Search results for "Particle physics"

showing 10 items of 6826 documents

First measurement of jet mass in Pb–Pb and p–Pb collisions at the LHC

2018

This letter presents the first measurement of jet mass in Pb–Pb and p–Pb collisions at sNN=2.76 TeV and sNN=5.02 TeV, respectively. Both the jet energy and the jet mass are expected to be sensitive to jet quenching in the hot Quantum Chromodynamics (QCD) matter created in nuclear collisions at collider energies. Jets are reconstructed from charged particles using the anti-kT jet algorithm and resolution parameter R=0.4. The jets are measured in the pseudorapidity range |ηjet|<0.5 and in three intervals of transverse momentum between 60 GeV/c and 120 GeV/c. The measurement of the jet mass in central Pb–Pb collisions is compared to the jet mass as measured in p–Pb reference collisions, to vac…

Nuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::Experimenthiukkasfysiikkaparticle physicsNuclear Experiment
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Measurement of the spin of the Xi(1530) resonance

2008

The properties of the Xi(1530) resonance are investigated in the Lambdac+ --&gt; Xi- pi+ K+ decay process. The data sample was collected with the BaBar detector at the SLAC PEP-II asymmetric-energy e+ e- collider operating at center of mass energies 10.58 and 10.54 GeV. The corresponding integrated luminosity is approximately 230 inverse fb. The spin of the Xi(1530) is established to be 3/2. The existence of an S-wave amplitude in the Xi- pi+ system is inferred, and its interference with the Xi(1530)0 amplitude provides the first clear demonstration of the Breit-Wigner phase motion expected for the Xi(1530). The P_1(cos[theta(Xi-)]) Legendre polynomial moment indicates the presence of a sig…

Nuclear and High Energy PhysicsBABARElectron–positron annihilationFOS: Physical sciencesDalitz plotMASSPARTICLE PHYSICS; PEP2; BABAR01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decay0103 physical sciencesPEP2MASS; PARITY; WIDTH[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsPhysicsPARITY010308 nuclear & particles physicsHyperonWIDTHResonanceBABAR detectorHEPCharmed baryonsAmplitudeBaBarPARTICLE PHYSICSCenter of massFísica de partículesExperiments
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Measurement of the Mass Difference m(B0) - m(B+)

2008

Using 230 million B Bbar events recorded with the BABAR detector at the e+ e- storage rings PEP-II, we reconstruct approximately 4100 B0 to J/psi K+ pi- and 9930 B+ to J/psi K+ decays with J/psi to mu+ mu- and e+ e-. From the measured B-momentum distributions in the e+ e- rest frame, we determine the mass difference m(B0) - m(B+) = (+0.33 +- 0.05 +- 0.03) MeV/c^2.

Nuclear and High Energy PhysicsBABARFOS: Physical sciencesNEUTRAL BPARTICLE PHYSICS; PEP2; BABAR01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsParticle decayHigh Energy Physics - Experiment (hep-ex)TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYCHARGED B0103 physical sciencesPEP2[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]B MESON; MASS DIFFERENCE; CHARGED B; NEUTRAL BMASS DIFFERENCE010306 general physicsPhysics010308 nuclear & particles physicsParticle physicsBABAR detectorHEPCrystallographyB MESONBaBarPARTICLE PHYSICS13.25.Hw 13.40.Dk 14.40.NdFísica de partículesExperiments
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Broad excitations in a 2+1D overoccupied gluon plasma

2021

Motivated by the initial stages of high-energy heavy-ion collisions, we study excitations of far-from-equilibrium 2+1 dimensional gauge theories using classical-statistical lattice simulations. We evolve field perturbations over a strongly overoccupied background undergoing self-similar evolution. While in 3+1D the excitations are described by hard-thermal loop theory, their structure in 2+1D is nontrivial and nonperturbative. These nonperturbative interactions lead to broad excitation peaks in spectral and statistical correlation functions. Their width is comparable to the frequency of soft excitations, demonstrating the absence of soft quasiparticles in these theories. Our results also su…

