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Table 1.

Hot coronal best fit parameters are reported, for the five models applied to the data.

Obs. date Best fit parameter χ2/d.o.f.
CUTOFF POWER LAW
Γ Ec (keV)
February 2013 1.79 ± 0.02 > 200 569/516
March 2014 1.92 ± 0.02 555/499
NTHCOMP
ΓNth kTe (keV)
February 2013 1.80 ± 0.02 > 40 574/516
March 2014 1.94 ± 0.02 560/499

COMPTTSLAB
τ kTe (keV)
February 2013 > 50 568/516
March 2014 555/499
COMPTTSPHERE
τ kTe (keV)
February 2013 > 40 569/516
March 2014 0.75 ± 0.55 555/499

MOCASLAB
τ kTe (keV)
February 2013 566/516
March 2014 552/499
MOCASPHERE
τ kTe (keV)
February 2013 561/516
March 2014 551/499
MOCASPHERECOMPACT
τ kTe (keV)
February 2013 95 ± 15 561/516
March 2014 0.35 ± 0.05 > 190 552/499

Notes. For the MOCASPHERECOMPACT models, we adopted a spherical hot corona configuration, extended from 6 to 100 rg and from 6 up to 20 rg for the 2013 and 2014 observations, respectively.

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