The compact radio jet in the center of the Teacup galaxy blows a lateral turbulent wind in the cold dense gas, as predicted by the simulations. Credit: HST/ ALMA/ VLA/ M. Meenakshi/ D. Mukherjee/ A. Audibert
In the summer of 2021, I joined the group of Dr. Cristina Ramos Almeida at the Instituto de Astrofísica de Canarias (IAC) in Tenerife, first as a postdoctoral research associate and one year later as a Juan de la Cierva fellow. I endeavored into more extreme AGN to investigate the impact of feedback from more powerful and luminous AGN on the host galaxies, part of the QSOFEED (Quasar Feedback) project. Our main goal is to conduct a comprehensive multi-phase analysis of outflow properties by looking at the gas in different phases (ionized, neutral, and molecular) in a sample of obscured type 2 quasars. I am leading the molecular phase facet of the project while also contributing to the broad multi-message perspective.
Radio jets launched by supermassive black holes are one of the potential drivers of multi-phase outflows and can alter the properties of the interstellar medium (ISM) of galaxies on (sub-)kpc scales. In order to investigate the impact of radio jets on the cold gas reservoirs of AGN, I analyzed ALMA CO(2-1) and CO(3-2) observations of the Teacup galaxy. This is a radio-quiet type-2 quasar with a compact low-power radio jet that subtends a small angle from the molecular gas disc. Enhanced emission line widths perpendicular to the jet orientation have been reported for several nearby AGN for the ionized gas. For the molecular gas in the Teacup, not only do we find this enhancement in the velocity dispersion but also a higher brightness temperature ratio (T32/T21) perpendicular to the radio jet compared to the ratios found in the galaxy disc. Our results and the comparison with simulations suggest that the radio jet is compressing and accelerating the molecular gas, and driving a lateral outflow that shows enhanced velocity dispersion and higher gas excitation. These results provide further evidence that the coupling between the jet and the ISM is relevant to AGN feedback even in the case of radio-quiet galaxies.
Brightness temperature ratio (T32/T21) and CO(2-1) velocity dispersion maps. The VLA 6GHz radio continuum is shown in black contours. On the right panel, the σ map of the gas from Simulation E in Meenakshi et al. (2022) for a jet power of Pjet=1045 erg/s, inclined 20◦ from the CO disc plane.
Check out the Press Releases:
IAC:
"Descubren chorros relativistas que producen burbujas en la región central de la galaxia Taza de Té" (Spanish version)
"Discovery of relativistic jets blowing bubbles in the central region of the Teacup Galaxy" (English version)
IAC's video for social media:
IUCAA - Inter-University Centre for Astronomy and Astrophysics
अंतर - विश्वविद्यालय केंद्र : खगोलविज्ञान और खगोलभौतिकी
"Jet blowing bubbles in the Teacup galaxy" (link)
Link for publication:
Jet-induced molecular gas excitation and turbulence in the Teacup, Audibert, A. et al. 2023, A&A Letters, 671, 12 (ADS link)
In this work we presented CO(2−1) and adjacent continuum observations of seven nearby radio-quiet type-2 quasars (QSO2s) obtained with ALMA at ∼0.2″ resolution (370 pc at z ∼ 0.1). These QSO2s are luminous (L[OIII]>108.5 L⊙), and their host galaxies massive (M*~1011 M⊙). The CO morphologies are diverse, including disks and interacting systems. The ionized and molecular gas kinematics and millimeter continuum emission indicate that these CO morphologies are most likely produced by AGN feedback in the form of outflows, jets, and/or shocks.
The CO kinematics of the QSO2s with CO(2−1) revealed molecular outflows that are mostly coplanar with the CO disks. These outflows have maximum velocities of 200-350 km/s and outflow mass rates of 8-16 M⊙/yr, lower than those expected from their AGN luminosities (Fiore+2017).
