A Dichotomy in the 1–24 GHz Parsec-scale Radio Spectra of Radio-quiet Quasars
We present the parsec-scale radio spectra of a representative sample of 13 Palomar–Green radio-quiet quasars, based on our new Very Long Baseline Array (VLBA) observations at 8.4 and 23.6 GHz and our earlier VLBA studies at 1.5 and 5.0 GHz. The radio core emission generally exhibits a flat spectrum...
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2025-01-01
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author | Sina Chen Ari Laor Ehud Behar Ranieri D. Baldi Joseph D. Gelfand Amy E. Kimball |
author_facet | Sina Chen Ari Laor Ehud Behar Ranieri D. Baldi Joseph D. Gelfand Amy E. Kimball |
author_sort | Sina Chen |
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description | We present the parsec-scale radio spectra of a representative sample of 13 Palomar–Green radio-quiet quasars, based on our new Very Long Baseline Array (VLBA) observations at 8.4 and 23.6 GHz and our earlier VLBA studies at 1.5 and 5.0 GHz. The radio core emission generally exhibits a flat spectrum at 1.5–5.0 GHz, which indicates a compact optically thick synchrotron source on a scale smaller than the broad-line region (BLR) radius R _BLR ∼ 0.01–0.1 pc. The 8.4–23.6 GHz spectral slope remains flat in four objects indicating the inner radius of the radio source R _in < 0.1 R _BLR , and becomes steep in four other objects indicating R _in ∼ 0.5 R _BLR . The flat 8.4–23.6 GHz slope sources may be associated with a continuous ejection starting at the accretion disk corona. The steep 8.4–23.6 GHz slope sources may be produced by an interaction of an active-galactic-nucleus-driven wind with the BLR gas or a low-power jet extending to the BLR scale. Seven of these eight objects, which have a flat or steep 8.4–23.6 GHz slope, reside at the Eddington ratios L / L _Edd < 0.3, and four of the remaining five objects, where the 8.4–23.6 GHz fluxes are too faint to significantly constrain the slope, reside at L / L _Edd > 0.3. The 8.4–23.6 GHz radio emission in the high- L / L _Edd objects may be weak due to more extended emission from a radiation-pressure-driven wind. Future submillimeter observations can further constrain the inward radial extent of the radio emission down to the coronal scale. |
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spelling | doaj-art-91a59c3fc3cd4a01b84aa8c1177b0f232025-01-29T07:01:41ZengIOP PublishingThe Astrophysical Journal1538-43572025-01-01979224110.3847/1538-4357/ada142A Dichotomy in the 1–24 GHz Parsec-scale Radio Spectra of Radio-quiet QuasarsSina Chen0https://orcid.org/0000-0003-1586-3653Ari Laor1https://orcid.org/0000-0002-1615-179XEhud Behar2https://orcid.org/0000-0001-9735-4873Ranieri D. Baldi3https://orcid.org/0000-0002-1824-0411Joseph D. Gelfand4https://orcid.org/0000-0003-4679-1058Amy E. Kimball5https://orcid.org/0000-0001-9324-6787Physics Department, Technion , Haifa 32000, Israel ; sina.chen@campus.technion.ac.ilPhysics Department, Technion , Haifa 32000, Israel ; sina.chen@campus.technion.ac.ilPhysics Department, Technion , Haifa 32000, Israel ; sina.chen@campus.technion.ac.ilINAF—Istituto di Radioastronomia , via Gobetti 101, 40129 Bologna, ItalyNYU Abu Dhabi , PO Box 129188, Abu Dhabi, UAENational Radio Astronomy Observatory , 1011 Lopezville Road, Socorro, NM 87801, USAWe present the parsec-scale radio spectra of a representative sample of 13 Palomar–Green radio-quiet quasars, based on our new Very Long Baseline Array (VLBA) observations at 8.4 and 23.6 GHz and our earlier VLBA studies at 1.5 and 5.0 GHz. The radio core emission generally exhibits a flat spectrum at 1.5–5.0 GHz, which indicates a compact optically thick synchrotron source on a scale smaller than the broad-line region (BLR) radius R _BLR ∼ 0.01–0.1 pc. The 8.4–23.6 GHz spectral slope remains flat in four objects indicating the inner radius of the radio source R _in < 0.1 R _BLR , and becomes steep in four other objects indicating R _in ∼ 0.5 R _BLR . The flat 8.4–23.6 GHz slope sources may be associated with a continuous ejection starting at the accretion disk corona. The steep 8.4–23.6 GHz slope sources may be produced by an interaction of an active-galactic-nucleus-driven wind with the BLR gas or a low-power jet extending to the BLR scale. Seven of these eight objects, which have a flat or steep 8.4–23.6 GHz slope, reside at the Eddington ratios L / L _Edd < 0.3, and four of the remaining five objects, where the 8.4–23.6 GHz fluxes are too faint to significantly constrain the slope, reside at L / L _Edd > 0.3. The 8.4–23.6 GHz radio emission in the high- L / L _Edd objects may be weak due to more extended emission from a radiation-pressure-driven wind. Future submillimeter observations can further constrain the inward radial extent of the radio emission down to the coronal scale.https://doi.org/10.3847/1538-4357/ada142Active galactic nucleiRadio quiet quasarsRadio continuum emission |
spellingShingle | Sina Chen Ari Laor Ehud Behar Ranieri D. Baldi Joseph D. Gelfand Amy E. Kimball A Dichotomy in the 1–24 GHz Parsec-scale Radio Spectra of Radio-quiet Quasars The Astrophysical Journal Active galactic nuclei Radio quiet quasars Radio continuum emission |
title | A Dichotomy in the 1–24 GHz Parsec-scale Radio Spectra of Radio-quiet Quasars |
title_full | A Dichotomy in the 1–24 GHz Parsec-scale Radio Spectra of Radio-quiet Quasars |
title_fullStr | A Dichotomy in the 1–24 GHz Parsec-scale Radio Spectra of Radio-quiet Quasars |
title_full_unstemmed | A Dichotomy in the 1–24 GHz Parsec-scale Radio Spectra of Radio-quiet Quasars |
title_short | A Dichotomy in the 1–24 GHz Parsec-scale Radio Spectra of Radio-quiet Quasars |
title_sort | dichotomy in the 1 24 ghz parsec scale radio spectra of radio quiet quasars |
topic | Active galactic nuclei Radio quiet quasars Radio continuum emission |
url | https://doi.org/10.3847/1538-4357/ada142 |
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