Função ovariana de novilhas Nelore alimentadas com dieta suplementada com gordura protegida ruminal

O objetivo deste trabalho foi avaliar o efeito da suplementação alimentar com gordura protegida ruminal sobre as estruturas ovarianas e sobre a concentração sérica de progesterona, em novilhas Nelore mantidas em pasto. Quarenta novilhas foram divididas em dois grupos: um suplementado com gordura protegida Megalac-E (G); e outro sem suplementação de gordura (C). O grupos foram avaliados em delineamento "crossover". Utilizaram-se dietas isoenergéticas e isoproteicas. Após 15 dias de suplementação, os animais foram submetidos a um protocolo hormonal, para avaliação da influência da suplementação com gordura no metabolismo da progesterona. Para isto, em um dia aleatório do ciclo (D0), inseriu-se um implante intravaginal de liberação de progesterona (CIDR), e aplicou-se prostaglandina F2α (PGF2α, i.m.). No D7, o implante foi retirado, e outra aplicaηão de PGF2α foi realizada. No D18, foi feita uma nova aplicaηão de PGF2α e, então, foram observados diariamente os exames ultrassonográficos ovarianos e a ocorrência de estro. Para o ensaio com progesterona, colheu-se sangue 4 dias após a inserção do implante e, novamente, 7 e 14 dias após a ovulação. A concentração de progesterona sérica no D4 foi maior no grupo G. Não houve diferença nas concentrações séricas de progesterona 7 e 14 dias após a ovulação, nem no diâmetro do folículo ovulatório, nem no volume luteal. A suplementação com Megalac-E altera o metabolismo de progesterona, mas não altera a função ovariana em novilhas zebuínas em pasto.The objective of this work was to evaluate the effect of rumen-protected fat supplementation on ovarian structures and on serum progesterone concentration in Nelore heifers kept in pasture. Forty heifers were divided into two groups: one supplemented with rumen-protected fat Megalac-E (F); and another without fat supplement (C). The groups were evaluated in a crossover design. The diets were isocaloric and isoproteic. After 15 days of supplementation, the animals were submitted to a hormonal protocol to evaluate the influence of fat supplementation on progesterone metabolism. For this, on a random day of the cycle (D0), the heifers received an intravaginal progesterone-releasing device (CIDR) and an injection of prostaglandin F2α (PGF2α, im). On D7, CIDR was removed and another injection of PGF2α was performed. On D18, a new treatment with PGF2α was done and, then, daily observations of estrus and ovarian ultrasound exams were carried out. For progesterone assay, blood samples were collected 4 days after CIDR insertion, and 7 and 14 days following ovulation. Serum progesterone concentration on D4 was higher for Group F. There was no difference between groups for serum progesterone concentration at 7 or 14 days following ovulation, neither in the ovulatory follicle, nor in the corpus luteum volume. Supplementation with Megalac-E alters progesterone metabolism, but does not affect ovarian function in zebu heifers kept in pasture

Measurement of the total cross section and ρ -parameter from elastic scattering in pp collisions at √s=13 TeV with the ATLAS detector

In a special run of the LHC with β⋆=2.5 km, proton–proton elastic-scattering events were recorded at s√=13 TeV with an integrated luminosity of 340 μb−1 using the ALFA subdetector of ATLAS in 2016. The elastic cross section was measured differentially in the Mandelstam t variable in the range from −t=2.5⋅10−4 GeV2 to −t=0.46 GeV2 using 6.9 million elastic-scattering candidates. This paper presents measurements of the total cross section σtot, parameters of the nuclear slope, and the ρ-parameter defined as the ratio of the real part to the imaginary part of the elastic-scattering amplitude in the limit t→0. These parameters are determined from a fit to the differential elastic cross section using the optical theorem and different parameterizations of the t-dependence. The results for σtot and ρ are σtot(pp→X)=104.7±1.1 mb ,ρ=0.098±0.011. The uncertainty in σtot is dominated by the luminosity measurement, and in ρ by imperfect knowledge of the detector alignment and by modelling of the nuclear amplitude.publishedVersio

Charged-hadron production in pp, p+Pb, Pb+Pb, and Xe+Xe collisions at sNN−−−√ = 5 TeV with the ATLAS detector at the LHC

