Search results for "Spins"

showing 10 items of 257 documents

Synchronised gravitational atoms from mergers of bosonic stars

2020

If ultralight bosonic fields exist in Nature as dark matter, superradiance spins down rotating black holes (BHs), dynamically endowing them with equilibrium bosonic clouds, here dubbed synchronised gravitational atoms (SGAs). The self-gravity of these same fields, on the other hand, can lump them into (scalar or vector) horizonless solitons known as bosonic stars (BSs). We show that the dynamics of BSs yields a new channel forming SGAs. We study BS binaries that merge to form spinning BHs. After horizon formation, the BH spins up by accreting the bosonic field, but a remnant lingers around the horizon. If just enough angular momentum is present, the BH spin up stalls precisely as the remnan…

PhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)High Energy Physics - TheoryAngular momentumSpins010308 nuclear & particles physicsHorizonAstrophysics::High Energy Astrophysical PhenomenaDark matterComputer Science::Neural and Evolutionary ComputationFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Quantum number01 natural sciences7. Clean energyAccretion (astrophysics)General Relativity and Quantum CosmologyGravitationHigh Energy Physics - Theory (hep-th)Quantum mechanics0103 physical sciencesBosonic field010306 general physicsAstrophysics - High Energy Astrophysical Phenomena
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Dipole and quadrupole moments of Cu73–78 as a test of the robustness of the Z=28 shell closure near Ni78

2017

Nuclear spins and precise values of the magnetic dipole and electric quadrupole moments of the ground-states of neutron-rich $^{76-78}$Cu isotopes were measured using the Collinear Resonance Ionization Spectroscopy (CRIS) experiment at ISOLDE, CERN. The nuclear moments of the less exotic $^{73,75}$Cu isotopes were re-measured with similar precision, yielding values that are consistent with earlier measurements. The moments of the odd-odd isotopes, and $^{78}_{29}$Cu ($N=49$) in particular, are used to investigate excitations of the assumed doubly-magic $^{78}$Ni core through comparisons with large-scale shell-model calculations. Despite the narrowing of the $Z=28$ shell gap between $N\sim45…

PhysicsLarge Hadron ColliderSpinsIsotope010308 nuclear & particles physicsShell (structure)01 natural sciencesNuclear physicsDipole0103 physical sciencesQuadrupoleAtomic physicsNuclear Experiment010306 general physicsSpectroscopyMagnetic dipolePhysical Review C
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Constraints on Spin-Dependent Short-Range Interaction between Nucleons

2013

We report on the search for a new spin-dependent P- and T-violating interaction between nucleons mediated by light, pseudoscalar bosons such as the axion which was invented to solve the strong CP problem. Our experimental approach is to use an ultra-sensitive low-field magnetometer based on the detection of free precession of co-located 3He and 129Xe nuclear spins using SQUIDs as low-noise magnetic flux detectors. In the presence of an unpolarized mass the precession frequency shif

PhysicsLarmor precessionParticle physicsSpinsHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFOS: Physical sciencesHigh Energy Physics - ExperimentMagnetic fieldPseudoscalarHigh Energy Physics - Experiment (hep-ex)NeutronNucleonAxionBoson
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Carrier-induced ferromagnetism in two-dimensional magnetically doped semiconductor structures

2021

We show theoretically that the magnetic ions, randomly distributed in a two-dimensional (2D) semiconductor system, can generate a ferromagnetic long-range order via the RKKY interaction. The main physical reason is the discrete (rather than continuous) symmetry of the 2D Ising model of the spin-spin interaction mediated by the spin-orbit coupling of 2D free carriers, which precludes the validity of the Mermin-Wagner theorem. Further, the analysis clearly illustrates the crucial role of the molecular field fluctuations as opposed to the mean field. The developed theoretical model describes the desired magnetization and phase-transition temperature ${T}_{c}$ in terms of a single parameter, na…

PhysicsMagnetizationRKKY interactionMean field theoryCondensed matter physicsSpinsFerromagnetismOrder (ring theory)Ising modelCoupling (probability)Physical Review B
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Tunable long-distance spin transport in a crystalline antiferromagnetic iron oxide.

2018

Spintronics relies on the transport of spins, the intrinsic angular momentum of electrons, as an alternative to the transport of electron charge as in conventional electronics. The long-term goal of spintronics research is to develop spin-based, low-dissipation computing-technology devices. Recently, long-distance transport of a spin current was demonstrated across ferromagnetic insulators1. However, antiferromagnetically ordered materials, the most common class of magnetic materials, have several crucial advantages over ferromagnetic systems for spintronics applications2: antiferromagnets have no net magnetic moment, making them stable and impervious to external fields, and can be operated…

PhysicsMultidisciplinaryMagnetic momentSpinsSpintronicsCondensed matter physics02 engineering and technologyElectron021001 nanoscience & nanotechnology01 natural sciences7. Clean energyMagnetic fieldFerromagnetism0103 physical sciencesSpin Hall effectAntiferromagnetismCondensed Matter::Strongly Correlated Electrons010306 general physics0210 nano-technologyNature
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Anisotropic Heisenberg chain with composite spin

1986

A family of one-dimensional magnetic Hamiltonians is introduced, where at each site there are $n$ spin-$S$ operators. It is shown that, for special couplings between spins and for $S=\frac{1}{2}$, the model contains the complete spectrum of the Heisenberg chain with spins \textonehalf{}, 1, frac32;, etc., and the ground state is that of the corresponding Heisenberg chain. By the varying of a single parameter the model allows continuous transitions between chains with different spin. We map the spin-($S+S$) model onto the nonlinear $\ensuremath{\sigma}$ model and discuss the possibility of a finite gap in the spin-(\textonehalf{}+\textonehalf{}) model.

