temperature dependence of the plasma does not shift to zero frequency ({\it i.e.} jcj_{c} = 0) at low temperatures, indicating that there is no transition from the 0-phase to the π\pi-phase in these compounds. The temperature dependence and the oscillator strength of the peak are different from those of other non-magnetic cuprates, and the origins of these anomalies are discussed.Comment: to appear in Phys. Rev.B Rapid Com

    Study of the crystal structure, superconducting and magnetic properties of Ru1-xFexSr2GdCu2O8

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    Samples of the Ru1-xFexSr2GdCu2O8 system with x = 0, 0.025, 0.05, 0.075, 0.1 and 0.2, were prepared and their structural, superconducting and magnetic properties were studied. Rietveld refinement of the X-ray diffraction patterns show that the Fe substitution occurs in both Ru and Cu sites. An increase of Fe concentration produces no significant changes in the bond angle Ru-O(3)-Ru, which is a measure of the rotation of the RuO6 octahedra around the c-axis, and also in the bond angle Ru-O(1)-Cu, which is a measure of the canting of the RuO6 octahedra. On the other hand, the bond angle Cu-O(2)-Cu, which is a measure of the buckling of the CuO2 layer, has a slight tendency to decrease with the increase of the Fe content. We found thet both ferromagnetic and superconducting transition temperatures are reduced with the increase of Fe concentration. Analisys related to the decay of the superconducting and ferromagnetic states is presented.Comment: 9 pages, 7 figure

    Mapping competencies taught in public health – Experience of the Europubhealth Consortium

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    International audienceBackground Public health education aims at producing a competent workforce. The WHO-ASPHER framework proposes a set of relevant public health competencies organised in 10 sections (e.g. science practice, leadership, law policies and ethics etc). As part of the Europubhealth consortium (EPHc), eight universities collaborate for the delivery of a 2-year international public health master course. The course includes a first-year, or foundation component (4 options), and a second-year or specialisation component (7 options). Objectives In 2020, EPHc decided to use the framework in order to map the competencies addressed, and the level of proficiency aimed at, by each Y1 and Y2 option of the Master. To that end, component&amp;#039;s coordinators answered an 84-item questionnaire covering the whole framework. Answers were summarised by calculating mean proficiency levels for each competency section. Results There were differences in overall proficiency levels between years with, as expected, higher scores in Y2. Options in Y1 reached medium to high proficiency scores for the sections “science practice”, “health promotion” and “communication” with scores of 2.6 to 3 (on a 1 to 4 scale). When compared with Y1 on a heat-map, Y2 options displayed more contrasted profiles, typically focussing (i.e. scores &amp;amp;amp;gt; 3.5) on 3 out of the 10 sections of competencies. Except for the “collaborations and partnership” section, the training pathways offered by the EPHc seem to offer opportunities for a high proficiency level in all domains of competencies. Conclusions The mapping proved a useful exercise to identify strengths and complementarities among the EPHc. The results suggest that the EPHc master course is coherent and offers students opportunities to gain proficiency in most competencies relevant to public health practice. Key messages • Competency-based education is likely to shape the future public health workforce. • The WHO-ASPHER framework proved a useful tool to map public health competencies addressed in the teaching of the Europubhealth international Master
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