Thick as thieves unveiling the most compact and obscured nuclei - - PowerPoint PPT Presentation
Thick as thieves unveiling the most compact and obscured nuclei - - PowerPoint PPT Presentation
Thick as thieves unveiling the most compact and obscured nuclei Susanne Aalto Department of Space, Earth and Environment (SEE), Chalmers University of Technology Sweden +many collaborators Outline Dusty nuclei Why do we care?
Outline
- Dusty nuclei
– Why do we care? – the torii – example NGC1068 – the Compact Obscured Nuclei (CONs) – example IC860 – ALMA CON-quest
- Related posters:
– CON-quest: Falstad, Onishi; – H2S: Sato
- Dusty Feedback
– AGN and starburst feedback – Collimated molecular outflows in dusty galaxies – example NGC1377
Dusty growth: U/LIRGs and obscured nuclei
- Luminous and Ultraluminous Infrared
Galaxies, (U)LIRGs (LIR>1011 Lsun), are dusty galaxies
– Often interacting - fundamental to our understanding of galaxy evolution (e.g. Elbaz & Cesarsky 2003; Sanders & Mirabel 1996). Some have even more embedded nuclei that harbour a very active evolutionary stage of AGNs and/or starbursts.
- Obscured AGNs
– Most AGNs in the universe are obscured (e.g. Brandt and Alexander) – Shape and structure of torus linked to feeding of SMBH and feedback – Starburst-AGN connection – How is the small scale (< 1 pc) obscuration linked to that at 10-100 pc – or on larger scales?
- The nuclear activity will often drive
mechanical feedback in the form of molecular winds, jets and outflows
The Antennae: 100 µm PACS
- n HST (Klaas +10)
Arp220
Winds and jets Garcia-Burillo+14
NASA, ESA, and C. Wilson
from Alexander 2011
Diaz-Santos+17
DUSTY NUCLEI
NGC1068: Imaging an AGN-obscuring dust torus with ALMA
- High resolution (0.”06) ALMA λ=450 µm
- bservations reveal:
- r=3.5 pc dusty turbulent torus with
Mgas=1x105 Msun (Garcia-Burillo+16, Gallimore+16).
- Diagnostic HCN/HCO+ line ratios change
with distance to nucleus (Garcia- Burillo+14, Viti+14, Imanishi+16,18).
For more ALMA studies of AGN torii see e.g. Combes+19 (survey) , Izumi+18 (Circinus), Espada+17 (Cen A) , Aalto+17,20 (NGC1377)
- Even higher resolution observations (0.”02)
reveal apparent counter-rotation. (Imanishi+18, Impellizzeri+19, Garcia- Burillo+19). Counter-rotation can be real, or an effect of inflow or ”outflowing torus”.
- Column density estimated to
N(H2)=1023 cm-2 on scales of a few pc
From Garcia- Burillo+19 (Garcia-Burillo+14,16)
OPAQUE NUCLEI – THE CONS
CONs – Compact Obscured Nuclei - N(H2)>1025 cm-2 Av>>1000
- Hidden growth in our time:
– AGN statistics and/or growth of nuclear stellar spheroid. – Starburst-AGN connection.
- Relation to distant DOGs? SMGs?
- Potential sources of cosmic neutrinos (e.g. Berezinskii & Ginzburg 1981;
Bahcall & Waxman 2001, Yoast-Hull+17).
- <0. “1 (<20 pc) nuclear
emission
- τ(860 μm) = 1 (i.e., NH>1025
cm−2). NGC4418
1 −1 −1 1 1 −1 R.A. offset [arcsec] −1 1
- Dec. offset [arcsec]
0.35" x 0.26" 50 pc (k) 860 µm 5 10 15
mm/submm continuum Example: NGC4418 (e.g Sakamoto+10,13, Costagliola+13 – see also Varenius+14 for VLBI imaging)
Some (U)LIRGs harbour CONs - Still unknown how common they are. Extremely important to understand
- bscured phase:
Buried nuclei can be traced by vibrationally excited molecules at long wavelengths– e.g. HCN
Vibrationally excited HCN (HCN-VIB) requires TB(14 µm) > 100 K.
