42,801 research outputs found

    Description of ρ(1700)\rho (1700) as a ρKKˉ\rho K \bar{K} system with the fixed center approximation

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    We study the ρKKˉ\rho K\bar{K} system with an aim to describe the ρ(1700)\rho (1700) resonance. The chiral unitary approach has achieved success in a description of systems of the light hadron sector. With this method, the KKˉK \bar{K} system in the isospin sector I=0I=0, is found to be a dominant component of the f0(980)f_0 (980) resonance. Therefore, by regarding the KKˉK\bar{K} system as a cluster, the f0(980)f_0 (980) resonance, we evaluate the ρKKˉ\rho K\bar{K} system applying the fixed center approximation to the Faddeev equations. We construct the ρK\rho K unitarized amplitude using the chiral unitary approach. As a result, we find a peak in the three-body amplitude around 1739 MeV and a width of about 227 MeV. The effect of the width of ρ\rho and f0(980)f_0 (980) is also discussed. We associate this peak to the ρ(1700)\rho (1700) which has a mass of 1720±201720 \pm 20 MeV and a width of 250±100250 \pm 100 MeV

    Geometric Mean Neutrino Mass Relation

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    Present experimental data from neutrino oscillations have provided much information about the neutrino mixing angles. Since neutrino oscillations only determine the mass squared differences Δmij2=mi2mj2\Delta m^2_{ij} = m^2_i - m^2_j, the absolute values for neutrino masses mim_i can not be determined using data just from oscillations. In this work we study implications on neutrino masses from a geometric mean mass relation m2=m1m3m_2=\sqrt{m_1 m_3} which enables one to determined the absolute masses of the neutrinos. We find that the central values of the three neutrino masses and their 2σ2\sigma errors to be m1=(1.58±0.18)meVm_1 = (1.58\pm 0.18){meV}, m2=(9.04±0.42)meVm_2 = (9.04\pm 0.42){meV}, and m3=(51.8±3.5)meVm_3 = (51.8\pm 3.5){meV}. Implications for cosmological observation, beta decay and neutrinoless double beta decays are discussed.Comment: 7 pages. Talk given at COSPA06. A reference adde

    Tunable Localization and Oscillation of Coupled Plasmon Waves in Graded Plasmonic Chains

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    The localization (confinement) of coupled plasmon modes, named as gradons, has been studied in metal nanoparticle chains immersed in a graded dielectric host. We exploited the time evolution of various initial wavepackets formed by the linear combination of the coupled modes. We found an important interplay between the localization of plasmonic gradons and the oscillation in such graded plasmonic chains. Unlike in optical superlattices, gradient cannot always lead to Bloch oscillations, which can only occur for wavepackets consisting of particular types of gradons. Moreover, the wavepackets will undergo different forms of oscillations. The correspondence can be applied to design a variety of optical devices by steering among various oscillations.Comment: Sumitted to Journal of Applied Physic

    ADVERTISING, STRUCTURAL CHANGE, AND U.S. NON-ALCOHOLIC BEVERAGE DEMAND

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    The dominant trend in U.S. non-alcoholic consumption over the past two decades has been a steady increase in soft-drink consumption, largely at the expense of milk and coffee and tea consumption. Our analysis suggests that the primary factors affecting this is that the price, advertising, and demographic elasticities estimated from the Rotterdam model are much smaller than the adjusted trend coefficients and the expenditure elasticities.Consumer/Household Economics, Demand and Price Analysis, Marketing,

    A narrow DNNDNN quasi-bound state

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    The energies and widths of DNNDNN quasi-bound states with isospin I=1/2 are evaluated in two methods, the fixed center approximation to the Faddeev equation and the variational method approach to the effective one-channel Hamiltonian. The DNDN interactions are constructed so that they dynamically generate the Λc(2595)\Lambda_c(2595) (I=0, Jπ=1/2J^{\pi} =1/2^-) resonance state. We find that the system is bound by about 250 MeV from the DNNDNN threshold, s3500\sqrt{s} \sim 3500 MeV. Its width including both the mesonic decay and the DD absorption, is estimated to be about 20-40 MeV. The I=0 DNDN pair in the DNNDNN system is found to form a cluster that is similar to the Λc(2595)\Lambda_c(2595).Comment: 17 pages, 18 figures, 3 table
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