30,934 research outputs found

    Anisotropic superconducting properties of aligned Sm0.95_{0.95}La0.05_{0.05}FeAsO0.85_{0.85}F0.15_{0.15} microcrystalline powder

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    The Sm0.95_{0.95}La0.05_{0.05}FeAsO0.85_{0.85}F0.15_{0.15} compound is a quasi-2D layered superconductor with a superconducting transition temperature Tc_c = 52 K. Due to the Fe spin-orbital related anisotropic exchange coupling (antiferromagnetic or ferromagnetic fluctuation), the tetragonal microcrystalline powder can be aligned at room temperature using the field-rotation method where the tetragonal ab\it{ab}-plane is parallel to the aligned magnetic field Ba_{a} and c\it{c}-axis along the rotation axis. Anisotropic superconducting properties with anisotropic diamagnetic ratio χc/χab∼\chi_{c}/\chi_{ab}\sim 2.4 + 0.6 was observed from low field susceptibility χ\chi(T) and magnetization M(Ba_{a}). The anisotropic low-field phase diagram with the variation of lower critical field gives a zero-temperature penetration depth λc\lambda_{c}(0) = 280 nm and λab\lambda_{ab}(0) = 120 nm. The magnetic fluctuation used for powder alignment at 300 K may be related with the pairing mechanism of superconductivity at lower temperature.Comment: 4 pages, 6 figure

    Ab initio many-body calculations of nucleon scattering on 4He, 7Li, 7Be, 12C and 16O

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    We combine a recently developed ab initio many-body approach capable of describing simultaneously both bound and scattering states, the ab initio NCSM/RGM, with an importance truncation scheme for the cluster eigenstate basis and demostrate its applicability to nuclei with mass numbers as high as 17. Using soft similarity renormalization group evolved chiral nucleon-nucleon interactions, we first calculate nucleon-4He phase shifts, cross sections and analyzing power. Next, we investigate nucleon scattering on 7Li, 7Be, 12C and 16O in coupled-channel NCSM/RGM calculations that include low-lying excited states of these nuclei. We check the convergence of phase shifts with the basis size and study A=8, 13, and 17 bound and unbound states. Our calculations predict low-lying resonances in 8Li and 8B that have not been experimentally clearly identified yet. We are able to reproduce reasonably well the structure of the A=13 low lying states. However, we find that A=17 states cannot be described without an improved treatment of 16O one-particle-one-hole excitations and alpha clustering.Comment: 18 pages, 20 figure

    Recrystallization of epitaxial GaN under indentation

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    We report recrystallization of epitaxial (epi-) GaN(0001) film under indentation.Hardness value is measured close to 10 GPa, using a Berkovich indenter. Pop-in burst in the loading line indicates nucleation of dislocations setting in plastic motion of lattice atoms under stress field for the recrystallization process. Micro-Raman studies are used to identify the recrystallization process. Raman area mapping indicates the crystallized region. Phonon mode corresponding to E2(high) close to 570 cm-1 in the as-grown epi-GaN is redshifted to stress free value close to 567 cm-1 in the indented region. Evolution of A1(TO) and E1(TO) phonon modes are also reported to signify the recrystallization process.Comment: 10 pages, 3 figures

    Surface optical Raman modes in InN nanostructures

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    Raman spectroscopic investigations are carried out on one-dimensional nanostructures of InN,such as nanowires and nanobelts synthesized by chemical vapor deposition. In addition to the optical phonons allowed by symmetry; A1, E1 and E2(high) modes, two additional Raman peaks are observed around 528 cm-1 and 560 cm-1 for these nanostructures. Calculations for the frequencies of surface optical (SO) phonon modes in InN nanostructures yield values close to those of the new Raman modes. A possible reason for large intensities for SO modes in these nanostructures is also discussed.Comment: 13 pages, 4 figures, Submitted in Journa

    Violating conformal invariance: Two-dimensional clusters grafted to wedges, cones, and branch points of Riemann surfaces

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    We present simulations of 2-d site animals on square and triangular lattices in non-trivial geomeLattice animals are one of the few critical models in statistical mechanics violating conformal invariance. We present here simulations of 2-d site animals on square and triangular lattices in non-trivial geometries. The simulations are done with the newly developed PERM algorithm which gives very precise estimates of the partition sum, yielding precise values for the entropic exponent θ\theta (ZN∼μNN−θZ_N \sim \mu^N N^{-\theta}). In particular, we studied animals grafted to the tips of wedges with a wide range of angles α\alpha, to the tips of cones (wedges with the sides glued together), and to branching points of Riemann surfaces. The latter can either have kk sheets and no boundary, generalizing in this way cones to angles α>360\alpha > 360 degrees, or can have boundaries, generalizing wedges. We find conformal invariance behavior, θ∼1/α\theta \sim 1/\alpha, only for small angles (α≪2π\alpha \ll 2\pi), while θ≈const−α/2π\theta \approx const -\alpha/2\pi for α≫2π\alpha \gg 2\pi. These scalings hold both for wedges and cones. A heuristic (non-conformal) argument for the behavior at large α\alpha is given, and comparison is made with critical percolation.Comment: 4 pages, includes 3 figure
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