66,985 research outputs found

    Stray field and superconducting surface spin valve effect in La0.7_{0.7}Ca0.3_{0.3}MnO3_3/YBa2_2Cu3_3O7−δ_{7-\delta} bilayers

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    Electronic transport and magnetization measurements were performed on La0.7_{0.7}Ca0.3_{0.3}MnO3_3/YBa2_2Cu3_3O7−δ_{7-\delta} (LCMO/YBCO) bilayers below the superconducting transition temperature in order to study the interaction between magnetism and superconductivity. This study shows that a substantial number of weakly pinned vortices are induced in the YBCO layer by the large out-of-plane stray field in the domain walls. Their motion gives rise to large dissipation peaks at the coercive field. The angular dependent magnetoresistance (MR) data reveal the interaction between the stripe domain structure present in the LCMO layer and the vortices and anti-vortices induced in the YBCO layer by the out-of-plane stray field. In addition, this study shows that a superconducting surface spin valve effect is present in these bilayers as a result of the relative orientation between the magnetization at the LCMO/YBCO interface and the magnetization in the interior of the LCMO layer that can be tuned by the rotation of a small HH. This latter finding will facilitate the development of superconductive magnetoresistive memory devices. These low-magnetic field MR data, furthermore, suggest that triplet superconductivity is induced in the LCMO layer, which is consistent with recent reports of triplet superconductivity in LCMO/YBCO/LCMO trilayers and LCMO/YBCO bilayers.Comment: 14 pages, 3 figure

    J/ψ(ηc)NJ/\psi (\eta_c) N and Υ(ηb)N\Upsilon (\eta_b) N cross sections

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    Inspired by the recent findings of the two Pc+P_c^+ states in the J/ψpJ/\psi p mass spectrum at LHCb, we investigate the elastic and inelastic cross sections of the J/ψNJ/\psi N, ηcN\eta_c N, ΥN\Upsilon N and ηbN\eta_b N channels within the constraints from heavy quark spin and flavour symmetry. The Dˉ(∗)Σc(∗)\bar{D}^{(*)} \Sigma_c^{(*)} (B(∗)Σb(∗)B^{(*)} \Sigma_b^{(*)}) bound states predicted in earlier works should be accessible in elastic and/or inelastic processes of the J/ψNJ/\psi N and/or ηcN\eta_c N (ΥN\Upsilon N and/or ηbN\eta_b N) interactions.Comment: Minor correction

    Heavy quark spin symmetric molecular states from Dˉ(∗)Σc(∗){\bar D}^{(*)}\Sigma_c^{(*)} and other coupled channels in the light of the recent LHCb pentaquarks

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    We consider the Dˉ(∗)Σc(∗){\bar D}^{(*)}\Sigma_c^{(*)} states, together with J/ψNJ/\psi N and other coupled channels, and take an interaction consistent with heavy quark spin symmetry, with the dynamical input obtained from an extension of the local hidden gauge approach. By fitting only one parameter to the recent three pentaquark states reported by the LHCb collaboration, we can reproduce the three of them in base to the mass and the width, providing for them the quantum numbers and approximate molecular structure as 1/2−1/2^- DˉΣc\bar{D} \Sigma_c, 1/2−1/2^- Dˉ∗Σc\bar{D}^* \Sigma_c, and 3/2−3/2^- Dˉ∗Σc\bar{D}^* \Sigma_c, and isospin I=1/2I=1/2. We find another state around 4374 MeV, of 3/2−3/2^- DˉΣc∗\bar{D} \Sigma_c^* structure, for which indications appear in the experimental spectrum. Two other near degenerate states of 1/2−1/2^- Dˉ∗Σc∗\bar{D}^* \Sigma_c^* and 3/2−3/2^- Dˉ∗Σc∗\bar{D}^* \Sigma_c^* nature are also found around 4520 MeV, which although less clear, are not incompatible with the observed spectrum. In addition, a 5/2−5/2^- Dˉ∗Σc∗\bar D^* \Sigma_c^* state at the same energy appears, which however does not couple to J/ψpJ/\psi p in S−S-wave, and hence it is not expected to show up in the LHCb experiment.Comment: 8 page

    Preface: Impacts of extreme climate events and disturbances on carbon dynamics

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    The impacts of extreme climate events and disturbances (ECE&D) on the carbon cycle have received growing attention in recent years. This special issue showcases a collection of recent advances in understanding the impacts of ECE&D on carbon cycling. Notable advances include quantifying how harvesting activities impact forest structure, carbon pool dynamics, and recovery processes; observed drastic increases of the concentrations of dissolved organic carbon and dissolved methane in thermokarst lakes in western Siberia during a summer warming event; disentangling the roles of herbivores and fire on forest carbon dioxide flux; direct and indirect impacts of fire on the global carbon balance; and improved atmospheric inversion of regional carbon sources and sinks by incorporating disturbances. Combined, studies herein indicate several major research needs. First, disturbances and extreme events can interact with one another, and it is important to understand their overall impacts and also disentangle their effects on the carbon cycle. Second, current ecosystem models are not skillful enough to correctly simulate the underlying processes and impacts of ECE&D (e.g., tree mortality and carbon consequences). Third, benchmark data characterizing the timing, location, type, and magnitude of disturbances must be systematically created to improve our ability to quantify carbon dynamics over large areas. Finally, improving the representation of ECE&D in regional climate/earth system models and accounting for the resulting feedbacks to climate are essential for understanding the interactions between climate and ecosystem dynamics
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