835 research outputs found

    The hole Fermi surface in Bi2_{2}Se3_{3} probed by quantum oscillations

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    Transport and torque magnetometry measurements are performed at high magnetic fields and low temperatures in a series of p-type (Ca-doped) Bi2_{2}Se3_{3} crystals. The angular dependence of the Shubnikov-de Haas and de Haas-van Alphen quantum oscillations enables us to determine the Fermi surface of the bulk valence band states as a function of the carrier density. At low density, the angular dependence exhibits a downturn in the oscillations frequency between 0∘0^\circ and 90∘90^\circ, reflecting a bag-shaped hole Fermi surface. The detection of a single frequency for all tilt angles rules out the existence of a Fermi surface with different extremal cross-sections down to 2424~meV. There is therefore no signature of a camel-back in the valence band of our bulk samples, in accordance with the direct band gap predicted by GWGW calculations.Comment: A supplemental material file giving a more detailed description of our work is available upon reques

    Spin dynamics and magnetic interactions of Mn dopants in the topological insulator Bi2_2Te3_3

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    The magnetic and electronic properties of the magnetically doped topological insulator Bi2−x_{\rm 2-x}Mnx_{\rm x}Te3_3 were studied using electron spin resonance (ESR) and measurements of static magnetization and electrical transport. The investigated high quality single crystals of Bi2−x_{\rm 2-x}Mnx_{\rm x}Te3_3 show a ferromagnetic phase transition for x≥0.04x\geq 0.04 at TC≈12T_{C}\approx 12 K. The Hall measurements reveal a p-type finite charge-carrier density. Measurements of the temperature dependence of the ESR signal of Mn dopants for different orientations of the external magnetic field give evidence that the localized Mn moments interact with the mobile charge carriers leading to a Ruderman-Kittel-Kasuya-Yosida-type ferromagnetic coupling between the Mn spins of order 2-3 meV. Furthermore, ESR reveals a low-dimensional character of magnetic correlations that persist far above the ferromagnetic ordering temperature

    Quantum Oscillations in Cux_xBi2_2Se3_3 in High Magnetic Fields

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    Cux_xBi2_2Se3_3 has drawn much attention as the leading candidate to be the first topological superconductor and the realization of coveted Majorana particles in a condensed matter system. However, there has been increasing controversy about the nature of its superconducting phase. This study sheds light on present ambiguity in the normal state electronic state, by providing a complete look at the quantum oscillations in magnetization in Cux_xBi2_2Se3_3 at intense high fields up to 31T. Our study focuses on the angular dependence of the quantum oscillation pattern in a low carrier concentration. As magnetic field tilts from along the crystalline c-axis to ab-plane, the change of the oscillation period follows the prediction of the ellipsoidal Fermi surface. As the doping level changes, the 3D Fermi surface is found to transform into quasi-cylindrical at high carrier density. Such a transition is potentially a Lifshitz transition of the electronic state in Cux_xBi2_2Se3_3.Comment: 6 pages, 6 figures, submitted to Phys. Rev.

    Oral cancer secretome: Identification of cancer-associated proteins

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    This study aims to identify cancer-associated proteins in the secretome of oral cancer cell lines. We have successfully established four primary cell cultures of normal cells with a limited lifespan without human telomerase reverse transcriptase (hTERT) immortalization. The secretome of these primary cell cultures were compared with that of oral cancer cell lines using 2DE. Thirty five protein spots were found to have changed in abundance. Unambiguous identification of these proteins was achieved by MALDI TOF/TOF. In silico analysis predicted that 24 of these proteins were secreted via classical or nonclassical mechanisms. The mRNA expression of six genes was found to correlate with the corresponding protein abundance. Ingenuity Pathway Analysis (IPA) core analysis revealed that the identified proteins were relevant in, and related to, cancer development with likely involvements in tumor growth, metastasis, hyperproliferation, tumorigenesis, neoplasia, hyperplasia, and cell transformation. In conclusion, we have demonstrated that a comparative study of the secretome of cancer versus normal cell lines can be used to identify cancer-associated proteins.Article Link: http://onlinelibrary.wiley.com/doi/10.1002/elps.201300126/abstrac

