479 research outputs found

    Herbicide Control of Tall Larkspurs on Mountain Rangeland

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    Tall larkspurs kill more cattle on mountain rangelands than any other plant or disease. Tall larkspurs are principal components of tall forb communities and occur in patches associated with snow drifts in mountain big sagebrush, aspen and subalpine plant communities. Controlling larkspur patches can substantially reduce cattle deaths (3). Larkspur will never be eradicated, but if its density could be reduced to where a cow could not eat enough larkspur, fast enough, death losses can be reduced

    Catch crop strategy and nitrate leaching following grazed grass-clover

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    Cultivation of grassland presents a high risk of nitrate leaching. This study aimed to determine if leaching could be reduced by growing spring barley (Hordeum vulgare L.) as a green crop for silage with undersown Italian ryegrass (Lolium multiïŹ‚orum Lam.) compared with barley grown to maturity with or without an undersown conventional catch crop of perennial ryegrass (Lolium perenne L.). All treatments received 0,60 or 120 kg of ammonium-N ha-1 in cattle slurry. In spring 2003, two grass-clover ïŹelds (3 and 5 years old, respectively, with different management histories) were ploughed. The effects of the treatments on yield and nitrate leaching were determined in the ïŹrst year, while the residual effects of the treatments were determined in the second year in a crop of spring barley⁄perennial ryegrass. Nitrate leaching was estimated in selected treatments using soil water samples from ceramic cups. The experiment showed that compared with treatments without catch crop, green barley⁄Italian ryegrass reduced leaching by 163–320 kg Nha-1, corresponding to 95–99%, and the perennial ryegrass reduced leaching to between 34 and 86 kg Nha-1, corresponding to a reduction of 80 and 66%. Also, in the second growing season, leaching following catchcrops was reduced compared with the bare soil treatment. It was concluded that the green barley⁄Italian ryegrass offers advantages not only for the environment but also for farmers, for whom it provides a fodder high in roughage and avoids the difïŹculties with clover fatigue increasingly experienced by Danish farmers

    Vector field localization and negative tension branes

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    It is shown that negative tension branes in higher dimensions may lead to an effective lower dimensional theory where the gauge-invariant vector fields associated with the fluctuations of the metric are always massless and localized on the brane. Explicit five-dimensional examples of this phenomenon are provided. Furthermore, it is shown that higher dimensional gauge fields can also be localized on these configurations with the zero mode separated from the massive tower by a gap.Comment: 16 pages, LaTeX style; to appear in Phys. Rev.

    Lattice Study of the Massive Schwinger Model with a Ξ\theta term under L\"uscher's "Admissibility" condition

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    We present a numerical study of the massive two-flavor QED in two dimensions with the gauge action proposed by L\"uscher, which allows only ``admissible'' gauge fields. We find that the admissibility condition does not allow any topology changes by the local updation in Hybrid Monte Carlo algorithm so that the configurations in each topological sector can be generated separately. By developing a new method to sum over different topological sectors, we investigate Ξ\theta vacuum effects. Combining with domain-wall fermion action, we obtain the fermion mass dependence and Ξ\theta dependence of the meson masses, which are consistent with the analytic results by mass perturbation in the continuum theory.Comment: 3 pages, Lattice2003(chiral

    Improved results for N=(2,2) super Yang-Mills theory using supersymmetric discrete light-cone quantization

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    We consider the (1+1)-dimensional N=(2,2){\cal N}=(2,2) super Yang--Mills theory which is obtained by dimensionally reducing N=1{\cal N}=1 super Yang--Mills theory in four dimension to two dimensions. We do our calculations in the large-NcN_c approximation using Supersymmetric Discrete Light Cone Quantization. The objective is to calculate quantities that might be investigated by researchers using other numerical methods. We present a precision study of the low-mass spectrum and the stress-energy correlator . We find that the mass gap of this theory closes as the numerical resolution goes to infinity and that the correlator in the intermediate rr region behaves like r−4.75r^{-4.75}.Comment: 18 pages, 8 figure

