8,878 research outputs found
Unidentified EGRET sources in the Galaxy
Identifying gamma-ray sources in the Galaxy is hampered by their poor
localization, source confusion, and the large variety of potential emitters.
Neutron stars and their environment offer various ways to power gamma-ray
sources: pulsed emission from the open magnetosphere and unpulsed gamma rays
from the wind nebula and from the cosmic rays accelerated in the supernova
remnant. While the latter still awaits confirmation, new candidate associations
bring forward the importance of 10-kyr old pulsars as GeV sources, with a
diversity that will help constrain the acceleration mechanisms near the pulsar
and in the wind. Theoretical interest in the gamma-ray activity of X-ray
binaries and micro-quasars has also been revived by the emergence of a subset
of variable sources in the inner Galaxy and another one in the halo.Comment: 8 pages, Proc. of the Texas Symposium, 2002, Florence, Ital
Off-Beam Gamma-Ray Pulsars and Unidentified EGRET Sources in the Gould Belt
We investigate whether gamma-ray pulsars viewed at a large angle to the
neutron star magnetic pole could contribute to the new population of galactic
unidentified EGRET sources associated with the Gould Belt. The faint, soft
nature of these sources is distinctly different from both the properties of
unidentified EGRET sources along the galactic plane and of the known gamma-ray
pulsars. We explore the possibility, within the polar cap model, that some of
these sources are emission from pulsars seen at lines of sight that miss both
the bright gamma-ray cone beams and the radio beam. The off-beam gamma-rays
come from high-altitude curvature emission of primary particles, are radiated
over a large solid angle and have a much softer spectrum than that of the main
beams. We estimate that the detectability of such off-beam emission is about a
factor of 4-5 higher than that of the on-beam emission. At least some of the
radio-quiet Gould Belt sources detected by EGRET could therefore be such
off-beam gamma-ray pulsars. GLAST should be able to detect pulsations in most
of these sources.Comment: 5 pages, uses emulateapj.sty, accepted for publication in ApJ Letter
Young and middle age pulsar light-curve morphology: Comparison of Fermi observations with gamma-ray and radio emission geometries
Thanks to the huge amount of gamma-ray pulsar photons collected by the Fermi
Large Area Telescope since June 2008, it is now possible to constrain gamma-ray
geometrical models by comparing simulated and observed light-curve
morphological characteristics. We assumed vacuum-retarded dipole pulsar
magnetic field and tested simulated and observed morphological light-curve
characteristics in the framework of two pole emission geometries, Polar Cap
(PC), radio, and Slot Gap (SG), and Outer Gap (OG)/One Pole Caustic (OPC)
emission geometries. We compared simulated and observed/estimated light-curve
morphological parameters as a function of observable and non-observable pulsar
parameters. The PC model gives the poorest description of the LAT pulsar
light-curve morphology. The OPC best explains both the observed gamma-ray peak
multiplicity and shape classes. The OPC and SG models describe the observed
gamma-ray peak-separation distribution for low- and high-peak separations,
respectively. This suggests that the OPC geometry best explains the single-peak
structure but does not manage to describe the widely separated peaks predicted
in the framework of the SG model as the emission from the two magnetic
hemispheres. The OPC radio-lag distribution shows higher agreement with
observations suggesting that assuming polar radio emission, the gamma-ray
emission regions are likely to be located in the outer magnetosphere. The
larger agreement between simulated and LAT estimations in the framework of the
OPC suggests that the OPC model best predicts the observed variety of profile
shapes. The larger agreement between observations and the OPC model jointly
with the need to explain the abundant 0.5 separated peaks with two-pole
emission geometries, calls for thin OPC gaps to explain the single-peak
geometry but highlights the need of two-pole caustic emission geometry to
explain widely separated peaks.Comment: 28 pages, 20 figures, 8 tables; accepted for publication in Astronomy
and Astrophysic
Cosmic-ray propagation properties for an origin in SNRs
We have studied the impact of cosmic-ray acceleration in SNR on the spectra
of cosmic-ray nuclei in the Galaxy using a series expansion of the propagation
equation, which allows us to use analytical solutions for part of the problem
and an efficient numerical treatment of the remaining equations and thus
accurately describes the cosmic-ray propagation on small scales around their
sources in three spatial dimensions and time. We found strong variations of the
cosmic-ray nuclei flux by typically 20% with occasional spikes of much higher
amplitude, but only minor changes in the spectral distribution. The locally
measured spectra of primary cosmic rays fit well into the obtained range of
possible spectra. We further showed that the spectra of the secondary element
Boron show almost no variations, so that the above findings also imply
significant fluctuations of the Boron-to-Carbon ratio. Therefore the commonly
used method of determining CR propagation parameters by fitting
secondary-to-primary ratios appears flawed on account of the variations that
these ratios would show throughout the Galaxy.Comment: Accepted for publication in Ap
The EGRET sky: a new interstellar emission model and source detection
The comparison of HI, CO, dust, and gamma-ray maps in the solar neighborhood has led to the discovery of large amounts of dark gas. The large mass and angular extent of the local dark clouds, as well as their clumpiness, imply severe revisions of the interstellar emission model to high latitudes, therefore of the detectability of a point-source above the diffuse background. We have used this new model to search for point-like sources at 5\degres|b|80\degres and we show that numerous persistent unidentified EGRET sources are not confirmed as significant sources
The Next Geminga: Deep Multiwavelength Observations of a Neutron Star Identified with 3EG J1835+5918
We describe Chandra, HST, and radio observations that reveal a radio-quiet
but magnetospherically active neutron star in the error circle of the
high-energy gamma-ray source 3EG J1835+5918, the brightest of the unidentified
EGRET sources at high Galactic latitude. A Chandra ACIS-S spectrum of the
ultrasoft X-ray source RX J1836.2+5925, suggested by Mirabal & Halpern as the
neutron star counterpart of 3EG J1835+5918, requires two components: a
blackbody of T~3x10^5 K and a hard tail that can be parameterized as a power
law of photon index Gamma~2. An upper limit of d < 800 pc can be derived from
the blackbody fit under an assumption of R = 10 km. Deep optical imaging with
the HST STIS CCD failed to detect this source to a limit of V > 28.5, thus
f_X/f_V > 6000 and d > 250 pc assuming the X-ray fitted temperature for the
full surface. Repeated observations with the 76 m Lovell telescope at Jodrell
Bank place an upper limit of < 0.1 mJy on the flux density at 1400 MHz for a
pulsar with P > 0.1 s, and < 0.25 mJy for a ~10 ms pulsar at the location of RX
J1836.2+5925. All of this evidence points to an older, possibly more distant
version of the highly efficient gamma-ray pulsar Geminga, as the origin of the
gamma-rays from 3EG J1835+5918.Comment: 4 pages, 4 figures, accepted for publication in ApJ Letter
- …