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The first full orbit of Eta Carinae seen by Fermi

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arxiv 1503.07637 v1 pith:XOO2NQXI submitted 2015-03-26 astro-ph.HE

classification astro-ph.HE
keywords spectralcarinaegamma-rayperiastronsourcefirstfluxperiod
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The binary system eta Carinae has completed its first 5.54y orbit since the beginning of science operation of the Fermi Large Area Telescope (LAT). We are now able to investigate the high-energy gamma-ray source at the position of eta Carinae over its full orbital period. By this, we can address and confirm earlier predictions for temporal and spectral variability. Newer versions of the LAT datasets, instrument response functions and background models allow for a more accurate analysis. Therefore it is important to re-evaluate the previously analyzed time period along with the new data to further constrain location, spectral shape, and flux time history of the gamma-ray source. We confirm earlier predictions of increasing flux values above 10 GeV toward the next periastron passage. For the most recent part of the data sample, flux values as high as those before the first periastron passage in 2008 are recorded. A comparison of spectral energy distributions around periastron and apastron passages reveals strong variation in the high-energy band. This is due to a second spectral component that is present only around periastron. Improved spatial consistency with the gamma-ray source at the position of eta Carinae along with the confirmation of temporal variability above 10 GeV in conjunction with the orbital period strengthens the argument for unambiguous source identification. Spectral variability provides additional constraints for future modeling of the particle acceleration and gamma-ray emission in colliding-wind binary systems.

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  1. An 18-year Fermi-LAT stacking limit on GeV $\gamma$-ray emission from particle-accelerating colliding-wind binaries

    astro-ph.HE 2026-07 accept novelty 6.0 of 10

    Clean stack of six high-latitude PACWBs is null (p=0.83), yielding F(>1 GeV)≲1.1e-11 ph cm^{-2} s^{-1} and η≲4e-6 (d/kpc)^2, two orders below η Car.

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