5,048 research outputs found

    Metal-to-semiconductor transition in squashed armchair carbon nanotubes

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    Journal ArticleWe investigate electronic transport properties of the squashed armchair carbon nanotubes, using tight-binding molecular dynamics and the Green's function method. We demonstrate a metal-to-semiconductor transition while squashing the nanotubes and a general mechanism for such a transition. It is the distinction of the two sublattices in the nanotube that opens an energy gap near the Fermi energy. We show that the transition has to be achieved by a combined effect of breaking of mirror symmetry and bond formation between the flattened faces in the squashed nanotubes

    Reducing the Tension Between the BICEP2 and the Planck Measurements: A Complete Exploration of the Parameter Space

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    A large inflationary tensor-to-scalar ratio r0.002=0.200.05+0.07r_\mathrm{0.002} = 0.20^{+0.07}_{-0.05} is reported by the BICEP2 team based on their B-mode polarization detection, which is outside of the 95%95\% confidence level of the Planck best fit model. We explore several possible ways to reduce the tension between the two by considering a model in which αs\alpha_\mathrm{s}, ntn_\mathrm{t}, nsn_\mathrm{s} and the neutrino parameters NeffN_\mathrm{eff} and Σmν\Sigma m_\mathrm{\nu} are set as free parameters. Using the Markov Chain Monte Carlo (MCMC) technique to survey the complete parameter space with and without the BICEP2 data, we find that the resulting constraints on r0.002r_\mathrm{0.002} are consistent with each other and the apparent tension seems to be relaxed. Further detailed investigations on those fittings suggest that NeffN_\mathrm{eff} probably plays the most important role in reducing the tension. We also find that the results obtained from fitting without adopting the consistency relation do not deviate much from the consistency relation. With available Planck, WMAP, BICEP2 and BAO datasets all together, we obtain r0.002=0.140.11+0.05r_{0.002} = 0.14_{-0.11}^{+0.05}, nt=0.350.47+0.28n_\mathrm{t} = 0.35_{-0.47}^{+0.28}, ns=0.980.02+0.02n_\mathrm{s}=0.98_{-0.02}^{+0.02}, and αs=0.00860.0189+0.0148\alpha_\mathrm{s}=-0.0086_{-0.0189}^{+0.0148}; if the consistency relation is adopted, we get r0.002=0.220.06+0.05r_{0.002} = 0.22_{-0.06}^{+0.05}.Comment: 8 pages, 4 figures, submitted to PL

    An optical fiber tip micrograting thermometer

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    An ~12 µm long Bragg grating was engraved in an ~5 µm diameter optical fiber tip by focused ion beam (FIB) milling. An ~10-dB extinction was achieved at 1570 nm with only 11 indentations. The grating was used for temperature sensing, and it exhibited a temperature sensitivity of ~22 pm/°C

    3-Nitro-5-(4-pyridinio)benzoate

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    The title compound, C12H8N2O4, crystallizes as a zwitterion in which the pyridyl N atom is protonated. The dihedral angle between the benzene and pyridinium rings is 27.9 (2)°. In the crystal, N—H⋯O hydrogen bonds link adjacent zwitterions into a three-dimensional structure
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