Search results for "Large"

showing 10 items of 2197 documents

Nuclear PDF constraints from p+Pb collisions at the LHC

2015

As the current nuclear PDF analyses are mainly constrained by fixed-target Drell-Yan and deeply inelastic scattering data only the quark nuclear modifications at fairly large $x$ values are in a good control. Inclusive pion production in d+Au collisions at RHIC provides some constraints for gluons but due to the limited kinematic reach of the data the gluon modifications remain uncertain especially at small values of $x$. In this talk, we discuss how the existing data from p+Pb collisions at the LHC can improve the nuclear PDF fits and which measurements would be sensitive to the small-$x$ gluons. In particular, we consider inclusive hadron production, compare this to direct photons, and sh…

QuarkParticle physicsPhotonNuclear TheoryNuclear TheoryHadronFOS: Physical sciencesGood control02 engineering and technologyInelastic scatteringNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Pion0202 electrical engineering electronic engineering information engineering0501 psychology and cognitive sciencesnuclear PDF constraintsNuclear Experiment050107 human factorsPhysicsLarge Hadron ColliderHigh Energy Physics::Phenomenology05 social sciences020207 software engineeringGluonHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentProceedings of XXIII International Workshop on Deep-Inelastic Scattering — PoS(DIS2015)
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Search for neutral and charged Higgs bosons in $e^+ e^-$ collisions at $\sqrt{s}$= 161 GeV and 172 GeV

1998

A search for neutral and charged Higgs bosons has been performed in the data collected by the {\sc DELPHI} detector at centre-of-mass energies of 161~GeV and 172~GeV. The analysis assumes either the pair-production of charged Higgs bosons, ${\mathrm H}^{\pm}$, or the production of the lightest neutral Higgs boson, h, with either a Z or a neutral pseudoscalar Higgs boson, A. All final state topologies expected from the decay of h and A %neutral Higgs particles into hadrons or a pair of $\tau$ leptons, and from the decay of ${\mathrm H}^{\pm}$ %charged Higgs bosons into a pair of quarks or a $\tau \nu_{\tau}$ pair have been considered. %In the case of the associated production with a Z boson,…

QuarkParticle physicsPhysics and Astronomy (miscellaneous)LOWEST ORDER CALCULATIONSElectron–positron annihilationHigh Energy Physics::LatticeHadronMONTE-CARLO SIMULATIONSTANDARD MODEL2-PHOTON PROCESSES01 natural sciencesPartícules (Física nuclear)Nuclear physicsPHYSICS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RADIATIVE-CORRECTIONSNuclear Experiment010306 general physicsEngineering (miscellaneous)SUPERSYMMETRYDELPHIBosonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySupersymmetryE+E-ANNIHILATIONLARGE ELECTRON POSITRON COLLIDERMONTE-CARLO SIMULATION; LOWEST ORDER CALCULATIONS; E+E-ANNIHILATION; RADIATIVE-CORRECTIONS; 2-PHOTON PROCESSES; STANDARD MODEL; Z(0) DECAYS; PHYSICS; SUPERSYMMETRYZ(0) DECAYSPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHILarge Electron–Positron ColliderHiggs bosonPARTICLE PHYSICSFísica nuclearHigh Energy Physics::ExperimentParticle Physics - ExperimentLepton
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MEASUREMENT OF THE FORWARD-BACKWARD ASYMMETRY OF CHARM AND BOTTOM QUARKS AT THE Z-POLE USING D-ASTERISK(+/-)-MESONS

1995

The forward-backward asymmetries for the processes $$e^ + e^ - \to c\bar c$$ and $$e^ + e^ - \to b\bar b$$ at theZ resonance are measured using identifiedD *± mesons. In 905,000 selected hadronic events, taken in 1991 and 1992 with the DEL-PHI detector at LEP, 4757D *+→D 0π+ decays are reconstructed. Thec andb quark forward-backward asymmetries are determined to be: $$\begin{gathered} A_{FB}^{c\bar c} = 0.077 \pm 0.029(stat) \pm 0.012(sys), \hfill \\ A_{FB}^{b\bar b} = 0.059 \pm 0.062(stat) \pm 0.024(sys). \hfill \\ \end{gathered} $$ Constraining theb asymmetry to the value measured by DELPHI using independent analyses, the charm asymmetry is determined to be: $$A_{FB}^{c,const} = 0.068 \pm…

QuarkParticle physicsPhysics and Astronomy (miscellaneous)MesonElectron–positron annihilationHadron01 natural sciencesDECAYSPartícules (Física nuclear)Charm quarkNuclear physicsDELPHI; forward-backward asymmetry; QCD0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]DECAYS; QCDCharm (quantum number)010306 general physicsEngineering (miscellaneous)DELPHIPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyWeinberg angleQCDLARGE ELECTRON POSITRON COLLIDERPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHILarge Electron–Positron ColliderPARTICLE PHYSICSforward-backward asymmetryHigh Energy Physics::ExperimentCol·lisionadors d'hadronsParticle Physics - Experiment
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EPPS16: Nuclear parton distributions with LHC data

