Search results for "LARGE HADRON COLLIDER"

showing 10 items of 1237 documents

Search for magnetic monopoles with the MoEDAL forward trapping detector in 2.11 fb −1 of 13 TeV proton–proton collisions at the LHC

2018

We update our previous search for trapped magnetic monopoles in LHC Run 2 using nearly six times more integrated luminosity and including additional models for the interpretation of the data. The MoEDAL forward trapping detector, comprising 222 kg of aluminium samples, was exposed to 2.11 fb−1 of 13 TeV proton–proton collisions near the LHCb interaction point and analysed by searching for induced persistent currents after passage through a superconducting magnetometer. Magnetic charges equal to the Dirac charge or above are excluded in all samples. The results are interpreted in Drell–Yan production models for monopoles with spins 0, 1/2 and 1: in addition to standard point-like couplings, …

Particle physicsNuclear and High Energy PhysicsProtonDirac (software)magnetic monopoleMagnetic monopoleFOS: Physical sciencesddc:500.2114 Physical sciences01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)0202 Atomic Molecular Nuclear Particle And Plasma PhysicsHigh Energy Physics - Phenomenology (hep-ph)STOPPING-POWER0103 physical sciencesFIELD010306 general physicsParticle Physics - PhenomenologyPhysicsLuminosity (scattering theory)Large Hadron ColliderInteraction point010308 nuclear & particles physicshep-exDrell–Yan processCharge (physics)hep-phNuclear & Particles Physicslcsh:QC1-999High Energy Physics - Phenomenologylcsh:PhysicsParticle Physics - Experiment
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Measurement of azimuthal hadron asymmetries in semi-inclusive deep inelastic scattering off unpolarised nucleons

2014

Spin-averaged asymmetries in the azimuthal distributions of positive and negative hadrons produced in deep inelastic scattering were measured using the CERN SPS muon beam at $160$ GeV/c and a $^6$LiD target. The amplitudes of the three azimuthal modulations $\cos\phi_h$, $\cos2\phi_h$ and $\sin\phi_h$ were obtained binning the data separately in each of the relevant kinematic variables $x$, $z$ or $p_T^{\,h}$ and binning in a three-dimensional grid of these three variables. The amplitudes of the $\cos \phi_h$ and $\cos 2\phi_h$ modulations show strong kinematic dependencies both for positive and negative hadrons.

Particle physicsNuclear and High Energy PhysicsTMD SIDIS PDFHadronFOS: Physical sciencesSIVERS ASYMMETRIESMUON PROTON-SCATTERINGCOLLINSSIDISPDF01 natural sciences530High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)LEPTOPRODUCTIONDEPENDENCE0103 physical sciencesDISTRIBUTIONSlcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsNuclear ExperimentPhysicsLarge Hadron ColliderMuon010308 nuclear & particles physicsTMDELECTROPRODUCTIONDeep inelastic scatteringAzimuthAmplitudeMUON PROTON-SCATTERING; SIVERS ASYMMETRIES; SPIN ASYMMETRIES; DISTRIBUTIONS; ELECTROPRODUCTION; LEPTOPRODUCTION; DEPENDENCE; COLLINSlcsh:QC770-798High Energy Physics::ExperimentNucleonSPIN ASYMMETRIESParticle Physics - ExperimentBeam (structure)
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Search for direct CP violation in the decays K-+/- -> 3 pi(+/-)

2006

Abstract We report a measurement of the direct CP violation asymmetry parameter A g in charged kaon decays K ± → π ± π + π − by the NA48/2 experiment at the CERN SPS. The experiment has been designed not to be limited by systematics in the asymmetry measurement. Using 1.67 × 10 9 such decays collected during the 2003 run, the charge asymmetry in the Dalitz plot linear slope parameter g has been measured to be A g = ( 1.7 ± 2.9 ) × 10 −4 . The precision of the result is limited by the statistics used.

Particle physicsNuclear and High Energy Physicsmedia_common.quotation_subjectDalitz plotviolazione CPcharged K mesonAsymmetryNEUTRAL KAONNuclear physicsmesoni K; violazione CPmesoni KCHARGE ASYMMETRY; NEUTRAL KAON; PARAMETER; NA48CP-violation asymmetriesCHARGE ASYMMETRYmedia_commonPhysicsLarge Hadron ColliderK meson; CP violationCharge (physics)PARAMETERK mesonkaon decayCP violationNA48CP violationkaon decay; charged K meson; CP-violation asymmetries
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Monopole production via photon fusion and Drell-Yan processes: MADGRAPH implementation and perturbativity via velocity-dependent coupling and magneti…