PhysicsNonlinear systemChain (algebraic topology)SpinsQuantum mechanicsSpectrum (functional analysis)SigmaCondensed Matter::Strongly Correlated ElectronsSpin (physics)Ground stateAnisotropyPhysical Review B
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Angular momentum projection of cranked Hartree-Fock states: Application to terminating bands inA~44nuclei

2007

We present the first systematic calculations based on the angular-momentum projection of cranked Slater determinants. We propose the Iy --> I scheme, by which one projects the angular momentum I from the 1D cranked state constrained to the average spin projection of =I. Calculations performed for the rotational band in 46Ti show that the AMP Iy --> I scheme offers a natural mechanism for correcting the cranking moment of inertia at low-spins and shifting the terminating state up by ~2 MeV, in accordance with data. We also apply this scheme to high-spin states near the band termination in A~44 nuclei, and compare results thereof with experimental data, shell-model calculations, and res…

PhysicsNuclear and High Energy PhysicsAngular momentumNuclear TheorySpinsNuclear TheoryNuclear structureHartree–Fock methodFOS: Physical sciencesMoment of inertiaNuclear Theory (nucl-th)Projection (relational algebra)Slater determinantAtomic physicsSpin (physics)Physical Review C
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Ground-state spins and moments of72,74,76,78Ga nuclei

2011

Laser spectroscopy was performed on the ${}^{72,74,76,78}$Ga isotopes at On-Line Isotope Mass Separator (ISOLDE) facility, CERN. Ground-state nuclear spins and moments were extracted from the measured hyperfine spectra. The results are compared to shell-model calculations, which provide a detailed probe of the nuclear wave function. The spin is established from the shape of the hyperfine structure and the parity inferred from a comparison of shell-model calculations with the measured nuclear moments. The ground states of ${}^{76,78}$Ga are both assigned a spin and parity of ${I}^{\ensuremath{\pi}}={2}^{\ensuremath{-}}$, while ${}^{74}$Ga is tentatively assigned as ${I}^{\ensuremath{\pi}}={3…

PhysicsNuclear and High Energy PhysicsAngular momentumSpinsMagnetic moment010308 nuclear & particles physics01 natural sciences7. Clean energySpectral line0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsWave functionGround stateSpectroscopyHyperfine structurePhysical Review C
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Magnetized boxes for housing polarized spins in homogeneous fields

2010

Abstract We present novel types of permanently magnetized as well as current powered boxes built from soft-ferromagnetic materials. They provide shielded magnetic fields which are homogeneous within a large fraction of the enclosed volume, thus minimizing size, weight, and costs. For the permanently magnetized solutions, homogenization is achieved either by an optimized distribution of the permanent field sources or by jacketing the field with a soft-ferromagnetic cylindrical shell which is magnetized in parallel to the enclosed field. The latter principle may be applied up to fields of about 0.1 T. With fields of about 1 mT, such boxes are being used for shipping spin-polarized 3 He worldw…

PhysicsNuclear and High Energy PhysicsCondensed matter physicsSpinsBiophysicsMechanicsModels TheoreticalCondensed Matter PhysicsBiochemistryHomogenization (chemistry)Magnetic fieldlaw.inventionMagneticsElectromagnetic FieldsHomogeneouslawShielded cableComputer SimulationSpin LabelsJournal of Magnetic Resonance
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The decay scheme of the 3-s Isomer of100Nb and the properties of levels in100Mo

1987

Theβ− decay of the longer-lived isomer in100Nb has been studied at the fission-product separator JOSEF. Measurements ofγ-ray singles spectra, ofγ-γ coincidences and ofγ-γ angular correlations have been performed. A value oft1/2=2.99(11)s has been determined for the isomer which probably hasIπ=4+ or 5+. A scheme of the levels of100Mo which are populated in the decay of this isomer has been established. Information on the spins of several states of100Mo has been obtained. Thus,I=0 levels have been identified at 1,505, 2,038 and 2,087 keV. The mixing ratios have been determined for the 22+→21+ and 23+→21+ transitions. The results provide evidence for a vibrational structure of100Mo with separa…

PhysicsNuclear and High Energy PhysicsDecay schemeSpinsExcited stateNuclear fusionAtomic physicsGround stateSpectral lineZeitschrift f�r Physik A Atomic Nuclei
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