Search results for "Expansion"

showing 10 items of 630 documents

Recent developments in the evaluation of Mössbauer line intensities

1985

The angular dependence of the intensities of pure or mixed multipole transitions is formulated in a new fashion, which takes into account arbitrary texture of the Mossbauer absorber ranging from complete orientation (single crystals) over preferred orientation to random powders and an anisotropic absorption fraction of the nuclei. The application of the theory is demonstrated by means of typical examples from the literature.

Nuclear and High Energy PhysicsMaterials sciencebusiness.industryCondensed Matter PhysicsAtomic and Molecular Physics and OpticsOpticsOrientation (geometry)Mössbauer spectroscopyTexture (crystalline)Physical and Theoretical ChemistryAtomic physicsThin filmbusinessMultipole expansionAnisotropyAbsorption (electromagnetic radiation)Line (formation)Hyperfine Interactions
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Analysis of the Intermediate-State Contributions to Neutrinoless Double β− Decays

2016

A comprehensive analysis of the structure of the nuclear matrix elements (NMEs) of neutrinoless double beta-minus (0νβ-β-) decays to the0+ground and first excited states is performed in terms of the contributing multipole states in the intermediate nuclei of0νβ-β-transitions. We concentrate on the transitions mediated by the light (l-NMEs) Majorana neutrinos. As nuclear model we use the proton-neutron quasiparticle random-phase approximation (pnQRPA) with a realistic two-nucleon interaction based on the Bonn one-boson-exchangeGmatrix. In the computations we include the appropriate short-range correlations, nucleon form factors, and higher-order nucleonic weak currents and restore the isospi…

Nuclear and High Energy PhysicsParticle physicsArticle SubjectNuclear Theorydouble beta decaynuclear matrix elements01 natural sciencesneutrinoless double beta decayNuclear physicsMatrix (mathematics)0103 physical sciences010306 general physicsNuclear ExperimentPhysicsta114010308 nuclear & particles physicslcsh:QC1-999MAJORANAExcited stateIsospinQuasiparticleNeutrinoMultipole expansionNucleonlcsh:PhysicsAdvances in High Energy Physics
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Cosmology with a very light Lμ − Lτ gauge boson

2019

In this paper, we explore in detail the cosmological implications of an abelian L − L gauge extension of the Standard Model featuring a light and weakly coupled Z′. Such a scenario is motivated by the longstanding ∼ 4σ discrepancy between the measured and predicted values of the muon’s anomalous magnetic moment, (g − 2) , as well as the tension between late and early time determinations of the Hubble constant. If sufficiently light, the Z′ population will decay to neutrinos, increasing the overall energy density of radiation and altering the expansion history of the early universe. We identify two distinct regions of parameter space in this model in which the Hubble tension can be significa…

Nuclear and High Energy PhysicsParticle physicscosmological modelZ': couplingPopulationNeutrino decoupling01 natural sciences7. Clean energygauge boson: abeliansymbols.namesakeradiation: density0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivityenergy: densityNeutrino Physics010306 general physicseducationPhysicsGauge bosoneducation.field_of_studyMuonHubble constantAnomalous magnetic dipole momentspace-time: expansionmuon: magnetic moment010308 nuclear & particles physicsCoupling (probability)Cosmology of Theories beyond the SMHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Beyond Standard Modelsymbolslcsh:QC770-798Neutrino[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]neutrino: decouplingAstrophysics - Cosmology and Nongalactic AstrophysicsHubble's lawJournal of High Energy Physics
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Compton Scattering by the Proton using a Large-Acceptance Arrangement

2001

Compton scattering by the proton has been measured over a wide range covering photon energies 250 MeV lt or approximately=E/sub gamma / lt or approximately=800 MeV and photon scattering angles 30 degrees lt or approximately= theta /sub gamma //sup lab/ lt or approximately=150 degrees , using the tagged-photon facility at MAMI (Mainz) and the large-acceptance arrangement LARA. The previously existing data base on proton Compton scattering is greatly enlarged by more than 700 new data points. The new data are interpreted in terms of dispersion theory based on the SAID-SM99K parametrization of photo-meson amplitudes. It is found that two-pion exchange in the t-channel is needed for a descripti…

Nuclear and High Energy PhysicsProtonNuclear TheoryFOS: Physical sciencesValue (computer science)01 natural sciencesResonance (particle physics)High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Dispersion relation0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentQCSpin-½Physics010308 nuclear & particles physicsCompton scatteringHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics::ExperimentMultipole expansion
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$W^{+}W^{-}$ production at the LHC: fiducial cross sections and distributions in NNLO QCD

2016

We consider QCD radiative corrections to $W^+W^-$ production at the LHC and present the first fully differential predictions for this process at next-to-next-to-leading order (NNLO) in perturbation theory. Our computation consistently includes the leptonic decays of the $W$ bosons, taking into account spin correlations, off-shell effects and non-resonant contributions. Detailed predictions are presented for the different-flavour channel $pp\to\mu^+e^-\nu_\mu {\bar \nu}_e+X$ at $\sqrt{s}=8$ and $13$ TeV. In particular, we discuss fiducial cross sections and distributions in the presence of standard selection cuts used in experimental $W^+W^-$ and $H\to W^+W^-$ analyses at the LHC. The inclus…

