Molecular absorption in Cen A on VLBI scales - PowerPoint PPT Presentation

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Molecular absorption in Cen A on VLBI scales

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Molecular absorption in. Cen A on VLBI scales. Huib Jan van Langevelde, JIVE. Ylva Pihlstr m, NRAO ... The physical and chemical properties of starburst ... – PowerPoint PPT presentation

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Title: Molecular absorption in Cen A on VLBI scales


1
Molecular absorption inCen A on VLBI scales
  • Huib Jan van Langevelde, JIVE
  • Ylva Pihlström, NRAO
  • Tony Beasley, CARMA

2
Goals Questions
  • The physical and chemical properties of starburst
    circumnuclear disks
  • What are good tracers of circumnuclear disks?
  • That allow high resolution VLBI measurements?
  • To weight black holes and measure accretion rates
  • Is the Cen A absorption associated with the
    nucleus or outer galaxy?
  • Geometric constraints (VLBI imaging)
  • Excitation constraints (modeling)
  • Chemical signatures, altered abundances
  • Physics of interstellar medium
  • In starburst/AGN connection

3
Centaurus A
  • In NGC5128, nearest AGN
  • D 3.4 Mpc, 1 16pc
  • Large double lobed radio source
  • Modest black hole ( 107 M?)
  • VLBI source, subluminal
  • Strong mm core
  • Elliptical with dust band
  • Recent merger (few 108 109 yr)
  • Star formation in dust band
  • Gas settling in potential of Elliptical
  • Feeding the central engine?

1pc
Cen A at 2.2 GHz Tingay Murphy 2001 ApJ 546 210
4
Molecules
Israel et al, 1991 AA 245 L13
Seaquist Bell 1990 ApJ 364 L94
5
Absorption HI
  • Absorption against nuclear radio source
  • Several narrow components on VLA scales
  • Red-shifted absorption only seen against core

Sarma et al, 2002 ApJ 564 696
Peck 1999, NMIMT thesis
6
Molecules IR
  • Molecular ring at 1.5 kpc
  • Warped or barred?
  • And a circumnuclear disk
  • Warmer gas at 100pc

100 pc
1 kpc
Wild et al 1997 AA 322 419
Leeuw et al 2002 565 131
7
Models
  • Molecular ring circumnuclear disk
  • Tilted and precessing thin rings
  • Or even a bar
  • Constrained by far-IR and CO imaging
  • Co-rotating high latitude gas may explain
    absorption

Liszt 2001 AA 371 865
8
Previous ATCA result on OH
OH 1667 absorption at 550 km/s
Van Langevelde et al 1995 ApJ 448 L123
9
Excitation model
  • Simple escape probability calculation
  • But does include OH hyperfine transitions
  • fOH (2-6) 10-7 (bit high compared to Galactic)
  • fform 10-10 (low compared to Galactic)
  • 2 components
  • local molecular cloud n104 cm-2, Tkin 10K
  • And 43 K IR radiation field
  • Additional radiation from AGN components
  • 150 K IR from circumnuclear component
  • Important for OH excitation
  • Flat spectrum radio source
  • Important for H2CO excitation
  • Parameterized as distance from nucleus

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11
blue
red
blue
systemic
red
systemic
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13
red
blue
red
systemic
systemic
blue
14
VLBA observations
  • 1995 1997
  • 10 Antennas, but 8 useful
  • Limited coverage
  • d -43o
  • Hard to image
  • Good spectral resolution
  • Confirms previous funny OH result

15
OH absorption on VLBI scales
Systemic
Red-shifted
1 pc
1667 absorption at 600 km/s
1667 absorption at 550 km/s
16
3s upper limit on t
t detected (gt2s)
jet side
counter jet side
17
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18
H2CO absorption
1 pc
19
Where is the core?
Tingay Murphy 2001 ApJ 546 210
20
Continuum
Imaging very difficult due to low elevation and
limited mutual visibility
1 pc
0.1 pc
2 cm
18 cm
6 cm
21
H2CO absorption
1 pc
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25
systemic
t 6cm maser
26
Interpretation
  • Absorption gradient over source
  • 20 mas 0.34pc scale !?
  • Could this be of nuclear origin?
  • Must be very thin, and still unrealistically
    close
  • Excitation, and velocity width seem to rule this
    out
  • Or in outer dust band?
  • Must have completely different scale size than
    OH, HCO, CO
  • Small clump at large distance
  • Chance alignment?
  • Note H2CO does not show red-shifted component
  • Size OK for small scale structure

27
Models
  • Molecular ring circumnuclear disk
  • Tilted and precessing thin rings
  • Or even a bar
  • Constrained by far-IR and CO imaging
  • Co-rotating high latitude gas may explain
    absorption

Eckart et al 1999 ApJ 516 769
28
Conclusions
  • Favour location in molecular ring
  • OH observations do not constrain location much
  • Confirming the ATCA conjugate line results
  • Notably traces different line of sight than most
    molecules
  • Excitation anomalous, but not excited by nuclear
    source
  • H2CO seems more complex
  • Absorption gradient over source
  • 20 mas 0.34pc scale!?
  • Still favour location in molecular ring 200
    2000 pc
  • In which H2CO is confined to the densest parts of
    the molecular ring (low z)
  • Excitation shows no sign of central radio source
  • Still need to work out abundances
  • Can probably compare H2CO to millimeter lines
    directly, distinctly different from OH

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30
OH continuum
1609 MHz
1716 MHz
1661 MHz
1663 MHz
31
  • Competition of satellite transitions
  • Depends critically on optical depth in far IR
  • Only in modest IR field and Galactic conditions
  • Allows a direct measure of OH column in
    individual clump
  • By comparing total column in absorption
  • And local column in excitation

32
OH ATCA maps
OH 1720 emission at 600 km/s
OH 1667 absorption at 550 km/s
33
Centaurus A
  • NGC 5128 picture
  • Dust band
  • Recent merger
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