Search results for "Particles"

showing 10 items of 8085 documents

Charged particle multiplicity distributions in restricted rapidity intervals in Z0 hadronic decays.

1991

The multiplicity distributions of charged particles in restricted rapidity intervals in Z0 hadronic decays measured by the DELPHI detector are presented. The data reveal a shoulder structure, best visible for intervals of intermediate size, i.e. for rapidity limits around ±1.5. The whole set of distributions including the shoulder structure is reproduced by the Lund Parton Shower model. The structure is found to be due to important contributions from 3-and 4-jet events with a hard gluon jet. A different model, based on the concept of independently produced groups of particles, "clans", fluctuating both in number per event and particle content per clan, has also been used to analyse the pres…

COLLISIONSParticle physicsE+E ANNIHILATIONPhysics and Astronomy (miscellaneous)LUND MONTE-CARLOElectron–positron annihilationHadronElementary particlePETRA ENERGIES01 natural sciences250 GEV/CNuclear physicsDEPENDENCE0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RapidityNuclear Experiment010306 general physicsParton showerEngineering (miscellaneous)LUND MONTE-CARLO; JET PRODUCTION-RATES; E+E ANNIHILATION; 250 GEV/C; PETRA ENERGIES; COLLISIONS; DEPENDENCE; FRAGMENTATION; QCD; RESONANCEPhysics010308 nuclear & particles physicsJET PRODUCTION-RATESMultiplicity (mathematics)RESONANCEQCDCharged particleGluonPhysique des particules élémentairesHigh Energy Physics::ExperimentFRAGMENTATIONParticle Physics - Experiment
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The one loop gluon emission light cone wave function

2017

Light cone perturbation theory has become an essential tool to calculate cross sections for various small-$x$ dilute-dense processes such as deep inelastic scattering and forward proton-proton and proton-nucleus collisions. Here we set out to do one loop calculations in an explicit helicity basis in the four dimensional helicity scheme. As a first process we calculate light cone wave function for one gluon emission to one-loop order in Hamiltonian perturbation theory on the light front. We regulate ultraviolet divergences with transverse dimensional regularization and soft divergences with using a cut-off on longitudinal momentum. We show that when all the renormalization constants are comb…

COLLISIONSParticle physicsNuclear TheoryRENORMALIZATIONQUANTUM ELECTRODYNAMICSGeneral Physics and AstronomyFOS: Physical sciencesloop calculations114 Physical sciences01 natural scienceslight cone perturbation theoryRenormalizationNuclear Theory (nucl-th)Dimensional regularizationHigh Energy Physics - Phenomenology (hep-ph)INFINITE-MOMENTUMLight cone0103 physical sciencesSCATTERINGHelicity basis010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsCoupling constantgluon emissionta114010308 nuclear & particles physicsCOLOR GLASS CONDENSATEDeep inelastic scatteringFRONT QCDHelicityEVOLUTIONHigh Energy Physics - PhenomenologyCHROMODYNAMICSQuantum electrodynamicsgluon saturation
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Inclusive Search for Standard Model Higgs Boson Production in the WW Decay Channel using the CDF II Detector

2010

We present a search for standard model (SM) Higgs boson production using p (p) over bar collision data at root s = 1. 96 TeV, collected with the CDF II detector and corresponding to an integrated luminosity of 4. 8 fb(-1). We search for Higgs bosons produced in all processes with a significant production rate and decaying to two W bosons. We find no evidence for SM Higgs boson production and place upper limits at the 95% confidence level on the SM production cross section (sigma(H)) for values of the Higgs boson mass (m(H)) in the range from 110 to 200 GeV. These limits are the most stringent for m(H) > 130 GeV and are 1.29 above the predicted value of sigma(H) for m(H) 165 GeV.

COLLISIONSParticle physicsZ-GAMMA PRODUCTION; HADRON COLLIDERS; QCD CORRECTIONS; NNLO QCD; COLLISIONS; FERMILABGeneral Physics and AstronomyLibrary scienceFOS: Physical sciencesddc:500.2114 Physical sciences01 natural sciencesZ-GAMMA PRODUCTIONBildungWorld classHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)NNLO QCDBasic research0103 physical sciencesHADRON COLLIDERSFERMILAB010306 general physicsChinaPhysicshep-ex010308 nuclear & particles physicsPhysicsHigh Energy Physics::Phenomenology3. Good healthChristian ministryHigh Energy Physics::ExperimentQCD CORRECTIONS
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Unequal rapidity correlators in the dilute limit of the JIMWLK evolution

2019

We study unequal rapidity correlators in the stochastic Langevin picture of Jalilian-Marian-Iancu-McLerran-Weigert-Leonidov-Kovner (JIMWLK) evolution in the color glass condensate effective field theory. We discuss a diagrammatic interpretation of the long-range con elators. By separately evolving the Wilson lines in the direct and complex conjugate amplitudes, we use the formalism to study two-particle production at large rapidity separations. We show that the evolution between the rapidities of the two produced particles can be expressed as a linear equation, even in the full nonlinear limit. We also show how the Langevin formalism for two-particle correlations reduces to a Balitsky-Fadin…