Nuclear and High Energy Physicsleptonic decay010308 nuclear & particles physics530 Physicsoff-shell [effect]High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciences10192 Physics Institute01 natural sciences2 [higher-order]High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CERN LHC Collcorrelation [spin]radiative correction [quantum chromodynamics]0103 physical sciencesddc:530High Energy Physics::Experimentexpansion 1/N3106 Nuclear and High Energy Physics010306 general physicsperturbation theoryJHEP
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Nuclear response functions in homogeneous matter with finite range effective interactions

2005

The question of nuclear response functions in a homogeneous medium is examined. A general method for calculating response functions in the random phase approximation (RPA) with exchange is presented. The method is applicable for finite-range nuclear interactions. Examples are shown in the case of symmetric nuclear matter described by a Gogny interaction. It is found that the convergence of the results with respect to the multipole truncation is quite fast. Various approximation schemes such as the Landau approximation, or the Landau approximation for the exchange terms only, are discussed in comparison with the exact results.

Nuclear and High Energy Physicsresponse functions[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryTruncationNuclear TheoryFOS: Physical sciencesFinite range21.30.Fe 21.60.Jz 21.65.+f 26.60.+c01 natural sciencesNuclear Theory (nucl-th)effective nuclear interactions0103 physical sciencesConvergence (routing)Statistical physics010306 general physicsPhysics010308 nuclear & particles physicsBorn–Huang approximationFísicaNuclear matter3. Good healthHomogeneousnuclear matterrandom phase approximationQuantum electrodynamicsRandom phase approximationMultipole expansion
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Mirror energy differences above the 0f7/2 shell: First γ-ray spectroscopy of the Tz = −2 nucleus 56Zn

2021

5 pags., 4 figs.

Nuclear and High Energy Physicssinkki (metallit)QC1-999Nuclear Theory01 natural sciencesnucleon removalmirror nuclei0103 physical sciencesSubatomic Physicsmedicine010306 general physicsSpectroscopyradioactive ion beamsNuclear ExperimentNucleonsPhysics[PHYS]Physics [physics]isotoopitValence (chemistry)Isovector010308 nuclear & particles physicsYrastPhysicsFísicaSymmetry Breakingmedicine.anatomical_structureisospin symmetryshell-model calculationsExcited stateEnergy DifferenceAtomic physicsMultipole expansionydinfysiikkaNucleusBeam (structure)
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The collective structure of106,108Ru

1984

Levels in106,108Ru have been studied by measuringγγ coincidences andγγ directional correlations of theγ-rays following theβ−-decay of 36 s106Tc and 5 s108Tc. Tc activities were separated chemically from the fission products of thermal neutron induced fission of239Pu by the continuously running system “SISAK 2” and theγ-radiation was measured on-line. An extended level scheme for108Ru, spin assignments,E2/M1 multipole mixing ratios andB(E2) ratios for106Ru and108Ru have been obtained. The collective structure of the two nuclei is discussed in the framework of different nuclear models.

Nuclear physicsPhysicsNuclear and High Energy PhysicsFission productsFissionStructure (category theory)Nuclear fusionSpin (physics)Multipole expansionMixing (physics)Neutron temperatureZeitschrift f�r Physik A Atoms and Nuclei
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Double Polarization Observables in η Electroproduction

2009

Abstract A new measurement of beam-recoil double-polarization observables in η electroproduction at the A1 collaboration at MAMI is presented. The energy region of the S 11 ( 1525 ) resonance was covered at a four-momentum transfer of Q 2 = 0.1 GeV 2 / c 2 . It turned out, that the usual interpretation of the reaction mechanism via S 11 and D 13 resonance fails to explain the relative phase between the corresponding multipole amplitudes tested by this experiment, while the new data are still in good agreement with previous measurements.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsAmplitudeMeson productionPolarization observablesObservableRelative phaseNuclear ExperimentMultipole expansionResonance (particle physics)Interpretation (model theory)Nuclear Physics A
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Theory of double beta decay

2005

Basic features of the two-neutrino double beta ( 2 ν β β ) decay and neutrinoless double beta ( 0 ν β β ) decay are discussed. A short review of the most important nuclear models, used to describe the ββ decay, is given. A deeper survey of the nuclear matrix elements, related to the above-mentioned decay modes, is performed using the proton-neutron quasiparticle random-phase approximation (pnQRPA). In particular, the extraction of a proper value of the proton-neutron particle-particle interaction parameter in this theory is addressed. The relevance of different multipoles in the multipole decomposition of the 0 ν β β matrix element is also discussed in the pnQRPA framework.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsDouble beta decayQuasiparticleMatrix elementBeta (velocity)Flory–Huggins solution theoryNuclear ExperimentMultipole expansionNuclear Physics A
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