%...Journal: PASP
%R=BibCode
%A=Authors
%B=Abstract
%c=Copyright
%D=Date of publication
%E=Electronic file
%F=Original File
%I=Institute and/or Footnotes
%J-last page
%K=Keywords
%T=Title

%R 1999PASP..111..919H
%F ori/PASPv111n762
%J-945
%T The Distribution of Heavy Elements in Spiral and Elliptical Galaxies. (Invited
   Review).
%A Henry, R.B.C.
%I Department of Physics and Astronomy, University of Oklahoma, Norman, OK 73019;
   (henry@mail.nhn.ou.edu) and
%A Worthey, Guy
%I Department of Physics and Astronomy, St. Ambrose University, Davenport, IA
   52803; (gworthey@saunix.sau.edu)
%B  In large disk and spheroidal galaxies, spatially resolved abundance
   information can be extracted by analysis of either emission lines, absorption
   lines, or both, depending on the situation. This review recaps significant
   results as they apply to nondwarf galaxies, including the Milky Way, spiral
   disks and bulges, and elliptical and lenticular galaxies. Methods for determining
   abundances are explained in appendices.\par Conclusions that span the galaxy
   types treated here are as follows. All galaxies, on average, have heavy-element
   abundances (metallicities) that systematically decrease outward from their
   galactic centers while their global metallicities increase with galaxy mass.
   Abundance gradients are steepest in normal spirals and are seen to be progressively
   flatter going in order from barred spirals to lenticulars to ellipticals.
   The distribution of abundances N(Z) versus {\em Z} is strongly peaked compared
   with simple closed-box model predictions of chemical enrichment in all galaxy
   types. That is, a ``G dwarf problem'', commonly known in the solar cylinder,
   exists for all large galaxies.\par For spiral galaxies, local metallicity
   appears to be correlated with total (disk+bulge) surface density. Examination
   of N/O versus O/H in spiral disks indicates that production of N is dominated
   by primary processes at low metallicity and secondary processes at high metallicity.
   Carbon production increases with increasing metallicity. Abundance ratios
   Ne/O, S/O, and Ar/O appear to be universally constant and independent of
   metallicity, which argues either that the initial mass function (IMF) is
   universally constant or that these ratios are not sensitive to IMF variations.
   In the Milky Way, there is a rough age-metallicity trend with much scatter,
   in the sense that older stars are more metal poor.\par In elliptical galaxies,
   nuclear abundances are in the range [Z/H]=0.0-0.4, but the element mixture
   is not scaled-solar. In large elliptical galaxies [Mg/Fe] is in the range
   0.3-0.5, decreasing to {approx}0 in smaller elliptical galaxies. Other light
   elements track the Mg enhancement, but the heavier Ca tracks Fe. Velocity
   dispersion appears to be a key parameter in the modulation of [Mg/Fe], but
   the cause of the connection is unclear.
%K Galaxy: Abundances
%K Galaxy: Evolution
%K Galaxies: Abundances
%K Galaxies: Elliptical and Lenticular, cD
%K Galaxies: Evolution
%K Galaxies: ISM
%K Galaxies: Spiral
%K ISM: Abundances

