Bibcode
Orienti, M.; Prieto, M. A.; Brunetti, G.; Mack, K.-H.; Massaro, F.; Harris, D. E.
Referencia bibliográfica
Monthly Notices of the Royal Astronomical Society, Volume 419, Issue 3, pp. 2338-2348.
Fecha de publicación:
1
2012
Número de citas
26
Número de citas referidas
25
Descripción
We investigate the nature of the broad-band emission associated with the
low-power radio hotspots 3C 105 South and 3C 445 South. Both hotspot
regions are resolved in multiple radio/optical components.
High-sensitivity radio Very Large Array, near-infrared/optical Very
Large Telescope and Hubble Space Telescope (HST) and X-ray Chandra data
have been used to construct the multiband spectra of individual hotspot
components. The radio-to-optical spectra of both hotspot regions are
well fitted by a synchrotron model with steep spectral indices
˜0.8 and break frequencies between 1012 and
1014 Hz. 3C 105 South is resolved in two optical components:
a primary one, aligned with the jet direction and possibly marking the
first jet impact with the surrounding medium, and a secondary, further
out from the jet and extended in a direction perpendicular to it. This
secondary region is interpreted as a splatter-spot formed by the
deflection of relativistic plasma from the primary hotspot. Radio and
optical images of 3C 445 South show a spectacular 10-kpc arc-shape
structure characterized by two main components, and perpendicular to the
jet direction. HST images in I and B bands further resolve the brightest
components into thin elongated features. In both 3C 105 South and 3C 445
South, the main hotspot components are enshrouded by diffuse optical
emission on scale of several kpc, indicating that very high energy
particles, possibly injected at strong shocks, are continuously
re-accelerated in situ by additional acceleration mechanisms. We suggest
that stochastic processes, linked to turbulence and instabilities, could
provide the required additional re-acceleration. a
Deconvolved angular sizes from a Gaussian fit. b The
angular sizes are derived from the lowest contour on the image plane.
c The diffuse emission is estimated by subtracting the flux
density of SW and SE from the total flux density (see Section 5.3).
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