共查询到20条相似文献,搜索用时 31 毫秒
1.
C. Masoller F.M. Atay 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2011,62(1):119-126
A network of delay-coupled logistic maps exhibits two different synchronization regimes,
depending on the distribution of the coupling delay times. When the delays are homogeneous
throughout the network, the network synchronizes to a time-dependent state [F.M. Atay, J.
Jost, A. Wende, Phys. Rev. Lett. 92, 144101 (2004)], which may be periodic or
chaotic depending on the delay; when the delays are sufficiently heterogeneous, the
synchronization proceeds to a steady-state, which is unstable for the uncoupled map [C.
Masoller, A.C. Marti, Phys. Rev. Lett. 94, 134102 (2005)]. Here we
characterize the transition from time-dependent to steady-state synchronization as the
width of the delay distribution increases. We also compare the two transitions to
synchronization as the coupling strength increases. We use transition probabilities
calculated via symbolic analysis and ordinal patterns. We find that, as the coupling
strength increases, before the onset of steady-state synchronization the network splits
into two clusters which are in anti-phase relation with each other. On the other hand,
with increasing delay heterogeneity, no cluster formation is seen at the onset of
steady-state synchronization; however, a rather complex unsynchronized state is detected,
revealed by a diversity of transition probabilities in the network nodes. 相似文献
2.
A. Dıaz-Sánchez L.A. Braunstein R.C. Buceta 《The European Physical Journal B - Condensed Matter and Complex Systems》2001,21(2):289-294
The roughening of interfaces moving in inhomogeneous media is investigated by numerical integration of the phenomenological
stochastic differential equation proposed by Kardar, Parisi, and Zhang [Phys. Rev. Lett. 56, 889 (1986)] with quenched noise (QKPZ) [Phys. Rev. Lett. 74, 920 (1995)]. We express the evolution equations for the mean height and the roughness into two contributions: the local
and the lateral one in order to compare them with the local and the lateral contributions obtained for the directed percolation
depinning models (DPD) introduced independently by Tang and Leschhorn [Phys. Rev A 45, R8309 (1992)] and Buldyrev et al. [Phys. Rev A 45, R8313 (1992)]. These models are classified in the same universality class of the QKPZ although the mechanisms of growth
are quite different. In the DPD models the lateral contribution is a coupled effect of the competition between the local growth
and the lateral one. In these models the lateral contribution leads to an increasing of the roughness near the criticality
while in the QKPZ equation this contribution always flattens the roughness.
Received 7 April 2000 and Received in final form 7 March 2001 相似文献
3.
L. Wu S. Zhu Y. Ni 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2007,41(2):349-354
Combination of two basic types of synchronization, anticipatory
synchronization and lagged synchronization, is investigated
numerically between two coupled semiconductor lasers. It is found
that lagged synchronization produced by a backward coupling with a
suitable delay can combine with the originally hidden anticipatory
synchronization and produce a type of synchronization overcoming the
original lagged synchronization produced by a forward coupling. We
study the combination synchronization phenomenon when the delay of
the backward coupling is different from that of the original
anticipatory synchronization. Our results suggest that the
synchronization combination phenomenon might allow an interpretation
of an experimental observation by Sivaprakasam et al. [Phys.
Rev. Lett. 87, 154101 (2001)] that the anticipating time is
irrespective of the external-cavity round trip time, which to date remains to be understood. 相似文献
4.
B. Audoin M. Perton N. Chigarev C. Rossignol 《The European physical journal. Special topics》2008,153(1):235-237
Investigation of thin metallic film properties by means
of picosecond ultrasonics [C. Thomsen et al., Phys. Rev. Lett. 53, 989 (1984)] has been under the scope of several studies.
Generation of longitudinal and shear waves [T. Pézeril et al., Phys. Rev. B 73, 132301 (2006); O. Matsuda et al., Phys. Rev. Lett. 93, 095501 (2004)] with a wave vector normal
to the film free surface has been demonstrated. Such measurements cannot
provide complete information about properties of anisotropic films. Extreme
focusing of a laser pump beam (≈0.5 μm) on the sample surface
has recently allowed us to provide evidence of picosecond acoustic
diffraction in thin metallic films (≈1 μm) [C. Rossignol et al., Phys. Rev. Lett. 94, 166106 (2005)]. The resulting
longitudinal and shear wavefronts propagate at group velocity through the
bulk of the film. To interpret the received signals, source directivity
diagrams are calculated taking into account material anisotropy, optical
penetration, and laser beam width on the sample surface. It is shown that
acoustic diffraction increases with optical penetration, so competing with
the increasing of directivity caused by beam width. Reflection with mode
conversion at the film-substrate interface is discussed. 相似文献
5.
The dynamics of indirectly coupled Lorenz circuits is investigated experimentally. The in-phase and anti-phase synchronization
of indirectly coupled chaotic oscillators reported in Phys. Rev.
