Search results for "electrons"

showing 10 items of 1325 documents

Heavy fermion spin liquid in herbertsmithite

2015

We analyze recent heat capacity measurements in herbertsmithite $\rm ZnCu_3(OH)_6Cl_2$ single crystal samples subjected to strong magnetic fields. We show that the temperature dependence of specific heat $C_{mag}$ formed by quantum spin liquid at different magnetic fields $B$ resembles the electronic heat capacity $C_{el}$ of the HF metal $\rm YbRh_2Si_2$. We demonstrate that the spinon effective mass $M^*_{mag}\propto C_{mag}/T$ exhibits a scaling behavior like that of $C_{el}/T$. We also show that the recent measurements of $C_{mag}$ are compatible with those obtained on powder samples. These observations allow us to conclude that $\rm ZnCu_3(OH)_6Cl_2$ holds a stable strongly correlated …

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsFOS: Physical sciencesGeneral Physics and Astronomyengineering.materialHeat capacitySpinonMagnetic fieldCondensed Matter - Strongly Correlated ElectronsEffective mass (solid-state physics)engineeringCondensed Matter::Strongly Correlated ElectronsHerbertsmithiteStrongly correlated materialFermi liquid theoryQuantum spin liquidPhysics Letters A
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Chaotic Antiferromagnetic Nano-Oscillator driven by Spin-Torque

2021

We theoretically describe the behavior of a terahertz nano-oscillator based on an anisotropic antiferromagnetic dynamical element driven by spin torque. We consider the situation when the polarization of the spin-current is perpendicular to the external magnetic field applied along the anisotropy easy-axis. We determine the domain of the parametric space (field, current) where the oscillator demonstrates chaotic dynamics. Characteristics of the chaotic regimes are analyzed using conventional techniques such as spectra of the Lyapunov exponents. We show that the threshold current of the chaos appearance is particularly low in the vicinity of the spin-flop transition. In this regime, we consi…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsField (physics)ChaoticFOS: Physical sciences02 engineering and technologyLyapunov exponent021001 nanoscience & nanotechnologyNonlinear Sciences - Chaotic Dynamics01 natural sciencesMagnetic fieldNonlinear Sciences::Chaotic Dynamicssymbols.namesakeMagnetic anisotropyCondensed Matter - Strongly Correlated ElectronsQuasiperiodic functionPhase space0103 physical sciencessymbolsChaotic Dynamics (nlin.CD)010306 general physics0210 nano-technologySpin-½
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Correlation energy of two-dimensional systems: Toward non-empirical and universal modeling

2009

The capability of density-functional theory to deal with the ground-state of strongly correlated low-dimensional systems, such as semiconductor quantum dots, depends on the accuracy of functionals developed for the exchange and correlation energies. Here we extend a successful approximation for the correlation energy of the three dimensional inhomogeneous electron gas, originally introduced by Becke [J. Chem. Phys. {\bf 88}, 1053 (1988)], to the two-dimensional case. The approach aims to non-empirical modeling of the correlation-hole functions satisfying a set of exact properties. Furthermore, the electron current and spin are explicitly taken into account. As a result, good performance is …

PhysicsStrongly Correlated Electrons (cond-mat.str-el)FOS: Physical sciencesCondensed Matter PhysicsElectron localization functionElectronic Optical and Magnetic MaterialsMagnetic fieldCondensed Matter - Strongly Correlated ElectronsQuantum dotQuantum mechanicsDensity functional theoryFermi gasGround stateEnergy (signal processing)Spin-½
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The Hubbard model beyond the two-pole approximation: a Composite Operator Method study

2014

Within the framework of the Composite Operator Method, a three-pole solution for the two-dimensional Hubbard model is presented and analyzed in detail. In addition to the two Hubbard operators, the operatorial basis comprises a third operator describing electronic transitions dressed by nearest-neighbor spin fluctuations. These latter, compared to charge and pair fluctuations, are assumed to be preeminent in the region of model-parameter space - small doping, low temperature and large on-site Coulomb repulsion - where one expects strong electronic correlations to dominate the physics of the system. This assumption and the consequent choice for the basic field, as well as the whole analytica…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Field (physics)Hubbard modelBasis (linear algebra)Numerical analysisCondensed Matter - SuperconductivityCrossoverFOS: Physical sciencesCharge (physics)Solid State and MaterialsCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsSuperconductivity (cond-mat.supr-con)Condensed Matter - Strongly Correlated ElectronsOperator (computer programming)Solid State and Materials;Statistical physicsSpin-½
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Magnetic properties of a strongly correlated system on the Bethe lattice

2010

We study the influence of an external magnetic field h on the phase diagram of a system of Fermi particles living on the sites of a Bethe lattice with coordination number z and interacting through on-site U and nearest-neighbor V interactions. This is a physical realization of the extended Hubbard model in the narrow-band limit. Our results establish that the magnetic field may dramatically affect the critical temperature below which a long-range charge ordered phase is observed, as well as the behavior of physical quantities, inducing, for instance, magnetization plateaus in the magnetization curves. Relevant thermodynamic quantities - such as the specific heat and the susceptibility - are…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelBethe latticeCondensed matter physicsFOS: Physical sciencesGeneral Physics and AstronomyCharge (physics)Magnetic fieldCondensed Matter - Strongly Correlated ElectronsMagnetizationPhase (matter)Phase diagramPhysical quantityJournal of Physical Studies
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Fourth-order perturbation theory for the half-filled Hubbard model in infinite dimensions

