Articles
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10/14/2022--
10/10/2022
Relativistic Gas: Invariant Lorentz Distribution for the velocities
In 1911, J\"uttner proposed the generalization, for a relativistic gas, of
the Maxwell-Boltzmann distribution of velocities. Here we want to discuss,
among others, J\"uttner probability density function (PDF). Both the velocity
space and, consequently, the momentum space are not flat in special relativity.
The velocity space corresponds to the Lobachevsky one, which has a negative
curvature. This curvature induces a specific power for the Lorentz factor in
the PDF, affecting J\"uttner normalization constant in one, two, and three
dimensions. Furthermore, J\"uttner distribution, written in terms of a more
convenient variable, the rapidity, presents a curvature change at the origin at
sufficiently high energy, which does not agree with our computational dynamics
simulations of a relativistic gas. However, in one dimension, the rapidity
satisfies a simple additivity law. This allows us to obtain, through the
Central Limit Theorem, a new, Lorentz-invariant, PDF whose curvature at the
origin does not change for any energy value and which agrees with our
computational dynamics simulations data. Also, we perform extensive
first-principle simulations of a one-dimensional relativistic gas constituted
by light and heavy particles.
Evaldo M. F. Curado
Carlos E. Cedeño
Ivano Damião Soares
Constantino Tsallis
12/04/2020--
09/18/2020
The Multipolar Magnetic Field of Millisecond Pulsar PSR J0030+0451
Modeling of the NICER X-ray waveform of the pulsar PSR J0030+0451, aimed to
constrain the neutron star mass and radius, has inferred surface hot-spots (the
magnetic polar caps) that imply significantly non-dipolar magnetic fields. To
this end, we investigate magnetic field configurations that comprise offset
dipole plus quadrupole components using static vacuum field and force-free
global magnetosphere models. Taking into account the compactness and observer
angle values provided by Miller et al. (2019) and Riley et al. (2019), we
compute geodesics from the observer plane to the polar caps to compute the
resulting X-ray light curve. We explore, through Markov chain Monte Carlo
techniques, the detailed magnetic field configurations that can reproduce the
observed X-ray light curve and have discovered degeneracies, i.e., diverse
field configurations, which can provide sufficient descriptions to the NICER
X-ray waveforms. Having obtained the force-free field structures, we then
compute the corresponding synchronous gamma-ray light curves following
Kalapotharakos et al. (2014) these we compare to those obtained by Fermi-LAT,
to provide models consistent with both the X-ray and the gamma-ray data,
thereby restricting further the multipole field parameters. An essential aspect
of this approach is the proper computation of the relative phase between the
synchronous X- and gamma-ray light curves. We conclude with a discussion of the
broader implications of our study.
Constantinos Kalapotharakos
Zorawar Wadiasingh
Alice K. Harding
Demosthenes Kazanas
10/15/2021--
10/29/2020
Learning Sampling Distributions Using Local 3D Workspace Decompositions for Motion Planning in High Dimensions
Earlier work has shown that reusing experience from prior motion planning
problems can improve the efficiency of similar, future motion planning queries.
However, for robots with many degrees-of-freedom, these methods exhibit poor
generalization across different environments and often require large datasets
that are impractical to gather. We present SPARK and FLAME , two
experience-based frameworks for sampling-based planning applicable to complex
manipulators in 3 D environments. Both combine samplers associated with
features from a workspace decomposition into a global biased sampling
distribution. SPARK decomposes the environment based on exact geometry while
FLAME is more general, and uses an octree-based decomposition obtained from
sensor data. We demonstrate the effectiveness of SPARK and FLAME on a Fetch
robot tasked with challenging pick-and-place manipulation problems. Our
approaches can be trained incrementally and significantly improve performance
with only a handful of examples, generalizing better over diverse tasks and
environments as compared to prior approaches.
Constantinos Chamzas
Zachary Kingston
Carlos Quintero-Peña
Anshumali Shrivastava
Lydia E. Kavraki
11/08/2005--
11/08/2005
Comment on ``Temporal scaling at Feigenbaum point and nonextensive thermodynamics" by P. Grassberger
Critiques presented by P. Grassberger in Phys. Rev. Lett. 95, 140601 (2005)
are addressed.
Constantino Tsallis
10/13/2004--
06/06/2004
Ageing in the critical contact process: a Monte Carlo study
The long-time dynamics of the critical contact process which is brought
suddenly out of an uncorrelated initial state undergoes ageing in close analogy
with quenched magnetic systems. In particular, we show through Monte Carlo
simulations in one and two dimensions and through mean-field theory that
time-translation invariance is broken and that dynamical scaling holds. We find
that the autocorrelation and autoresponse exponents lambda_{Gamma} and lambda_R
are equal but, in contrast to systems relaxing to equilibrium, the ageing
exponents a and b are distinct. A recent proposal to define a non-equilibrium
temperature through the short-time limit of the fluctuation-dissipation ratio
is therefore not applicable.
