G. Mahout
University of Birmingham
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by G. Mahout.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2003
J. Garvey; S. J. Hillier; G. Mahout; R. Staley; P. M. Watkins; A. T. Watson; R. Achenbach; P. Hanke; W Hinderer; D Kaiser; E.-E. Kluge; K. Meier; O. Nix; K. Penno; K. Schmitt; B. Bauss; A. Dahlhoff; K. Jakobs; K. Mahboubi; U. Schäfer; J. Thomas; T. Trefzger; E. Eisenhandler; Murrough Landon; D Mills; E. Moyse; P Apostologlou; B.M. Barnett; I.P. Brawn; A.O. Davis
Abstract At the full LHC design luminosity of 10 34 cm −2 s −1 , there will be approximately 10 9 proton–proton interactions per second. The ATLAS level-1 trigger is required to have an acceptance factor of ∼10 −3 . The calorimeter trigger covers the region | η |⩽5.0, and φ =0 to 2 π . The distribution of transverse energy over the trigger phase space is analysed to identify candidates for electrons/photons, isolated hadrons, QCD jets and non-interacting particles. The Cluster Processor of the level-1 calorimeter trigger is designed to identify transverse energy clusters associated with the first two of these. The algorithms based on the trigger tower energies which have been designed to identify such clusters, are described here. The algorithms are evaluated using an FPGA. The reasons for the choice of the actual FPGA being used are given. The performance of the FPGA has been fully simulated, and the expected latency has been shown to be within the limits of the time allocated to the cluster trigger. These results, together with the results of measurements made with real data into a fully configured FPGA, are presented and discussed.
IEEE Transactions on Nuclear Science | 2004
J. Garvey; S. J. Hillier; G. Mahout; T.H. Moye; R. Staley; P. M. Watkins; A. T. Watson; R. Achenbach; P. Hanke; E.-E. Kluge; K. Meier; P. Meshkov; O. Nix; K. Penno; K. Schmitt; C. Ay; B. Bauss; A. Dahlhoff; K. Jakobs; K. Mahboubi; U. Schäfer; T. Trefzger; E. Eisenhandler; Murrough Landon; E. J. W. Moyse; J. P. Thomas; P. Apostoglou; B. M. Barnett; I.P. Brawn; A.O. Davis
The architecture of the ATLAS Level-1 Calorimeter Trigger system (L1Calo) is presented. Common approaches have been adopted for data distribution, result merging, readout, and slow control across the three different subsystems. A significant amount of common hardware is utilized, yielding substantial savings in cost, spares, and development effort. A custom, high-density backplane has been developed with data paths suitable for both the em//spl tau/ cluster processor (CP) and jet/energy-summation processor (JEP) subsystems. Common modules also provide interfaces to VME, CANbus and the LHC timing, trigger and control system (TTC). A common data merger module (CMM) uses field-programmable gate arrays (FPGAs) with multiple configurations for summing electron/photon and /spl tau//hadron cluster multiplicities, jet multiplicities, or total and missing transverse energy. The CMM performs both crate- and system-level merging. A common, FPGA-based readout driver (ROD) is used by all of the subsystems to send input, intermediate and output data to the data acquisition (DAQ) system, and region-of-interest (RoI) data to the level-2 triggers. Extensive use of FPGAs throughout the system makes the trigger flexible and upgradable, and several architectural choices have been made to reduce the number of intercrate links and make the hardware more robust.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000
G. Mahout; M. Pearce; M. L. Andrieux; C. B. Arvidsson; D. G. Charlton; B. Dinkespiler; J.D. Dowell; L. Gallin-Martel; R.J. Homer; P. Jovanovic; Ian Kenyon; G. Kuyt; J. Lundquist; Igor Mandic; O. Martin; H.R. Shaylor; R. Stroynowski; J.K Troska; R. Wastie; Anthony Weidberg; J. A. Wilson; J. Ye
The radiation tolerance of three multimode optical fibres has been investigated to establish their suitability for the use in the front-end data links of the ATLAS experiment. Both gamma and neutro ...
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2000
D. G. Charlton; J.D. Dowell; R.J. Homer; P. Jovanovic; Ian Kenyon; G. Mahout; H.R. Shaylor; J. A. Wilson; A. Rudge; J. Fopma; Igor Mandic; R. B. Nickerson; P.D. Shield; R. Wastie; Anthony Weidberg; L.O. Eek; A. Go; B. Lund-Jensen; M. Pearce; J. Soderqvist; M.C. Morrissey; D.J. White
A prototype optical data and Timing Trigger and Control transmission system based on LEDs and PIN-diodes has been constructed. The system would be suitable in terms of radiation hardness and radiat ...