This suggests that it is not only AGN luminosity that drives massive molecular outflows. Other factors such as jet power, coupling between winds, jets, and/or ionized outflows and the CO disks, and amount or geometry of dense gas in the nuclear regions might also be relevant. Thus, although we did not find evidence for a significant impact of quasar feedback on the total molecular gas reservoirs and star formation rates, it appears to be modifying the distribution of cold molecular gas in the central kiloparsec of the galaxies.
Check out the IAC Press Release:
"Los agujeros negros supermasivos modifican la región central de las galaxias" (Spanish version)
"Supermassive black holes change the central regions of galaxies" (English version)
Artist’s composition: Supermassive black holes modify the distribution of dense gas in the central regions of galaxies. Credits: HST and C. Ramos Almeida.
Cartoon proposed to explain the scenarios to launch more massive ourflows (left) and modest (right) ones, according to relative the geometry of the disks and the jets/winds.
Link for publication:
The diverse cold molecular gas contents, morphologies, and kinematics of type-2 quasars as seen by ALMA, Ramos Almeida, C., Bischetti, M., García-Burillo, S., Alonso-Herrero, Audibert, A. et al. 2022, A&A, 658, 155 (ADS link)
The first CO luminosity function of radio galaxies derived for the local Universe (0.005 < z < 0.3, left panel) and to the cosmic noon ( 1 < z < 2.5 , right panel) using the ALMA Radio-source Catalogue (ARC).
In my first postdoctoral position in Athens, Greece, in 2019 I joined the group of Prof. Kalliopi Dasyra as the scientific PI of the project entitled “Do massive winds induced by black-hole jets alter galaxy evolution? Evidence from galaxies in the ALMA Radio-source Catalog- ARC”. The goal was to study the importance of radio jets in shaping galaxy evolution and was the first attempt to build the CO luminosity functions of radio galaxies (RGs) using a representative sample of 120 RGs from the local Universe up to z ∼ 2.5 observed with ALMA (66 ALMA +54 literature). This work demonstrates the potential of exploring the wealth of the ALMA archival observations, including calibrators, for scientific purposes. The local mass function reveals that the number density of low-z RGs with detectable molecular gas reservoirs is only a little lower (a factor of ∼4) than that of AGN in simulations. At 1 < z < 2.5, there is a significant decrease in the number density of RGs due to the rarity of bright RGs. The CO luminosity function of RGs derived in this work is useful for benchmarking cosmological simulations and constraining the gaseous content of RGs at the local Universe up to the star formation/activity history peak at z≲2.5, where feedback appears to be crucial for galaxy evolution.
Example of the variety of distribution of the molecular gas reservoirs of radio galaxies as seen with ALMA as part of the CO-ARC survey.
Molecular masses derived for the CO-ARC sample compared to the predicted evolution of the molecular gas content with redshift from semi-empirical models of normal star-forming galaxies. Detection are shown with filled circles and upper limits are indicated with open circles and arrows.
Link for publication:
CO in the ALMA Radio-source Catalogue (ARC): The molecular gas content of radio galaxies as a function of redshift, Audibert, A. et al. 2022, A&A, 668, 67 (ADS link)
In 2015, I started my Ph.D. at the Observatoire de Paris under the supervision of Prof. Françoise Combes, becoming a part of the NUclei of GAlaxies (NUGA) collaboration.
In my Ph.D. I studied the fuelling/feedback cycle in low luminosity AGN (LLAGN) part of NUGA. I used observations from the Atacama Large Millimeter/submillimeter Array (ALMA) of a sample of 7 nearby NUGA galaxies was observed with superb spatial resolution of 0.1" (4-9 pc).
High-resolution ALMA CO(3-2) intensity and velocity maps of the NUGA sample.
The work developed in my Ph.D. revealed molecular galaxy disk morphologies with cold rings of a few hundred of pc probing nursery spots of stars, supporting the long-established role of bars as an efficient way to drive and pile up the molecular gas in rings. However, additional mechanisms are required to bring the gas to the very center and feed the modest black holes at the center of these LLAGN: we discovered nuclear-trailing spirals in 3 galaxies, providing the fuel necessary to feed the SMBH in timescales of ~10Myr.
