共查询到20条相似文献,搜索用时 62 毫秒
1.
Vl.A. Margulis S.V. Makarov T.V. Piterimova E.A. Gaiduk 《The European Physical Journal B - Condensed Matter and Complex Systems》2003,33(2):153-164
Using a mean-field approximation, we have developed a systematic treatment of collective electronic modes in a semiconductor
superlattice (SL) in the presence of strong electric and magnetic fields parallel to the SL axis. The spectrum of collective
modes with zero wavevector along the SL axis is shown to consist of a principle magnetoplasmon mode and an infinite set of
Bernstein-like modes. For non-zero wavevector along the SL axis, in addition to the cyclotron modes, extra collective modes
are found at the frequencies |Nω
c±Mω
s|, which we call cyclotron-Stark modes (ω
c and ω
s are respectively the cyclotron and Stark frequencies, N and M are integer numbers). The frequencies of the modes propagating in “oblique” direction with respect to the SL axis show oscillatory
behavior as a function of electric field strength. All the modes considered have very weak spatial dispersion and they are
not Landau damped. The specific predictions made for the dispersion relations of the collective excitations should be observable
in resonant Raman scattering experiments.
Received 29 August 2002 / Received in final form 25 February 2003 Published online 4 June 2003
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ID="a"e-mail: 612033@inbox.ru 相似文献
2.
V.Yu. Irkhin M.I. Katsnelson 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,30(4):481-486
Peculiarities of transport properties of three- and two-dimensional half-metallic ferromagnets are investigated, which are
connected with the absence of spin-flip scattering processes. The temperature and magnetic field dependences of resistivity
in various regimes are calculated. The resistivity is proportional to T
9/2 for T < T
* and to T
7/2 for T > T
*, T* being the crossover temperature for longitudinal scattering processes. The latter scale plays also an important role in magnetoresistance.
The contribution of non-quasiparticle (incoherent) states to the transport properties is discussed. It is shown that they
can dominate in the temperature dependence of the impurity-induced resistivity and in the tunnel junction conductivity.
Received 16 September 2002 / Received in final form 6 November 2002 Published online 31 December 2002 相似文献
3.
Josephson oscillation of a superfluid Fermi gas 总被引:1,自引:0,他引:1
S. K. Adhikari 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2008,47(3):413-419
Using the complete numerical solution of a time-dependent
three-dimensional mean-field model we
study the Josephson oscillation of a superfluid Fermi gas (SFG) at zero temperature formed in a combined axially-symmetric
harmonic plus one-dimensional periodic optical-lattice (OL) potentials after displacing the harmonic trap along the axial
OL
axis. We study the dependence of Josephson frequency on the strength of the OL potential. The Josephson frequency decreases
with increasing strength as found in the experiment of Cataliotti et al. [Science 293, 843 (2001)] for a Bose-Einstein condensate and of the experiment of Pezzè et al. [Phys. Rev. Lett. 93, 120401 (2004)] for an ideal Fermi gas. We demonstrate a
breakdown of Josephson oscillation in the SFG for a large displacement
of the harmonic trap. These features of Josephson oscillation of a SFG can be tested experimentally. 相似文献
4.
M.L. Chiofalo M. Polini M.P. Tosi 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2000,11(3):371-378
We study the dispersion relation of the excitations of a dilute Bose-Einstein condensate confined in a periodic optical potential
and its Bloch oscillations in an accelerated frame. The problem is reduced to one-dimensionality through a renormalization
of the s-wave scattering length and the solution of the Bogolubov-de Gennes equations is formulated in terms of the appropriate Wannier
functions. Some exact properties of a periodic one-dimensional condensate are easily demonstrated: (i) the lowest band at
positive energy refers to phase modulations of the condensate and has a linear dispersion relation near the Brillouin zone
centre; (ii) the higher bands arise from the superposition of localized excitations with definite phase relationships; and
(iii) the wavenumber-dependent current under a constant force in the semiclassical transport regime vanishes at the zone boundaries.
