The radio luminosity function from the low-frequency 3CRR, 6CE and 7CRS complete samples
We measure the radio luminosity function (RLF) of steep-spectrum radio sources using three redshift surveys of flux-limited samples selected at low (151 and 178 MHz) radio frequency, low-frequency source counts and the local RLF. The redshift surveys used are the new 7C Redshift Survey (7CRS) and th...
| Main Authors: | , , , , |
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| Format: | Journal article |
| Language: | English |
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2000
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| _version_ | 1797095012571283456 |
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| author | Willott, C Rawlings, S Blundell, K Lacy, M Eales, SA |
| author_facet | Willott, C Rawlings, S Blundell, K Lacy, M Eales, SA |
| author_sort | Willott, C |
| collection | OXFORD |
| description | We measure the radio luminosity function (RLF) of steep-spectrum radio sources using three redshift surveys of flux-limited samples selected at low (151 and 178 MHz) radio frequency, low-frequency source counts and the local RLF. The redshift surveys used are the new 7C Redshift Survey (7CRS) and the brighter 3CRR and 6CE surveys totalling 356 sources with virtually complete redshift information. This yields unprecedented coverage of the radio luminosity versus z plane for steep-spectrum sources, and hence the most accurate measurements of the steep-spectrum RLF yet made. We find that a simple dual-population model for the RLF fits the data well, requiring differential density evolution (with z) for the two populations. The low-luminosity population can be associated with radio galaxies with weak emission lines, and includes sources with both FRI and FRII radio structures; its comoving space density $\rho$ rises by about one dex between z~0 and z~1 but cannot yet be meaningfully constrained at higher redshifts. The high-luminosity population can be associated with FRII radio galaxies and quasars with strong emission lines; its $\rho$ rises by nearly three dex between z~0 and z~2. These results mirror the situation seen in X-ray and optically-selected AGN. The integrated radio luminosity density of the combination of the two populations is controlled by the value of $\rho$ at the low-luminosity end of the RLF of the high-luminosity population, a quantity which has been directly measured at z~1 by the 7CRS. We argue that robust determination of this quantity at higher redshifts requires a new redshift survey based on a large (~1000 source) sample about five times fainter than the 7CRS. |
| first_indexed | 2024-03-07T04:21:56Z |
| format | Journal article |
| id | oxford-uuid:cb4dea1b-1714-4ec9-994d-003132c053c2 |
| institution | University of Oxford |
| language | English |
| last_indexed | 2024-03-07T04:21:56Z |
| publishDate | 2000 |
| record_format | dspace |
| spelling | oxford-uuid:cb4dea1b-1714-4ec9-994d-003132c053c22022-03-27T07:13:55ZThe radio luminosity function from the low-frequency 3CRR, 6CE and 7CRS complete samplesJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:cb4dea1b-1714-4ec9-994d-003132c053c2EnglishSymplectic Elements at Oxford2000Willott, CRawlings, SBlundell, KLacy, MEales, SAWe measure the radio luminosity function (RLF) of steep-spectrum radio sources using three redshift surveys of flux-limited samples selected at low (151 and 178 MHz) radio frequency, low-frequency source counts and the local RLF. The redshift surveys used are the new 7C Redshift Survey (7CRS) and the brighter 3CRR and 6CE surveys totalling 356 sources with virtually complete redshift information. This yields unprecedented coverage of the radio luminosity versus z plane for steep-spectrum sources, and hence the most accurate measurements of the steep-spectrum RLF yet made. We find that a simple dual-population model for the RLF fits the data well, requiring differential density evolution (with z) for the two populations. The low-luminosity population can be associated with radio galaxies with weak emission lines, and includes sources with both FRI and FRII radio structures; its comoving space density $\rho$ rises by about one dex between z~0 and z~1 but cannot yet be meaningfully constrained at higher redshifts. The high-luminosity population can be associated with FRII radio galaxies and quasars with strong emission lines; its $\rho$ rises by nearly three dex between z~0 and z~2. These results mirror the situation seen in X-ray and optically-selected AGN. The integrated radio luminosity density of the combination of the two populations is controlled by the value of $\rho$ at the low-luminosity end of the RLF of the high-luminosity population, a quantity which has been directly measured at z~1 by the 7CRS. We argue that robust determination of this quantity at higher redshifts requires a new redshift survey based on a large (~1000 source) sample about five times fainter than the 7CRS. |
| spellingShingle | Willott, C Rawlings, S Blundell, K Lacy, M Eales, SA The radio luminosity function from the low-frequency 3CRR, 6CE and 7CRS complete samples |
| title | The radio luminosity function from the low-frequency 3CRR, 6CE and 7CRS
complete samples |
| title_full | The radio luminosity function from the low-frequency 3CRR, 6CE and 7CRS
complete samples |
| title_fullStr | The radio luminosity function from the low-frequency 3CRR, 6CE and 7CRS
complete samples |
| title_full_unstemmed | The radio luminosity function from the low-frequency 3CRR, 6CE and 7CRS
complete samples |
| title_short | The radio luminosity function from the low-frequency 3CRR, 6CE and 7CRS
complete samples |
| title_sort | radio luminosity function from the low frequency 3crr 6ce and 7crs complete samples |
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