14,978 research outputs found

    Exchange Field-Mediated Magnetoresistance in the Correlated Insulator Phase of Be Films

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    We present a study of the proximity effect between a ferromagnet and a paramagnetic metal of varying disorder. Thin beryllium films are deposited onto a 5 nm-thick layer of the ferromagnetic insulator EuS. This bilayer arrangement induces an exchange field, HexH_{ex}, of a few tesla in low resistance Be films with sheet resistance R≪RQR\ll R_Q, where RQ=h/e2R_Q=h/e^2 is the quantum resistance. We show that HexH_{ex} survives in very high resistance films and, in fact, appears to be relatively insensitive to the Be disorder. We exploit this fact to produce a giant low-field magnetoresistance in the correlated insulator phase of Be films with R≫RQR\gg R_Q.Comment: To be published in Physical Review Letter

    Structural and Physical Properties of CaFe4As3 Single Crystals

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    We report the synthesis, and structural and physical properties of CaFe4As3 single crystals. Needle-like single crystals of CaFe4As3 were grown out of Sn flux and the compound adopts an orthorhombic structure as determined by X-ray diffraction measurements. Electrical, magnetic, and thermal properties indicate that the system undergoes two successive phase transitions occurring at TN1 ~ 90 K and TN2 ~ 26 K. At TN1, electrical resistivities (\rho(b) and \rho(ac)) are enhanced while magnetic susceptibilities (\chi(b) and \chi(ac)) are reduced in both directions parallel and perpendicular to the b-axis, consistent with the scenario of antiferromagnetic spin-density-wave formation. At TN2, specific heat reveals a slope change, and \chi(ac) decreases sharply but \chi(b) has a clear jump before it decreases again with decreasing temperature. Remarkably, both \rho(b) and \rho(ac) decrease sharply with thermal hysteresis, indicating the first-order nature of the phase transition at TN2. At low temperatures, \rho(b) and \rho(ac) can be described by {\rho} = {\rho}0 + AT^\alpha ({\rho}0, A, and {\alpha} are constants). Interestingly, these constants vary with applied magnetic field. The ground state of CaFe4As3 is discussed.Comment: 15 pages, 8 figures, Submitted to Physical Review

    Robust Subjective Visual Property Prediction from Crowdsourced Pairwise Labels.

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    The problem of estimating subjective visual properties from image and video has attracted increasing interest. A subjective visual property is useful either on its own (e.g. image and video interestingness) or as an intermediate representation for visual recognition (e.g. a relative attribute). Due to its ambiguous nature, annotating the value of a subjective visual property for learning a prediction model is challenging. To make the annotation more reliable, recent studies employ crowdsourcing tools to collect pairwise comparison labels because human annotators are much better at ranking two images/videos (e.g. which one is more interesting) than giving an absolute value to each of them separately. However, using crowdsourced data also introduces outliers. Existing methods rely on majority voting to prune the annotation outliers/errors. They thus require large amount of pairwise labels to be collected. More importantly as a local outlier detection method, majority voting is ineffective in identifying outliers that can cause global ranking inconsistencies. In this paper, we propose a more principled way to identify annotation outliers by formulating the subjective visual property prediction task as a unified robust learning to rank problem, tackling both the outlier detection and learning to rank jointly. Differing from existing methods, the proposed method integrates local pairwise comparison labels together to minimise a cost that corresponds to global inconsistency of ranking order. This not only leads to better detection of annotation outliers but also enables learning with extremely sparse annotations. Extensive experiments on various benchmark datasets demonstrate that our new approach significantly outperforms state-of-the-arts alternatives.Comment: 14 pages, accepted by IEEE TPAM

    Comment on "Isoelectronic Ru substitution at Fe-site in Sm(Fe1−x_{1-x}Rux_x)AsO0.85_{0.85}F0.15_{0.15} compound and its effects on structural, superconducting and normal state properties" (arXiv:1004.1978)

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    Based on the five-orbital model, we derive the reduced impurity scattering rate g=zγ/2πTc0g=z\gamma/2\pi T_{c0} in Sm(Fe1−x_{1-x}Rux_{x})AsO0.85_{0.85}F0.15_{0.15} from the residual resistivity. At x=0x=0, the transition temperature is Tc0=50T_{c0}=50 K. For 0.05Tc/Tc0>0.30.05T_{c}/T_{c0}>0.3) the obtained value of gg ranges from 1.5 to 2.9, which suggests that the s±s_\pm-wave state cannot survive. We point out that the magnetoresistance frequently gives an underestimated value of gg in correlated electron systems.Comment: 2 page

    Effect of synthesized temperature on the assembly and properties of four lanthanide supramolecular frameworks

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    Four new lanthanide coordination polymers, [H3O][Ln3(HPA)10(H2O)3·2H2O] (Ln = Pr for 1, Ln = Nd for 2), [Ln2(HPA)6(H2O)4·2H2O] (Ln = Sm for 3, Ln = Tb for 4) (HHPA =3-(4-hydroxyphenyl)propanoic acid), were successfully synthesized and characterized. 1 and 2 are isostructural and have 1D metal chain structure, while 3 and 4 show 0D network with binuclear subunits. The results indicated that the effect of reaction temperature can modulate the final structures. The HPA ligands adopt bidentate chelating and tridentate chelating bridging modes to coordinate with Ln(III) ions in 1-4. It has been shown that 4 can act as a fluorescent sensor for highly sensitive detection of nitroaromatics and Fe3+.               KEY WORDS: Sensor, Lanthanide, Structure, Temperature Bull. Chem. Soc. Ethiop. 2019, 33(1), 113-125DOI: https://dx.doi.org/10.4314/bcse.v33i1.1

    Magnetic and Transport Properties in CoSr2Y1−xCaxCu2O7CoSr_2Y_{1-x}Ca_xCu_2O_7 (xx=0∼\sim0.4)

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    Magnetic and transport properties of CoSr2Y1−xCaxCu2O7Co Sr_2 Y_{1-x} Ca_x Cu_2 O_7 (x=0∼0.4x=0 \sim 0.4) system have been investigated. A broad maximum in M(T) curve, indicative of low-dimensional antiferromagnetic ordering originated from CoO1+δCoO_{1+\delta} layers, is observed in Ca-free sample. With increasing Ca doping level up to 0.2, the M(T) curve remains almost unchanged, while resistivity is reduced by three orders. Higher Ca doping level leads to a drastic change of magnetic properties. In comparison with the samples with x=0.0∼0.2x=0.0 \sim 0.2, the temperature corresponding to the maximum of M(T) is much lowered for the sample xx=0.3. The sample xx=0.4 shows a small kink instead of a broad maximum and a weak ferromagnetic feature. The electrical transport behavior is found to be closely related to magnetic properties for the sample xx=0.2, 0.25, 0.3, 0.4. It suggests that CoO1+δCoO_{1+\delta} layers are involved in charge transport in addition to conducting CuO2CuO_2 planes to interpret the correlation between magnetism and charge transport. X-ray photoelectron spectroscopy studies give an additional evidence of the the transfer of the holes into the CoO1+δCoO_{1+\delta} charge reservoir
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