Search results for "Interactions"

showing 10 items of 1963 documents

Dielectron production in proton-proton and proton-lead collisions at √sNN=5.02TeV

2020

The first measurements of dielectron production at midrapidity (|ηe| < 0.8) in proton–proton and proton–lead collisions at √sNN = 5.02 TeV at the LHC are presented. The dielectron cross section is measured with the ALICE detector as a function of the invariant mass mee and the pair transverse momentum pT, ee in the ranges mee < 3.5 GeV/c2 and pT, ee < 8 GeV/c, in both collision systems. In proton–proton collisions, the charm and beauty cross sections are determined at midrapidity from a fit to the data with two different event generators. This complements the existing dielectron measurements performed at √s = 7 and 13 TeV. The slope of the √s dependence of the three measurements is…

Nuclear and High Energy Physics:Kjerne- og elementærpartikkelfysikk: 431 [VDP]ProtonHadronNuclear Theorydielectrondielectron production01 natural sciences7. Clean energyNuclear physicshadron-ion interactionshadron-hadron collisions; dielectron production;Ionic Collisionsdielectron cross sectiondielectron nuclear modification factor0103 physical sciencesInvariant massDielectronCharm (quantum number)Dielectron; hadron-hadron interactions; hadron-ion interactionsPhysics::Atomic PhysicsIonic Collisions; Relativistic Heavy-ion Collisions; Quark-Gluon Plasma010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsPhysicsVDP::Kjerne- og elementærpartikkelfysikk: 431hadron-hadron interactionNuclear matterhadron-hadron collisionsNATURAL SCIENCES. Physics.ALICE LHC proton-lead collisions proton-proton collisionsPRIRODNE ZNANOSTI. Fizika.:Nuclear and elementary particle physics: 431 [VDP]VDP::Nuclear and elementary particle physics: 431dielectron ; LHC ; dielectron cross section ; dielectron nuclear modification factorQuark–gluon plasmaQuark-Gluon PlasmaHigh Energy Physics::ExperimentLHChadron-hadron interactionsRelativistic Heavy-ion Collisions
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Searching for hidden sectors in multiparticle production at the LHC

2016

Most signatures of new physics in colliders have been studied so far on the transverse plane with respect to the beam direction. In this work however we study the impact of a hidden sector beyond the Standard Model (SM) on inclusive (pseudo)rapidity correlations and moments of the multiplicity distributions, with special emphasis in the LHC results.

Nuclear and High Energy PhysicsFactorialParticle physicsPhysics beyond the Standard ModelMultihadron correlationsFOS: Physical sciencesFactorial and cumulant moments01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)pp interactions at LHC0103 physical sciencesProduction (economics)RapidityStatistical physics010306 general physicsCumulantParticle Physics - PhenomenologyPhysicsLarge Hadron Collider010308 nuclear & particles physicsFísicaMultiplicity (mathematics)Hidden Valley modelslcsh:QC1-999Hidden sectorHigh Energy Physics - PhenomenologyTransverse planeMoment (physics)Beam directionPhysics::Accelerator PhysicsModels beyond the Standard Modellcsh:PhysicsNuclear and Particle Physics Proceedings
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Odd parity bottom-flavored baryon resonances

2013

The LHCb Collaboration has recently observed two narrow baryon resonances with beauty. Their masses and decay modes look consistent with the quark model orbitally excited states Lambda(b)(5912) and Lambda(b)*(5920), with quantum numbers J(P) = 1/2(-) and 3/2(-), respectively. We predict the existence of these states within a unitarized meson-baryon coupled-channel dynamical model, which implements heavy-quark spin symmetry. Masses, quantum numbers and couplings of these resonances to the different meson-baryon channels are obtained. We find that the resonances Lambda(0)(b)(5912) and Lambda(0)(b)(5920) are heavy-quark spin symmetry partners, which naturally explains their approximate mass de…

Nuclear and High Energy PhysicsParticle physicsCharmNuclear TheoryN-asteriskHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences01 natural sciencesCHARMNuclear Theory (nucl-th)SUM-RULESHigh Energy Physics - Phenomenology (hep-ph)Heavy-quark symmetryMESON-EXCHANGE0103 physical sciencesChiral dynamicsNuclear Experiment010306 general physicsNuclear theorySpectroscopyKaon-nucleon interactionsPhysicsMeson-exchangeStatesSPECTROSCOPYCoupled-channelN-ASTERISK010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyCHIRAL DYNAMICSFísicaCOUPLED-CHANNELHEAVY-QUARK SYMMETRYHigh Energy Physics - PhenomenologySTATESSum-rulesKAON-NUCLEON INTERACTIONSHigh Energy Physics::ExperimentSpin symmetryHumanities
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S-wave Kpi scattering in chiral perturbation theory with resonances

