Search results for "collider"

showing 10 items of 1690 documents

Combination of the Searches for Pair-Produced Vectorlike Partners of the Third-Generation Quarks at s=13  TeV with the ATLAS Detector

2018

A combination of the searches for pair-produced vectorlike partners of the top and bottom quarks in various decay channels (T -> Zt/Wb/Ht, B -> Zb/Wt/Hb) is performed using 36.1 fb(-1) of pp ...

QuarkPhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsAtlas detectorGeneral Physics and AstronomyElementary particle01 natural sciencesThird generation3. Good healthmedicine.anatomical_structureAtlas (anatomy)Isospin0103 physical sciencesmedicine010306 general physicsTellurium compoundsPhysical Review Letters
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Search for Scalar Charm Quark Pair Production inppCollisions ats=8  TeVwith the ATLAS Detector

2015

The results of a dedicated search for pair production of scalar partners of charm quarks are reported. The search is based on an integrated luminosity of 20.3 fb(-1) of pp collisions at root s = 8 TeV recorded with the ATLAS detector at the LHC. The search is performed using events with large missing transverse momentum and at least two jets, where the two leading jets are each tagged as originating from c quarks. Events containing isolated electrons or muons are vetoed. In an R-parity-conserving minimal super-symmetric scenario in which a single scalar-charm state is kinematically accessible, and where it decays exclusively into a charm quark and a neutralino, 95% confidence-level upper li…

QuarkPhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGeneral Physics and Astronomy7. Clean energy01 natural sciencesCharm quarkNuclear physicsmedicine.anatomical_structurePair productionPionAtlas (anatomy)0103 physical sciencesNeutralinomedicineHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsMinimal Supersymmetric Standard ModelPhysical Review Letters
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A search for quarks in the CERN SPS neutrino beam

1978

Quarks and leptons are the only pointlike particles known so far. However, a search for a proton-breaking mechanism in high-energy neutrino-nucleon interactions had never been performed. We present here the results of the first experiment in this field.

QuarkPhysicsParticle physicsLarge Hadron ColliderField (physics)Settore FIS/01 - Fisica SperimentaleNuclear TheoryHigh Energy Physics::PhenomenologyElementary particleNeutrino beamParticle detectorGluonNuclear physicsFree quark searchElementary Particles SPS CERNHigh Energy Physics::ExperimentNuclear ExperimentParticle Physics - ExperimentLeptonIl Nuovo Cimento A
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Open-charm production measurements in pp, 1 p-Pb and Pb-Pb collisions with ALICE at the LHC

2017

ALICE (A Large Ion Collider Experiment) is designed to study the strongly in teracting matter, the Quark-Gluon Plasma (QGP), created in heavy-ion collisions at LHC energies. Charm and beauty quarks are powerful probes to study the QGP. Produced in hard partonic scattering processes on a short time scale, they are expected to traverse the QCD medium, interacting with its constituents and losing energy through radiative and collisional processes. In ALICE, open-charm production is studied through the reconstruction of the hadronic decays of D 0 , D + , D *+ and D s + mesons at mid-rapidity. High precision tracking, good vertexing capabilities and excellent particle identification offered by A…

QuarkPhysicsParticle physicsLarge Hadron ColliderMeson010308 nuclear & particles physicsPhysicsQC1-999Nuclear TheoryHigh Energy Physics::PhenomenologyHadron01 natural sciences7. Clean energyParticle identificationlaw.inventionNuclear physicslaw0103 physical sciencesQuark–gluon plasmaNuclear Physics - ExperimentHigh Energy Physics::ExperimentCharm (quantum number)Nuclear Experiment010306 general physicsColliderEPJ Web of Conferences
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Constraints for the nuclear sea quark distributions from the Drell–Yan process at the SPS

2000

Nuclear modifications to the Drell-Yan dilepton production cross sections in p+A and A+A collisions in the leading twist approximation are caused by nuclear effects in the parton distributions of bound nucleons. For non-isoscalar nuclei, isospin corrections must also be considered. We calculate these effects for p+A and Pb+Pb collisions at CERN SPS energies. Our goal is to place constraints on nuclear effects in sea quark distributions in the region x > 0.2. We show that the net nuclear corrections remain small for p+A collisions at E_lab=450 GeV. However, in Pb+Pb collisions at E_lab=158 AGeV, effects of > 20% are predicted at large M. The data collected by the NA50 collaboration cou…

QuarkPhysicsParticle physicsLarge Hadron ColliderNuclear TheoryPhysics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyNuclear TheoryEMC effectFOS: Physical sciencesDrell–Yan processPartonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)IsospinHigh Energy Physics::ExperimentTwistNuclear ExperimentNucleonEngineering (miscellaneous)The European Physical Journal C
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Measurements of the Total and Differential Higgs Boson Production Cross Sections Combining theH→γγandH→ZZ*→4ℓDecay Channels ats=8  TeVwith the ATLAS …