2017

We introduce a global analysis of collinearly factorized nuclear parton distribution functions (PDFs) including, for the first time, data constraints from LHC proton-lead collisions. In comparison to our previous analysis, EPS09, where data only from charged-lepton-nucleus deep inelastic scattering (DIS), Drell-Yan (DY) dilepton production in proton-nucleus collisions and inclusive pion production in deuteron-nucleus collisions were the input, we now increase the variety of data constraints to cover also neutrino-nucleus DIS and low-mass DY production in pion-nucleus collisions. The new LHC data significantly extend the kinematic reach of the data constraints. We now allow much more freedom…

QuarkParticle physicsPhysics and Astronomy (miscellaneous)Nuclear TheoryNuclear TheoryFOS: Physical sciencesPartonhiukkasfysiikka114 Physical sciences01 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)PionINELASTIC MUON SCATTERINGpartonit0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPLUS PB COLLISIONSEngineering (miscellaneous)Nuclear ExperimentPhysicsGauge bosonnuclear partonsLarge Hadron Collider010308 nuclear & particles physicsLEADING ORDERHigh Energy Physics::PhenomenologyLEPTON CHARGE ASYMMETRYSTRUCTURE-FUNCTION RATIOSDeep inelastic scatteringPPB COLLISIONSGluonnuclear parton distribution functionsHigh Energy Physics - PhenomenologyDIMUON PRODUCTIONPERTURBATION-THEORYJET CROSS-SECTIONSHigh Energy Physics::ExperimentHADRON-COLLISIONSRegular Article - Theoretical PhysicsNeutrino
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Consistent measurements of alpha(s) from precise oriented event shape distributions

2000

An updated analysis using about 1.5 million events recorded at $\sqrt{s} = M_Z$ with the DELPHI detector in 1994 is presented. Eighteen infrared and collinear safe event shape observables are measured as a function of the polar angle of the thrust axis. The data are compared to theoretical calculations in ${\cal O} (\alpha_s^2)$ including the event orientation. A combined fit of $\alpha_s$ and of the renormalization scale $x_{\mu}$ in $\cal O(\alpha_s^2$) yields an excellent description of the high statistics data. The weighted average from 18 observables including quark mass effects and correlations is $\alpha_s(M_Z^2) = 0.1174 \pm 0.0026$. The final result, derived from the jet cone energ…

QuarkParticle physicsPhysics and Astronomy (miscellaneous)OPTIMIZED PERTURBATION-THEORY; JET CROSS-SECTIONS; E+ E ANNIHILATION; QUANTUM CHROMODYNAMICS; E(+)E(-) ANNIHILATION; QCD CALCULATIONS; Z0 RESONANCE; MONTE-CARLO; DECAYS; ALPHA(S)(M(Z)(2))QCD CALCULATIONSFOS: Physical sciencesScale (descriptive set theory)01 natural sciences7. Clean energyDECAYSPartícules (Física nuclear)High Energy Physics - ExperimentRenormalizationHigh Energy Physics - Experiment (hep-ex)MONTE-CARLO0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Engineering (miscellaneous); Physics and Astronomy (miscellaneous)010306 general physicsEngineering (miscellaneous)ALPHA(S)(M(Z)(2))DELPHIPhysicsQUANTUM CHROMODYNAMICS010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyOrder (ring theory)ObservableFunction (mathematics)E(+)E(-) ANNIHILATIONLARGE ELECTRON POSITRON COLLIDEROrientation (vector space)Experimental uncertainty analysisOPTIMIZED PERTURBATION-THEORYPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSJET CROSS-SECTIONSFísica nuclearHigh Energy Physics::ExperimentE+ E ANNIHILATIONZ0 RESONANCEParticle Physics - Experiment
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First global next-to-leading order determination of diffractive parton distribution functions and their uncertainties within the {\tt xFitter} framew…

2018

We present {\tt GKG18-DPDFs}, a next-to-leading order (NLO) QCD analysis of diffractive parton distribution functions (diffractive PDFs) and their uncertainties. This is the first global set of diffractive PDFs determined within the {\tt xFitter} framework. This analysis is motivated by all available and most up-to-date data on inclusive diffractive deep inelastic scattering (diffractive DIS). Heavy quark contributions are considered within the framework of the Thorne-Roberts (TR) general mass variable flavor number scheme (GM-VFNS). We form a mutually consistent set of diffractive PDFs due to the inclusion of high-precision data from H1/ZEUS combined inclusive diffractive cross sections me…

