Search results for "53"

showing 10 items of 2908 documents

Partial wave analysis of ψ(2S)→ppˉη

2013

Using a sample of 1.06 x 10(8) psi(2) events collected with the BESIII detector at BEPCII, the decay psi(2S) -> p (p) over bar eta is studied. A partial wave analysis determines that the intermediate state N(1535) with a mass of 1524 +/- 5(-4)(+10) MeV/c(2) and a width of 130(-24-10)(+27+57) MeV/c(2) is dominant in the decay; the product branching fraction is determined to be B(psi(2S) -> N(1535)(p) over bar x B(N(1535) -> p eta + c.c. = 5.2 +/- 0.3(-1.2)(+3.2)) x 10(-5). Furthermore, the branching fraction of psi(2S) -> p (p) over bar eta is measured to be (6.4 +/- 0.2 +/- 0.6) x 10(-5). Here, the first error is statistical and the second is systematic.

Nuclear and High Energy PhysicsElectron–positron annihilationPartial wave analysiseta --> 2photonAnalytical chemistryannihilation [electron positron]mass spectrumAngular distributionIntermediate stateddc:530angular distributionpsi(3685) --> N(1535) anti-pPhysicsassociated production [eta]BESBranching fractionpsi(3685) --> p anti-p etabranching ratio: measured [psi(3685)]intermediate state [N(1535)]partial wave analysisBeijing StorN(1535) --> p eta3.68 GeV-cmsMass spectrumHigh Energy Physics::ExperimentAtomic physicshadronic decay [psi(3685)]pair production [p]Bar (unit)experimental results
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Change in structure between the $I = 1/2$ states in $^{181}$Tl and $^{177,179}$Au

2018

Abstract The first accurate measurements of the α-decay branching ratio and half-life of the I π = 1 / 2 + ground state in 181Tl have been made, along with the first determination of the magnetic moments and I = 1 / 2 spin assignments of the ground states in 177,179Au. The results are discussed within the complementary systematics of the reduced α-decay widths and nuclear g factors of low-lying, I π = 1 / 2 + states in the neutron-deficient lead region. The findings shed light on the unexpected hindrance of the 1 / 2 + → 1 / 2 + , 181Tl → g 177 Aug α decay, which is explained by a mixing of π 3 s 1 / 2 and π 2 d 3 / 2 configurations in 177Aug, whilst 181Tlg remains a near-pure π 3 s 1 / 2 .…

Nuclear and High Energy PhysicsHadronNuclear physicsThallium nuclei[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences0103 physical sciencesddc:530Nuclear Physics - ExperimentLaser spectroscopy010306 general physicsSpin (physics)PhysicsMagnetic moment010308 nuclear & particles physicsBranching fractionLandé g-factorGold nucleiDecay spectroscopylcsh:QC1-9993. Good healthNuclear deformationPräzisionsexperimente - Abteilung BlaumAtomic physicsGround stateNucleonlcsh:PhysicsDimensionless quantity
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Simplified models for resonant neutral scalar production with missing transverse energy final states

2022

Journal of high energy physics 11(11), 042 (2022). doi:10.1007/JHEP11(2022)042

Nuclear and High Energy PhysicsHiggs particle: decaytransverse energy: missing-energyOther Weak Scale BSM ModelsHiggs particle: heavyFísicaFOS: Physical sciencesdecay [Higgs particle]Monte Carlo [numerical calculations]530High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)heavy [Higgs particle]High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)missing-energy [transverse energy]topological [model]ddc:530model: topologicalnumerical calculations: Monte CarloMulti-Higgs ModelsSpecific BSM Phenomenology
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Vacuum correlators at short distances from lattice QCD

2021

Non-perturbatively computing the hadronic vacuum polarization at large photon virtualities and making contact with perturbation theory enables a precision determination of the electromagnetic coupling at the $Z$ pole, which enters global electroweak fits. In order to achieve this goal ab initio using lattice QCD, one faces the challenge that, at the short distances which dominate the observable, discretization errors are hard to control. Here we address challenges of this type with the help of static screening correlators in the high-temperature phase of QCD, yet without incurring any bias. The idea is motivated by the observations that (a) the cost of high-temperature simulations is typica…

Nuclear and High Energy PhysicsHigh Energy Physics::Latticepolecostshep-latFOS: Physical sciencesLattice QCDQC770-798nonperturbativeoperator product expansion53001 natural sciences7. Clean energythermal [correlation function]lattice [perturbation theory]High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. Radioactivityprecision measurement [electroweak interaction]quantum chromodynamics0103 physical sciencesPerturbative QCDhadronic [vacuum polarization]ddc:530010306 general physicsParticle Physics - Phenomenology010308 nuclear & particles physicsscreeningComputer Science::Information RetrievalphotonHigh Energy Physics - Lattice (hep-lat)lattice field theorytemperaturehep-phParticle Physics - LatticeHigh Energy Physics - Phenomenologyelectromagnetic [coupling]flavor [quark]Journal of High Energy Physics
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The FIRST experiment at GSI

2012

The FIRST (Fragmentation of Ions Relevant for Space and Therapy) experiment at the SIS accelerator of GSI laboratory in Darmstadt has been designed for the measurement of ion fragmentation cross-sections at different angles and energies between 100 and 1000 MeV/nucleon. Nuclear fragmentation processes are relevant in several fields of basic research and applied physics and are of particular interest for tumor therapy and for space radiation protection applications. The start of the scientific program of the FIRST experiment was on summer 2011 and was focused on the measurement of 400 MeV/nucleon 12C beam fragmentation on thin (8 mm) graphite target. The detector is partly based on an alread…

