5,236 research outputs found
The Very Bright and Nearby GRB 130427A: The Extra Hard Spectral Component and Implications for Very High-energy Gamma-ray Observations of Gamma-ray Bursts
The extended high-energy gamma-ray (>100 MeV) emission occurring after the
prompt gamma-ray bursts (GRBs) is usually characterized by a single power-law
spectrum, which has been explained as the afterglow synchrotron radiation. We
report on the Fermi Large Area Telescope (LAT) observations of the >100 MeV
emission from the very bright and nearby GRB 130427A, up to ~100 GeV. By
performing time-resolved spectral fits of GRB 130427A, we found a strong
evidence of an extra hard spectral component above a few GeV that exists in the
extended high-energy emission of this GRB. This extra spectral component may
represent the first clear evidence of the long sought-after afterglow inverse
Compton emission. Prospects for observations at the very high-energy
gamma-rays, i.e., above 100 GeV, are described.Comment: 6 pages, 2 figures, presented at the 4th High Energy Phenomena in
Relativistic Outflows (HEPRO IV) meeting held in Heidelberg, July 23-26,
2013; to be published in IJMPC
Discovery of GeV emission from the direction of the luminous infrared galaxy NGC 2146
Recent detection of high-energy gamma-ray emission from starburst galaxies
M82 and NGC 253 suggests that starburst galaxies are huge reservoirs of cosmic
rays and these cosmic rays convert a significant fraction of their energy into
gamma-rays by colliding with the dense interstellar medium. In this paper, we
report the search for high-energy gamma-ray emission from several nearby
star-forming and starburst galaxies using the 68 month data obtained with the
Fermi Large Area Telescope. We found a detection of gamma-ray
emission above 200{\rm MeV} from a source spatially coincident with the
location of the luminous infrared galaxy NGC~2146. Taking into account also the
temporal and spectral properties of the gamma-ray emission, we suggest that the
gamma-ray source is likely to be the counterpart of NGC~2146. The gamma-ray
luminosity suggests that cosmic rays in NGC~2146 convert most of their energy
into secondary pions, so NGC~2146 is a "proton calorimeter". It is also found
that NGC~2146 obeys the quasi-linear scaling relation between the gamma-ray
luminosity and total infrared luminosity for star-forming galaxies,
strengthening the connection between massive star formation and gamma-ray
emission of star-forming galaxies. Possible TeV emission from NGC~2146 is
predicted and the implications for high-energy neutrino emission from starburst
galaxies are discussed.Comment: Accepted by ApJ, discussions revised following the referee report,
results and conclusions unchange
Possible methods for the determination of the -parity of the -pentaquark in NN-collisions
We present two possibilities to determine the P-parity of the pentaquark
, in a model independent way, via the measurement of polarization
observables in , or , in
the near threshold region. Besides the measurement of the spin correlation
coefficient, , (in collisions of transversally polarized
nucleons), the coefficient of polarization transfer from the initial
proton to the final hyperon is also unambiguously
related to the parity.Comment: 7 pages, 1 figur
Evidence of a spectral break in the gamma-ray emission of the disk component of Large Magellanic Cloud: a hadronic origin?
It has been suggested that high-energy gamma-ray emission ()
of nearby star-forming galaxies may be produced predominantly by cosmic rays
colliding with the interstellar medium through neutral pion decay. The
pion-decay mechanism predicts a unique spectral signature in the gamma-ray
spectrum, characterized by a fast rising spectrum and a spectral break below a
few hundreds of MeV. We here report the evidence of a spectral break around 500
MeV in the disk emission of Large Magellanic Cloud (LMC), which is found in the
analysis of the gamma-ray data extending down to 60 MeV observed by {\it
Fermi}-Large Area Telescope. The break is well consistent with the pion-decay
model for the gamma-ray emission, although leptonic models, such as the
electron bremsstrahlung emission, cannot be ruled out completely.Comment: 11 pages, 4 figures, Accepted by Ap
High energy emission of GRB 130821A: constraining the density profile of the circum-burst medium as well as the initial Lorentz factor of the outflow
GRB 130821A was detected by Fermi-GBM/LAT, Konus-Wind, SPI-ACS/INTEGRAL,
RHESSI and Mars Odyssey-HEND. Although the data of GRB 130821A are very
limited, we show in this work that the high energy gamma-ray emission (i.e.,
above 100 MeV) alone imposes tight constraint on the density profile of the
circum-burst medium as well as the initial Lorentz factor of the outflow. The
temporal behavior of the high energy gamma-ray emission is consistent with the
forward shock synchrotron radiation model and the circum-burst medium likely
has a constant-density profile. The Lorentz factor is about a few hundred,
similar to other bright GRBs.Comment: 7 pages, 4 figures, 2 tables, ApJ, in pres
Discovery of an extra hard spectral component in the high-energy afterglow emission of GRB 130427A
The extended high-energy gamma-ray (>100 MeV) emission occurred after the
prompt gamma-ray bursts (GRBs) is usually characterized by a single power-law
spectrum, which has been explained as the afterglow synchrotron radiation. The
afterglow inverse-Compton emission has long been predicted to be able to
produce a high-energy component as well, but previous observations have not
revealed such a signature clearly, probably due to the small number of >10 GeV
photons even for the brightest GRBs known so far. In this Letter, we report on
the Fermi Large Area Telescope (LAT) observations of the >100 MeV emission from
the very bright and nearby GRB 130427A. We characterize the time-resolved
spectra of the GeV emission from the GRB onset to the afterglow phase. By
performing time-resolved spectral fits of GRB 130427A, we found a strong
evidence of an extra hard spectral component that exists in the extended
high-energy emission of this GRB. We argue that this hard component may arise
from the afterglow inverse Compton emission.Comment: 5 pages, 2 figures, 2 tables, ApJL, in pres
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