Jose J. Ramasco
Malte Henkel
Maria Augusta Santos
Constantino A. da Silva Santos
08/21/2013--
08/21/2013
Reducing influence of antiferromagnetic interactions on ferromagnetic properties of p-(Cd,Mn)Te quantum wells
In order to explain the absence of hysteresis in ferromagnetic p-type
(Cd,Mn)Te quantum wells (QWs), spin dynamics was previously investigated by
Monte Carlo simulations combining the Metropolis algorithm with the
determination of hole eigenfunctions at each Monte Carlo sweep. Short-range
antiferromagnetic superexchange interactions between Mn spins - which compete
with the hole-mediated long-range ferromagnetic coupling - were found to
accelerate magnetization dynamics if the the layer containing Mn spins is wider
than the vertical range of the hole wave function. Employing this approach it
is shown here that appreciate magnitudes of remanence and coercivity can be
obtained if Mn ions are introduced to the quantum well in a delta-like fashion.
C. Simserides
A. Lipinska
K. N. Trohidou
T. Dietl
05/24/2004--
05/24/2004
Fast and reliable MCMC for cosmological parameter estimation
Markov Chain Monte Carlo (MCMC) techniques are now widely used for
cosmological parameter estimation. Chains are generated to sample the posterior
probability distribution obtained following the Bayesian approach. An important
issue is how to optimize the efficiency of such sampling and how to diagnose
whether a finite-length chain has adequately sampled the underlying posterior
probability distribution. We show how the power spectrum of a single such
finite chain may be used as a convergence diagnostic by means of a fitting
function, and discuss strategies for optimizing the distribution for the
proposed steps. The methods developed are applied to current CMB and LSS data
interpreted using both a pure adiabatic cosmological model and a mixed
adiabatic/isocurvature cosmological model including possible correlations
between modes. For the latter application, because of the increased
dimensionality and the presence of degeneracies, the need for tuning MCMC
methods for maximum efficiency becomes particularly acute.
Joanna Dunkley
Martin Bucher
Pedro G. Ferreira
Kavilan Moodley
Constantinos Skordis
03/28/2007--
03/28/2007
Deviation from Gaussianity in the cosmic microwave background temperature fluctuations
Recent measurements of the temperature fluctuations of the cosmic microwave
background (CMB) radiation from the WMAP satellite provide indication of a
non-Gaussian behavior. Although the observed feature is small, it is detectable
and analyzable. Indeed, the temperature distribution P^{CMB}(Delta T) of these
data can be quite well fitted by the anomalous probability distribution
emerging within nonextensive statistical mechanics, based on the entropy S_q =
k (1 - \int dx [P(x)]^q)/(q - 1) (where in the limit case q -> 1 we obtain the
Boltzmann-Gibbs entropy S_1 = - k \int dx P(x) ln[P(x)]). For the CMB
frequencies analysed, \nu= 40.7, 60.8, and 93.5 GHz, P^{CMB}(Delta T) is well
described by P_q(Delta T) \propto 1/[1 + (q-1) B(\nu) (Delta T)^2]^{1/(q-1)},
with q = 1.04 \pm 0.01, the strongest non-Gaussian contribution coming from the
South-East sector of the celestial sphere. Moreover, Monte Carlo simulations
exclude, at the 99% confidence level, P_1(Delta T) \propto e^{- B(\nu) (Delta
T)^2} to fit the three-year WMAP data.
Armando Bernui
Constantino Tsallis
Thyrso Villela
10/25/2010--
10/25/2010
Detection of coarse-grained unstable states of microscopic/stochastic systems: a timestepper-based iterative protocol
We address an iterative procedure that can be used to detect coarse-grained
hyperbolic unstable equilibria (saddle points) of microscopic simulators when
no equations at the macroscopic level are available. The scheme is based on the
concept of coarse timestepping [Kevrekidis et al., 2003] incorporating an
adaptive mechanism based on the chord method allowing the location of
coarse-grained saddle points directly. Ultimately, it can be used in a
consecutive manner to trace the coarse-grained open-loop saddle-node
bifurcation diagrams. We illustrate the procedure through two indicatively
examples including (i) a kinetic Monte Carlo simulation (kMC) of simple surface
catalytic reactions and (ii) a simple agent-based model, a financial caricature
which is used to simulate the dynamics of buying and selling of a large
population of interacting individuals in the presence of mimesis. Both models
exhibit coarse-grained regular turning points which give rise to branches of
saddle points.
A. C. Tsoumanis
C. I. Siettos
10/04/2011--
06/25/2011
Measurement of the Cross Section for Prompt Isolated Diphoton Production in p\bar p Collisions at \sqrt{s} = 1.96 TeV
This article reports a measurement of the production cross section of prompt
isolated photon pairs in proton-antiproton collisions at \sqrt{s} = 1.96 TeV
using the CDF II detector at the Fermilab Tevatron collider. The data
correspond to an integrated luminosity of 5.36/fb. The cross section is
presented as a function of kinematic variables sensitive to the reaction
mechanisms. The results are compared with three perturbative QCD calculations:
(1) a leading order parton shower Monte Carlo, (2) a fixed next-to-leading
order calculation and (3) a next-to-leading order/next-to-next-to-leading-log
resummed calculation. The comparisons show that, within their known
limitations, all calculations predict the main features of the data, but no
calculation adequately describes all aspects of the data.
CDF Collaboration
T. Aaltonen
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