3,181 research outputs found

    Generalized tt-jj Model

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    By parameterizing the t-j model we present a new electron correlation model with one free parameter for high-temperature superconductivity. This model is of SUq(1,2)SU_{q}(1,2) symmetry. The energy spectrums are shown to be modulated by the free parameter in the model. The solution and symmetric structures of the Hilbert space, as well as the Bethe ansatz approach are discussed for special cases.Comment: 13 page, Latex, to appear in J. Phys.

    Lepton flavor violating semileptonic τ\tau decays τlP(V)\tau\to lP(V) in a topcolor scenario

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    The contributions of the neutral top-pion πt0\pi_{t}^{0} and the non-universal gauge boson ZZ' predicted by topcolor scenario to the lepton flavor violating (LFV)(LFV) semileptonic τ\tau decays τlP(V)\tau\to lP(V) (P=π0,η,η(P=\pi^{0}, \eta, \eta' and V=ρ0,ϕ) V=\rho^{0}, \phi) are discussed. We find that the contributions of ZZ' to these decay processes are generally larger than those from πt0\pi_{t}^{0}. πt0\pi_{t}^{0} can only make the value of the branching ratio Br(τlP)Br(\tau\to lP) in the range of 1×1011\times10^{-11} \sim 1×1016\times10^{-16}, which is far below the sensitivity of foreseeable experiments. With reasonable values of the free parameters, the non-universal gauge boson ZZ' can make the value of the branching ratio Br(τμϕ)Br(\tau^{-}\to \mu^{-}\phi) reach 1×107\times10^{-7}, which might approach the observable threshold of near-future experiments.Comment: 15 pages. Discussions added, some typos correcte

    The asymptotic behavior of globally smooth solutions of bipolar non-isentropic compressible Euler-Maxwell system for plasma

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    The bipolar non-isentropic compressible Euler-Maxwell system is investigated in R3R^3 in the present paper, and the LqL^q time decay rate for the global smooth solution is established. It is shown that the total densities, total temperatures and magnetic field of two carriers converge to the equilibrium states at the same rate (1+t)3/2+3q/2(1+t)^{-3/2+3q/2} in LqL^q norm. But, both the difference of densities and the difference of temperatures of two carriers decay at the rate (1+t)21q(1+t)^{-2-\frac{1}{q}}, and the velocity and electric field decay at the rate (1+t)3/2+12q(1+t)^{-3/2+\frac{1}{2q}}. This phenomenon on the charge transport shows the essential difference between the non-isentropic unipolar Euler-Maxwell and the bipolar isentropic Euler-Maxwell system.Comment: 27page

    Hydrodynamic Description of Granular Convection

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    We present a hydrodynamic model that captures the essence of granular dynamics in a vibrating bed. We carry out the linear stability analysis and uncover the instability mechanism that leads to the appearance of the convective rolls via a supercritical bifurcation of a bouncing solution. We also explicitly determine the onset of convection as a function of control parameters and confirm our picture by numerical simulations of the continuum equations.Comment: 14 pages, RevTex 11pages + 3 pages figures (Type csh

    Soliton Solutions on Noncommutative Orbifold $ T^2/Z_4

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    In this paper, we explicitly construct a series of projectors on integral noncommutative orbifold T2/Z4T^2/Z_4 by extended GHSGHS constrution. They include integration of two arbitary functions with Z4Z_4 symmetry. Our expressions possess manifest Z4Z_{4} symmetry. It is proved that the expression include all projectors with minimal trace and in their standard expansions, the eigen value functions of coefficient operators are continuous with respect to the arguments kk and qq. Based on the integral expression, we alternately show the derivative expression in terms of the similar kernal to the integral one.Since projectors correspond to soliton solutions of the field theory on the noncommutative orbifold, we thus present a series of corresponding solitons.Comment: 18 pages, no figure; referrences adde

    Effect of non-phytate phosphorus levels and phytase sources on the growth performance, serum biochemical and tibial parameters of broiler chickens

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    A 3×3 fattorial arrangement with dietary non-phytate phosphorus (NPP) levels and phytase sources (3- and 6-phytase) was conducted to evaluate the effects of NPP levels, phytase sources and their possible interactions on growth performance, serum biochemical and tibia parameters of broiler chickens from hatch to 42 days of age. A total of 540 1-day-old Arbor Acres male broiler chicks were randomly allocated into nine dietary treatments, each containing 5 replicates pens with 12 birds per pen. Interaction was statistically significant in the performance till day 21 of trial, supplementation of low NPP diet decreased body weight (BW) (P<0.001), depressed average daily gain (ADG) (P<0.001) and deteriorated average daily feed intake (ADFI) (P<0.001) over day 42. During the 8-to-21-day period, even if interaction between NPP levels and phytase sources was significant (P<0.01), BW, ADG and ADFI always increased due to dietary supplementation of phytase, with source not differing. Dietary high NPP enhanced serum calcium and P concentrations on day 21 and 42 (linear contrast, P<0.01), while decreased alkaline phosphatase (AKP) activity on day 42 (linear contrast, P<0.001), and interaction was not significant. Both dietary sources of phytase decreased serum AKP activities on day 42 (P<0.001), and urea nitrogen content on day 21 (P<0.01) and 42 (P<0.001). Both phytase improved ash percentage on day 21 and P content in tibia at 21 and 42 days of age (P<0.001). The results confirmed that dietary supplementation of phytase may enhance P availability during the 8-to-21-day period. Nevertheless, no difference between the two phytase sources was observed

    Pair production of charged Higgs bosons in the Left-Right Twin Higgs model at the ILC and LHC

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    Left-Right twin Higgs(LRTH) model predicts the existence of a pair of charged Higgs ϕ±\phi^{\pm}. In this paper, we study the production of the charged Higgs bosons pair ϕ±\phi^{\pm} via the process e+eϕ+ϕe^{+}e^{-}\to \phi^{+}\phi^{-} at the International Linear Collider(ILC). The numerical results show that the production rates are at the level of several tens fb, this process can produce the adequate distinct multi-jet final states and the SM background can be efficiently reduced. We also discuss the charged Higgs boson pair production via the process qqˉϕ+ϕq\bar{q}\to \phi^{+}\phi^{-} at the CERNCERN Large Hadron Collider(LHC) and estimate there production rates. We find that, as long as the charged Higgs bosons are not too heavy, they can be abundantly produced at the LHC. The possible signatures of these new particles might be detected at the ILC and LHC experiments.Comment: 15 pages, 5 figures, discussion extended, reference added, typos fixed, revised version to be published in Eur.Phys.J.
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