1,146 research outputs found

    Elastic Meson-Nucleon and Nucleon-Nucleon Scattering: Models vs. All Available Data

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    We consider simple-pole descriptions of soft elastic scattering at small tt and ss, and allow for the presence of a hard pomeron. We have built and analyzed an exhaustive dataset and we show that simple poles provide an excellent description of the data in the region 0.5- 0.5 GeV2<t<^2 < t < 0.1- 0.1 GeV2^2, 6 GeV<s<<\sqrt{s}<63 GeV. We show that new form factors have to be used, and get information on the trajectories of the soft and hard pomerons.Comment: Contribution to the proceedings of the XIth International Conference on Elastic and Diffractive Scattering, Chateau de Blois, France, May 15 - 20, 2005. Needs Blois.sty (provided

    Temperature - pressure phase diagram of CeCoSi: Pressure induced high-temperature phase

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    We have studied the temperature-pressure phase diagram of CeCoSi by electrical-resistivity experiments under pressure. Our measurements revealed a very unusual phase diagram. While at low pressures no dramatic changes and only a slight shift of the Ne\'{e}l temperature TNT_N (10\approx 10 K) are observed, at about 1.45 GPa a sharp and large anomaly, indicative of the opening of a spin-density-wave (SDW) gap, appears at a comparatively high temperature TS38T_S \approx 38 K. With further increasing pressure TST_S shifts rapidly to low temperatures and disappears at about 2.15 GPa, likely continuously in a quantum critical point, but without evidence for superconductivity. Even more surprisingly, we observed a clear shift of TST_S to higher temperatures upon applying a magnetic field. We discuss two possible origins for TST_S, either magnetic ordering of Co or a meta-orbital type of transition of Ce.Comment: 6 pages, 5 figure

    Hard pomeron contribution to forward elastic scattering

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    The introduction of a hard singularity in fits to total cross sections and to the ratio of real to imaginary parts enables to reproduce perfectly the data for sqrt(s)< 100 GeV using only simple-pole parametrisations, both for the soft and for the hard pomerons.Comment: Contribution to the proceedings of the XIth International Conference on Elastic and Diffractive Scattering, Chateau de Blois, France, May 15 - 20, 2005. Needs Blois.sty (provided

    Turing Instability in a Boundary-fed System

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    The formation of localized structures in the chlorine dioxide-idodine-malonic acid (CDIMA) reaction-diffusion system is investigated numerically using a realistic model of this system. We analyze the one-dimensional patterns formed along the gradients imposed by boundary feeds, and study their linear stability to symmetry-breaking perturbations (Turing instability) in the plane transverse to these gradients. We establish that an often-invoked simple local linear analysis which neglects longitudinal diffusion is inappropriate for predicting the linear stability of these patterns. Using a fully nonuniform analysis, we investigate the structure of the patterns formed along the gradients and their stability to transverse Turing pattern formation as a function of the values of two control parameters: the malonic acid feed concentration and the size of the reactor in the dimension along the gradients. The results from this investigation are compared with existing experiments.Comment: 41 pages, 18 figures, to be published in Physical Review

    Avoided ferromagnetic quantum critical point in CeRuPO

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    CeRuPO is a rare example of a ferromagnetic (FM) Kondo-lattice system. External pressure suppresses the ordering temperature to zero at about pc3p_c\approx3 GPa. Our ac-susceptibility and electrical-resistivity investigations evidence that the type of magnetic ordering changes from FM to antiferromagnetic (AFM) at about p0.87p^*\approx0.87 GPa. Studies in applied magnetic fields suggest that ferromagnetic and antiferromagnetic correlations compete for the ground state at p>pp>p^*, but finally the AFM correlations win. The change in the magnetic ground-state properties is closely related to the pressure evolution of the crystalline-electric-field level (CEF) scheme and the magnetic Ruderman-Kittel-Kasuya-Yosida (RKKY) exchange interaction. The N\'{e}el temperature disappears abruptly in a first-order-like fashion at pcp_c, hinting at the absence of a quantum critical point. This is consistent with the low-temperature transport properties exhibiting Landau-Fermi-liquid (LFL) behavior in the whole investigated pressure range up to 7.5 GPa.Comment: 12 figure

    Effect of Co doping and hydrostatic pressure on SrFe2As2

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    We report a pressure study on electron doped SrFe2x_{2-x}Cox_xAs2_2 by electrical-resistivity (ρ\rho) and magnetic-susceptibility (χ\chi) experiments. Application of either external pressure or Co substitution rapidly suppresses the spin-density wave ordering of the Fe moments and induces superconductivity in SrFe2_2As2_2. At x=0.2x=0.2 the broad superconducting (SC) dome in the TpT-p phase diagram exhibits its maximum Tc,max=20T_{c,{\rm max}}=20 K at a pressure of only pmax0.75p_{\rm max}\approx 0.75 GPa. In SrFe1.5_{1.5}Co0.5_{0.5}As2_2 no superconductivity is observed anymore up to 2.8 GPa. Upon increasing the Co concentration the maximum of the SC dome shifts toward lower pressure accompanied by a decrease in the value of Tc,maxT_{c,{\rm max}}. Even though, superconductivity is induced by both tuning methods, Co substitution leads to a much more robust SC state. Our study evidences that in SrFe2x_{2-x}Cox_xAs2_2 both, the effect of pressure and Co-substitution, have to be considered in order to understand the SC phase-diagram and further attests the close relationship of SrFe2_2As2_2 and its sister compound BaFe2_2As2_2.Comment: 6 pages, 6 figure

    Direct extraction of hadronic form factors from elastic-scattering data

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    Non-forward elastic hadron-scattering data are collected and analysed within the Regge approach. Through an analysis of the data in small bins in tt, we have directly extracted the pomeron trajectory and the hadronic form factors (or reggeon couplings). We found higher values than usually used for the intercept and for the slope of the soft pomeron trajectory. The presence of zeros in tt for the effective hadronic form factors is emphasised.Comment: 4 pages, 5 figures, talk given at Diffraction 2004, Cala Gonone, Sardinia, Italy, 18-23 September 200
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