Search results for "Acting"

showing 10 items of 338 documents

2019

Abstract We perform calculations of structure functions for elastic and inelastic spin-dependent scattering of weakly interacting massive particles (WIMPs) off 125Te, 129Xe, and 131Xe. The nuclear structure calculations are performed in the microscopic interacting boson-fermion model (IBFM-2). In our calculations we employ one-body and leading long-range two-body WIMP-nucleus currents derived from chiral effective field theory. We demonstrate that the relevant matrix elements can be reliably computed in the IBFM-2, which will allow investigation of heavy deformed nuclei previously inaccessible to theoretical calculations.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsScatteringNuclear structureFermion01 natural sciencesWIMPWeakly interacting massive particles0103 physical sciencesEffective field theory010306 general physicsBosonSpin-½Nuclear Physics A
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Cold positrons from decaying dark matter

2012

Many models of dark matter contain more than one new particle beyond those in the Standard Model. Often heavier particles decay into the lightest dark matter particle as the Universe evolves. Here we explore the possibilities that arise if one of the products in a (Heavy Particle) $\rightarrow$ (Dark Matter) decay is a positron, and the lifetime is shorter than the age of the Universe. The positrons cool down by scattering off the cosmic microwave background and eventually annihilate when they fall into Galactic potential wells. The resulting 511 keV flux not only places constraints on this class of models but might even be consistent with that observed by the INTEGRAL satellite.

PhysicsNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Astrophysics::High Energy Astrophysical PhenomenaHot dark matterDark matterScalar field dark matterFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Weakly interacting massive particlesMixed dark matterWarm dark matterLight dark matterDark fluidAstrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review D
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Likelihood approach to the first dark matter results from XENON100

2011

Many experiments that aim at the direct detection of Dark Matter are able to distinguish a dominant background from the expected feeble signals, based on some measured discrimination parameter. We develop a statistical model for such experiments using the Profile Likelihood ratio as a test statistic in a frequentist approach. We take data from calibrations as control measurements for signal and background, and the method allows the inclusion of data from Monte Carlo simulations. Systematic detector uncertainties, such as uncertainties in the energy scale, as well as astrophysical uncertainties, are included in the model. The statistical model can be used to either set an exclusion limit or …

PhysicsNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Scale (ratio)010308 nuclear & particles physicsMonte Carlo methodDark matterFOS: Physical sciencesStatistical model01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Frequentist inferenceWeakly interacting massive particles0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Test statisticLimit (mathematics)Statistical physics010306 general physicsAstrophysics - Cosmology and Nongalactic AstrophysicsPhysical Review D
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Neutrinoless double-electron capture

2014

Direct determination of the neutrino mass is at the present time one of the most important aims of experimental and theoretical research in nuclear and particle physics. A possible way of detection is through neutrinoless double-electron capture, $0\ensuremath{\nu}\mathrm{ECEC}$. This process can only occur when the energy of the initial state matches precisely that of the final state. We present here a calculation of prefactors (PFs) and nuclear matrix elements (NMEs) within the framework of the microscopic interacting boson model (IBM-2) for $^{124}\mathrm{Xe}$, $^{152}\mathrm{Gd}$, $^{156}\mathrm{Dy}$, $^{164}\mathrm{Er}$, and $^{180}\mathrm{W}$. From the PF and NME we calculate the expe…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theoryta114010308 nuclear & particles physicsElectron captureneutrinoless double-electron captureOrder (ring theory)FOS: Physical sciencesTheoretical researchState (functional analysis)01 natural sciencesNuclear Theory (nucl-th)0103 physical sciencesInteracting boson modelNeutrino010306 general physicsNuclear theoryEnergy (signal processing)
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Collective and broken pair states of65,67Ga

1999

Excited states of 65Ga and 67Ga nuclei were populated through the 12C(58Ni,αp) and 12C(58Ni,3p) reactions, respectively, and investigated by in-beam γ-ray spectroscopic methods. The NORDBALL array equipped with a charged particle ball and 11 neutron detectors was used to detect the evaporated particles and γ rays. The level schemes of 65,67Ga were constructed on the basis of γγ-coincidence relations up to 8.6 and 10 MeV excitation energy, and Iπ=27/2 and 33/2+ spin and parity, respectively. The structure of 65,67Ga nuclei was described in the interacting boson-fermion plus broken pair model, including quasiproton, quasiproton-two-quasineutron, and three-quasiproton fermion configurations in…

PhysicsNuclear and High Energy PhysicsPhononExcited stateNuclear structureQuasiparticleNeutronFermionAtomic physicsInteracting boson modelCharged particlePhysical Review C
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Experimental investigation of the 02+ band in Sm154 as a β-vibrational band

2014

Abstract A study of Sm 154 through γ -ray and internal conversion electron coincidence measurements was performed using the Silicon And GErmanium spectrometer (SAGE). An upper limit for the ρ 2 ( E 0 ; 2 2 + → 2 1 + ) and measurement of the ρ 2 ( E 0 ; 4 2 + → 4 1 + ) monopole transitions strengths were determined. The extracted transition strength for each is significantly lower than that predicted by either the Bohr and Mottelson β -vibration description or the interacting boson model. Hence, the long standing interpretation of these states as a collective band built on the 0 2 + state, which is conventionally assigned as a Bohr and Mottelson β vibration is questionable.

