Search results for "Observable"

showing 10 items of 634 documents

The ASY-EOS experiment at GSI: Investigating the symmetry energy at supra-saturation densities

2012

The elliptic-flow ratio of neutrons with respect to protons in reactions of neutron rich heavy-ions systems at intermediate energies has been proposed as an observable sensitive to the strength of the symmetry term in the nuclear Equation Of State (EOS) at supra-saturation densities. The recent results obtained from the existing FOPI/LAND data for $^{197}$Au+$^{197}$Au collisions at 400 MeV/nucleon in comparison with the UrQMD model allowed a first estimate of the symmetry term of the EOS but suffer from a considerable statistical uncertainty. In order to obtain an improved data set for Au+Au collisions and to extend the study to other systems, a new experiment was carried out at the GSI la…

Particle physicsHistoryQC1-999Nuclear TheoryFOS: Physical sciencesand isobaric spin 24.10.Pa Thermal and statistical models[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]EducationNuclear physicsPhysics and Astronomy (all)nuclear physics; heavy-ions; symmetry energy; Au+Au collisionsNeutronNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentComputingMilieux_MISCELLANEOUSPhysicssezelePhysicsOrder (ring theory)Nuclear equation of stateObservableNuclear Experiment; Nuclear Experiment21.65.-f Nuclear matter 27.80.+w 190(less-than-or-equal-to)A(less-than-or-equal-to)219 24.60.-k Statistical theory and fluctuations 25.75.Gz Particle correlations and fluctuations 21.10.Hw SpinSymmetry (physics)Term (time)Computer Science ApplicationsparityNuclear reactionsSaturation (chemistry)NucleonEnergy (signal processing)
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Nuclear gluons at RHIC in a multi-observable approach

2019

We explore the possibility of measuring nuclear gluon distributions at the Relativistic Heavy-Ion Collider (RHIC) with $\sqrt{s}=200 \, {\rm GeV}$ proton-nucleus collisions. In addition to measurements at central rapidity, we consider also observables at forward rapidity, consistent with proposed upgrades to the experimental capabilities of STAR and sPHENIX. The processes we consider consist of Drell-Yan dilepton, dijet, and direct photon-jet production. The Drell-Yan process is found to be an efficient probe of gluons at small momentum fractions. In order to fully utilize the potential of Drell-Yan measurements we demonstrate how the overall normalization uncertainty present in the experim…

Particle physicsNuclear TheoryFOS: Physical scienceshiukkasfysiikka114 Physical sciences01 natural sciences7. Clean energylaw.inventionHigh Energy Physics - ExperimentMomentumHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)law0103 physical sciencesnuclear gluonsRapidityNuclear Experiment (nucl-ex)010306 general physicsColliderNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyOrder (ring theory)Drell–Yan processObservableGluonHigh Energy Physics - PhenomenologygluonitProduction (computer science)High Energy Physics::Experimentydinfysiikka
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Ballistic protons in incoherent exclusive vector meson production as a measure of rare parton fluctuations at an Electron-Ion Collider

2014

We argue that the proton multiplicities measured in Roman pot detectors at an electron ion collider can be used to determine centrality classes in incoherent diffractive scattering. Incoherent diffraction probes the fluctuations in the interaction strengths of multi-parton Fock states in the nuclear wavefunctions. In particular, the saturation scale that characterizes this multi-parton dynamics is significantly larger in central events relative to minimum bias events. As an application, we study the centrality dependence of incoherent diffractive vector meson production. We identify an observable which is simultaneously very sensitive to centrality triggered parton fluctuations and insensit…

Particle physicsNuclear TheoryIncoherent scatterGeneral Physics and AstronomyFOS: Physical sciencesPartonElectronlaw.inventionNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)lawnuclear wave functionsVector mesonNuclear Experiment (nucl-ex)ColliderNuclear ExperimentNuclear ExperimentPhysicsLarge Hadron Colliderta114protonsRoman potObservableHigh Energy Physics - PhenomenologyHigh Energy Physics::Experimentincoherent scattering
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An analysis of the impact of LHC Run I proton–lead data on nuclear parton densities

