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The AGN Obscuring Torus

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Presentation on theme: "The AGN Obscuring Torus"— Presentation transcript:

1 The AGN Obscuring Torus
Moshe Elitzur University of Kentucky & LAOG, Grenoble

2 Happy Birthday, young man!

3 Coupled Escape Probability optical depth zone # tz = tt z tz-1 ti i
i,i Ti Ci pi  ni1 ni2 ij = |i – j| ti-1 t2 2 t1 Coupled Escape Probability 1 t0 = 0

4 Elitzur & Asensio Ramos 2006, MNRAS 365, 779
2-level Atom  = 10-3 : Semi-infinite Atmosphere (10-3    107) Slab t = 500 Time %error zones ALI CEP 20 0.39 36.3 104 40 1.10 23.9 45.7 100 4.39 0.06 10.9 14.0 200 11.6 0.89 5.5 5.4 600 44.9 1.70 1.6 1.2 Time %error, S zones ALI CEP 1 0.03 99.5 55.5 20 1.02 88.2 23.0 40 3.29 79.8 15.5 100 12.6 .033 62.5 6.5 200 28.1 .085 46.4 2.2 Elitzur & Asensio Ramos 2006, MNRAS 365, 779

5 Toroidal Obscuration Required by Unification Schemes
Unified Scheme for AGN Toroidal Obscuration Required by Unification Schemes

6 General folklore: R  100 pc
Torus Properties From the statistics of type 1 vs type 2: H/R ~ 1 (Schmitt et al ’01) R = ? Must rely on IR emission General folklore: R  100 pc

7 Origin of the 100’s pc Torus – Modeling IR emission
Pier & Krolik 92 5-10 pc Pier & Krolik 93 ~100 pc Dearth of IR emission in smooth-density models T  r Granato et al ’94, ‘97: Uniform density Rout ~ 100 – 300 pc  = 45°

8 Observations – NGC 1068, CO at R ~ 70 pc, H ~ 9 – 10 pc  H/R ~ 0.15
Schinnerer et al ’00 at R ~ 70 pc, H ~ 9 – 10 pc  H/R ~ 0.15

9 Observations – NGC 1068, CO & H2
20 pc 140 pc Galliano et al ’03: H/R ~ 0.15

10 IR – Observations NGC1068: 2m imaging – R ~ 1 pc (Weigelt et al 04) 10m interferometry – R ~ 2 pc (Jaffe et al 04) Cen A: 2m – R < 0.5 pc (Prieto et al 04) & 10m – R ~ 1.5 pc (Karovska et al 03) Circinus: 2m – R ~ 1pc (Prieto et al 04) & 18m – R < 2 pc (Packham et al 05) NGC1097 & NGC5506: 2m – R < 5 pc (Prieto et al 04)

11 The Torus Size Crisis Observations – compact (pc-size) torus
Theory – extended (100’s pc) torus r  1.7 pc: T = 320 K Jaffe et al ‘04 VLTI – NGC1068: Poncelet et al ‘06 Lbol = 2·1045 erg s (Mason et al ’06) T(r = 2pc) = 960 K r(T = 320 K) = 26 pc r(T = 226 K) = 57 pc

12 Temperature in Clumpy Medium
Tmax Tmin Nenkova et al 2006

13 Temperature–Distance Relation
Smooth density – T & R uniquely related Clumpy density – different T at same R different R, same T

14 AGN Clumpy Torus: Size Effect
Ri = 0.9 pc L½ Y = Ro/Ri N  N0r -q exp(-2/2) N0 = 5  = 45º V = 60 Clumping solves the compact emission problem!

15 Dynamic Origin of Vertical Structure
Cloud accretion from the galaxy? No need in a compact torus!

16 The Torus as a Disk-Wind Region
Bottorff et al 97

17 Unification Scheme

18 Grand Unification Scheme
masers BLR Torus BAL Emmering, Blandford & Shlosman 92

19 Cloud Properties in Torus-Wind
Size – shear resistance: Density: Mass: Magnetic field: Elitzur & Shlosman 2006

20 Water Masers – Glimpse of Torus Clouds?
NGC 3079 Kondratko, Greenhill & Moran ‘05 High-latitude features – disk rotational imprint: uplifted clouds

21 Outflow and Accretion Torus disappearance at L  1043 erg s-1 !
Narrow-line Seyfert 1 radio galaxies? Chiaberge et al ’99; Whysong & Antonucci ‘04

22 Conclusions No bagel Toroidal Obscuration Required by Unified Scheme – just a region in the disk-wind


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