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Properties of the NLR from Spatially Resolved Spectroscopy Nicola Bennert University of California Riverside Collaborators: Bruno Jungwiert, Stefanie Komossa,

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Presentation on theme: "Properties of the NLR from Spatially Resolved Spectroscopy Nicola Bennert University of California Riverside Collaborators: Bruno Jungwiert, Stefanie Komossa,"— Presentation transcript:

1 Properties of the NLR from Spatially Resolved Spectroscopy Nicola Bennert University of California Riverside Collaborators: Bruno Jungwiert, Stefanie Komossa, Martin Haas, Rolf Chini

2 The Narrow-Line Region of Active Galaxies Extended enough to be directly accessible Affected by ionizing source, presence of torus, jets, … Forbidden lines for diagnostics [OIII] narrow-band imaging commonly used (e.g. Mulchaey et al. 1996, Schmitt et al. 2003)

3 NLR size-luminosity relation constant product U x n AGNs: same U, n, ionizing SED? (Netzer 1990) Bennert et al. 2002 Schmitt et al. 2003 Strömgren: constant density? ⇒ ionization mechanism, AGN lifetimes (Martini et al. 2004), BH mass? ⇒ Disappearing NLR (Netzer et al. 2004)? ⇒ Disappearing NLR (Netzer et al. 2004)?

4 The Narrow-Line Region of Active Galaxies Extended enough to be directly accessible Affected by ionizing source, presence of torus, jets, … Forbidden lines for diagnostics [OIII] narrow-band imaging commonly used (e.g. Mulchaey et al. 1996, Schmitt et al. 2003) But: dependency on sensitivity Mulchaey et al. 1996 vs. Schmitt et al. 2003: 6 times larger NLRs! And: emission contaminated by contributions from e.g. star formation/shock-ionized gas

5 Answers from Spectroscopy Correction of stellar contribution: galaxy itself at 18‘‘ distance Reddening correction (dust) VLT & NTT observations of 6 Sy1s, 6 Sy2s (Bennert et al. 2006a,b,c) Detailed case study: Seyfert-2 galaxy NGC 1386 (Bennert et al. 2006a) Bennert et al. 2006 Probe AGN photoionization, measure „true“ NLR size (diagnostic diagrams) Probe physical parameters (U, n, E_(B-V), T, v, surface brightness)

6 Spatially resolved diagnostics ⇒ NLR size free of stellar contamination: r ~ 6‘‘ (here) vs. r ~ 3‘‘ (Schmitt et al. 2003) vs. r ~ 12‘‘ (Fraquelli et al. 2003) Separation NLR/HII region (2Sy1s, 2Sy2s), confirmed by CLOUDY modeling

7 Electron density and ionization parameter ⇒ excitation of the NLR due to photoionization ⇒ No Strömgren behaviour Both radially decreasing (1/r)

8 Stellar and gaseous kinematics curves similar, signs of rotational motion, no difference in HII region ⇒ torus axis not aligned with galaxy axis, ionization cone lies in disk? Central AGN and galaxy randomly orientated? (e.g. Kinney et al. 2000) ⇒ NLR gas distributed in a disk rather than a sphere

9 The Narrow-Line Region of Active Galaxies NLR size free of stellar contamination NLR size free of stellar contamination NLR photoionized NLR gas in a disk Torus axis in galaxy disk? Unified model supported

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11 BLR size from literature („reverberation mapping“; Kaspi et al. 2000) ⇒ determine BH masses M BH = (10 5.22 M ⊙ ) v 3000 2 R NLR,1 0.88 M BH = (10 8.83 M ⊙ ) v 3000 2 L 44,[OIII] 0.48 M BH = (10 5.22 M ⊙ ) v 3000 2 R NLR,1 0.88 M BH = (10 8.83 M ⊙ ) v 3000 2 L 44,[OIII] 0.48 NLR size versus BLR size Bennert et al. 2004

12 Modeling: NLR size and luminosity ⇒ Different slopes for type 1/2 flatter than flatter than Unified model (Antonucci 1993) & „receding“ torus (Lawrence 1991)

13 determined from Hα/Hβ continuum slope Hα/Hβ continuum slope Reddening ⇒ locally varying amount of dust intrinsic to the NLR? (true for all objects)

14 Comparison of type-1 and type-2 Seyfert 1s [OIII] 4363, [FeVII], [FeX] higher Ionization parameter higher, decreases faster Higher temperatures Seyfert 2s Reddening of nuclear spectrum higher Electron densities comparable (decrease faster in Sy1s) (decrease faster in Sy1s) In agreement with statistics: high-ionization lines & high-critical-density lines stronger in Sy1s ⇒ Highly-ionized gas clouds are located close to nucleus and can be hidden by torus (e.g. Nagao et al. 2000) by torus (e.g. Nagao et al. 2000)

15 Solid line 1: ionization parameter (log U = -4.0 … -1.5 steps of 0.5, from bottom to top; n = 800, 400, 200 cm -3 ; r = 50, 100, 250 pc, from right to left) Dotted lines 2&3: metal abundances (Z = 3…0.05 solar, from right to left; log U = -2.8 for line 2; log U = -3.7 for line 3) Dash-dotted lines 4&5: N & S abundances (Z, U dito 2&3) Dashed line 6: high density (n = 1000000 cm -3 ; U dito 1) CLOUDY modeling ⇒ transition in first and third diagnostic diagram: decreasing ionization parameter & metallicity But not for second diagnostic diagram But not for second diagnostic diagram

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