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1.
The ground state of a quasi-particle (exciton, electron or hole) interacting with optical and acoustic phonons in a one-dimensional chain, is investigated using a variational method. The phase diagrams are obtained which show the regions of the electron-phonon coupling constant and nonadiabaticity parameter where the ground state of a quasiparticle is described as almost free electron state, small polaron, or spontaneously localized state. It is shown that the formation of a soliton-like state has a threshold with respect to the value of electron-phonon interaction. The corresponding critical value of the coupling constant increases with the nonadiabaticity parameter increasing. 相似文献
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I.I. Satija 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,29(2):345-348
Disordered systems exhibiting exponential localization are mapped to anisotropic spin chains with localization length being
related to the anisotropy of the spin model. This relates localization phenomenon in fermions to the rotational symmetry breaking
in the critical spin chains. One of the intriguing consequence is that the statement of Onsager universality in spin chains
implies universality of the localized fermions where the fluctuations in localized wave functions are universal. We further
show that the fluctuations about localized nonrelativistic fermions describe relativistic fermions. This provides a new approach
to understand the absence of localization in disordered Dirac fermions. We investigate how disorder affects well known universality
of the spin chains by examining the multifractal exponents. Finally, we examine the effects of correlations on the localization
characteristics of relativistic fermions.
Received 28 September 2001 / Received in final form 30 November 2001 Published online 2 October 2002
RID="a"
ID="a"e-mail: isatija@nickel.nist.gov 相似文献
4.
Based on a theoretical model proposed for interchain-coupled quasi-one-dimensional organic magnetic polymer, the effects of the interchain couplings and electron–electron interactions on the charge density wave (CDW) and spin density wave (SDW) that exist in the system are studied. It is found that the amplitude of the SDW along the main chain will decrease with increasing of the oscillatory term of the interchain couplings in the system, which is unfavorable to the ferromagnetic ground state of the system. Moreover, with different interchain couplings, there will all exist a critical value of the inter-site electron–electron Coulomb repulsion, and at this value, the system will experience a transformation from strong SDW state to strong CDW one, which will weaken the mediating function of the antiferromagnetic SDW along the main chain. As a result, the ferromagnetic correlation intensity between the spins of the side radicals will be affected and consequently the stability of the ferromagnetic state in the system will be weakened. 相似文献
5.
M.S.S. Brooks 《Applied Physics A: Materials Science & Processing》2001,73(6):659-661
Large spin–orbit interaction produces large orbital magnetic moments in narrow energy bands. Since the orbital character of
the wave functions is more important in orbital than in spin magnetism, the limitations of the local spin density approximation
become evident. It is possible to keep the orbital dependence of the exchange interactions by using an orbital polarization
scheme or by using Hartree–Fock theory with screened Slater integrals for exchange. This leads to an enhancement of the calculated
orbital moment when the magnetism is strong. Recently calculated magnetic moments and calculated sum rules for X-ray magnetic
circular dichroism in US are described.
Received: 23 May 2001 / Accepted: 4 July 2001 / Published online: 5 October 2001 相似文献
6.
A. P. Chetverikov W. Ebeling M. G. Velarde 《The European Physical Journal B - Condensed Matter and Complex Systems》2006,51(1):87-99
We investigate the onset and maintenance of nonlinear soliton-like excitations in chains
of atoms with Morse interactions at rather high densities, where
the exponential repulsion dominates.
First we discuss the atomic interactions and approximate the
Morse potential by an effective Toda potential with
adapted density-dependent parameters.
Then we study several mechanisms to generate
and stabilize the soliton-like excitations:
(i) External forcing: we shake the masses periodically, mimicking a
piezoelectric-like excitation, and delay subsequent damping
by thermal excitation;
(ii) heating, quenching and active friction:
we heat up the system to a relatively high temperature Gaussian
distribution, then quench to a low temperature,
and subsequently stabilize by active friction. Finally,
we assume that the atoms in the chain are ionized with free electrons able to move along the lattice.
We show that the nonlinear soliton-like excitations
running on the chain interact with the electrons. They
influence their motion in the presence of an external field creating dynamic
bound states (“solectrons”, etc.). We show that these
bound states
can move very fast and create extra current.
The soliton-induced contribution to the current
is constant, field-independent for a significant range of values when approaching the zero-field value. 相似文献
7.
