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1996, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
DELPHI (DEtector with Lepton, Photon and Hadron Identification) is a detector for e+e-physics, designed to provide high granularity over a 47r solid angle, allowing an effective particle identification. It has been operating at the LEP (Large Electron-Positron) collider at CERN since 1989. This article reviews its performance.
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 1991
The measurement of the moments of hadronic mass spectrum and of lepton energy spectrum based on a sample of semileptonic decays of the b hadron selected from Z 0 → b b events recorded with the Delphi detector at LEP, are presented. These results are interpreted in terms of constraints on the quark masses and on the b-quark kinetic energy value.
A search for excited leptons with the DELPHI detector at LEP is reported. The data analysed correspond to an integrated luminosity of about 539 pb −1 collected at centre-of-mass energies ranging from 189 GeV to 208 GeV. The search for pairproduced excited leptons establishes 95% confidence level mass limits in the region between 95 GeV/c 2 and 103 GeV/c 2 , depending on the channel. The search for singly produced excited leptons establishes upper limits on the ratio of the coupling of the excited lepton to its mass (λ/m * ) as a function of the mass.
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 1995
The general purpose particle detector DELPHI at the Large Electron Positron collider at CERN was built to give the complete information of each event. DELPHI uses ring imaging Cherenkov counters to provide hadron identification in most of the momentum range below 40 GeV/c and over almost the full solid angle. Charged particles traversing gaseous and liquid fluorocarbon radiators create photons used for Cherenkov angle reconstruction. Some of the design features of the detector will be presented, with emphasis on the experience which was gained in the operation of these large systems. The hadron identification power of the ring imaging Cherenkov detector closely meets the main design values. Data processing and performance of the detector will be discussed using dimuon events collected during 1994. Pion rejection factors for kaon tagging will be shown.
IEEE Transactions on Nuclear Science, 1993
One quarter of the Forward Ring Imaging Cherenkov detector is installed and has been operated in the DELPHI experiment. The detector covers the forward-backward regions (15°<8@<35°). Two radiator systems are used for particle identification in the momentum range up to 40 GeV/c, a liquid Perfluorohexane and the Perfluorobutane gas. UV-photons with wave lenghts from ~170 nm to ~200 nm (7.3-6.2eV) are detected with high efficiency. The total active area of the photon detector is ~8m2.
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 1995
The ring imaging Cherenkov detector in the DELPHI Experiment at LEP allows hadron identification over a momentum range up to about 40 Gev/c over a near to 4rr solid angle. Photons emitted by charged particles traversing gas and liquid radiators which are filled with UV-transparent perfluorocarbons, are used for Cherenkov angle reconstruction. Stable operation ensures that the detector is an efficient and powerful instrument. Monitoring of the detector parameters is of utmost importance to achieve good data quality and adequate data processing. The hadron identifying power of the ring imaging Cherenkov detector closely meets the main design values. Computerized control and monitoring features of the different subsystems will be presented. The interplay between detector parameters and the particle separating capacity of the detector will be discussed.
The European Physical Journal C, 2004
Hadronic event shape distributions are determined from data in e + e -collisions between 183 and 207 GeV. From these the strong coupling α s is extracted in O(α 2 s ), NLLA and matched O(α 2 s )+NLLA theory. Hadronisation corrections evaluated with fragmentation model generators as well as an analytical power ansatz are applied. Comparing these measurements to those obtained at and around M Z allows a combined measurement of α s from all DELPHI data and a test of the energy dependence of the strong coupling.
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 1994
The ring imaging Cherenkov detector system in the DELPHI experiment at the Large Electron-Positron storage ring at CERN, is designed to do particle identification over most of the solid angle in the momentum range from -2 GeV/c to -40 GeV/c. Two radiator media are used to cover the momentum range; (i) a 1 cm layer of liquid C6 F14 , and (ii) a volume filled with gaseous CSFi2 or C4F lo . Photosensitive time projection chambers record the conversion points of the ultraviolet photons produced in both radiator systems. The total active area is -30 mz in the barrel region and -8 mZ m the two endcaps.
The European Physical Journal C - Particles and Fields, 2004
Final results from the DELPHI Collaboration on the lifetime of B + and B 0 mesons and the mean b-hadron lifetime, are presented using the data collected at the Z 0 peak in 1994 and 1995. Elaborate, inclusive, secondary vertexing methods have been employed to ensure a b-hadron reconstruction with good efficiency. To separate samples of B + and B 0 mesons, high performance neural network techniques are used that achieve very high purity signals. The results obtained are:
The European Physical Journal C, 2005
Measurement of the energy dependence of hadronic jet rates and the strong coupling α s from the four-jet rate with the DELPHI detector at LEP
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