International Symposium on Optical Science and Technology | 2000
G. Mahout; David G. Charlton; J.D. Dowell; Ingrid-Maria Gregor; R.J. Homer; P. Jovanovic; A. Kootz; R. B. Nickerson; R. Wastie; Anthony Weidberg
This paper reports the radiation hardness of optical components to be used in the binary readout of one of the next generation of detectors in high energy physics. The optical components will have to sustain a total ionizing dose of 500 kGy and a 1 MeV equivalent neutron fluence of 1015 n cm-2. Emitters of VCSEL type have been chosen and have shown a shift of 1 mA in the laser threshold current after irradiation, but are still suitable for our purpose. The epitaxial Si PIN photodiode receivers have an acceptable 30% drop in responsivity providing a higher reverse bias is applied. Speed and lifetime of both components appear to be unaffected by the radiation damage. Temperature characteristics showing differences from un- irradiated materials will be also presented.
ieee nuclear science symposium | 2008
R. Achenbach; P. Adragna; M. Aharrouche; V. Andrei; B. Åsman; B. M. Barnett; B. Bauss; M. Bendel; C. Bohm; J.R.A. Booth; J. Bracinik; I.P. Brawn; D. G. Charlton; J. T. Childers; N. J. Collins; C. J. Curtis; A.O. Davis; S. Eckweiler; E. Eisenhandler; P.J.W. Faulkner; J. Fleckner; F. Föhlisch; C. N. P. Gee; A. R. Gillman; C. Goringer; M. Groll; D. R. Hadley; P. Hanke; S. Hellman; A. Hidvegi
The ATLAS Level-1 Calorimeter Trigger is one of the main elements of the first stage of event selection for the ATLAS experiment at the LHC. The input stage consists of a mixed analogue/digital component taking trigger sums from the ATLAS calorimeters. The trigger logic is performed in a digital, pipelined system with several stages of processing, largely based on FPGAs, which perform programmable algorithms in parallel with a fixed latency to process about 300 Gbyte/s of input data. The real-time output consists of counts of different types of physics objects, and energy sums. The final system consists of over 300 custom-built VME modules, of several different types. The installation at ATLAS of these modules, and the necessary infrastructure, was completed at the end of 2007. The system has since undergone intensive testing, both in standalone mode, and in conjunction with the whole of the ATLAS detector in combined running. The final steps of commissioning, and experience with running the full-scale system are presented. Results of integration tests performed with the upstream calorimeters, and downstream trigger and data-flow systems, are shown, along with an analysis of the performance of the calorimeter trigger in full ATLAS data-taking. This includes trigger operation during the cosmic muon runs from before LHC start-up, and a first look at LHC proton beam data.
ieee nuclear science symposium | 2003
J. Garvey; S. J. Hillier; G. Mahout; T.H. Moye; R. Staley; P. M. Watkins; A. T. Watson; R. Achenbach; P. Hanke; E.-E. Kluge; K. Meier; P. Meshkov; O. Nix; K. Penno; K. Schmitt; C. Ay; B. Bauss; A. Dahlhoff; K. Jakobs; K. Mahboubi; U. Schäfer; T. Trefzger; E. Eisenhandler; Murrough Landon; E. J. W. Moyse; J. P. Thomas; P. Apostologlou; B. M. Barnett; I.P. Brawn; A.O. Davis
The ATLAS Level-1 Calorimeter Trigger consists of a Preprocessor, a Cluster Processor (CP), and a Jet/Energy-sum Processor (JEP). The CP and JEP receive digitised trigger-tower data from the Preprocessor and produce trigger multiplicities and total and missing energy for the final trigger decision. The trigger will also provide region-of-interest (RoI) information for the Level-2 trigger and intermediate results of the data acquisition (DAQ) system for monitoring and diagnostics by using readout driver modules (ROD). The Jet/Energy-sum Processor identifies and localises jets, and sums total and missing transverse energy information from the trigger data. The Jet/Energy Module (JEM) is the main module of the Jet/Energy-sum Processor. The JEM prototype is designed to be functionally identical to the final production module for ATLAS, and have the full number of channels. Three JEM prototypes have been built and successfully tested. Various test vector patterns were used to test the energy summation and the jet algorithms. Data communication between adjacent Jet/Energy Modules and all other relevant modules of the Jet/Energy-sum Processor has been tested. Recent test results using the Jet/Energy Module prototypes are presented and discussed.