2000

32 páginas, 6 figuras, 2 tablas.-- PACS: 11.80.Et; 12.39.Fe; 13.75.Lb; 13.85.Fb.-- arXiv:hep-ph/0006045v1

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryScalar (mathematics)FOS: Physical sciencesMeson–meson interactionsHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)S-wavePartial-wave analysisddc:530Nuclear Experiment (nucl-ex)Nuclear ExperimentPhysicsScatteringtwo-particle final states [Inelastic scattering]ResonanceFísicaRange (mathematics)High Energy Physics - PhenomenologyUnitarisationInelastic scattering: two-particle final statesChiral lagrangiansEnergy (signal processing)
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Measurement of the mass of the W boson using direct reconstruction at √s = 183 GeV

1999

From data corresponding to an integrated luminosity of 53.5 pb(-1) taken during the 183 GeV run in 1997, DELPHI has measured the W mass from direct reconstruction of WW --> lq (q) over bar and WW --> q (q) over bar q (q) over bar events. Combining these channels, a value of m(w) = 80.238 +/- 0.154(stat) +/- 0.035(syst) +/- 0.035(fsi) +/- 0.021 (LEP) GeV/c(2) is obtained, where fsi denotes final state interaction. Combined with the W mass obtained by DELPHI from the WW production cross-section and with the direct measurement at 172 GeV this leads to a measured value of m(w) = 80.270 +/- 0.137(stat) +/- 0.031(syst) +/- 0.030(fsi) +/- 0.021(LEP)GeV/c(2), in good agreement with the Standard Mod…

Nuclear and High Energy PhysicsParticle physicsEINSTEIN CORRELATIONSCLUSTERING-ALGORITHMElectron–positron annihilationMathematicsofComputing_GENERALCOLOR DIPOLE MODEL01 natural sciencesComputer Science::Digital LibrariesPartícules (Física nuclear)LuminosityStandard ModelPHYSICSEVENTSNuclear physicsLEP20103 physical sciencesMONTE-CARLO PROGRAM[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ANNIHILATION010306 general physicsDELPHIPhysicsAnnihilation010308 nuclear & particles physicsE(+)E(-) INTERACTIONSTheoryofComputation_GENERALLARGE ELECTRON POSITRON COLLIDERMONTE-CARLO PROGRAM; PAIR CROSS-SECTION; COLOR DIPOLE MODEL; E(+)E(-) INTERACTIONS; EINSTEIN CORRELATIONS; CLUSTERING-ALGORITHM; ANNIHILATION; PHYSICS; EVENTS; LEP2PARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIComputer Science::Mathematical SoftwarePARTICLE PHYSICSProduction (computer science)Física nuclearPAIR CROSS-SECTIONParticle Physics - ExperimentBar (unit)
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Observation of charmonium pairs produced exclusively in $pp$ collisions

2014

A search is performed for the central exclusive production of pairs of charmonia produced in proton-proton collisions. Using data corresponding to an integrated luminosity of $3{\rm\ fb}^{-1}$ collected at centre-of-mass energies of 7 and 8 TeV, $J/\psi J/\psi$ and $J/\psi\psi(2S)$ pairs are observed, which have been produced in the absence of any other activity inside the LHCb acceptance that is sensitive to charged particles in the pseudorapidity ranges $(-3.5,-1.5)$ and $(1.5,5.0)$. Searches are also performed for pairs of P-wave charmonia and limits are set on their production. The cross-sections for these processes, where the dimeson system has a rapidity between 2.0 and 4.5, are measu…

Nuclear and High Energy PhysicsParticle physicsNuclear TheorydiffractionFOS: Physical sciencesLHCb - Abteilung HofmannHEAVY-ION COLLISIONSQCD diffraction charmoniaNOHigh Energy Physics - ExperimentLuminosityHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Quantum chromodynamiccharmonia; diffraction; QCDcharmonia; diffraction; QCD; Nuclear and High Energy PhysicsRapiditySDG 7 - Affordable and Clean EnergyNuclear ExperimentQCPhysics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyhep-ex12.38.-tParticle physicsHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadronHEAVY-ION COLLISIONS; 450 GEV/C; DIFFRACTION; LHCQCDCromodinàmica quànticaLHCbDifracció450 GEV/CPseudorapidityPhysics::Accelerator PhysicscharmoniaFísica nuclearHigh Energy Physics::ExperimentProduction (computer science)LHCHEAVYFísica de partículesExperiments13.85.NiDiffractionQuantum chromodynamicsParticle Physics - ExperimentJournal of Physics G: Nuclear and Particle Physics
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Dynamically generated resonances from the vector octet-baryon octet interaction

