Performance of the LHCb RICH detectors during the LHC Run II

The LHCb RICH system provides hadron identification over a wide momentum range (2-100 GeV/c). This detector system is key to LHCb's precision flavour physics programme, which has unique sensitivity to physics beyond the standard model. This paper reports on the performance of the LHCb RICH in Run II, following significant changes in the detector and operating conditions. The changes include the refurbishment of significant number of photon detectors, assembled using new vacuum technologies, and the removal of the aerogel radiator. The start of Run II of the LHC saw the beam energy increase to 6.5 TeV per beam and a new trigger strategy for LHCb with full online detector calibration. The RICH information has also been made available for all trigger streams in the High Level Trigger for the first time.Comment: Updated authors' details and DO

The LHCb RICH Detector Control System

The efficient operation of the two Ring Imaging Cherenkov (RICH) detectors of the LHCb experiment is essential for hadron identification. This operation is achieved by the Detector Control System (DCS) with the integration of the control and monitoring functions of the various subsystems. The DCS controls the various power supplies required for the operation of the Hybrid Photon Detectors (HPDs) and related electronics, collects information about the operating environment of the HPDs to ensure safe operation, and monitors the RICH radiators (pressure, temperature, humidity, gas quality). The system is able to inform the operator or take automatic actions when any monitored quantities go outside predefined safe limits. It is fully integrated in the LHCb Experiment Control System and can apply different configurations using recipes. The LHCb RICH DCS has been fully commissioned and is ready for the LHC start-up

The LHCb RICH Detector Control System

The efficient operation of the two Ring Imaging Cherenkov (RICH) detectors of the LHCb experiment is essential for hadron identification. This operation is achieved by the Detector Control System (DCS) with the integration of the control and monitoring functions of the various subsystems. The DCS controls the various power supplies required for the operation of the Hybrid Photon Detectors (HPDs) and related electronics, collects information about the operating environment of the HPDs to ensure safe operation, and monitors the RICH radiators (pressure, temperature, humidity, gas quality). The system is able to inform the operator or take automatic actions when any monitored quantities go outside predefined safe limits. It is fully integrated in the LHCb Experiment Control System and can apply different configurations using recipes. The LHCb RICH DCS has been fully commissioned and is ready for the LHC start-up

Investigation of the Performance of Microstrip Gas Detectors for X-rays and Evaluation of their Application to Mammography

SIGLEAvailable from British Library Document Supply Centre-DSC:DXN023480 / BLDSC - British Library Document Supply CentreGBUnited Kingdo

A Two-Stage, High Gain Micro-strip Detector

A two stage position-sensitive gas proportional counter has been constructed by tightly coupling a Gas Electron Multiplier (GEM) with a Micro-Groove Detector (MGD). The GEM was used as the first amplifying stage and was optimised to transmit close to 100~\% of the primary charge even at very high drift fields (10~kV/cm). Very narrow GEM--MGD seperations (0--600~$\mu$m) were used so that the active volume of the detector is still very thin (3--3.6~mm) and the required drift field could be maintaine d using an acceptable drift voltage (around 4000~V). Very high combined gains (up to 3~$\times$10$^5$) were obtained with this system. The detector was found to be spark-free in the presence of HIPs (alpha particles) up to gains in excess of 10,000

The Micro-Groove Detector

We introduce the Micro-Groove Detector (MGD), a new type of position-sensitive gas proportional counter produced using advanced printed circuit board (PCB) technology. The MGD is based on a thin kapt on foil, clad with gold-plated copper on both sides. An array of micro-strips at a typical pitch of 200um is defined on the top metal layer. Using as a protection mask the metal left after the patter ning, charge amplifying micro-grooves are etched into the kapton layer. These end on a second micro-strip pattern which is defined on the bottom metal plane. The two arrays of micro-strips can have a n arbitrary relative orientation and so can be used for read-out to obtain 2-D positional information. First results from our systematic assessment of this device are reported: gas gain > 15000, rat e capability above 10^6mm-2s-1, energy resolution 22% at 5.4 keV, no significant charging or aging effects up to 5mC/cm, full primary charge collection efficiency even at high drift fields

The WELL Detector

We introduce the WELL detector, a new type of position-sensitive gas proportional counter produced using advanced printed circuit board (PCB) technology. The WELL is based on a thin kapton foil, copp erclad on both sides. Charge amplifying micro-wells are etched into the first metal and kapton layers. These end on a micro-strip pattern which is defined on the second metal plane. The array of micr o-strips is used for read-out to obtain 1-D positional information. First results from our systematic assessment of this device are reported

Test of the photon detection system for the LHCb RICH Upgrade in a charged particle beam

The LHCb detector will be upgraded to make more efficient use of the available luminosity at the LHC in Run III and extend its potential for discovery. The Ring Imaging Cherenkov detectors are key components of the LHCb detector for particle identification. In this paper we describe the setup and the results of tests in a charged particle beam, carried out to assess prototypes of the upgraded opto-electronic chain from the Multi-Anode PMT photosensor to the readout and data acquisition system.Comment: 25 pages, 22 figure

The CMS Micro-strip Gas Chamber Project: Development of a high resolution tracking detector for harsh radiation environments

Thirty-two large area Micro-Strip Gas Chambers were tested in a high intensity, 350~MeV pion beam at PSI to prove that we had reached a Milestone for the Compact Muon Solenoid (CMS) experiment. The particle rate was approximately 6 kHz/mm2, distributed over the whole active area of the detectors, and this rate was maintained for a total integrated time of 493 hours. All of the chambers were operated with signal-to-noise values at or above that corresponding to 98 % hit detection efficiency at CMS; the average S/N was 31. No indications of any gain instabilities or ageing effects were observed. In the official 3-week Milestone period, three strips from a total of 16384 were damaged, a result which is twenty times lower than the minimal requirement for CMS. The spark rate of the detectors was very low and decreased with time to an average of one spark per chamber per day. The cathode voltages of 24 of the chambers were increased over a one week period to investigate the behaviour of the detectors at higher gains; the maximum S/N value was 2.4 times that at the normal working point. No significant increase in spark rate or strip loss rate was detected and the chambers operated stably. The detector efficiencies and imaging capabilities were also investigated. The MSGC design features and the assembly and test methodologies that enabled us to achieve these results are reported