Inverse Compton Origin of the Hard X-Ray and Soft Gamma-Ray Emission from the Galactic Ridge
By Troy A. Porter, Igor V. Moskalenko, A. Strong, E. Orlando, L. Bouchet. 2008
214 citations recorded by the source corpus.
A recent redetermination of the nonthermal component of the hard X-ray to soft γ-ray emission from the Galactic ridge, using the SPI instrument on the International Gamma-Ray Astrophysics Laboratory (INTEGRAL), is shown to be well reproduced as inverse Compton emission from the interstellar medium. Both cosmic-ray primary electrons and secondary electrons and positrons contribute to the emission. The prediction uses the GALPROP model and includes a new calculation of the interstellar radiation field. This may solve a long-standing mystery of the origin of this emission, and potentially opens a new window on Galactic cosmic rays.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/e7b2865b2da62588605d98d828448d21718542ea
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Astronomy and Astrophysics
- A. Strong
- E. Orlando
- Bing Zhang
- Anna Franckowiak
- Troy A. Porter
- L. Strigari
- Igor V. Moskalenko
- Christoph Weniger
In Nuclear and High Energy Physics
- A. Strong
- L. Strigari
- E. Orlando
- Anna Franckowiak
- Christoph Weniger
- Troy A. Porter
- N. Fornengo
- I. Cholis
Citations in the corpus
- Galactic electrons and positrons at the Earth: new estimate of the primary and secondary fluxes (2010, methodology): “2, we report the ISRF data that we extracted from the analysis of Porter et al. (2008), and averaged in cylinders of radius and half-height of 500 pc (model 2, M2) and 2 kpc (model 1, M1) about the Earth, on top of which we show that a sum of black-body distributions can provide a reasonable fit.”
- FERMI LARGE AREA TELESCOPE OBSERVATIONS OF THE SUPERNOVA REMNANT W28 (G6.4−0.1) (2010, methodology): “The infrared and optical components are taken from the interstellar radiation field at the location of W28 in the GALPROP code (Porter et al. 2008).”
- Galactic secondary positron flux at the Earth (2008, result): “The positron flux, by itself, does not exhibit unusual features and is in basic agreement with the results of Moskalenko & Strong (1998) and Porter et al. (2008).”
- Background model systematics for the Fermi GeV excess (2014, background): “[110] for a description on how it is constructed).”
- DEVELOPMENT OF THE MODEL OF GALACTIC INTERSTELLAR EMISSION FOR STANDARD POINT-SOURCE ANALYSIS OF FERMI LARGE AREA TELESCOPE DATA (2016, methodology): “We have decomposed the total SEDs into contributions originating from the interstellar gas (atomic, molecular, and DNM), from an axisymmetric Galactic ISRF for the IC radiation, and from the EEE.”
- FERMI LAT DISCOVERY OF EXTENDED GAMMA-RAY EMISSION IN THE DIRECTION OF SUPERNOVA REMNANT W51C (2009, methodology): “The infrared and optical components are adjusted to reproduce the interstellar radiation field in the GALPROP code (Porter et al. 2008).”
- FERMI/LARGE AREA TELESCOPE BRIGHT GAMMA-RAY SOURCE LIST (2009, methodology): “For this work, the GALPROP package has been updated to include recent H I and CO surveys, more accurate decomposition into Galactocentric rings, as well as a new calculation of the interstellar radiation field for inverse Compton emission (Porter et al. 2008).”
- The Fermi Galactic Center GeV Excess and Implications for Dark Matter (2017, methodology): “…we will model Galactic interstellar emission from the large-scale CR populations in the Galaxy starting from predictions obtained through the GALPROP code71 (Moskalenko & Strong 1998; Strong et al. 2000, 2004; Ptuskin et al. 2006; Strong et al. 2007; Porter et al. 2008; Vladimirov et al. 2011).”
- THE SPECTRUM OF ISOTROPIC DIFFUSE GAMMA-RAY EMISSION BETWEEN 100 MeV AND 820 GeV (2014, methodology): “We use the ISRF model introduced in Porter et al. (2008), which is available within GALPROP.”
- FERMI-LAT OBSERVATIONS OF HIGH-ENERGY γ-RAY EMISSION TOWARD THE GALACTIC CENTER (2015, methodology): “Another possible explanation is a higher intensity for the radiation field energy density in the inner Galaxy than used in the standard ISRF model of Porter et al. (2008); these possibilities are not tested here because they require detailed investigations that are beyond the scope of the current…”
- Dark Matter Searches with Astroparticle Data (2011, methodology): “The IC templates are obtained from runs of the GALPROP code (http://galprop.stanford.edu) using a model for the ISRF that has uncertainties, particularly in the inner Galaxy, that have not been completely quantified (Porter & Strong, 2005; Porter et al., 2008).”
- Galactic synchrotron emission with cosmic ray propagation models (2013, methodology): “Gas maps and ISRF are provided and updated to the most recent observations (Porter et al. 2008; Ackermann et al. 2012).”
- The interstellar cosmic-ray electron spectrum from synchrotron radiation and direct measurements. (2011, methodology): “A description of the GALPROP3 model can be found in Strong et al. (2007) and references therein; in particular see Strong & Moskalenko (1998), Strong et al. (2004a) and Porter et al. (2008), and the GALPROP Explanatory Supplement available from the GALPROP website.”
- THE FIRST FERMI LAT SUPERNOVA REMNANT CATALOG (2015, methodology): “The IC map is obtained using GALPROP to reproduce the direct CR measurements with a realistic model of the Galactic interstellar radiation field (ISRF), as was done in Porter et al. (2008).”
- THE LARGE AREA TELESCOPE ON THE FERMI GAMMA-RAY SPACE TELESCOPE MISSION (2009, background): “…EGRET data have concluded that the EGRET sensitivity above 1 GeV has been overestimated (Stecker et al. 2008) or underestimated (Baughman et al. 2007) or imply different cosmic-ray energy spectra in other parts of the Galaxy compared to the local values (Strong et al. 2004a; Porter et al. 2008).”
- CONSTRAINTS ON COSMIC-RAY PROPAGATION MODELS FROM A GLOBAL BAYESIAN ANALYSIS (2010, methodology): “The γ-rays are calculated using the propagated CR distributions, including a contribution from secondary particles such as positrons and electrons from inelastic processes in the ISM that increases the γ-ray flux at MeV energies (Strong et al. 2004; Porter et al. 2008).”