Search results for "ddc:"

showing 10 items of 3080 documents

A new assessment of the alleged link between element 115 and element 117 decay chains

2016

Physics letters 760, 293-296(2016). doi:10.1016/j.physletb.2016.07.008

PhysicsNuclear and High Energy PhysicsIsotope010308 nuclear & particles physicsSuperheavy elementscorrelation analysisSuperheavy Elements53001 natural scienceslcsh:QC1-999Nuclear physics0103 physical sciencesCorrelation analysisSubatomic Physicsddc:530Atomic numberDecay chainAtomic physicsElement (category theory)010306 general physicsLink (knot theory)Spectroscopylcsh:PhysicsPhysics Letters B
researchProduct

High-resolution laser resonance ionization spectroscopy of $^{143-147}$Pm

2020

The European physical journal / A 56(2), 69 (2020). doi:10.1140/epja/s10050-020-00061-8

PhysicsNuclear and High Energy PhysicsIsotope530 Physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530 Physik53001 natural sciencesIon source010305 fluids & plasmasIonization0103 physical sciencesQuadrupoleNuclear fusionddc:530Physics::Atomic PhysicsAtomic physics010306 general physicsSpectroscopyNuclear ExperimentHyperfine structureMagnetic dipole
researchProduct

Letter

2021

We present a study of the power threshold for L–H transitions (PLH) in almost pure helium plasmas, obtained in recent experiments at JET with an ITER-like wall (Be wall and W divertor). The most notable new result is that the density at which PLH is minimum, ${\bar{n}}_{\text{e},\mathrm{min}}$, is considerably higher for helium than for deuterium and hydrogen plasmas. We discuss the possible implications for ITER in its pre-fusion operating power phase.

PhysicsNuclear and High Energy PhysicsJet (fluid)L–H transitionchemistry.chemical_elementPlasmaheliumCondensed Matter Physics01 natural sciences010305 fluids & plasmasddc:chemistry0103 physical sciencesAtomic physics010306 general physicstokamakHelium
researchProduct

Silicon microstrip detectors for the ATLAS SCT

2002

Abstract The ATLAS Semiconductor Tracker at the Large Hadron Collider (LHC) will incorporate ∼20,000 individual silicon microstrip sensors representing ∼60 m 2 of silicon. Production and delivery of the sensors is already underway and scheduled for completion by late 2002. The sensors have been optimised for operation in the harsh radiation environment of the LHC, and subjected to an extensive qualification program in which their pre- and post-irradiation characteristics have been evaluated. The sensor design features are reviewed, together with their electrical characteristics and the Quality Control procedures adopted by ATLAS during production.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderSiliconbusiness.industryQuality controlchemistry.chemical_elementddc:500.2Linear particle acceleratorParticle detectorSemiconductor detectorNuclear physicsmedicine.anatomical_structureSemiconductorchemistryAtlas (anatomy)medicineElectronic engineeringIrradiationATLAS SCTbusinessInstrumentationSilicon microstrip detectorsSilicon microstrip detectorsNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
researchProduct

Precision measurement of the conversion electron spectrum of 83mKr with a solenoid retarding spectrometer

1992

This paper reports on precision measurements of conversion lines in the decay of 83mKr with nuclear transition energies of 32.1 keV and 9.4 keV, respectively. The spectra were taken from a submonolayer surface of 83mKr frozen onto a cold backing, using the new Mainz solenoid retarding spectrometer. The high luminosity and resolution of this instrument enables the observation of all allowed conversion lines up to the N-shell and to fully separate the elastic component from inelastic satellites. The combined analysis of the data yields the transition energies Ey=32151.5±1.1 eV and 9405.9±0.8 eV, respectively. The experiment served also to pilot the application of this spectrometer to the ques…

PhysicsNuclear and High Energy PhysicsLuminosity (scattering theory)SpectrometerSolenoidElectronpacs:29.30.Dnpacs:27.50.+eElectron spectroscopySpectral lineNuclear physicsNuclear fusionddc:530NeutrinoAtomic physics
researchProduct

Excitation energy dependence of fragment-mass distributions from fission of 180,190 Hg formed in fusion reactions of 36 Ar + 144,154 Sm

