P(B) = [2 / (n/2)^n (n/2)] B^{n-1} exp(-nB^2/2) (2)
where n is the dimensionality of the field.
Figure 6. Loci in the colour-colour plane for two-dimensional random field radio spectra, for the set of frequencies (6, 20, 91) cm.
I have simulated synchrotron spectra for the two- and one-dimensional cases, assuming that the averaging is over all angles. This assumes that the source contains planes or tubes of field that are randomly oriented. Fig. 6 shows colour-colour diagrams for a two-dimensional field. I have also considered the case where a two-dimensional field is present in a single plane at various angles to the line of sight. The resulting colour-colour diagram is very similar to the integrated two-dimensional case.
Figure 7. A colour-colour diagram with D=0.1 for a random magnetic field in one-, two-, and three-dimensions, for the set of frequencies (6, 20, 91) cm.
The colour-colour plots for the different dimensional cases are shown for a diffusion coefficient D=0.1 in Fig. 7. While the colour-colour loci of the various models have the same general shape, changing the dimensionality of the field makes substantial detailed differences to the colour-colour diagram. The parallel section of the colour-colour locus moves closer to the equal spectral index line as the dimensionality of the field decreases. This is attractive, as the colour-colour diagram for Cygnus A shows a parallel section that is close to the diagonal (Katz-Stone et al. 1993).
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Up to: ___________________________________ Peter Tribble, peter.tribble@gmail.com