109 research outputs found

    Search for neutral heavy leptons produced in ZZ decays

    Get PDF
    Weak isosinglet Neutral Heavy Leptons (νm) have been searched for using data collected by the DELPHI detector corresponding to 3.3 × 106 hadronic Z0 decays at LEP1. Four separate searches have been performed, for short-lived νm production giving monojet or acollinear jet topologies, and for long-lived νm giving detectable secondary vertices or calorimeter clusters. No indication of the existence of these particles has been found, leading to an upper limit for the branching ratio BR(Z0 → νmν̄) of about 1.3 × 10-6 at 95% confidence level for νm masses between 3.5 and 50 GeV/c2. Outside this range the limit weakens rapidly with the νm mass. The results are also interpreted in terms of limits for the single production of excited neutrinos. © Springer-Verlag 1997

    Linking quality assurance and quality of care

    No full text

    The DELPHI Detector (DEtector with Lepton Photon and Hadron Identification)

    No full text
    % DELPHI The DELPHI Detector (Detector with Lepton Photon and Hadron Identification) \\ \\DELPHI is a general purpose detector for physics at LEP on and above the Z0^0, offering three-dimensional information on curvature and energy deposition with fine spatial granularity as well as identification of leptons and hadrons over most of the solid angle. A superconducting coil provides a 1.2~T solenoidal field of high uniformity. Tracking relies on the silicon vertex detector, the inner detector, the Time Projection Chamber (TPC), the outer detector and forward drift chambers. Electromagnetic showers are measured in the barrel with high granularity by the High Density Projection Chamber (HPC) and in the endcaps by 10 1 ^0 ~x~10 1 ^0 projective towers composed of lead glass as active material and phototriode read-out. Hadron identification is provided mainly by liquid and gas Ring Imaging Counters (RICH). The instrumented magnet yoke serves for hadron calorimetry and as filter for muons, which are identified in two drift chamber layers. In addition, scintillator systems are implemented in the barrel and forward regions, as well as a Scintillation TIle Calorimeter (STIC) and a Very Small Angle Tagger (VSAT) for luminosity determination, a 3-layer micro vertex silicon detector for high precision vertex and lifetime measurements and a very Forward Silicon Tracker (VFT) for improved tracking and hermeticity at small polar angles
    corecore