Search results for "Root-s=7"

showing 10 items of 17 documents

Measurement of K⁎(892)± production in inelastic pp collisions at the LHC

2022

The first results on K⁎(892)± resonance production in inelastic pp collisions at LHC energies of s=5.02, 8, and 13 TeV are presented. The K⁎(892)± has been reconstructed via its hadronic decay channel K⁎(892)→±KS0+π± with the ALICE detector. Measurements of transverse momentum distributions, pT-integrated yields, and mean transverse momenta for charged K⁎(892) are found to be consistent with previous ALICE measurements for neutral K⁎(892) within uncertainties. For pT>1 GeV/c the K⁎(892)± transverse momentum spectra become harder with increasing centre-of-mass energy from 5.02 to 13 TeV, similar to what previously observed for charged kaons and pions. For pT<1 GeV/c the K⁎(892)± yield does n…

Nuclear and High Energy PhysicsMultiplicity dependencePionhiukkasfysiikkaPb collisionsKaonRoot-s=7Proton-proton collisions
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Measurements of Higgs boson production and couplings in diboson final states with the ATLAS detector at the LHC

2013

We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; ISF, MINERVA, GIF, DIP and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW, Poland; GRICES and FCT, Portu…

Standard Modeldilepton: mass spectrumCiencias Físicas01 natural sciences7. Clean energySettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentHiggs particle: hadroproduction//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)vector boson: fusion[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]QCBosonPhysicsHIGGS BOSONLarge Hadron Collidervector boson: pair productiontransverse energy: missing-energy4. EducationATLAS experimentSettore FIS/01 - Fisica SperimentaleATLAS3. Good healthMassless particleCERN LHC CollHiggs particle: massPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs boson7000: 8000 GeV-cmsFísica nuclearAtlasLhcNeutrinoHiggs particle: decay modesParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASp p: scatteringNuclear and High Energy PhysicsParticle physicsmass spectrum: (4lepton)530 PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2ATLASdetector; LHC; Higgsbosonproduction; diboson530Massless ParticlesNnlo QCDNuclear physics0103 physical sciencesFysikddc:530High Energy Physics010306 general physicsTransverse-MomentumCondensed Matter::Quantum GasesHiggs particle: couplingScience & Technologyhep-ex010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaQCD CorrectionsFermion//purl.org/becyt/ford/1.3 [https]Hadron CollidersDiboson ProductionAstronomíavector boson: leptonic decayHADRON-HADRON COLLISIONSProton-Proton CollisionsRoot-S=7 TevHiggs particle: hadroproduction ; Higgs particle: coupling ; vector boson: fusion ; p p: scattering ; CERN LHC Coll ; ATLAS ; Higgs particle: decay modes ; vector boson: pair production ; vector boson: leptonic decay ; mass spectrum: two-photon ; mass spectrum: (4lepton) ; dilepton: mass spectrum ; transverse energy: missing-energy ; Higgs particle: mass ; experimental results ; 7000: 8000 GeV-cmsExperimental High Energy PhysicsHigh Energy Physics::ExperimentCross-Sectionsmass spectrum: two-photonexperimental resultsLeptonBroken Symmetries
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Study of W Boson Production in Association with Beauty and Charm

2015

The associated production of a W boson with a jet originating from either a light parton or heavy-flavor quark is studied in the forward region using proton-proton collisions. The analysis uses data corresponding to integrated luminosities of 1.0 and 2.0  fb[superscript -1] collected with the LHCb detector at center-of-mass energies of 7 and 8 TeV, respectively. The W bosons are reconstructed using the W → μν decay and muons with a transverse momentum, p[subscript T], larger than 20 GeV in the pseudorapidity range 2.0 20  GeV and 2.2 20  GeV. The fraction of W + jet events that originate from beauty and charm quarks is measured, along with the charge asymmetries of the W + b and W + c produ…