Outflows were detected in half of the sample. The mass outflow rates derived confirmed the expectations from theoretical models, even in the case of LLAGN: the mass outflow rates increase with the radio power and the AGN luminosity. This indicates that molecular outflows are likely entrained by the interaction between the radio jet and the ISM.
Thanks to ALMA’s remarkable spatial resolution, we resolved “molecular tori” around massive black holes in 7 out of 8 NUGA galaxies (Combes et al. 2019). These tori are revealed as nuclear circumnuclear disks of a few tens of pc size whose morphologies and kinematics are decoupled from the main host galaxy disks.
Link for publication summarizing the NUGA results:
Feeding and feedback in nuclei of galaxies, Audibert, A. et al. 2021, IAUS, 359, 307 (ADS link)
In the Seyfert/nuclear starburst galaxy NGC 613, we have combined ALMA Cycles 3 and 4 observations at a spatial resolution of 17 pc. The morphology of CO(3-2) line emission reveals a 2-arm trailing nuclear spiral at r <100 pc inside the Inner Lindblad Resonance (ILR) ring. This nuclear spiral is efficiently driving gas towards the center in ∼10 Myr dynamical timescales.
We find broad wings in the nuclear spectra of CO and dense gas tracers, with velocities reaching up to ±300 km/s, associated with a molecular outflow emanating from the nucleus (r ∼25 pc). We derive a molecular mass outflow rate of Mout =27 M⊙/yr. The outflow is mainly boosted by the AGN through entrainment by the radio jet, but given the weak nuclear activity of NGC 613, we proposed that we might be witnessing a fossil outflow, resulted from a strong past AGN that now has already faded.
Left: the nuclear CO(3-2) spectrum with the blue (-400 to -120 km/s) and red (120 to 300 km/s) wings associated to the outflow. Middle and right: the velocity distribution of the CO(3-2) emission with the VLA radio contours at 4.86 GHz and a zoom of the velocity distribution and the contours of the blue and red wings emission.
NGC 613 is a remarkable example of the complexity of fuelling and feedback mechanisms in AGN: given the relative short flow timescale, tflow~104 yr, the molecular outflow could be a response of the inflowing gas, and eventually acts to self-regulate the gas accretion.
Top: deprojected image of the CO(3-2) emission of NGC 613 and the grativity toques map. Bottom: the radial distribution of the torque, quantified by the fraction of the angular momentum transferred from the gas in one rotation, dL/L.
Link for publication:
ALMA captures feeding and feedback from the active galactic nucleus in NGC 613, Audibert, A. et al. 2019, A&A, 632, 33 (ADS link)
The “hot spot” HII/Sy galaxy NGC 1808 was studied using ALMA Cycle 3 observations at 12 pc spatial resolution. Inside the star-forming ring, a 2-arm spiral structure is clearly detected at ∼50 pc radius. We found that the nuclear spiral is kinematically decoupled from the larger disk, the position angle being tilted from 323◦ to close to 270◦ What is remarkable in our observations, is that the nuclear trailing spiral is even more contrasted in the dense gas tracers. The computations of the torques exerted on the gas by the barred stellar potential reveal that the gas within a radius of 100 pc is feeding the nucleus on a timescale of five rotations or on an average timescale of ∼60 Myr.
We found a HCN enhancement in circumnuclear molecular gas around AGN, by measuring the HCN(4-3)/HCO+(4-3) and HCN(4-3)/CS(7-6) intensity ratios in the submillimetre diagram (Izumi et al. 2016). We find that the nuclear region of NGC 1808 presents line ratios that indicate excitation conditions typical of X-ray dominated regions in the vicinity of AGN.
There is a molecular outflow detected at ≥250 pc in the NE direction that is likely due to supernovae feedback and it is connected to the kpc-scale superwind.
