Search results for " Collider"

showing 10 items of 1415 documents

Minimal supersymmetric inverse seesaw: neutrino masses, lepton flavour violation and LHC phenomenology

2009

We study neutrino masses in the framework of the supersymmetric inverse seesaw model. Different from the non-supersymmetric version a minimal realization with just one pair of singlets is sufficient to explain all neutrino data. We compute the neutrino mass matrix up to 1-loop order and show how neutrino data can be described in terms of the model parameters. We then calculate rates for lepton flavour violating (LFV) processes, such as mu -> e gamma and chargino decays to singlet scalar neutrinos. The latter decays are potentially observable at the LHC and show a characteristic decay pattern dictated by the same parameters which generate the observed large neutrino angles.

Nuclear and High Energy PhysicsParticle physicsSupersymmetric Standard ModelPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciences01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)CharginoSeesaw molecular geometry0103 physical sciencesNeutrino Physics010306 general physicsParticle Physics - PhenomenologyPhysicsLarge Hadron Collider010308 nuclear & particles physicsRare DecaysHigh Energy Physics::PhenomenologyFísicaObservableMass matrixHigh Energy Physics - PhenomenologyBeyond Standard ModelHigh Energy Physics::ExperimentNeutrinoPhenomenology (particle physics)Lepton
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Consistent searches for SMEFT effects in non-resonant dijet events

2018

We investigate the bounds which can be placed on generic new-physics contributions to dijet production at the LHC using the framework of the Standard Model Effective Field Theory, deriving the first consistently-treated EFT bounds from non-resonant high-energy data. We recast an analysis searching for quark compositeness, equivalent to treating the SM with one higher-dimensional operator as a complete UV model. In order to reach consistent, model-independent EFT conclusions, it is necessary to truncate the EFT effects consistently at order $1/\Lambda^2$ and to include the possibility of multiple operators simultaneously contributing to the observables, neither of which has been done in prev…

Nuclear and High Energy PhysicsParticle physicsTevatronFOS: Physical sciencesParameter space01 natural sciencesHigh Energy Physics - ExperimentStandard ModelHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Perturbative QCD0103 physical sciencesEffective field theorylcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsLinear combinationPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyEffective Field TheoriesTechnicolor and Composite ModelsObservableWeinberg angleHigh Energy Physics - PhenomenologyBeyond Standard Modellcsh:QC770-798Journal of High Energy Physics
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Observation of Exclusive Dijet Production at the Fermilab Tevatron p-pbar Collider

2007

We present the first observation and cross section measurement of exclusive dijet production in pbar-p interactions, pbar + p --> pbar + dijet + p. Using a data sample of 310 pb-1 collected by the Run II Collider Detector at Fermilab at sqrt{s}=1.96 TeV, exclusive cross sections for events with two jets of transverse energy ET >= 10 GeV have been measured as a function of minimum ET(jet). The exclusive signal is extracted from fits to data distributions based on Monte Carlo simulations of expected dijet signal and background shapes. The simulated background distribution shapes are checked in a study of a largely independent data sample of 200 pb-1 of b-tagged jet events, where exclusi…

Nuclear and High Energy PhysicsParticle physicsTevatronFOS: Physical sciencesddc:500.201 natural scienceslaw.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decaylaw0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsColliderPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::Phenomenology13.87.Ce 12.38.Qk 12.40.NnHiggs boson_Production (computer science)High Energy Physics::ExperimentCollider Detector at FermilabEnergy (signal processing)
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Improved measurements of cross sections and asymmetries at the Z0 resonance

1994

During the 1992 running period of the LEP e+e- collider, the DELPHI experiment accumulated approximately 24 pb-1 of data at the Z0 peak. The decays into hadrons and charged leptons have been analysed to give values for the cross sections and leptonic forward-backward asymmetries which are significantly improved with respect to those previously published by the DELPHI collaboration. Incorporating these new data, more precise values for the Z0 resonance parameters are obtained from model-independent fits. The results are interpreted within the framework of the Standard Model, yielding for the top quark mass m(t) = 157(-48)+36(expt.)-20(+19)(Higgs) GeV, and for the effective mixing angle sin2 …

