共查询到20条相似文献,搜索用时 15 毫秒
1.
T. Vaz Martins R. Toral M. A. Santos 《The European Physical Journal B - Condensed Matter and Complex Systems》2009,67(3):329-336
We study an Ising model in a network with disorder induced by the presence of both attractive and repulsive links and subjected
to a periodic subthreshold signal. By means of numerical simulations and analytical calculations we give evidence that the
global response of the system reaches a maximum value for a given fraction of the number of repulsive interactions. The model
can represent a network of spin-like neurons with excitatory and inhibitory couplings, or a simple opinion spreading model.
In this context, attractive/repulsive links represent friends and enemies. “Divide and Conquer” refers to the fact that in
order to force a society to adopt a new point of view, it helps to break its homogeneity by fostering enmities amongst its
members. 相似文献
2.
A. Fiasconaro W. Ebeling E. Gudowska-Nowak 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,65(3):403-414
We give an overview over recent studies on the model of Active Brownian Motion (ABM) coupled to reservoirs providing free
energy which may be converted into kinetic energy of motion. First, we present an introduction to a general concept of active
Brownian particles which are capable to take up energy from the source and transform part of it in order to perform various
activities. In the second part of our presentation we consider applications of ABM to ratchet systems with different forms
of differentiable potentials. Both analytical and numerical evaluations are discussed for three cases of sinusoidal, staircaselike
and Mateos ratchet potentials, also with the additional loads modelled by tilted potential structure. In addition, stochastic
character of the kinetics is investigated by considering perturbation by Gaussian white noise which is shown to be responsible
for driving the directionality of the asymptotic flux in the ratchet. This stochastically driven directionality effect is visualized as a strong nonmonotonic dependence of the statistics of the right versus left trajectories of motion
leading to a net current of particles. Possible applications of the ratchet systems to molecular motors are also briefly discussed. 相似文献
3.
Y. Liu Z-Y. Sun L-J. An 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,62(4):481-484
Banded spherulite patterns are simulated in two dimensions by means of a
coupled logistic map lattice model. Both target pattern and spiral pattern
which have been proved to be existent experimentally in banded spherulite
are obtained by choosing suitable parameters in the model. The simulation
results also indicate that the band spacing is decreased with the increase
of parameter μ in the logistic map and increased with the increase of
the coupling parameter ε, which is quite similar to the results
in some experiments. Moreover, the relationship between the parameters and
the corresponding patterns is obtained, and the target patterns and spiral
patterns are distinguished for a given group of initial values, which may
guide the study of banded spherulite. 相似文献
4.
T. Carletti D. Fanelli A. Guarino F. Bagnoli A. Guazzini 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,64(2):285-292
We here discuss the process of opinion formation in an open community where agents are made to interact and consequently update
their beliefs. New actors (birth) are assumed to replace individuals that abandon the community (deaths). This dynamics is
simulated in the framework of a simplified model that accounts for mutual affinity between agents. A rich phenomenology is
presented and discussed with reference to the original (closed group) setting. Numerical findings are supported by analytical
calculations. 相似文献
5.
V. A. Benderskii E. I. Kats 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2009,54(3):597-605
We investigate the time evolution process of one selected (initially prepared by optical pumping) vibrational molecular state
S, coupled to all other intra-molecular vibrational states R of the same molecule, and also to its environment Q. Molecular
states forming the first reservoir R are characterized by a discrete dense spectrum, whereas the environment reservoir Q states
form a continuous spectrum. Assuming the equidistant reservoir R states we find the exact analytical solution of the quantum
dynamic equations. S-Q and R-Q couplings yield to spontaneous decay of the S and R states, whereas S-R exchange leads to recurrence
cycles and Loschmidt echo at frequencies of S-R transitions and double resonances at the interlevel reservoir R transitions.
Due to these couplings the system S time evolution is not reduced to a simple exponential relaxation. We predict various regimes
of the system S dynamics, ranging from exponential decay to irregular damped oscillations. Namely, we show that there are
possible four dynamic regimes of the evolution: (i) independent of the environment Q exponential decay suppressing backward
R - S transitions, (ii) Loschmidt echo regime, (iii) incoherent dynamics with multicomponent Loschmidt echo, when the system
state is exchanged its energy with many states of the reservoir, (iv) cycle mixing regime, when long time system dynamics
looks as a random-like. We suggest applications of our results for interpretation of femtosecond vibration spectra of large
molecules and nano-systems. 相似文献
6.
