31,084 research outputs found

    Semileptonic Kaon Decay in Staggered Chiral Perturbation Theory

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    The determination of ∣Vus∣\vert V_{us}\vert from kaon semileptonic decays requires the value of the form factor f+(q2=0)f_+(q^2=0), which can be calculated precisely on the lattice. We provide the one-loop partially quenched staggered chiral perturbation theory expressions that may be employed to analyze staggered simulations of f+(q2)f_+(q^2) with three light flavors. We consider both the case of a mixed action, where the valence and sea sectors have different staggered actions, and the standard case where these actions are the same. The momentum transfer q2q^2 of the form factor is allowed to have an arbitrary value. We give results for the generic situation where the uu, dd, and ss quark masses are all different, Nf=1+1+1N_f=1+1+1, and for the isospin limit, Nf=2+1N_f=2+1. The expression we obtain for f+(q2)f_+(q^2) is independent of the mass of the (valence) spectator quark. In the limit of vanishing lattice spacing, our results reduce to the one-loop continuum partially quenched expression for f+(q2)f_+(q^2), which has not previously been reported in the literature for the Nf=1+1+1N_f=1+1+1 case. Our expressions have already been used in staggered lattice analyses of f+(0)f_+(0), and should prove useful in future calculations as well.Comment: 33 pages, 5 figures; v2: some referencing change

    \u3ci\u3eCryptopygus Bipunctatus\u3c/i\u3e (Collembola: Isotomidae) in North America, and \u3ci\u3eC. Posteroculatus\u3c/i\u3e N. Comb.

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    Specimens of Cryptopygus bipunctatus are reported and described from North America (Michigan) for the first time. The species is easily recognized by its lack of color, one pair of ocelli on black eyespots, and one flair of ventral manubrial setae. Michigan and European specimens are very· similar. A very similar Polish species, Isotomina posteroculata, is transferred to Cryptopygus

    Tests of non-standard electroweak couplings of right-handed quarks

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    The standard model can be interpreted as the leading order of a Low-Energy Effective Theory (LEET) invariant under a higher non linearly realized symmetry Snat⊃SU(2)W×U(1)YS_{nat}\supset SU(2)_W \times U(1)_Y equipped with a systematic power counting. Within the minimal version of this ``not quite decoupling'' LEET, the dominant non-standard effect appears at next-to-leading order (NLO) and is a modification of the couplings of fermions to W and Z. In particular, the coupling of right-handed quarks to Z is modified and a direct coupling of right-handed quarks to W emerges. Charged right-handed lepton currents are forbidden by an additional discrete symmetry in the lepton sector originally designed to suppress Dirac neutrino masses. A complete NLO analysis of experimental constraints on these modified couplings is presented. Concerning couplings of light quarks, the interface of the electroweak tests with QCD aspects is discussed in detail.Comment: 56 pages, 14 figures, v2: references added, minor modifications in the text, accepted for publication in JHE

    The pion charge radius from charged pion electroproduction

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    We analyze a low-energy theorem of threshold pion electroproduction which allows one to determine the charge radius of the pion. We show that at the same order where the radius appears, pion loops induce a correction to the momentum dependence of the longitudinal dipole amplitude L0+(−)L_{0+}^{(-)}. This model-independent correction amounts to an increase of the pion charge radius squared from the electroproduction data by about 0.26~fm2^2. It sheds light on the apparent discrepancy between the recent determination of the pion radius from electroproduction data and the one based on pion-electron scattering.Comment: 3 pp, REVTeX, uses eps

    Pion-Nucleon Phase Shifts in Heavy Baryon Chiral Perturbation Theory

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    We calculate the phase shifts in the pion-nucleon scattering using the heavy baryon formalism. We consider phase shifts for the pion energy range of 140 to 200200 MeV. We employ two different methods for calculating the phase shifts - the first using the full third order calculation of the pion-nucleon scattering amplitude and the second by including the resonances Δ\Delta and N∗N^* as explicit degrees of freedom in the Lagrangian. We compare the results of the two methods with phase shifts extracted from fits to the pion-nucleon scattering data. We find good to fair agreement between the calculations and the phase shifts from scattering data.Comment: 14 pages, Latex, 6figures. Revised version to appear in Phys.Rev.
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