Nuclear and High Energy PhysicsParticle physicsTop quarkLUND MONTE-CARLOElectron–positron annihilationLEP-SLC ENERGIESElementary particle7. Clean energy01 natural sciencesJET FRAGMENTATIONStandard ModelPHYSICSNuclear physicsBHABHA SCATTERINGParticle decay0103 physical sciencesPROGRAM[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RADIATIVE-CORRECTIONSZ0010306 general physicsDELPHIPhysicsLOWEST-ORDER CALCULATIONScross section010308 nuclear & particles physicsDELPHI; Bhabha scattering; cross section; Z0High Energy Physics::PhenomenologyLARGE ELECTRON POSITRON COLLIDERLUND MONTE-CARLO; ELECTRON-POSITRON COLLISIONS; LOWEST-ORDER CALCULATIONS; LEP-SLC ENERGIES; BHABHA SCATTERING; RADIATIVE-CORRECTIONS; JET FRAGMENTATION; PROGRAM; PHYSICSPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHILarge Electron–Positron ColliderHiggs bosonPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentELECTRON-POSITRON COLLISIONSParticle Physics - ExperimentLepton
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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 --> W+b W-bbar --> 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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The HiggsTools handbook: a beginners guide to decoding the Higgs sector

2018

This report summarises some of the activities of the HiggsTools initial training network working group in the period 2015–2017. The main goal of this working group was to produce a document discussing various aspects of state-of-the-art Higgs physics at the large hadron collider (LHC) in a pedagogic manner. The first part of the report is devoted to a description of phenomenological searches for new physics (NP) at the LHC. All of the available studies of the couplings of the new resonance discovered in 2012 by the ATLAS and CMS experiments (Aad et al (ATLAS Collaboration) 2012 Phys. Lett. B 716 1–29; Chatrchyan et al (CMS Collaboration) 2012 Phys. Lett. B 716 30–61) conclude that it is com…

Nuclear and High Energy PhysicsParticle physicsTop quarkcoupling [Higgs particle]Higgs particle: decayHiggs bosonPhysics beyond the Standard Modelmomentum spectrum [transverse momentum]01 natural sciencesStandard ModelHiggs sectortransverse momentum: momentum spectrumeffective field theoryeffective field theories; Higgs boson; Higgs momentum distributions; LHC physics; new physics searchessearch for [new physics][ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]0103 physical sciencesEffective field theory[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]effective field theoriesddc:530effective field theorie010306 general physicsMonte CarloPhysicsLHC physicLarge Hadron ColliderHiggs particle: coupling010308 nuclear & particles physicsHiggs momentum distributionsnew physics: search forElectroweak interactionHigh Energy Physics::PhenomenologyLHC physicsnew physics searchedecay [Higgs particle]two-photon [final state]Higgs momentum distributionproduction [Higgs particle]CERN LHC CollHiggs particle: production[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Higgs bosonnew physics searches[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentfinal state: two-photon
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Inclusive production of ρ0(770), f0(980) and f2(1270) mesons in νμ charged current interactions

2001

The inclusive production of the meson resonances $\rho^{0}(770)$, $f_0(980)$ and $f_2(1270)$ in neutrino-nucleus charged current interactions has been studied with the NOMAD detector exposed to the wide band neutrino beam generated by 450 GeV protons at the CERN SPS. For the first time the $f_{0}(980)$ meson is observed in neutrino interactions. The statistical significance of its observation is 6 standard deviations. The presence of $f_{2}(1270)$ in neutrino interactions is reliably established. The average multiplicity of these three resonances is measured as a function of several kinematic variables. The experimental results are compared to the multiplicities obtained from a simulation b…

Nuclear and High Energy PhysicsParticle physics[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]MesonPhysics::Instrumentation and DetectorsNuclear TheoryNeutrino beam01 natural sciences7. Clean energyHigh Energy Physics - Experiment0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Wide bandNuclear Experiment010306 general physicsSimulation basedCharged currentPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaMultiplicity (mathematics)High Energy Physics::ExperimentNeutrinoParticle Physics - ExperimentNuclear Physics B
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The beam and detector for the NA48 neutral kaon CP violation experiment at CERN

2007

The beam and detector, used for the NA48 experiment, devoted to the measurement of Re (ε{lunate}′ / ε{lunate}), and for the NA48/1 experiment on rare KS and neutral hyperon decays, are described. © 2007 Elsevier B.V. All rights reserved.

