S. D. Kolya
University of Manchester
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by S. D. Kolya.
ieee nuclear science symposium | 2000
A. Baird; E. Elsen; Y.H. Fleming; M. Kolander; S. D. Kolya; D. Meer; D. Mercer; J. Naumann; P. R. Newman; Dave Sankey; A. Schöning; Hans-Christian Schultz-Coulon; C. Wissing
After 2001 the upgraded ep collider HERA will provide an about five times higher luminosity for the two experiments H1 and ZEUS. In order to cope with the expected higher event rates the H1 collaboration is building a track based trigger system, the Fast Track Trigger (FTT). It will be integrated in the first three levels (L1–L3) of the H1 trigger scheme to provide higher selectivity for events with charged particles. The FTT will allow to reconstruct 3-dimensional tracks in the central drift chamber down to 100 MeV/c within the L2 latency of ∼23 μs. To reach the necessary momentum resolution of ∼5% (at 1 GeV/c) sophisticated reconstruction algorithms have to be implemented using high density Field Programmable Gate Arrays (FPGA) and their embedded Content Addressable Memories (CAM). The final track parameter optimization will be done using non-iterative fits implemented in DSPs. While at the first trigger level rough track information will be provided, at L2 tracks with high resolution are available to form trigger decisions on topological and other track based criteria like multiplicities and momenta. At the third trigger level a farm of commercial processor boards will be used to compute physics quantities such as invariant masses. Keywords— Trigger, Fast Track Trigger, Track Trigger, FPGA, Content Addressable Memory, CAM, DSP, H1 Collaboration, HERA ColliderAfter 2001, the upgraded ep collider HERA will provide an about five times higher luminosity for the two experiments H1 and ZEUS. To cope with the expected higher event rates, the H1 collaboration is building a track-based trigger system, the Fast Track Trigger (FTT). It will be integrated in the first three levels (L1-L3) of the H1 trigger scheme to provide higher selectivity for events with charged particles. The FTT will allow reconstruction of three-dimensional tracks in the central drift chamber down to 100 MeV/c within the L2 latency of /spl sim/23 /spl mu/s. To reach the necessary momentum resolution of /spl sim/5% (at 1 GeV/c), sophisticated reconstruction algorithms have to be implemented using high-density field-programmable gate arrays and their embedded content addressable memories. The final track parameter optimization will be done using noniterative fits implemented in digital signal processors. While at the first trigger level rough track information will be provided, at L2 tracks with high resolution are available to form trigger decisions on topological and other track-based criteria like multiplicities and momenta. At the third trigger level, a farm of commercial processor boards will be used to compute physics quantities such as invariant masses.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2011
P. Grenier; G. Alimonti; M. Barbero; Richard Bates; E. Bolle; M. Borri; M. Boscardin; Craig Buttar; M. Capua; M. Cavalli-Sforza; M. Cobal; Andrea Cristofoli; G.-F. Dalla Betta; G. Darbo; C. Da Via; E. Devetak; B. DeWilde; D. Dobos; K. Einsweiler; David Esseni; S. Fazio; C. Fleta; J. Freestone; C. Gallrapp; M. Garcia-Sciveres; G. Gariano; C. Gemme; MarioPaolo Giordani; H. Gjersdal; S. Grinstein
Results on beam tests of 3D silicon pixel sensors aimed at the ATLAS Insertable B-Layer and High Luminosity LHC (HL-LHC) upgrades are presented. Measurements include charge collection, tracking efficiency and charge sharing between pixel cells, as a function of track incident angle, and were performed with and without a 1.6 T magnetic field oriented as the ATLAS inner detector solenoid field. Sensors were bump-bonded to the front-end chip currently used in the ATLAS pixel detector. Full 3D sensors, with electrodes penetrating through the entire wafer thickness and active edge, and double-sided 3D sensors with partially overlapping bias and read-out electrodes were tested and showed comparable performance.
Physics Letters B | 1988
J.F. Bak; Dario Barberis; T. J. Brodbeck; A.T. Doyle; R.J. Ellison; K. Elsener; R. E. Hughes-Jones; S. D. Kolya; D. Mercer; S.P. Møller; D. Newton; P.J. Ottewell; J.B.B. Petersen; P. Siffert; A.H. Sørensen; R. J. Thompson; E. Uggerhøj; G.W. Wilson
Experimental results are presented on the pair production from high-energy photons (40–150 GeV) incident on a 0.5 mm Ge single crystal around the 〈110〉 axis. The observed enhancement increases from around 1 at threshold (40 GeV) to 7 at 1 50 GeV for photons aligned with the axis. Also the angilar dependence and the differential e+/e− spectra have been studied. For photons aligned with the axis, the results are in good agreement with calculations based on the constant field approximation.
