Search results for "dipole"

showing 10 items of 982 documents

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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Photon Scattering with the Lorentz Integral Transform Method

2011

The application of the Lorentz integral transform (LIT) method to photon scattering off nuclei is presented in general. As an example, elastic photon scattering off the deuteron in the unretarded dipole approximation is considered using the LIT method. The inversion of the integral transform is discussed in detail paying particular attention to the high-energy contributions in the resonance term. The obtained E1-polarizabilities are compared to results from the literature. The corresponding theoretical cross section is confronted with experimental results confirming, as already known from previous studies, that the E1-contribution is the most important one at lower energies.

PhysicsNuclear and High Energy PhysicsPhotonNuclear TheoryLorentz transformationFOS: Physical sciencesElementary particleDiscrete dipole approximationIntegral transformMassless particleNuclear Theory (nucl-th)symbols.namesakeDipolePolarizabilityQuantum mechanicsQuantum electrodynamicssymbols
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Few-neutron removal from238U at relativistic energies

1995

As part of a comprehensive study of uranium fragmentation at relativistic energies at the GSI projectile fragment separator, FRS, inclusive neutron-removal cross sections have been measured for severalxn channels at projectile energies of 600 and 950A MeV using targets of Al, Cu and Pb. The variation of the experimental cross sections with target nuclear charge is used to disentangle nuclear and electromagnetic contributions. The electromagnetic cross sections agree surprisingly well with a simple harmonic oscillator calculation of giant dipole resonances based on measured photonuclear cross sections and do not require an extra enhancement of the two-phonon giant dipole excitation as conclu…

PhysicsNuclear and High Energy PhysicsProjectileNuclear Theorychemistry.chemical_elementSimple harmonic motionUraniumEffective nuclear chargeNuclear physicsDipoleFragmentation (mass spectrometry)chemistryNuclear fusionNeutronAtomic physicsNuclear ExperimentNuclear PhysicsZeitschrift für Physik A Hadrons and Nuclei
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Nuclear moments of neon isotopes in the range fromNe17at the proton drip line to neutron-richNe25

2005

Nuclear moments of odd-A neon isotopes in the range 17 ≤ A ≤ 25 have been determined from optical hyperfine structures measured by collinear fast-beam laser spectroscopy. The magnetic dipole moments of 17 Ne, 23 Ne and 25 Ne, as well as the electric quadrupole moment of 23 Ne are either reported for the first time or improved considerably. The measurements also decide for a 1/2 + ground state of 25 Ne. The behavior of the magnetic moments of the proton drip-line nucleus 17 Ne and its mirror partner 17 N suggests isospin symmetry. Thus, no clear indication of an anomalous nuclear structure is found for 17 Ne. The magnetic moments of the investigated nuclei are discussed in a shell-model appr…

PhysicsNuclear and High Energy PhysicsProtonMagnetic momentNuclear TheoryIsotopes of neonQuadrupoleNeutronPhysics::Atomic PhysicsMirror nucleiAtomic physicsNuclear ExperimentHyperfine structureMagnetic dipolePhysical Review C
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Coexistence of triaxial and prolate shapes in 171Ir

1999

Abstract Excited states in 171Ir have been observed for the first time. Gamma-rays were assigned to the nucleus by the recoil-decay tagging method. The ground-state band has a structure consistent with an h 11 2 proton coupled to a core of large triaxial deformation. At high spins, a bandcrossing occurs which is interpreted as a change in shape to a prolate deformation. Band-mixing calculations are performed for 171–175Ir. These show that shape-coexistence between triaxial and prolate states in these nuclei follows the same systematics found in their Pt and Os neighbours. The systematics are also compared with deformations calculated for 171–179Ir using the code “Ultimate Cranker”. Dipole b…

PhysicsNuclear and High Energy PhysicsProtonSpinsNuclear TheoryDeformation (meteorology)RotationCore (optical fiber)Dipolemedicine.anatomical_structureExcited statemedicineAtomic physicsNucleusNuclear Physics A
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Spectroscopy ofAt201including the observation of a shears band and the29/2+isomeric state

2015

The excited states of $^{201}\mathrm{At}$ were studied and an isomeric $29/{2}^{+}$ state $[{T}_{\textonehalf{}}=3.39(9)\phantom{\rule{0.28em}{0ex}}\ensuremath{\mu}\mathrm{s}]$ was identified by using a fusion-evaporation reaction, a gas-filled recoil separator, and recoil gating techniques. The $29/{2}^{+}$ state is suggested to originate from the $\ensuremath{\pi}({h}_{9/2})\ensuremath{\bigotimes}|^{200}\mathrm{Po};{11}^{\ensuremath{-}}\ensuremath{\rangle}$ configuration, and it decays through the 269- and 339-keV $E2$- and $E3$-type transitions, respectively. Moreover, a cascade of magnetic dipole transitions that is suggested to originate from a shears band was observed by using recoil-…

