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1.
It is argued that the Hall resistance of macroscopic samples can be directly obtained by ensemble averaged transport properties of mesoscopic systems. The resulting formula relates the Hall current to the part of the magnetic moment of Fermi electrons, which originates in macroscopic currents only. As one of the possible application the Hall resistance of the periodically modulated two-dimensional electron system in the strong magnetic field is briefly discussed. 相似文献
2.
K. Pomorski K. Dietrich 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》1998,4(3):353-364
We investigate the existence of stable charged metallic bubbles using the shell correction method. We find that for a given
mesoscopic system of n atoms of a given metal and (positive) elementary charges, a metallic bubble turns out to have a lower total energy than a compact spherical cluster,
whenever the charge number q is larger than a critical charge number qc. For a magic number (n-q) of free electrons, the spherical metallic bubble may become stable against fission.
Received: 17 November 1997 / Revised: 28 May 1998 / Accepted: 20 July 1998 相似文献
3.
Ying-Hua Ji 《Physics letters. A》2008,372(21):3874-3877
Taking into account the interactions between electrons and phonons, we study the dynamic behavior of a dissipative mesoscopic circuit for pure initial coherent state of phonon bath modes by virtue of the IWOP technique. It shows that if the bath modes are initially in coherent states, some phenomena like Brownian behavior will appear in mean charge and current of the mesoscopic circuit. The quantum fluctuations of charge and current are constant and irrelevant to the coupled coefficients between electrons and phonons. 相似文献
4.
A.A. Zvyagin 《The European Physical Journal B - Condensed Matter and Complex Systems》2003,32(3):351-360
The behavior of charge and spin persistent currents in an integrable lattice ring of strongly correlated electrons with a
magnetic impurity is exactly studied. Our results manifest that the oscillations of charge and spin persistent currents are
similar to the ones, earlier obtained for integrable continuum models with a magnetic impurity. The difference is due to two
(instead of one) Fermi velocities of low-lying excitations. The form of oscillations in the ground state is “saw-tooth”-like,
generic for any multi-particle coherent one-dimensional models. The integrable magnetic impurity introduces net charge and
spin chiralities in the generic integrable lattice system, which determine the initial phase shifts of charge and spin persistent
currents. We show that the magnitude of the charge persistent current in the generic Kondo situation does not depend on the
parameters of the magnetic impurity, unlike the (magneto)resistivity of transport currents.
Received 30 January 2003 / Received in final form 12 March 2003 Published online 11 April 2003
RID="a"
ID="a"e-mail: zvyagin@fy.chalmers.se 相似文献
5.
V. F. Elesin 《Journal of Experimental and Theoretical Physics》1997,85(2):264-271
A theory is developed for steady-state single-mode lasing in coherent quantum-well cascade lasers. This laser model is an
example of a strictly quantum mechanical problem in which approximate kinetic approaches are not used to account for dissipative
scattering processes. Exact wave functions are found for the system in weak and strong electromagnetic fields, so that the
output power and frequency can be determined as functions of the coherent pump current and system parameters. It is shown
that for pumping by monoenergetic electrons the power has a nonlinear (root) dependence and tends to saturate in strong fields.
It is predicted that the coherent pumping efficiency may be increased by adjusting the energy of the pump electrons, which
will lead to a linear power dependence, a high efficiency, and low threshold currents. A population inversion is found not
be a necessary condition for lasing in the coherent laser. In particular, in the high field regime the population of the lower
level exceeds that of the upper, while in the optimally adjusted regime they are the same.
Zh. éksp. Teor. Fiz. 112, 483–498 (August 1997) 相似文献
6.
S. A. Jafari 《The European Physical Journal B - Condensed Matter and Complex Systems》2009,68(4):537-542
Renormalization is one of the basic notions of condensed matter physics. Based on the concept of renormalization, the Landau’s
Fermi liquid theory has been able to explain, why despite the presence of Coulomb interactions, the free electron theory works so well
for simple metals with extended Fermi surface (FS). The recent synthesis of graphene has provided the condensed matter physicists
with a low energy laboratory of Dirac fermions where instead of a FS, one has two Fermi points. Many exciting phenomena in
graphene can be successfully interpreted in terms of free Dirac electrons. In this paper, employing dynamical mean field theory
(DMFT), we show that an interacting Dirac sea is essentially an effective free Dirac theory. This observation suggests the
notion of Dirac liquid as a fixed point of interacting 2 + 1 dimensional Dirac fermions. We find one more fixed point at strong interactions describing
a Mott insulating state, and address the nature of semi-metal to insulator (SMIT) transition in this system. 相似文献
7.