E 81, 046216 (2010) is verified by physical experiments with electronic circuits. Two chaotic systems coupled through a common
dynamic environment shows the verity of synchronization behaviours such as anti-phase synchronization, in-phase synchronization,
identical synchronization, anti-synchronization, etc. 相似文献
6.
I. A. Lubashevsky A. Heuer R. Friedrich R. Usmanov 《The European Physical Journal B - Condensed Matter and Complex Systems》2010,78(2):207-216
We consider a previously devised model describing Lévy random walks [I. Lubashevsky, R. Friedrich, A. Heuer, Phys. Rev. E
79, 011110 (2009); I. Lubashevsky, R. Friedrich, A. Heuer, Phys. Rev. E 80, 031148
(2009)]. It is demonstrated numerically that the given model describes Lévy random walks with superdiffusive, ballistic, as
well as superballistic dynamics. Previously only the superdiffusive regime has been analyzed. In this model the walker velocity
is governed by a nonlinear Langevin equation. Analyzing the crossover from small to large time scales we find the time scales
on which the velocity correlations decay and the walker motion essentially exhibits Lévy statistics. Our analysis is based
on the analysis of the geometric means of walker displacements and allows us to tackle probability density functions with
power-law tails and, correspondingly, divergent moments. 相似文献
7.
We propose a scheme for constructing classical spin Hamiltonians from Hunds
coupled spin-fermion models in the limit JH/t →∞. The
strong coupling between fermions and the core spins requires self-consistent
calculation of the effective exchange in the model, either in the presence
of inhomogeneities or with changing temperature. In this paper we establish
the formalism and discuss
results mainly on the “clean” double exchange model,
with self consistently renormalised
couplings, and compare our results with exact simulations.
Our method allows access to system sizes much beyond the reach of exact
simulations, and we can study transport and optical properties of the model
without artificial broadening.
The method discussed here forms the foundation of our papers
[Phys. Rev. Lett. 91, 246602 (2003), and
Phys. Rev. Lett. 92, 126602 (2004)]. 相似文献
8.
We study the Stark effect on doubly excited states of the helium atom below N=2. We present the ab initio photoionization and total inelastic photon scattering cross sections calculated with the method of complex scaling for field strengths F 相似文献
9.
A theoretical explanation is given for the “unexpected” behavior recently observed in the radiation spectrum of ultrarelativistic
electrons in a thin layer of matter in an experimental investigation of the Landau-Pomeranchuk-Migdal effect at SLAC [S. R.
Klein et al., Preprint SLAC-6378, Stanford (1993); P. L. Anthony et al., Phys. Rev. Lett. 75, 1949 (1995)].
Pis’ma Zh. éksp. Teor. Fiz. 63, No. 11, 837–840 (10 June 1996) 相似文献
10.
11.
O. I. Moskalenko A. E. Hramov A. A. Koronovskii A. A. Ovchinnikov 《The European Physical Journal B - Condensed Matter and Complex Systems》2011,82(1):69-82
The influence of noise on the generalized synchronization
regime in the chaotic systems with dissipative coupling is
considered. If attractors of the drive and response systems have an
infinitely large basin of attraction, generalized
synchronization is shown to possess a great stability with
respect to noise. The reasons of the revealed particularity are
explained by means of the modified system approach [A.E. Hramov,
A.A. Koronovskii, Phys. Rev. E 71, 067201 (2005)] and
confirmed by the results of numerical calculations and experimental
studies. The main results are illustrated using the examples of
unidirectionally coupled chaotic oscillators and discrete maps as
well as spatially extended dynamical systems. Different types of the
model noise are analyzed. Possible applications of the revealed
particularity are briefly discussed. 相似文献
12.
Maradudin AA 《Optics letters》2001,26(8):480-481
We show that there is no contradiction between the results presented by Pan [Opt. Lett. 25, 369 (2000)] and the 1/L(2) dependence of the radiative energy flux between two half-spaces separated by a small vacuum gap of width L obtained by Polder and Van Hove [Phys. Rev. B 4, 3303 (1971)] and by Loomis and Maris [Phys. Rev. B 50, 18517 (1994)]. 相似文献
13.
It has recently been claimed that the dynamics
of long-wavelength phason fluctuations has been observed in
i-AlPdMn quasicrystals [S. Francoual et al.
Phys. Rev. Lett. 91, 225501 (2003);
A. Létoublon et al. 54, 753 (2001)]. We will show that
the data reported call for a more detailed development of
the elasticity theory of Jarić and Nelsson [M.V. Jarić and D.R. Nelsson, Phys. Rev. B 37,
4458 (1988)]
in order to determine the nature of small phonon-like atomic displacements
with a symmetry that follows the phason elastic constants.