Rotational transitions in the mm/submm. (e.g. Sakamoto+10, Aalto+15a,b, Imanishi+13, Martin+16, Aalto+16, Imanishi+16); cm wavelengths (e.g. Salter+08); mid-IR HCN absorption line (Lahuis+07)
14 µm IR field Vibrationally excited HCN (HCN-VIB)
ν=0 ladder ν2=2 ladder
Cartoon by F. Costagliola
ALMA 345-100 GHz, 25-90 mas
- bservations of the early-type LIRG IC860 (Aalto+19)
- HCN-VIB probes inner region – but opacities. Tex -TB matching: diminishing
line-to-continuum ratio in inner r=4 pc.
- mm continuum optically thick: – N(H2) >1026 cm-2 - ”brick wall”. Average
gas densities n>107 cm-3 within r=9pc. (Assuming standard dust-gas ratio. Compare ULIRG core Arp220 (Scoville+17, Sakamoto+17, Barcos- Munos+18).(Beware of potential self-heating (Kaufman+98,Gonzalez- Alfonso+19).
- Rotating thick turbulent nuclear disk + inflow+outflow
Nature of buried source:
- Accreting SMBH – potentially undermassive
- A starburst consisting only of massive O-stars – i.e. extremely
skewed initial mass function (IMF).
MilliArc seconds MilliArc seconds 100 50
- 50
- 100
- 150
150 100 50
- 50
- 100
HCN-VIB 3-2
Major axis
- f rotation
14 pc
IC 860
Ground state HCN, HCO+, CS lines continuum- and self absorbed in central 50 pc.
Minor and major axis position-velociy diagrams
Massive inflow + onset of extremely dusty feedback?
Layered structure of non-circular motions:
- Assymmetric foreground absorption inflow:
Reversed P-Cygni in HCN, HCO+. Inflow on scales >50 pc down to nucleus. The time-scale of gas to reach the nucleus from r=50 pc is 1 Myr
- Compact, dense outflow: P-Cygni in CS 7-6, HC15N out to
- 300 km/s. Broad, minor axis HCN-VIB features may be
base of outflow. Vibrationally excited HC3N v7=2 also seen along minor axis. Extent of dense outflow: 20 pc Cartoons of two scenarios:
- A. near-face-on with out-of-plane inflow.
- B. Near-edge-on where obscuration consists of
torus and in-plane inflow
A. B.
Massive inflow supplies nuclear gas/dust column – what allows for the build-up of of N(H2)=1026 cm-2? Witnessing the onset of dense feedback? – Or a failed wind? Timescales? Ongoing radio studies (Merlin/VLA/VLBI) reveal compaxt collimated jet-like structures + SNRs
ALMA CON-quest survey
(see posters by Falstad and Onishi)
- CON-quest: Deep survey of 38 nearby
ULIRGs, LIRGs and low luminosity dusty
- galaxies. (PI: S.Aalto)
– HCN, HCO+, HOC+, HCN-VIB 3-2 – Dense outflow statistics – Resolved HCN/HCO+ ratio maps – Nuclear dynamics and SMBH masses – Deep 1mm continuum images – Prime data analysts: König, Falstad, Onishi, Nishimura
- What are CONs and what are their
timescales??
- How common are they? Is there a
luminosity dependence on their prevalence?
– Preliminary: The CON detection rates are 20 − 25% in FIR-selected (U)LIRGs with LFIR>1011 Lsun, and 0% in lower luminosity galaxies.’
- CON hosts?
– Preliminary: Major merger ULIRGs – minor merger LIRGs? Possible link to post- starburst signatures still needs investigation.
Example of LIRG CON hosts: Dusty S0/galaxies – minor mergers: HST V-band Images HST GO-1: J. Gallagher, Sample CON-quest HCN, HCN/HCO+ ratio, spectra and continuum maps
Zw049.057 NGC4418
CON-quest members: S. Aalto; N. Falstad; S. König; K. Onishi; Y. Nishimura; G. Privon; ; J. Mangum; S. Martin; K. Sakamoto S. Muller; S. Garcia-Burillo; E. Gonzalez-Alfonso; G. Fuller; T. Greve; F. Combes; C. Henkel; A. Evans; S. Mühle; T. Diaz-Santos; C. Ricci; K. Kohno; N. Harada; T. Izumi; M. Imanishi; J. Gallagher III; S. Viti; P. van der Werf; L. Barcos- Munos; S. Linden
Hot and opaque cores – where are the
- utflows? (Hallqvist+17, Falstad+19)
- HCN-VIB luminous galaxies do not
show strong FIR OH λ=119 µm P- Cygni profiles. But they do show inflows.
