The flux density estimates used in this redetermination of the 1934-638
spectrum are listed in the second column of Table 1. The fitted value from
the revised polynomial is shown in column 3 while the difference between
this and the previous fit is shown in column 4 (in the sense new-old).
The origin of each measurement is given in column 5 with additional notes
below the Table. The formal errors in all measurements above 1GHz are
1% or less and are not shown.
The flux values listed are of three types;
There is good evidence from Bonn (Ott et al. 1993) and the VLA
(Perley 1993, priv. comm.) that, in the frequency range 110GHz,
3C286 has not changed by more than
1% from the spectrum published
by Baars et al. (1977). The ATCA flux densities in the Table have all
been calculated using the Ott et al. (1993) spectrum for 3C286, which
differs by no more than 1
2% from either the Baars et al. (1977)
spectrum or from the spectrum currently used at the VLA.
Ott et al. (1993) found that both Hydra A and Virgo A have changed significantly from their Baars et al. (1977) values so in each case the revised spectrum of Ott et al. (1993) has been used. It is clear from the Table that the single dish fluxes agree rather well with the ATCA interferometer fluxes, confirming the flux ratio of 3C286 to Hydra A implied in the results of Ott et al. (1993).
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