Central UV spikes in two galactic spheroids

Formation of Galactic Bulges Cambridge University Press (2000) 191-194

Authors:

Michele Cappellari, F Bertola, D Burstein, LM Buson, L Greggio, A Renzini

Abstract:

FOS spectra and FOC photometry of two centrally located, UV-bright spikes in the elliptical galaxy NGC 4552 and the bulge-dominated early spiral NGC 2681, are presented. These spectra reveal that such point-like UV sources detected by means of HST within a relatively large fraction ~15% of bulges can be related to radically different phenomena. While the UV unresolved emission in NGC 4552 represents a transient event likely induced by an accretion event onto a supermassive black hole, the spike seen at the center of NGC 2681 is not variable and it is stellar in nature.

The Bulge-Disk Orthogonal Decoupling in Galaxies: NGC 4698 and NGC 4672

Chapter in The Formation of Galactic Bulges, Cambridge University Press (CUP) (2000) 165-169

Authors:

F Bertola, EM Corsini, M Cappellari, JC Vega Beltrán, A Pizzella, M Sarzi, JG Funes

Near infrared imaging spectroscopy of NGC1275

ArXiv astro-ph/0001052 (2000)

Authors:

Alfred Krabbe, Bruce J Sams III, Reinhard Genzel, Niranjan Thatte, Francisco Prada

Abstract:

We present H and K band imaging spectroscopy of the core regions of the cD/AGN galaxy NGC1275. The spectra, including lines from H2, H, 12CO bandheads, [FeII], and [FeIII], are exploited to constrain the star formation and excitation mechanisms in the galaxy's nucleus. The near-infrared properties can largely be accounted for by ionized gas in the NLR, dense molecular gas, and hot dust concentrated near the active nucleus of NGC1275. The strong and compact H2 emission is mostly from circumnuclear gas excited by the AGN and not from the cooling flow. The extended emission of latetype stars is diluted in the center by the thermal emission of hot dust.

ALFA & 3D: Integral field spectroscopy with adaptive optics

Proceedings of SPIE - The International Society for Optical Engineering 4007 (2000)

Authors:

RI Davies, M Kasper, N Thatte, M Tecza, LE Tacconi-Garman, S Anders, T Herbst

Abstract:

One of the most important techniques for astrophysics with adaptive optics is the ability to do spectroscopy at diffraction limited scales. The extreme difficulty of positioning a faint target accurately on a very narrow slit can be avoided by using an integral field unit, which provides the added benefit of full spatial coverage. During 1998, working with ALFA and the 3D integral field spectrometer, we demonstrated the validity of this technique by extracting and distinguishing spectra from binary stars separated by only 0.26 inch. The combination of ALFA & 3D is also ideally suited to imaging distant galaxies or the nuclei of nearby ones, as its field of view can be changed between 1.2 inches×1.2 inches and 4 inches×4 inches, depending on the pixel scale chosen. In this contribution we present new results both on galactic targets, namely young stellar objects, as well as extra-galactic objects including a Seyfert and a starburst nucleus.

Axisymmetric, three-integral models of galaxies: A massive black hole in NGC 3379

Astronomical Journal 119:3 (2000) 1157-1171

Authors:

K Gebhardt, D Richstone, J Kormendy, TR Lauer, EA Ajhar, R Bender, A Dressler, SM Faber, C Grillmair, J Magorrian, S Tremaine

Abstract:

We fit axisymmetric three-integral dynamical models to NGC 3379 using the line-of-sight velocity distribution obtained from Hubble Space Telescope FOS spectra of the galaxy center and ground-based long-slit spectroscopy along four position angles, with the light distribution constrained by WFPC2 and ground-based images. We have fitted models with inclinations from 29° (intrinsic galaxy type E5) to 90° (intrinsic E1) and black hole masses from 0 to 109 M⊙. The best-fit black hole masses range from 6 × 107 to 2 × 108 M⊙, depending on inclination. The preferred inclination is 90° (edge-on); however, the constraints on allowed inclination are not very strong, owing to our assumption of constant M/LV. The velocity ellipsoid of the best model is not consistent with either isotropy or a two-integral distribution function. Along the major axis, the velocity ellipsoid becomes tangential at the innermost bin, radial in the midrange radii, and tangential again at the outermost bins. The rotation rises quickly at small radii owing to the presence of the black hole. For the acceptable models, the radial-to-tangential [(σ2θ + σ2φ)/2] dispersion in the midrange radii ranges over 1.1 < σr/σt < 1.7, with the smaller black holes requiring larger radial anisotropy. Compared with these three-integral models, two-integral isotropic models overestimate the black hole mass since they cannot provide adequate radial motion. However, the models presented in this paper still contain restrictive assumptions - namely, assumptions of constant M/LV and spheroidal symmetry - requiring yet more models to study black hole properties in complete generality.