Early results by Slater [Phys. Rev. 87, 807 (1952)] on a soluble problem in electron energy bands are used to specify the conditions under which the Wannier functions
may be approximated by on-site tight-binding orbitals of harmonic-oscillator form. In this approximation the connections between
the low-lying excitations in a lattice and those in a harmonic well are easily visualized. Analytic results are obtained in
the tight-binding scheme and are illustrated with simple numerical calculations for the dispersion relation and semiclassical
transport in the lowest energy band, at values of the system parameters which are relevant to experiment.
Received 3 December 1999 and Received in final form 22 March 2000 相似文献
5.
M.A. Itskovsky 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,23(3):283-296
Theory of magnetoquantum oscillations with spin-split structure in strongly anisotropic (two-dimensional (2D)) metal is developed
in the formalism of level approach. Parametric method for exact calculation of oscillations wave forms and amplitudes, developed
earlier for spin degenerate levels is generalized on a 2D electron system with spin-split levels. General results are proved:
1) proportionality relation between magnetization and chemical potential oscillations accounting for spin-split energy levels
and magnetic field unperturbed levels (states of reservoir), 2) basic equation for chemical potential oscillations invariant
to various models of 2D and 1D energy bands (intersecting or overlapping) and localized states. Equilibrium transfer of carriers
between overlapping 2D and 1D bands, characterizing the band structure of organic quasi 2D metals, is considered. Transfer
parameter, calculated in this model to be of the order of unity, confirms the fact that the wave form of oscillations in organic metals should be quasisymmetric up to ultralow temperature. Presented theory accounts for spin-split magnetization oscillations at magnetic field directions tilted relative to the anisotropic
axis of a metal. Theoretical results are compared with available experimental data on organic quasi-2D metal α-(BEDT-TTF)2KHg(SNC)4 explaining the appearance of clear split structure under the kink magnetic field and absence above by the corresponding change
in the electron g-factor rather than cyclotron mass.
Received 20 December 2000 and Received in final form 13 July 2001 相似文献
6.
M.V. Moskalets 《The European Physical Journal B - Condensed Matter and Complex Systems》2000,15(3):523-529
The peculiarities of a low temperature heat transfer through a ballistic quantum dot (a double potential barrier) with interacting
leads due to a long-range Coulomb interaction (in the geometrical capacitance approach) are considered. It is found that the
thermal conductance K shows periodic peaks as a function of the electrostatic potential of a dot at low temperatures. At the peak maximum it is
whereas near the minimum it is . Near the peak maximum the dependence K(T) is essentially nonmonotonic at the temperatures correspondent to the level spacing in the quantum dot.
Received 20 October 1999 and Received in final form 20 January 2000 相似文献
7.
Summary The dispersion relations and the shear modulus of the 2D Wigner crystal (WC) in the presence of a strong magnetic field are
evaluated using a density functional method which includes the effect of electronic correlations. Comparison is made with
previous theoretical results on the magnetophonons and the shear modulus. The effect of correlation on the stability of the
crystal is discussed.
In honour of Prof. Fausto Fumi on the occasion of his retirement from teaching. 相似文献
8.
R. Lazzari I. Simonsen D. Bedeaux J. Vlieger J. Jupille 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,24(2):267-284
The light scattering by three-dimensional clusters supported by a substrate is modelled by representing clusters by truncated
spheroids whose polarizability is calculated via a multipolar development of the potential in the quasi-static limit. The determination of the mean island radius, density
and aspect ratio from the optical response is examined. The strong influence of both the particle-substrate interaction and
the particle shape on the optical behaviour is demonstrated, showing the limits of effective medium and dipolar theories.
The Surface Differential Reflectance spectra of silver on MgO(100) and titanium or aluminium on α-Al2O3(0001) surfaces have then been modelled by using the above model, illustrating the capability of optical means to deal with
various metals, including those belonging to transition series. In all cases, it is highlighted that the aspect ratio is central
in modelling the optical response of supported particles.