COLLISIONSPosition and momentum spacehiukkasfysiikkafield theory114 Physical sciences01 natural sciencesColor-glass condensatenuclear physicsINFINITE-MOMENTUM0103 physical sciencesEQUATIONEffective field theorySCATTERINGRapidity010306 general physicsMathematical physicsPhysicsComplex conjugate010308 nuclear & particles physicsStochastic processCOLOR GLASS CONDENSATENONLINEAR GLUON EVOLUTIONNonlinear systemDIPOLE PICTUREkvanttikenttäteoriaydinfysiikkaLinear equationPhysical Review D
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A multifuctional nanoplatform for drug targeted delivery based on radiation-engineered nanogels

2020

Abstract Under a rational design, combining biologically active molecules, ligands to specific cell receptors and fluorescent, radioactive or paramagnetic labels into a single nano-object can bridge the unique properties of the individual components and improve conventional sensing, imaging and therapeutic efficacies. The validation of these functional nano-objects requires careful testing both in terms of physico-chemical properties and biological behaviour in vitro and in vivo, prior to translation into the clinic. Ionising radiation of aqueous polymer solutions is a viable strategy to produce multifunctional nanogels from aqueous solutions of hydrophilic polymers. By proper selection of …

COLON-CANCER CELLSPULSE-RADIOLYSISDrugINDUCED CROSS-LINKINGSPECTRAL PROPERTIESmedia_common.quotation_subjectNanogelsConjugation reactionsNanotechnology01 natural sciencesAQUEOUS-SOLUTIONFLUORESCEIN030218 nuclear medicine & medical imagingNanogel03 medical and health sciences0302 clinical medicineHydrophilic polymers0103 physical sciencesNANOPARTICLESMoleculeIonising radiation synthesiIN-VIVOmedia_commonchemistry.chemical_classificationRadiationAqueous solution010308 nuclear & particles physicsIonising radiation synthesisRational designPolymerINSULINNanomedicineConjugation reactionchemistryDrug deliveryDrug deliveryNanomedicineSettore CHIM/07 - Fondamenti Chimici Delle TecnologieACID) NANOGELSRadiation Physics and Chemistry
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CFD simulation of ZnO nanoparticle precipitation in a supercritical water synthesis reactor

2012

International audience; Continuous hydrothermal flow synthesis process has shown great advantages concerning the control of particle size and morphology through the optimization of supercritical water processing parameters. In particular, micromixing is a key issue of the process for controlling the nucleation mechanism. A Computational Fluid Dynamics (CFD) model is suggested for nanoparticle size determination using a population balance approach. Models for reaction kinetics, thermodynamics, nucleation and growth are presented. The effects of base concentration and hydrodynamics are investigated. Results show that the CFD may be valuable simulation tool for controlling the size and the sha…

CONTINUOUS HYDROTHERMAL SYNTHESISMaterials scienceFLOWGeneral Chemical EngineeringPopulationNucleationNanoparticleNanotechnologyCrystal growth02 engineering and technologyComputational fluid dynamicsVALIDATIONNANOPOWDERSMETAL-OXIDE NANOPARTICLES020401 chemical engineeringPARTICLE FORMATION0204 chemical engineeringPhysical and Theoretical Chemistryeducationeducation.field_of_studybusiness.industryFLUID-DYNAMICSAGGREGATION021001 nanoscience & nanotechnologyCondensed Matter PhysicsSupercritical fluidMicromixingChemical engineeringPOPULATION BALANCEParticle sizeCRYSTALLIZATION0210 nano-technologybusinessThe Journal of Supercritical Fluids
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CODEX Weak Lensing Mass Catalogue and implications on the mass-richness relation

2021

The COnstrain Dark Energy with X-ray clusters (CODEX) sample contains the largest flux limited sample of X-ray clusters at $0.35 = \alpha \mu + \beta$, with $\mu = \ln (M_{200c}/M_{\mathrm{piv}})$, and $M_{\mathrm{piv}} = 10^{14.81} M_{\odot}$. We find a slope $\alpha = 0.49^{+0.20}_{-0.15}$, normalization $ \exp(\beta) = 84.0^{+9.2}_{-14.8}$ and $\sigma_{\ln \lambda | \mu} = 0.17^{+0.13}_{-0.09}$ using CFHT richness estimates. In comparison to other weak lensing richness-mass relations, we find the normalization of the richness statistically agreeing with the normalization of other scaling relations from a broad redshift range ($0.0<z<0.65$) and with different cluster selection (X-ray, Sun…

