Search results for "numerical calculations"

showing 10 items of 91 documents

On the pion cloud of the nucleon

2003

We evaluate the two--pion contribution to the nucleon electromagnetic form factors by use of dispersion analysis and chiral perturbation theory. After subtraction of the rho--meson component, we calculate the distributions of charge and magnetization in coordinate space, which can be interpreted as the effects of the pion cloud. We find that the charge distribution of this pion cloud effect peaks at distances of about 0.3 fm. Furthermore, we calculate the contribution of the pion cloud to the isovector charges and radii of the nucleon.

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear Theorydispersion relationHigh Energy Physics::LatticeisovectorNuclear Theorychiral [perturbation theory]FOS: Physical sciencestwo-pion [effect]form factor [nucleon]density [charge]Nuclear physicsNuclear Theory (nucl-th)PionHigh Energy Physics - Phenomenology (hep-ph)ddc:530Perturbation theoryCoordinate spacenumerical calculationsNuclear ExperimentPhysicsIsovectorpole [rho(770)]Charge densityCharge (physics)High Energy Physics - Phenomenologycloud [pi]High Energy Physics::Experimentspectral representationNucleon
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Determining Sneutrino Masses and Physical Implications

2005

In some areas of supersymmetry parameter space, sneutrinos are lighter than the charginos and the next-to-lightest neutralino, and they decay into the invisible neutrino plus lightest-neutralino channel with probability one. In such a scenario they can be searched for in decays of charginos that are pair-produced in e+e- collisions, and in associated sneutrino-chargino production in photon-electron collisions. The sneutrino properties can be determined with high accuracy from the edges of the decay energy spectra in the first case and from threshold scans in the second. In the final part of the report we investigate the mass difference of sneutrinos and charged sleptons between the third an…

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesannihilation [electron positron]decay modes [chargino]SO(10) [grand unified theory]Nuclear physicsParticle decayHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometrypair production [chargino]interaction [photon electron]Invariant massddc:530numerical calculationsPhysicsmass difference [slepton]High Energy Physics::PhenomenologySuperpartnerSupersymmetryboundary conditionseesaw modelHigh Energy Physics - PhenomenologyPair productionNeutralino(4lepton 2sneutrino) [final state]width [chargino]branching ratio [chargino]High Energy Physics::Experimentassociated production [sneutrino]Neutrinomass spectrum [sneutrino]
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Quark-model based study of the triton binding energy

2001

The three-nucleon bound state problem is studied employing a nucleon-nucleon potential obtained from a basic quark-quark interaction in a five-channel Faddeev calculation. The obtained triton binding energy is comparable to those predicted by conventional models of the $NN$ force.

Nuclear and High Energy PhysicsParticle physicsNuclear Theorycoupled channel [partial wave analysis]Nuclear TheoryBinding energyFOS: Physical scienceselastic scattering [nucleon nucleon]Few-body systemsinteraction [quark quark]Nuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Bound stateddc:530numerical calculationsNuclear ExperimentNuclear theoryPhysicsQuark modelbinding energy [tritium]Three-body problemHigh Energy Physics - Phenomenologynonrelativistic [quark]three-body problempotential [nucleon nucleon]Physical Review C
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Study of the f(2)(1270) , f(2)'(1525) , f(0)(1370) and f(0)(1710) in the J/psi radiative decays

2009

In this paper we present an approach to study the radiative decay modes of the J/psi into a photon and one of the tensor mesons f (2)(1270) , f' (2)(1525) , as well as the scalar ones f (0)(1370) and f (0)(1710) . Especially, we compare predictions that emerge from a scheme where the states appear dynamically in the solution of vector meson-vector meson scattering amplitudes to those from a (admittedly naive) quark model. We provide evidence that it might be possible to distinguish amongst the two scenarios, once improved data are available.

