232 research outputs found
Herbicide-resistant crops : A weed scientistâs perspective
Les cultures rĂ©sistantes aux herbicides reprĂ©sentent une stratĂ©gie alternative potentiellement intĂ©ressante pour la gestion des mauvaises herbes. Si utilisĂ©es de façon adĂ©quate, elles peuvent promouvoir l'utilisation d'herbicides moins dommageables pour l'environnement que ceux qu'ils remplacent, et ainsi procurer aux producteurs des moyens supplĂ©mentaires de lutte contre les mauvaises herbes. Cependant, la controverse entourant le dĂ©veloppement et l'utilisation de ces cultivars peut limiter et Ă©ventuellement empĂȘcher leur adoption sur une grande Ă©chelle. Les prĂ©occupations comprennent: la surutilisation d'herbicides, la transmission de gĂšnes de rĂ©sistance entre les cultivars rĂ©sistants et les mauvaises herbes qui leur sont apparentĂ©es, le risque que les modifications gĂ©nĂ©tiques pour la rĂ©sistance confĂšrent des caractĂšres nuisibles au cultivar (Le. plantes spontanĂ©es dans des cultures subsĂ©quentes), les effets plĂ©iotropiques potentiels des modifications gĂ©nĂ©tiques pour la rĂ©sistance, et finalement, la sĂ©lection de nouvelles mauvaises herbes rĂ©sistantes aux herbicides dans ce nouveau rĂ©gime d'herbicides. Parmi ces prĂ©occupations, c'est la propabilitĂ© de sĂ©lectionner de nouvelles mauvaises herbes rĂ©sistantes qui peut avoir le plus de chances d'affecter le succĂšs Ă long terme des cultures rĂ©sistantes aux herbicides.Herbicide-resistant crops offer a potentially valuable alternative strategy for weed management. If used appropriately, they may promote the use of agrichemicals more environmentally benign than the herbicides they replace, and provide producers with additional tools for controlling weeds. However, the controversy surrounding the development and use of these cultivars may limit and eventually prevent their widespread adoption. Concerns include: overuse of herbicides, escape of herbicide resistance genes from resistant cultivars into weedy relatives, genetic modifications for resistance conferring weediness to the cultivar (i.e. volunteer plants insubsequent crops), potential pleiotropic effects of genetic modifications for resistance, and selection of new herbicide-resistant weeds in the new herbicide regime. Of these concerns, the potential for selecting new resistant weeds may have the highest likelihood of affecting the long-term success of herbicide-resistant crops
Large Scale Structures in Kinetic Gravity Braiding Model That Can Be Unbraided
We study cosmological consequences of a kinetic gravity braiding model, which
is proposed as an alternative to the dark energy model. The kinetic braiding
model we study is characterized by a parameter n, which corresponds to the
original galileon cosmological model for n=1. We find that the background
expansion of the universe of the kinetic braiding model is the same as the
Dvali-Turner's model, which reduces to that of the standard cold dark matter
model with a cosmological constant (LCDM model) for n equal to infinity. We
also find that the evolution of the linear cosmological perturbation in the
kinetic braiding model reduces to that of the LCDM model for n=\infty. Then, we
focus our study on the growth history of the linear density perturbation as
well as the spherical collapse in the nonlinear regime of the density
perturbations, which might be important in order to distinguish between the
kinetic braiding model and the LCDM model when n is finite. The theoretical
prediction for the large scale structure is confronted with the multipole power
spectrum of the luminous red galaxy sample of the Sloan Digital Sky survey. We
also discuss future prospects of constraining the kinetic braiding model using
a future redshift survey like the WFMOS/SuMIRe PFS survey as well as the
cluster redshift distribution in the South Pole Telescope survey.Comment: 41 pages, 20 figures; This version was accepted for publication in
JCA
Measurement of the p-pbar -> Wgamma + X cross section at sqrt(s) = 1.96 TeV and WWgamma anomalous coupling limits
The WWgamma triple gauge boson coupling parameters are studied using p-pbar
-> l nu gamma + X (l = e,mu) events at sqrt(s) = 1.96 TeV. The data were
collected with the DO detector from an integrated luminosity of 162 pb^{-1}
delivered by the Fermilab Tevatron Collider. The cross section times branching
fraction for p-pbar -> W(gamma) + X -> l nu gamma + X with E_T^{gamma} > 8 GeV
and Delta R_{l gamma} > 0.7 is 14.8 +/- 1.6 (stat) +/- 1.0 (syst) +/- 1.0 (lum)
pb. The one-dimensional 95% confidence level limits on anomalous couplings are
-0.88 < Delta kappa_{gamma} < 0.96 and -0.20 < lambda_{gamma} < 0.20.Comment: Submitted to Phys. Rev. D Rapid Communication