%R 1999PASP..111..946E
%F ori/PASPv111n762
%J-953
%T KECK HIRES Spectroscopy of APM 08279+5255(1). (Research Note).
%A Ellison, Sara L. (2)
%A Lewis, Geraint F. (3)
%A Pettini, Max (2)
%A Sargent, Wallace L.W. (4)
%A Chaffee, Frederic H. (5)
%A Foltz, Craig B. (6)
%A Rauch, Michael (7)
%A Irwin, Mike J. (2)
%B  With an optical {\em R}-band magnitude of 15.2, the recently discovered
   z=3.911 broad absorption line quasar APM 08279+5255 is an exceptionally bright
   high-redshift source. Its brightness has allowed us to acquire a high signal-to-noise
   ratio (~80), high-resolution (~6 km.s^-1^) spectrum using the HIRES echelle
   spectrograph on the 10 m Keck I telescope. Given the quality of the data,
   these observations provide an unprecedented view of associated and intervening
   absorption systems. Here we announce the availability of this spectrum to
   the general astronomical community and present a brief analysis of some of
   its main features.
%K Galaxies: Quasars: Absorption Lines
%K quasars: individual (APM 08279+5255)
%I (1) The data presented herein were obtained at the W. M. Keck Observatory,
   which is operated as a scientific partnership among the California Institute
   of Technology, the University of California, and the National Aeronautics
   and Space Administration. The Observatory was made possible by the generous
   financial support of the W. M. Keck Foundation.
%I (2) Institute of Astronomy, Madingley Road, Cambridge CB3 0HA, England,
   UK; (sara@ast.cam.ac.uk).
%I (3) Fellow of the Pacific Institute of Mathematical Sciences 1998-1999,
   Department of Physics and Astronomy, University of Victoria, P.O. Box 3055,
   Victoria, BC V8W 3P6, Canada; and Astronomy Department, University of Washington,
   Box 351580, Seattle, WA 98195-1580.
%I (4) Palomar Observatory, Caltech 105-24, Pasadena, CA 91125.
%I (5) W. M. Keck Observatory, 65-1120 Mamalahoa Highway, Kamuela, HI 96743.
%I (6) MMT Observatory, University of Arizona, Tucson, AZ 85721.
%I (7) European Southern Observatory, Karl-Schwarzschild-Strasse 2, D-85748
   Garching bei Munchen, Germany.

%R 1999PASP..111..954K
%F ori/PASPv111n762
%J-963
%T Broad Absorption Line Quasars and the Radio-Loud/Radio-Quiet Dichotomy.
%A Kuncic, Zdenka (1)
%I Department of Physics and Astronomy, University of Victoria, Victoria, BC
   V8W 3P6, Canada
%B  The observation that the extremely broad, blueshifted absorption troughs
   which characterize broad absorption line quasars (BALQs) occur exclusively
   in radio-quiet quasars (RQQs) suggests that this class of active galactic
   nuclei (AGN) may offer important clues to the radio-loud/radio-quiet (RL/RQ)
   dichotomy in quasars. Interestingly, there is also substantial observational
   evidence for similar, but lower velocity, intrinsic absorption outflows in
   some Seyfert galaxies and radio-loud quasars (RLQs) as well. Theoretically,
   however, it is difficult to interpret this broad range of mass ejection phenomena
   in the context of the standard model for BALQs. Thus, a new model is considered
   here in which the thermal gas producing the blueshifted absorption troughs
   is associated with a poorly collimated outflow of weakly radio-emitting plasma--in
   essence, a weak jet. This model provides an appropriate framework not only
   for assessing the possible connection between the BAL phenomenon in RQQs
   and related intrinsic absorption outflows in stronger radio sources and in
   less luminous sources, both of which are known to possess jetlike radio structure,
   but also for understanding the RL/RQ dichotomy in light of recent observations
   which indicate that at least some RQQs possess central engines that are capable
   of producing weak versions of the powerful radio jets characteristic of RLQs.
   In the context of a weak jet model for BALQs, it is shown that observational
   constraints on the physical properties of the radio-emitting plasma are consistent
   with other theoretical arguments suggesting that the differences amongst
   RL and RQ sources can be attributed to jets with intrinsically different
   physical properties. Similarly, theoretical constraints on the physical properties
   of absorbing clouds embedded in weak jets are shown to be consistent with
   the properties directly inferred from the observed BAL troughs. Most importantly,
   however, it is argued that a weak jet model provides a successful explanation
   for the anticorrelation between the terminal velocity of the absorption outflow
   and the radio power of the quasar.
%K Galaxies: Active
%K Galaxies: Jets
%K Galaxies: Magnetic Fields
%K Galaxies: Quasars: General
%K Radio Continuum
%I (1) (zdenka@uvastro.phys.uvic.ca).