Received 5 June 2000 and Received in final form 31 July 2001 相似文献
9.
C. Albertus E. Hernández J. Nieves J. M. Verde-Velasco 《The European Physical Journal A - Hadrons and Nuclei》2007,32(2):183-199
We evaluate static properties and semileptonic decays for the ground state of doubly heavy Ξ, Ξ', Ξ
* and Ω, Ω', Ω
* baryons. Working in the framework of a nonrelativistic quark model, we solve the three-body problem by means of a variational
ansatz made possible by heavy-quark spin symmetry constraints. To check the dependence of our results on the inter-quark interaction
we use five different quark-quark potentials that include a confining term plus Coulomb and hyperfine terms coming from one-gluon
exchange. Our results for static properties (masses, charge radii and magnetic moments) are, with a few exceptions for the
magnetic moments, in good agreement with a previous Faddeev calculation. Our much simpler wave functions are used to evaluate
semileptonic decays of doubly heavy Ξ, Ξ'(J = 1/2) and Ω, Ω'(J = 1/2) baryons. Our results for the decay widths are in good agreement with calculations done within a relativistic quark
model in the quark-diquark approximation.
An erratum to this article is available at . 相似文献
10.
N.N. Beletskii Y.V. Bludov 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,29(2):331-334
The paper deals with the theoretical investigation of nonlinear surface polaritons (NSP) in isolated two-dimensional electron
system (2DES) arranged at the interface between linear and nonlinear media and placed into the external quantizing magnetic
field directed perpendicularly to 2DES. We consider that nonlinear medium dielectric permeability depends upon the tangential
component of electric field only. It is shown that under the integer quantum Hall effect conditions all NSP characteristics
are represented by the quantized values. It is found that the NSP spectrum contains two NSP modes - high-frequency and low-frequency
ones. It is shown that the NSP can exist only in the case where the value of tangential component of electric field at the
interface is less than a certain critical value. It is found that the resonant interaction between the NSP high-frequency
mode and surface polariton mode occurs in the vicinity of the cyclotron resonance subharmonic.
Received 23 September 2001 / Received in final form 31 January 2002 Published online 2 October 2002
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ID="a"e-mail: bludov@ire.kharkov.ua 相似文献
11.
I. Bâldea H. Köppel L.S. Cederbaum 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,20(2):289-299
We present a new effect that is possible for strongly correlated electrons in commensurate mesoscopic rings: the collective tunneling of electrons between classically equivalent configurations, corresponding to ordered states possessing charge and
spin density waves (CDW, SDW) and charge separation (CS). Within an extended Hubbard model at half filling studied by exact
numerical diagonalization, we demonstrate that the ground state phase diagram comprises, besides conventional critical lines
separating states characterized by different orderings (e.g. CDW, SDW, CS), critical lines separating phases with the same ordering (e.g. CDW-CDW) but with different symmetries. While the former also exist in infinite systems, the latter are specific for mesoscopic systems and directly related to a collective tunnel effect. We emphasize that, in order to construct correctly
a phase diagram for mesoscopic rings, the examination of CDW, SDW and CS correlation functions alone is not sufficient, and
one should also consider the symmetry of the wave function that cannot be broken. We present examples demonstrating that the
jumps in relevant physical properties at the conventional and new critical lines are of comparable magnitude. These transitions
could be studied experimentally e.g. by optical absorption in mesoscopic systems. Possible candidates are cyclic molecules and ring-like nanostructures of quantum
dots.
Received 27 November 2000 相似文献
12.
Yu.L. Sokolov V.P. Yakovlev V.G. Pal'chikov Yu.A. Pchelin 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2002,18(1):27-36
The properties of two-dimensional magnetic traps for laser-cooled atoms are analysed using complex functions. The two components
of the magnetic field from a series of parallel, infinitely long, current-carrying wires are represented by a single complex
number. The regions of the field where paramagnetic atoms can be trapped occur where the magnetic field is zero. The locations
of the zeroes of the field are obtained as the solution to a polynomial and the multiplicity m of the solution determines both the 2(m + 1)-pole nature of the trap and the field gradient through the centre. The zeroes of the field can be merged or split by
varying the locations of the currents, their strengths or by applying a uniform magnetic field. The theory is applied to magnetic
traps created from long thin wires or permanent magnets on a substrate. The properties of a number of magnetic trap configurations
used for atom guides are discussed.
