Search results for "LESS"

showing 10 items of 2452 documents

Double pion photoproduction off nuclei - Are there effects beyond final-state interaction?

2013

Photoproduction of $\pi^{0}\pi^{0}$ and $\pi^{0}\pi^{\pm}$ pairs from nuclei has been measured over a wide mass range ($^2$H, $^{7}$Li, $^{12}$C, $^{40}$Ca, and $^{\rm nat}$Pb) for photon energies from threshold to 600 MeV. The experiments were performed at the MAMI accelerator in Mainz, using the Glasgow photon tagging spectrometer and a 4$\pi$ electromagnetic calorimeter consisting of the Crystal Ball and TAPS detectors. A shift of the pion-pion invariant mass spectra for heavy nuclei to small invariant masses has been observed for $\pi^0$ pairs but also for the mixed-charge pairs. The precise results allow for the first time a model-independent analysis of the influence of pion final-sta…

PhysicsNuclear and High Energy PhysicsParticle physicsdouble pion photoproduction; crystal ball; sigma-in-medium modificationPhotonMeson010308 nuclear & particles physicsHadronNuclear TheoryCarbon-12FOS: Physical sciencesElementary particle01 natural sciences7. Clean energyNuclear physicsMassless particlePion0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentCrystal Ball
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Photon Scattering with the Lorentz Integral Transform Method

2011

The application of the Lorentz integral transform (LIT) method to photon scattering off nuclei is presented in general. As an example, elastic photon scattering off the deuteron in the unretarded dipole approximation is considered using the LIT method. The inversion of the integral transform is discussed in detail paying particular attention to the high-energy contributions in the resonance term. The obtained E1-polarizabilities are compared to results from the literature. The corresponding theoretical cross section is confronted with experimental results confirming, as already known from previous studies, that the E1-contribution is the most important one at lower energies.

PhysicsNuclear and High Energy PhysicsPhotonNuclear TheoryLorentz transformationFOS: Physical sciencesElementary particleDiscrete dipole approximationIntegral transformMassless particleNuclear Theory (nucl-th)symbols.namesakeDipolePolarizabilityQuantum mechanicsQuantum electrodynamicssymbols
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Enhancement of thermal photon production in event-by-event hydrodynamics

2011

Thermal photon emission is widely believed to reflect properties of the earliest, hottest evolution stage of the medium created in ultra-relativistic heavy-ion collisions. Previous computations of photon emission have been carried out using a hydrodynamical medium description with smooth, averaged initial conditions. Recently, more sophisticated hydrodynamical models which calculate observables by averaging over many evolutions with event-by-event fluctuating initial conditions (IC) have been developed. Given their direct connection to the early time dynamics, thermal photon emission appears an ideal observable to probe fluctuations in the medium initial state. In this work, we demonstrate …

PhysicsNuclear and High Energy PhysicsPhotonPhoton antibunchingta114010308 nuclear & particles physicsFOS: Physical sciencesElementary particleMonte Carlo method for photon transportObservable01 natural sciences7. Clean energyNuclear physicsMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesThermal010306 general physicsEvent (particle physics)
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Results from the AMANDA telescope

2003

We present results from the AMANDA high energy neutrino telescope located at the South Pole. They include measurements of the atmospheric neutrino flux, search for UHE point sources, and diffuse sources producing electromagnetic/hadronic showers at the detector or close to it.

PhysicsNuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyAstrophysics::Instrumentation and Methods for AstrophysicsAstronomyFluxCosmic rayAstrophysicsParticle detectorlaw.inventionMassless particleTelescopeNeutrino detectorlawHigh Energy Physics::ExperimentNeutrinoLeptonNuclear Physics A
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Precision measurements of proton emission from the ground states ofTa156andRe160

2011

The decays of the $\ensuremath{\pi}{d}_{3/2}$ ground states of $^{156}\mathrm{Ta}$ and $^{160}\mathrm{Re}$ have been studied in detail using the GREAT spectrometer. More than 7000 $^{160}\mathrm{Re}$ nuclei were produced in reactions of 290- and 300-MeV $^{58}\mathrm{Ni}$ ions with an isotopically enriched $^{106}\mathrm{Cd}$ target and separated in flight using the RITU separator. The proton and $\ensuremath{\alpha}$ decays of the $\ensuremath{\pi}{d}_{3/2}$ level were confirmed and the half-life and branching ratios of this state were determined with improved precision to be ${t}_{1/2}=611\ifmmode\pm\else\textpm\fi{}7$ $\ensuremath{\mu}$s and ${b}_{\mathrm{p}}=89\ifmmode\pm\else\textpm\fi…

PhysicsNuclear and High Energy PhysicsProtonBranching fractionHadronElementary particleAlpha decayAtomic physicsNucleonGround stateDimensionless quantityPhysical Review C
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Two-neutrino double-beta decay of76Ge in an anharmonic vibrator approach