    HeMIS: Hetero-Modal Image Segmentation

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    We introduce a deep learning image segmentation framework that is extremely robust to missing imaging modalities. Instead of attempting to impute or synthesize missing data, the proposed approach learns, for each modality, an embedding of the input image into a single latent vector space for which arithmetic operations (such as taking the mean) are well defined. Points in that space, which are averaged over modalities available at inference time, can then be further processed to yield the desired segmentation. As such, any combinatorial subset of available modalities can be provided as input, without having to learn a combinatorial number of imputation models. Evaluated on two neurological MRI datasets (brain tumors and MS lesions), the approach yields state-of-the-art segmentation results when provided with all modalities; moreover, its performance degrades remarkably gracefully when modalities are removed, significantly more so than alternative mean-filling or other synthesis approaches.Comment: Accepted as an oral presentation at MICCAI 201

    Granular circulation in a cylindrical pan: simulations of reversing radial and tangential flows

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    Granular flows due to simultaneous vertical and horizontal excitations of a flat-bottomed cylindrical pan are investigated using event-driven molecular dynamics simulations. In agreement with recent experimental results, we observe a transition from a solid-like state, to a fluidized state in which circulatory flow occurs simultaneously in the radial and tangential directions. By going beyond the range of conditions explored experimentally, we find that each of these circulations reverse their direction as a function of the control parameters of the motion. We numerically evaluate the dynamical phase diagram for this system and show, using a simple model, that the solid-fluid transition can be understood in terms of a critical value of the radial acceleration of the pan bottom; and that the circulation reversals are controlled by the phase shift relating the horizontal and vertical components of the vibrations. We also discuss the crucial role played by the geometry of the boundary conditions, and point out a relationship of the circulation observed here and the flows generated in vibratory conveyors.Comment: 10 pages, 8 figure

    Intrinsic electronic superconducting phases at 60 K and 90 K in double-layer YBa2_2Cu3_3O6+δ_{6+\delta}

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    We study superconducting transition temperature (TcT_c) of oxygen-doped double-layer high-temperature superconductors YBa2_2Cu3_3O6+δ_{6+\delta} (0 ≤\le δ\delta ≤\le 1) as a function of the oxygen dopant concentration (δ\delta) and planar hole-doping concentration (PplP_{pl}). We find that TcT_c, while clearly influenced by the development of the chain ordering as seen in the TcT_c vs.vs. δ\delta plot, lies on a universal curve originating at the critical hole concentration (PcP_c) = 1/16 in the TcT_c vs.vs. PplP_{pl} plot. Our analysis suggests that the universal behavior of TcT_c(PplP_{pl}) can be understood in terms of the competition and collaboration of chemical-phases and electronic-phases that exist in the system. We conclude that the global superconductivity behavior of YBa2_2Cu3_3O6+δ_{6+\delta} as a function of doping is electronically driven and dictated by pristine electronic phases at magic doping numbers that follow the hierarchical order based on PcP_c, such as 2 ×\times PcP_c, 3 ×\times PcP_c and 4 ×\times PcP_c. We find that there are at least two intrinsic electronic superconducting phases of TcT_c = 60 K at 2 ×\times PcP_c = 1/8 and TcT_c = 90 K at 3 ×\times PcP_c = 3/16.Comment: 4 pages, 2 figure

    Determination of the Energy Band Gap of Bi₂Se₃

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    Despite intensive investigations of Bi2Se3 in past few years, the size and nature of the bulk energy band gap of this well-known 3D topological insulator still remain unclear. Here we report on a combined magneto-transport, photoluminescence and infrared transmission study of Bi2Se3, which unambiguously shows that the energy band gap of this material is direct and reaches Eg = (220 ± 5) meV at low temperatures
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