Y.-C. Lai K. Park L. Rajagopalan 《The European Physical Journal B - Condensed Matter and Complex Systems》2009,69(1):65-70
We investigate a class of nonlinear wave equations subject to
periodic forcing and noise, and address the issue of energy optimization.
Numerically, we use a pseudo-spectral method to solve the nonlinear stochastic
partial differential equation and compute the energy of the system as a
function of the driving amplitude in the presence of noise.
In the fairly general setting where the system possesses two coexisting
states, one with low and another with high energy, noise can induce
intermittent switchings between the two states. A striking finding is that,
for fixed noise, the system energy can be optimized by the driving in a
form of resonance. The phenomenon can be explained by the Langevin dynamics
of particle motion in a double-well potential system with symmetry breaking.
The finding can have applications to small-size devices such as
microelectromechanical resonators and to waves in fluid and plasma. 相似文献
7.
J. Ma Z. H. Hou H. W. Xin 《The European Physical Journal B - Condensed Matter and Complex Systems》2009,69(1):101-107
We study the effect of recycled noise, generated by the superposition of a
primary Gaussian noise source with a second component of constant delay, in
a parameter region below the threshold of supercritical Hopf bifurcation, by
focussing on the performance of noise induced oscillations and coherence
resonance. For fixed noise intensity, the amplitude and signal-to-noise
ratio of the oscillation show periodic dependences on the delay time. The
optimal noise intensity for the occurrence of coherence resonance also shows
a periodic dependence on the delay. A theoretical analysis based on the
stochastic normal form theory is presented, which qualitatively reproduces
the simulation results with good agreement. This work presents a possible
strategy for controlling noise induced oscillations and coherence resonance
by deliberately adjusting the parameters of the recycled noise. 相似文献
8.
A. Shabunin A. Efimov 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,65(3):387-393
A spatio-temporal process in the Lattice Lotka Volterra (LLV) model, when realized on low dimensional support, is studied.
It is shown that the introduction of a long-range mixing causes a drastic change in the system’s behavior, which transits
from small random-like fluctuations to global oscillations when the mixing rate transcends above a critical point. The amplitude
of the induced oscillations is well defined by the mixing rate and is insensitive to the initial conditions and the lattice
size variations. The observed behavior essentially differs from that predicted by the Mean-Field model which is conservative.
The oscillations are of limit-cycle type and appear as a stochastic analog of a Hopf bifurcation. 相似文献
9.
A. A. Rybakov E. D. Belega D. N. Trubnikov 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2007,41(2):297-302
The dependence of the internal dynamics of triatomic van der Waals
clusters on the rate of nonrigid rotation has been studied. The method of
decomposition of the system's motion into orthogonal modes of the motion has
been proposed. Additionally, a new method of separation of the kinetic energy,
captured by the modes, into rotational and vibrational components has been
developed. It has been found that the most significant factor for the chaotic
behavior of the cluster is the partitioning of the vibrational and rotational
energies among the modes. 相似文献
10.
A. A. Koronovskii A. E. Hramov 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,62(4):447-452
We consider a type of intermittent behavior that occurs
as the result of the interplay between dynamical mechanisms giving
rise to type-II intermittency and random dynamics. We analytically
deduce the law for the distribution of the laminar phases, which has
never been obtained hitherto. The already known dependence of the
mean length of the laminar phases on the criticality parameter [Phys. Rev. E
68, 036203 (2003)] follows as a corollary of the carried out
research. We also prove that this dependence obtained earlier under
the assumption of the fixed form of the reinjection probability does
not depend on the relaminarization properties, and, correspondingly,
the obtained expression of the mean length of the laminar phases on
the criticality parameter remains
correct for different types of the reinjection probability. 相似文献
11.
