574,056 research outputs found

    N-port rectangular-shaped distributed RC NETWORKS

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    Dielectric material between resistive thin film and pure conductor considered as n-port distributed RC networ

    Lattice QCD study on K∗(892)K^\ast(892) meson decay width

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    We deliver an exploratory lattice QCD examination of the K∗(892)K^\ast(892) meson decay width with the help of the p-wave scattering phase δ1\delta_1 of pion-kaon (πK\pi K) system in the isospin I=1/2I=1/2 channel, which are extracted by the modified Rummukainen-Gottlieb formula for two-particle system with arbitrary mass, and it clearly reveals the entity of a resonance at a mass around K∗(892)K^\ast(892) meson mass. The effective range formula is applied to describe the energy dependence of the scattering phase and we obtain the effective K∗→πKK^\ast \to \pi K coupling constant as gK∗πK=6.38(78)g_{K^\ast \pi K} = 6.38(78), and subsequently achieve the decay width to be 64.9±8.064.9 \pm 8.0 MeV, which is in reasonable accordance with the current experiment. Our lattice investigations are conducted on a 203×4820^3\times48 MILC full QCD gauge configuration at (mπ+mK)/mK∗≈0.739(m_\pi + m_K) / m_{K^\ast} \approx 0.739 and the lattice spacing a≈0.15a \approx 0.15 fm.Comment: Correct some typos and replace some figures with high quality one

    su(2) and su(1,1) displaced number states and their nonclassical properties

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    We study su(2) and su(1,1) displaced number states. Those states are eigenstates of density-dependent interaction systems of quantized radiation field with classical current. Those states are intermediate states interpolating between number and displaced number states. Their photon number distribution, statistical and squeezing properties are studied in detail. It is show that these states exhibit strong nonclassical properties.Comment: 10 pages, 3 figure

    Intermediate coherent-phase(PB) states of radiation fields and their nonclassical properties

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    Intermediate states interpolating coherent states and Pegg-Barnett phase states are investigated using the ladder operator approach. These states reduce to coherent and Pegg-Barnett phase states in two different limits. Statistical and squeezing properties are studied in detail.Comment: 9 pages, 3 EPS figures, use epsf.sty. Accepted for publication in Phys.Lett.
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