28,504 research outputs found

    Some sharp inequalities involving Seiffert and other means and their concise proofs

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    In the paper, by establishing the monotonicity of some functions involving the sine and cosine functions, the authors provide concise proofs of some known inequalities and find some new sharp inequalities involving the Seiffert, contra-harmonic, centroidal, arithmetic, geometric, harmonic, and root-square means of two positive real numbers aa and bb with a≠ba\ne b.Comment: 10 page

    Geometric convexity of the generalized sine and the generalized hyperbolic sine

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    In the paper, the authors prove that the generalized sine function sin⁑p,q(x)\sin_{p,q}(x) and the generalized hyperbolic sine function sinh⁑p,q(x)\sinh_{p,q}(x) are geometrically concave and geometrically convex, respectively. Consequently, the authors verify a conjecture posed in the paper "B. A. Bhayo and M. Vuorinen, On generalized trigonometric functions with two parameters, J. Approx. Theory 164 (2012), no.~10, 1415\nobreakdash--1426; Available online at \url{http://dx.doi.org/10.1016/j.jat.2012.06.003}".Comment: 5 page

    Fully open-flavor tetraquark states bcqˉsˉbc\bar{q}\bar{s} and scqˉbˉsc\bar{q}\bar{b} with JP=0+,1+J^{P}=0^{+},1^{+}

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    We have studied the masses for fully open-flavor tetraquark states bcqΛ‰sΛ‰bc\bar{q}\bar{s} and scqΛ‰bΛ‰sc\bar{q}\bar{b} with quantum numbers JP=0+,1+J^{P}=0^{+},1^{+}. We systematically construct all diquark-antiquark interpolating currents and calculate the two-point correlation functions and spectral densities in the framework of QCD sum rule method. Our calculations show that the masses are about 7.1βˆ’7.27.1-7.2 GeV for the bcqΛ‰sΛ‰bc\bar{q}\bar{s} tetraquark states and 7.0βˆ’7.17.0-7.1 GeV for the scqΛ‰bΛ‰sc\bar{q}\bar{b} tetraquarks. The masses of bcqΛ‰sΛ‰bc\bar{q}\bar{s} tetraquarks are below the thresholds of BΛ‰sD\bar{B}_{s}D and BΛ‰sβˆ—D\bar{B}_{s}^{*}D final states for the scalar and axial-vector channels respectively. The scqΛ‰bΛ‰sc\bar{q}\bar{b} tetraquark states with JP=1+J^{P}=1^{+} lie below the Bc+Kβˆ—B_{c}^{+}K^{*} and Bsβˆ—DB_{s}^{*}D thresholds. Such low masses for these possible tetraquark states indicate that they can only decay via weak interaction and thus are very narrow and stable.Comment: 17 pages, 4 figure
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