Search results for "SPECTRA"

showing 10 items of 3542 documents

Suppression of charged particle production at large transverse momentum in central Pb–Pb collisions at sNN=2.76 TeV

2011

Inclusive transverse momentum spectra of primary charged particles in Pb-Pb collisions at root s(NN) = 2.76 TeV have been measured by the ALICE Collaboration at the LHC. The data are presented for central and peripheral collisions, corresponding to 0-5% and 70-80% of the hadronic Pb-Pb cross section. The measured charged particle spectra in |eta| < 0.8 and 0.3 < p(T) < 20 GeV/c are compared to the expectation in pp collisions at the same root s(NN), scaled by the number of underlying nucleon-nucleon collisions. The comparison is expressed in terms of the nuclear modification factor R-AA. The result indicates only weak medium effects (R-AA approximate to 0.7) in peripheral collisions. In cen…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHadronModification factor01 natural sciencesCentral regionSpectral lineCharged particleNuclear physicsCross section (physics)0103 physical sciencesTransverse momentumNuclear Experiment010306 general physicsPhysics Letters B
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Production of charged pions, kaons and protons at large transverse momenta in pp and Pb–Pb collisions at sNN=2.76 TeV

2014

Transverse momentum spectra of pi(+/-), K-+/- and p((p) over bar) up to p(T) = 20 GeV/c at mid-rapidity in pp, peripheral (60-80%) and central (0-5%) Pb-Pb collisions at v root s(NN) = 2.76 TeV have been measured using the ALICE detector at the Large Hadron Collider. The proton-to-pion and the kaon-to-pionratios both show a distinct peak at p(T) approximate to 3 GeV/c in central Pb-Pb collisions. Below the peak, p(T) 10 GeV/c particle ratios in pp and Pb-Pb collisions are in agreement and the nuclear modification factors for pi(+/-), K-+/- and p((p) over bar) indicate that, within the systematic and statistical uncertainties, the suppression is the same. This suggests that the chemical comp…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderJet (particle physics)Charged particleSpectral lineBaryonNuclear physicsTransverse planePionHigh Energy Physics::ExperimentNuclear ExperimentBar (unit)Physics Letters B
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A perturbative QCD analysis of charged-particle distributions in hadronic and nuclear collisions

2002

We compute the distributions of charged particles at large transverse momenta in $p\bar p(p)$, $pA$ and $AA$ collisions in the framework of perturbative QCD, by using collinear factorization and the modern PDFs and fragmentation functions. At the highest cms-energies the shape of the spectra measured in $p\bar p(p)$ collisions at large $q_T$ can be well explained. The difference between the data and the lowest-order computation is quantified in terms of a constant $K$-factor for each energy. The $K$-factor is found to systematically decrease with growing $\sqrt s$. Also a lower limit for the partonic transverse momentum, $p_0$, is extracted for each $\sqrt s$ based on the comparison with th…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderNuclear Theory010308 nuclear & particles physicsHadronPerturbative QCDFOS: Physical sciencesParton01 natural sciencesCharged particleSpectral lineNuclear Theory (nucl-th)High Energy Physics - PhenomenologyTransverse planeHigh Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciences010306 general physicsNuclear Experiment
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What to learn from dilepton transverse momentum spectra in heavy-ion collisions?

2007

Recently the NA60 collaboration has presented high precision measurements of dimuon spectra double differential in invariant mass $M$ and transverse pair momentum $p_T$ in In-In collisions at $158 {\rm AGeV}$. While the $M$-dependence is important for an understanding of in-medium changes of light vector mesons and is $p_T$ integrated insensitive to collective expansion, the $p_T$-dependence arises from an interplay between emission temperature and collective transverse flow. This fact can be exploited to derive constraints on the evolution model and in particular on the contributions of different phases of the evolution to dimuon radiation into a given $M$ window. We present arguments that…

PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsPhase (waves)FOS: Physical sciencesRadiation01 natural sciencesSpectral lineMomentumTransverse planeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Flow (mathematics)0103 physical sciencesInvariant massHigh Energy Physics::Experiment010306 general physicsNuclear Experiment
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Towards the understanding of the meson spectra

2004

We present a quark-quark interaction for the complete study of the meson spectra, from the light to the heavy sector. We compare the quark model predictions against well-established $q\bar q$ experimental data. This allows to identify discrepancies between quark model results and experiment that may signal physics beyond conventional hadron spectroscopy.

