7 research outputs found

    Re-visiting the Radio-Mechanical Feedback in Brightest Cluster Galaxies

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    The self-regulated feedback from the Active Galactic Nucleus (AGN) plays a key role in the formation and evolution of galaxies by heating and expelling gas in galaxies. The goal of this thesis is to investigate the role of radio-mechanical AGN feedback in expelling gas in central cluster galaxies (BCGs), triggering star formation in the outflowing gas and promoting runaway cooling of the hot intracluster medium gas. We used ALMA observations to characterize molecular gas flows in 14 BCGs and compared them with molecular flows observed in nearby AGN hosting and starburst galaxies. The molecular flows in BCGs are slower, 10–1000 times larger, 10–100 times heavier and carry more momentum compared to outflows driven by quasar mode AGN feedback and starbursts. The kinetic power of flows lies substantially below driving power. The lifting factor, a product of flow mass and radius divided by the driving power, is substantially larger in BCGs showing that radio feedback, when active, is more effective at lifting gas. BCGs form fewer stars per unit molecular gas mass, suggesting that star formation is suppressed, perhaps because the gas in these systems rarely forms molecular disks. The radio mode feedback can drive massive gas outflows and suppress star formation in negative feedback. Paradoxically, radio jets can not only inhibit star formation but also trigger star formation. In chapter 3, we studied one such example of radio-jet triggered star formation in the BCG of the Abell 1795 cluster using VLT optical spectroscopy, HST and ALMA data. Abell 1795 has bright UV filaments surrounding radio jets indicating recent radio jet-triggered star formation. The total extinction corrected star formation rate in the BCG is 9–21 M⊙ yr−1 . We showed that the star formation follows the Kennicutt-Schmidt law with a low efficiency. The gas depletion time of 1 Gyr due to star formation is longer than the dynamical time of the outflow, indicating that star formation may be eventually quenched. The velocity structure function of the warm ionized gas suggests that radio jets may be able to drive supersonic turbulence. Thus radio-mechanical feedback can both trigger and inhibit star formation in the same galaxy on different timescales. Heating from radio-mode feedback does not completely offset cooling of hot gas at all times, as many BCGs have large amounts of cold gas. We also studied the formation of cold gas by cooling of uplifted low entropy gas from centres of galaxy clusters by cavities in 24 galaxy clusters and their BCGs. We showed that single generation of cavities cannot lift enough low entropy gas to form observed amount of cold gas in BCGs. The amount of uplifted gas expected to have cooled from cavities within their lifetimes is less than the observed cold gas mass in many BCGs suggesting that either efficient gas cooling is v required or that the uplift mechanism alone cannot produce all the cold gas in BCGs. The average altitude to which the gas needs to be lifted by cavities to cool before it falls back is also large (∼80 kpc) compared to the observed extent of nebular emission even in the most extended systems. Therefore, we found that stimulated feedback by uplift alone is generally insufficient to explain the observed levels of molecular gas mass in BCGs

    J021659-044920: a relic giant radio galaxy at z ~ 1.3

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    We report the discovery of a relic Giant Radio Galaxy (GRG) J021659-044920 at redshift z1.3z \sim 1.3 that exhibits large-scale extended, nearly co-spatial, radio and X-ray emission from radio lobes, but no detection of Active Galactic Nuclei core, jets and hotspots. The total angular extent of the GRG at the observed frame 0.325 GHz, using Giant Metrewave Radio Telescope observations is found to be {\sim} 2.4 arcmin, that corresponds to a total projected linear size of \sim 1.2 Mpc. The integrated radio spectrum between 0.240 and 1.4 GHz shows high spectral curvature (α0.610 GHz1.4 GHzα0.240 GHz0.325 GHz{\alpha}_{\rm 0.610~GHz}^{\rm 1.4~GHz} - {\alpha}_{\rm 0.240~GHz}^{\rm 0.325~GHz} >> 1.19) with sharp steepening above 0.325 GHz, consistent with relic radio emission that is \sim 8 ×\times 106^{6} yr old. The radio spectral index map between observed frame 0.325 and 1.4~GHz for the two lobes varies from 1.4 to 2.5 with the steepening trend from outer-end to inner-end, indicating backflow of plasma in the lobes. The extended X-ray emission characterized by an absorbed power-law with photon index \sim 1.86 favours inverse-Compton scattering of the Cosmic Microwave Background (ICCMB) photons as the plausible origin. Using both X-ray and radio fluxes under the assumption of ICCMB we estimate the magnetic field in the lobes to be 3.3 μ\muG. The magnetic field estimate based on energy equipartition is \sim 3.5 μ\muG. Our work presents a case study of a rare example of a GRG caught in dying phase in the distant Universe.Comment: 10 pages, 5 figures, 3 tables. Published in MNRAS. Corrected typos and added a referenc