A.K. Hüttel S. Ludwig K. Eberl J.P. Kotthaus 《Physica E: Low-dimensional Systems and Nanostructures》2006,35(2):278
Semiconductor quantum dots, so-called artificial atoms, have attracted considerable interest as mesoscopic model systems and prospective building blocks of the “quantum computer”. Electrons are trapped locally in quantum dots, forming controllable and coherent mesoscopic atom- and moleculelike systems. Electrostatic definition of quantum dots by use of top gates on a GaAs/AlGaAs heterostructure allows wide variation of the potential in the underlying two-dimensional electron gas. By distorting the trapping potential of a single quantum dot, a strongly tunnel-coupled double quantum dot can be defined. Transport spectroscopy measurements on such a system charged with N=0,1,2,… electrons are presented. In particular, the tunnel splitting of the double well potential for up to one trapped electron is unambiguously identified. It becomes visible as a pronounced level anticrossing at finite source drain voltage. A magnetic field perpendicular to the two-dimensional electron gas also modulates the orbital excitation energies in each individual dot. By tuning the asymmetry of the double well potential at finite magnetic field the chemical potentials of an excited state of one of the quantum dots and the ground state of the other quantum dot can be aligned, resulting in a second level anticrossing with a larger tunnel splitting. In addition, data on the two-electron transport spectrum are presented. 相似文献
8.
P. Nozières 《The European Physical Journal B - Condensed Matter and Complex Systems》1998,4(4):447-457
The so called exhaustion problem occurs when few electrons have to screen many spins in a metal with magnetic impurities.
A singlet Fermi liquid ground state is possible only if all impurities are “isotropized” in such a way as to suppress their
entropy. That takes a time and the corresponding energy limits the Fermi liquid range. The present note explores that issue of time and energy scales, and it concludes that is much smaller than the single impurity Kondo temperature. Similarly the relevant energy scale is proportional to the number
of electrons. Recent results on the Mott metal insulator transition in infinite dimension are reconsidered in the light of
these results: controversies in that respect are shown to reduce to a simple physical question, with no firm answer as to
now.
Received: 5 May 1998 / Received in final form and Accepted: 29 July 1998 相似文献
9.
This paper studies the quantum dynamics of electrons in a surface
quantum well in the time domain with autocorrelation of wave packet.
The evolution of the wave packet for different manifold eigenstates with
finite and infinite lifetimes is investigated analytically. It is
found that the quantum coherence and evolution of the surface electronic
wave packet can be controlled by the laser central energy and
electric field. The results show that the finite lifetime of excited
states expedites the dephasing of the coherent electronic wave
packet significantly. The correspondence between classical and
quantum mechanics is shown explicitly in the system. 相似文献
10.
Transmission resonances in magnetic-barrier structures 总被引:1,自引:0,他引:1
Y. Guo Z.-Q. Li B.-L. Gu Q. Sun J.-Z. Yu Y. Kawazoe 《The European Physical Journal B - Condensed Matter and Complex Systems》1998,3(2):263-270
Quantum transport properties of electrons in simple magnetic-barrier (MB) structures and in finite MB superlattices are investigated
in detail. It is shown that there exists a transition of transmission resonances, i.e., from incomplete transmission resonances in simple MB structures consisting of unidentical blocks, to complete transmission
resonances in comparatively complex MB structures (, n is the number of barriers). In simple unidentical block arrangements in double- and triple-MB structures we can also obtain
complete transmission by properly adjusting parameters of the building blocks according to ky-value (ky is the wave vector in y direction). Strong suppression of the transmission and of the conductance is found in MB superlattices which are periodic
arrangements of two different blocks. The resonance splitting effect in finite MB superlattices is examined. It is confirmed
that the rule (i.e., for n-barrier tunneling the splitting would be (n-1)-fold) obtained in periodic electric superlattices can be extended to periodically arranged MB superlattices of identical
blocks through which electrons with tunnel, and it is no longer proper for electrons with k
y
<0 to tunnel.
Received: 18 August 1997 / Revised: 20 September 1997 / Accepted: 13 October 1997 相似文献
11.