2009

We have calculated the nuclear matrix element of two-neutrino double-beta (2???) decay of 76Ge by using the proton?neutron microscopic anharmonic vibrator approach (pnMAVA). In the pnMAVA the wavefunctions of the intermediate 1+ states in 76As have a one-phonon part containing the proton?neutron QRPA (pnQRPA) phonons and a two-phonon part built by coupling the pnQRPA and charge-conserving QRPA phonons. We compare the measured GT? and GT+ Gamow?Teller strength functions with the measured ones. The two-phonon components of the pnMAVA wavefunctions cause the pnQRPA strength to redistribute over a finite energy range. This has only a small effect on the value 2??? nuclear matrix element. This s…

PhysicsNuclear and High Energy PhysicsProtonNuclear TheoryAnharmonicityElementary particleNuclear physicsMassless particleDouble beta decayNeutronAtomic physicsNeutrinoNuclear ExperimentWave functionJournal of Physics G: Nuclear and Particle Physics
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Duality relation between radiation thermodynamics and cosmic string loop thermodynamics

2011

We discuss thermodynamics of electromagnetic radiation, with p=(1/3){rho} and S{proportional_to}T{sup 3}V, and of cosmic string loops, with p=-(1/3){rho} and S{proportional_to}T{sup -3}V, where p stands for pressure, T temperature, {rho} energy density, S entropy, and V volume. We write the thermodynamic formalisms under a common framework that illustrates their formal relationship and allows us to go from one to the other through a smooth transformation. From a microscopic perspective, these relations arise from the energy relations u({lambda})=hc/{lambda} for the photons of electromagnetic radiation, and u(l)=(c{sup 4}/a{sup 2}G)l for cosmic string loops, a being a numerical (dimensionles…

PhysicsNuclear and High Energy PhysicsThermodynamicsElementary particleLambdaPlanck constantElectromagnetic radiationGravitational constantCosmic stringEntropy (classical thermodynamics)symbols.namesakeQuantum mechanicssymbolscosmic stringelectromagnetic radiation thermodynamics T-duality thermal duality.Settore MAT/07 - Fisica MatematicaDimensionless quantityPhysical Review D
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Measurement oftt¯production in theτ+jetstopology usingpp¯collisions ats=1.96  TeV

2010

We present a measurement of the t (t) over bar production cross section multiplied by the branching ratio to tau lepton decaying semihadronically (tau(h)) plus jets, sigma(p (p) over bar -> t (t) over bar + X) center dot BR(t (t) over bar -> tau(h) + jets), at a center of mass energy root s = 1.96 TeV using 1 fb(-1) of integrated luminosity collected with the D0 detector. Assuming a top quark mass of 170 GeV, we measure sigma(t (t) over bar) center dot BR tau h (+ j) = 0.60(-0.22)(+0.23)(stat)(-0.14)(+0.15)(syst) +/- 0.04(lumi) pb. In addition, we extract the t (t) over bar production cross section using the t (t) over bar -> tau(h) + jets topology, with the result sigma(t (t) over bar) = 6…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physics010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyElementary particleTopology01 natural sciencesNuclear physicsParticle decay0103 physical sciencesHigh Energy Physics::ExperimentCenter of mass010306 general physicsLeptonDimensionless quantityBar (unit)Physical Review D
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Universal features of the nuclear matrix elements governing the mass sector of the 0νββ decay

2005

In this work we report on manifest universal features found in the nuclear matrix elements which govern the mass sector of the neutrinoless double beta decay. The results are based on the analysis of the calculated matrix elements corresponding to the decays of 76Ge, 82Se, 100Mo, and 116Cd. The results suggest a dominance of few low-lying nuclear states of few multipoles in these matrix elements. Dedicated charge-exchange reactions could be used to probe these key states to determine experimentally the value of the nuclear matrix element.

PhysicsNuclear and High Energy PhysicsWork (thermodynamics)MatrixFísicaNeutrinoless double betaNuclear matrixNuclear physicsMatrix (mathematics)Double beta decayPartículas ElementalesElement (category theory)Multipole expansionNuclear ExperimentCiencias ExactasPhysics Letters B
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Massive neutrinos and right-handed weak currents in double beta decay.

1993

The contributions of right-handed weak currents in neutrinoless double beta decay are studied taking explicitly into account the mass corrections to the intermediate neutrino propagator. Due to these corrections the right-handed currents become effective even if all neutrinos are light ([ital m][sub [nu]][gt]10 MeV). Explicit expressions for the neutrino-momentum integrals and the decay half-life are derived. As an example two neutrino-mass scenarios containing the hypothetical 17-keV neutrino are discussed. The experimental half-life of the [sup 76]Ge[r arrow][sup 76]Se decay is used to obtain an upper limit for a new kind of effective right-handed coupling within the two scenarios.

PhysicsNuclear physicsMassless particleNuclear and High Energy PhysicsParticle physicsIsotopes of germaniumDouble beta decayHigh Energy Physics::ExperimentElementary particleNeutrinoBeta decayRadioactive decayLeptonPhysical review. C, Nuclear physics
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