QuarkParticle physicsPhysics and Astronomy (miscellaneous)parton distribution functionsHERAPREDICTIONSFOS: Physical scienceslcsh:AstrophysicsPartonhiukkasfysiikkaPROTON114 Physical sciences01 natural sciencesZeus (malware)CROSS-SECTIONSHigh Energy Physics - ExperimentDEEP-INELASTIC SCATTERINGHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)deep inelastic scatteringlcsh:QB460-4660103 physical sciencesquantum chromodynamicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityQCD ANALYSIS010306 general physicsEngineering (miscellaneous)PhysicsQuantum chromodynamicsLarge Hadron Collider010308 nuclear & particles physicsHERADeep inelastic scatteringHigh Energy Physics - PhenomenologyDistribution functionTESTSPHOTOPRODUCTIONlcsh:QC770-798LHC
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Neutrino Mass Ordering from Oscillations and Beyond: 2018 Status and Future Prospects

2018

The ordering of the neutrino masses is a crucial input for a deep understanding of flavor physics, and its determination may provide the key to establish the relationship among the lepton masses and mixings and their analogous properties in the quark sector. The extraction of the neutrino mass ordering is a data-driven field expected to evolve very rapidly in the next decade. In this review, we both analyze the present status and describe the physics of subsequent prospects. Firstly, the different current available tools to measure the neutrino mass ordering are described. Namely, reactor, long-baseline (accelerator and atmospheric) neutrino beams, laboratory searches for beta and neutrinol…

QuarkParticle physicsneutrino masses and flavor mixingCosmology and Nongalactic Astrophysics (astro-ph.CO)Field (physics)lcsh:AstronomyCosmic background radiationneutrino mass orderingFOS: Physical scienceslarge scale structure formation7. Clean energy01 natural sciencesCosmologyPartícules (Física nuclear)lcsh:QB1-991High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutrino oscillation010303 astronomy & astrophysicsPhysicsneutrino oscillations010308 nuclear & particles physicslcsh:QC801-809High Energy Physics::Phenomenologyneutrinoless double beta (0vββ) decayAstronomy and AstrophysicsHigh Energy Physics - PhenomenologySupernovalcsh:Geophysics. Cosmic physicscosmic microwave Background (CMB)High Energy Physics::ExperimentNeutrinoAstrophysics - Cosmology and Nongalactic AstrophysicsLeptonFrontiers in Astronomy and Space Sciences
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Production of exotic tetraquarks QQq¯q¯ in heavy-ion collisions at the LHC

2019

We investigate the production of exotic tetraquarks, $QQ\overline{q}\overline{q}\ensuremath{\equiv}{T}_{QQ}$ ($Q=c$ or $b$ and $q=u$ or $d$), in relativistic heavy-ion collisions using the quark coalescence model. The ${T}_{QQ}$ yield is given by the overlap of the density matrix of the constituents in the emission source with the Wigner function of the produced tetraquark. The tetraquark wave function is obtained from exact solutions of the four-body problem using realistic constituent models. The production yields are typically one order of magnitude smaller than previous estimations based on simplified wave functions for the tetraquarks. We also evaluate the consequences of the partial r…

QuarkPhysicsDensity matrixParticle physicsLarge Hadron Collider010308 nuclear & particles physicsQuark model01 natural sciencesHadronization0103 physical sciencesWigner distribution functionTetraquark010306 general physicsWave functionPhysical Review D
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Flavour Symmetries and SUSY Soft Breaking in the LHC Era

2007

The so-called supersymmetric flavour problem does not exist in isolation to the Standard Model flavour problem. We show that a realistic flavour symmetry can simultaneously solve both problems without ad hoc modifications of the SUSY model. Furthermore, departures from the SM expectations in these models can be used to discriminate among different possibilities. In particular we present the expected values for the electron EDM in a flavour model solving the supersymmetric flavour and CP problems.

QuarkPhysicsHistoryParticle physicsLarge Hadron ColliderPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFlavourFOS: Physical sciencesSupersymmetryExpected valueSymmetry (physics)Computer Science ApplicationsEducationHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Homogeneous spaceHigh Energy Physics::ExperimentMixing (physics)LeptonProgress of Theoretical Physics Supplement
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Top physics studies at the LHC in the standard model and beyond with the ATLAS detector

2009

The LHC will be a Top quark factory, producing large numbers of Top quarks even at the initial low luminosities. This will enable a rich program of Top quark Physics to be explored, both within the Standard Model and using Top quarks as probes of Physics Beyond the Standard Model. Recent studies from ATLAS will be presented, including prospects for the measurements of the production of Top pairs and single Top production, angular correlations in the Top decay, and the precision measurement of the Top quark mass. The search for Physics beyond the Standard Model will be illustrated with searches for rare Top decays involving Flavour Changing Neutral Currents, and the reconstruction of tt-bar …

QuarkPhysicsHistoryTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFlavourTop quark condensateOmega baryon01 natural sciencesComputer Science::Computers and SocietyComputer Science ApplicationsEducationSigma baryonNonlinear Sciences::Chaotic DynamicsNuclear physicsNonlinear Sciences::Exactly Solvable and Integrable Systems0103 physical sciencesPhysics::Atomic and Molecular ClustersHigh Energy Physics::ExperimentDetectors and Experimental Techniques010306 general physicsJournal of Physics: Conference Series
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