Search results for "hadron"

showing 10 items of 3505 documents

Alma Mater

2015

Jauno mūzikas grupu konkurss studentiem «Hadrons» – platforma jauniešiem ceļā uz lielo skatuviERASMUS+ prakses iespējas studentiemzinātnē viens nav karotājs [Neirozinātniece Inga Kadiša]Mālu mīcīšana 40 gadu garumāNākotnes materiāli. Epoksīda sveķu uzlabošana ar oglekļa nanopildvielāmRakstīt ir tikpat dabiski kā ēst gulēt un mazgātiessaules enerģija jaunajiem izgudrotājiem [«Saules kauss 2015»]Studiju programmas Latvijas Universitātē 2015./2016. akadēmiskajā gadārektora stāsts [Latvijas Universitāte – kad globālais satiekas ar lokālo]«Mans hobijs ir cilvēki» [Mateo Frejs no Šveices]
researchProduct

Alma Mater: 2013/ Vasara

2013

Jauno mūzikas grupu konkurss «Hadrons 2013»Fizikas un matemātikas fakultātes jauktais koris "Aura"Latvijas Universitātes Botāniskais dārzsProfesors Viktors FreibergsKaspars AdijānsProjekts «Atbalsts Latvijas Universitātes starptautiskās sadarbības projektiem un citiem starptautiskās sadarbības pasākumiem zinātnē un tehnoloģijās»Studiju kvalitāte -- Latvijas UniversitāteDiriģents Edgars VītolsLatvijas Universitātes basketbola komandaLatvijas Universitātes Studentu padome -- Projektu konkursiStarptautiskais kognitīvo zinātņu loģikas un komunikācijas simpozijs «Uztvere un koncepti»Aktuālie notikumi Latvijas UniversitātēCouple Learning programme
researchProduct

Differential branching fraction and angular analysis of the decay $B^{0} \to K^{*0} \mu^{+}\mu^{-}$

2013

The angular distribution and differential branching fraction of the decay B-0 -> K*(0)mu(+)mu(-) are studied using a data sample, collected by the LHCb experiment in pp collisions at root s = 7 TeV, corresponding to an integrated luminosity of 1.0 fb(-1). Several angular observables are measured in bins of the dimuon invariant mass squared, q(2). A first measurement of the zero-crossing point of the forward-backward asymmetry of the dimuon system is also presented. The zero-crossing point is measured to be q(0)(2) = 4.9 +/- 0.9 GeV2/c(4), where the uncertainty is the sum of statistical and systematic uncertainties. The results are consistent with the Standard Model predictions.

K-ASTERISK-L(+)L(-)12.15.Mm01 natural sciencesB physicsLuminositydecayHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareNeutral currentFlavor physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massQCDetectors de radiaciómedia_commonPhysicsB0 mesonHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadronObservableCP violationFIS/01 - FISICA SPERIMENTALENuclear countersLeptonic semileptonic and radiative decays of bottom mesonsFísica nuclearLHCB physics; Flavor physics; Flavour Changing Neutral Currents; Hadron-Hadron Scattering; Rare decayParticle Physics - ExperimentParticle physicsNuclear and High Energy Physicsmedia_common.quotation_subject14.40.NdFlavour Changing Neutral CurrentsHadronsAsymmetryPartícules (Física nuclear)Standard ModelB physics; Flavor physics; Flavour Changing Neutral Currents; Hadron-Hadron Scattering; Rare decay; Nuclear and High Energy PhysicsNeutral currentsAngular distributionASYMMETRIES0103 physical sciencesLeptonic semileptonic and radiative decays of bottom mesonLHC flavour physics010306 general physicsHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadronsB0 meson; decay; LHCb; LHCHadron-Hadron Scattering010308 nuclear & particles physicsBranching fractionCromodinàmica quànticaLHCbRare decay13.20.HeBottom mesons (|B|>0); Leptonic semileptonic and radiative decays of bottom mesons; Hadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadrons; Neutral currents; 14.40.Nd; 13.20.He; 13.85.Ni; 12.15.Mm;Bottom mesons (|B|>0)High Energy Physics::Experiment13.85.NiDifferential (mathematics)FIS/04 - FISICA NUCLEARE E SUBNUCLEAREQuantum chromodynamicsexperimental results
researchProduct

Performance of ATLAS tracking detector

2012

The track and vertex reconstruction algorithms of the ATLAS Inner Detector have demonstrated excellent performance in the early data from the LHC. However, the rapidly increas- ing number of interactions per bunch crossing introduces new challenges both in computational aspects and physics performance. The combination of both silicon and gas based detectors provides high precision impact parameter and momentum measurement of charged particles, with high efficiency and small fake rate. Vertex reconstruction is used to identify with high efficiency the hard scattering process and to measure the amount of pile-up interactions, both aspects are cru- cial for many physics analyses. The performan…

Large Hadron ColliderAtlas (topology)Computer scienceDetectorScattering processImpact parameterDetectors and Experimental TechniquesImage resolutionCharged particleComputational science
researchProduct

An FPGA based Topological Processor Prototype for the ATLAS Level-1 Trigger Upgrade

