107 research outputs found

    Quantum point contact conductance in NINS junctions

    Full text link
    The effect of an insulating barrier located at a distance aa from a NS quantum point contact is analyzed in this work. The Bogoliubov de Gennes equations are solved for NINS junctions (S: anysotropic superconductor, I: insulator and N: normal metal), where the NIN region is a quantum wire. For a0% a\neq0, bound states and resonances in the differential conductance are predicted. These resonances depend on the symmetry of the pair potential, the strength of the insulating barrier and aa . Our results show that in a NINS quantum point contact the number of resonances vary with the symmetry of the order parameter. This is to be contrasted with the results for the NINS junction, in which only the position of the resonances changes with the symmetry.Comment: 5 pages, 5 Figures, RevTex

    Observation of Wigner cusps in a metallic carbon nanotube

    Full text link
    Previous gate-dependent conductance measurements of metallic carbon nanotubes have revealed unexplainable conductance suppressions, occurring at two different gate voltages. These were previously attributed to the gate-dependency of contact resistance. Our gate-dependent conductivity measurements on a metallic nanotube with known chirality show that these bimodal conductance suppressions are the manifestations of Wigner cusps, often seen in atomic and nuclear physics experiments.Comment: 6 pages, 3 figure

    Uncovering the dominant scatterer in graphene sheets on SiO2

    Get PDF
    We have measured the impact of atomic hydrogen adsorption on the electronic transport properties of graphene sheets as a function of hydrogen coverage and initial, pre-hydrogenation field-effect mobility. Our results are compatible with hydrogen adsorbates inducing intervalley mixing by exerting a short-range scattering potential. The saturation coverages for different devices are found to be proportional to their initial mobility, indicating that the number of native scatterers is proportional to the saturation coverage of hydrogen. By extrapolating this proportionality, we show that the field-effect mobility can reach 1.5 x 10(4) cm(2)/V s in the absence of the hydrogen-adsorbing sites. This affinity to hydrogen is the signature of the most dominant type of native scatterers in graphene-based field-effect transistors on SiO2

    A specific case in the classification of woods by FTIR and chemometric: discrimination of Fagales from Malpighiales

    Get PDF
    Fourier transform infrared (FTIR) spectroscopic data was used to classify wood samples from nine species within the Fagales and Malpighiales using a range of multivariate statistical methods. Taxonomic classification of the family Fagaceae and Betulaceae from Angiosperm Phylogenetic System Classification (APG II System) was successfully performed using supervised pattern recognition techniques. A methodology for wood sample discrimination was developed using both sapwood and heartwood samples. Ten and eight biomarkers emerged from the dataset to discriminate order and family, respectively. In the species studied FTIR in combination with multivariate analysis highlighted significant chemical differences in hemicelluloses, cellulose and guaiacyl (lignin) and shows promise as a suitable approach for wood sample classification

    Spin dependence in the pp-wave resonance of 139La+n{^{139}\vec{\rm{La}}+\vec{n}}

    Full text link
    We measured the spin dependence in a neutron-induced pp-wave resonance by using a polarized epithermal neutron beam and a polarized nuclear target. Our study focuses on the 0.75~eV pp-wave resonance state of 139^{139}La+nn, where largely enhanced parity violation has been observed. We determined the partial neutron width of the pp-wave resonance by measuring the spin dependence of the neutron absorption cross section between polarized 139La^{139}\rm{La} and polarized neutrons. Our findings serve as a foundation for the quantitative study of the enhancement effect of the discrete symmetry violations caused by mixing between partial amplitudes in the compound nuclei

    Non-strange Dibaryon Resonances Observed in the γdπ0π0d\gamma d\to \pi^0\pi^0 d Reaction

    Full text link
    Coherent double neutral-pion photoproduction on the deuteron, γd\gamma{d}{\to}π0π0d\pi^0\pi^0{d}, has been experimentally studied at incident photon energies ranging from 0.75 to 1.15 GeV. The total cross section as a function of the γd\gamma{d} center-of-mass energy shows resonance-like behavior, which peaks at approximately 2.47 and 2.63 GeV. The measured angular distribution of deuteron emission is rather flat, which cannot be reproduced by the kinematics of quasi-free π0π0\pi^0\pi^0 production with deuteron coalescence. In π0d\pi^0d invariant-mass distributions, a clear peak is observed at 2.14±0.012.14{\pm}0.01 GeV/c2/c^2 with a width of 0.09±0.010.09{\pm}0.01 GeV/c2/c^2. The spin-parity of this state is restricted to 1+1^+, 2+2^+ or 33^- from the angular distributions of the two π0\pi^0s. The present work shows strong evidence for the existence of an isovector dibaryon resonance with a mass of 2.14 GeV/c2/c^2. The 2+2^+ assignment is consistent with the theoretically predicted D12{\cal{D}}_{12} state, and also with the energy dependence of the πd\pi{d} partial-wave amplitude 3 ⁣P2^3\!P_2 for the π±d\pi^{\pm}d{\to}π±d\pi^{\pm}d and π+d\pi^+d{\to}pp{pp} reactions.Comment: 12 pages, 6 figure

    Effects of Layer Stacking on the Combination Raman modes in Graphene

    Full text link
    We have observed new combination modes in the range from 1650 - 2300 cm-1 in single-(SLG), bi-, few-layer and incommensurate bilayer graphene (IBLG) on silicon dioxide substrates. The M band at ~1750 cm-1 is suppressed for both SLG and IBLG. A peak at ~1860 cm-1 (iTALO-) is observed due to a combination of the iTA and LO phonons. The intensity of this peak decreases with increasing number of layers and this peak is absent in bulk graphite. Two previously unidentified modes at ~1880 cm-1 (iTALO+) and ~2220 cm-1 (iTOTA) in SLG are tentatively assigned as combination modes around the K point of the graphene Brillouin zone. The peak frequencies of the iTALO+ (iTOTA) modes are observed to increase (decrease) linearly with increasing graphene layers.Comment: 11 Pages, 4 Figure
    corecore