Figure 6.
The derived KLF from our simple evolutionary scenario, assuming a fraction f = 0.1 of highly accreting sources are HK and a fraction of 1 − f = 0.9 highly accreting sources are HR. The KLF is shown at z = 0 (red), 1 (orange), 2 (green) and 3 (blue). The dashed lines correspond to the HK plus f = 0.1 of LK sources and the dotted lines correspond to the HR plus 1 − f = 0.9 of LK sources. Sources with kinetic luminosities Lkin > 1045 erg s−1 (corresponding to the minimum jet energy we consider to create FR II type lobes) are mostly HK sources.

The derived KLF from our simple evolutionary scenario, assuming a fraction f = 0.1 of highly accreting sources are HK and a fraction of 1 − f = 0.9 highly accreting sources are HR. The KLF is shown at z = 0 (red), 1 (orange), 2 (green) and 3 (blue). The dashed lines correspond to the HK plus f = 0.1 of LK sources and the dotted lines correspond to the HR plus 1 − f = 0.9 of LK sources. Sources with kinetic luminosities Lkin > 1045 erg s−1 (corresponding to the minimum jet energy we consider to create FR II type lobes) are mostly HK sources.

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