Nuclear and High Energy PhysicsParticle physicsacceleratoriNA62 experiment01 natural sciencesLIQUID-KRYPTON CALORIMETERDECAYSNOfasci di particelleKaon beamsNuclear physicsDRIFT CHAMBER ELECTRONICSCERNViolazione di CP0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Kaon decaysdetector; CP violation; Kaon decays010306 general physicsInstrumentation07.05.Fb; 13.20.Eb; 29.40.Vj; 29.27.EgPhysicsCalorimeterLarge Hadron ColliderdetectorCRYSTAL010308 nuclear & particles physicsLIQUID-KRYPTON CALORIMETER; DRIFT CHAMBER ELECTRONICS; PROTON TAGGING DETECTOR; PC FARM; TRIGGER; SYSTEM; READOUT; DECAYS; PERFORMANCE; CRYSTALDetectorPC FARMHyperonNA48 experimentDetectorsMagnetic spectrometerPERFORMANCErivelatoriREADOUTkaon decayCalorimeterTriggerCP violationfasci di particelle; acceleratori; CERN; Violazione di CP; rivelatori; kaon decayCP violationHigh Energy Physics::ExperimentParticle Physics - ExperimentPROTON TAGGING DETECTORSYSTEMBeam (structure)
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Measurement of the Spin Structure of the Deuteron in the DIS Region

2005

We present a new measurement of the longitudinal spin asymmetry A_1^d and the spin-dependent structure function g_1^d of the deuteron in the range 1 GeV^2 < Q^2 < 100 GeV^2 and 0.004< x <0.7. The data were obtained by the COMPASS experiment at CERN using a 160 GeV polarised muon beam and a large polarised 6-LiD target. The results are in agreement with those from previous experiments and improve considerably the statistical accuracy in the region 0.004 < x < 0.03.

Nuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectFOS: Physical sciencesSpin structure01 natural sciencesAsymmetryCOMPASSHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)deep inelastic scatteringstructure function0103 physical sciencesCOMPASS experiment010306 general physicsNuclear Experimentmedia_commonSpin-½PhysicsLarge Hadron ColliderMuon010308 nuclear & particles physicsDeep inelastic scatteringstructure function; COMPASS; DEEP INELASTIC-SCATTERINGstructure functionsDEEP INELASTIC-SCATTERINGHigh Energy Physics::ExperimentParticle Physics - ExperimentBeam (structure)
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Jet evolution in a dense medium: event-by-event fluctuations and multi-particle correlations

2017

International audience; We study the gluon distribution produced via successive medium-induced branchings by an energetic jet propagating through a weakly-coupled quark-gluon plasma. We show that under suitable approximations, the jet evolution is a Markovian stochastic process, which is exactly solvable. For this process, we construct exact analytic solutions for all the n-point correlation functions describing the gluon distribution in the space of energy [M. A. Escobedo, E. Iancu, Event-by-event fluctuations in the medium-induced jet evolution, JHEP 05 (2016) 008. arXiv: arXiv:1601.03629 , doi: http://dx.doi.org/10.1007/JHEP05(2016)008 , M. A. Escobedo, E. Iancu, Multi-particle correlati…

Nuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectenergy lossMarkov chainKNOformula01 natural sciencesAsymmetryStandard deviationjet0103 physical sciencespropagationscaling: KNOmultiplicityStatistical physicscorrelation function010306 general physicsScalingquark gluon: plasmaBranching processmedia_commonPhysicsLarge Hadron Collidergluon: distribution functionta114Markovian stochastic process010308 nuclear & particles physicsStochastic processfluctuationdijet: asymmetryPlasmajet: asymmetrynucleus nucleus: scatteringGluonwide-anglepath lengthCERN LHC Colljet: energy lossnuclear mattercorrelationevolution equation[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentheavy ion: colliding beamsPhenomenology (particle physics)jet evolution
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