Nuclear and High Energy PhysicsCOLLISIONSNuclear TheoryField (physics)FOS: Physical sciencesLattice QCDQC770-798hiukkasfysiikka01 natural sciences114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesPerturbative QCDfysikkField theory (psychology)Gauge theory010306 general physicsKINETIC-THEORYUNIVERSAL DYNAMICSPhysics:Matematikk og Naturvitenskap: 400::Fysikk: 430 [VDP]MASS SCALENUCLEI010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)kvarkki-gluoniplasmaPerturbative QCDLattice QCDFIELD-THEORY3. Good healthGluonHigh Energy Physics - PhenomenologyQuantum electrodynamicsQuark–gluon plasmaQuasiparticleQuark-Gluon PlasmaGAUGE-THEORIESJournal of High Energy Physics
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Measurement of the radiative K-e3 branching ratio

2005

We present a measurement of the relative branching ratio of the decay KL -&gt; pi e nu gamma (Ke3gamma) with respect to KL-&gt; pi e nu (gamma) (Ke3+Ke3gamma) decay. The result is based on observation of 19 000 Ke3gamma and 5.6 x 10^6 Ke3 decays. The value of the branching ratio is Br(Ke3gamma, Egamma^*&gt;30 MeV,theta(e,gamma)^*&gt;20^o)/Br(Ke3)= (0.964+-0.008+0.011-0.009)%. This result agrees with theoretical predictions but is at variance with a recently published result.

Nuclear and High Energy PhysicsChiral perturbation theoryPhotonHadronFOS: Physical scienceskaon decay; NEUTRAL KAON; branching ratio7. Clean energy01 natural sciencesNEUTRAL KAONHigh Energy Physics - ExperimentNuclear physicsmesoni KHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesRadiative transfer[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]radiative kaon decays010306 general physicsmesoni K; decadimenti radiativiPhysics010308 nuclear & particles physicsBranching fractionK13 DECAYSBremsstrahlungkaon decayAmplitudedecadimenti radiativibranching ratioAtomic physicsParticle Physics - Experiment
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Far-off-resonance averaging of dipolar interactions in solids

1997

Abstract The far-off-resonance performance of several line-narrowing sequences is investigated. Both theoretically and experimentally, it is found that transverse relaxation times, dominated by dipole–dipole interactions, are most effectively prolonged not only on-resonance but also for certain, generally large, resonance offsets. These correspond to a situation when, during the basic pulse separation, the frequency offset rotates the toggling-frame Hamiltonian by multiples of 180°. The implications of these results for the study of macroscopic translational diffusion using static-field-gradient NMR are discussed.

Nuclear and High Energy PhysicsCondensed matter physicsChemistryBiophysicsCondensed Matter PhysicsBiochemistryMolecular physicsResonance (particle physics)530Pulse separationDipolesymbols.namesakeTransverse relaxationOff resonancesymbolsFrequency offsetDiffusion (business)Hamiltonian (quantum mechanics)
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The DAMPE silicon–tungsten tracker

2016

Abstract The DArk Matter Particle Explorer (DAMPE) is a spaceborne astroparticle physics experiment, launched on 17 December 2015. DAMPE will identify possible dark matter signatures by detecting electrons and photons in the 5 GeV–10 TeV energy range. It will also measure the flux of nuclei up to 100 TeV, for the study of the high energy cosmic ray origin and propagation mechanisms. DAMPE is composed of four sub-detectors: a plastic strip scintillator, a silicon–tungsten tracker–converter (STK), a BGO imaging calorimeter and a neutron detector. The STK is composed of six tracking planes of 2 orthogonal layers of single-sided micro-strip detectors, for a total detector surface of ca. 7 m2. T…

Nuclear and High Energy PhysicsCosmic rays; Dark matter; Silicon tracker; Spaceborne experiment; Nuclear and High Energy Physics; InstrumentationPhysics::Instrumentation and DetectorsCosmic rayParticle detectorsTracking (particle physics)01 natural sciencesParticle detectorOpticscosmic rays0103 physical sciencesDark matterNeutron detection010303 astronomy & astrophysicsInstrumentationAstroparticle physicsPhysicsLarge Hadron ColliderCalorimeter (particle physics)010308 nuclear & particles physicsbusiness.industryDetectorSettore FIS/01 - Fisica SperimentaleParticle detectors cosmic raysSpaceborne experimentSilicon trackerHigh Energy Physics::Experimentbusiness
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Searching for Earth/Solar axion halos

