4,124 research outputs found

    Measurement of the topological surface state optical conductance in bulk-insulating Sn-doped Bi1.1_{1.1}Sb0.9_{0.9}Te2_2S single crystals

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    Topological surface states have been extensively observed via optics in thin films of topological insulators. However, in typical thick single crystals of these materials, bulk states are dominant and it is difficult for optics to verify the existence of topological surface states definitively. In this work, we studied the charge dynamics of the newly formulated bulk-insulating Sn-doped Bi1.1_{1.1}Sb0.9_{0.9}Te2_2S crystal by using time-domain terahertz spectroscopy. This compound shows much better insulating behavior than any other bulk-insulating topological insulators reported previously. The transmission can be enhanced an amount which is 5%\% of the zero-field transmission by applying magnetic field to 7 T, an effect which we believe is due to the suppression of topological surface states. This suppression is essentially independent of the thicknesses of the samples, showing the two-dimensional nature of the transport. The suppression of surface states in field allows us to use the crystal slab itself as a reference sample to extract the surface conductance, mobility, charge density and scattering rate. Our measurements set the stage for the investigation of phenomena out of the semi-classical regime, such as the topological magneto-electric effect.Comment: 5 pages, 3 figures, submitted in Augus

    Comment on ``Scientific collaboration networks. II. Shortest paths, weighted networks, and centrality"

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    In this comment, we investigate a common used algorithm proposed by Newman [M. E. J. Newman, Phys. Rev. E {\bf 64}, 016132(2001)] to calculate the betweenness centrality for all vertices. The inaccurateness of Newman's algorithm is pointed out and a corrected algorithm, also with O(MNMN) time complexity, is given. In addition, the comparison of calculating results for these two algorithm aiming the protein interaction network of Yeast is shown.Comment: 3 pages, 2 tables, and 2 figure

    The role of N(1535)N^*(1535) in ppppϕpp \to pp \phi and πpnϕ\pi^- p \to n \phi reactions

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    The near threshold ϕ\phi meson production in proton-proton and πp\pi^- p collisions is studied with the assumption that the production mechanism is due to the sub-NϕN\phi-threshold N(1535)N^*(1535) resonance. The π0\pi^0, η\eta and ρ0\rho^0-meson exchanges for proton-proton collisions are considered. It is shown that the contribution to the ppppϕpp \to pp \phi reaction from the t-channel π0\pi^0 meson exchange is dominant. With a significant N(1535)NϕN^*(1535)N\phi coupling (gN(1535)Nϕ2/4πg^2_{N^*(1535)N \phi}/4 \pi = 0.13), both ppppϕpp \to pp \phi and πpnϕ\pi^- p \to n \phi data are very well reproduced. The significant coupling of the N(1535)N^*(1535) resonance to NϕN \phi is compatible with previous indications of a large ssˉs \bar{s} component in the quark wave function of the N(1535)N^*(1535) resonance and may be the real origin of the significant enhancement of the ϕ\phi production over the naive OZI-rule predictions.Comment: 15 pages, 6 figure

    Spatial Distribution of Metal Emissions in SNR 3C 397 Viewed with Chandra and XMM

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    We present X-ray equivalent width imaging of the supernova remnant (SNR) 3C 397 for Mg He\alpha, Si He\alpha, S He\alpha, and Fe K\alpha complex lines with the Chandra and XMM-Newton observations. The images reveal that the heavier the element is, the smaller the extent of the element distribution is. The Mg emission is evidently enhanced in the southeastern blow-out region, well along the radio boundary there, and appears to partially envelope the eastern Fe knot. Two bilateral hat-like Si line-emitting structures are along the northern and southern borders, roughly symmetric with respect to the southeast-northwest elongation axis. An S line-emitting shell is located just inner to the northern radio and IR shell, indicating of a layer of reversely shocked sulphur in the ejecta. A few enhanced Fe features are basically aligned along the diagonal of the rectangular shape of the SNR, which implicates an early asymmetric SN explosion.Comment: 4 pages, 4 figures, appears in Science China Physics, Mechanics & Astronomy, 2010, 53 (Suppl.1), 267-27

    Effects of Wetness Duration and Grain Development Stages on Sorghum Grain Mold Infection

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    Grain mold caused by a complex of fungi is an economically important disease of sorghum worldwide. Little is known about the epidemiology of sorghum grain mold, which is essential for its management. Studies were conducted to quantify the effects of wetness duration on grain mold development under controlled conditions at ICRISAT. Six major sorghum grain mold fungi determined from previous field experiments,Curvularia lunata, Cladosporium oxysporum, Bipolaris australiensis, Fusarium moniliforme, F. pallidoroseum, and Phoma sorghina, were used. Panicles of a pot-grown mold-susceptible sorghum line, IS 10513, were spray inoculated with each fungus at five growth stages: flowering (F), milk (M), soft dough (S), hard dough (H), and physiological maturity (P), and were incubated in dew chambers for 0, 16, 24, 40, 48, and 72 h. Then, the plants were placed on greenhouse benches at 25 ± 1°C to allow grain mold infection to develop. Eight days after treatments, grains from F, M, and S stages were plated onto potato dextrose agar, while those from H and P stages were incubated in blotter paper humid chambers at 28 ± 1°C. Fungal colonization of grains were scored after 7 days. Results indicated a significant (P \u3c 0.01) correlation between wetness duration and grain mold development at different stages of inoculation. Generally, with increasing wetness duration, there was an increase in grain infection by all six fungi. However, infection frequency varied among fungi and grain development stages, indicating that individual fungi might have different windows for maximum infection during the grain development stages

    Topological regluing of rational functions

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    Regluing is a topological operation that helps to construct topological models for rational functions on the boundaries of certain hyperbolic components. It also has a holomorphic interpretation, with the flavor of infinite dimensional Thurston--Teichm\"uller theory. We will discuss a topological theory of regluing, and trace a direction in which a holomorphic theory can develop.Comment: 38 page

    Real Time Evaluation of Tissue Optical Properties during Thermal Ablation of \u3cem\u3eex vivo\u3c/em\u3e Liver Tissues

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    Complete ablation of liver tumors is vital for minimizing the risk of local tumor recurrence. Accurately identifying the hallmarks of tissue necrosis during thermal ablative therapies may significantly increase the efficacy of ablation, while minimizing unnecessary damage to the surrounding normal tissues or critical structures. Light propagation in biological tissues is sensitive to the tissue microstructure and chromophore concentrations. In our previous studies, we found that the wavelength (λ) averaged liver tissue absorption coefficient μa and reduced scattering coefficient μs’ change significantly upon heating which may be used for assessment of tissue damage during thermal ablation of solid tumors. Here, we seek to demonstrate the use of an integrated fiber-optic probe for continuous monitoring of the local tissue temperature (T), μa(λ) and μs’(λ) during thermal ablation of ex vivo porcine livers. The wavelength-averaged (435–630 nm) tissue absorption and scattering (μa and μs’) increased rapidly at 45 °C and plateaued at 67 °C. The mean μa and μs’ for liver tissue at 37 °C (n = 10) were 8.5 ± 3.7 and 2.8 ± 1.1 cm−1, respectively. The relative changes in μa and μs’ at 37, 55, and 65 °C were significantly different (p \u3c .02) from each other. A relationship between the relative changes in μa and μs’ and the degree of tissue damage estimated using the temperature-based Arrhenius model for porcine liver tissues was established and studied
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