We also show that a simple model with a single diffusing tile is sufficient
to produce a signal that (1) is situated at a “satellite position”
at a distance q from each Bragg peak; that (2) has an intensity that
scales with the intensity of the corresponding Bragg peak;
(3) falls off as 1/q2; and (4) has a time decay constant that is proportional to 1/Dq2.
It is thus superfluous to call for a picture of “phason waves” in order to explain such data, especially as such “waves” violate
many physical principles. 相似文献
14.
G. De Polsi C. Cabeza A.C. Marti C. Masoller 《The European physical journal. Special topics》2013,222(2):501-510
We propose a novel method of symbolic time-series analysis aimed at characterizing the regular or chaotic dynamics of coupled oscillators. The method is applied to two identical pendulums mounted on a frictionless platform, resembling Huygens’ clocks. Employing a transformation rule inspired in ordinal analysis [C. Bandt and B. Pompe, Phys. Rev. Lett. 88, 174102 (2002)], the dynamics of the coupled system is represented by a sequence of symbols that are determined by the order in which the trajectory of each pendulum intersects an appropriately chosen hyperplane in the phase space. For two coupled pendulums we use four symbols corresponding to the crossings of the vertical axis (at the bottom equilibrium point), either clock-wise or anti-clock wise. The complexity of the motion, quantified in terms of the entropy of the symbolic sequence, is compared with the degree of chaos, quantified in terms of the largest Lyapunov exponent. We demonstrate that the symbolic entropy sheds light into the large variety of different periodic and chaotic motions, with different types synchronization, that cannot be inferred from the Lyapunov analysis. 相似文献
15.
We present a mathematical framework for the theory of a synchronization phenomenon for dynamical systems discovered by Pecora and Carroll [Phys. Rev. Lett. 64, 821-824 (1990)]. From this perspective, we can synchronize, using a single coordinate, an open dense set of linear systems. We use our insights to synchronize nonlinear systems which were not previously recognized as being synchronizable. (c) 1995 American Institute of Physics. 相似文献
16.
We discuss a general mechanism explaining the taming effect of phase disorder in external forces on chaotic solitons in damped, driven, Frenkel-Kontorova chains. We deduce analytically an effective random equation of motion governing the dynamics of the soliton center of mass for which we obtain numerically the regions in the control parameter space where chaotic solitons are suppressed. We find that such predictions are in excellent agreement with results of computer simulations of the original Frenkel-Kontorova chains. We show theoretically how such a fundamental mechanism explains recent numerical results concerning extended chaos in arrays of coupled pendula [S. F. Brandt, Phys. Rev. Lett. 96, 034104 (2006)10.1103/PhysRevLett.96.034104]. 相似文献
17.
We show that a quantum Hall bilayer with the total filling nu = 1 should exhibit a dynamical regime similar to the flux flow in large Josephson junctions. This analogy may explain a conspicuous peak in the interlayer tunneling conductance [Phys. Rev. Lett. 84, 5808 (2000)]. The flux flow is likely to be spatiotemporally chaotic at low-bias voltage, which will manifest itself through broadband noise. The peak position can be controlled by an in-plane magnetic field. 相似文献
18.
<正>The influence of parameter mismatches on multirhythmic patterns in chains of coupled Rossler circuits are explored experimentally.The parameter mismatches in coupled chaotic oscillators are found to help form a kind of multirhythmic pattern as reported in chains of biological coupled oscillators[Phys.Rev.Lett.92 228102].Moreover,a new type of multirhythmic pattern based on the envelope of time series is observed. 相似文献
19.
Recently, a scheme based on the method of weak measurements to register the trajectories of photons passing through a nested Mach–Zehnder interferometer was proposed [L. Vaidman, Phys. Rev. A 87, 052104 (2013)] and then realized [A. Danan, D. Farfurnik, S. Bar-Ad, et al., Phys. Rev. Lett. 111, 240402 (2013)]. Interpreting the results of the experiment, the authors concluded that “the photons do not always follow continuous trajectories.” It is shown in this work that these results can be easily and clearly explained in terms of traditional classical electrodynamics or quantum mechanics implying the continuity of all possible paths of photons. Consequently, a new concept of disconnected trajectories proposed by the authors of work [Phys. Rev. Lett. 111, 240402 (2013)] is unnecessary. 相似文献
20.
We develop a scheme to exactly evaluate the correlation energy in the random-phase approximation, based on linear response theory [Y. R. Shimizu, J. D. Garrett, R. A. Broglia, M. Gallardo, and E. Vigezzi, Rev. Mod. Phys. 61, 131 (1989)]. It is demonstrated that our formula is equivalent to a contour integral representation recently proposed [F. Donau, D. Almehed, and R. G. Nazmitdinov, Phys. Rev. Lett. 83, 280 (1999)] being numerically more efficient for realistic calculations. Examples are presented for pairing correlations in rapidly rotating nuclei. 相似文献