2003

We calculate the zero-temperature self-energy to fourth-order perturbation theory in the Hubbard interaction $U$ for the half-filled Hubbard model in infinite dimensions. For the Bethe lattice with bare bandwidth $W$, we compare our perturbative results for the self-energy, the single-particle density of states, and the momentum distribution to those from approximate analytical and numerical studies of the model. Results for the density of states from perturbation theory at $U/W=0.4$ agree very well with those from the Dynamical Mean-Field Theory treated with the Fixed-Energy Exact Diagonalization and with the Dynamical Density-Matrix Renormalization Group. In contrast, our results reveal t…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelBethe latticeFOS: Physical sciencesRenormalization groupCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated ElectronsFourth orderIterated functionQuasiparticleDensity of statesCondensed Matter::Strongly Correlated ElectronsPerturbation theory (quantum mechanics)Mathematical physicsThe European Physical Journal B - Condensed Matter
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Universal probes for antiferromagnetic correlations and entropy in cold fermions on optical lattices

2012

We determine antiferromagnetic (AF) signatures in the half-filled Hubbard model at strong coupling on a cubic lattice and in lower dimensions. Upon cooling, the transition from the charge-excitation regime to the AF Heisenberg regime is signaled by a universal minimum of the double occupancy at entropy s=S/(N k_B)=s*=ln(2) per particle and a linear increase of the next-nearest neighbor (NNN) spin correlation function for s<s*. This crossover, driven by a gain in kinetic exchange energy, appears as the essential AF physics relevant for current cold-atom experiments. The onset of long-range AF order (at low s on cubic lattices) is hardly visible in nearest-neighbor spin correlations versus s,…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelCondensed matter physicsExchange interactionFOS: Physical sciencesFermionApproxKinetic energyAtomic and Molecular Physics and OpticsCondensed Matter - Strongly Correlated ElectronsQuantum Gases (cond-mat.quant-gas)Lattice (order)AntiferromagnetismCondensed Matter::Strongly Correlated ElectronsCondensed Matter - Quantum GasesEntropy (order and disorder)
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Defect states and excitations in a Mott insulator with orbital degrees of freedom: Mott-Hubbard gap versus optical and transport gaps in doped systems

2013

We address the role played by charged defects in doped Mott insulators with active orbital degrees of freedom. It is observed that defects feature a rather complex and rich physics, which is well captured by a degenerate Hubbard model extended by terms that describe crystal-field splittings and orbital-lattice coupling, as well as by terms generated by defects such as the Coulomb potential terms that act both on doped holes and on electrons within occupied orbitals at undoped sites. We show that the multiplet structure of the excited states generated in such systems by strong electron interactions is well described within the unrestricted Hartree-Fock approximation, once the symmetry breaki…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelCondensed matter physicsMott insulatorFOS: Physical sciencesOrder (ring theory)Condensed Matter PhysicsCoupling (probability)Electronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated ElectronsAtomic orbitalNon-bonding orbitalCondensed Matter::Strongly Correlated ElectronsSpin (physics)Multiplet
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Orbital-selective Mott transitions in the anisotropic two-band Hubbard model at finite temperatures

2005

The anisotropic degenerate two-orbital Hubbard model is studied within dynamical mean-field theory at low temperatures. High-precision calculations on the basis of a refined quantum Monte Carlo (QMC) method reveal that two distinct orbital-selective Mott transitions occur for a bandwidth ratio of 2 even in the absence of spin-flip contributions to the Hund exchange. The second transition -- not seen in earlier studies using QMC, iterative perturbation theory, and exact diagonalization -- is clearly exposed in a low-frequency analysis of the self-energy and in local spectra.

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelCondensed matter physicsQuantum Monte CarloDegenerate energy levelsFOS: Physical sciencesCondensed Matter PhysicsSpectral lineElectronic Optical and Magnetic MaterialsMott transitionCondensed Matter - Strongly Correlated ElectronsMean field theoryQuantum mechanicsStrongly correlated materialCondensed Matter::Strongly Correlated ElectronsAnisotropy
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Density gradients for the exchange energy of electrons in two dimensions

2009

We derive a generalized gradient approximation to the exchange energy to be used in density functional theory calculations of two-dimensional systems. This class of approximations has a long and successful history, but it has not yet been fully investigated for electrons in two dimensions. We follow the approach originally proposed by Becke for three-dimensional systems [Int. J. Quantum Chem. 23, 1915 (1983), J. Chem. Phys. 85, 7184 (1986)]. The resulting functional depends on two parameters that are adjusted to a test set of parabolically confined quantum dots. Our exchange functional is then tested on a variety of systems with promising results, reducing the error in the exchange energy b…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Orbital-free density functional theoryExchange interactionFOS: Physical sciences02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesAtomic and Molecular Physics and OpticsHybrid functionalCondensed Matter - Strongly Correlated ElectronsQuantum dotQuantum mechanics0103 physical sciencesDensity functional theoryLocal-density approximation010306 general physics0210 nano-technologyQuantumElectronic density
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