M. Agop P. E. Nica P. D. Ioannou A. Antici V. P. Paun 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2008,49(2):239-248
The scale relativity model was extended for the motions on fractal curves of fractal dimension D F and third order terms in the equation of motion of a complex speed field. It results that, in a fractal fluid, the convection, dissipation and dispersion are compensating at any scale (differentiable or non-differentiable), whereas a generalized Schrödinger type equation is obtained for an irrotational movement of the fractal fluid. For D F = 2 and the dissipative approximation of the motions, the fractal model of atom is build: the real part of the complex speed field describes the electron motion on stationary orbits according to a quantification condition, while the imaginary part of the complex speed field gives the electron energy quantification. For D F = 3 and the dispersive approximation of motions, some properties of the matter are explained: at the differentiable scale the flowing regimes (non-quasi-autonomous and quasi-autonomous) of the fractal fluids are separated by the experimental “0.7 structure”, while for the non-differentiable scale the fractal potential acts as an energy accumulator and controls through coherence the transport phenomena. Moreover, the compatibility between the differentiable and non-differentiable scales implies a Cantor space-time, and consequently a fractal at any scale. Thus, some properties of the matter (the anomaly of nano-fluids thermal conductivity, the superconductivity etc.) can be explained by this model. 相似文献
12.
J. P. Salas 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2007,41(1):95-102
In this paper, we present the study of the global classical dynamics of a rigid diatomic molecule in the presence of combined
electrostatic and nonresonant polarized laser fields. In particular, we focus on the collinear field case, which is an integrable
system because the z-component Pφ of the angular momentum is conserved. The study involves the complete analysis of the stability of the equilibrium points,
their bifurcations and the evolution of the phase flow as a function of the field strengths and Pφ. Finally, the influence of the bifurcations on the orientation of the quantum states is studied. 相似文献
13.
D. Valenti G. Augello B. Spagnolo 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,65(3):443-451
We analyze the dynamics of the FitzHugh-Nagumo (FHN) model in the presence of colored noise and a periodic signal. Two cases
are considered: (i) the dynamics of the membrane potential is affected by the noise, (ii) the slow dynamics of the recovery
variable is subject to noise. We investigate the role of the colored noise on the neuron dynamics by the mean response time
(MRT) of the neuron. We find meaningful modifications of the resonant activation (RA) and noise enhanced stability (NES) phenomena
due to the correlation time of the noise. For strongly correlated noise we observe suppression of NES effect and persistence
of RA phenomenon, with an efficiency enhancement of the neuronal response. Finally we show that the self-correlation of the
colored noise causes a reduction of the effective noise intensity, which appears as a rescaling of the fluctuations affecting
the FHN system. 相似文献
14.
G. Ruiz C. Tsallis 《The European Physical Journal B - Condensed Matter and Complex Systems》2009,67(4):577-584
We introduce a new universality class of one-dimensional unimodal dissipative maps. The new family, from now on referred to
as the (z1, z2)-logarithmic map,
corresponds to a generalization of the z-logistic map. The
Feigenbaum-like constants of these maps are determined.
It has been recently shown that the probability density of sums of iterates at the edge of chaos of the z-logistic map is
numerically consistent with a q-Gaussian, the distribution which, under appropriate constraints, optimizes the nonadditive
entropy Sq. We focus here on the presently generalized maps to check whether they constitute a new universality class with regard to
q-Gaussian attractor distributions.
We also study the generalized q-entropy production per unit time on the new unimodal dissipative maps, both for strong
and weak
chaotic cases. The q-sensitivity indices are obtained as well.
Our results are, like those for the z-logistic maps, numerically compatible with the q-generalization of a Pesin-like identity
for ensemble averages. 相似文献
15.
We present a basic model for an instability leading to a novel type of electroconvection patterns observed above the splay Fréedericksz transition in nematics. Such patterns, with wave vector perpendicular to the director easy axis, are found in planar sandwich cells under crossed polarizers, they do not produce shadowgraph images at onset. An adaptation of the classical Carr Helfrich mechanism is introduced. The ground state is a tilted director field uniform in the cell plane. The proposed mechanism destabilizes this director field and leads to a structure with modulated out-of-plane (twist) deformations. Experimental confirmation is provided by polarizing microscopy. All experimental observations are qualitatively explained with the proposed model. 相似文献
16.