PartonATLAS DETECTOR01 natural sciencesPRODUCTION CROSS-SECTIONSHigh Energy Physics - ExperimentPhysics Particles & FieldsSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Charm (quantum number)Nuclear ExperimentBosonPhysicsPhysicsParticle physics14.70.FmPseudorapidityPhysical Sciences13.87.-aLHCParticle Physics - ExperimentQuarkNuclear and High Energy PhysicsParticle physicsCOLLISIONSAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesLHCb - Abteilung HofmannHadronsAstronomy & AstrophysicsCharm quarkStandard ModelNOJets in large-Q2 scatteringNuclear physicsRATIO0103 physical sciencesSDG 7 - Affordable and Clean Energy010306 general physicsLarge Hadron Collider (France and Switzerland)MuonScience & Technology/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyROOT-S=7 TEV010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGran Col·lisionador d'HadronsHEPLHCbJETSW bosonHigh Energy Physics::ExperimentFísica de partículesExperimentsDECAY
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Search for supersymmetry in events with large missing transverse momentum, jets, and at least one tau lepton in 7 TeV proton-proton collision data wi…

2012

A search for supersymmetry (SUSY) in events with large missing transverse momentum, jets, and at least one hadronically decaying τ lepton, with zero or one additional light lepton (e/μ), has been performed using 4.7 fb[superscript −1] of proton-proton collision data at √s = 7 TeV recorded with the ATLAS detector at the Large Hadron Collider. No excess above the Standard Model background expectation is observed and a 95 % confidence level visible cross-sectionupper limit for new phenomena is set. In the framework of gauge-mediated SUSY-breaking models, lower limits on the mass scale Λ are set at 54 TeV in the regions where the [bar over τ]1 is the next-to-lightest SUSY particle (tanβ > 20). …

CollisionPhysics and Astronomy (miscellaneous)Atlas detectorLarge hadron colliderNuclear physicsE(+)E(-) CollisionsParameter space7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)ExtensionNaturvetenskap[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesDetectors de radiacióTransverse momentumddc:539PhysicsLarge Hadron ColliderAtlas (topology)PhysicsSettore FIS/01 - Fisica SperimentaleParticle physicsSupersymmetryATLASTransverse momentumComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCNatural SciencesParticle Physics - ExperimentParticle physicsCiências Naturais::Ciências FísicasAtlas detectorSupergauge Transformations:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2530Partícules (Física nuclear)LeptonNuclear physicsParameter space0103 physical sciencesddc:530High Energy PhysicsEngineering (miscellaneous); Physics and Astronomy (miscellaneous)010306 general physicsEngineering (miscellaneous)Hadron-Hadron ScatteringScience & Technology010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaQC0793Breaking TopologiesCollisionCollaborationGeneratorsOf-Mass EnergiesHADRON-HADRON COLLISIONSRoot-S=7 TevCol·lisions (Física nuclear)Experimental High Energy PhysicsHigh Energy Physics::ExperimentSupersymmetryModelLepton
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Combination of D0 measurements of the top quark mass

2017

We present a combination of measurements of the top quark mass by the D0 experiment in the lepton+jets and dilepton channels. We use all the data collected in Run I (1992--1996) at $\sqrt s=1.8$ TeV and Run II (2001--2011) at $\sqrt s=1.96$ TeV of the Tevatron $p \bar{p}$ collider, corresponding to integrated luminosities of 0.1 fb$^{-1}$ and 9.7 fb$^{-1}$, respectively. The combined result is: $m_t = 174.95 \pm0.40\,{\rm(stat)} \pm 0.64\,{\rm(syst)}\,{\rm{GeV}}=174.95 \pm 0.75 \, {\rm{GeV}}$.

Top quarkQ007TPtop: mass: measured((n)jet dilepton) [final state]Tevatronpair production [top]01 natural scienceslaw.inventionPhysics Particles & FieldsHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)lawDZERO[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Batavia TEVATRON CollNuclear ExperimentPhysicsscattering [anti-p p]PhysicsGLOBAL QCD ANALYSISDetectorROOT-S=7ATLASPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGmass: measured [top]top: pair production((n)jet lepton) [final state]Particle physics1800 GeV-cms1960 GeV-cmsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesfinal state: ((n)jet lepton)Astronomy & Astrophysicsanti-p p: colliding beamsNuclear physicsEVENTS[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]0103 physical sciencesanti-p p: scatteringddc:530Combined resultHigh Energy Physics010306 general physicsColliderDETECTORScience & TechnologyPP COLLISIONS1960 GeV-cms010308 nuclear & particles physicsfinal state: ((n)jet dilepton)hep-exHigh Energy Physics::PhenomenologyD0 experimentDIFFERENCEPARTON DISTRIBUTIONSExperimental High Energy PhysicsPhysics::Accelerator PhysicsTEVHigh Energy Physics::Experiment1800 GeV-cmscolliding beams [anti-p p]Leptonexperimental results
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Observing Higgs boson production through its decay into gamma-rays: A messenger for Dark Matter candidates

