118617754
Search for low mass Higgs at the Tevatron (ZH and H to gamma gamma)
17003556
Observation of exclusive electron-positron production in hadron-hadron collisions.
We present the first observation of exclusive e(+)e(-) production in hadron-hadron collisions, using pp[over] collision data at (square root) s = 1.96 TeV taken by the run II Collider Detector at Fermilab, and corresponding to an integrated luminosity of 532 pb(-1). We require the absence of any particle signatures in the detector except for an electron and a positron candidate, each with transverse energy E(T) > 5 GeV and pseudorapidity |eta| < 2. With these criteria, 16 events are observed compared to a background expectation of 1.9+/-0.3 events. These events are consistent in cross section and properties with the QED process pp[over] --> p + e(+)e(-) + p[over] through two-photon exchange. The measured cross section is 1.6(-0.3)(+0.5)(stat) +/- 0.3(syst) pb. This agrees with the theoretical prediction of 1.71+/-0.01 pb.
18284543
Measurement of the top pair production cross section in the lepton+jets channel using a jet flavor discriminant
We present a new method to measure the top quark pair production cross section and the background rates with data corresponding to an integrated luminosity of 2.7  fb-1 from pp collisions at √s=1.96  TeV collected with the CDF II Detector. We select events with a single electron or muon candidate, missing transverse energy, and at least one b-tagged jet. We perform a simultaneous fit to a jet flavor discriminant across nine samples defined by the number of jets and b tags. An advantage of this approach is that many systematic uncertainties are measured in situ and inversely scale with integrated luminosity. We measure a top cross section of σtt =7.64±0.57(stat+syst)±0.45(luminosity)  pb.
36027906
Search for Higgs bosons predicted in two-Higgs-doublet models via decays to tau lepton pairs in 1.96 TeV pp collisions.
We present the results of a search for Higgs bosons predicted in two-Higgs-doublet models, in the case where the Higgs bosons decay to tau lepton pairs, using 1.8 fb(-1) of integrated luminosity of pp collisions recorded by the CDF II experiment at the Fermilab Tevatron. Studying the mass distribution in events where one or both tau leptons decay leptonically, no evidence for a Higgs boson signal is observed. The result is used to infer exclusion limits in the two-dimensional space of tanbeta versus m(A) (the ratio of the vacuum expectation values of the two Higgs doublets and the mass of the pseudoscalar boson, respectively).
60626146
ILC Reference Design Report: ILC Global Design Effort and World Wide Study
40926063
First simultaneous measurement of the top quark mass in the lepton + jets and dilepton channels at CDF
We present a measurement of the mass of the top quark using data corresponding to an integrated luminosity of 1.9 fb{sup -1} of pp collisions collected at {radical}(s)=1.96 TeV with the CDF II detector at Fermilab's Tevatron. This is the first measurement of the top quark mass using top-antitop pair candidate events in the lepton+jets and dilepton decay channels simultaneously. We reconstruct two observables in each channel and use a nonparametric kernel density estimation technique to derive two-dimensional probability density functions from simulated signal and background samples. The observables are the top quark mass and the invariant mass of two jets from the W decay in the lepton+jets channel, and the top quark mass and the scalar sum of transverse energy of the event in the dilepton channel. We perform a simultaneous fit for the top quark mass and the jet energy scale, which is constrained in situ by the hadronic W boson mass. Using 332 lepton+jets candidate events and 144 dilepton candidate events, we measure the top quark mass to be M{sub top}=171.9{+-}1.7(stat+JES){+-}1.1(other syst) GeV/c{sup 2}=171.9{+-}2.0 GeV/c{sup 2}.
201932480
Commissioning of the CMS Detector
The Compact Muon Solenoid 1 (CMS) is one of the four experiments operating at the CERN Large Hadron Collider (LHC). A schematic view of the detector is shown in Fig. 1. The tracking system is made of a pixel detector close to the beam pipe surrounded by a silicon strip detector: its high granularity (70 millions pixels, 10 millions strips) and precision ensures good track reconstruction efficiency. It is placed inside a 3.8T superconducting solenoid together with the electromagnetic calorimeter (ECAL), made of lead tungstate crystals, and the brass-scintillator sampling hadronic calorimeter (HCAL). Forward sampling calorimeters increase the pseudorapidity coverage up to |η| ≤ 5. The magnet return yoke is instrumented with 4 stations of muon chambers: Drift Tubes (DT) in the barrel region, Cathode Strip Chambers (CSC) in the endcap, Resistive Plate Chambers (RPC), providing a better time resolution, in both; they cover most of the 4π solid angle.