We report results of an 18-ks exposure with the ACIS instrument on Chandra
of the powerful z = 0.62 radio galaxy 3C 220.1. The X-ray emission separate
s into cluster gas of emission-weighted kT similar to 5 keV, 0.7-12 keV lum
inosity (to a radius of 45 arcsec) of 5.6 x 10(44) erg s(-1) and unresolved
emission (coincident with the radio core). while the extended X-ray emissi
on is clearly thermal in nature, a straightforward cooling-flow model, even
in conjunction with a point-source component, is a poor fit to the radial
profile of the X-ray emission. This is despite the fact that the measured p
roperties of the gas suggest a massive cooling flow of similar to 130 M-. y
r(-1), and the data show weak evidence for a temperature gradient. The cent
ral unresolved X-ray emission has a power-law spectral energy index alpha s
imilar to 0.7 and 0.7-12 keV luminosity of 10(45) erg s(-1), and any intrin
sic absorption is relatively small. The two-point spectrum of the core emis
sion between radio and X-ray energies has alpha (rx) = 0.75. Since this is
a flatter spectrum than seen in other sources where the X-ray emission is p
resumed to be radio-related, regions close to the active galactic nucleus (
AGN) in this source may dominate the central X-ray output, as is believed t
o be the case for lobe-dominated quasars. Simple unification models would b
e challenged if this were found to be the case for a large fraction of high
-power radio galaxies.