Table 9
Faraday components vs. synchrotron components correspondence.
| Source | Faraday | Polarization | Synchrotron | Correspondence |
|---|---|---|---|---|
| name | components | parameter | components | [y–n–a] |
| 0239–0234 | 2 | σRM | 2 | y |
| 0243–0550 | 2 | σRM | 2 | y |
| 0751+2716 | 3 | σRM | 1 | n |
| 0845+0439 | 2 | σRM | 2 | y |
| 0958+3224 | 3 | ΔRM | 2–3 | a |
| 1048+0141 | 2 | σRM | 1 | n |
| 1146+5356 | 2 | σRM | 3 | n |
| 1246–0730 | 2 | ΔRM | 2–3 | a |
| 1311+1417 | 3 | σRM | 1–2 | n |
| 1312+5548 | 3 | σRM | 1 | n |
| 1405+0415 | 2 | σRM | 1 | n |
| 1549+5038 | 3 | σRM | 3 | y |
| 1616+0459 | 2 | σRM | 2 | y |
| 2245+0324 | 3 | σRM | 3 | y |
Notes. In the table – y means there is correspondence between synchrotron components and Faraday components between C and X bands; a means there is almost a correspondence between synchrotron components and Faraday components between C and X bands: n means there is no correspondence between synchrotron components and Faraday components between C and X bands. Eight sources show correspondence, clear correspondence (y) and a marginal correspondence (a), between thenumber of Faraday components used to model the depolarization effects and the synchrotron components used to fit their radio spectrum. The remaining six sources do not show correspondence (n).
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