2,074 research outputs found
Realistic Simulations of the Galactic Polarized Foreground: Consequences for 21-cm Reionization Detection Experiments
Experiments designed to measure the redshifted 21~cm line from the Epoch of
Reionization (EoR) are challenged by strong astrophysical foreground
contamination, ionospheric distortions, complex instrumental response and other
different types of noise (e.g. radio frequency interference). The astrophysical
foregrounds are dominated by diffuse synchrotron emission from our Galaxy. Here
we present a simulation of the Galactic emission used as a foreground module
for the LOFAR- EoR key science project end-to-end simulations. The simulation
produces total and polarized intensity over maps of
the Galactic synchrotron and free-free emission, including all observed
characteristics of the emission: spatial fluctuations of amplitude and spectral
index of the synchrotron emission, together with Faraday rotation effects. The
importance of these simulations arise from the fact that the Galactic polarized
emission could behave in a manner similar to the EoR signal along the frequency
direction. As a consequence, an improper instrumental calibration will give
rise to leakages of the polarized to the total signal and mask the desired EoR
signal. In this paper we address this for the first time through realistic
simulations.Comment: 14 pages, 8 figures, published in MNRA
The MeV spectral tail in Cyg X-1 and optically-thin emission of jets
We study the average X-ray and soft gamma-ray spectrum of Cyg X-1 in the hard
spectral state, using data from INTEGRAL. We compare these results with those
from CGRO, and find a good agreement. Confirming previous studies, we find the
presence of a high-energy MeV tail beyond a thermal-Comptonization spectrum;
however, the tail is much softer and weaker than that recently published by
Laurent et al. In spite of this difference, the observed high-energy tail could
still be due to the synchrotron emission of the jet of Cyg X-1, as claimed by
Laurent et al.
To test this possibility, we study optically-thin synchrotron and
self-Compton emission from partially self-absorbed jets. We develop formalisms
for calculating both emission of the jet base (which we define here as the
region where the jet starts its emission) and emission of the entire jet. We
require the emission to match that observed at the turnover energy. The
optically thin emission is dominated by that from the jet base, and it has to
become self-absorbed within it at the turnover frequency. We find this implies
the magnetic field strength at the jet base of B_0 prop. to z_0^4, where z_0 is
the distance of the base from the black-hole centre. The value of B_0 is then
constrained from below by the condition that the self-Compton emission is below
an upper limit in the GeV range, and from above by the condition that the
Poynting flux does not exceed the jet kinetic power. This yields B_0 of the
order of ~10^4 G and the location of the jet base at ~10^3 gravitational radii.
Using our formalism, we find the MeV tail can be due to jet synchrotron
emission, but this requires the electron acceleration at a rather hard
power-law index, p~1.3-1.6. For acceleration indices of p> 2, the amplitude of
the synchrotron component is much below that of MeV tail, and its origin is
likely to be due to hybrid Comptonization in the accretion flow.Comment: MNRAS, in press, 13 page
The X-ray spectrum of the newly discovered accreting millisecond pulsar IGR J17511-3057
We report on an XMM-Newton observation of the accreting millisecond pulsar,
IGR J17511-3057. Pulsations at 244.8339512(1) Hz are observed with an RMS
pulsed fraction of 14.4(3)%. A precise solution for the P_orb=12487.51(2)s
binary system is derived. The measured mass function indicates a main sequence
companion with a mass between 0.15 and 0.44 Msun. The XMM-Newton spectrum of
the source can be modelled by at least three components, multicoloured disc
emission, thermal emission from the NS surface and thermal Comptonization
emission. Spectral fit of the XMM-Newton data and of the RXTE data, taken in a
simultaneous temporal window, constrain the Comptonization parameters: the
electron temperature, kT_e=51(+6,-4) keV, is rather high, while the optical
depth (tau=1.34(+0.03,-0.06)) is moderate. The energy dependence of the pulsed
fraction supports the interpretation of the cooler thermal component as coming
from the accretion disc, and indicates that the Comptonizing plasma surrounds
