Search results for " Collider"

showing 10 items of 1415 documents

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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Spin on same-sign W -boson pair production

2019

We demonstrate that the LHC will be sensitive to quantum correlations between two quarks inside the proton. Same-sign W-boson pair production is the most promising channel for clear measurements of double parton scattering. The left-handed nature of the coupling between quarks and W-bosons makes it a prime probe to measure parton spin correlations. We perform a detailed analysis of double parton scattering, including relevant backgrounds. The analysis reveals that measurements comparing the rate at which two muons from W boson decays are produced in the same compared to opposite hemispheres are especially sensitive to spin correlations between two quarks inside the proton. We provide estima…

QuarkPhysicsParticle physicsMuonLarge Hadron ColliderProton010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFOS: Physical sciencesParton01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Pair production0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsSpin-½Physical Review D
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Search for heavy particles decaying into a top-quark pair in the fully hadronic final state in pp collisions at s=13  TeV with the ATLAS detector

2019

A search for new particles decaying into a pair of top quarks is performed using proton-proton collision data recorded with the ATLAS detector at the Large Hadron Collider at a center-of-mass energ ...

QuarkPhysicsParticle physicsTop quarkLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAtlas (topology)Nuclear TheoryHadronCollision01 natural sciencesGravitation0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentParticle physics experimentsNuclear Experiment010306 general physicsPhysical Review D
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Charge asymmetry of top quarks

2010

The LHC is a promising machine to discover new physics in the top sector. There are several models that predict the existence of heavy colored resonances decaying to top quarks in the TeV energy range. The production of such resonances might generate a sizable charge asymmetry of top versus antitop quarks. At the Tevatron, a 2 sigma discrepancy with the SM prediction for the forward--backward asymmetry has been found, boosting a renewed interest for this kind of models. We consider a toy model with general flavour dependent couplings of the resonance to quarks, of both vector and axial-vector kind and investigate the possible constraints on the coupling space from the measurement of the asy…

QuarkPhysicsParticle physicsToy modelLarge Hadron ColliderPhysics beyond the Standard Modelmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyFlavourTevatronFOS: Physical sciencesAsymmetryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentInvariant massmedia_commonProceedings of XVIII International Workshop on Deep-Inelastic Scattering and Related Subjects — PoS(DIS 2010)
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Cross section and longitudinal single-spin asymmetry AL for forward W±→μ±ν production in polarized p+p collisions at s=510  GeV

2018

We have measured the cross section and single-spin asymmetries from forward W±→μ±ν production in longitudinally polarized p+p collisions at s=510 GeV using the PHENIX detector at the Relativistic Heavy Ion Collider. The cross sections are consistent with previous measurements at this collision energy, while the most forward and backward longitudinal single spin asymmetries provide new insights into the sea quark helicities in the proton. The charge of the W bosons provides a natural flavor separation of the participating partons. © 2018 authors. Published by the American Physical Society.

QuarkPhysicsProton010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyParton01 natural sciences7. Clean energyAsymmetryNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentPHENIX detectorNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderBosonSpin-½media_commonPhysical Review D
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