PhysicsNuclear and High Energy PhysicsSilicon010308 nuclear & particles physicsGamma raychemistry.chemical_elementGermaniumElectron01 natural sciencesBohr modelsymbols.namesakeInternal conversionchemistry0103 physical sciencessymbolsInteracting boson modelAtomic physics010306 general physicsSpectroscopyPhysics Letters B
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Collective features of Cr and Fe isotopes

2014

The question of the sudden increase of collectivity in neutron-rich nuclei when approaching $N=40$ has recently interested both experimentalists and theorists. In this paper we study the development of collectivity along the chromium and iron isotopic chains. The calculations are performed within two different perspectives, namely, the proton-neutron interacting boson model (IBM-2) and interacting shell model (ISM) and compared with the available experimental data. The onset of collectivity is studied through nuclear quantities and observables that suggest differences in the nuclear structure of Cr and Fe isotopical chains. Furthermore, a prediction for the shape transition from a spherical…

PhysicsNuclear and High Energy Physicsta114IsotopeNuclear TheorySHELL modelNuclear structureObservableNuclear physicsmedicine.anatomical_structureCritical point (thermodynamics)medicineInteracting boson modelNuclear ExperimentNucleus
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Evidence for oblate structure inPb186

2005

In-beam $\ensuremath{\gamma}\ensuremath{\gamma}$ coincidence data have been collected for $^{186}\mathrm{Pb}$ by combining the JUROGAM Ge-detector array and the GREAT spectrometer with the RITU gas-filled recoil separator for recoil-decay tagging measurements. In addition to the known prolate yrast band in $^{186}\mathrm{Pb}$, these data have enabled a new low-lying side band to be identified. Based on the analysis of its decay pattern and comparison with Interacting Boson Model (IBM) calculations, the new band is associated with an oblate shape.

PhysicsNuclear physicsNuclear and High Energy PhysicsSpectrometerYrastStructure (category theory)Nuclear structureGamma spectroscopyInteracting boson modelRadioactive decayCoincidencePhysical Review C
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γ-ray spectroscopy approaching the limits of existence of atomic nuclei: A study of the excited states ofPt168andPt169

2009

Excited states in the $N=90$ and $N=91$ Pt nuclei have been investigated using the JUROGAM and GREAT spectrometers in conjunction with the RITU gas-filled separator. These nuclei were populated via the reactions $^{92}\mathrm{Mo}(^{78}\mathrm{Kr},2n)$ and $^{94}\mathrm{Mo}(^{78}\mathrm{Kr},3n)$ at 335 and 348 MeV, respectively. The recoil-decay tagging technique has been used to correlate prompt $\ensuremath{\gamma}$ radiation with the characteristic $\ensuremath{\alpha}$ decays of $^{168}\mathrm{Pt}$ and $^{169}\mathrm{Pt}$. A $\ensuremath{\gamma}\text{\ensuremath{-}}\ensuremath{\gamma}$ analysis has allowed a level scheme for $^{168}\mathrm{Pt}$ to be reported for the first time and the l…

PhysicsNuclear reactionNuclear and High Energy PhysicsNeutron emissionYrastExcited stateAtomic nucleusGamma spectroscopyAlpha decayAtomic physicsInteracting boson modelPhysical Review C
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X-Ray Lines from Dark Matter Annihilation at the keV Scale.

2018

In 2014, several groups reported hints for a yet unidentified line in astrophysical x-ray signals from galaxies and galaxy clusters at an energy of 3.5 keV. While it is not unlikely that this line is simply a reflection of imperfectly modeled atomic transitions, it has renewed the community’s interest in models of keV-scale dark matter, whose decay would lead to such a line. The alternative possibility of dark matter annihilation into monochromatic photons is far less explored, a lapse that we strive to amend in this Letter. More precisely, we introduce a novel model of fermionic dark matter χ with O(keV) mass, annihilating to a scalar state ϕ which in turn decays to photons, for instance v…

PhysicsParticle physics010308 nuclear & particles physicsHot dark matterDark matterScalar field dark matterGeneral Physics and Astronomy01 natural sciencesBaryonic dark matterWeakly interacting massive particles0103 physical sciencesWarm dark matter010303 astronomy & astrophysicsLight dark matterDark fluidPhysical review letters
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