Javascript must be enabled to continue!
Source number counts at high energies: Swift versus NuSTAR
View through CrossRef
The hard X-ray sky at energies above 10 keV has been extensively explored by the Swift/Gehrels and the NuSTAR missions in the 14−195 keV and the 3−24 keV bands. respectively. The main population of the hard X-ray detected sources are active galactic nuclei (AGN). A discrepancy has been reported between the number count distributions of the two missions in the sense that the extrapolation of the Swift/Gehrels number counts in the flux regime sampled by NuSTAR lies significantly below the NuSTAR counts. We explore this aspect anew by comparing the number count distributions derived from the Swift/Gehrels 105-month catalogue with those from the serendipitous NuSTAR source catalogue. We use a novel number count distribution estimator that makes use of the C-statistic on the unbinned data. In the 14−195 keV band, the Swift/BAT counts follow a Euclidean slope with α = 1.51 ± 0.10 (90% confidence level). The NuSTAR counts in the 8−24 keV band present a steeper slope with α = 1.71 ± 0.20 because of an upturn at fluxes below ∼2 × 10−13 erg cm−2 s−1. The same upturn is observed in the soft (3−8 keV) NuSTAR number counts, which generally also present a steep slope with α = 1.82 ± 0.15. Only the bright part of the NuSTAR 3−8 keV counts agrees with the Chandra number counts in the 2−10 keV band, while the fainter part (below ∼7 × 10−13 erg cm−2 s−1) of the soft NuSTAR counts is in marked disagreement with the Chandra counts. Next, we compare the derived number counts in the different bands using our X-ray AGN population synthesis models. The comparison between the Chandra and the Swift/BAT number counts shows a very good agreement for the standard AGN spectrum with a power-law slope Γ = 1.9, a high-energy cut-off at ∼130 keV and a 2−10 keV reflection component of 3%. On the other hand, using this standard AGN spectral model, only the bright part of the NuSTAR 8−24 keV and 3−8 keV number counts agrees with the model predictions. It is therefore most likely that the disagreement between the X-ray number counts in the different bands is caused by the faint NuSTAR number counts. We discuss various possibilities for the origin of this disagreement.
Title: Source number counts at high energies: Swift versus NuSTAR
Description:
The hard X-ray sky at energies above 10 keV has been extensively explored by the Swift/Gehrels and the NuSTAR missions in the 14−195 keV and the 3−24 keV bands.
respectively.
The main population of the hard X-ray detected sources are active galactic nuclei (AGN).
A discrepancy has been reported between the number count distributions of the two missions in the sense that the extrapolation of the Swift/Gehrels number counts in the flux regime sampled by NuSTAR lies significantly below the NuSTAR counts.
We explore this aspect anew by comparing the number count distributions derived from the Swift/Gehrels 105-month catalogue with those from the serendipitous NuSTAR source catalogue.
We use a novel number count distribution estimator that makes use of the C-statistic on the unbinned data.
In the 14−195 keV band, the Swift/BAT counts follow a Euclidean slope with α = 1.
51 ± 0.
10 (90% confidence level).
The NuSTAR counts in the 8−24 keV band present a steeper slope with α = 1.
71 ± 0.
20 because of an upturn at fluxes below ∼2 × 10−13 erg cm−2 s−1.
The same upturn is observed in the soft (3−8 keV) NuSTAR number counts, which generally also present a steep slope with α = 1.
82 ± 0.
15.
Only the bright part of the NuSTAR 3−8 keV counts agrees with the Chandra number counts in the 2−10 keV band, while the fainter part (below ∼7 × 10−13 erg cm−2 s−1) of the soft NuSTAR counts is in marked disagreement with the Chandra counts.
Next, we compare the derived number counts in the different bands using our X-ray AGN population synthesis models.
The comparison between the Chandra and the Swift/BAT number counts shows a very good agreement for the standard AGN spectrum with a power-law slope Γ = 1.
9, a high-energy cut-off at ∼130 keV and a 2−10 keV reflection component of 3%.
On the other hand, using this standard AGN spectral model, only the bright part of the NuSTAR 8−24 keV and 3−8 keV number counts agrees with the model predictions.
It is therefore most likely that the disagreement between the X-ray number counts in the different bands is caused by the faint NuSTAR number counts.
We discuss various possibilities for the origin of this disagreement.
Related Results
NuSTAR Hard X-Ray Spectra of Radio Galaxies
NuSTAR Hard X-Ray Spectra of Radio Galaxies
Abstract
The Nuclear Spectroscopic Telescope Array (NuSTAR) observatory, with its 3–78 keV broadband spectral coverage, enables the detection of the high-energy cuto...
Density functional theory for comprehensive orbital energy calculations
Density functional theory for comprehensive orbital energy calculations
This study reveals the reason core 1s orbital energies and the highest occupied molecular orbital (HOMO) energies of hydrogen and rare gas atoms are underestimated by long-range co...
Update of the SWIFT model for polar stratospheric ozone loss
(SWIFT version 2)
Update of the SWIFT model for polar stratospheric ozone loss
(SWIFT version 2)
Abstract. The SWIFT model is a fast scheme for calculating the chemistry of stratospheric ozone depletion in polar winter. It is intended for use in Global Climate Models (GCMs) an...
Application of Immunocytochemistry to Monitor the T Cell Subset Counts in Patients with Sepsis
Application of Immunocytochemistry to Monitor the T Cell Subset Counts in Patients with Sepsis
Abstract
[Objective]: To evaluate the application significance of immunocytochemistry for monitoring peripheral blood CD3+ T cell subset (CD3+/CD3+CD4+/CD3+CD8+) counts in ...
International Breast Cancer Study Group (IBCSG)
International Breast Cancer Study Group (IBCSG)
This section provides current contact details and a summary of recent or ongoing clinical trials being coordinated by International Breast Cancer Study Group (IBCSG). Clinical tria...
“fuimus Torys”: Swift and Regime Change, 1714–1718
“fuimus Torys”: Swift and Regime Change, 1714–1718
Accounts of Swift’s life in the months and years following Queen Anne’s death (August 1714) stress his melancholic acceptance of the new world of Hanoverian rule: however unhappy h...
Influence of saturation level on the acoustic emission characteristics of gas hydrate-bearing coal
Influence of saturation level on the acoustic emission characteristics of gas hydrate-bearing coal
AbstractTo study the effects of gas hydrates on the prevention and control of coal and gas protrusions, this paper reports the results of acoustic emission experiments on coal bodi...
The Politics of A Modest Proposal: Swift and the Irish Crisis of the Late 1720s
The Politics of A Modest Proposal: Swift and the Irish Crisis of the Late 1720s
Abstract
Swift’s Modest Proposal (1729) is widely regarded as the most brilliant satire in the English language, but its political context has never been properly ex...


