522 research outputs found
The Pierre Auger Observatory: status, results and perspective
While the completion of the Pierre Auger Observatory (or simply ``Auger'') is
still underway, the 5165 km^2.sr.yr integrated acceptance accumulated since the
January 1st, 2004 is now significantly larger than what was gathered by the
previous experiments dedicated to the detection of ultra-high-energy cosmic
rays (UHECRs). We report on the development status of Auger and present some
results related to the cosmic-ray energy spectrum, composition and
anisotropies, and the photon fraction at ultra-high energy. We briefly discuss
the importance of the ankle region to understand the overall phenomenology of
cosmic-rays, and mention future enhancements of Auger focusing on this energy
range.Comment: 10 pages, 10 figures, Invited talk at the International Symposium on
Astronomy and Astrophysics of the Extreme Universe, March 22-23, 2007, RIKEN,
Tokyo (Japan
Light Element Abundance Patterns in the Orion Association: I) HST Observations of Boron in G-dwarfs
The boron abundances for two young solar-type members of the Orion
association, BD -6 1250 and HD 294297, are derived from HST STIS spectra of the
B I transition at 2496.771 A. The best-fit boron abundances for the target
stars are 0.13 and 0.44 dex lower than the solar meteoritic value of log
e(B)=2.78. An anticorrelation of boron and oxygen is found for Orion when these
results are added to previous abundances obtained for 4 B-type stars and the
G-type star BD -5 1317. An analysis of the uncertainties in the abundance
calculations indicates that the observed anticorrelation is probably real. The
B versus O relation observed in the Orion association does not follow the
positive correlation of boron versus oxygen which is observed for the field
stars with roughly solar metallicity. The observed anticorrelation can be
accounted for by a simple model in which two poorly mixed components of gas
(supernova ejecta and boron-enriched ambient medium) contribute to the new
stars that form within the lifetime of the association. This model predicts an
anticorrelation for Be as well, at least as strong as for boron.Comment: 16 pages + 1 table + 7 figures, accepted for publication in Ap
Cosmic-rays: an unsolved mystery at all energies!
We consider the phenomenology of cosmic-rays (CRs) and stress the interest of
jointly studying their properties over the whole energy spectrum. While UHECRs
are known to raise important physical and astrophysical problems, we recall
that low-energy CRs also remain poorly understood, and we indicate the possibly
important role of superbubbles in accelerating CRs up to a few EeV. We also
investigate the viability of holistic models, and show that a unique type of
sources producing CRs with a spectrum in E^{-2.3} could in principle account
for all the CRs in the universe.Comment: 6 pages (uses vietnam.sty). To appear in the proceedings of the 5th
Rencontres du Vietnam, "New Views on the Universe", Hanoi, August 5-11, 200
GRBs and the 511 keV emission of the Galactic bulge
We consider the phenomenology of the 511 keV emission in the Galactic bulge,
as recently observed by INTEGRAL, and propose a model is which the positrons
are produced by gamma-ray bursts (GRB) associated with mini starbursts in the
central molecular zone (CMZ). We show that the positrons can easily diffuse
across the bulge on timescales of about 10^7 yr, and that their injection rate
by GRBs is compatible with the observed fluxes if the mean time between two
GRBs in the bulge is about 8 10^4 yr x E_GRB_51. We also explain the low
disk-to-bulge emission ratio by noting that positrons from GRBs in the Galactic
disk should annihilate on timescales of < 10^4 yr in the dense shell of the
underlying supernova remnant, after the radiative transition, while the
remnants of GRBs occurring in the hot, low-density medium produced by recurrent
starbursts in the CMZ become subsonic before they can form a radiative shell,
allowing the positrons to escape and fill the whole Galactic bulge. If the mean
time between GRBs is smaller than 10^4 E_51 yr, INTEGRAL should be able to
detect the (localized) 511 keV emission associated with one or a few GRB
explosions in the disk.Comment: 6 pages, accepted for publication in A&
On the viability of holistic cosmic-ray source models
We consider the energy spectrum of cosmic-rays (CRs) from a purely
phenomenological point of view and investigate the possibility that they all be
produced by the same type of sources with a single power-law spectrum, in
E^{-x}, from thermal to ultra-high energies. We show that the relative fluxes
