Mapping the kinematics of the narrow-line region in the Seyfert galaxy NGC 4151

被引:134
作者
Das, V
Crenshaw, DM
Hutchings, JB
Deo, RP
Kraemer, SB
Gull, TR
Kaiser, ME
Nelson, CH
Weistrop, D
机构
[1] Georgia State Univ, Dept Phys & Astron, Astron Off, Atlanta, GA 30303 USA
[2] Natl Res Council Canada, Herzberg Inst Astrophys, Dominion Astrophys Observ, Victoria, BC V9E 2E7, Canada
[3] NASA, Goddard Space Flight Ctr, Astron & Solar Phys Lab, Greenbelt, MD 20771 USA
[4] Catholic Univ Amer, Washington, DC 20064 USA
[5] Johns Hopkins Univ, Dept Phys & Astron, Baltimore, MD 21218 USA
[6] Drake Univ, Dept Phys & Astron, Des Moines, IA 50311 USA
[7] Univ Nevada, Dept Phys, Las Vegas, NV 89154 USA
关键词
galaxies : individual ( NGC 4151); galaxies : kinematics and dynamics; galaxies : Seyfert; ISM : jets and outflows; ultraviolet : galaxies;
D O I
10.1086/432255
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Using the Hubble Space Telescope (HST) Space Telescope Imaging Spectrograph (STIS), observations of the [O III] emission from the narrow-line region (NLR) of NGC 4151 were obtained and radial velocities determined. Five orbits of HST time were used to obtain spectra at five parallel slit configurations at a position angle of 58 degrees, with spatial resolution 0.''2 across and 0."1 along each slit. A spectral resolving power (Delta lambda/lambda) of similar to 9000 with the G430M grating gave velocity measurements accurate to similar to 34 km s(-1). A kinematic model was generated to match the radial velocities for comparison to previous kinematic models of biconical radial outflow developed for low-dispersion spectra at two slit positions. The new high-resolution spectra permit the measurement of accurate velocity dispersions for each radial velocity component. The FWHM reaches a maximum of 1000 km s(-1) near the nucleus and generally decreases with increasing distance to about 100 km s(-1) in the extended NLR, starting at about 600 from the nucleus. In addition to the bright emission knots, which generally fit our model, there are faint high-velocity clouds that do not fit the biconical outflow pattern of our kinematic model. These faint clouds occur at the turnover points of the outflowing bright clouds. We suggest possible scenarios that could explain these rogue clouds: ( 1) backflow resulting from shocks and ( 2) outflow outside of the bicones, although the latter does not explain how the knots are ionized and accelerated. A comparison of our observations with a high-resolution radio map shows that there is no evidence that the kinematics of the NLR clouds are affected by the radio lobes that comprise the inner jet.
引用
收藏
页码:945 / 956
页数:12
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