European Physical Journal C | 1989
R. J. Apsimon; M. Atkinson; M. Baake; L. S. Bagdasarian; Dario Barberis; T. J. Brodbeck; N. H. Brook; T. Charity; A. B. Clegg; P. Coyle; S. Danaher; S. Danagulian; M. Davenport; B. Dickinson; B. Diekmann; A. Donnachie; A. T. Doyle; J. Eades; R. J. Ellison; P. S. Flower; J. M. Foster; W. Galbraith; P. I. Galumian; C. Gapp; F. Gebert; G. Hallewell; K. Heinloth; R. C. W. Henderson; M. T. Hickman; C. Hoeger
Single charged-particle inclusive cross sections for photon, pion and kaon beams on hydrogen at the CERN-SPS are presented as functions ofpT andxF. Data cover the range 0.0<pT<5.0 GeV/c and 0.0<xF<1.0 at incident momenta from 70 to 170 GeV/c. The comparison between photon- and hadron-induced data indicates a relative excess of particles withpT>1.6 GeV/c for the photon-induced data. Using the hadron-induced data to estimate the hadronic behaviour of the photon, the difference distributions and ratios of cross sections are a measure of the contribution of the point-like photon interactions. The data are compared with QCD calculations and show broadly similar features.
European Physical Journal C | 1992
R. J. Apsimon; M. Atkinson; M. Baake; L. S. Bagdasarian; Dario Barberis; T. J. Brodbeck; Nicholas Brook; T. Charity; A. B. Clegg; P. Coyle; S. Danaher; S. Danagulian; M. Davenport; B. Dickinson; B. Diekmann; A. Donnachie; A. T. Doyle; J. Eades; R. J. Ellison; Frank Fiedler; P. S. Flower; J. M. Foster; W. Galbraith; P. I. Galumian; C. Gapp; F. Gebert; G. Hallewell; K. Heinloth; R. C. W. Henderson; M. T. Hickman
The inclusive production of ρ0 mesons was measured in γp andh±p collisions at beam energies of 65 GeV≦Eγ≦175 GeV andEh=80, 140 GeV, respectively, whereh is π orK. Cross sections were determined for all beams and energies as functions ofxF (−0.1≦xF≦1.0),pT (0≦pT≦3.5 GeV/c) and the polar decay angle of the ρ0 by fitting the ρ0 signal in π+π- mass distributions. The ρ0 line shape is found to be distorted from a pure Breit-Wigner distribution throughout most of thexF−pT plane for both photon and hadron beams and a simple explanation is suggested. Throughout the paper emphasis is put on the comparison of photon and hadron beam data. The comparison of cross sections of γp andhp data provides a measure of the Vector Meson Dominance factor throughout thexF−pT range of the ρ0. The ρ0 production at lowpT can be described for both photon and hadron beams by a triple regge model at largexF. Similarly central production is well described by the quark-antiquark fusion model. At largepT there is an excess of ρ0 photoproduction which is consistent with the expected onset of pointlike photon interactions.
European Physical Journal C | 1991
R. J. Apsimon; M. Atkinson; M. Baake; L. S. Bagdasarian; Dario Barberis; T. J. Brodbeck; N. H. Brook; T. Charity; A. B. Clegg; P. Coyle; S. Danaher; S. Danagulian; M. Davenport; B. Dickinson; B. Diekmann; A. Donnachie; A. T. Doyle; J. Eades; R. J. Ellison; P. S. Flower; J. M. Foster; W. Galbraith; P. I. Galumian; C. Gapp; F. Gebert; G. Hallewell; K. Heinloth; R. C. W. Henderson; M. T. Hickman; C. Hoeger
Measurements are reported of inclusive production of π0-mesons in the beam fragmentation region in γp, πp andKp collisions. Results include the ratio of π0 production inKp and πp collisions, showing reduced production from fragmentation of theK-meson, and the ratio of π0 production in photon and hadron collisions which shows agreement with modified Vector Meson Dominance at lowPT, and departures at higherPT signalling the onset of direct photon reactions. The pattern of departure from Feynman scaling at highPT points to a contribution of hard parton-parton collisions in both γp and πp collisions.