%R 1999PASP..111..964M
%F ori/PASPv111n762
%J-968
%T The Late-Time Light Curve of SN 1998bw Associated with GRB 980425.
%A McKenzie, Eric H. (1)
%A Schaefer, Bradley E. (2)
%I Department of Physics, Yale University, 260 Whitney Avenue, JWG 463, New
   Haven, CT 06520-8120
%B  We report 139 photometric observations through the {\em B}, {\em V},
   and {\em I} filters of the supernova SN 1998bw, an object which is associated
   with the gamma-ray burst GRB 980425. Detailed light curves of this unique
   supernova can be compared with theoretical models, so we report here our
   light curve for 123 days between 1998 June 27 and 1998 October 28. The light
   curve of SN 1998bw is consistent with those of the Type Ic class. We find
   that the magnitude versus time relation for this supernova is linear to within
   0.05 mag in all colors over the entire duration of our study. Our measured
   uniform decline rates are 0.0141+/-0.0002, 0.0184+/-0.0003, and 0.0181+/-0.0003
   mag per day in the {\em B}, {\em V}, and {\em I} bands. The linear decline
   and the rate of that decline suggest that the late-time light curve is powered
   by the radioactive decay of cobalt with some leakage of the gamma rays.
%K Gamma Rays
%K Stars: Supernovae: General
%K supernovae: individual (SN 1998bw)
%I (1) (eric.mckenzie@yale.edu).
%I (2) (schaefer@grb2.physics.yale.edu).

%R 1999PASP..111..969F
%F ori/PASPv111n762
%J-979
%T A Black Hole in the X-Ray Nova Velorum 1993.
%A Filippenko, Alexei V.
%A Leonard, Douglas C.
%A Matheson, Thomas
%A Li, Weidong
%A Moran, Edward C. (1)
%A Riess, Adam G.
%I Department of Astronomy, University of California, Berkeley, CA 94720-3411;
   (alex@astro.berkeley.edu), (dleonard@astro.berkeley.edu), (tmatheson@astro.berkeley.edu),
   (wli@astro.berkeley.edu), (emoran@astro.berkeley.edu), (ariess@astro.berkeley.edu)
%B  We have obtained 17 moderate-resolution (~2.5 {AA}) optical spectra of
   the Galactic X-ray Nova Velorum 1993 in quiescence with the Keck II telescope.
   Cross-correlation with the spectra of late-type dwarfs (especially K7-M0)
   yields excellent radial velocities for the secondary star. The orbital period
   ({\em P}) is 0.285206+/-0.0000014 days, and the semiamplitude (K_2_) is 475.4+/-5.9
   km.s^-1^. Our derived mass function, f(M_1_)=PK^3^_2_/2{pi}G=3.17+/-0.12 {\em
   M}_{sun}_, is close to the conventional absolute limiting mass for a neutron
   star (~3.0-3.2 {\em M}_{sun}_)--but if the orbital inclination i{<~}80{deg}
   (given the absences of eclipses), then M_1_{>~}4.2-4.4 {\em M}_{sun}_ for
   nominal secondary-star masses of 0.5 {\em M}_{sun}_ (M0) to 0.65 {\em M}_{sun}_
   (K6). Even if the secondary is quite undermassive (e.g., M_2_=0.3 {\em M}_{sun}_),
   we derive M_1_{>~}3.9 {\em M}_{sun}_. The primary star is therefore almost
   certainly a black hole rather than a neutron star.\par Fits to the wings
   of the double-peaked H{alpha} emission line yield approximate radial velocities
   for the compact primary. The velocity curve has a semiamplitude (K_1_) of
   65.3+/-7.0 km.s^-1^, but with a phase offset by 237{deg} (rather than 180{deg}) from
   that of the secondary star. Under the assumption that the observed semiamplitude
   reflects the motion of the primary (despite this offset, which is common),
   the mass ratio q=M_2_/M_1_=K_1_/K_2_=0.137+/-0.015, and hence for M_2_=0.5-0.65
   {\em M}_{sun}_ we derive M_1_=3.64-4.74 {\em M}_{sun}_. The constraints from
   {\em q} and the mass function yield M_1_=4.4 {\em M}_{sun}_ and i{approx}78{deg}
   if we use a normal K7-K8 secondary (M_2_{approx}0.6 {\em M}_{sun}_). Indeed,
   consistency cannot be achieved for M_2_{<~}0.59 {\em M}_{sun}_ if the maximum
   inclination estimate (80{deg}) is correct. An adopted mass M_1_{approx}4.4 {\em
   M}_{sun}_ is significantly below the typical value of ~7 {\em M}_{sun}_ found
   for black holes in other low-mass X-ray binaries.\par Keck observations of
   MXB 1659-29 (V2134 Oph) in quiescence reveal a probable optical counterpart
   at R=23.6+/-0.4 mag. This object recently went into a new X-ray and optical
   (R{approx}18 mag) outburst, after about 21 years of inactivity.
%K Stars: Binaries: Close
%K Stars: Novae, Cataclysmic Variables
%K stars: individual (Nova Velorum 1993, MXB 1659-29)
%K X-Rays
%I (1) Chandra Fellow.