2015

Physics letters / B 748, 89 - 94 (2015). doi:10.1016/j.physletb.2015.06.068

PhysicsNuclear and High Energy PhysicsMass asymmetryCluster decayIsotopeFissionNuclear Theory180190HgFusion–fissionActinide530lcsh:QC1-999Mass asymmetric fissionMass spectrumNuclear fusionddc:530Atomic physicsNuclear Experimentlcsh:PhysicsExcitationPhysics Letters B
researchProduct

The magnetic moment of the ρ-meson

2014

The magnetic moment of the \rho-meson is calculated in the framework of a low-energy effective field theory of the strong interactions. We find that the complex-valued strong interaction corrections to the gyromagnetic ratio are small leading to a value close to the real leading tree level result, g_\rho = 2. This is in a reasonably good agreement with the available lattice QCD calculations for this quantity.

PhysicsNuclear and High Energy PhysicsMesonMagnetic moment010308 nuclear & particles physicsHigh Energy Physics::LatticeGyromagnetic ratioStrong interactionLattice QCDReal tree01 natural sciencesHigh Energy Physics - PhenomenologyQuantum electrodynamics0103 physical sciencesEffective field theoryddc:530010306 general physicsValue (mathematics)
researchProduct

Helicity Amplitudes of the Lambda(1670) and two Lambda(1405) as dynamically generated resonances

2010

We determine the helicity amplitudes A(1/2) and radiative decay widths in the transition Lambda(1670) -> gamma Y (Y = Lambda or Sigma(0)). The Lambda(1670) is treated as a dynamically generated resonance in meson-baryon chiral dynamics. We obtain the radiative decay widths of the Lambda(1670) to gamma Lambda as 2 +/- 1 keV and to -gamma Sigma(0) as 120 +/- 50 keV. Also, the Q(2)-dependence of the helicity amplitudes A(1/2) is calculated. We find that the K Xi component in the Lambda(1670) structure, mainly responsible for the dynamical generation of this resonance, is also responsible for the significant suppression of the decay ratio Gamma(gamma A)/Gamma(gamma Sigma 0). A measurement of th…

PhysicsNuclear and High Energy PhysicsNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaAnalytic continuationFísicaResonanceFOS: Physical sciencesLambdaHelicityLoop (topology)Nuclear Theory (nucl-th)symbols.namesakeAmplitudesymbolsFeynman diagramddc:530Atomic physicsComplex plane
researchProduct

The electroweak sector of the NMSSM at the one-loop level

2010

We present the electroweak spectrum for the Next-to-Minimal Supersymmetric Standard Model at the one-loop level, e. g. the masses of Higgs bosons, sleptons, charginos and neutralinos. For the numerical evaluation we present a mSUGRA variant with non-universal Higgs mass parameters squared and we compare our results with existing ones in the literature. Moreover, we briefly discuss the implications of our results for the calculation of the relic density.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsElectroweak interactionSpectrum (functional analysis)High Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesLoop (topology)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonddc:530High Energy Physics::Experiment010306 general physicsParticle Physics - PhenomenologyMinimal Supersymmetric Standard ModelBoson
researchProduct

Cross section measurements of high-p(T) dilepton final-state processes using a global fitting method

2008

We present a new method for studying high-$p_T$ dilepton events ($e^{\pm}e^{\mp}$, $\mu^{\pm}\mu^{\mp}$, $e^{\pm}\mu^{\mp}$) and simultaneously extracting the production cross sections of $p\bar{p} \to t\bar{t}$, $p\bar{p} \to W^+W^-$, and $p\bar{p} \to \ztt$ at a center-of-mass energy of $\sqrt{s} = 1.96$ TeV. We perform a likelihood fit to the dilepton data in a parameter space defined by the missing transverse energy and the number of jets in the event. Our results, which use $360 {\rm pb^{-1}}$ of data recorded with the CDF II detector at the Fermilab Tevatron Collider, are $\sigma(t\bar{t}) = 8.5_{-2.2}^{+2.7}$ pb, $\sigma(W^+W^-) = 16.3^{+5.2}_{-4.4}$ pb, and $\sigma(\ztt) =291^{+50}_…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyGlobal fittingFOS: Physical sciencesddc:500.2State (functional analysis)Astronomy & Astrophysics;; Physics Particles & Fields01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)CrystallographyTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciences_High Energy Physics::ExperimentProduction (computer science)010306 general physicsEnergy (signal processing)Bar (unit)Lepton
researchProduct