- Why?
- Outflow collimation.
- Obscured, compact flows
CO outflow signatures now found for most CONs: I17208 (Garcia-Burillo+14); Zw049 (Falstad+18);NGC4418 (Fluetsch+18); Arp220 (e.g. Barcos-Munos+17); ESO320 (Pereirs-Santaella+16); IC860 (Aalto+19) Follow up studies on MUSE,HST, VLA, ALMA (CON-firm, PI: Falstad)
Plot from Falstad+19
Median OH outflow velocity as a function of the HCN-vib luminosity relative to the the total infrared luminosity. Velocities Vout (from Veilleux+13)
OH inflow signature
MOLECULAR OUTFLOWS
The nuclear activity will often drive mechanical feedback in the form of winds, jets and
- utflows. The feedback may:
– Regulate SMBH growth and link it to the host galaxy – Magorrian relation. – help partially explain ” dead” properties of local ellipticals. – reduce star formation efficiency
Outflows and winds from galaxies are multi-phase. There is mounting evidence that cold (10-100 K) molecular gas in
- utflows is common and that the cold gas
may in some cases dominate mass and momentum flux
AGN and starburst feedback
M82 NGC1377
Artists impression
NGC253
MOLECULAR ”JETS” IN DUSTY NUCLEI?
Collimated outflows in CONs?
400 km/s OH (4-6 GHz) VLA line wing seen with the VLA (Falstad+19 see also Baan+89). Weak radio continuum (5 GHz associated with collimated NIR dust feature or shadow.
HST image of Zw049 (Falstad+18, Gallagher et al in prep.)
CO 2-1, 6-5 tracing very dense nuclear
- utflow . Also the 690
GHz dust is partially tracing the nuclear
- uflow. (ALMA+SMA)
Arp220
- ALMA reveals very dense and
fast (850 km/s) outflow in ULIRG Arp220. TB(HCN) > TB(CO) (Barcos-Munos+17). Very opaque dust in core and
- utflow (Scoville+17,
Sakamoto+17) Zw049.057
The most extreme FIR-excess, radio-quiet galaxy NGC1377
Small, lenticular galaxy LFIR=5x109 Lsun Excess FIR emission with q>3.9 – off FIR-Radio correlation by factor >37 Deep silicate absorption (Spoon+07). No Pα, Br γ - Faint Hα, [N II] and [Ne II] lines, Faint PAH (Roussel+03,06). Roussel+06
Featureless morphology apart from southern minor axis dust structure Post- starburst/LINER
- ptical characteristics
What is powering the compact IR luminosity - Obscured AGN or nascent starburst? HST v-band
ALMA reveals a molecular jet - precessing?
Grey scale: Systemic velocities Red and blue: High velocity gas High velocity gas aligned along line-of- sight 100 pc
A molecular ”jet” swirling around an axis perpendicular to the line of sight may reproduce
- bservations. May signal obscured, accreting SMBH
- 1
- 0.5
- Dec. offset ["]
- 2
- 1.5
- 1
- 0.5
- 1
- 0.5
- Dec. offset ["]
- 2
- 1.5
- 1
- 0.5
Compare to garden sprinkler
Molecular mass: jet: 1-6x107, (“wind”: 108 M⊙) - Extent: 400 pc Opening angle: jet:small, wind: 50◦– 70◦ Age: jet: 0.5-2 Myr? Outflow velocity: jet: 200 - 800 kms-1, wind: 30-100 kms-1 dM/dt: jet: 6–30 M⊙ yr−1 dP/dt: jet:10-40LIR/c
ALMA Band 9, 50 mas CO 6-5 observations show base of molecular jet
- Dense (n>104 cm-3), warm molecular gas (>100 K) in the jet +
narrow wind on scales 10-20 pc (Aalto+17)
- Strong excitation gradient along jet.
- Herschel shows very high CO excitation – originating in jet launch
region in nucleus?
