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Table 2

Summary of the kinematic data.

Lines Component Velocity Δ Velocity Δ z Δ Ref.
width shift
(km s-1) (km s-1) (km s-1) (km s-1)
(1) (2) (3) (4) (5) (6) (7) (8) (9)

Optical
[O III] n unres +162 21 0.06466 0.00007 H08
b 569 35 0 20 0.06412 0.00014 H08
1 Gaussian 411 17 H08
Radio
H I n  ~50 –24 0.06404 M1
b  ~280a 162 to –119 M1
62 † –192† V0†
Mid-IR
[Ne II], [Ne III] 1 Gaussian -87 60 0.06383 0.00020 D11
[O IV], H2
near-IR
Paschen α –126 60 0.06370 0.00015
[Fe II] –6 30 0.0641 0.0001
S(3) –36 90 0.0640 0.0003
s(1) –36 60 0.0640 0.00015

Notes. Columns are: (1) measured emission/absorption line, (2) emission/absorption line component, (3, 4) velocity width (FWHM) and error in km s-1, (5, 6) velocity shift and error (km s-1) with respect to the assumed systemic velocity (taken to be the nuclear broad component of [O III]; see Sect. 3), (7, 8) redshift and error with respect to the broad component of [O III].

References. H08: Holt et al. (2008); M01: Morganti et al. (2001); D11: Dicken et al. (2011); V0: Véron-Cetty et al. (2000). † Véron-Cetty et al. (2000) give e.g. FWZI and we have estimated the FWHM from their figures, but also give their data here.

(a)

Full width at zero intensity (FWZI) of the broad, shallow absorption.

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