International Symposium on Optical Science and Technology | 2000
J. Troska; J.D. Dowell; Ingrid-Maria Gregor; R.J. Homer; P. Jovanovic; G. Mahout; Igor Mandic; R. Wastie; Anthony Weidberg; D.J. White
The ATLAS experiment is currently in the final pre-production design phase to allow timely installation at the CERN Large Hadron Collider in 2005. The sub-systems closest to the interaction point--the tracking detectors, will be subject to significant total radiation dose at high flux. Optical data transmission has been chosen for the Pixel and SemiConductor Tracker to both deliver timing and control information to the detector modules and transmit tracking data to the remote counting room. Of considerable concern is the radiation hardness, both transient and total dose, of not just the optoelectronic components but also the driver/receiver electronics. In this paper we report on total dose radiation testing of the VCSEL driver and photodiode receiver ASICs designed using a range of techniques in a nominally radiation-soft process. Both ASICs will be shown to be tolerant to a total gamma dose of 100 kGy and a total neutron fluence (1 MeV equiv.) of 2 X 1014 n/cm2, as required for this system. Single-event upset (SEU) studies have also been carried out using a high-energy pion beam, showing the system to be sufficiently robust to SEU at an ATLAS- like particle flux.
IEEE Transactions on Nuclear Science | 2008
R. Achenbach; P. Adragna; V. Andrei; B. M. Barnett; B. Bauss; M. Bendel; C. Bohm; J.R.A. Booth; I.P. Brawn; D. G. Charlton; C. J. Curtis; A.O. Davis; E. Eisenhandler; P.J.W. Faulkner; F. Föhlisch; C. N. P. Gee; C. Geweniger; A. R. Gillman; P. Hanke; S. Hellman; A. Hidvegi; S. J. Hillier; M. Johansen; E.-E. Kluge; Murrough Landon; V. Lendermann; K. Mahboubi; G. Mahout; K. Meier; A. Neusiedl
The ATLAS Level-1 Calorimeter Trigger is one of the main elements of the first stage of event selection for the ATLAS experiment at the LHC. The input stage consists of a mixed analogue/digital component taking trigger sums from the ATLAS calorimeters. The trigger logic is performed in a digital, pipelined system with several stages of processing, largely based on FPGAs, which perform programmable algorithms in parallel with a fixed latency to process about 300 Gbyte/s of input data. The real-time output consists of counts of different types of physics objects and energy sums. The production of final modules started in 2006, and installation of these modules and the necessary infrastructure at ATLAS has been underway for some time, with the intention of having a full system in situ during 2007, before first collisions at the LHC. The first experiences of commissioning and running the full scale system will be presented, along with results from integration tests performed with the upstream calorimeters, and the downstream trigger and data flow systems.
IEEE Symposium Conference Record Nuclear Science 2004. | 2004
J. Garvey; S. J. Hillier; G. Mahout; T.H. Moye; R. Staley; J. P. Thomas; D. Typaldos; P. M. Watkins; A. T. Watson; R. Achenbach; F. Föhlisch; C. Geweniger; P. Hanke; E.-E. Kluge; K. Mahboubi; K. Meier; P. Meshkov; F. Rühr; K. Schmitt; Hans-Christian Schultz-Coulon; C. Ay; B. Bauss; Andrey Belkin; S. Rieke; U. Schäfer; S. Tapprogge; T. Trefzger; G. Weber; E. Eisenhandler; Murrough Landon
The level-1 calorimeter trigger consists of a preprocessor (PP), a cluster processor (CP), and a jet/energy-sum processor (JEP). The CP and JEP receive digitised trigger-tower data from the preprocessor and produce regions-of-interest (RoIs) and trigger multiplicities. The latter are sent in real time to the central trigger processor (CTP) where the level-1 decision is made. On receipt of a level-1 accept, readout driver modules (RODs) provide intermediate results to the data acquisition (DAQ) system for monitoring and diagnostic purposes. RoI information is sent to the RoI builder (RoIB) to help reduce the amount of data required for the level-2 trigger. The level-1 calorimeter trigger system at the test beam consisted of 1 preprocessor module, 1 cluster processor module, 1 jet/energy module and 2 common merger modules. Calorimeter energies were successfully handled throughout the chain and trigger objects sent to the CTP. Level-1 accepts were successfully produced and used to drive the readout path. Online diagnostics were made using 4 RODs. Energy histograms were plotted and the integrity of data between the different modules was checked. All ATLAS detectors in the test beam were able to build full events based on triggers delivered by the calorimeter trigger system.