Yu Li R.W. Peng G.J. Jin Mu Wang X.Q. Huang A. Hu S.S. Jiang 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,25(4):497-503
In the tight-binding approximation, we have investigated the behaviour of persistent currents in a one-dimensional Thue-Morse
mesoscopic ring threaded by a magnetic flux. By applying a transfer-matrix technique, the energy spectra and the persistent
currents in the system have been numerically calculated. It is shown that the flux-dependent eigenenergies form “band” structures
and the energy gaps will enlarge if the site energy increases. Actually, the site energy and the filling-up number of electrons
are two important factors which have much influence upon the persistent current. Increment of the site energy in the system
will lead to a dramatic suppression of the currents. When the highest-occupied energy level is on the top of the band, the
total current is limited; otherwise, the persistent current increases by several orders of magnitude. Generally, this kind
of large scale change in the magnitude of the current can easily be observed in the vicinity of band gaps. The parity effect
in the Thue-Morse ring is also discussed.
Received 22 January 2001 and Received in final form 25 October 2001 相似文献
12.
L. Brossard R. Clerac C. Coulon M. Tokumoto T. Ziman D.K. Petrov V.N. Laukhin M.J. Naughton A. Audouard F. Goze A. Kobayashi H. Kobayashi P. Cassoux 《The European Physical Journal B - Condensed Matter and Complex Systems》1998,1(4):439-452
In order to understand the magnetic field-induced restoration of a highly conductive state in , static (SQUID) and dynamic (ESR and AFR) magnetization measurements were performed on polycrystalline samples and single
crystals, respectively. In addition, cantilever and resistivity measurements under steady fields were performed. While the
metal-insulator transition curve of the () phase diagram exhibits a first order character, a “spin-flop” transition line divides the insulating state when the magnetic
field is applied along the easy axis of magnetization. The effects of a RKKY-type indirect exchange and of applied magnetic
field are described within the framework of a generalized Kondo lattice, namely two chains of localised spins coupled through the itinerant spins of the 2D sheets of BETS. The calculations, which can incorporate intramolecular
electron correlations within a mean field theory, are in qualitative agreement with the field induced transition from the
antiferromagnetic insulating ground state to a canted one, i.e. a not fully oriented paramagnetic, but metallic state.
Received: 6 August 1997 / Received: 5 November 1997 / Accepted: 10 November 1997 相似文献
13.
基于介观体系电子动态输运的自洽理论,讨论了介观结构的动态电导.作为该理论的应用,采用一介观相干平行板电容器模型来进行研究. 结果表明:体系的动态电导与外场频率和体系费米能有关,为一复数且有有限虚部. 当外场频率较小时,动态电导随费米能的变化所呈现的特性和直流情形非常相似,但是随着外场频率的增加,两者差异就变得非常明显,体系动态电导随外场频率的变化呈现一些峰值结构. 在给定体系费米能时,动态电导随着外场频率的变化而产生振荡,并且出现了负的电导虚部,电导虚部的正负表明了体系的电容特性和电感特性.
关键词:
自洽输运理论
相干平行板电容器
电导
介观体系 相似文献
14.
W. Apel H.-U. Everts U. Körner 《The European Physical Journal B - Condensed Matter and Complex Systems》1998,5(3):317-324
A coherent state representation for the electrons of ordered antiferromagnets is used to derive effective Hamiltonians for
the dynamics of holes in such systems. By an appropriate choice of these states, the constraint of forbidden double occupancy
can be implemented rigorously. Using these coherent states, one arrives at a path integral representation of the partition
function of the systems, from which the effective Hamiltonians can be read off. We apply this method to the t-J model on the square lattice and on the triangular lattice. In the former case, we reproduce the well-known fermion-boson
Hamiltonian for a hole in a collinear antiferromagnet. We demonstrate that our method also works for non-collinear antiferromagnets
by calculating the spectrum of a hole in the triangular antiferromagnet in the self-consistent Born approximation and by comparing
it with numerically exact results.
Received: 23 December 1997 / Accepted: 17 March 1998 相似文献
15.
M. Henkel D. Karevski 《The European Physical Journal B - Condensed Matter and Complex Systems》1998,5(3):787-792
The effect of point defects on persistent currents in mesoscopic rings is studied in a simple tight-binding model. Using an
analogy with the treatment of the critical quantum Ising chain with defects, conformal invariance techniques are employed
to relate the persistent current amplitude to the Hamiltonian spectrum just above the Fermi energy. From this, the dependence
of the current on the magnetic flux is found exactly for a ring with one or two point defects. The effect of an aperiodic
modulation of the ring, generated through a binary substitution sequence, on the persistent current is also studied. The flux-dependence
of the current is found to vary remarkably between the Fibonacci and the Thue-Morse sequences.