2010

We study the interaction of vector mesons with the octet of stable baryons in the framework of the local hidden gauge formalism using a coupled-channels unitary approach. We examine the scattering amplitudes and their poles, which can be associated to known J(P) = 1/2(-), 3/2(-) baryon resonances, in some cases, or give predictions in other ones. The formalism employed produces doublets of degenerate J(P) = 1/2(-), 3/2(-) states, a pattern which is observed experimentally in several cases. The findings of this work should also be useful to guide present experimental programs searching for new resonances, in particular in the strange sector where the current information is very poor.

Nuclear and High Energy PhysicsParticle physicsOctetMesonNuclear TheoryNuclear TheoryFOS: Physical sciences01 natural sciencesUnitary stateNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBaryonsMesons (Nuclear physics)Mesons (Física nuclear)010306 general physicsBarionsPhysicsWeak interactions (Nuclear physics)010308 nuclear & particles physicsDegenerate energy levelsHigh Energy Physics::PhenomenologyInteraccions febles (Física nuclear)FísicaScattering amplitudeBaryonFormalism (philosophy of mathematics)High Energy Physics - PhenomenologyProjecte 227431
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Glueball enhancement by color deconfinement

2007

5 pages, 4 figures.-- PACS nrs.: 14.80.-j; 24.80.+y; 25.75.Nq.-- ISI Article Identifier: 000245333000063.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0609219

Nuclear and High Energy PhysicsParticle physics[PACS] Nuclear tests of fundamental interactions and symmetriesNuclear Theory[PACS] Quark deconfinement quark-gluon plasma production and phase transitions in heavy-ion collisionsHigh Energy Physics::LatticeFOS: Physical sciencesDeconfinementQuantum chromodynamics (QCD)Nuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Color confinementNuclear ExperimentNuclear theoryQuantum chromodynamicsPhysicsQuark confinementGlueball[PACS] Other particles (including hypothetical)High Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyColor modelHeavy ion-nucleus reactions
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Effects of spin-orbit interaction on nuclear response and neutrino mean free path

2006

PTH; The effects of the spin-orbit component of the particle-hole interaction on nuclear response functions and neutrino mean free path are examined. A complete treatment of the full Skyrme interaction in the case of symmetric nuclear matter and pure neutron matter is given. Numerical results for neutron matter are discussed. It is shown that the effects of the spin-orbit interaction remain small, even at momentum transfer larger than the Fermi momentum. The neutrino mean free paths are marginally affected.

Nuclear and High Energy PhysicsParticle physicsresponse functionsNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Mean free pathAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryFOS: Physical sciencesAstrophysics01 natural sciences21.30.Fe 21.60.Jz 21.65.+f 26.60.+cNuclear Theory (nucl-th)Nuclear physicsMomentum[PHYS.ASTR.CO]Physics [physics]/Astrophysics [astro-ph]/Cosmology and Extra-Galactic Astrophysics [astro-ph.CO]0103 physical sciencesNeutronspin-orbit interaction010306 general physicsPhysics[SDU.ASTR]Sciences of the Universe [physics]/Astrophysics [astro-ph]010308 nuclear & particles physicsAstrophysics (astro-ph)Momentum transferFísicaSpin–orbit interactionNuclear matterNeutron starnuclear matterrandom phase approximationeffective Skyrme interactionsNeutrino
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Pion-photon transition distribution amplitudes in the Nambu-Jona-Lasinio model

2007

12 pages, 6 figures.-- PACS nrs.: 13.60.-r; 11.10.St; 12.38.Lg; 24.10.Jv.-- ISI Article Identifier: 000251327200049.-- ArXiv pre-print available at: http://arxiv.org/abs/0707.3366

Nuclear and High Energy PhysicsPhotonBethe–Salpeter equationHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences[PACS] Relativistic models of nucleiPartícules (Física nuclear)PionHigh Energy Physics - Phenomenology (hep-ph)Nambu–Jona-Lasinio modelBound stateVirtual Compton-scatteringCovariant transformation[PACS] Photon and charged-lepton interactions with hadrons[PACS] Bound and unstable statesMathematical physicsQuantum chromodynamicsPhysicsHigh Energy Physics::PhenomenologyGeneralized Parton distributions[PACS] Bound and unstable states; Bethe-Salpeter equations[PACS] Other nonperturbative calculations in QCDHigh Energy Physics - PhenomenologyAmplitudeQuantum electrodynamicsBethe-Salpeter equationsFísica nuclear
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