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    Pointwise estimates for the Bergman kernel of the weighted Fock space

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    We prove upper pointwise estimates for the Bergman kernel of the weighted Fock space of entire functions in L2(e2ϕ)L^2(e^{-2\phi}) where ϕ\phi is a subharmonic function with Δϕ\Delta \phi a doubling measure. We derive estimates for the canonical solution operator to the inhomogeneous Cauchy-Riemann equation and we characterize the compactness of this operator in terms of Δϕ\Delta \phi

    Metamaterial with polarization and direction insensitive resonant transmission response mimicking electromagnetically induced transparency

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    We report on a planar metamaterial, the resonant transmission frequency of which does not depend on the polarization and angle of incidence of electromagnetic waves. The resonance results from the excitation of high-Q antisymmetric trapped current mode and shows sharp phase dispersion characteristic to Fano-type resonances of the electromagnetically induced transparency phenomenon

    The Influences of Outflow on the Dynamics of Inflow

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    Both numerical simulations and observations indicate that in an advection-dominated accretion flow most of the accretion material supplied at the outer boundary will not reach the inner boundary. Rather, they are lost via outflow. Previously, the influence of outflow on the dynamics of inflow is taken into account only by adopting a radius-dependent mass accretion rate M˙=M˙0(r/rout)s\dot{M}=\dot{M}_0 (r/r_{\rm out})^s with s>0s>0. In this paper, based on a 1.5 dimensional description to the accretion flow, we investigate this problem in more detail by considering the interchange of mass, radial and azimuthal momentum, and the energy between the outflow and inflow. The physical quantities of the outflow is parameterized based on our current understandings to the properties of outflow mainly from numerical simulations of accretion flows. Our results indicate that under reasonable assumptions to the properties of outflow, the main influence of outflow has been properly included by adopting M˙=M˙0(r/rout)s\dot{M}=\dot{M}_0 (r/r_{\rm out})^s.Comment: 16 pages, 5 figures. accepted for publication in Ap
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