PhysicsNuclear and High Energy PhysicsParticle physicsMesonBar (music)High Energy Physics::LatticeQuark modelNuclear TheoryHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesAstronomy and AstrophysicsSignalAtomic and Molecular Physics and OpticsSpectral lineHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Hadron spectroscopyHigh Energy Physics::ExperimentNuclear Experiment
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Measurements of |Vcb|, form factors and branching fractions in the decays → ℓ and → ℓ

1997

Two samples of exclusive semileptonic decays, 579 B0 -> D*+l-νl events and 261 B0 -> D+l-νl events, are selected from approximately 3.9 million hadronic Z decays collected by the ALEPH detector at LEP. From the reconstructed differential decay rate of each sample, the product of the hadronic form factor F(ω) at zero recoil of the D(*)+ meson and the CKM matrix element Vcb are measured to be FD*+ (1) Vcb = (31.9 +/- 1.8stat +/- 1.9syst) × 10-3,FD+ (1) Vcb = (27.8 +/- 6.8stat +/- 6.5syst) × 10-3. The ratio of the form factorsFD+ (1) and FD*+ (1) is measured to beFD+ (1)/FD*+ (1) = 0.87 +/- 0.22stat +/- 0.21syst. A value of Vcb is extracted from the two samples, using theoretical constraints o…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonCabibbo–Kobayashi–Maskawa matrixElectron–positron annihilationHigh Energy Physics::PhenomenologyHadronCurvatureSpectral lineALEPH ExperimentRecoilHigh Energy Physics::ExperimentAtomic physicsALEPH experimentPhysics Letters B
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IS THE MESON SPECTRUM LIMITED?

2011

A precise description of the high excited meson spectra is obtained from the solution of the spinless Salpeter equation for a static radial potential. The coulombic asymptotic behavior of such potential suggests that the meson spectra are limited so that no single [Formula: see text] states may exist beyond a limiting mass.

PhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::PhenomenologyNuclear TheorySpectrum (functional analysis)Eta mesonAstronomy and AstrophysicsLimitingAtomic and Molecular Physics and OpticsSpectral lineQuantum electrodynamicsExcited stateInternational Journal of Modern Physics A
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Constituent quark model study of the meson spectra

2004

The $q\bar q$ spectrum is studied in a generalized constituent quark model constrained in the study of the $NN$ phenomenology and the baryon spectrum. An overall good fit to the available experimental data is obtained. A detailed analysis of all sectors from the light-pseudoscalar and vector mesons to bottomonium is performed paying special attention to the existence and nature of some non well-established states. These results should serve as a complementary tool in distinguishing conventional quark model mesons from glueballs, hybrids or multiquark states.

PhysicsNuclear and High Energy PhysicsParticle physicsMesonModel studyHigh Energy Physics::LatticeQuark modelNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesConstituent quarkFísicaSpectral lineBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentPhenomenology (particle physics)
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Supernova Bounds on Supersymmetric $R$-parity Violating Interactions

1996

We re-examine resonant massless-neutrino conversions in a dense medium induced by flavour changing neutral current (FCNC) interactions. We show how the observed $\bar\nu_e$ energy spectra from SN1987a and the supernova $r$-process nucleosynthesis provide constraints on supersymmetric models with $R$ parity violation, which are much more stringent than those obtained from the laboratory. We also suggest that resonant massless-neutrino conversions may play a positive role in supernova shock reheating. Finally, we examine the constraints on explicit $R$-parity-violating FCNCs in the presence of non-zero neutrino masses in the eV range, as indicated by present hot dark matter observations.

PhysicsNuclear and High Energy PhysicsParticle physicsNeutral currentHot dark matterAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaParity (physics)AstrophysicsSpectral lineSupernovaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)NucleosynthesisR-parityHigh Energy Physics::ExperimentNeutrino
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Antikaon-nucleon interaction and Lambda(1405) in chiral SU(3) dynamics

2016

The properties of the Lambda(1405) resonance are key ingredients for determining the antikaon-nucleon interaction in strangeness nuclear physics, and the novel internal structure of the Lambda(1405) is of great interest in hadron physics, as a prototype case of a baryon that does not fit into the simple three-quark picture. We show that a quantitative description of the antikaon-nucleon interaction with the Lambda(1405) is achieved in the framework of chiral SU(3) dynamics, with the help of recent experimental progress. Further constraints on the Kbar N subthreshold interaction are provided by analyzing pi Sigma spectra in various processes, such as the K-d -&gt; pi Sigma n reaction and the…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsHadronNuclear TheoryFOS: Physical sciencesMolecular configurationStrangeness16. Peace & justice01 natural sciencesResonance (particle physics)Spectral lineBaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNucleonWave functionNuclear Experiment
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