2018

In this work we consider point-like monopole production via photon-fusion and Drell-Yan processes in the framework of an effective U(1) gauge field theory obtained from conventional models describing the interaction of spin 0, 1/2, 1 magnetically-charged fields with ordinary photons, upon electric-magnetic dualisation. We present arguments based on such dualities which support the conjecture of an effective monopole-velocity-dependent magnetic charge. For the cases of spin-1/2 and spin-1 monopoles, we also include a magnetic-moment term kappa, which is treated as a new phenomenological parameter and, together with the velocity-dependent coupling, allows for a perturbative treatment of the c…

Particle physicsPhotonPhysics and Astronomy (miscellaneous)Field (physics)Regular Article - Experimental PhysicsMagnetic monopoleDegrees of freedom (statistics)FOS: Physical scienceslcsh:Astrophysics01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)lcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityGauge theory010306 general physicsEngineering (miscellaneous)Spin-½PhysicsLarge Hadron ColliderUnitarity010308 nuclear & particles physicsHigh Energy Physics - Phenomenologylcsh:QC770-798
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The beam and detector of the NA62 experiment at CERN

2017

NA62 is a fixed-target experiment at the CERN SPS dedicated to measurements of rare kaon decays. Such measurements, like the branching fraction of the $K^{+} \rightarrow \pi^{+} \nu \bar\nu$ decay, have the potential to bring significant insights into new physics processes when comparison is made with precise theoretical predictions. For this purpose, innovative techniques have been developed, in particular, in the domain of low-mass tracking devices. Detector construction spanned several years from 2009 to 2014. The collaboration started detector commissioning in 2014 and will collect data until the end of 2018. The beam line and detector components are described together with their early …

Particle physicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsFOS: Physical scienceslarge detector systems for particle and astroparticle physicsCalorimeters; Cherenkov detectors; Large detector systems for particle and astroparticle physics; Particle tracking detectors; Instrumentation; Mathematical PhysicsNA62 experimentTracking (particle physics)7. Clean energy01 natural sciencesParticle detectorHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareNONuclear physicsmathematical physicsHigh Energy Physics - Experiment (hep-ex)Calorimeters0103 physical sciencesparticle tracking detectorsDetectors and Experimental Techniques010306 general physicsParticle Physicsphysics.ins-detCalorimeters; Cherenkov detectors; large detector systems for particle and astroparticle physics; particle tracking detectors; instrumentation; mathematical physicsPhysicsinstrumentationCalorimeterLarge Hadron Collider010308 nuclear & particles physicsBranching fractionhep-exDetectorCherenkov detectorsInstrumentation and Detectors (physics.ins-det)Particle tracking detectorBeamlineLarge detector systems for particle and astroparticle physicHigh Energy Physics::ExperimentBeam (structure)Particle Physics - ExperimentCherenkov detector
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Axion search with BabyIAXO in view of IAXO

2020

Axions are a natural consequence of the Peccei-Quinn mechanism, the most compelling solution to the strong-CP problem. Similar axion-like particles (ALPs) also appear in a number of possible extensions of the Standard Model, notably in string theories. Both axions and ALPs are very well motivated candidates for Dark Matter, and in addition, they would be copiously produced at the sun's core. A relevant effort during the last decade has been the CAST experiment at CERN, the most sensitive axion helioscope to-date. The International Axion Observatory (IAXO) is a large-scale 4th generation helioscope. As its primary physics goal, IAXO will look for solar axions or ALPs with a signal to backgro…

Particle physicsPhysics - Instrumentation and Detectorssolar axion[PHYS.ASTR.IM]Physics [physics]/Astrophysics [astro-ph]/Instrumentation and Methods for Astrophysic [astro-ph.IM]experimental methodsDark matterFOS: Physical sciences7. Clean energyString (physics)Standard Modelaxion helioscopedesign [detector]International Axion Observatory (IAXO)ObservatoryPeccei-Quinn mechanismDark Matterdetector design[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental TechniquesAxionsun-tracking systemsphysics.ins-detactivity reportdetector: designPhysicsinstrumentationHelioscopeLarge Hadron Colliderdetectorsolar [axion]DESYInstrumentation and Detectors (physics.ins-det)[PHYS.ASTR.SR]Physics [physics]/Astrophysics [astro-ph]/Solar and Stellar Astrophysics [astro-ph.SR]IAXOmagnetopticsaxion: solar
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Improved luminosity determination in pp collisions at root s=7 TeV using the ATLAS detector at the LHC

2013

The luminosity calibration for the ATLAS detector at the LHC during pp collisions at sqrt(s) = 7 TeV in 2010 and 2011 is presented. Evaluation of the luminosity scale is performed using several luminosity-sensitive detectors, and comparisons are made of the long-term stability and accuracy of this calibration applied to the pp collisions at sqrt(s) = 7 TeV. A luminosity uncertainty of Delta L/L = +/- 3.5% is obtained for the 47 pb-1 of data delivered to ATLAS in 2010, and an uncertainty of Delta L/L = +/- 1.8% is obtained for the 5.5 fb-1 delivered in 2011.