2015

Measurements of the total and differential cross sections of Higgs boson production are performed using 20.3 fb(-1) of pp collisions produced by the Large Hadron Collider at a center-of-mass energy of root s = 8 TeV and recorded by the ATLAS detector. Cross sections are obtained from measured H -> gamma gamma and H -> ZZ*. 4l event yields, which are combined accounting for detector efficiencies, fiducial acceptances, and branching fractions. Differential cross sections are reported as a function of Higgs boson transverse momentum, Higgs boson rapidity, number of jets in the event, and transverse momentum of the leading jet. The total production cross section is determined to be sigma(pp -> …

QuarkPhysicsParticle physicsLarge Hadron ColliderPhoton010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyDetectorGeneral Physics and AstronomySigma7. Clean energy01 natural sciencesNuclear physics0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentRapidity010306 general physicsPhysical Review Letters
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LHC diphoton resonance from gauge symmetry

2015

Motivated by what is possibly the first sign of new physics seen at the LHC, the diphoton excess at $750$ GeV in ATLAS and CMS, we present a model that provides naturally the necessary ingredients to explain the resonance. The simplest phenomenological explanation for the diphoton excess requires a new scalar state, $X(750)$, as well as additional vector-like (VL) fermions introduced in an ad-hoc way in order to enhance its decays into a pair of photons and/or increase its production cross-section. We show that the requiered VL quarks and their couplings can emerge naturally from a complete framework based on the $SU(3)_L \otimes U(1)_\mathcal{X}$ gauge symmetry.

QuarkPhysicsParticle physicsLarge Hadron ColliderPhoton010308 nuclear & particles physicsPhysics beyond the Standard ModelScalar (mathematics)FOS: Physical sciencesFermionParameter space01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsGauge symmetryPhysical Review D
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Charge asymmetry in hadroproduction of heavy quarks

1998

A sizeable difference in the differential production cross section of top and antitop quarks, respectively, is predicted for hadronically produced heavy quarks. It is of order $\alpha_s$ and arises from the interference between charge odd and even amplitudes respectively. For the TEVATRON it amounts to approximately 5-10% in the region where the cross section is large and could therefore be measured in the next round of experiments. At the LHC the asymmetry can be studied by selecting appropriately chosen kinematical regions.

QuarkPhysicsParticle physicsLarge Hadron Collidermedia_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronFísicaGeneral Physics and AstronomyOrder (ring theory)FOS: Physical sciencesCharge (physics)AsymmetryNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Production (computer science)High Energy Physics::ExperimentFermilabmedia_common
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Cold-Nuclear-Matter Effects on Heavy-Quark Production ind+AuCollisions atsNN=200  GeV

2012

The PHENIX experiment has measured electrons and positrons at midrapidity from the decays of hadrons containing charm and bottom quarks produced in d+Au and p+p collisions at sqrt[S(NN)]=200 GeV in the transverse-momentum range 0.85 ≤ p(T)(e) ≤ 8.5 GeV/c. In central d+Au collisions, the nuclear modification factor R(dA) at 1.5<p(T)<5 GeV/c displays evidence of enhancement of these electrons, relative to those produced in p+p collisions, and shows that the mass-dependent Cronin enhancement observed at the Relativistic Heavy Ion Collider extends to the heavy D meson family. A comparison with the neutral-pion data suggests that the difference in cold-nuclear-matter effects on light- and heavy-…

QuarkPhysicsParticle physicsMeson010308 nuclear & particles physicsNuclear TheoryHigh Energy Physics::PhenomenologyHadronGeneral Physics and AstronomyElectronNuclear matter01 natural sciences7. Clean energyNuclear physics0103 physical sciencesD mesonHigh Energy Physics::ExperimentCharm (quantum number)Nuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderPhysical Review Letters
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Search for New Phenomena in Final States with Two Leptons and One or No b -Tagged Jets at s=13  TeV Using the ATLAS Detector

2021

A search for new phenomena is presented in final states with two leptons and one or no $b$-tagged jets. The event selection requires the two leptons to have opposite charge, the same flavor (electrons or muons), and a large invariant mass. The analysis is based on the full Run-2 proton-proton collision dataset recorded at a center-of-mass energy of $\sqrt{s} = 13$ TeV by the ATLAS experiment at the LHC, corresponding to an integrated luminosity of 139 fb$^{-1}$. No significant deviation from the expected background is observed in the data. A four-fermion contact interaction between two quarks ($b,s$) and two leptons ($ee$ or $\mu\mu$), inspired by the $B$-meson decay anomalies, is used as a…

QuarkPhysicsParticle physicsMuonLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyATLAS experimentGeneral Physics and AstronomyLambdaCoupling (probability)7. Clean energy01 natural sciences0103 physical sciencesHigh Energy Physics::ExperimentInvariant mass010306 general physicsLeptonPhysical Review Letters
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