We study the Ruderman–Kittle–Kasuya–Yosida (RKKY) interaction in doped armchair graphene nanoribbon. The effects of both external magnetic field and electron-Holstein phonon on RKKY interaction have been addressed. RKKY interaction as a function of distance between localized moments has been analyzed. It has been shown that a magnetic field along the z-axis mediates an anisotropic interaction which corresponds to a XXZ model interaction between two magnetic moments. In order to calculate the exchange interaction along arbitrary direction between two magnetic moments, we should obtain both transverse and longitudinal static spin susceptibilities of armchair graphene nanoribbon in the presence of electron-phonon coupling and magnetic field. The spin susceptibility components are calculated using the spin dependent Green’s function approach for Holstein model Hamiltonian. The effects of spin polarization on the dependence of exchange interaction on distance between moments are investigated via calculating correlation function of spin density operators. Our results show the influences of magnetic field on the spatial behavior of in-plane and longitudinal RKKY interactions are different in the presence of magnetic field. 相似文献
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We study the Ruderman-Kittle-Kasuya-Yosida (RKKY) interaction in doped armchair nanotube in the presence of gap parameter. The effects of both next nearest neighbor hopping parameter and electron-Holstein phonon on RKKY interaction have been addressed. RKKY interaction as a function of distance between localized moments have been analyzed. In order to calculate the exchange interaction along arbitrary direction between two magnetic moments, we should obtain the transverse static spin susceptibility of armchair graphene nanoribbon in the presence of electron-phonon coupling and gap parameter. The spin susceptibility components are calculated using Green’s function approach for Holstein model Hamiltonian. The effects of electron doping on dependence of exchange interaction on distance between moments are investigated via calculating correlation function of spin density operators. Our results show the influences of next nearest neighbor hopping parameter on the spatial behavior of RKKY interactions are different in the presence of electron phonon coupling. 相似文献
10.
J.-P. Wang H. Meng 《The European Physical Journal B - Condensed Matter and Complex Systems》2007,59(4):471-474
Spin torque transfer structures with new spin switching configurations are
proposed, fabricated and investigated in this paper. The non-uniform
current-induced magnetization switching is implemented based on both GMR and
MTJ nano devices. The proposed new spin transfer structure has a hybrid free
layer that consists of a layer with conductive channels (magnetic) and
non-conductive matrix (non-magnetic) and traditional free layer(s). Two
mechanisms, a higher local current density by nano-current-channels and a
non-uniform magnetization switching (reversal domain nucleation and growth)
by a magnetic nanocomposite structure, contribute in reducing the switching
current density. The critical switching current density for the new spin
transfer structure is reduced to one third of the typical value for the
normal structure. It can be expected to have one order of magnitude or more
reduction for the critical current density if the optimization of materials
and fabrication processes could be done further. Meanwhile, the thermal
stability of this new spin transfer structure is not degraded, which may
solve the long-standing scaling problem for magnetic random access memory
(MRAM). This spin transfer structure, with the proposed and demonstrated new
spin switching configurations, not only provides a solid approach for the
practical application of spin transfer devices but also forms a unique
platform for researchers to explore the non-uniform current-induced
switching process. 相似文献
11.
The next-nearest neighbor hopping interactions of π-electrons in quasi-one-dimensional organic polymer ferromagnets are considered.
Within the mean-field theory and allowing for full lattice relaxation, a set of self-consistent equations is established to
study the system. It is found that with increasing of the next-nearest neighbor interaction a charge-density-wave (CDW) transition
will happen. At the CDW state, a strong charge density distribution along the main chain will appear, and the spin density-wave
(SDW) along the main chian will be tuned by the CDW. Consequently the ferromagnetic state, in which all the spins of the unpaired
electrons at side freeradicals are arranged parallely, will be no longer the stable ground state of the system. 相似文献
12.
B. Binz D. Baeriswyl B. Douçot 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,25(1):69-87
The weak coupling instabilities of a two dimensional Fermi system are investigated for the case of a square lattice using
a Wilson renormalization group scheme to one loop order. We focus on a situation where the Fermi surface passes through two
saddle points of the single particle dispersion. In the case of perfect nesting, the dominant instability is a spin density
wave but d-wave superconductivity as well as charge or spin flux phases are also obtained in certain regions in the space of coupling
parameters. The low energy regime in the vicinity of these instabilities can be studied analytically. Although saddle points
play a major role (through their large contribution to the single particle density of states), the presence of low energy
excitations along the Fermi surface rather than at isolated points is crucial and leads to an asymptotic decoupling of the
various instabilities. This suggests a more mean-field like picture of these instabilities, than the one recently established
by numerical studies using discretized Fermi surfaces.
Received 11 April 2001 and Received in final form 6 September 2001 相似文献
13.
Anupam Madhukar 《Solid State Communications》1973,13(11):1767-1770
A simple criterion for antiferromagnetic ordering versus lattice distortion in very narrow band materials is obtained. The model describing these narrow band materials contains the Hubbard Hamiltonian, short ranged interatomic Coulomb and exchange interactions, and the electron-phonon interaction. 相似文献
14.