Particle physicsPhysics and Astronomy (miscellaneous)530 PhysicsAtlas detectorPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsInteraction-Point01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Atlas (anatomy)0103 physical sciencesmedicineCalibration[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fysikddc:530High Energy Physics010306 general physicsNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Engineering (miscellaneous)PhysicsLarge Hadron ColliderLuminosity (scattering theory)Sensors010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleDetectorFísicaBeamATLASmedicine.anatomical_structureExperimental High Energy PhysicsPhysical SciencesHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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Determination of the muonic branching ratio of the W boson and its total width via cross-section measurements at the Tevatron and LHC

2016

The total $W$-boson decay width $\Gamma_W$ is an important observable which allows testing of the standard model. The current world average value is based on direct measurements of final state kinematic properties of $W$-boson decays, and has a relative uncertainty of 2%. The indirect determination of $\Gamma_W$ via the cross-section measurements of vector-boson production can lead to a similar accuracy. The same methodology leads also to a determination of the leptonic branching ratio. This approach has been successfully pursued by the CDF and D0 experiments at the Tevatron collider, as well as by the CMS collaboration at the LHC. In this paper we present for the first time a combination o…

Particle physicsPhysics and Astronomy (miscellaneous)HadronTevatronFOS: Physical sciences01 natural sciencesStandard Modellaw.inventionHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)law0103 physical sciences010306 general physicsColliderEngineering (miscellaneous)PhysicsLarge Hadron Collider010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyObservableHigh Energy Physics - PhenomenologyProduction (computer science)High Energy Physics::ExperimentParticle Physics - ExperimentEuropean Physical Journal C
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The Z boson spin observables as messengers of new physics

2017

We demonstrate that the 8 multipole parameters describing the spin state of the $Z$ boson are able to disentangle known $Z$ production mechanisms and signals from new physics at the LHC. They can be extracted from appropriate asymmetries in the angular distribution of lepton pairs from the $Z$ boson decay. The power of this analysis is illustrated by (i) the production of $Z$ boson plus jets; (ii) $Z$ boson plus missing transverse energy; (iii) $W$ and $Z$ bosons originating from the two-body decay of a heavy resonance.

Particle physicsPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelFOS: Physical scienceslcsh:Astrophysics01 natural sciencesResonance (particle physics)Light Supersymmetric ParticleHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Standard Model Predictionlcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Spin-½BosonCondensed Matter::Quantum GasesPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyAngular DistributionCharged LeptonObservable3. Good healthHigh Energy Physics - PhenomenologyLarge Hadron Colliderlcsh:QC770-798High Energy Physics::ExperimentMultipole expansionLeptonThe European Physical Journal C
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Search for an excess of events with an identical flavour lepton pair and significant missing transverse momentum in root s=7 TeV proton-proton collis…

2011

Results are presented of a search for supersymmetric particles decaying into final states with significant missing transverse momentum and exactly two identical flavour leptons (e or mu) of opposite charge in sqrt{s}=7 TeV collisions at the Large Hadron Collider. This channel is particularly sensitive to supersymmetric particle cascade decays producing flavour correlated lepton pairs. Flavour uncorrelated backgrounds are subtracted using a sample of opposite flavour lepton pair events. Observation of an excess beyond Standard Model expectations following this subtraction procedure would offer one of the best routes to measuring the masses of supersymmetric particles. In a data sample corres…

Particle physicsPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelFlavourSupergauge TransformationsFOS: Physical sciencesddc:500.2Parameter space01 natural sciences530Settore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pionsparticle: cascade decay ; sparticle: search for ; electron: pair production ; muon: pair production ; p p: inelastic scattering ; transverse momentum: missing-energy ; supersymmetry: parameter space ; CERN LHC Coll ; new physics ; ATLAS ; dilepton: mass spectrum ; experimental results ; 7000 GeV-cmsPions0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]FysikHigh Energy Physics010306 general physicsEngineering (miscellaneous)PhysicsLarge Hadron ColliderScience & TechnologyATLAS detector010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyATLASGeneratorsCascadeTransverse momentumPhysical SciencesExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - ExperimentLeptonModel
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