2016

We report on an analysis of the impact of available experimental data on hard processes in proton-lead collisions during Run I at the Large Hadron Collider on nuclear modifications of parton distribution functions. Our analysis is restricted to the EPS09 and DSSZ global fits. The measurements that we consider comprise production of massive gauge bosons, jets, charged hadrons and pions. This is the first time a study of nuclear PDFs includes this number of different observables. The goal of the paper is twofold: i) checking the description of the data by nPDFs, as well as the relevance of these nuclear effects, in a quantitative manner; ii) testing the constraining power of these data in eve…

Particle physicsNuclear TheoryPhysics and Astronomy (miscellaneous)ProtoneducationHadronNuclear TheoryFOS: Physical sciencesproton-lead collisionsParton114 Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Pion0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentEngineering (miscellaneous)PhysicsGauge bosonLarge Hadron Collider010308 nuclear & particles physicsObservable3. Good healthHigh Energy Physics - PhenomenologyDistribution functionRegular Article - Theoretical PhysicsThe European Physical Journal. C, Particles and Fields
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Cosmological axion and neutrino mass constraints from Planck 2015 temperature and polarization data

2015

Axions currently provide the most compelling solution to the strong CP problem. These particles may be copiously produced in the early universe, including via thermal processes. Therefore, relic axions constitute a hot dark matter component and their masses are strongly degenerate with those of the three active neutrinos, as they leave identical signatures in the different cosmological observables. In addition, thermal axions, while still relativistic states, also contribute to the relativistic degrees of freedom, parameterised via $N_{eff}$. We present the cosmological bounds on the relic axion and neutrino masses, exploiting the full Planck mission data, which include polarization measure…

Particle physicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Dark matterFOS: Physical sciencesAstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencessymbols.namesake0103 physical sciencesPlanck010303 astronomy & astrophysicsAxionPhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)[SDU.ASTR]Sciences of the Universe [physics]/Astrophysics [astro-ph]010308 nuclear & particles physicsAxion Dark Matter ExperimentHot dark matterHigh Energy Physics::PhenomenologyObservablelcsh:QC1-999symbolsStrong CP problemNeutrinoAstrophysics - High Energy Astrophysical Phenomenalcsh:PhysicsAstrophysics - Cosmology and Nongalactic AstrophysicsPhysics Letters B
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Measurement of trilinear gauge couplings in e(+)e(-) collisions at 161 GeV and 172 GeV

1998

Trilinear gauge boson couplings are measured using data taken by DELPHI at 161 GeV and 172 GeV, Values for WWV couplings (V = Z,gamma) are determined from a study of the reactions e(+)e(-) --> W+W- and e(+)e(-) --> We nu, using differential distributions from the WW final state in which one W decays hadronically and the other leptonically, and total cross,section data from other channels, Limits are also derived on neutral ZV gamma couplings from an analysis of the reaction e(+)e(-) --> gamma + invisible particles. (C) 1998 Elsevier Science B.V.

Particle physicsNuclear and High Energy PhysicsElectron–positron annihilation7. Clean energy01 natural sciencesNuclear physics0103 physical sciencesOPTIMAL OBSERVABLES[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentOPTIMAL OBSERVABLES; PHOTON COUPLINGS; ROOT-S=1.8 TEVDELPHIPhysicsGauge boson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyROOT-S=1.8 TEVGauge (firearms)LARGE ELECTRON POSITRON COLLIDERPHOTON COUPLINGSLarge Electron–Positron ColliderPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSHigh Energy Physics::ExperimentParticle Physics - Experiment
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Lepton universality violation with lepton flavor conservation in B-meson decays

2015

Anomalies in semileptonic B-meson decays present interesting patterns that might be revealing the shape of the new physics to come. Under the assumption that neutrino and charged lepton mass terms are the only sources of flavor violation and given the hierarchy between the two, we find that charged lepton universality violation without charged lepton flavor violation naturally arises. This can account for a deficit of B + → K + μμ over B + → K + ee decays with new physics coupled predominantly to muons and a new physics scale of a few TeV. A generic prediction of this scenario is a large enhacement of tauonic B decay rates that, in particular, could accommodate an excess in B → D (∗) τ ν. F…

