Thick as thieves unveiling the most compact and obscured nuclei - - PowerPoint PPT Presentation

thick as thieves unveiling the most compact and obscured
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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?


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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

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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

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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

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DUSTY NUCLEI

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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)

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OPAQUE NUCLEI – THE CONS

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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:
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SLIDE 8

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

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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

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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

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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

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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

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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

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MOLECULAR OUTFLOWS

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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

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MOLECULAR ”JETS” IN DUSTY NUCLEI?

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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

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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

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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
Channel Map: Observed R.A. offset ["]
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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

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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?

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THE DUAL MOLECULAR ”JETS” OF THE LIRG MERGER NGC3256

Extreme jet collimation. Molecular gas along spine

  • f jet

Narrow wind

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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

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SLIDE 22

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?

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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

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SLIDE 24

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

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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?

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HCN 3−2

Moment 0

HCO+ 3−2 HCO+ 3−2 HCN 3−2

Moment 1

Complex ground state HCN/HCO+ emission/absorption profiles