Search results for "capture"

showing 10 items of 463 documents

Muon-capture strength functions in intermediate nuclei of 0νββ decays

2019

Capture rates of ordinary muon capture (OMC) to the intermediate nuclei of neutrinoless double beta ($0\ensuremath{\nu}\ensuremath{\beta}\ensuremath{\beta}$) decays of current experimental interest are computed. The corresponding OMC (capture-rate) strength functions have been analyzed in terms of multipole decompositions. The computed low-energy OMC-rate distribution to $^{76}\mathrm{As}$ is compared with the available data of Zinatulina et al. [Phys. Rev. C 99, 024327 (2019)]. The present OMC computations are performed using the Morita-Fujii formalism by extending the original formalism beyond the leading order. The participant nuclear wave functions are obtained in extended no-core singl…

PhysicsParticle physics010308 nuclear & particles physics01 natural sciencesMuon captureRenormalizationFormalism (philosophy of mathematics)symbols.namesake0103 physical sciencesQuasiparticlesymbols010306 general physicsWave functionMultipole expansionHamiltonian (quantum mechanics)Physical Review C
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Neutrino mass ordering at DUNE: An extra ν bonus

2019

We study the possibility of extracting the neutrino mass ordering at the future Deep Underground Neutrino Experiment using atmospheric neutrinos, which will be available before the muon neutrino beam starts being perational. The large statistics of the atmospheric muon neutrino and antineutrino samples at the far detector, together with the baselines of thousands of kilometers that these atmospheric (anti)neutrinos travel, provide the ideal ingredients to extract the neutrino mass ordering via matter effects in the neutrino propagation through the Earth. Crucially, muon capture by Argon provides excellent charge-tagging, allowing to disentangle the neutrino and antineutrino signature. This …

PhysicsParticle physicsArgonTime projection chamber010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaDetectorHigh Energy Physics::Phenomenologychemistry.chemical_element01 natural sciences7. Clean energyHigh Energy Physics - ExperimentMuon captureHigh Energy Physics - Phenomenologychemistry13. Climate action0103 physical sciencesDeep Underground Neutrino ExperimentMuon neutrinoHigh Energy Physics::ExperimentNeutrino010306 general physicsBeam (structure)Physical Review D
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A Monochromatic Neutrino Beam to Obtain U(e3) and the CP Phase

2007

The goal for future neutrino facilities is the determination of the [Ue3] mixing and CP violation in neutrino oscillations. This will require precision experiments with a very intense neutrino source. The future experiments such as T2K, NOVA and Double CHOOZ will measure the [Ue3] mixing. In order to explore CP violation, we present a novel method to create a monochromatic neutrino beam based on the recent discovery of nuclei that decay fast through electron capture in a superallowed Gamow-Teller transition. The boost of such radioactive ions will generate an intense monochromatic directional neutrino beam when decaying at high energy in a storage ring with long straight sections. We show t…

PhysicsParticle physicsElectron capturePhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFísicaCHOOZSolar neutrino problemNuclear physicsCP violationMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationAIP Conference Proceedings
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Nuclear responses for double beta decay and muon capture

2019

The existence of the neutrinoless double beta (0νββ) decay is one of the most intriguing open questions in the neutrino physics field. Despite many large-scale experiments have aimed to measure the reaction for decades, it has not yet been observed. Therefore, accurate theoretical calculations on 0νββ are crucial. To describe the double beta decay processes reliably one needs a possibility to test the involved virtual transitions against experimental data. In this work we manifest how to utilise the charge-exchange and ordinary muon capture (OMC) data in the study of 0νββ decay.The existence of the neutrinoless double beta (0νββ) decay is one of the most intriguing open questions in the neu…

PhysicsParticle physicsField (physics)Double beta decayMeasure (physics)neutriinotBeta (velocity)High Energy Physics::ExperimentNeutrinohiukkasfysiikkaydinfysiikkaMuon capture
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Physics potential of beta/EC beams in regard to CP violation in neutrino oscillations

2007

The goal for future neutrino facilities is the determination of the [Ue3] mixing and CP violation in neutrino oscillations. This will require precision experiments with a very intense neutrino source. With this objective the creation of neutrino beams from the radioactive decay of boosted ions by the SPS of CERN from either beta or electron capture transitions has been propossed. We discuss the capabilities of such facilities as a function of the energy of the boost and the baseline for the detector. We conclude that the SPS upgrade to 1000 GeV is crucial to have a better sensitivity to CP violation if it is accompanied by a longer baseline. We compare the physics potential for two differen…

PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsElectron captureHigh Energy Physics::PhenomenologyFísicaNuclear physicsUpgradeBeta (plasma physics)Physics::Accelerator PhysicsCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationRadioactive decay
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Energy dependence of CP-violation reach for monochromatic neutrino beam

2008

The ultimate goal for future neutrino facilities is the determination of CP violation in neutrino oscillations. Besides $| U(e3) | \ne 0$, this will require precision experiments with a very intense neutrino source and energy control. With this objective in mind, the creation of monochromatic neutrino beams from the electron capture decay of boosted ions by the SPS of CERN has been proposed. We discuss the capabilities of such a facility as a function of the energy of the boost and the baseline for the detector. We compare the physics potential for two different configurations: I) $\gamma=90$ and $\gamma=195$ (maximum achievable at present SPS) to Frejus; II) $\gamma=195$ and $\gamma=440$ (…

PhysicsParticle physicsNuclear and High Energy PhysicsLarge Hadron ColliderElectron capturePhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFísicaElementary particleMassless particleNuclear physicsHigh Energy Physics - PhenomenologyUpgradeCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationNuclear ExperimentPhysics Letters B
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Equivalence between local Fermi gas and shell models in inclusive muon capture from nuclei

2005

Motivated by recent studies of inclusive neutrino nucleus processes and muon capture within a correlated local Fermi gas model (LFG), we discuss the relevance of nuclear finite size effects in these reactions at low energy, in particular for muon capture. To disentangle these effects from others coming from the reaction dynamics we employ here a simple uncorrelated shell model that embodies the typical finite size content of the problem. The integrated decay widths of muon atoms calculated with this shell model are then compared for several nuclei with those obtained within the uncorrelated LFG, using in both models exactly the same theoretical ingredients and parameters. We find that the t…

PhysicsParticle physicsNuclear and High Energy PhysicsMuonNuclear Theorynucl-thHadronShell (structure)FOS: Physical sciencesFísicaObservableMuon captureNuclear Theory (nucl-th)Nuclear physicsReaction dynamicsNuclear fusionNeutrinoWave functionFermi gas
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Rare weak decays and nuclear structure

2014

Abstract. Weak interactions cause the atomic nuclei to decay via beta and double beta decays. Double beta decays are extremely rare since they are weak-interaction processes of the second order. Also (single) beta decays can be extremely rare. This can be caused by either a large di ff erence between the spins of the initial and final state (the so-called “forbidden” beta decays) or an extremely small Q value (decay energy) of the decay. All these cases are discussed in this article, and particular emphasis is given to the neutrino- less double electron capture on the double beta side of decays. peerReviewed

PhysicsParticle physicsSpinsta114Q valueElectron capturePhysicsQC1-999Nuclear structureweak decaysNuclear physicsDecay energyatomic nucleiAtomic nucleusnuclear structureweak interactionsBeta (velocity)High Energy Physics::ExperimentNeutrinoEPJ Web of Conferences
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Study of the $^{15}$O(2p, γ )$^{17}$Ne cross section by Coulomb dissociation of $^{17}$Ne for the rp process of nucleosynthesis

2014

Acta physica Polonica / B 45(2), 229 - 234 (2014). doi:10.5506/APhysPolB.45.229

PhysicsRadiative captureNuclear structureGeneral Physics and AstronomySigma25.40.Lw 25.70.De 26.30.Ca 27.20.+nrp-process[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530Dissociation (chemistry)Nuclear physicsNucleosynthesisTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYCoulombddc:530Atomic physicsExcitationComputingMilieux_MISCELLANEOUS
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SU-FF-T-180: Dosimetric Characteristics of Tm-170 as a Radionuclide for Its Possible Use in Brachytherapy

2006

In clinical brachytherapy several types of photon sources are used, mainly Cs‐137, Ir‐192, I‐125, and Pd‐103. The Tm‐170 is a promising radionuclide for use in brachytherapy because of the low mean‐energy (46.75 keV or 66.39 keV if the lines below 10 keV are removed) and the possible high specific activity (2.21×1014 Bq/g for a half life of 128.6 days). Tm‐170 is produced in a nuclear reactor by neutron absorption of the natural Tm‐169 and decays mainly via β‐emission. The maximum energies of the β‐rays are 0.290 and 0.323 MeV. These β particles are thus absorbed in the source core and in the encapsulation cover producing bremsstrahlung that contributes significantly to the dose. These fact…

PhysicsRadionuclidePhotonPoint sourcebusiness.industrymedicine.medical_treatmentMonte Carlo methodBrachytherapyBremsstrahlungGeneral MedicineComputational physicsNeutron capturemedicineDosimetryNuclear medicinebusinessMedical Physics
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