    Molecular Flows in Contemporary Active Galaxies and the Efficacy of Radio-Mechanical Feedback

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    Molecular gas flows are analysed in 14 cluster galaxies (BCGs) centred in cooling hot atmospheres. The BCGs contain 109−1011 M⊙ of molecular gas, much of which is being moved by radio jets and lobes. The molecular flows and radio jet powers are compared to molecular outflows in 45 active galaxies within z < 0.2. We seek to understand the relative efficacy of radio, quasar, and starburst feedback over a range of active galaxy types. Molecular flows powered by radio feedback in BCGs are ∼10–1000 times larger in extent compared to contemporary galaxies hosting quasar nuclei and starbursts. Radio feedback yields lower flow velocities but higher momenta compared to quasar nuclei, as the molecular gas flows in BCGs are usually ∼10–100 times more massive. The product of the molecular gas mass and lifting altitude divided by the AGN or starburst power – a parameter referred to as the lifting factor – exceeds starbursts and quasar nuclei by 2–3 orders of magnitude, respectively. When active, radio feedback is generally more effective at lifting gas in galaxies compared to quasars and starburst winds. The kinetic energy flux of molecular clouds generally lies below and often substantially below a few per cent of the driving power. We find tentatively that star formation is suppressed in BCGs relative to other active galaxies, perhaps because these systems rarely form molecular discs that are more impervious to feedback and are better able to promote star formation

    Radio jet–ISM interaction and positive radio-mechanical feedback in Abell 1795

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    We present XSHOOTER observations with previous ALMA, MUSE, and HST observations to study the nature of radio jet triggered star formation and the interaction of radio jets with the interstellar medium in the brightest cluster galaxy (BCG) in the Abell 1795 cluster. Using HST UV data, we determined an ongoing star formation rate of 9.3 M⊙ yr−1. The star formation follows the global Kennicutt–Schmidt law; however, it has a low efficiency compared to circumnuclear starbursts in nearby galaxies with an average depletion time of ∼1 Gyr. The star formation and molecular gas are offset by ∼1 kpc indicating that stars have decoupled from the gas. We detected an arc of high linewidth in ionized gas where electron densities are elevated by a factor of ∼4 suggesting a shock front driven by radio jets or peculiar motion of the BCG. An analysis of nebular emission line flux ratios suggests that the gas is predominantly ionized by star formation with a small contribution from shocks. We also calculated the velocity structure function (VSF) of the ionized and molecular gases using velocity maps to characterize turbulent motion in the gas. The ionized gas VSF suggests that the radio jets are driving supersonic turbulence in the gas. Thus radio jets cannot only heat the atmosphere on large scales and may quench star formation on longer time-scales while triggering star formation in positive feedback on short time-scales of a few million years

    Atmospheric Pressure and Molecular Cloud Formation in Early-type Galaxies

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    A strong correlation between atmospheric pressure and molecular gas mass is found in central cluster galaxies and early-type galaxies. This trend and a similar trend with atmospheric gas density would naturally arise if the molecular clouds condensed from hot atmospheres. Limits on the ratio of molecular to atomic hydrogen in these systems exceed unity. The data are consistent with ambient pressure being a significant factor in the rapid conversion of atomic hydrogen into molecules as found in normal spiral galaxies

    Radio jet-ISM interaction and positive radio-mechanical feedback in Abell 1795

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    We present XSHOOTER observations with previous ALMA, MUSE and HSTHST observations to study the nature of radio-jet triggered star formation and the interaction of radio jets with the interstellar medium in the brightest cluster galaxy (BCG) in the Abell 1795 cluster. Using HSTHST UV data we determined an ongoing star formation rate of 9.3 M_\odot yr1^{-1}. The star formation follows the global Kennicutt-Schmidt law, however, it has a low efficiency compared to circumnuclear starbursts in nearby galaxies with an average depletion time of \sim1 Gyr. The star formation and molecular gas are offset by 1\sim1 kpc indicating that stars have decoupled from the gas. We detected an arc of high linewidth in ionized gas where electron densities are elevated by a factor of \sim4 suggesting a shock front driven by radio jets or peculiar motion of the BCG. An analysis of nebular emission line flux ratios suggests that the gas is predominantly ionized by star formation with a small contribution from shocks. We also calculated the velocity structure function (VSF) of the ionized and molecular gases using velocity maps to characterize turbulent motion in the gas. The ionized gas VSF suggests that the radio jets are driving supersonic turbulence in the gas. Thus radio jets can not only heat the atmosphere on large scales and may quench star formation on longer timescales while triggering star formation in positive feedback on short timescales of a few million years
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