2012

In this Letter, we study the gamma-ray signatures subsequent to the production of a Higgs boson in space by dark matter annihilations. We investigate the cases where the Higgs boson is produced at rest or slightly boosted and show that such configurations can produce characteristic bumps in the gamma-ray data. These results are relevant in the case of the Standard Model-like Higgs boson provided that the dark matter mass is about 63 GeV, 109 GeV or 126 GeV, but can be generalized to any other Higgs boson masses. Here, we point out that it may be worth looking for a 63 GeV line since it could be the signature of the decay of a Standard Model-like Higgs boson produced in space, as in the case…

Particle physicsNuclear and High Energy Physics[PHYS.ASTR.HE]Physics [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]Physics beyond the Standard ModelAstrophysics::High Energy Astrophysical PhenomenaDark matterFOS: Physical sciencesNeutralino annihilationElementary particle7. Clean energy01 natural sciencesNuclear physicssymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsLight dark matterBosonPhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)010308 nuclear & particles physics[SDU.ASTR.HE]Sciences of the Universe [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]High Energy Physics::PhenomenologyScalar bosonHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Higgs bosonsymbolsHigh Energy Physics::ExperimentAstrophysics - High Energy Astrophysical PhenomenaHiggs mechanismRoot-s=7 tev
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Top-quark production in proton–nucleus and nucleus–nucleus collisions at LHC energies and beyond

2015

Single and pair top-quark production in proton-lead (p-Pb) and lead-lead (Pb-Pb) collisions at the CERN Large Hadron Collider (LHC) and future circular collider (FCC) energies, are studied with next-to-leading-order perturbative QCD calculations including nuclear parton distribution functions. At the LHC, the pair-production cross sections amount to sigma(t-tbar) = 3.4 mub in Pb-Pb at sqrt(s) = 5.5 TeV, and sigma(t-tbar) = 60 nb in p-Pb at sqrt(s) = 8.8 TeV. At the FCC energies of sqrt(s) = 39 and 63 TeV, the same cross sections are factors of 90 and 55 times larger respectively. In the leptonic final-state t-tbar --&gt; W+b W-bbar --&gt; b bbar l+l- nu+nu-, after typical acceptance and eff…

Nuclear and High Energy PhysicsParticle physicsTop quarkNuclear TheoryProtontop-quark productionFOS: Physical sciencesParton114 Physical sciences7. Clean energyFuture Circular ColliderHigh Energy Physics - ExperimentNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)CHANNELPAIRNuclear Experiment (nucl-ex)LEPTONNuclear ExperimentNuclear ExperimentParticle Physics - PhenomenologyPhysicsPP COLLISIONSLarge Hadron Colliderta114ROOT-S=7 TEVp–Pb collisionsHigh Energy Physics::PhenomenologyPerturbative QCDBOSONATLASPRODUCTION CROSS-SECTIONFINAL-STATESlcsh:QC1-999GluonHigh Energy Physics - PhenomenologyPb–Pb collisionsJETSHigh Energy Physics::Experimentlcsh:PhysicsLeptonPhysics Letters B
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Tevatron Combination of Single-Top-Quark Cross Sections and Determination of the Magnitude of the Cabibbo-Kobayashi-Maskawa Matrix Element Vtb

2015

et al.

QuarkTop quarkParticle physicsP(P)OVER-BAR COLLISIONS; JET IDENTIFICATION; ROOT-S=7 TEV; HIGGS-BOSON; CHANNEL; DETECTOR; ATLASJET IDENTIFICATIONmeasured [channel cross section]P(P)OVER-BAR COLLISIONSTevatronGeneral Physics and AstronomyFOS: Physical sciencesmeasured [cross section]Astrophysics::Cosmology and Extragalactic Astrophysicssingle production [top]7. Clean energyHigh Energy Physics - ExperimentMeasurements of cross sections for single-top-quark productionNuclear physicsproton-antiproton collisionsHigh Energy Physics - Experiment (hep-ex)Physics and Astronomy (all)CHANNELDZEROddc:550[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Batavia TEVATRON Collcross section measurementDETECTORPhysicsscattering [anti-p p]1960 GeV-cmsROOT-S=7 TEVCabibbo–Kobayashi–Maskawa matrixSigmaATLASMeasurements of cross sections for single-top-quark production; proton-antiproton collisions; cross section measurement2 [dimension]missing-energy [transverse energy]CKM matrixExperimental High Energy PhysicsHiggs bosonComputingMethodologies_DOCUMENTANDTEXTPROCESSINGCDFHigh Energy Physics::ExperimentPhysics and Astronomy (all) Nuclear and high energy physicscolliding beams [anti-p p]coupling [quark]HIGGS-BOSON
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Search for photonic signatures of gauge-mediated supersymmetry in 8TeV pp collisions with the ATLAS detector