the hot spots on the NS surface, which provide the seed photons. Signatures of
reflection, such as a broadened iron K-alpha emission line and a Compton hump
at 30 keV ca., are also detected. We derive from the smearing of the reflection
component an inner disc radius of ~> 40 km for a 1.4 Msun neutron star, and an
inclination between 38{\deg} and 68{\deg}. XMM-Newton also observed two type-I
X-ray bursts, probably ignited in a nearly pure helium environment. No
photospheric radius expansion is observed, thus leading to an upper limit on
the distance to the source of 10 kpc. A lower limit of 6.5 kpc can be also set
if it is assumed that emission during the decaying part of the burst involves
the whole neutron star surface. Pulsations observed during the burst decay are
compatible with being phase locked, and have a similar amplitude, than
pre-burst pulsations.Comment: 16 pages, 10 figures, 4 tables, accepted for publication in MNRA
Superorbital variability of X-ray and radio emission of Cyg X-1. I. Emission anisotropy of precessing sources
We study theoretical interpretations of the 150-d (superorbital) modulation
observed in X-ray and radio emission of Cyg X-1 in the framework of models
connecting this phenomenon to precession. Precession changes the orientation of
the emission source (either disc or jet) relative to the observer. This leads
to emission modulation due to an anisotropic emission pattern of the source or
orientation-dependent amount of absorbing medium along the line of sight or
both. We consider, in particular, anisotropy patterns of blackbody-type
emission, thermal Comptonization in slab geometry, jet/outflow beaming, and
absorption in a coronal-type medium above the disc. We then fit these models to
the data from the RXTE/ASM, CGRO/BATSE, and the Ryle and Green Bank radio
telescopes, and find relatively small best-fit angles between the precession
and orbital planes, ~10-20 degrees. The thermal Comptonization model for the
X-ray emission explains well the observed decrease of the variability amplitude
from 1 to 300 keV as a result of a reduced anisotropy of the emission due to
multiple scatterings. Our modeling also yield the jet bulk velocity of
~(0.3-0.5)c, which is in agreement with the previous constraint from the lack
of an observed counterjet and lack of short-term X-ray/radio correlations.Comment: 10 pages, 9 figures and 2 tables, accepted to MNRA
Foreground simulations for the LOFAR - Epoch of Reionization Experiment
Future high redshift 21-cm experiments will suffer from a high degree of
contamination, due both to astrophysical foregrounds and to non-astrophysical
and instrumental effects. In order to reliably extract the cosmological signal
from the observed data, it is essential to understand very well all data
components and their influence on the extracted signal. Here we present
simulated astrophysical foregrounds datacubes and discuss their possible
statistical effects on the data. The foreground maps are produced assuming 5
deg x 5 deg windows that match those expected to be observed by the LOFAR
Epoch-of-Reionization (EoR) key science project. We show that with the expected
LOFAR-EoR sky and receiver noise levels, which amount to ~52 mK at 150 MHz
after 300 hours of total observing time, a simple polynomial fit allows a
statistical reconstruction of the signal. We also show that the polynomial
fitting will work for maps with realistic yet idealised instrument response,
i.e., a response that includes only a uniform uv coverage as a function of
frequency and ignores many other uncertainties. Polarized galactic synchrotron
maps that include internal polarization and a number of Faraday screens along
the line of sight are also simulated. The importance of these stems from the
fact that the LOFAR instrument, in common with all current interferometric EoR
experiments has an instrumentally polarized response.Comment: 18 figures, 3 tables, accepted to be published in MNRA
Charge separation relative to the reaction plane in Pb-Pb collisions at TeV
Measurements of charge dependent azimuthal correlations with the ALICE
detector at the LHC are reported for Pb-Pb collisions at TeV. Two- and three-particle charge-dependent azimuthal correlations in
the pseudo-rapidity range are presented as a function of the
collision centrality, particle separation in pseudo-rapidity, and transverse
momentum. A clear signal compatible with a charge-dependent separation relative