Nuclear and High Energy PhysicsParticle physicsPhotonMesonScalar (mathematics)Radiative decayhadronic decay [J/psi(3100)]01 natural sciencesf0(1710)bound state [vector meson]radiative decay [J/psi(3100)]0103 physical sciencesRadiative transferddc:530f0(1370)Tensor010306 general physicsnumerical calculationsdecay modes [J/psi(3100)]Physicsquark modelf2(1525)ratio [width]010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyQuark modelFísicascalar meson3. Good healthScattering amplitudef2(1270)tensor mesonHigh Energy Physics - Phenomenologywidth [J/psi(3100)]High Energy Physics::Experiment
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The radiative decay of the Lambda(1405) and its two-pole structure

2007

We evaluate theoretically the radiative decay widths into $\gamma\Lambda$ and $\gamma\Sigma^0$ of the two poles of the $\Lambda(1405)$ found in chiral unitary theories and we find quite different results for each of the two poles. We show that, depending on which reaction is used to measure the $\Lambda(1405)$ radiative decays, one gives more weight to one or the other pole, resulting in quite different shapes in the $\gamma\Lambda(\Sigma^0)$ invariant mass distributions. Our results for the high-energy pole agree with those of the empirical determination of the $\gamma\Lambda$ and $\gamma\Sigma^0$ radiative widths (based on an isobar model fitting of the $K^-p$ atom data), which are someti…

Nuclear and High Energy PhysicsParticle physicsRadiative decayStructure (category theory)radiative decay [Lambda(1405)]chiral [perturbation theory]Lambda(Sigma0 photon) [mass spectrum]Measure (mathematics)Lambda(1405) --> Lambda photonK- p --> Lambda pi0 photonK- p --> Sigma0 pi0 photonAtompi- p --> Lambda K0 photonpi- p --> Sigma0 K0 photonRadiative transferddc:530Invariant massnumerical calculationsPhysicsLambda(1405) --> Sigma0 photonSigma0inelastic scattering [K- p]Físicapole [approximation]hadroproduction [Lambda(1405)]High Energy Physics - Phenomenology(Lambda photon) [mass spectrum]Isobarinelastic scattering [pi- p]hadroproduction [hyperon]width [Lambda(1405)]
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s-wave pion-nucleus optical potential

2007

We calculate the s-wave part of the pion-nucleus optical potential using a unitarized chiral approach that has been previously used to simultaneously describe pionic hydrogen and deuterium data as well as low energy pi N scattering in the vacuum. This energy dependent model allows for additional isoscalar parts in the potential from multiple rescattering. We consider Pauli blocking and pion polarization in an asymmetric nuclear matter environment. Also, higher order corrections of the pi N amplitude are included. The model can accommodate the repulsion required by phenomenological fits, though the theoretical uncertainties are bigger than previously thought. At the same time, we also find a…

Nuclear and High Energy PhysicsParticle physicsscattering amplitude [pi nucleon]Nuclear Theorymedia_common.quotation_subjectIsoscalarpartial waveNuclear TheoryFOS: Physical sciencesAsymmetryrenormalizationNuclear physicsNuclear Theory (nucl-th)symbols.namesakePionPauli exclusion principlemesic atom [deuterium]unitarityddc:530higher-order [Feynman graph]nuclear reaction [pi nucleus]numerical calculationsNuclear Experimentmedia_commonPhysicschiral [symmetry]UnitarityIsovectorN(1440)FísicaNuclear mattermesic atom [hydrogen]propagator [pi]Scattering amplitudenuclear mattersymbolsoptical [potential]correction [vertex function]
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Radioactivity control strategy for the JUNO detector

2021

JUNO is a massive liquid scintillator detector with a primary scientific goal of determining the neutrino mass ordering by studying the oscillated anti-neutrino flux coming from two nuclear power plants at 53 km distance. The expected signal anti-neutrino interaction rate is only 60 counts per day, therefore a careful control of the background sources due to radioactivity is critical. In particular, natural radioactivity present in all materials and in the environment represents a serious issue that could impair the sensitivity of the experiment if appropriate countermeasures were not foreseen. In this paper we discuss the background reduction strategies undertaken by the JUNO collaboration…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsNuclear engineeringMonte Carlo methodControl (management)measurement methodsFOS: Physical sciencesQC770-798Scintillator7. Clean energy01 natural sciencesNOPE2_2Nuclear and particle physics. Atomic energy. Radioactivity0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530Sensitivity (control systems)010306 general physicsPhysicsJUNOliquid [scintillation counter]010308 nuclear & particles physicsbusiness.industryDetectorSettore FIS/01 - Fisica Sperimentaleradioactivity [background]suppression [background]Instrumentation and Detectors (physics.ins-det)Monte Carlo [numerical calculations]Nuclear powerthreshold [energy]sensitivityNeutrino Detectors and Telescopes (experiments)GEANTNeutrinobusinessEnergy (signal processing)
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Efficiency and timing performance of the MuPix7 high-voltage monolithic active pixel sensor

