1,921 research outputs found
Correlated versus Ferromagnetic State in Repulsively Interacting Two-Component Fermi Gases
Whether a spin-1/2 Fermi gas will become ferromagnetic as the strength of
repulsive interaction increases is a long-standing controversial issue.
Recently this problem is studied experimentally by Jo et al, Science, 325, 1521
(2009) in which the authors claim a ferromagnetic transition is observed. This
work is to point out the results of this experiment can not distinguish whether
the system is in a ferromagnetic state or in a non-magnetic but strongly
short-range correlated state. A conclusive experimental demonstration of
ferromagnetism relies on the observation of ferromagnetic domains.Comment: 4 pages, 2 figures, published versio
Itinerant ferromagnetism in the multiorbital Hubbard model: a dynamical mean-field study
In order to resolve the long-standing issue of how the itinerant
ferromagnetism is affected by the lattice structure and Hund's coupling, we
have compared various three-dimensional lattice structures in the single- and
multiorbital Hubbard models with the dynamical mean-field theory with an
improved quantum Monte Carlo algorithm that preserves the spin-SU(2) symmetry.
The result indicates that {\it both} the lattice structure and the d-orbital
degeneracy are essential for the ferromagnetism in the parameter region
representing a transition metal. Specifically, (a) Hund's coupling, despite the
common belief, is important, which is here identified to come from
particle-hole scatterings, and (b) the ferromagnetism is a correlation effect
(outside the Stoner picture) as indicated from the band-filling dependence.Comment: 4 pages, 5 figure
Magnetism of Cold Fermionic Atoms on p-Band of an Optical Lattice
We carry out \textit{ab initio} study of ground state phase diagram of
spin-1/2 cold fermionic atoms within two-fold degenerate -band of an
anisotropic optical lattice. Using the Gutzwiller variational approach, we show
that a robust ferromagnetic phase exists for a vast range of band fillings and
interacting strengths. The ground state crosses over from spin density wave
state to spin-1 Neel state at half filling. Additional harmonic trap will
induce spatial separation of varies phases. We also discuss several relevant
observable consequences and detection methods. Experimental test of the results
reported here may shed some light on the long-standing issue of itinerant
ferromagnetism.Comment: 5 pages, 4 figure
Pairing, Ferromagnetism, and Condensation of a normal spin-1 Bose gas
We theoretically study the stability of a normal, spin disordered, homogenous
spin-1 Bose gas against ferromagnetism, pairing, and condensation through a
Random Phase Approximation which includes exchange (RPA-X). Repulsive
spin-independent interactions stabilize the normal state against both
ferromagnetism and pairing, and for typical interaction strengths leads to a
direct transition from an unordered normal state to a fully ordered single
particle condensate. Atoms with much larger spin-dependent interaction may
experience a transition to a ferromagnetic normal state or a paired superfluid,
but, within the RPA-X, there is no instability towards a normal state with
spontaneous nematic order. We analyze the role of the quadratic Zeeman effect
and finite system size.Comment: 4 pages, 3 figures, 1 table. Supplementary materials attache
Coupling between magnetic ordering and structural instabilities in perovskite biferroics: A first-principles study
We use first-principles density functional theory-based calculations to
investigate structural instabilities in the high symmetry cubic perovskite
structure of rare-earth (R La, Y, Lu) and Bi-based biferroic chromites,
focusing on and point phonons of states with para-, ferro-, and
antiferromagnetic ordering. We find that (a) the structure with G-type
antiferromagnetic ordering is most stable, (b) the most dominant structural
instabilities in these oxides are the ones associated with rotations of oxygen
octahedra, and (c) structural instabilities involving changes in Cr-O-Cr bond
angle depend sensitively on the changes in magnetic ordering. The dependence of
structural instabilities on magnetic ordering can be understood in terms of how
super-exchange interactions depend on the Cr-O-Cr bond angles and Cr-O bond
lengths. We demonstrate how adequate buckling of Cr-O-Cr chains can favour
ferromagnetism. Born effective charges (BEC) calculated using the Berry phase
expression are found to be anomalously large for the A-cations, indicating
their chemical relevance to ferroelectric distortions.Comment: 8 pages, 13 figure
Validity of the scattering length approximation in strongly interacting Fermi systems
We investigate the energy spectrum of systems of two, three and four spin-1/2
fermions with short range attractive interactions both exactly, and within the