Nuclear and High Energy PhysicsIon beamPhysics::Instrumentation and Detectorsmedicine.medical_treatmentNuclear physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ScintillatorElementary-particleFIRST7. Clean energy01 natural sciencesParticle detectorWire chamberNuclear physicsDipole magnetFragmentationPARTICLE THERAPYhadrontherapy; fragmentation; nuclear physics; elementary-particle; instrumentation; experimental methodsHadrontherapy0103 physical sciencesmedicineNeutron detectionddc:530Gaseous detectorION-BEAM010306 general physicsNuclear ExperimentDETECTORInstrumentationGEANT4PARTICLE THERAPY; FLUKA CODE; ION-BEAM; FRAGMENTATION; BENCHMARKING; RADIOTHERAPY; TRANSPORT; DETECTOR; GEANT4; FIRSTPhysicsParticle therapyTime projection chamber010308 nuclear & particles physicsExperimental methodsDetectorScintillatorTRANSPORTSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Hadrontherapy; Fragmentation; Nuclear physics; Elementary-particle; Experimental methods; InstrumentationFLUKA CODEBENCHMARKINGElementary-particle; Experimental methods; Fragmentation; Hadrontherapy; Instrumentation; Nuclear physics; Instrumentation; Nuclear and High Energy PhysicsRADIOTHERAPY
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First intense isotopic titanium-50 beam using MIVOC method

2012

Abstract An organometallic compound isotopically enriched in titanium-50 has been successfully used for the first time to produce intense ion beams with an ECR ion source by means of the MIVOC method. After some fruitful tests performed with compounds produced at IPHC Strasbourg with natural titanium, enriched organometallic titanium compound was produced successfully, beam extracted from ECR ion sources and accelerated through a K = 130 MeV cyclotron to an energy of 242 MeV. This isotopic 50 Ti 11 + beam was used for the first time in three week-experiment with typical MIVOC stable operating conditions. After optimization, up to 19.4 μA of titanium-50 in charge state 11 + could be extracte…

Nuclear and High Energy PhysicsIon beamta114010308 nuclear & particles physicsMaterial consumptionRadiochemistryCyclotronAnalytical chemistrychemistry.chemical_element7. Clean energy01 natural sciencesElectron cyclotron resonanceIon sourceIonlaw.inventionchemistrylaw0103 physical sciencesddc:530010306 general physicsInstrumentationBeam (structure)Titanium
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Monte Carlo simulation of a single detector unit for the neutron detector array NEDA

2012

WOS: 000301813500009

Nuclear and High Energy PhysicsLiquid scintillatorBC501Physics::Instrumentation and DetectorsNeutron detectorMonte Carlo methodGeant4ScintillatorNEDA7. Clean energy01 natural sciencesSignalNuclear physicsOpticsBC501A0103 physical sciencesNeutron detectionFysikNeutron[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsInstrumentationMonte Carlo simulationPhysicsBC537010308 nuclear & particles physicsbusiness.industryDetector16. Peace & justiceDeuteriumPhysical SciencesHigh Energy Physics::Experimentbusiness
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Electronic Structure of Lr+ (Z = 103) from Ab Initio Calculations

2022

Atoms 10(2), 48 (2022). doi:10.3390/atoms10020048

Nuclear and High Energy PhysicsMRCIddc:530MRCI; electronic structure; electric dipole transitionselectric dipole transitionselectronic structureCondensed Matter Physics530Atomic and Molecular Physics and OpticsAtoms
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Ultrafast Dynamics of Magnetic Domain Structures Probed by Coherent Free-Electron Laser Light

2013

Synchrotron radiation news 26(6), 27 - 32 (2013). doi:10.1080/08940886.2013.850384

Nuclear and High Energy PhysicsMagnetic domainMagnetismAstrophysics::High Energy Astrophysical Phenomena02 engineering and technology53001 natural scienceslaw.inventionOpticslaw0103 physical sciencesddc:530010306 general physicsComputingMilieux_MISCELLANEOUSPhysicsMagnetic circular dichroismbusiness.industryScatteringFree-electron laser021001 nanoscience & nanotechnologyLaserAtomic and Molecular Physics and Optics[PHYS.COND.CM-MS]Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]Physics::Accelerator PhysicsAtomic physics0210 nano-technologybusinessUltrashort pulseFermi Gamma-ray Space TelescopeSynchrotron Radiation News
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Experimental Determination of Four-Time Stimulated Echoes in Liquids, Colloidal Suspensions, and Crystals

1998

Four-time stimulated echo experiments have been used to monitor the temporal evolution of the reorientation rates of deuterated molecules or colloidal suspensions. We present extended phase cycles for this seven-pulse experiment. In order to test its performance three vastly different materials are chosen. These include a crystal in which the molecules carry out well-defined 180 degrees flips and a supercooled liquid characterized by a distribution of jump angles centered around 10 degrees. As an example for rotational diffusion, data on a concentrated suspension of polystyrene spheres in a viscous medium are presented. Copyright 1998 Academic Press.

Nuclear and High Energy PhysicsMaterials scienceBiophysicsRotational diffusionCondensed Matter Physics530BiochemistrySuspension (chemistry)Condensed Matter::Soft Condensed MatterCrystalCrystallographyColloidDeuteriumChemical physicsMoleculeStimulated echoPhysics::Chemical PhysicsSupercoolingJournal of magnetic resonance (San Diego, Calif. : 1997)
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