2012

By 2014 the LHC will collide proton bunches at 14TeV with an increased instantaneous luminosity up to 3·10³⁴cm⁻²s⁻¹. The resulting higher event rate will challenge the existing ATLAS trigger system. A reduction on the trigger rate can be achieved by selecting interesting channels based on their expected decay topology and thus reducing background. This will be achieved by introducing of a new FPGA based module in the Level-1 trigger: the Topological Processor L1Topo. With L1Topo it will be possible for the first time to concentrate detailed information from the entire calorimeters and the muon detector into a single module. L1Topo will receive a total aggregate bandwidth of 1Tb/s. The data …

Large Hadron ColliderBandwidth (signal processing)TopologyLinear particle acceleratorComputer Science::Hardware ArchitectureData acquisitionBunchesUpgradePhysics::Accelerator PhysicsTransceiverDetectors and Experimental TechniquesField-programmable gate arrayInstrumentationMathematical Physics
researchProduct

The ATLAS Level-1 Calorimeter Trigger: PreProcessor implementation and performance

2012

The PreProcessor system of the ATLAS Level-1 Calorimeter Trigger (L1Calo) receives about 7200 analogue signals from the electromagnetic and hadronic components of the calorimetric detector system. Lateral division results in cells which are pre-summed to so-called Trigger Towers of size 0.1 × 0.1 along azimuth (phi) and pseudorapidity (η). The received calorimeter signals represent deposits of transverse energy. The system consists of 124 individual PreProcessor modules that digitise the input signals for each LHC collision, and provide energy and timing information to the digital processors of the L1Calo system, which identify physics objects forming much of the basis for the full ATLAS fi…

Large Hadron ColliderCalorimeter (particle physics)010308 nuclear & particles physicsComputer sciencebusiness.industryPhysics::Instrumentation and DetectorsDetectorElectrical engineering01 natural scienceslaw.inventionMicroprocessormedicine.anatomical_structureAtlas (anatomy)lawPseudorapidity0103 physical sciencesmedicinePreprocessorDetectors and Experimental Techniques010306 general physicsbusinessInstrumentationMathematical PhysicsEnergy (signal processing)Computer hardware
researchProduct

The Optical Multiplexer Board for the ATLAS Hadronic Tile Calorimeter

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 manufacturing features of these prototypes are described. These prototypes are being validated while firmware developments are being implemented in the programmable devices of the board.

Large Hadron ColliderCalorimeter (particle physics)Physics::Instrumentation and Detectorsbusiness.industryFirmwareComputer scienceElectrical engineeringcomputer.software_genreMultiplexerData acquisitionmedicine.anatomical_structureAtlas (anatomy)visual_artNuclear electronicsvisual_art.visual_art_mediummedicineTilebusinesscomputerComputer hardware2007 IEEE Nuclear Science Symposium Conference Record
researchProduct

Accelerating Radioactive Ion Beams With REX-ISOLDE

2003

The post accelerator REX‐ISOLDE is installed at the ISOLDE facility at CERN, where a broad variety of radioactive ions can be addressed. Since the end of 2001 beams at the final energy of 2.2 MeV/u are available. REX‐ISOLDE uses a unique system of beam bunching and charge breeding. First a Penning trap accumulates and bunches the ions, which are delivered as a quasi‐continuous beam from the ISOLDE target‐ion‐source, and then an electron beam ion source (EBIS) charge‐breeds them to a mass‐to‐charge ratio below 4.5. This enables a very compact design for the following LINAC, consisting of a 4 rod RFQ, an IH structure and three 7‐gap‐resonators. The later ones allow a variation of the final en…

Large Hadron ColliderChemistryParticle acceleratorPenning trapIon sourceLinear particle acceleratorlaw.inventionNuclear physicsBuncheslawPhysics::Accelerator PhysicsNeutronAtomic physicsNuclear ExperimentBeam (structure)AIP Conference Proceedings
researchProduct

Readout system of the ALICE Fast Interaction Trigger

2020

Large Hadron ColliderComputer sciencebusiness.industryMeasuring instrumentElectrical engineeringALICE (propellant)businessInstrumentationMathematical PhysicsParticle identificationParticle detectorJournal of Instrumentation
researchProduct

MuPix and ATLASPix -- Architectures and Results

2020

High Voltage Monolithic Active Pixel Sensors (HV-MAPS) are based on a commercial High Voltage CMOS process and collect charge by drift inside a reversely biased diode. HV-MAPS represent a promising technology for future pixel tracking detectors. Two recent developments are presented. The MuPix has a continuous readout and is being developed for the Mu3e experiment whereas the ATLASPix is being developed for LHC applications with a triggered readout. Both variants have a fully monolithic design including state machines, clock circuitries and serial drivers. Several prototypes and design variants were characterised in the lab and in testbeam campaigns to measure efficiencies, noise, time reso…

Large Hadron ColliderFinite-state machinePhysics - Instrumentation and DetectorsPixelComputer scienceDetectorFOS: Physical sciencesHigh voltageInstrumentation and Detectors (physics.ins-det)Tracking (particle physics)7. Clean energyNoise (electronics)Electronic engineeringDetectors and Experimental Techniquesddc:620physics.ins-detEngineering & allied operationsDiode
researchProduct