2018

The MuPix7 is a prototype high voltage monolithic active pixel sensor with 103 times 80 um2 pixels thinned to 64 um and incorporating the complete read-out circuitry including a 1.25 Gbit/s differential data link. Using data taken at the DESY electron test beam, we demonstrate an efficiency of 99.3% and a time resolution of 14 ns. The efficiency and time resolution are studied with sub-pixel resolution and reproduced in simulations.

Nuclear and High Energy Physicsirradiation [electron]Physics - Instrumentation and DetectorsFOS: Physical sciencesElectron01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesddc:530DESY Lab010306 general physicsnumerical calculationsInstrumentationtime resolutionPhysicspixel [semiconductor detector]CMOS sensorPixel010308 nuclear & particles physicsbusiness.industryResolution (electron density)High voltageDESYTime resolutionInstrumentation and Detectors (physics.ins-det)Test beamefficiencyOptoelectronicsbusinessperformance
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General Flavor Blind MSSM and CP Violation

2001

We study the implications on flavor changing neutral current and CP violating processes in the context of supersymmetric theories without a new flavor structure (flavor blind supersymmetry). The low energy parameters are determined by the running of the soft breaking terms from the grand unified scale with SUSY phases consistent with the EDM constraints. We find that the CP asymmetry in b --> s gamma can reach large values potentially measurable at B factories, especially in the low BR(b --> s gamma) region. We perform a fit of the unitarity triangle including all the relevant observables. In this case, no sizeable deviations from the SM expectations are found. Finally we analyze the …

Particle physicsFOS: Physical sciences030204 cardiovascular system & hematology01 natural sciencesviolation [CP]bottombranching ratio [quark]03 medical and health sciencesradiative decay [quark]0302 clinical medicineHigh Energy Physics - Phenomenology (hep-ph)interpretation of experiments [numerical calculations]magnetic moment [muon]mass spectrum [sparticle]unitarityddc:530electric moment [electron]0101 mathematicsFlavorPhysicstables010102 general mathematicsHigh Energy Physics::Phenomenologybibliographymass [Higgs particle]3. Good healthHigh Energy Physics - Phenomenologygrand unified theoryCP violationflavor changing [neutral current]High Energy Physics::Experimentbeauty --> strangeness photonsupersymmetry
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Effective Majorana mass matrix from tau and pseudoscalar meson lepton number violating decays

2018

An observation of any lepton number violating process will undoubtedly point towards the existence of new physics and indirectly to the clear Majorana nature of the exchanged fermion. In this work, we explore the potential of a minimal extension of the Standard Model via heavy sterile fermions with masses in the $[ 0.1 - 10]$ GeV range concerning an extensive array of "neutrinoless" meson and tau decay processes. We assume that the Majorana neutrinos are produced on-shell, and focus on three-body decays. We conduct an update on the bounds on the active-sterile mixing elements, $|U_{\ell_\alpha 4} U_{\ell_\beta 4}|$, taking into account the most recent experimental bounds (and constraints) a…

Particle physicsNuclear and High Energy PhysicsMesonPhysics beyond the Standard ModelFOS: Physical sciences7. Clean energy01 natural sciencesPseudoscalar mesonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)double-beta decay: (0neutrino)0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutrino Physics010306 general physicsnumerical calculationslepton number: violationPhysicsneutrino: heavy: decay010308 nuclear & particles physicsnew physicsHigh Energy Physics::Phenomenologyneutrino: Majorana: massFermionneutrino: sterileMass matrixsensitivityLepton numberMAJORANAHigh Energy Physics - Phenomenologypseudoscalar meson: decay[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Beyond Standard Modellcsh:QC770-798neutrino: Majorana[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimenttau: decayNeutrinoneutrino: mixing
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