P. H. Chavanis L. Delfini 《The European Physical Journal B - Condensed Matter and Complex Systems》2009,69(3):389-429
We apply the Nyquist method to the Hamiltonian mean field (HMF) model in order to settle the linear dynamical stability of
a spatially homogeneous distribution function with respect to the
Vlasov equation. We consider the case of Maxwell (isothermal) and Tsallis (polytropic) distributions and show that the system
is stable above a critical kinetic temperature Tc and unstable below it. Then, we consider a symmetric double-humped distribution, made of the superposition of two decentered
Maxwellians, and show the existence of a re-entrant phase in the stability diagram. When we consider an asymmetric double-humped
distribution, the re-entrant phase disappears above a
critical value of the asymmetry factor Δ > 1.09. We also consider the HMF model with a repulsive interaction. In that case,
single-humped distributions are always stable. For asymmetric double-humped distributions, there is a re-entrant phase for
1 ≤ Δ < 25.6, a double re-entrant phase for 25.6 < Δ < 43.9 and no re-entrant phase for Δ > 43.9. Finally, we extend our results
to arbitrary potentials of interaction and mention the connexion between the HMF model, Coulombian plasmas and gravitational
systems. We discuss the relation between linear dynamical stability and formal nonlinear dynamical stability and show their
equivalence for spatially
homogeneous distributions. We also provide a criterion of dynamical stability for spatially inhomogeneous systems. 相似文献
17.
The transverse energy distribution in ultra-relativistic heavy-ion collisions has been obtained as a convolution over the number of projectile and target participants. The latter is computed using the geometrical overlap model as a function of impact parameter. The data from 10 A GeV to 200 A GeV heavy ion beams on various targets in different pseudo-rapidity domains have been successfully described. 相似文献
18.
P. H. Chavanis 《The European Physical Journal B - Condensed Matter and Complex Systems》2007,57(4):391-409
We derive the exact expression of the diffusion
coefficient of a self-gravitating Brownian gas in two
dimensions. Our formula generalizes the usual Einstein relation for
a free Brownian motion to the context of two-dimensional gravity. We
show the existence of a critical temperature Tc at which the
diffusion coefficient vanishes. For T < Tc, the diffusion
coefficient is negative and the gas undergoes gravitational
collapse. This leads to the formation of a Dirac peak concentrating
the whole mass in a finite time. We also stress that the critical
temperature Tc is different from the collapse temperature
T* at which the partition function diverges. These quantities
differ by a factor 1-1/N where N is the number of particles in
the system. We provide clear evidence of this difference by
explicitly solving the case N = 2. We also mention the analogy with
the chemotactic aggregation of bacteria in biology, the formation
of “atoms” in a two-dimensional (2D) plasma and the formation of
dipoles or “supervortices” in 2D point vortex dynamics. 相似文献
19.
M. K. Hossain Y. Kitahama G. G. Huang T. Kaneko Y. Ozaki 《Applied physics. B, Lasers and optics》2008,93(1):165-170
In this study, surface plasmon resonance (SPR) and surface-enhanced Raman scattering (SERS) characteristics of gold nanoaggregates
with different morphologies are examined to elucidate the correlation between SPR and SERS of the object. Nanoaggregates,
defined as random aggregates (hereafter RA), elongated aggregates (hereafter EA) and two-dimensional layered aggregates (hereafter
2DLA) are fabricated by immobilizing colloidal gold nanoparticles on glass substrates. The color variation observed in the
RA and EA samples indicates the variation in localized SPR excitations excited on the samples. The RA sample mostly shows
a broadened and shifted SPR peak centered at 570 nm in addition to another peak in the longer wavelength region (∼700 nm),
whereas in the EA sample a weak blue-shifted peak is observed near 450 nm in addition to a broadened peak centered at 570 nm
covering a trail for another one near 700 nm. In the case of the 2DLA sample, more than one SPR peaks are observed in the
longer wavelength region. The SERS observation confirms million times higher enhancement at least in Raman intensity using
the gold nanoaggregates adsorbed by dye molecules. The EA sample of gold nanoparticles shows ∼5 times higher enhancement in
Raman signal compared to that of the RA and 2DLA sample. 相似文献
20.
C. J. Tessone D. H. Zanette R. Toral 《The European Physical Journal B - Condensed Matter and Complex Systems》2008,62(3):319-326
We study the influence of repulsive interactions on an
ensemble of coupled excitable rotators. We find that a moderate
fraction of repulsive interactions can trigger global firing of the
ensemble. The regime of global firing, however, is suppressed in
sufficiently large systems if the network of repulsive interactions
is fully random, due to self-averaging in its degree distribution.
We thus introduce a model of partially random networks with a broad
degree distribution, where self-averaging due to size growth is
absent. In this case, the regime of global firing persists for large
sizes. Our results extend previous work on the constructive effects
of diversity in the collective dynamics of complex systems. 相似文献