R.T. Senger A. Erçelebi 《The European Physical Journal B - Condensed Matter and Complex Systems》2000,16(3):439-446
In the limit of strong electron-phonon coupling, we provide a unified insight into the stability criterion for bipolaron formation
in low-dimensionally confined media. The model that we use consists of a pair of electrons immersed in a reservoir of bulk
LO phonons and confined within an anisotropic parabolic potential box, whose barrier slopes can be tuned arbitrarily from
zero to infinity. Thus, encompassing the bulk and all low-dimensional geometric configurations of general interest, we obtain
an explicit tracking of the critical ratio of dielectric constants below which bipolarons can exist.
Received 15 September 1999 and Received in final form 20 March 2000 相似文献
15.
S. Villain-Guillot C. Josserand 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,29(2):305-309
We develop a new technique describing the non linear growth of interfaces. We apply this analytical approach to the one dimensional
Cahn-Hilliard equation. The dynamics is captured through a solvability condition performed over a particular family of quasi-static
solutions. The main result is that the dynamics along this particular class of solutions can be expressed in terms of a simple
ordinary differential equation. The density profile of the stationary regime found at the end of the non-linear growth is
also well characterized. Numerical simulations are compared in a satisfactory way with the analytical results through three
different fitting methods and asymptotic dynamics are well recovered, even far from the region where the approximations hold.
Received 16 October 2001 / Received in final form 15 March 2002 Published online 2 October 2002
RID="a"
ID="a"e-mail: josseran@lmm.jussieu.fr
RID="b"
ID="b"UMR CNRS 7607 相似文献
16.
K.S.D. Beach R.J. Gooding 《The European Physical Journal B - Condensed Matter and Complex Systems》2000,16(4):579-591
We examine the role of spin twists in the formation of domain walls, often called stripes, by focusing on the spin textures
found in the cluster spin glass phases of and . To this end, we derive improved analytic expressions for the spin distortions produced by a frustrating bond, both near
the core region of the bond and in the far field, and then derive an improved expression for interaction energies between
such bonds. We critique our analytical theory by comparison to numerical solutions of this problem and find excellent agreement.
By looking at collections of small numbers of such bonds localized in some region of a lattice, we demonstrate the stability
of small “clusters” of spins, each cluster having its own orientation of its antiferromagnetic order parameter. Then, we display
a domain wall corresponding to spin twists between clusters of locally ordered spins showing how spin twists can serve as
a mechanism for stripe formation. Since the charges are localized in this model, we emphasize that these domain walls are
produced in a situation for which no kinetic energy is present in the problem.
Received 10 January 2000 相似文献
17.
《Journal of magnetism and magnetic materials》2001,223(2):156-162
We studied zero-temperature magnetic ordering in a model organic ferrimagnet- polyallyl spin-1/2 chain as a function of the exchange integral λ describing the interaction between spins of radical centers and the main chain. Exact diagonalization and density matrix renormalization group (DMRG) methods demonstrated that for small applied fields, the difference in zero-temperature magnetizations of the sublattices reaches a maximum value at λ=0.70. It was shown that there is a critical value of magnetic field, above which this ferrimagnetic ordering is destroyed. We also present the results of DMRG calculations that show the gap character of excitations without decrease of the total spin for λ⩾0.4. 相似文献
18.
A. Eilmes R.A. Römer M. Schreiber 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,23(2):229-234
We study the influence of many-particle interactions on a metal-insulator transition. We consider the two-interacting-particle
problem for onsite interacting particles on a one-dimensional quasiperiodic chain, the so-called Aubry-André model. We show
numerically by the decimation method and finite-size scaling that the interaction does not modify the critical parameters
such as the transition point and the localization-length exponent. We compare our results to the case of finite density systems
studied by means of the density-matrix renormalization scheme.
Received 28 June 2001 相似文献
19.
The anchoring of nematic liquid crystals on surfaces with grafted liquid-crystalline chain molecules is studied by computer
simulations and within a mean-field approach. The computer simulations show that a swollen layer of collectively tilted chains
may induce untilted homeotropic (perpendicular) alignment in the nematic fluid. The results can be understood within a simple
theoretical model. The anchoring on a layer of mutually attractive chains is determined by the structure of the interface
between the layer of chain molecules and the solvent. It is controlled by an interplay between the attractive chain interactions,
the translational entropy of the solvent and its elasticity. A second-order anchoring transition driven by the grafting density
from tilted-to-homeotropic alignment is predicted.
Received 5 July 2001 and Received in final form 16 November 2001 相似文献
20.
J. Berg S. Franz M. Sellitto 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,26(3):349-356
The Edwards hypothesis of ergodicity of blocked configurations for gently tapped granular materials is tested for aaabstract
models of spin systems on random graphs and spin chains with kinetic constraints. The tapping dynamics is modeled by considering
two distinct mechanisms of energy injection: thermal and random tapping. We find that ergodicity depends upon the tapping procedure (i.e. the way the blocked configurations are dynamically accessed): for thermal tapping ergodicity is a good approximation, while
it fails to describe the asymptotic stationary state reached by the random tapping dynamics.
Received 30 November 2001 相似文献