Abstract
We present results from a 244 ks \$NuSTAR\$ observation of 3C 273, obtained
during a cross-calibration campaign with the \$Chandra\$, \$INTEGRAL\$, \$Suzaku\$,
\$Swift\$, and \$XMM-Newton\$ observatories. We show that the spectrum, when fit
with a power-law model using data from all observatories except \$INTEGRAL\$ over
the 1-78 keV band, leaves significant residuals in the \$NuSTAR\$ data between
30-78 keV. The \$NuSTAR\$ 3-78 keV spectrum is well-described by an exponentially
cutoff power-law (\$\Gamma = 1.646 0.006\$, E\$\_cutoff =
202\_-34^+51\$ keV) with a weak reflection component from cold, dense
material. There is also evidence for a weak (\$EW = 23 11\$ eV) neutral iron
line. We interpret these features as arising from coronal emission plus
reflection off an accretion disk or distant material. Beyond 80 keV \$INTEGRAL\$
data show clear excess flux relative to an extrapolation of the AGN model fit
to \$NuSTAR\$. This high-energy power-law is consistent with the presence of a
beamed jet, which begins to dominate over emission from the inner accretion
flow at 30-40 keV. Modeling the jet as a power-law, we find the coronal
component is fit by \$\Gamma\_AGN = 1.638 0.045\$,
\$E\_cutfoff = 47 15\$ keV, and jet photon index by
\$\Gamma\_jet = 1.05 0.4\$. We applied comptonizing coronal electron
plasma models to place constraints on the plasma temperature and optical depth.
Finally, we investigate the variability and find an inverse correlation between
flux and \$\Gamma\$. We interpret this hardening of the spectrum with increasing
flux to be due to the jet.
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