COSMOLOGICAL CONSTRAINTSCosmology and Nongalactic Astrophysics (astro-ph.CO)FOS: Physical sciencesAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsLambdaPROFILE01 natural sciences114 Physical sciencesgravitational lensing: weakMAXBCGweak [gravitational lensing]0103 physical sciencesLARGE-SCALE STRUCTUREclusters: general [galaxies]PROBE010303 astronomy & astrophysicsWeak gravitational lensingGalaxy clusterLOCUSSPhysicsTEMPERATURE RELATION010308 nuclear & particles physicsAstronomy and Astrophysicsobservations [cosmology]RedshiftREDUCTIONSpace and Planetary Sciencegravitational lensing: weak; galaxies: clusters: general; cosmology: observationsgalaxies: clusters: generalcosmology: observationsGIANTSGALAXY CLUSTERS[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Astrophysics - Cosmology and Nongalactic Astrophysics
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Abelian realization of phenomenological two-zero neutrino textures

2014

In an attempt at explaining the observed neutrino mass-squared differences and leptonic mixing, lepton mass matrices with zero textures have been widely studied. In the weak basis where the charged lepton mass matrix is diagonal, various neutrino mass matrices with two zeros have been shown to be consistent with the current experimental data. Using the canonical and Smith normal form methods, we construct the minimal Abelian symmetry realizations of these phenomenological two-zero neutrino textures. The implementation of these symmetries in the context of the seesaw mechanism for Majorana neutrino masses is also discussed.

CP ViolationPhysicsSterile neutrinoParticle physicsNuclear and High Energy Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesZerosHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismMass Matrix0103 physical sciencesCP violationlcsh:QC770-798High Energy Physics::Experimentlcsh:Nuclear and particle physics. Atomic energy. RadioactivityAbelian groupNeutrino010306 general physicsNeutrino oscillationLeptonNuclear Physics B
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Search for CP violation using T-odd correlations in D-0 -> K+K-pi(+)pi(-) decays

2014

A search for $CP$ violation using $T$-odd correlations is performed using the four-body $D^0 \to K^+K^-\pi^+\pi^-$ decay, selected from semileptonic $B$ decays. The data sample corresponds to integrated luminosities of $1.0\,\text{fb}^{-1}$ and $2.0\,\text{fb}^{-1}$ recorded at the centre-of-mass energies of 7 TeV and 8 TeV, respectively. The $CP$-violating asymmetry $a_{CP}^{T\text{-odd}}$ is measured to be $(0.18\pm 0.29\text{(stat)}\pm 0.04\text{(syst)})\%$. Searches for $CP$ violation in different regions of phase space of the four-body decay, and as a function of the $D^0$ decay time, are also presented. No significant deviation from the $CP$ conservation hypothesis is found.

CP violation Charm physics Hadron-Hadron Scattering Flavor physics14.40.Lb01 natural sciencesSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - ExperimentFlavor physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ASTRONOMY & ASTROPHYSICSQCmedia_commonCharm physicsPhysicsHadronic decays of charmed mesonCharm physics; CP violation; Flavor physics; Hadron-Hadron ScatteringPhysicsPHYSICS PARTICLES & FIELDSParticle physicsCharge conjugation parity time reversal and other discrete symmetrieDecay timeCP violationPhysical Sciences13.25.FtCP violationFísica nuclearLHCParticle Physics - ExperimentTRIPLE-PRODUCT CORRELATIONSPACS: 13.25.Ft 11.30.ErCharm physicNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectLHCb - Abteilung HofmannHadronsAsymmetryNONuclear physicsTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesPiSDG 7 - Affordable and Clean Energy010306 general physicsLarge Hadron Collider (France and Switzerland)Science & Technology/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyHadron-Hadron Scatteringhep-ex010308 nuclear & particles physicsGran Col·lisionador d'HadronsCharm physics; CP violation; Flavor physics; Hadron-Hadron Scattering; Nuclear and High Energy PhysicsBABAR detectorHEPANGULAR-CORRELATIONSLHCbFlavor physicPhase spaceBaBar11.30.ErFísica de partículesExperimentsCharmed mesons (|C|>0 B=0)
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Nucleon localization function in rotating nuclei

2020

Background: An electron localization function was originally introduced to visualize bond structures in molecules. It became a useful tool to describe electron configurations in atoms, molecules and solids. In nuclear physics, a nucleon localization function (NLF) has been used to characterize clusters in light nuclei, fragment formation in fission and pasta phases in the inner crust of neutron stars. Purpose: We use the NLF to study the nuclear response to fast rotation. Methods: We generalize the NLF to the case of nuclear rotation. The extended expressions involve both time-even and time-odd local densities. Since current density and density gradient contribute to the NLF primarily at th…

CURRENTSAngular momentumNuclear TheoryMEAN-FIELDNuclear TheoryFOS: Physical sciences114 Physical sciences01 natural sciencesNuclear Theory (nucl-th)Total angular momentum quantum number0103 physical sciencesSUPERDEFORMED BANDSDISTRIBUTIONScollective levelsNeutron010306 general physicsSpin (physics)EQUATIONSPhysicsCRANKED HARMONIC-OSCILLATOR010308 nuclear & particles physicsYrastnucleon distributionnuclear structure and decaysSTATEElectron localization functionComputational physicsELECTRON LOCALIZATIONMean field theorySYMMETRIESydinfysiikkaNucleonPhysical Review C
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