Search results for "Boson production"

showing 10 items of 145 documents

Probing the small- x nuclear gluon distributions with isolated photons at forward rapidities in p+Pb collisions at the LHC

2014

Inclusive direct photon production in p+Pb collisions at the LHC is studied within the NLO perturbative QCD. Our aim is to quantify the dominant $x$ regions probed at different rapidities and to identify the best conditions for testing the nuclear gluon parton distribution functions (nPDFs) at small $x$. A comparison to the inclusive pion production reveals that from these two processes the photons carry more sensitivity to the small-$x$ partons and that this sensitivity can be further increased by imposing an isolation cut for the photon events. The details of the isolation criteria, however, seem to make only a small difference to the studied $x$ sensitivity and have practically no effect…

Particle physicsNuclear and High Energy PhysicsPhotonmedia_common.quotation_subjectFRAGMENTATION FUNCTIONSeducationFOS: Physical sciencesPREDICTIONSPartonPROTONAsymmetry114 Physical sciencesPionHigh Energy Physics - Phenomenology (hep-ph)PERTURBATIVE QCDSCATTERINGHadronic CollidersNuclear Experimentmedia_commonPhysicsBOSON PRODUCTIONPROMPT PHOTONLarge Hadron Colliderta114QUARKPerturbative QCDHeavy Ion PhenomenologyGluonHigh Energy Physics - PhenomenologyDistribution functionPARTON DISTRIBUTIONSHigh Energy Physics::ExperimentPDFSJHEP
researchProduct

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
researchProduct

"Table 19: Mass distribution, 2 tag, mbb window 130" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in th…

2018

The mass distribution of the llbb system used in the fit to derive the limits for the mbb window centered at 130 GeV for the nb = 2 (2 tag) category.

Z0 --> MU+ MU-2HDMZ0 --> E+ E-13000.0P P --> HIGGSHIGGS --> BQ BQBARgluon-gluon fusionmass distributionb-associated productionMHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
researchProduct

"Table 3: Cross-section limits b-associated production" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in…

2018

The cross section times BR(A->ZH) times BR(H->bb) limits for a narrow width A boson produced in association with b-quarks. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The result refers to the combination of the nb=2 and nb>=3 categories.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0CLSb-associated productioncross section limitsHiggs boson productionHIGGS --> Z0 HIGGS
researchProduct

"Table 1: Signal Efficiency" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final st…

2018

The signal efficiency for the production modes (gluon-gluon fusion and b-associated production) and the signal regions used in the analysis. The efficiency denominator has the total number of generated MC events. The numerator includes the events passing the full signal region selection, including the mbb window cuts. The table shows for each signal mass pair (mA, mH) 3 efficiencies corresponding to the two production modes in the two categories, 2tag and 3tag. These corresponds to "nb = 2 category" and "nb >= 3 category", respectively, of the preprint. No numbers for gluon-gluon fusion in the 3tag category are provided since those are not used in the analysis. The efficiencies are given…

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0EFFHiggs boson productionHIGGS --> Z0 HIGGSselection efficiency
researchProduct

"Table 18: Cross-section limits flipped tanb 20" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\…

2018

The cross section times BR(A->ZH) times BR(H->bb) limits for an A boson in the flipped, tanbeta 20, 2HDM. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used. For flipped both gluon-gluon fusion and b-associated production are used and the nb=2 and nb>=3 categories are combined.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionCLSb-associated productioncross section limitsHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
researchProduct

"Table 8: Cross-section limits type-II tanb 1" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\el…

2018

The cross section times BR(A->ZH) times BR(H->bb) limits for an A boson in the type-II, tanbeta 1, 2HDM. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used. For type-II both gluon-gluon fusion and b-associated production are used and the nb=2 and nb>=3 categories are combined.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionCLSb-associated productioncross section limitsHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
researchProduct

"Table 16: Cross-section limits flipped tanb 5" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\e…

2018

The cross section times BR(A->ZH) times BR(H->bb) limits for an A boson in the flipped, tanbeta 5, 2HDM. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used. For flipped both gluon-gluon fusion and b-associated production are used and the nb=2 and nb>=3 categories are combined.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionCLSb-associated productioncross section limitsHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
researchProduct

"Table 10: Cross-section limits type-II tanb 10" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\…

2018

The cross section times BR(A->ZH) times BR(H->bb) limits for an A boson in the type-II, tanbeta 10, 2HDM. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used. For type-II both gluon-gluon fusion and b-associated production are used and the nb=2 and nb>=3 categories are combined.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionCLSb-associated productioncross section limitsHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
researchProduct

"Table 17: Cross-section limits flipped tanb 10" of "Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\…

2018

The cross section times BR(A->ZH) times BR(H->bb) limits for an A boson in the flipped, tanbeta 10, 2HDM. For each signal point, characterised by the mass pair (mA, mH), two limits are provided, the observed and the expected. The correct width as predicted by this particular parameter choice of the 2HDM is used. For flipped both gluon-gluon fusion and b-associated production are used and the nb=2 and nb>=3 categories are combined.

Z0 --> MU+ MU-Z0 --> E+ E-2HDMP P --> HIGGSHIGGS --> BQ BQBAR13000.0gluon-gluon fusionCLSb-associated productioncross section limitsHiggs boson productionHIGGS --> Z0 HIGGSgluon fusion
researchProduct