    A Lattice Study of the Nucleon Excited States with Domain Wall Fermions

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    We present results of our numerical calculation of the mass spectrum for isospin one-half and spin one-half non-strange baryons, i.e. the ground and excited states of the nucleon, in quenched lattice QCD. We use a new lattice discretization scheme for fermions, domain wall fermions, which possess almost exact chiral symmetry at non-zero lattice spacing. We make a systematic investigation of the negative-parity N∗N^* spectrum by using two distinct interpolating operators at ÎČ=6/g2=6.0\beta=6/g^2=6.0 on a 163×32×1616^3 \times 32 \times 16 lattice. The mass estimates extracted from the two operators are consistent with each other. The observed large mass splitting between this state, N∗(1535)N^*(1535), and the positive-parity ground state, the nucleon N(939), is well reproduced by our calculations. We have also calculated the mass of the first positive-parity excited state and found that it is heavier than the negative-parity excited state for the quark masses studied.Comment: 46 pages, REVTeX, 11 figures included, revised version accepted for publication in Phys. Rev.

    Numerical Study of Gluon Propagator and Confinement Scenario in Minimal Coulomb Gauge

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    We present numerical results in SU(2) lattice gauge theory for the space-space and time-time components of the gluon propagator at equal time in the minimal Coulomb gauge. It is found that the equal-time would-be physical 3-dimensionally transverse gluon propagator Dtr(k⃗)D^{tr}(\vec{k}) vanishes at k⃗=0\vec{k} = 0 when extrapolated to infinite lattice volume, whereas the instantaneous color-Coulomb potential D44(k⃗)D_{44}(\vec{k}) is strongly enhanced at k⃗=0\vec{k} = 0. This has a natural interpretation in a confinement scenario in which the would-be physical gluons leave the physical spectrum while the long-range Coulomb force confines color. Gribov's formula Dtr(k⃗)=(∣k⃗∣/2)[(k⃗2)2+M4]1/2D^{tr}(\vec{k}) = (|\vec{k}|/2)[(\vec{k}^2)^2 + M^4]^{1/2} provides an excellent fit to our data for the 3-dimensionally transverse equal-time gluon propagator Dtr(k⃗)D^{tr}(\vec{k}) for relevant values of k⃗\vec{k}.Comment: 23 pages, 12 figures, TeX file. Minor modifications, incorporating referee's suggestion

    K* nucleon hyperon form factors and nucleon strangeness

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    A crucial input for recent meson hyperon cloud model estimates of the nucleon matrix element of the strangeness current are the nucleon-hyperon-K* (NYK*) form factors which regularize some of the arising loops. Prompted by new and forthcoming information on these form factors from hyperon-nucleon potential models, we analyze the dependence of the loop model results for the strange-quark observables on the NYK* form factors and couplings. We find, in particular, that the now generally favored soft N-Lambda-K* form factors can reduce the magnitude of the K* contributions in such models by more than an order of magnitude, compared to previous results with hard form factors. We also discuss some general implications of our results for hadronic loop models.Comment: 9 pages, 8 figures, new co-author, discussion extended to the momentum dependence of the strange vector form factor

    Effective Lagrangian for strongly coupled domain wall fermions

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    We derive the effective Lagrangian for mesons in lattice gauge theory with domain-wall fermions in the strong-coupling and large-N_c limits. We use the formalism of supergroups to deal with the Pauli-Villars fields, needed to regulate the contributions of the heavy fermions. We calculate the spectrum of pseudo-Goldstone bosons and show that domain wall fermions are doubled and massive in this regime. Since we take the extent and lattice spacing of the fifth dimension to infinity and zero respectively, our conclusions apply also to overlap fermions.Comment: 26 pp. RevTeX and 3 figures; corrected error in symmetry breaking scheme and added comments to discussio
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