Search results for " Collider"

showing 10 items of 1415 documents

Design and test of a prototype silicon detector module for ATLAS Semiconductor Tracker endcaps

2005

The ATLAS Semiconductor Tracker (SCT) will be a central part of the tracking system of the ATLAS experiment. The SCT consists of four concentric barrels of silicon detectors as well as two silicon endcap detectors formed by nine disks each. The layout of the forward silicon detector module presented in this paper is based on the approved layout of the silicon detectors of the SCT, their geometry and arrangement in disks, but uses otherwise components identical to the barrel modules of the SCT. The module layout is optimized for excellent thermal management and electrical performance, while keeping the assembly simple and adequate for a large scale module production. This paper summarizes th…

Radiation hardnessPhysicsNuclear and High Energy PhysicsLarge Hadron ColliderSiliconbusiness.industryDetectorATLAS experimentSemicondutor radiation detectorATLAS experimentchemistry.chemical_elementTracking systemddc:500.2VLSI readoutParticle detectorSemiconductor detectorchemistryHardware_INTEGRATEDCIRCUITSLHCThermal managementbusinessInstrumentationRadiation hardeningSilicon strip detectorComputer hardwareNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The Miniball spectrometer

2013

The Miniball germanium detector array has been operational at the REX (Radioactive ion beam EXperiment) post accelerator at the Isotope Separator On-Line facility ISOLDE at CERN since 2001. During the last decade, a series of successful Coulomb excitation and transfer reaction studies have been performed with this array, utilizing the unique and high-quality radioactive ion beams which are available at ISOLDE. In this article, an overview is given of the technical details of the full Miniball setup, including a description of the γ-ray and particle detectors, beam monitoring devices and methods to deal with beam contamination. The specific timing properties of the REX-ISOLDE facility are hi…

Radioactive ion beamsNuclear and High Energy PhysicsIon beamREX-ISOLDEONLINECoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physicsSETUPCOULOMB-EXCITATION0103 physical sciencesNuclear fusionSILICON STRIP DETECTOR[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]RELATIVISTIC ENERGIES010306 general physicsNuclear ExperimentNEUTRON KNOCKOUTPhysicsNuclear Physics; Heavy Ions; Hadrons; Particle and Nuclear Physics; Nuclear FusionLarge Hadron ColliderSpectrometerNUCLEI010308 nuclear & particles physicsDetectorRADIOACTIVE ION-BEAMSemiconductor detectorPhysics::Accelerator PhysicsGE DETECTORS
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The SPEDE spectrometer

2017

8 pags., 10 figs., 2 tabs.

Radioactive ion beamsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsElectron spectrometerPhysics::Instrumentation and DetectorsFOS: Physical sciencesElectronnucl-ex7. Clean energy01 natural sciencesMomentumNuclear physicsInternal conversion0103 physical sciencesNuclear Physics - ExperimentDetectors and Experimental TechniquesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear Experimentphysics.ins-detPhysicsLarge Hadron ColliderSpectrometer010308 nuclear & particles physicsInstrumentation and Detectors (physics.ins-det)Magnetic fieldPhysics::Accelerator Physics
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The upgraded ISOLDE yield database – A new tool to predict beam intensities

2020

At the CERN-ISOLDE facility a variety of radioactive ion beams are available to users of the facility. The number of extractable isotopes estimated from yield database data exceeds 1000 and is still increasing. Due to high demand and scarcity of available beam time, precise experiment planning is required. The yield database stores information about radioactive beam yields and the combination of target material and ion source needed to extract a certain beam along with their respective operating conditions. It allows to investigate the feasibility of an experiment and the estimation of required beamtime. With the increasing demand for ever more exotic beams, needs arise to extend the functi…

Radioactive ion beamsNuclear and High Energy PhysicsYieldsComputer sciencecomputer.software_genre114 Physical sciences01 natural sciencesISOLDEDatabaseFLUKACERN0103 physical sciencesddc:530Production Yield010306 general physicsInstrumentationLarge Hadron ColliderDatabase010308 nuclear & particles physicsIn-target productionYield predictionCross sectionsYield (chemistry)ABRABLAIONIZATIONRelease efficiencycomputerRadioactive beamBeam (structure)Radioactive beamsNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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The SPEDE Spectrometer: Combined In-Beam γ-ray and Conversion Electron Spectroscopy with Radioactive Ion Beams

2015

The SPEDE spectrometer [1] aims to combine a silicon detector, for the detection of electrons, with the MINIBALL γ-ray detection array for in-beam studies employing radioactive ion beams at the HIE-ISOLDE facility at CERN. The setup will be primarily used for octupole collectivity [2] and shape coexistence studies [3, 4] in Coulomb excitation experiments. In the shape coexistence cases the transitions between states of the same spin and parity have enhanced E0 strength [5]. Additionally the 0→0 transitions, typically present in nuclei exhibiting shape coexistence [6], can only occur via E0 transitions, i.e. via internal conversion electron emission.

