Search results for "Condensed Matter::Strongly Correlated Electrons"

showing 10 items of 888 documents

Spin-Wave Driven Bidirectional Domain Wall Motion in Kagome Antiferromagnets

2021

We predict a mechanism to controllably manipulate domain walls in kagome antiferromagnets via a single linearly polarized spin-wave source. We show by means of atomistic spin dynamics simulations of antiferromagnets with kagome structure that the speed and direction of the domain wall motion can be regulated by only tuning the frequency of the applied spin-wave. Starting from microscopics, we establish an effective action and derive the corresponding equations of motion for the spin-wave-driven domain wall. Our analytical calculations reveal that the coupling of two spin-wave modes inside the domain wall explains the frequency-dependent velocity of the spin texture. Such a highly tunable sp…

CouplingPhysicsCondensed Matter - Materials ScienceCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsLinear polarizationMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesGeneral Physics and AstronomyEquations of motionPhysik (inkl. Astronomie)Domain wall (string theory)Spin waveMesoscale and Nanoscale Physics (cond-mat.mes-hall)Domain (ring theory)AntiferromagnetismCondensed Matter::Strongly Correlated ElectronsSpin-½
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Spin-orbit-torque-induced skyrmion dynamics for different types of spin-orbit coupling

2018

Abstract We investigate current-induced skyrmion dynamics in the presence of Dzyaloshinskii-Moriya interaction and spin-orbit spin-transfer torque corresponding to various types of spin-orbit coupling. We determine the symmetries of Dzyaloshinskii-Moriya interaction and spin-orbit spin-transfer torque based on linear spin-orbit coupling model. We find that like interfacial Dzyaloshinskii-Moriya interaction (Rashba spin-orbit coupling) and bulk Dzyaloshinskii-Moriya interaction (Weyl spin-orbit coupling), Dresselhaus spin-orbit coupling also has a possibility for stabilizing skyrmion and current-induced skyrmion dynamics.

CouplingPhysicsCondensed matter physicsSkyrmionDynamics (mechanics)02 engineering and technologySpin–orbit interactionCondensed Matter::Mesoscopic Systems and Quantum Hall Effect021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesElectronic Optical and Magnetic MaterialsQuantum mechanics0103 physical sciencesHomogeneous spaceTorqueCondensed Matter::Strongly Correlated ElectronsAstrophysics::Earth and Planetary Astrophysics010306 general physics0210 nano-technologySpin orbit torqueJournal of Magnetism and Magnetic Materials
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Spin Crossover in Fe(II) Molecular Compounds — Mössbauer and µSR Investigations

2002

The compound [Fe(ptz)6](C104)2 (ptz = 1-propyl-tetrazole) displays a complete and gradual spin crossover centred around 125 K as evidenced by magnetic and muon measurements over the temperature range ∼ 4.2–300 K. Although the crystal structure reveals only one crystallographic site, line broadening is observed in the Mossbauer spectra in the vicinity of the spin transition. The muon spin relaxation behaviour of this compound indicates that a structural transformation rather than dynamic processes may account for the observed spectral features. Both the Mossbauer and muon measurements are consistent with a mixture of high and low spin Fe ions in the transition region.

CrystallographyMuonMaterials scienceSpin crossoverRelaxation (NMR)Mössbauer spectroscopySpin transitionCondensed Matter::Strongly Correlated ElectronsCrystal structureMuon spin spectroscopySimulationSpin-½
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Selective Photoswitching of the Binuclear Spin Crossover Compound{[Fe(bt)(NCS)2]2(bpm)}into Two Distinct Macroscopic Phases

2005

The low-spin (LS-LS, $S=0$) diamagnetic form of the binuclear spin crossover complex ${[\mathrm{Fe}(\mathrm{bt})(\mathrm{NCS}{)}_{2}{]}_{2}(\mathrm{bpm})}$ was selectively photoconverted into two distinct macroscopic phases at different excitation wavelengths (1342 or 647.1 nm). These long-lived metastable phases have been identified, respectively, as the symmetry-broken paramagnetic form (HS-LS, $\mathrm{S}=2$) and the antiferromagnetically coupled (HS-HS, $S=0$) high-spin form of the compound. The selectivity may be explained by the strong coupling of the primary excited states to the paramagnetic state.

CrystallographyParamagnetismMaterials scienceCondensed matter physicsSpin crossoverMetastabilityExcited stateStrong couplingGeneral Physics and AstronomyDiamagnetismCondensed Matter::Strongly Correlated ElectronsSelectivityExcitationPhysical Review Letters
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Geometric, electronic, and magnetic structure ofCo2FeSi: Curie temperature and magnetic moment measurements and calculations

2005

In this work a simple concept was used for a systematic search for materials with high spin polarization. It is based on two semiempirical models. First, the Slater-Pauling rule was used for estimation of the magnetic moment. This model is well supported by electronic structure calculations. The second model was found particularly for ${\mathrm{Co}}_{2}$ based Heusler compounds when comparing their magnetic properties. It turned out that these compounds exhibit seemingly a linear dependence of the Curie temperature as function of the magnetic moment. Stimulated by these models, ${\mathrm{Co}}_{2}\mathrm{FeSi}$ was revisited. The compound was investigated in detail concerning its geometrical…

Curie–Weiss lawMaterials scienceExtended X-ray absorption fine structureCondensed matter physicsMagnetic momentMagnetic structureCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCondensed Matter::Materials ScienceMagnetizationParamagnetismCurie's lawCurie temperatureCondensed Matter::Strongly Correlated ElectronsPhysical Review B
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Orthogonality Catastrophe and Decoherence in a Trapped-Fermion Environment

2012

The Fermi edge singularity and the Anderson orthogonality catastrophe describe the universal physics which occurs when a Fermi sea is locally quenched by the sudden switching of a scattering potential, leading to a brutal disturbance of its ground state. We demonstrate that the effect can be seen in the controllable domain of ultracold trapped gases by providing an analytic description of the out-of-equilibrium response to an atomic impurity, both at zero and at finite temperature. Furthermore, we link the transient behavior of the gas to the decoherence of the impurity, and, in particular to the amount of non-markovianity of its dynamics.