Received 28 February 2001 and Received in final form 6 July 2001 相似文献
13.
Magnetism in Rh clusters under hydrostatic deformations 总被引:1,自引:0,他引:1
E.O. Berlanga-Ramırez F. Aguilera-Granja A. Dıaz-Ortiz A. Vega 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2003,23(3):343-349
The magnetic behavior of rhodium clusters RhN (N = 4-38) under hydrostatic deformations was investigated. The starting cluster structures were obtained from an evolutionary
search algorithm applied to a Gupta potential. The spin-polarized electronic structure and related magnetic properties were
calculated using a self-consistent spd tight-binding Hamiltonian within the unrestricted Hartree-Fock approximation. The magnetic behavior was analyzed in terms
of the interdependence between the geometrical parameters and the electronic structure. Anomalous magnetic effects were found
in some cases.
Received 5 August 2002 / Received in final form 10 January 2003 Published online 4 March 2003
RID="a"
ID="a"e-mail: berlanga@dec1.ifisica.uaslp.mx 相似文献
14.
M. Raşa D. Bica A. Philipse L. Vékás 《The European physical journal. E, Soft matter》2002,7(3):209-220
The aim of the paper is to study the deviation of magnetic properties of the magnetic fluids prepared for this study, from
ideal (Langevin) behaviour, i.e. to estimate particle interaction influence and dimensions and influence of particle aggregates, as well as to explain the
related effects observed. We also determine the particle coupling parameter, the particle nonmagnetic layer thickness, and
the particle distribution, which are fundamental for sample characterization. A comparison of the studied magnetic fluids
with each other, with respect to microstructure formation and particle interaction strength is finally done. For these purposes,
a concentration dependence study, following the proposed “dilution series approach”, is performed. Three series of dilutions
of three types of magnetic fluids were prepared and analyzed.
Received 27 August 2001 相似文献
15.
C. Hordequin D. Ristoiu L. Ranno J. Pierre 《The European Physical Journal B - Condensed Matter and Complex Systems》2000,16(2):287-293
Magnetism and transport properties of the semi-Heusler compound NiMnSb are re-examined in great details. A wide set of experiments
(elastic and inelastic neutron scattering, static magnetic measurements, magnetoresistance, Hall effect, thermopower, FMR)
have been performed on polycrystals, single crystals or single-crystalline thin films, and the results are analysed. Special
emphasis is given to the magnetic excitations and to the relaxation mechanisms in this metallic ferromagnet. At low temperatures,
all experimental results hint at the existence of a fully spin-polarized conduction band (half metallic state). At higher
temperature (T > 80 K), but well below the Curie temperature (730 K), a cross-over to a usual metallic ferromagnetic state is evidenced
and discussed.
Received 10 January 2000 相似文献
16.
O. Bourgeois P. Gandit J. Lesueur A. Sulpice X. Grison J. Chaussy 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,21(1):75-80
We report transport measurements on Superconductor/Ferromagnet/Superconductor (S/F/S) junctions: Nb/Al/Gd/Al/Nb where gadolinium
(Gd) is a weakly polarized ferromagnet. A sizeable critical current I
c is observed in the I(V) characteristics. This current can be modulated by a weak magnetic field, as expected for a Josephson current. With these
experiments, we establish that superconducting coherent transport survives across a small ferromagnetic layer. The penetration
depth of Cooper pairs in Gd has been measured. An extensive study of the Josephson critical current in temperature for different
thicknesses of magnetic compounds is presented. A comparison of transport measurements with S/N/S junction is given through
measurements made on Nb/Al/Y/Al/Nb, where yttrium (Y) is used as non magnetic rare earth metal.