2020

We discuss the sensitivity of the present and near-future axion dark matter experiments to a halo of axions or axion-like particles gravitationally bound to the Earth or the Sun. The existence of such halos, assuming they are formed, renders a significant gain in the sensitivity of axion searches while satisfying all the present experimental bounds. The structure and coherence properties of these halos also imply novel signals, which can depend on the latitude or orientation of the detector. We demonstrate this by analysing the sensitivity of several distinct types of axion dark matter experiments.

Nuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Atomic Physics (physics.atom-ph)Physics::Instrumentation and DetectorsDark matterFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysics01 natural sciencesPhysics - Atomic PhysicsHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsAxionAstrophysics::Galaxy AstrophysicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyCosmology of Theories beyond the SMHigh Energy Physics - PhenomenologyCP violationBeyond Standard Modellcsh:QC770-798CP violationHaloEarth (classical element)Astrophysics - Cosmology and Nongalactic AstrophysicsCoherence (physics)Journal of High Energy Physics
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Critical point Higgs inflation in the Palatini formulation

2021

We study Higgs inflation in the Palatini formulation with the renormalisation group improved potential in the case when loop corrections generate a feature similar to an inflection point. Assuming that there is a threshold correction for the Higgs quartic coupling $\lambda$ and the top Yukawa coupling $y_t$, we scan the three-dimensional parameter space formed by the two jumps and the non-minimal coupling $\xi$. The spectral index $n_s$ can take any value in the observationally allowed range. The lower limit for the running is $\alpha_s>-3.5\times10^{-3}$, and $\alpha_s$ can be as large as the observational upper limit. Running of the running is small. The tensor-to-scalar ratio is $2.2\tim…

Nuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)FOS: Physical sciencesRIEMANNGeneral Relativity and Quantum Cosmology (gr-qc)Parameter spaceINITIAL CONDITIONSkosmologia01 natural sciences114 Physical sciencesGeneral Relativity and Quantum CosmologyEINSTEINCritical point (thermodynamics)0103 physical sciencesRenormalization Grouplcsh:Nuclear and particle physics. Atomic energy. Radioactivityteoreettinen fysiikkaGENERAL-RELATIVITY010306 general physicscosmology of theories beyond the SMDISSIPATIONBosonMathematical physicsInflation (cosmology)Physics010308 nuclear & particles physicsYukawa potentialCONSTRAINTSBOSONGRAVITATIONRenormalization groupAFFINE VARIATIONAL-PRINCIPLESCosmology of Theories beyond the SMInflection pointHiggs bosonSCALARONlcsh:QC770-798renormalization groupAstrophysics - Cosmology and Nongalactic AstrophysicsJournal of High Energy Physics
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Production of dark-matter bound states in the early universe by three-body recombination

2018

The small-scale structure problems of the universe can be solved by self-interacting dark matter that becomes strongly interacting at low energy. A particularly predictive model for the self-interactions is resonant short-range interactions with an S-wave scattering length that is much larger than the range. The velocity dependence of the cross section in such a model provides an excellent fit to self-interaction cross sections inferred from dark-matter halos of galaxies and clusters of galaxies if the dark-matter mass is about 19 GeV and the scattering length is about 17 fm. Such a model makes definite predictions for the few-body physics of weakly bound clusters of the dark-matter particl…

Nuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Nuclear Theorymedia_common.quotation_subjectPhysics beyond the Standard ModelDark matterFOS: Physical sciencesAstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound stateEffective field theoryCluster (physics)lcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment (nucl-ex)010306 general physicsNuclear Experimentmedia_commonPhysics010308 nuclear & particles physicsScattering lengthCosmology of Theories beyond the SMUniverseGalaxyHigh Energy Physics - PhenomenologyBeyond Standard Modellcsh:QC770-798Astrophysics - Cosmology and Nongalactic Astrophysics
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