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    Finite-region boundedness and stabilization for 2D continuous-discrete systems in Roesser model

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    This paper investigates the finite-region boundedness (FRB) and stabilization problems for two-dimensional continuous-discrete linear Roesser models subject to two kinds of disturbances. For two-dimensional continuous-discrete system, we first put forward the concepts of finite-region stability and FRB. Then, by establishing special recursive formulas, sufficient conditions of FRB for two-dimensional continuous-discrete systems with two kinds of disturbances are formulated. Furthermore, we analyze the finite-region stabilization issues for the corresponding two-dimensional continuous-discrete systems and give generic sufficient conditions and sufficient conditions that can be verified by linear matrix inequalities for designing the state feedback controllers which ensure the closed-loop systems FRB. Finally, viable experimental results are demonstrated by illustrative examples

    Analysis of the strong vertices of Ξ£cNDβˆ—\Sigma_cND^{*} and Ξ£bNBβˆ—\Sigma_bNB^{*} in QCD sum rules

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    The strong coupling constant is an important parameter which can help us to understand the strong decay behaviors of baryons. In our previous work, we have analyzed strong vertices Ξ£cβˆ—ND\Sigma_{c}^{*}ND, Ξ£bβˆ—NB\Sigma_{b}^{*}NB, Ξ£cND\Sigma_{c}ND, Ξ£bNB\Sigma_{b}NB in QCD sum rules. Following these work, we further analyze the strong vertices Ξ£cNDβˆ—\Sigma_{c}ND^{*} and Ξ£bNBβˆ—\Sigma_{b}NB^{*} using the three-point QCD sum rules under Dirac structures q ⁣ ⁣ ⁣/p ⁣ ⁣ ⁣/Ξ³Ξ±q\!\!\!/p\!\!\!/\gamma_{\alpha} and q ⁣ ⁣ ⁣/p ⁣ ⁣ ⁣/pΞ±q\!\!\!/p\!\!\!/p_{\alpha}. In this work, we first calculate strong form factors considering contributions of the perturbative part and the condensate terms ⟨qβ€Ύq⟩\langle\overline{q}q\rangle, ⟨αsΟ€GG⟩\langle\frac{\alpha_{s}}{\pi}GG\rangle and ⟨qβ€ΎgsΟƒGq⟩\langle\overline{q}g_{s}\sigma Gq\rangle. Then, these form factors are used to fit into analytical functions. According to these functions, we finally determine the values of the strong coupling constants for these two vertices Ξ£cNDβˆ—\Sigma_{c}ND^{*} and Ξ£bNBβˆ—\Sigma_{b}NB^{*}.Comment: arXiv admin note: text overlap with arXiv:1705.0322
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