European Physical Journal C | 1990
R. J. Apsimon; M. Atkinson; M. Baake; L. S. Bagdasarian; Dario Barberis; T. J. Brodbeck; N. H. Brook; T. Charity; A. B. Clegg; P. Coyle; S. Danaher; S. Danagulian; M. Davenport; B. Dickinson; B. Diekmann; A. Donnachie; A. T. Doyle; J. Eades; R. J. Ellison; P. S. Flower; J. M. Foster; W. Galbraith; P. I. Galumian; C. Gapp; F. Gebert; G. Hallewell; K. Heinloth; R. C. W. Henderson; M. T. Hickman; C. Hoeger
Energy-flow distributions for charged hadrons from interactions of photons, pions and kaons on hydrogen are presented as functions of ΣpT2 in the event plane. Data cover the range 0.0<ΣpT in2<10.0(GeV/c)2 and 0.0<xF<1.0 for beam momenta from 65 to 170 GeV/c. The comparisons between photon-and hadron-induced data show an excess of events with larger ΣpT in2 for the photon-induced data. Using the hadron-induced data to parameterise the hadronic behaviour of the photon, the differences between cross sections are used to measure the contribution of the point-like photon interactions. Quantitative calculations of the point-like photon interactions using the Lund Monte-Carlo program LUCIFER, based on QCD, are in agreement with the data.
Physics Letters B | 1988
J.F. Bak; Dario Barberis; T. J. Brodbeck; A.T. Doyle; R.J. Ellison; K. Elsener; R. E. Hughes-Jones; S. D. Kolya; D. Mercer; S.P. Møller; D. Newton; P.J. Ottewell; J.B.B. Petersen; P. Siffert; A.H. Sørensen; R. J. Thompson; E. Uggerhøj; G.W. Wilson
The first results from a broad angular beam experiment on emission of high-energy photons from 170 GeV electrons and positrons are presented. The targets were 0.5 mm thick Si and Ge crystals. A dramatic enhancement in the emitted radiation is found for angles of incidence close to the 〈110〉 axis. The experimental results are compared to a constant-field cascade calculation.
ieee nuclear science symposium | 2000
R. E. Blair; J. Dawson; W. Haberichter; James Schlereth; R. Bock; A. Bogaerts; M. Boosten; R. Dobinson; M. Dobson; N. Ellis; M. Elsing; F. Giacomini; E. Knezo; B. Martin; T. Shears; S. Tapprogge; P. Werner; J. R. Hansen; A. Waananen; K. Korcyl; J. Lokier; S. George; B. Green; J. A. Strong; P. E. L. Clarke; R. Cranfield; G. Crone; P. Sherwood; S. Wheeler; R. E. Hughes-Jones
The Level-2 Trigger Pilot Project of ATLAS, one of the two general purpose LHC experiments, is part of the on-going programme to develop the ATLAS High Level Triggers (HLT). The Level-2 Trigger will receive events at up to 100 kHz, which has to be reduced to a rate suitable for full event-building of the order of 1 kHz. To reduce the data collection bandwidth and processing power required for the challenging Level-2 task it is planned to use Region of Interest guidance (from Level-1) and sequential processing. The Pilot Project included the construction and use of testbeds of up to 48 processing nodes, development of optimised components and computer simulations of a full system. It has shown how the required performance can be achieved, using largely commodity components and operating systems, and validated an architecture for the Level-2 system. This paper describes the principal achievements and conclusions of this project.
European Physical Journal C | 1992
R. J. Apsimon; M. Atkinson; M. Baake; L. S. Bagdasarian; Dario Barberis; T. J. Brodbeck; N. H. Brook; T. Charity; Ab Clegg; P. Coyle; S. Danaher; S. Danagulian; M. Davenport; B. Dickinson; B. Diekmann; A. Donnachie; A. T. Doyle; J. Eades; R. J. Ellison; F. Fiedler; P. S. Flower; J. M. Foster; W. Galbraith; P. I. Galumian; C. Gapp; F. Gebert; G. Hallewell; K. Heinloth; R. C. W. Henderson; M. T. Hickman
AbstractMeasurements are reported of inclusivef2(1270) andf0(975) production in γp, π±p andK±p collisions at photon beam energies of 65 to 175 GeV and hadron beam energies of 80 and 140 GeV. Thef2 andf0 mesons were found at masses of 1.250 GeV and 0.961 GeV respectively. Inclusivef2 production at lowxF was found to have a similarpT dependence for each beam type, whereas an additional pion-exchange contribution was found for production by pions at highxF. Cross sections are compared with those for ρ0 production and give no indication of a non-q