Search results for "forbidden beta decay"

showing 7 items of 7 documents

Mesonic enhancement of the weak axial charge and its effect on the half-lives and spectral shapes of first-forbidden J+↔J− decays

2018

The effects of the enhancement of the axial-charge matrix element γ5 were studied in medium heavy and heavy nuclei for first-forbidden J+↔J− decay transitions using the nuclear shell model. Noticeable dependence on the enhancement ϵMEC of the axial-charge matrix element, as well as on the value of the axial-vector coupling constant gA was found in the spectral shapes of $^{93}$Y, $^{95}$Sr, and $^{97}$Y. The importance of the spectrum of $^{138}$Cs in the determination of gA is discussed. Half-life analyses in the A≈95 and A≈135 regions were done, and consistent results gA≈0.90, 0.75, and 0.65, corresponding to the three enhancement scenarios ϵMEC=1.4, 1.7, and 2.0, were obtained. Connectio…

Coupling constantPhysicsNuclear and High Energy PhysicsSpectral shape analysista114010308 nuclear & particles physicsSpectrum (functional analysis)forbidden beta decaysNuclear shell modelCharge (physics)01 natural scienceslcsh:QC1-999nuclear medium effectsspectral shapemeson-exchange currents0103 physical sciencesweak interactionsMatrix elementAtomic physicsAnomaly (physics)ydinfysiikka010306 general physicslcsh:PhysicsPhysics Letters B
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Spin-dipole nuclear matrix elements for double beta decays and astro-neutrinos

2014

Spin-dipole (SD) nuclear matrix elements (NMEs) M±(SD2) for unique first forbidden β±2−→0+ ground-state-to-ground-state transitions are studied by using effective microscopic two-nucleon interactions in realistic single-particle model spaces. The observed values of the NMEs Mexp±(SD2) are compared with the values of the single-quasiparticle NMEs Mqp±(SD2) without nucleon spin–isospin (στ) correlation and the QRPA NMEs MQRPA±(SD2) with the στ correlation. The observed SD matrix elements are found to be reduced by the factor k≈0.2 with respect to Mqp±(SD2) and by the factor kNM≈0.5 with respect to MQRPA±(SD2). We then infer that the SD NME is reduced considerably partly by the nucleon στ corr…

PhysicsNuclear and High Energy PhysicsParticle physicsta114Renormalization of the axial-vector weak coupling constantPhysics::Medical PhysicsNuclear Theorycoupling constantdouble beta decayrenormalization of the axial-vector weakDouble beta decayspin-dipole matrix elementNuclear physicsDipoleMatrix (mathematics)Double beta decaySpin-dipole matrix elementBeta (velocity)Neutrinounique forbidden beta decayNuclear ExperimentSpin (physics)NucleonUnique forbidden beta decayPhysics Letters B
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Double β Decay and the Axial Strength

2019

Quenching of the weak axial strength gA is discussed and relations of this quenching to the nuclear matrix elements of double beta decays are highlighted. An analysis of Gamow-Teller transitions in the mass range A = 62 − 142 is presented and its results are compared with those of many previous works. The enhancement of the axial charge is discussed for first-forbidden pseudoscalar β transitions. Higher-forbidden β transitions are introduced and their role in determining the effective value of gA is examined, in particular from the point of view of the β-decay half-lives and the shapes of electron spectra of forbidden non-unique β transitions. peerReviewed

Semileptonic decayHigh Energy Physics::LatticeMaterials Science (miscellaneous)Nuclear TheoryBiophysicsGeneral Physics and Astronomydouble beta decay01 natural sciencesDouble beta decay0103 physical sciencesBeta (velocity)Physical and Theoretical Chemistry010306 general physicsMathematical PhysicsPhysicsQuenchingRange (particle radiation)Gamow-Teller beta decayta114Electron spectradigestive oral and skin physiologyCharge (physics)electron spectral shapeslcsh:QC1-999quenching of weak axial couplingPseudoscalarenhancement of weak axial chargeforbidden beta decayAtomic physicsydinfysiikkalcsh:Physics
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Value of the Axial-Vector Coupling Strength in β and ββ Decays : A Review