of the Galactic (GCR) and extra-galactic (EGCR) components are compatible with
such a holistic model, provided that the index of the source spectrum be x
\simeq 2.23\pm 0.07. This is compatible with the best-fit indices for both GCRs
and EGCRs, assuming that their source composition is the same, which is indeed
the case in a holistic model. It is also compatible with theoretical
expectations for particle acceleration at relativistic shocks.Comment: 5 pages, 1 figure, Accepted for publication in Astronomy and
Astrophysic
The Compton trail of gamma-ray bursts: A long-after glow
AUGERAs they travel through the gas of the host galaxy, some of the gamma-rays emitted in a Gamma-Ray Burst (GRB) may experience Compton scattering and reach an observer even if he is not located in the direction of the primary photon beam. Such a process will last until the GRB photons have left their host galaxy, and the ambient electron density becomes negligible. We investigate the observability of this indirect GRB light, which would be seen as a faint trail along the path of the GRB photons, long after the initial event. We find that the so-called Compton trail of a 1051 erg GRB can easily be observed from Earth, wherever the explosion occurred in our Galaxy in the past few thousand years. Gamma-ray surveys of the Galaxy can therefore provide constraints on the true GRB rate (or number of GRBs per supernova), independently of the GRB beaming angle. We also calculate the expected light curve and shape of the emitting region as a function of time
Acceleration of cosmic rays and gamma-ray emission from supernova remnants in the Galaxy
Galactic cosmic rays are believed to be accelerated at supernova remnant
shocks. Though very popular and robust, this conjecture still needs a
conclusive proof. The strongest support to this idea is probably the fact that
supernova remnants are observed in gamma-rays, which are indeed expected as the
result of the hadronic interactions between the cosmic rays accelerated at the
shock and the ambient gas. However, also leptonic processes can, in most cases,
explain the observed gamma-ray emission. This implies that the detections in
gamma rays do not necessarily mean that supernova remnants accelerate cosmic
ray protons. To overcome this degeneracy, the multi-wavelength emission (from
radio to gamma rays) from individual supernova remnants has been studied and in
a few cases it has been possible to ascribe the gamma-ray emission to one of
the two processes (hadronic or leptonic). Here we adopt a different approach
and, instead of a case-by-case study we aim for a population study and we
compute the number of supernova remnants which are expected to be seen in TeV
gamma rays above a given flux under the assumption that these objects indeed
are the sources of cosmic rays. The predictions found here match well with
current observational results, thus providing a novel consistency check for the
supernova remnant paradigm for the origin of galactic cosmic rays. Moreover,
hints are presented for the fact that particle spectra significantly steeper
than E^-2 are produced at supernova remnants. Finally, we expect that several
of the supernova remnants detected by H.E.S.S. in the survey of the galactic
plane should exhibit a gamma-ray emission dominated by hadronic processes (i.e.
neutral pion decay). The fraction of the detected remnants for which the
leptonic emission dominates over the hadronic one depends on the assumed values
of the physical parameters and can be as high as roughly a half.Comment: 14 pages, 4 figures, 4 tables, submitted to MNRA
Shading and Smothering of Gamma Ray Bursts
The gamma ray burst (GRB) 980425 is distinctive in that it seems to be
associated with supernova (SN) 1998bw, has no X-ray afterglow, and has a single
peak light curve and a soft spectrum. The supernova is itself unusual in that
its expansion velocity exceeds c/6. We suggest that many of these features can
be accounted for with the hypothesis that we observe the GRB along a penumbral
line of sight that contains mainly photons that have scattered off ejected
baryons. The hypothesis suggests a baryon poor jet (BPJ) existing within a
baryon rich outflow. The sharp distinction can be attributed to whether or not
the magnetic field lines thread an event horizon. Such a configuration suggests
that there will be some non-thermal acceleration of pick-up ex-neutrons within
the BPJ. This scenario might produce observable spallation products and
neutrinos.Comment: 7 pages, 2 figures, submitted to ApJ
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