to the reaction plane is observed, which shows little or no collision energy
dependence when compared to measurements at RHIC energies. This provides a new
insight for understanding the nature of the charge dependent azimuthal
correlations observed at RHIC and LHC energies.Comment: 12 pages, 3 captioned figures, authors from page 2 to 6, published
version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/286
A note on comonotonicity and positivity of the control components of decoupled quadratic FBSDE
In this small note we are concerned with the solution of Forward-Backward
Stochastic Differential Equations (FBSDE) with drivers that grow quadratically
in the control component (quadratic growth FBSDE or qgFBSDE). The main theorem
is a comparison result that allows comparing componentwise the signs of the
control processes of two different qgFBSDE. As a byproduct one obtains
conditions that allow establishing the positivity of the control process.Comment: accepted for publicatio
Multiplicity dependence of jet-like two-particle correlations in p-Pb collisions at = 5.02 TeV
Two-particle angular correlations between unidentified charged trigger and
associated particles are measured by the ALICE detector in p-Pb collisions at a
nucleon-nucleon centre-of-mass energy of 5.02 TeV. The transverse-momentum
range 0.7 5.0 GeV/ is examined,
to include correlations induced by jets originating from low
momen\-tum-transfer scatterings (minijets). The correlations expressed as
associated yield per trigger particle are obtained in the pseudorapidity range
. The near-side long-range pseudorapidity correlations observed in
high-multiplicity p-Pb collisions are subtracted from both near-side
short-range and away-side correlations in order to remove the non-jet-like
components. The yields in the jet-like peaks are found to be invariant with
event multiplicity with the exception of events with low multiplicity. This
invariance is consistent with the particles being produced via the incoherent
fragmentation of multiple parton--parton scatterings, while the yield related
to the previously observed ridge structures is not jet-related. The number of
uncorrelated sources of particle production is found to increase linearly with
multiplicity, suggesting no saturation of the number of multi-parton
interactions even in the highest multiplicity p-Pb collisions. Further, the
number scales in the intermediate multiplicity region with the number of binary
nucleon-nucleon collisions estimated with a Glauber Monte-Carlo simulation.Comment: 23 pages, 6 captioned figures, 1 table, authors from page 17,
published version, figures at
http://aliceinfo.cern.ch/ArtSubmission/node/161
Multi-particle azimuthal correlations in p-Pb and Pb-Pb collisions at the CERN Large Hadron Collider
Measurements of multi-particle azimuthal correlations (cumulants) for charged
particles in p-Pb and Pb-Pb collisions are presented. They help address the
question of whether there is evidence for global, flow-like, azimuthal
correlations in the p-Pb system. Comparisons are made to measurements from the
larger Pb-Pb system, where such evidence is established. In particular, the
second harmonic two-particle cumulants are found to decrease with multiplicity,
characteristic of a dominance of few-particle correlations in p-Pb collisions.
However, when a gap is placed to suppress such correlations,
the two-particle cumulants begin to rise at high-multiplicity, indicating the
presence of global azimuthal correlations. The Pb-Pb values are higher than the
p-Pb values at similar multiplicities. In both systems, the second harmonic
four-particle cumulants exhibit a transition from positive to negative values
when the multiplicity increases. The negative values allow for a measurement of
to be made, which is found to be higher in Pb-Pb collisions at
similar multiplicities. The second harmonic six-particle cumulants are also
found to be higher in Pb-Pb collisions. In Pb-Pb collisions, we generally find
which is indicative of a Bessel-Gaussian
function for the distribution. For very high-multiplicity Pb-Pb
collisions, we observe that the four- and six-particle cumulants become
consistent with 0. Finally, third harmonic two-particle cumulants in p-Pb and
Pb-Pb are measured. These are found to be similar for overlapping
multiplicities, when a gap is placed.Comment: 25 pages, 11 captioned figures, 3 tables, authors from page 20,
published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/87
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