24,136 research outputs found

    Work Function of Single-wall Silicon Carbide Nanotube

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    Using first-principles calculations, we study the work function of single wall silicon carbide nanotube (SiCNT). The work function is found to be highly dependent on the tube chirality and diameter. It increases with decreasing the tube diameter. The work function of zigzag SiCNT is always larger than that of armchair SiCNT. We reveal that the difference between the work function of zigzag and armchair SiCNT comes from their different intrinsic electronic structures, for which the singly degenerate energy band above the Fermi level of zigzag SiCNT is specifically responsible. Our finding offers potential usages of SiCNT in field-emission devices.Comment: 3 pages, 3 figure

    Nodeless superconductivity in Ir1βˆ’x_{1-x}Ptx_xTe2_2 with strong spin-orbital coupling

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    The thermal conductivity ΞΊ\kappa of superconductor Ir1βˆ’x_{1-x}Ptx_{x}Te2_2 (xx = 0.05) single crystal with strong spin-orbital coupling was measured down to 50 mK. The residual linear term ΞΊ0/T\kappa_0/T is negligible in zero magnetic field. In low magnetic field, ΞΊ0/T\kappa_0/T shows a slow field dependence. These results demonstrate that the superconducting gap of Ir1βˆ’x_{1-x}Ptx_{x}Te2_2 is nodeless, and the pairing symmetry is likely conventional s-wave, despite the existence of strong spin-orbital coupling and a quantum critical point.Comment: 5 pages, 4 figure

    Binomial coefficients, Catalan numbers and Lucas quotients

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    Let pp be an odd prime and let a,ma,m be integers with a>0a>0 and m≑̸0(modp)m \not\equiv0\pmod p. In this paper we determine βˆ‘k=0paβˆ’1(2kk+d)/mk\sum_{k=0}^{p^a-1}\binom{2k}{k+d}/m^k mod p2p^2 for d=0,1d=0,1; for example, βˆ‘k=0paβˆ’1(2kk)mk≑(m2βˆ’4mpa)+(m2βˆ’4mpaβˆ’1)upβˆ’(m2βˆ’4mp)(modp2),\sum_{k=0}^{p^a-1}\frac{\binom{2k}k}{m^k}\equiv\left(\frac{m^2-4m}{p^a}\right)+\left(\frac{m^2-4m}{p^{a-1}}\right)u_{p-(\frac{m^2-4m}{p})}\pmod{p^2}, where (βˆ’)(-) is the Jacobi symbol, and {un}nβ©Ύ0\{u_n\}_{n\geqslant0} is the Lucas sequence given by u0=0u_0=0, u1=1u_1=1 and un+1=(mβˆ’2)unβˆ’unβˆ’1u_{n+1}=(m-2)u_n-u_{n-1} for n=1,2,3,…n=1,2,3,\ldots. As an application, we determine βˆ‘0<k<pa, k≑r(modpβˆ’1)Ck\sum_{0<k<p^a,\, k\equiv r\pmod{p-1}}C_k modulo p2p^2 for any integer rr, where CkC_k denotes the Catalan number (2kk)/(k+1)\binom{2k}k/(k+1). We also pose some related conjectures.Comment: 24 pages. Correct few typo

    S-shaped flow curves of shear thickening suspensions: Direct observation of frictional rheology

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    We study the rheological behavior of concentrated granular suspensions of simple spherical particles. Under controlled stress, the system exhibits an S-shaped flow curve (stress vs. shear rate) with a negative slope in between the low-viscosity Newtonian regime and the shear thickened regime. Under controlled shear rate, a discontinuous transition between the two states is observed. Stress visualization experiments with a novel fluorescent probe suggest that friction is at the origin of shear thickening. Stress visualization shows that the stress in the system remains homogeneous (no shear banding) if a stress is imposed that is intermediate between the high and low-stress branches. The S-shaped shear thickening is then due to the discontinuous formation of a frictional force network between particles upon increasing the stress.Comment: 5 pages + 6 figure
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