2,395 research outputs found

    Data reconstruction with the LHCb VELO: Hit processing, tracking, vertexing and luminosity monitoring

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    The LHCb experiment is dedicated to performing a detailed study of CP symmetry violation and rare decays of B and D mesons. In order to reach these physics goals the LHCb spectrometer must provide excellent vertexing and tracking performance both off-line and on-line in the trigger. The LHCb VELO (VErtex LOcator) is the silicon microstrip detector which surrounds the collision point and hence is critical to these aims. Its hit processing and zero suppression is performed in a series of algorithms implemented on FPGAs. The tuning of the parameters of these algorithms is performed using a bit-perfect emulation of these algorithms integrated in to the full off-line software of the experiment. Tracking and vertexing is then performed using the clusters produced. These algorithms are described and the results for primary and secondary vertex resolutions are given. Finally, a novel technique for measuring the absolute luminosity using gas injection in the VELO is described

    Description of the Vetra Project and its Application for the VELO Detector

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    Vetra is the LHCb data reconstruction project which emulates the performance of the TELL1 readout board processing algorithms. This project is required for monitoring and commissioning the LHCb silicon detectors. A bit-perfect emulation of the TELL1 processing algorithms is performed. This project allows raw data (non-zero suppressed) to be processed to produce the standard zero suppressed cluster data, used by the LHCb reconstruction project Brunel. The Vetra framework is used by the VELO and ST detectors in LHCb. This note provides a general description of Vetra but concentrates on the VELO usage. Vetra is used to monitor the performance of the detector and the data acquisition board algorithms. The parameters that control the data acquisition boards are determined and optimised using Vetra. The project is used widely in the VELO and is used for testbeam and laboratory tests, including production testing for the modules

    Velo Event Model

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    This note presents the Velo Event Model, it describes the classes and data flow used in the Velo software for all stages up to and including the clusters. The description is provided for the classes used for both the real data and the simulation. This description includes the data classes used during the standard running and simulation of the experiment, and all classes defined for calibration and commissioning

    Testbeam studies of pre-prototype silicon strip sensors for the LHCb UT upgrade project

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    The LHCb experiment is preparing for a major upgrade in 2018-2019. One of the key components in the upgrade is a new silicon tracker situated upstream of the analysis magnet of the experiment. The Upstream Tracker (UT) will consist of four planes of silicon strip detectors, with each plane covering an area of about 2 m2^2. An important consideration of these detectors is their performance after they have been exposed to a large radiation dose. In this article we present test beam results of pre-prototype n-in-p and p-in-n sensors that have been irradiated with fluences up to 4.0×10144.0\times10^{14} neqn_{\rm eq} cm2^{-2}.Comment: 25 pages, 20 figure

    Performance of the LHCb Vertex Detector Alignment Algorithm determined with Beam Test Data

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    LHCb is the dedicated heavy flavour experiment at the Large Hadron Collider at CERN. The partially assembled silicon vertex locator (VELO) of the LHCb experiment has been tested in a beam test. The data from this beam test have been used to determine the performance of the VELO alignment algorithm. The relative alignment of the two silicon sensors in a module and the relative alignment of the modules has been extracted. This alignment is shown to be accurate at a level of approximately 2 micron and 0.1 mrad for translations and rotations, respectively in the plane of the sensors. A single hit precision at normal track incidence of about 10 micron is obtained for the sensors. The alignment of the system is shown to be stable at better than the 10 micron level under air to vacuum pressure changes and mechanical movements of the assembled system.Comment: accepted for publication in NIM

    Testbeam studies of pre-prototype silicon strip sensors for the LHCb UT upgrade project

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    AbstractThe LHCb experiment is preparing for a major upgrade in 2018–2019. One of the key components in the upgrade is a new silicon tracker situated upstream of the analysis magnet of the experiment. The Upstream Tracker (UT) will consist of four planes of silicon strip detectors, with each plane covering an area of about 2m2. An important consideration of these detectors is their performance after they have been exposed to a large radiation dose. In this paper we present test beam results of pre-prototype n-in-p and p-in-n sensors that have been irradiated with fluences up to 4.0×1014neq/cm2

    Radiation damage in the LHCb vertex locator

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    The LHCb Vertex Locator (VELO) is a silicon strip detector designed to reconstruct charged particle trajectories and vertices produced at the LHCb interaction region. During the first two years of data collection, the 84 VELO sensors have been exposed to a range of fluences up to a maximum value of approximately 45 × 1012 1 MeV neutron equivalent (1 MeV neq). At the operational sensor temperature of approximately −7 °C, the average rate of sensor current increase is 18 μA per fb−1, in excellent agreement with predictions. The silicon effective bandgap has been determined using current versus temperature scan data after irradiation, with an average value of Eg = 1.16±0.03±0.04 eV obtained. The first observation of n+-on-n sensor type inversion at the LHC has been made, occurring at a fluence of around 15 × 1012 of 1 MeV neq. The only n+-on-p sensors in use at the LHC have also been studied. With an initial fluence of approximately 3 × 1012 1 MeV neq, a decrease in the Effective Depletion Voltage (EDV) of around 25 V is observed. Following this initial decrease, the EDV increases at a comparable rate to the type inverted n+-on-n type sensors, with rates of (1.43±0.16) × 10−12 V/ 1 MeV neq and (1.35±0.25) × 10−12 V/ 1 MeV neq measured for n+-on-p and n+-on-n type sensors, respectively. A reduction in the charge collection efficiency due to an unexpected effect involving the second metal layer readout lines is observed

    Precision luminosity measurements at LHCb

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    Measuring cross-sections at the LHC requires the luminosity to be determined accurately at each centre-of-mass energy √s. In this paper results are reported from the luminosity calibrations carried out at the LHC interaction point 8 with the LHCb detector for √s = 2.76, 7 and 8 TeV (proton-proton collisions) and for √sNN = 5 TeV (proton-lead collisions). Both the "van der Meer scan" and "beam-gas imaging" luminosity calibration methods were employed. It is observed that the beam density profile cannot always be described by a function that is factorizable in the two transverse coordinates. The introduction of a two-dimensional description of the beams improves significantly the consistency of the results. For proton-proton interactions at √s = 8 TeV a relative precision of the luminosity calibration of 1.47% is obtained using van der Meer scans and 1.43% using beam-gas imaging, resulting in a combined precision of 1.12%. Applying the calibration to the full data set determines the luminosity with a precision of 1.16%. This represents the most precise luminosity measurement achieved so far at a bunched-beam hadron collider
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