Received 20 September 2000 and Received in final form 22 February 2001 相似文献
17.
J.L. Ricardo-Chávez G.M. Pastor 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2001,16(1):169-172
The properties of magnetic impurities in small metallic clusters are investigated in the framework of the Anderson model by
using exact diagonalization methods. Parameters representative of the Kondo limit are considered. The spin gap ΔE = E(S=1, 3/2) - E(S=0, 1/2) shows a remarkable band-filling dependence that can be interpreted in terms of the cluster-specific conduction-electron
spectrum. Finite-temperature properties such as the magnetic susceptibility and specific heat are calculated exactly in the
canonical and grand canonical ensembles. The structural dependence is illustrated.
Received 30 November 2000 相似文献
18.
F. Delfino R. Procopio M. Rossi 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,25(1):31-38
The evaluation of the total force of magnetic origin acting upon a body in a stationary magnetic field is often carried out
using the so-called magnetic energy (or co-energy) method, which is based on the derivation of the magnetic energy (or co-energy) with respect to a virtual rigid displacement
of the considered body. The application of this method is usually justified by resorting to the energy conservation principle,
written in terms both of electrical and of mechanical quantities. In this paper we shall re-examine the whole matter in the
context of classical thermodynamics, in order to obtain a more comprehensive and general proof of the validity of the energy
(or co-energy) approach and to point out its limitations. Two typical configurations will be discussed; in the first one,
the field sources are represented by conducting bodies carrying free currents, whereas in the second one a permanent magnet
creates the driving field. All magnetic materials are assumed to be non-hysteretic and permanent magnets are represented by
means of the well-known linear model in the second quadrant of the (B,H) plane.
Received 25 July 2001 and Received in final form 5 November 2001 相似文献
19.
D. Mannix P.C. de Camargo C. Giles A.J.A. de Oliveira F. Yokaichiya C. Vettier 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,20(1):19-25
We report on X-ray magnetic diffraction studies of the spin density wave antiferromagnetism formed in the conduction electron
band of chromium. Non-resonant X-ray magnetic scattering was used to directly determine that chromium has zero orbital magnetisation.
Furthermore, the azimuthal dependence of this scattering provides unique evidence that chromium forms a linearly polarised
wave. In the vicinity of the K absorption edge, resonant X-ray magnetic scattering was observed. A consistent model of the
magnetic scattering has been derived from the resonant and non-resonant magnetic amplitudes. The enhancement of the magnetic
intensity arises primarily from dipole transitions from the core 1s level to 4p states. Quadrupole transitions to the magnetic 3d states are essentially non-existent due to their sensitivity to (and the absence of) orbital moment. This effect is predicted
from atomic considerations of the 3d5 ( = 0) transition metal ions.
Received 22 September 2000 相似文献
20.
A. M. Panich A. I. Shames H.-M. Vieth E. Ōsawa M. Takahashi A. Ya. Vul' 《The European Physical Journal B - Condensed Matter and Complex Systems》2006,52(3):397-402
We report on a nuclear magnetic resonance (NMR) study of
ultrananocrystalline diamond (UNCD) materials produced by detonation
technique. Analysis of the 13C and 1H NMR spectra, spin-spin and
spin-lattice relaxation times in purified UNCD samples is presented. Our
measurements show that UNCD particles consist of a diamond core that is
partially covered by a sp
2-carbon fullerene-like shell. The uncovered
part of outer diamond surface comprises a number of hydrocarbon groups that
saturate the dangling bonds. Our findings are discussed along with recent
calculations of the UNCD structure. Significant increase in the spin-lattice
relaxation rate (in comparison with that of natural diamond), as well as
stretched exponential character of the magnetization recovery, are
attributed to the interaction of nuclear spins with paramagnetic centers
which are likely fabrication-driven dangling bonds with unpaired electrons.
We show that these centers are located mainly at the interface between the
diamond core and shell. 相似文献