2017

In this review the quenching of the weak axial-vector coupling constant, $g_{\rm A}$, is discussed in nuclear $\beta$ and double-$\beta$ decays. On one hand, the nuclear-medium and nuclear many-body effects are separated, and on the other hand the quenching is discussed from the points of view of different many-body methods and different $\beta$-decay and double-$\beta$-decay processes. Both the historical background and the present status are reviewed and contrasted against each other. The theoretical considerations are tied to performed and planned measurements, and possible new measurements are urged, whenever relevant and doable. Relation of the quenching problem to the measurements of …

Semileptonic decayParticle physicsaxial-vector coupling strengthMaterials Science (miscellaneous)Biophysicsforbidden beta decaysGeneral Physics and Astronomy01 natural sciencesbeta spectra0103 physical sciencesPhysical and Theoretical Chemistry010306 general physicsPseudovectorMathematical PhysicsPhysicsQuenchingCoupling constantdouble beta decaysCoupling strength010308 nuclear & particles physicsmuon captureNuclear matterlcsh:QC1-999Muon capturecharge-exchange reactionsGamow-Teller beta decaysValue (mathematics)lcsh:Physicsstrength functions
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Beta-spectrum shapes of forbidden β decays

2018

The neutrinoless [Formula: see text] decay of atomic nuclei continues to attract fervent interest due to its potential to confirm the possible Majorana nature of the neutrino, and thus the nonconservation of the lepton number. At the same time, the direct dark matter experiments are looking for weakly interacting massive particles (WIMPs) through their scattering on nuclei. The neutrino-oscillation experiments on reactor antineutrinos base their analyses on speculations of [Formula: see text]-spectrum shapes of nuclear decays, thus leading to the notorious “reactor antineutrino anomaly.” In all these experimental efforts, one encounters the problem of [Formula: see text]-spectrum shapes of…

direct dark matter searchNuclear and High Energy Physicsaxial-vector coupling strengthSHELL modelforbidden beta decaysdouble beta decay01 natural sciencesNuclear physicsDouble beta decay0103 physical sciencesBeta (velocity)beta spectrum shapes010306 general physicsreactor antineutrino anomalyaxial-charge matrix elementPhysicsta114010308 nuclear & particles physicsSpectrum (functional analysis)Astronomy and AstrophysicsAtomic and Molecular Physics and OpticsMAJORANAAtomic nucleusHigh Energy Physics::ExperimentNeutrinoInternational Journal of Modern Physics A
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Value of the Axial-Vector Coupling Strength in β and ββ Decays : A Review

2017

double beta decaysaxial-vector coupling strengthta114beta spectramuon captureforbidden beta decayscharge-exchange reactionsGamow-Teller beta decaysstrength functionsFrontiers in Physics
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Spin-multipole nuclear matrix elements in the pn quasiparticle random-phase approximation: Implications for β and ββ half-lives

2017

Half-lives for 148 potentially measurable 2nd-, 3rd-, 4th-, 5th-, 6th-, and 7th-forbidden unique beta transitions are predicted. To achieve this, the ratio of the nuclear matrix elements (NMEs), calculated by the proton-neutron quasiparticle random-phase approximation (pnQRPA), MpnQRPA, and a two-quasiparticle (two-qp) model, Mqp, is studied and compared with earlier calculations for the allowed Gamow-Teller (GT) 1+ and first-forbidden spin-dipole (SD) 2− transitions. The present calculations are done using realistic single-particle model spaces and G-matrix based microscopic two-body interactions. In terms of the ratio k = MpnQRPA/Mqp the studied decays fall into two groups: for GROUP 1, w…

forbidden beta decaybeta decaynuclear matrix elementsproton-neutron quasiparticle random-phase approximation
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