The resolved narrow-line region in NGC 4151

We present slitless spectra of the narrow-line region (NLR) in NGC 4151 fro m the Space Telescope Imaging Spectrograph (STIS) on the Hubble Space Teles cope and investigate the kinematics and physical conditions of the emission -line clouds in this region. Using medium resolution (similar to 0.5 Angstr om) slitless spectra at two roll angles and narrow-band undispersed images, we have mapped the NLR velocity field from 1.2 kpc to within 13 pc (H-0 = 75 km s(-1) Mpc(-1)) of the nucleus. The inner biconical cloud distribution exhibits recessional velocities relative to the nucleus to the NE and appr oaching velocities to the SW of the nucleus. We find evidence for at least two kinematic components in the NLR. One kinematic component is characteriz ed by low velocities and low velocity dispersions (LVLVD clouds: \ v \ < 40 0 km (-1), and Delta v < 130 km s(-1)). This population extends through the NLR, and their observed kinematics may be gravitationally associated with the host galaxy. Another component is characterized by high velocities and high velocity dispersions (HVHVD clouds: 400 < \ v \ less than or similar t o 1700 km s(-1), Delta v greater than or equal to 130 km s(-1)). This set o f clouds is located within 1." 1 (similar to 70 pc) of the nucleus and has radial velocities that are too high to be gravitational in origin but show no strong correlation between velocity or velocity dispersion and the posit ion of the radio knots. Outflow scenarios will be discussed as the driving mechanism for these HVHVD clouds. We also find clouds characterized by low velocities and high velocity dispersions (LVHVD clouds: \ v \ < 400 km s(-1 ), Delta v greater than or equal to 130 km s(-1)). These clouds are located within 3." 2 (similar to 200 pc) of the nucleus. It is not clear if the LV HVD clouds are HVHVD clouds whose low velocities are the result of projecti on effects. Within 3." 2 (similar to 200 pc) of the nucleus, the [O III]/H beta ratio declines roughly linearly for both the high-velocity-dispersion (HVD) and LVLVD clouds. Since the ionization parameter is proportional to r (-2)n(-1), it appears that the density, n, must decrease as similar to r(-1 ) for the clouds within the inner similar to 3." 2. At distances further fr om the nucleus, the [O III]/H beta ratio is roughly constant.