Table 2.
Kinematic parameters.
H I | H2 | [Fe II] | [Mg IV] | |
---|---|---|---|---|
W nucleus | ||||
ΔV1 | 0 ± 1 |
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−111 ± 3 |
FWHM1 | 238 ± 2 |
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ΔV2 | −72 ± 2 | – |
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– |
FWHM2 |
![]() |
– |
![]() |
– |
W80 | 370 ± 3 | 270 ± 20 | 380 ± 3 | 260 ± 10 |
V10 | −250 ± 2 | −180 ± 15 | −270 ± 6 | −265 ± 10 |
Vmax |
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560 ± 25 | 309 ± 8 |
E nucleus | ||||
ΔV1 |
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−40 ± 5 |
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![]() |
FWHM1 |
![]() |
230 ± 3 |
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![]() |
ΔV2 |
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−60 ± 30 | – |
FWHM2 |
![]() |
405 ± 10 |
![]() |
– |
W80 | 370 ± 30 | 440 ± 50 | 380 ± 42 | 400 ± 30 |
V10 | −250 ± 20 | −370 ± 30 | −250 ± 42 | −370 ± 20 |
Vmax |
![]() |
![]() |
![]() |
440 ± 20 |
NE cluster | ||||
ΔV1 |
![]() |
−40 ± 5 |
![]() |
![]() |
FWHM1 |
![]() |
![]() |
210 ± 30 | 260 ± 10 |
ΔV2 | – | – |
![]() |
– |
FWHM2 | – | – |
![]() |
– |
W80 | 250 ± 10 |
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290 ± 40 | 305 ± 40 |
V10 | −160 ± 10 |
![]() |
−170 ± 30 | −240 ± 30 |
Vmax |
![]() |
![]() |
190 ± 20 | 300 ± 6 |
NW outflow | ||||
ΔV1 |
![]() |
![]() |
![]() |
– |
FWHM1 |
![]() |
![]() |
![]() |
– |
ΔV2 |
![]() |
![]() |
– | – |
FWHM2 |
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![]() |
– | – |
ΔV3 | – |
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– | – |
FWHM3 | – |
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– | – |
W80 |
![]() |
715 ± 10 | 715 ± 40 | – |
V10 | −690 ± 30 | −590 ± 15 | −670 ± 35 | – |
Vmax |
![]() |
820 ± 35 |
![]() |
– |
Notes. All kinematic parameters are given in km s−1. Velocity shifts ΔVi and line width FWHMi refer to the individual Gaussian components (i = 1 to 3, at maximum) required to model the emission line profiles. V10 is defined as 10th percentile velocity of the fitted line profile, while W80 is defined as the difference between the 90th and 10th percentiles. Vmax is defined as |ΔVbroad|+2σbroad.
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