Search results for "Magnetic dipole transition"

showing 6 items of 6 documents

<title>Influence of radiation defects on exciton-magnon interactions in nickel oxide</title>

2005

Influence of radiation defects on the optical absorption spectrum of nickel oxide (NiO) was studied at 6 K in the near-IR energy range of 7750-8300 cm-1 corresponding to the magnetic-dipole transition 3A 2g(F )->3T 2g(F ) at nickel sites. NiO single crystals grown by the method of chemical transport reactions on the MgO(100) substrates were irradiated by the neutron fluences up to 5x1018 cm-2. Two sharp lines were observed at the low-energy side of the band: the peak at 7805 cm-1 is assigned to the pure exciton transition, whereas the peak at 7845 cm-1, to the exciton-magnon excitation that occurs at the Brillouin zone-center (BZC). An increase of the defect concentration at higher fluences…

Absorption spectroscopyCondensed matter physicsMagnetic dipole transitionNickel oxideMagnonExcitonchemistry.chemical_elementCondensed Matter::Materials ScienceNickelNuclear magnetic resonancechemistryCondensed Matter::Strongly Correlated ElectronsIrradiationAbsorption (electromagnetic radiation)SPIE Proceedings
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Measuring the magnetic dipole transition of single nanorods by spectroscopy and Fourier microscopy

2020

International audience; Rare-earth doped nanocrystals possess optical transitions with significant either electric or magnetic dipole characters. They are of considerable interest for understanding and engineering light-matter interactions at the nanoscale with numerous applications in nanophotonics. Here, we study the 5 D 0 → 7 F 1 transition dipole vector in individual NaYF 4 : Eu 3+ nanorod crystals by Fourier and confocal micro-scopies. A single-crystal host matrix leads to narrow emission lines at room temperature that permit separation of the Stark sublevels resulting from the crystal-field splitting. We observe a fully magnetic transition and low variability of the transition dipole …

PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsMagnetic dipole transitionNanophotonicsGeneral Physics and AstronomyPhysics::OpticsFOS: Physical sciences02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesMolecular physicsDipoleCrystal field theory0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)[PHYS.COND.CM-MS]Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]NanorodEmission spectrum010306 general physics0210 nano-technologySpectroscopyMagnetic dipole
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Hyperfine-structure measurements on trapped Pb II.

1992

The 6${\mathit{P}}_{3/2}$-6${\mathit{P}}_{1/2}$ magnetic dipole resonance transition in ${\mathrm{Pb}}^{+}$ has been observed by cw laser excitation of an ion cloud stored in a Paul trap and subsequent detection of the fluorescence radiation. From the hyperfine-structure splitting of the spectrum we determine the A factor for the ground state, A(${\mathit{P}}_{1/2}$)=12.967(13) GHz, and the excited state, A(${\mathit{P}}_{3/2}$)=0.580(3) GHz. From a contamination of $^{208}\mathrm{Pb}$ in our sample we derived the $^{207}\mathrm{Pb}^{+}$${\mathrm{\ensuremath{-}}}^{208}$${\mathrm{Pb}}^{+}$ isotope shift [\ensuremath{\Delta}\ensuremath{\nu}=311(14) MHz]. A small electric quadrupole admixture …

PhysicsCondensed matter physicsMagnetic dipole transitionExcited stateQuadrupoleResonanceAtomic physicsGround stateHyperfine structureAtomic and Molecular Physics and OpticsExcitationIonPhysical review. A, Atomic, molecular, and optical physics
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The generalized Gerasimov–Drell–Hearn sum rule for deuteron electrodisintegration

2004

The generalized Gerasimov-Drell-Hearn sum rule $I^{GDH}_{\gamma^*d}(Q^2)$ for deuteron electrodisintegration $d(e,e')np$ as function of the squared four-momentum transfer $Q^2$ is evaluated by explicit integration. The calculation is based on a conventional nonrelativistic framework using a realistic $NN$-potential and including contributions from meson exchange currents, isobar configurations and leading order relativistic terms. Good convergence is achieved. The prominent feature is a deep negative minimum, $I_{\gamma^* d}^{GDH}=-9.5$ mb, at low $Q^2\approx 0.2$ fm$^{-2}$ which is almost exclusively driven by the nucleon isovector anomalous magnetic moment contribution to the magnetic dip…

PhysicsNuclear and High Energy PhysicsNuclear TheoryAnomalous magnetic dipole momentMesonIsovectorMagnetic dipole transitionMomentum transferFOS: Physical sciencesNuclear Theory (nucl-th)Nuclear physicsIsobarSum rule in quantum mechanicsNucleonPhysics Letters B
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Leptonic universality breaking in Upsilon decays as a probe of new physics

2003

In this work we examine the possible existence of new physics beyond the standard model which could modify the branching fractions of the leptonic (mainly tauonic) decays of bottomonium vector resonances below the $B\bar{B}$ threshold. The decay width is factorized as the product of two pieces: a) the probability of an intermediate pseudoscalar color-singlet $b\bar{b}$ state (coupling to the dominant Fock state of the Upsilon via a magnetic dipole transition) and a soft (undetected) photon; b) the annihilation width of the $b\bar{b}$ pair into two leptons, mediated by a non-standard CP-odd Higgs boson of mass about 10 GeV, introducing a quadratic dependence on the lepton mass in the partial…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonAnnihilationMagnetic dipole transitionPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesAstronomy and AstrophysicsAtomic and Molecular Physics and OpticsPseudoscalarHigh Energy Physics - PhenomenologyFock stateHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentLepton
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Fast-timing study of the l-forbidden 1/2+ -> 3/2+ M1 transition in 129Sn

2016

The levels in 129Sn populated from the β− decay of 129In isomers were investigated at the ISOLDE facility of CERN using the newly commissioned ISOLDE Decay Station (IDS). The lowest 1/2+ state and the 3/2+ ground state in 129Sn are expected to have configurations dominated by the neutron s1/2 (l = 0) and d3/2 (l = 2) single-particle states, respectively. Consequently, these states should be connected by a somewhat slow l-forbidden M1 transition. Using fast-timing spectroscopy we have measured the half-life of the 1/2+ 315.3-keV state, T1/2 = 19(10) ps, which corresponds to a moderately fast M1 transition. Shell-model calculations using the CD-Bonn effective interaction, with standard effect…

fast-timing spectroscopyneutron-rich nucleimagnetic dipole transitionstina
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