Search for direct production of charginos and neutralinos in events with three leptons and missing transverse momentum in √s = 7 TeV pp collisions with the ATLAS detector

A search for the direct production of charginos and neutralinos in final states with three electrons or muons and missing transverse momentum is presented. The analysis is based on 4.7 fb−1 of proton–proton collision data delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in three signal regions that are either depleted or enriched in Z-boson decays. Upper limits at 95% confidence level are set in R-parity conserving phenomenological minimal supersymmetric models and in simplified models, significantly extending previous results

Jet size dependence of single jet suppression in lead-lead collisions at sqrt(s(NN)) = 2.76 TeV with the ATLAS detector at the LHC

Measurements of inclusive jet suppression in heavy ion collisions at the LHC provide direct sensitivity to the physics of jet quenching. In a sample of lead-lead collisions at sqrt(s) = 2.76 TeV corresponding to an integrated luminosity of approximately 7 inverse microbarns, ATLAS has measured jets with a calorimeter over the pseudorapidity interval |eta| < 2.1 and over the transverse momentum range 38 < pT < 210 GeV. Jets were reconstructed using the anti-kt algorithm with values for the distance parameter that determines the nominal jet radius of R = 0.2, 0.3, 0.4 and 0.5. The centrality dependence of the jet yield is characterized by the jet "central-to-peripheral ratio," Rcp. Jet production is found to be suppressed by approximately a factor of two in the 10% most central collisions relative to peripheral collisions. Rcp varies smoothly with centrality as characterized by the number of participating nucleons. The observed suppression is only weakly dependent on jet radius and transverse momentum. These results provide the first direct measurement of inclusive jet suppression in heavy ion collisions and complement previous measurements of dijet transverse energy imbalance at the LHC.Comment: 15 pages plus author list (30 pages total), 8 figures, 2 tables, submitted to Physics Letters B. All figures including auxiliary figures are available at http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HION-2011-02

Perfil sanguíneo e peso de órgãos internos de bezerros leiteiros criados em diferentes sistemas de aleitamento

Objetivou-se avaliar o perfil sanguíneo e o tamanho absoluto e relativo dos órgãos internos de bezerros em sistema de aleitamento convencional ou fracionado. Foram utilizadas 10 fêmeas, com peso corporal inicial médio de 37,53 kg (±2,36) e 12 machos com peso corporal médio de 81,6 kg (±8,6), ambos da raça Holandesa. O aleitamento convencional constituiu-se de quatro litros de leite fornecidos diariamente durante 54 dias de avaliação e o fracionado, de seis litros do 6º ao 25º dias de idade, quatro litros do 26º ao 45º dias de idade e dois litros do 46º ao 59º dias de idade, além de concentrado, feno de Cynodon sp., água e suplemento mineral fornecidos ad libitum. O delineamento experimental foi inteiramente ao acaso, com cinco repetições para os parâmetros sanguíneos e seis repetições para o desenvolvimento dos órgãos internos. As coletas de sangue foram realizadas nas fêmeas nos dias sete, 21, 28, 42, 49 e 56 de idade. Para a avaliação dos órgãos internos os machos foram abatidos aos dois meses de idade, após jejum de 16 horas. Não foram observadas diferenças para os valores de proteínas totais, albumina, globulina, creatinina, ureia, colesterol e β-hidroxibutirato nas idades avaliadas (p>0,05). Entretanto, para a concentração de glicose houve interação entre os sistemas de aleitamento e os períodos avaliados, podendo ser observado que com 21 dias de idade a concentração foi maior nas bezerras mantidas em sistema fracionado, quando comparadas aos animais do grupo convencional. O sistema de aleitamento não alterou o peso corporal final, peso corporal final vazio e o peso dos órgãos internos, exceto para o coração, demonstrando que o sistema de aleitamento fracionado não altera as avaliações dos órgãos internos

Measurement of the View the tt production cross-section using eμ events with b-tagged jets in pp collisions at √s = 13 TeV with the ATLAS detector

This paper describes a measurement of the inclusive top quark pair production cross-section (σtt¯) with a data sample of 3.2 fb−1 of proton–proton collisions at a centre-of-mass energy of √s = 13 TeV, collected in 2015 by the ATLAS detector at the LHC. This measurement uses events with an opposite-charge electron–muon pair in the final state. Jets containing b-quarks are tagged using an algorithm based on track impact parameters and reconstructed secondary vertices. The numbers of events with exactly one and exactly two b-tagged jets are counted and used to determine simultaneously σtt¯ and the efficiency to reconstruct and b-tag a jet from a top quark decay, thereby minimising the associated systematic uncertainties. The cross-section is measured to be: σtt¯ = 818 ± 8 (stat) ± 27 (syst) ± 19 (lumi) ± 12 (beam) pb, where the four uncertainties arise from data statistics, experimental and theoretical systematic effects, the integrated luminosity and the LHC beam energy, giving a total relative uncertainty of 4.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. A fiducial measurement corresponding to the experimental acceptance of the leptons is also presented

Search for dark matter produced in association with a hadronically decaying vector boson in pp collisions at sqrt (s) = 13 TeV with the ATLAS detector

A search is presented for dark matter produced in association with a hadronically decaying W or Z boson using 3.2 fb−1 of pp collisions at View the MathML sources=13 TeV recorded by the ATLAS detector at the Large Hadron Collider. Events with a hadronic jet compatible with a W or Z boson and with large missing transverse momentum are analysed. The data are consistent with the Standard Model predictions and are interpreted in terms of both an effective field theory and a simplified model containing dark matter