Received: 4 March 1998 / Revised: 20 April 1998 / Accepted: 30 April 1998 相似文献
16.
P. Sharma 《Journal of Experimental and Theoretical Physics》2018,126(2):201-209
I discuss heat and momentum transport in a mesoscopic film of 3He, confined by rough walls in the normal Fermi liquid state. Inelastic binary quasiparticle scattering mediated by elastic scattering from the surface roughness gives rise to a coherent “mixed” scattering channel that drives anomalous transport over a range of temperature. I calculate the thermal conductivity and viscosity of the film in this regime and derive these in terms of the film thickness and autocorrelation function of the surface roughness, which enters the formulation as an independent input. This calculation can be useful in understanding and isolating the effects of confinement and surface roughness, especially in the context of exploring the superfluid state in the film. 相似文献
17.
R. Egger A.O. Gogolin 《The European Physical Journal B - Condensed Matter and Complex Systems》1998,3(3):281-300
We derive the effective low-energy theory for single-wall carbon nanotubes including the Coulomb interactions among electrons.
The generic model found here consists of two spin-fermion chains which are coupled by the interaction. We analyze the theory using bosonization, renormalization-group techniques,
and Majorana refermionization. Several experimentally relevant consequences of the breakdown of Fermi liquid theory observed
here are discussed in detail, e.g., magnetic instabilities, anomalous conductance laws, and impurity screening profiles.
Received: 12 December 1997 / Revised: 9 March 1998 / Accepted: 12 March 1998 相似文献
18.
A new interpretation of light-induced magnetization changes of a magnetic semiconductor, manganese arsenide (MnAs), observed
by the authors of references [1,2], is proposed in this paper. Contrary to references [1,2], where the results of experiments
were interpreted as the observation of light-induced phase transition, here we propose a completely different approach. It
suggests that at least far from the vicinity of T
c, there are no real magnetization changes as in case of phase transition, but there are changes of the magnetic flux threading
the MnAs-sample. These changes are due to non-equilibrium light-induced diamagnetic moments of quasi-free electrons of narrow
d-subbands of the MnAs-conduction band. The other aspects of the experiments of [1,2] are also discussed and some similarity
between this effect and the orbital diamgnetism due to persistent currents in mesoscopic structures is emphasised.
Received 7 November 2000 相似文献
19.
Shi-Biao Zheng Guang-Can Guo 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》1998,1(1):105-107
We propose a method for preparing superpositions of coherent states of the motion of an ion in an anisotropic two-dimensional
trap, in which the ion is tightly bound in the y direction. In the scheme the ion is excited by two resonant laser beams with equal amplitude, propagating along the x and y directions, respectively. In the Dicke-Lamb limit, an initial coherent state of the ion motion can be converted into a superposition
of several coherent states on a circle through the laser-ion interactions and state-selective measurements on the ion.
Received: 30 May 1997 / Revised: 29 July 1997 / Accepted: 22 October 1997 相似文献
20.
The interaction of magnetostatic waves with charge carriers in ferrite-semiconductor and ferrite-electron flux structures is reviewed. The basic equations needed to calculate the interaction effects in these structures are provided. Attention is turned to the possibility of amplifying fast magnetostatic waves in bodies of revolution by means of circular electron drift over the body surface. The possibility is discussed of amplifying magnetostatic waves in a ferrite film by an electron flux band. The interaction of magnetoelastic waves with electrons in ferrite-semiconductor structures is considered. A method of calculating the static EMF (electromotive force), induced by traveling MSW (magnetostatic waves) in a ferrite-semiconductor structure, is discussed. Attention is turned to circular currents, flowing in the semiconductor, which can vary substantially the longitudinal EMF and lead to generation of a transverse EMF in the structure. We discuss experimental studies on detection of interaction of magnetostatic waves with charge carriers, suggesting the possibility of wave amplification in ferrite-semiconductor and ferrite-electron flux structures, and exploring EMF induction mechanisms in the regime of traveling waves and ferromagnetic resonance.Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 1, pp. 5–29, January, 1989. 相似文献