2015

A search is presented for photonic signatures motivated by generalized models of gauge-mediated supersymmetry breaking. This search makes use of 20.3  fb[superscript −1] of proton-proton collision data at √s = 8  TeV recorded by the ATLAS detector at the LHC, and explores models dominated by both strong and electroweak production of supersymmetric partner states. Four experimental signatures incorporating an isolated photon and significant missing transverse momentum are explored. These signatures include events with an additional photon, lepton, b-quark jet, or jet activity not associated with any specific underlying quark flavor. No significant excess of events is observed above the Stand…

transverse momentum [photon]Большой адронный коллайдерCiencias FísicasPhysics beyond the Standard ModelPROTON-PROTON COLLISIONSFORTRAN CODEElementary particlesymmetry breaking [supersymmetry]gravitinoHigh Energy Physics - ExperimentMEASUREMENTSubatomär fysik//purl.org/becyt/ford/1 [https]High Energy Physics - Experiment (hep-ex)суперсимметрияSubatomic Physicsscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]HADRON COLLIDERSGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)QC8000 GeV-cmsPhysicsLarge Hadron ColliderJET ENERGYSettore FIS/01 - Fisica SperimentaleElectroweak interactionPhotonicSUPERGAUGE TRANSFORMATIONSSupersymmetryATLASbottom [jet]Supersymmetry breakingCERN LHC CollPhotonic signaturesgauge [mediation]Physical Sciencesflavor [quark]GravitinoLHCcolliding beams [p p]CIENCIAS NATURALES Y EXACTASsignatureParticle Physics - ExperimentParticle physicsNuclear and High Energy Physics530 PhysicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesстолкновение частицpair production [neutralino]530MISSING TRANSVERSE-MOMENTUMNuclear physicsGauge-mediatedphotonic signatures; gauge-mediated supersymmetry; ATLAS detectorFysikddc:530High Energy PhysicsCiencias ExactasPROTON-PROTON COLLISIONS; MISSING TRANSVERSE-MOMENTUM; JET ENERGY; MEASUREMENT; ROOT-S=7 TEV; HADRON COLLIDERS; SUPERGAUGE TRANSFORMATIONS; FORTRAN CODE; MODEL; LHC; PERFORMANCEScience & Technologyelectroweak interactionATLAS detectorROOT-S=7 TEVHigh Energy Physics::PhenomenologyFísica//purl.org/becyt/ford/1.3 [https]PERFORMANCEAstronomíaMODELgravitationmissing-energy [transverse momentum]Proton-Proton CollisionsExperimental High Energy PhysicsHigh Energy Physics::ExperimentSupersymmetryATLAS детекторexperimental resultsLepton
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Supersymmetric type-III seesaw mechanism: Lepton flavor violation and LHC phenomenology

2013

We study a supersymmetric version of the type-III seesaw mechanism considering two variants of the model: a minimal version for explaining neutrino data with only two copies of 24 superfields and a model with three generations of 24-plets. The latter predicts, in general, rates for mu -> e gamma inconsistent with experimental data. However, this bound can be evaded if certain special conditions within the neutrino sector are fulfilled. In the case of two 24-plets, lepton flavor violation constraints can be satisfied much more easily. After specifying the corresponding regions in the minimal supergravity parameter space, we show that under favorable conditions one can test the corresponding …

Nuclear and High Energy PhysicsParticle physicsMassesPhysics beyond the Standard Model01 natural sciences0103 physical sciencesRoot-S=7 tev010306 general physicsRight-handed neutrinosPhysicsLarge Hadron ColliderElectroweak010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionFísicaNon-conservationSupersymmetrySeesaw mechanismUnificationGrand unified theoriesHigh Energy Physics::ExperimentNeutrinoModel higgs-bosonDecaysPhenomenology (particle physics)LeptonStandard model
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