PhysicsNuclear and High Energy PhysicsRecoil010308 nuclear & particles physicsExcited state0103 physical sciencesState (functional analysis)Atomic physics010306 general physicsSpectroscopy01 natural sciencesMagnetic dipoleRecoil separatorPhysical Review C
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The three-spectrometer facility at the Mainz microtron MAMI

1998

Abstract A set-up of three high-resolution magnetic spectrometers, for simplicity named A, B and C, has been built as the central facility for the precise determination of double and triple coincidence cross sections of hadron knock-out and meson production through the scattering of electrons at the Mainz microtron MAMI. The spectrometers A and C with point-to-point optics in the dispersive plane and parallel-to-point optics in the non-dispersive plane have a solid angle of 28 msr and a momentum acceptance of 20 and 25%, respectively. They each consist of a quadrupole, a sextupole and two dipole magnets, reaching maximum momenta of 735 and 550 MeV/c, respectively. The spectrometer B has a s…

PhysicsNuclear and High Energy PhysicsSpectrometerCherenkov detectorSolid angleElectronlaw.inventionNuclear physicsDipoleDipole magnetlawQuadrupoleNuclear ExperimentInstrumentationMicrotronNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Nuclear spins, moments and charge radii of108?111Sn

1987

The hyperfine structure splittings (hfs) and isotope shifts (IS) in the atomic transitions 5s2 5p21S0 → 5s2 5p6s1,3P1 have been measured for the radioactive isotopes108−111Sn and all stable ones. The tin isotopes were prepared as fast atomic beams for collinear laser spectroscopy at the GSI online mass separator following a fusion reaction. Nuclear spins, magnetic dipole, electric quadrupole moments and changes in mean square charge radii have been determined. In109Sn the spinI=5/2 was measured for the nuclear ground state (T1/2=18 min) in contradiction to the literature value. The mean square charge radii show a parabolic behaviour with a maximum at N=66. This is interpreted by collective …

PhysicsNuclear and High Energy PhysicsSpinsIsotopes of tinQuadrupoleNuclear fusionPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentGround stateSpectroscopyHyperfine structureMagnetic dipoleZeitschrift f�r Physik A Atomic Nuclei
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Nuclear spins, moments, and changes of the mean square charge radii of sup.(140-153)Eu

1985

The hyperfine structures and isotope shifts of 14 isotopes of Eu (Z=63) in the mass range 140≦A≦153, partly with isomeric states, have been measured in the atomic transitions at 4,594 A and 4,627 A, using the technique of collinear fast-beam laser spectroscopy at the ISOLDE facility at CERN. The nuclear spins, the magnetic dipole and electric quadrupole moments, and the changes in the mean square charge radii have been evaluated. These nuclear parameters clearly reflect the effects of theN=82 neutron-shell closure in the single-proton hole states with respect to the semi-magic gadolinium (Z=64), and theN=88−90 shape transition.

PhysicsNuclear and High Energy PhysicsSpinsNuclear TheoryEffective nuclear chargeMolecular electronic transitionQuadrupolePhysics::Accelerator PhysicsNuclear fusionNuclear Physics - ExperimentPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentSpectroscopyHyperfine structureMagnetic dipole
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Continuous Stern–Gerlach effect and the magnetic moment of the antiproton

2004

Abstract The measurement of the magnetic moment (or g-factor ) of the antiproton and of the proton is a sensitive test of CPT invariance. We discuss the possibility of applying the continuous Stern–Gerlach effect to detect quantum jumps between the two spin states (spin up and spin down) of the antiproton. The measurement will be performed on a single antiproton stored in a Penning trap. The g -factor of the antiproton is determined by measuring its cyclotron frequency and its spin precession frequency in the magnetic field of the trap. With the double Penning trap method the g -factor of the antiproton can be determined with an accuracy of 1 ppb.

PhysicsNuclear and High Energy PhysicsStern–Gerlach experimentSpin polarizationProton magnetic momentPenning trapElectron magnetic dipole momentSpin magnetic momentNuclear physicsAntiprotonNuclear magnetic momentPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentPhysics::Atomic PhysicsNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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