Radioactive ion beamsPhysicsLarge Hadron ColliderSpectrometerta114Physics::Instrumentation and DetectorsParity (physics)Coulomb excitationElectronElectron spectroscopyPhysics::Accelerator PhysicsSilicon detectorAtomic physicsconversion electron spectrometersNuclear Experiment
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Inclusive double-helicity asymmetries in neutral-pion and eta-meson production in p → + p → collisions at s =200GeV

2014

Abstract: Results are presented from data recorded in 2009 by the PHENIX experiment at the Relativistic Heavy Ion Collider for the double-longitudinal spin asymmetry, A LL , for π 0 and η production in ffiffiffi s p ¼ 200 GeV polarized p þ p collisions. Comparison of the π 0 results with different theory expectations based on fits of other published data showed a preference for small positive values of gluon polarization, Δ G , in the proton in the probed Bjorken x range. The effect of adding the new 2009 π 0 data to a recent global analysis of polarized scattering data is also shown, resulting in a best fit value Δ G ½ 0 . 05 ; 0 . 2 DSSV ¼ 0 . 06 þ 0 . 11 − 0 . 15 in the range 0 . 05 <x< …

Relativistic Heavy Ion Colliderdouble-longitudinal spin asymmetry
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Measurement ofΥ(1S+2S+3S)production inp+pand Au + Au collisions atsNN=200GeV

2015

Measurements of bottomonium production in heavy-ion and p + p collisions at the Relativistic Heavy Ion Collider (RHIC) are presented. The inclusive yield of the three states, (1S + 2S + 3S), was measured in the PHENIX experiment via electron-positron decay pairs at midrapidity for Au + Au and p + p collisions at root sNN = 200 GeV. The (1S + 2S + 3S) -> e(+)e(-) differential cross section at midrapidity was found to be B(ee)d sigma/dy = 108 +/- 38 (stat) +/- 15 (syst) +/- 11 (luminosity) pb in p + p collisions. The nuclear modification factor in the 30% most central Au + Au collisions indicates a suppression of the total. state yield relative to the extrapolation from p + p collision data. …

Scattering cross-sectionPhysicsNuclear and High Energy PhysicsLarge Hadron Collider010308 nuclear & particles physicsModification factor01 natural sciencesLuminosityNuclear physicsYield (chemistry)0103 physical sciencesHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderPhysical Review C
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Top-quark mass measurements using jet rates at LHC

2013

This work presents a new method to measure the top-quark mass in hadronic collisions[1]. The method uses the sensitivity of the tt̄ + 1-jet production on the top-quark mass. In detail we study the ℛ distribution defined as the tt̄ + 1-jet normalized cross section differential in the invariant mass of the total system and calculated at NLO accuracy. We prove that the ℛ distribution has a high sensitivity to the top-quark mass. Furthermore we investigate and quantify the impact of the dominant theoretical and experimental uncertainties. The results obtained show, that the method has the potential to be competitive in precision with established approaches and allows a complementary measurement…

Scattering cross-sectionPhysicsTop quarkParticle physicsLarge Hadron ColliderPhysicsQC1-999HadronHigh Energy Physics::PhenomenologyInvariant (physics)Nuclear physicsRenormalizationPhysics and Astronomy (all)High Energy Physics::ExperimentMass parameterEPJ Web of Conferences
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TileCal optical multiplexer board 9U prototype

2007

This paper presents the architecture and the status of the optical multiplexer board (OMB) for the ATLAS/LHC Tile hadronic calorimeter (TileCal). This board will analyze the front-end data CRC to prevent bit and burst errors produced by radiation. Besides, due to its position within the data acquisition chain it will be used to emulate front-end data for tests. The first two prototypes of the final OMB 9U version have been produced at CERN. Detailed design issues and manufacture features of these prototypes are described. These prototypes are being validated whereas some firmware developments are being implemented in the programmable devices of the board. Functional descriptions of the boar…

ScheduleEngineeringLarge Hadron ColliderFirmwarebusiness.industrycomputer.software_genreMultiplexerData acquisitionSingle event upsetNuclear electronicsEmbedded systemField-programmable gate arraybusinesscomputer
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Measurement of the forward-backward asymmetry of e(+)e(-)-]z-]b(b)over-bar using prompt leptons and a lifetime tag

1995

The forward-backward asymmetry of the process e+e-→Z→b {Mathematical expression} has been measured using events collected by the DELPHI experiment during the 1991 and 1992 LEP runs. This data sample corresponded to 884 000 hadronic Z decays at a centre-of-mass energy {Mathematical expression}. The tagging of b-quark events was performed using two approaches; the first was based on the semileptonic decay channels b→X+μ and b→X+e, the second used a lifetime tag with jet-charge reconstruction. The results of these two methods were combined to give {Mathematical expression} With the semileptonic sample, the forward-backward asymmetry of the process e+e-→Z→ {Mathematical expression} was also mea…

Semileptonic decayParticle physicsFERMION PAIR PRODUCTIONPhysics and Astronomy (miscellaneous)LUND MONTE-CARLOENERGIESElectron–positron annihilationQED CORRECTIONSD-MESONSEMILEPTONIC DECAY01 natural sciencesJET FRAGMENTATIONb-taggingPartícules (Física nuclear)PHYSICSNuclear physics0103 physical sciencesDELPHI; forward-backward asymmetry; b-tagging; jet reconstructionFERMION PAIR PRODUCTION; LUND MONTE-CARLO; E+E-ANNIHILATION; SEMILEPTONIC DECAY; JET FRAGMENTATION; QED CORRECTIONS; FINAL-STATES; D-MESON; ENERGIES; PHYSICS010306 general physicsEngineering (miscellaneous)jet reconstructionDetectors de radiacióDELPHIPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyWeinberg angleE+E-ANNIHILATIONLARGE ELECTRON POSITRON COLLIDERFINAL-STATESb-taggingPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHILarge Electron–Positron ColliderPARTICLE PHYSICSHigh Energy Physics::Experimentforward-backward asymmetryEnergy (signal processing)Particle Physics - ExperimentLeptonBar (unit)
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