DYNAMICSQuantum decoherenceSINGULARITIESCarbon nanotubesFOS: Physical sciencesGeneral Physics and AstronomyX-RAY ABSORPTIONPolaronCARBON NANOTUBESSettore FIS/03 - Fisica Della MateriaX-ray absorptionEmissionSingularityOrthogonalityQuantum mechanicsMesoscale and Nanoscale Physics (cond-mat.mes-hall)Condensed Matter::Quantum GasesPhysicsQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsScatteringPolaronsFermionKONDO PROBLEMDynamicsKondo problemMetalsPOLARONSCondensed Matter::Strongly Correlated ElectronsGravitational singularityMETALSEMISSIONSingularitiesQuantum Physics (quant-ph)Ground statePhysical Review Letters
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Exchange-transfer in mixed-valence clusters with one migrating hole

1996

Abstract A new mechanism for exchange-transfer specific to hole-type mixed-valence clusters is proposed. The intermediate state in the second-order exchange-transfer process is achieved by the jump of the electron from the spin-core of the dn+1 ion into the empty orbital of the dn ion. As distinguished from the mixed-valence clusters with one delocalized electron this intermediate state is the high-spin one giving rise to a ferromagnetic contribution to the ground manifold. On the basis of angular momentum theory a general solution of the exchange-transfer problem is given for arbitrary nuclearity mixed-valence hole-type clusters with many-electron paramagnetic spin-cores. The interplay bet…

Delocalized electronParamagnetismAngular momentumValence (chemistry)FerromagnetismChemistryGeneral Physics and AstronomyIntermediate stateCondensed Matter::Strongly Correlated ElectronsElectronPhysical and Theoretical ChemistryAtomic physicsIonChemical Physics Letters
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ChemInform Abstract: Spin Density Distribution in Transition Metal Complexes: Some Thoughts and Hints

2010

Abstract The spin density distribution in transition metal complexes is discussed in qualitative terms, taking into account the coexistence of spin delocalization and spin polarization mechanisms, with the help of numerical results for several complexes obtained from density functional calculations. The covalent character of the metal-ligand bonds as well as the σ- or π-characteristics of the partially filled d orbitals must be taken into account to qualitatively predict the sign of the spin density at a particular atom within a ligand. The same patterns can be applied to binuclear complexes and can be helpful in determining the ferro- or antiferromagnetic character of the exchange coupling…

Delocalized electronParamagnetismCondensed matter physicsAtomic orbitalTransition metalSpin polarizationChemistryAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsMolecular orbitalGeneral MedicineSpin-½ChemInform
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Phase diagram of the quarter-filled extended Hubbard model on a two-leg ladder

2000

We investigate the ground-state phase diagram of the quarter-filled Hubbard ladder with nearest-neighbor Coulomb repulsion V using the Density Matrix Renormalization Group technique. The ground-state is homogeneous at small V, a ``checkerboard'' charge--ordered insulator at large V and not too small on-site Coulomb repulsion U, and is phase-separated for moderate or large V and small U. The zero-temperature transition between the homogeneous and the charge-ordered phase is found to be second order. In both the homogeneous and the charge-ordered phases the existence of a spin gap mainly depends on the ratio of interchain to intrachain hopping. In the second part of the paper, we construct an…

Density matrixPhysicsStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelCondensed matter physicsFOS: Physical sciences02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesSpin chainsymbols.namesakeCondensed Matter - Strongly Correlated ElectronsHomogeneous0103 physical sciencessymbolsStrongly correlated materialCondensed Matter::Strongly Correlated Electrons010306 general physics0210 nano-technologyGround stateHamiltonian (quantum mechanics)Phase diagram
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Stripe formation in doped Hubbard ladders

2004

We investigate the formation of stripes in $7\chunks \times 6$ Hubbard ladders with $4\chunks$ holes doped away from half filling using the density-matrix renormalization group (DMRG) method. A parallelized code allows us to keep enough density-matrix eigenstates (up to $m=8000$) and to study sufficiently large systems (with up to $7\chunks = 21$ rungs) to extrapolate the stripe amplitude to the limits of vanishing DMRG truncation error and infinitely long ladders. Our work gives strong evidence that stripes exist in the ground state for strong coupling ($U=12t$) but that the structures found in the hole density at weaker coupling ($U=3t$) are an artifact of the DMRG approach.

Density matrixPhysicsTruncation errorHubbard modelCondensed matter physicsStrongly Correlated Electrons (cond-mat.str-el)Density matrix renormalization groupFOS: Physical sciencesRenormalization groupCondensed Matter PhysicsCoupling (probability)Electronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated ElectronsQuantum mechanicsStrongly correlated materialCondensed Matter::Strongly Correlated ElectronsGround state
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