scattering length approximation. The formation of molecular bound states and
the ferromagnetic transition of the excited scattering state are examined
systematically as a function of the 2-body scattering length. Identification of
the upper branch (scattering states) is discussed and a general approach valid
for systems with many particles is given. We show that an adiabatic
ferromagnetic transition occurs, but at a critical transition point kF a much
higher than predicted from previous calculations, almost all of which use the
scattering length approximation. In the 4-particle system the discrepancy is a
factor of 2. The exact critical interaction strength calculated in the
4-particle system is consistent with that reported by experiment. To make
comparisons with the adiabatic transition, we study the quench dynamics of the
pairing instability using the eigenstate wavefunctions.Comment: 7 pages, 7 figure
Quantum nucleation in a single-chain magnet
The field sweep rate (v=dH/dt) and temperature (T) dependence of the
magnetization reversal of a single-chain magnet (SCM) is studied at low
temperatures. As expected for a thermally activated process, the nucleation
field (H_n) increases with decreasing T and increasing v. The set of H_n(T,v)
data is analyzed with a model of thermally activated nucleation of
magnetization reversal. Below 1 K, H_n becomes temperature independent but
remains strongly sweep rate dependent. In this temperature range, the reversal
of the magnetization is induced by a quantum nucleation of a domain wall that
then propagates due to the applied field.Comment: 5 pages, 4 figure
Nearly flat band with Chern number C=2 on the dice lattice
We point out the possibility of nearly flat band with Chern number C=2 on the
dice lattice in a simple nearest-neighbor tightbinding model. This lattice can
be naturally formed by three adjacent layers of cubic lattice, which
may be realized in certain thin films or artificial heterostructures, such as
SrTiO/SrIrO/SrTiO trilayer heterostructure grown along
direction. The flatness of two bands is protected by the bipartite nature of
the lattice. Including the Rashba spin-orbit coupling on nearest-neighbor bonds
separate the flat bands with others but maintains their flatness. Repulsive
interaction will drive spontaneous ferromagnetism on the Kramer pair of flat
bands and split them into two nearly flat bands with Chern number . We
thus propose that this may be a route to quantum anomalous Hall effect and
further conjecture that partial filling of the C=2 band may realize exotic
fractional quantum Hall effects.Comment: updated references, 5 pages, 4 figures, RevTex
Magnetism of 3d transition metal atoms on W(001): submonolayer films
We have investigated random submonolayer films of 3d transition metals on
W(001). The tight-binding linear muffin-tin orbital method combined with the
coherent potential approximation was employed to calculate the electronic
structure of the films. We have estimated local magnetic moments and the
stability of different magnetic structures, namely the ferromagnetic order, the
disordered local moments and the non-magnetic state, by comparing the total
energies of the corresponding systems. It has been found that the magnetic
moments of V and Cr decrease and eventually disappear with decreasing coverage.
On the other hand, Fe retains approximately the same magnetic moment throughout
the whole concentration range from a single impurity to the monolayer coverage.
Mn is an intermediate case between Cr and Fe since it is non-magnetic at very
low coverages and ferromagnetic otherwise.Comment: 5 pages, 3 figures in 6 files; presented at ICN&T 2006, Basel,
Switzerlan
Hysteretic properties of a magnetic particle with strong surface anisotropy
We study the influence of surface anisotropy on the zero-temperature
hysteretic properties of a small single-domain magnetic particle, and give an
estimation of the anisotropy constant for which deviations from the
Stoner-Wohlfarth model are observed due to non-uniform reversal of the
particle's magnetisation. For this purpose, we consider a spherical particle
with simple cubic crystalline structure, a uniaxial anisotropy for core spins
and radial anisotropy on the surface. The hysteresis loop is obtained by
solving the local (coupled) Landau-Lifschitz equations for classical spin
vectors. We find that when the surface anisotropy constant is at least of the
order of the exchange coupling, large deviations are observed with respect to
the Stoner-Wohlfarth model in the hysteresis loop and thereby the
limit-of-metastability curve, since in this case the magnetisation reverses its
direction in a non-uniform manner via a progressive switching of spin clusters.
In this case the critical field, as a function of the particle's size, behaves
as observed in experiments.Comment: 12 pages, 15 eps figure
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