Women with TT genotype for eNOS gene are more responsive in lowering blood pressure in response to exercise

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Measurement of the tt̄ production cross section in pp̄ collisions at √s = 1.96 TeV in dilepton final states

We present a measurement of the top quark pair (tt̄) production cross section in pp̄ collisions at √s=1.96 TeV using events with two charged leptons in the final state. This analysis utilizes an integrated luminosity of 224-243 pb-1 collected with the DØ detector at the Fermilab Tevatron Collider. We observe 13 events in the e+e -, eμ and μ+μ- channels with an expected background of 3.2±0.7 events. For a top quark mass of 175 GeV, we measure a tt̄ production cross section of σtt̄=8. 6-2.7 +3.2(stat)±1.1(syst)±0.6(lumi) pb, consistent with the standard model prediction. © 2005 Elsevier B.V. All rights reserved.

Measurement of the tt̄ production cross section in the τ+jets channel in pp collisions at √s = 7 TeV

The top-quark pair production cross section in 7 TeV center-of-mass energy proton-proton collisions is measured using data collected by the CMS detector at the LHC. The measurement uses events with one jet identified as a hadronically decaying τ lepton and at least four additional energetic jets, at least one of which is identified as coming from a b quark. The analyzed data sample corresponds to an integrated luminosity of 3.9 fb-1 recorded by a dedicated multijet plus hadronically decaying τ trigger. A neural network has been developed to separate the top-quark pairs from the W+jets and multijet backgrounds. The measured value of σtt̄= 152 ± 12,(stat.) ± 32,(syst.) ±,(lum.) pb is consistent with the standard model predictions. © 2013 CERN for the benefit of the CMS collaboration.

Search for Z′ resonances decaying to tt̄ in dilepton+jets final states in pp collisions at √s=7 TeV

A search for resonances decaying to top quark-antiquark pairs is performed using a dilepton+jets data sample recorded by the CMS experiment at the LHC in pp collisions at √s=7 TeV corresponding to an integrated luminosity of 5.0 fb-1. No significant deviations from the standard model background are observed. Upper limits are presented for the production cross section times branching fraction of top quark-antiquark resonances for masses from 750 to 3000 GeV. In particular, the existence of a leptophobic topcolor particle Z′ is excluded at the 95% confidence level for resonance masses MZ ′<1.3 TeV for ΓZ′=0.012MZ ′, and M<1.9 TeV for ΓZ′=0.10MZ ′. © 2013 CERN.

Measurement of masses in the tt̄ system by kinematic endpoints in pp collisions at √s = 7 TeV

A simultaneous measurement of the top-quark, W-boson, and neutrino masses is reported for tt̄ events selected in the dilepton final state from a data sample corresponding to an integrated luminosity of 5.0 fb-1 collected by the CMS experiment in pp collisions at √s = 7 TeV. The analysis is based on endpoint determinations in kinematic distributions. When the neutrino and W-boson masses are constrained to their world-average values, a top-quark mass value of Mt = 173.9 ± 0.9 (stat)+1.7 -2.1(syst.) GeV is obtained. When such constraints are not used, the three particle masses are obtained in a simultaneous fit. In this unconstrained mode the study serves as a test of mass determination methods that may be used in beyond standard model physics scenarios where several masses in a decay chain may be unknown and undetected particles lead to underconstrained kinematics. © 2013 CERN for the benefit of the CMS collaboration.

Measurement of the differential cross section of tt pairs in pp collision at sqrt(s) = 7TeV with the ATLAS detector at the LHC

In this thesis three measurements of top-antitop differential cross section at an energy in the center of mass of 7 TeV will be shown, as a function of the transverse momentum, the mass and the rapidity of the top-antitop system. The analysis has been carried over a data sample of about 5/fb recorded with the ATLAS detector. The events have been selected with a cut based approach in the "one lepton plus jets" channel, where the lepton can be either an electron or a muon. The most relevant backgrounds (multi-jet QCD and W+jets) have been extracted using data driven methods; the others (Z+ jets, diboson and single top) have been simulated with Monte Carlo techniques. The final, background-subtracted, distributions have been corrected, using unfolding methods, for the detector and selection effects. At the end, the results have been compared with the theoretical predictions. The measurements are dominated by the systematic uncertainties and show no relevant deviation from the Standard Model predictions.

Misura della sezione d'urto di produzione tt-barra nel canale adronico in collisioni pp con radice di s = 8tev a cms

La sezione d'urto di produzione per coppie tt-barra viene misurata utilizzando dati raccolti dall'esperimento CMS in collisioni protone-protone ad LHC, con energia nel sistema del centro di massa radice di s = 8 TeV. Il campione raccolto corrisponde ad una luminosità integrata di 19.5 fb^-1. La misura viene effettuata su eventi che contano un numero di jet pari o superiore a 6, almeno due dei quali identificati come prodotto dell'adronizzazione di quark bottom. Il valore di sezione d'urto ottenuto è (260 pm 10 (stat)) pb, in accordo con le previsioni teoriche del Modello Standard.

Measurement of tt ̄production cross section at 13 TeV in the fully-hadronic channel with CMS

Lo scopo di questa tesi è la misura di sezione d’urto di produzione di coppie top-antitop nel canale adronico. Per la misura sono stati utilizzati i dati raccolti dall’esperimento CMS in collisioni protone-protone ad LHC, con un’energia nel centro di massa pari a 13 TeV. Il campione di dati utilizzato corrisponde ad una luminosità integrata di 2.474 f b^ −1 . L’analisi dati inizia selezionando gli eventi che soddisfano determinate condizioni (e.g. trigger, tagli cinematici, sei o più jet, almeno 2 jet provenienti dall’adronizzazione di due quark bottom) con lo scopo di incrementare la purezza del segnale scartando il più possibile gli eventi di fondo. A seguire, viene ricostruita la massa del quark top usando un fit cinematico. Sulle distribuzioni di tale massa si basa la stima degli eventi di fondo e di segnale. Infine, attraverso un fit di verosimiglianza, si ottiene il valore della sezione d’urto: σ t t ̄ = 893 ± 57 (stat) ± 104 (syst) pb. Questo risultato è in buon accordo con il valore teorico di 832 pb e con altre misure di CMS effettuate in canali differenti.