This paper presents measurements of charged-hadron spectra obtained in pp, p+Pb, and Pb+Pb collisions at s√ or sNN−−−√ = 5.02 TeV, and in Xe+Xe collisions at sNN−−−√ = 5.44 TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25 pb−1, 28 nb−1, 0.50 nb−1, and 3 μb−1, respectively. The nuclear modification factors RpPb and RAA are obtained by comparing the spectra in heavy-ion and pp collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor RpPb shows a moderate enhancement above unity with a maximum at pT ≈ 3 GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct pT-dependence with a local maximum at pT ≈ 2 GeV and a local minimum at pT ≈ 7 GeV. This dependence is more distinguishable in more central collisions. No significant |η|-dependence is found. A comprehensive comparison with several theoretical predictions is also provided. They typically describe RAA better in central collisions and in the pT range from about 10 to 100 GeV

Evidence of off-shell Higgs boson production from ZZ leptonic decay channels and constraints on its total width with the ATLAS detector

This Letter reports on a search for off-shell production of the Higgs boson using 139 fb−1 of pp collision data at √s = 13 TeV collected by the ATLAS detector at the Large Hadron Collider. The signature is a pair of Z bosons, with contributions from both the production and subsequent decay of a virtual Higgs boson and the interference of that process with other processes. The two observable final states are Z Z → 4 and Z Z → 22ν with = e or μ. In the Z Z → 4 final state, a dense Neural Network is used to enhance analysis sensitivity with respect to matrix element-based discrimination. The backgroundonly hypothesis is rejected with an observed (expected) significance of 3.3 (2.2) standard deviations, representing experimental evidence for off-shell Higgs boson production. Assuming that no new particles enter the production of the virtual Higgs boson, its total width can be deduced from the measurement of its off-shell production cross-section. The measured total width of the Higgs boson is 4.5+3.3 −2.5 MeV, and the observed (expected) upper limit on the total width is found to be 10.5 (10.9) MeV at 95% confidence level

Measurements of Zγ+jets differential cross sections in pp collisions at s√ = 13 TeV with the ATLAS detector

Differential cross-section measurements of Zγ production in association with hadronic jets are presented, using the full 139 fb−1 dataset of s√ = 13 TeV proton–proton collisions collected by the ATLAS detector during Run 2 of the LHC. Distributions are measured using events in which the Z boson decays leptonically and the photon is usually radiated from an initial-state quark. Measurements are made in both one and two observables, including those sensitive to the hard scattering in the event and others which probe additional soft and collinear radiation. Different Standard Model predictions, from both parton-shower Monte Carlo simulation and fixed-order QCD calculations, are compared with the measurements. In general, good agreement is observed between data and predictions from MATRIX and MiNNLOPS, as well as next-to-leading-order predictions from MADGRAPH5_AMC@NLO and SHERPA

Measurement of double-differential charged-current Drell-Yan cross-sections at high transverse masses in pp collisions at √s = 13 TeV with the ATLAS detector

This paper presents a first measurement of the cross-section for the charged-current Drell-Yan process $pp\rightarrow W^{\pm} \rightarrow \ell^{\pm} \nu$ above the resonance region, where $\ell$ is an electron or muon. The measurement is performed for transverse masses, $m_{\text{T}}^{\text{W}}$, between 200 GeV and 5000 GeV, using a sample of 140 fb$^{-1}$ of $pp$ collision data at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV collected by the ATLAS detector at the LHC during 2015-2018. The data are presented single differentially in transverse mass and double differentially in transverse mass and absolute lepton pseudorapidity. A test of lepton flavour universality shows no significant deviations from the Standard Model. The electron and muon channel measurements are combined to achieve a total experimental precision of 3% at low $m_{\text{T}}^{\text{W}}$. The single- and double differential $W$-boson charge asymmetries are evaluated from the measurements. A comparison to next-to-next-to-leading-order perturbative QCD predictions using several recent parton distribution functions and including next-to-leading-order electroweak effects indicates the potential of the data to constrain parton distribution functions. The data are also used to constrain four fermion operators in the Standard Model Effective Field Theory formalism, in particular the lepton-quark operator Wilson coefficient $c_{\ell q}^{(3)}.