THE DUAL MOLECULAR ”JETS” OF THE LIRG MERGER NGC3256
Extreme jet collimation. Molecular gas along spine
- f jet
Narrow wind
A rotating disk wind
- Jet is surrounded by a
narrow rotating disk-wind
- Wind may be magneto-
centrifugally driven
- Energetics also allow jet
to be a gravitationally powered magneto- centrifugal wind
- Jet is changing direction –
jet/wind interactions
Projected 60-80 kms-1
High dispersion and gas inflow
- Velocity widths in jet ΔV>80 km/s on 2 pc scales – for r>30
pc.
- Jet may inject turbulence in jet-wind interactions
- ΔV>30 km/s in r=50 pc gas structure in ”disk”, but rotation
- f molecular disk is extremely slow suggesting a structure
with σ/vrot >1
- Redshifted CO and HCO+ self-absorption 20-30 km/s.
Foreground cool shell of infalling gas?
- Non-circular motion in nuclear disk matching
Keplerian rotation – inflow or projected outflow? Evidence for 10-15 degree warping out to r=20 pc - created by inflow?
NGC1377 – a post-CON?
- Compact 0.8 mm dust continuum suggest
an asymmetric dusty torus of radius r=2 pc.
- Column densities N(H2) > 1024 cm-2
for r<1-2 pc
- Nuclear dynamics is complex – launch
site of rotating wind, possible inflow. Cannot exclude binary SMBH. NGC1377 similar to CON host galaxies. But
- bscuration appears to occur on smaller scales
than in CONs. Disk gas may have been ejected by the molecular jet and wind. Feeding-cycle where ejected material return to fuel further growth? Would explain
- rigin of nuclear gas
0.8 mm continuum 5 pc
Nuclear high-velocity gas
2 pc
Compare to gas entrained/pushed by radio jets
- Molecular gas found lining radio jets – gas is pushed and heated – e.g. M51, NGC1068, IC5063 (e.g.
Matsushita+06,14; Garcia-Burillo+14,+17, Morganti+15, Dasyra+16, Oosterloo+17). In ESO 420-G13 a previously unknown jet is revealed through its interaction with the ISM.
- In NGC1377- no radio jet detected so far and the molecular gas appears to be on the jet axis:
Entrainment vs disk-wind? Is the jet powered by accretion onto the CND – not the accretion disk? The angular momentum loss may help the remaining gas reach the nucleus.
M51 NGC1068 (Garcia-Burillo+17)
(Matsushita+14)
colour: C2H (N=1-0) emission contours: jet emission @87GHz
Red: HCN(1-0)/CO(1-0) ratio
- map. Blue: 6 cm continuum
ESO 420-G13 (Fernández-Ontiveros+19)
Colour: ALMA CO 2-1 Contour: Ne II
Conclusions
- Compact Obscured Nuclei – CONS (N(H2)>1025 cm-2) are found in
some U/LIRGs. Rich in molecules.
– Can be probed by e.g. mid-IR pumped HCN. ALMA CON-quest survey. – IC860: massive inflow + nuclear column N(H2)>1026 cm-2. Evidence of very dense outflow.
- Accreting SMBH or top-heavy IMF SB?
– CONs appear at first not to have outflows – but mm/cm observations reveal fast outflows – collimated and obscured. – There is some evidence that CONs may have recurrent, cyclic nuclear activity.
- Extremely collimated and radio-quiet molecular jet in NGC1377.
MHD disk-wind?
– Jet appears to be precessing inside a rotating molecular wind. – Different from radio-jet driven molecular gas (or so it seems…) – New form of feedback: Outflow helped nuclear growth rather than negative feedback?
200 400 600 800 MilliArc seconds MilliArc seconds 200 100
- 100
- 200
- 300
300 200 100
- 100
- 200
- 300
200 400 600 800 MilliArc seconds MilliArc seconds 200 100
- 100
- 200
- 300
300 200 100
- 100
- 200
- 300
3700 3800 3900 4000 MilliArc seconds MilliArc seconds 200 100
- 100
- 200
- 300
300 200 100
- 100
- 200
- 300
3700 3800 3900 4000 MilliArc seconds MilliArc seconds 200 100
- 100
- 200
- 300
300 200 100
- 100
- 200
- 300
HCN 3−2
Moment 0
HCO+ 3−2 HCO+ 3−2 HCN 3−2
Moment 1
Complex ground state HCN/HCO+ emission/absorption profiles