Particle physicsNuclear and High Energy PhysicsPhysics beyond the Standard ModelB-PhysicsAtomicMathematical SciencesParticle and Plasma PhysicsEffective field theoryLeptoquarkB mesonNuclearMathematical PhysicsPhysicsQuantum PhysicsMuonRare DecaysHigh Energy Physics::PhenomenologyMolecularObservablehep-phNuclear & Particles PhysicsPhysical SciencesBeyond Standard ModelHigh Energy Physics::ExperimentNeutrinoLeptonJournal of High Energy Physics
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Determination of the muonic branching ratio of the W boson and its total width via cross-section measurements at the Tevatron and LHC

2016

The total $W$-boson decay width $\Gamma_W$ is an important observable which allows testing of the standard model. The current world average value is based on direct measurements of final state kinematic properties of $W$-boson decays, and has a relative uncertainty of 2%. The indirect determination of $\Gamma_W$ via the cross-section measurements of vector-boson production can lead to a similar accuracy. The same methodology leads also to a determination of the leptonic branching ratio. This approach has been successfully pursued by the CDF and D0 experiments at the Tevatron collider, as well as by the CMS collaboration at the LHC. In this paper we present for the first time a combination o…

Particle physicsPhysics and Astronomy (miscellaneous)HadronTevatronFOS: Physical sciences01 natural sciencesStandard Modellaw.inventionHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)law0103 physical sciences010306 general physicsColliderEngineering (miscellaneous)PhysicsLarge Hadron Collider010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyObservableHigh Energy Physics - PhenomenologyProduction (computer science)High Energy Physics::ExperimentParticle Physics - ExperimentEuropean Physical Journal C
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The Z boson spin observables as messengers of new physics

2017

We demonstrate that the 8 multipole parameters describing the spin state of the $Z$ boson are able to disentangle known $Z$ production mechanisms and signals from new physics at the LHC. They can be extracted from appropriate asymmetries in the angular distribution of lepton pairs from the $Z$ boson decay. The power of this analysis is illustrated by (i) the production of $Z$ boson plus jets; (ii) $Z$ boson plus missing transverse energy; (iii) $W$ and $Z$ bosons originating from the two-body decay of a heavy resonance.

Particle physicsPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelFOS: Physical scienceslcsh:Astrophysics01 natural sciencesResonance (particle physics)Light Supersymmetric ParticleHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Standard Model Predictionlcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Spin-½BosonCondensed Matter::Quantum GasesPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyAngular DistributionCharged LeptonObservable3. Good healthHigh Energy Physics - PhenomenologyLarge Hadron Colliderlcsh:QC770-798High Energy Physics::ExperimentMultipole expansionLeptonThe European Physical Journal C
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Structure of pion photoproduction amplitudes

2018

We derive and apply the finite energy sum rules to pion photoproduction. We evaluate the low energy part of the sum rules using several state-of-the-art models. We show how the differences in the low energy side of the sum rules might originate from different quantum number assignments of baryon resonances. We interpret the observed features in the low energy side of the sum rules with the expectation from Regge theory. Finally, we present a model, in terms of a Regge-pole expansion, that matches the sum rules and the high-energy observables.

Particle physicsStructure (category theory)FOS: Physical sciences01 natural sciencesPOLARIZED PHOTONSCHARGED PIONSPionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesT DISPERSION-RELATIONSPhysics and Astronomy (miscellaneous); high energy; pion photoproduction010306 general physicsCOMPTON-SCATTERINGPhysicsREGGE-POLES010308 nuclear & particles physicsObservablePI0 PHOTOPRODUCTIONQuantum numberBaryonRegge theoryHigh Energy Physics - PhenomenologyAmplitudeBARYON RESONANCESPhysics and AstronomyPI-0 PHOTOPRODUCTIONMESON PHOTOPRODUCTIONENERGY SUM-RULESEnergy (signal processing)
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