Measurement of the ttbar Production Cross Section in ppbar Collisions at sqrt{s} = 1.96 TeV using Kinematic Characteristics of Lepton + Jets Events
We present a measurement of the top quark pair ttbar production cross section
in ppbar collisions at a center-of-mass energy of 1.96 TeV using 230 pb**{-1}
of data collected by the DO detector at the Fermilab Tevatron Collider. We
select events with one charged lepton (electron or muon), large missing
transverse energy, and at least four jets, and extract the ttbar content of the
sample based on the kinematic characteristics of the events. For a top quark
mass of 175 GeV, we measure sigma(ttbar) = 6.7 {+1.4-1.3} (stat) {+1.6- 1.1}
(syst) +/-0.4 (lumi) pb, in good agreement with the standard model prediction.Comment: submitted to Phys.Rev.Let
Measurement of the ttbar Production Cross Section in ppbar Collisions at sqrt(s)=1.96 TeV using Lepton + Jets Events with Lifetime b-tagging
We present a measurement of the top quark pair () production cross
section () in collisions at TeV
using 230 pb of data collected by the D0 experiment at the Fermilab
Tevatron Collider. We select events with one charged lepton (electron or muon),
missing transverse energy, and jets in the final state. We employ
lifetime-based b-jet identification techniques to further enhance the
purity of the selected sample. For a top quark mass of 175 GeV, we
measure pb, in
agreement with the standard model expectation.Comment: 7 pages, 2 figures, 3 tables Submitted to Phys.Rev.Let
Search for W' bosons decaying to an electron and a neutrino with the D0 detector
This Letter describes the search for a new heavy charged gauge boson W'
decaying into an electron and a neutrino. The data were collected with the D0
detector at the Fermilab Tevatron proton-antiproton Collider at a
center-of-mass energy of 1.96 TeV, and correspond to an integrated luminosity
of about 1 inverse femtobarn. Lacking any significant excess in the data in
comparison with known processes, an upper limit is set on the production cross
section times branching fraction, and a W' boson with mass below 1.00 TeV can
be excluded at the 95% C.L., assuming standard-model-like couplings to
fermions. This result significantly improves upon previous limits, and is the
most stringent to date.Comment: submitted to Phys. Rev. Let
Search for a scalar or vector particle decaying into Zgamma in ppbar collisions at sqrt(s) = 1.96 TeV
We present a search for a narrow scalar or vector resonance decaying into
Zgamma with a subsequent Z decay into a pair of electrons or muons. The data
for this search were collected with the D0 detector at the Fermilab Tevatron
ppbar collider at a center of mass energy sqrt(s) = 1.96 TeV. Using 1.1 (1.0)
fb-1 of data, we observe 49 (50) candidate events in the electron (muon)
channel, in good agreement with the standard model prediction. From the
combination of both channels, we derive 95% C.L. upper limits on the cross
section times branching fraction (sigma x B) into Zgamma. These limits range
from 0.19 (0.20) pb for a scalar (vector) resonance mass of 600 GeV/c^2 to 2.5
(3.1) pb for a mass of 140 GeV/c^2.Comment: Published by Phys. Lett.
Measurement of the ratios of the Z/G* + >= n jet production cross sections to the total inclusive Z/G* cross section in ppbar collisions at sqrt(s) = 1.96 TeV
We present a study of events with Z bosons and jets produced at the Fermilab
Tevatron Collider in ppbar collisions at a center of mass energy of 1.96 TeV.
The data sample consists of nearly 14,000 Z/G* -> e+e- candidates corresponding
to the integrated luminosity of 0.4 fb-1 collected using the D0 detector.
Ratios of the Z/G* + >= n jet cross sections to the total inclusive Z/G* cross
section have been measured for n = 1 to 4 jet events. Our measurements are
found to be in good agreement with a next-to-leading order QCD calculation and
with a tree-level QCD prediction with parton shower simulation and
hadronization.Comment: 7 pages, 2 figures, slightly modified, submitted to Phys. Lett.
Ant species distribution along a topographic gradient in a "terra-firme" forest reserve in Central Amazonia
Measurement of the Isolated Photon Cross Section in p-pbar Collisions at sqrt{s}=1.96 TeV
The cross section for the inclusive production of isolated photons has been
measured in p anti-p collisions at sqrt{s}=1.96 TeV with the D0 detector at the
Fermilab Tevatron Collider. The photons span transverse momenta 23 to 300 GeV
and have pseudorapidity |eta|<0.9. The cross section is compared with the
results from two next-to-leading order perturbative QCD calculations. The
theoretical predictions agree with the measurement within uncertainties.Comment: 7 pages, 5 figures, submitted to Phys.Lett.
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