ALMA 0.2" observations of the doubled-barred galaxy NGC1808. Left: CO(3-2) distribution with the main features observed. The top right shows a zoomed inset of the ∼100 pc trailing nuclear spiral, also detected in the dense gas tracers HCN(4- 3), HCO+(4-3) and CS(7-6) in the bottom right panels.
Top: velocity and dispersion maps of NGC1808. The misaligment in the nuclear region from a position angle being tilted from 323º in the main disk to close to 270º in the nucleus. Bottom: position-velocity diagram along the minor axis (cyan area in dispersion map). The non-circular motions in the NE direction are likely due to a starburst-driven molecular outflow.
Link for publication:
Black hole feeding and star formation in NGC 1808, Audibert, A. et al. 2021, A&A, 656, 60 (ADS link)
Our aim was to explore the close environment of AGN, and the dynamical structures leading to their fueling, through the morphology and kinematics of the gas inside the sphere of influence of the black hole. We used ALMA observations of CO(3-2) emission in the NUGA sample of seven Seyfert/LINER galaxies at the unprecedented spatial resolution of 0.″1 = 4-8 pc.
The observed maps reveal the existence molecular tori: circumnuclear disk structures, defined by their morphology and decoupled kinematics. They have varying orientations along the line of sight, unaligned with the host galaxy orientation. The radius of the tori ranges from 6 to 27 pc and usually the torus and the AGN are slightly off-centered with respect to the bar-resonant ring position, implying that the black hole is wandering by a few 10 pc amplitude around the center of mass of the galaxy.
Our spatial resolution allows us to measure gas velocities inside the sphere of influence of the central black holes. By fitting the observations with different simulated cubes, varying the torus inclination and the black hole mass, it is possible to estimate the mass of the central black hole, which is in general difficult for such late-type galaxies, with only a pseudo-bulge.
Link for publication:
ALMA observations of molecular tori around massive black holes, Combes, F., García-Burillo, S., Audibert, A. et al. 2019, A&A, 623, 79 (ADS link)
Everything started with my fascination for active galaxies when I was a student in Brazil at the Universidade Federal do Rio Grande do Sul, one of the top research institutes in astrophysics in Brazil, located in Porto Alegre. Under the supervision of Dr. Rogério Riffel and Dr. Miriani Pastoriza, I began my research by studying the mid-infrared properties of nearby AGN. The mid-infrared spectral range is crucial for studying the torus, a key component in the Unified Model of AGN. In this unification model, an obscuring torus of gas and dust envelops the central SMBH and the broad line region, and the different observed AGN types are explained by the observer's orientation.
High-resolution ALMA CO(3-2) intensity and velocity maps of the NUGA sample.
During my B.Sc. and M.Sc. studies, I analyzed Spitzer/IRS spectra (5-35𝜇m) of ~100 Seyfert galaxies, a common type of AGN in the nearby Universe. I compared these spectra with theoretical spectral energy distribution (SED) from the CLUMPY torus models. The main goal was to discern the differences in the physical parameters of tori between type 1 and type 2 AGN. I found that the classification of a galaxy may also depend on the intrinsic properties of the torus clouds rather than simply on their inclination, in contradiction to the unification model orientation assumption, in agreement with previous studies using smaller samples.
Illustration of the distribution of number of clouds along the equatorial plane, N , and torus opening angle, σ, and their correlation with the covering factor, CT, in colors. The closed diamonds represent the Sy 1 objects and the circles show the Sy 2 types. Sy 2 galaxies are more likely drawn from the distribution of higher covering factors than Sy 1 types.
Seyfert 2 galaxies have more clouds along the line-of-sight, Nobs and these clouds present higher optical depths τV.
Schematic torus cross-section illustrates the main differences between the torus physical properties.
Link for publication:
Probing the active galactic nucleus unified model torus properties in Seyfert galaxies, Audibert, A. et al. 2017, MNRAS, 464, 2139 (ADS link)