%R 1999PASP..111..980S
%F ori/PASPv111n762
%J-985
%T Globular Cluster Winds Driven by Main-Sequence Stars.
%A Smith, Graeme H.
%I University of California Observatories/Lick Observatory, University of California,
   Santa Cruz, CA 95064; (graeme@ucolick.org)
%B  If Population II main-sequence stars have winds similar to the solar
   wind, then these stars could provide a feasible mechanism for expelling red-giant
   ejecta from globular clusters. For clusters having line-of-sight velocity
   dispersions less than 22 km.s^-1^, the mass and energy output of main-sequence
   star winds is found to be sufficient to establish a cluster outflow which
   is capable of removing all red-giant ejecta. This mechanism provides a natural
   means for continuously sweeping all or most globular clusters of stellar
   ejecta.
%K Galaxy: Globular Clusters: General
%K Stars: Mass Loss
%K Stars: Population II

%R 1999PASP..111..986R
%F ori/PASPv111n762
%J-989
%T {\em BVR} Photometry of Northern Hemisphere Luminous Stars. III. LS and HD
   Stars(1).
%A Reed, B.Cameron
%I Department of Physics, Alma College, Alma, MI 48801; (reed@alma.edu)
%A Reed, Laureen G.
%I Department of Physics, Saginaw Valley State University, University Center,
   MI 48710; (lgreed@svsu.edu)
%B  CCD-based {\em BVR} photometry of 48 previously unobserved stars drawn
   from volumes V and VI of the {\em Luminous Stars in the Northern Milky Way,
   Luminous Stars in the Southern Milky Way}, and HD catalogs is reported.
%K Stars: Early-Type
%I (1) This research was performed at the Lowell Observatory 31 inch telescope,
   which, under an agreement with Northern Arizona University and the NURO consortium,
   is operated 60% of the time as the National Undergraduate Research Observatory.

%R 1999PASP..111..990R
%F ori/PASPv111n762
%J-996
%T Filling Factor and Signal-to-Noise Ratios in Optical Interferometric Arrays.
%A Roddier, Fran\c{c}ois
%I Institute for Astronomy, 2680 Woodlawn Drive, Honolulu, HI 96822; (roddier@ifa.hawaii.edu)
   and
%A Ridgway, Stephen T.
%I National Optical Astronomical Observatories (1) 950 North Cherry Avenue,
   Tucson, AZ 85726; (ridgway@noao.edu)
%B  Signal-to-noise ratios are derived for an interferometric array of {\em
   N} diffraction-limited optical/IR telescopes with a Fizeau-type beam recombination.
   We consider two types of objects--extended sources and point sources--and three
   sources of noise--signal photon noise, sky background noise, and detector
   noise. We compare the results with that of a filled aperture, and also to
   that of an incoherent array, each with the same total collecting area. Implications
   are briefly discussed.
%K Instrumentation: Interferometers
%K Telescopes
%I (1) NOAO is operated by the Association of Universities for Research
   in Astronomy (AURA), under cooperative operating agreement with the National
   Science Foundation.

%R 1999PASP..111..997M
%F ori/PASPv111n762
%J-1008
%T NIRIM: A Dual-Purpose Near-Infrared (0.76-2.5 {mu}m) Imaging Camera for Wide-Field
   and High-Resolution Imaging.
%A Meixner, Margaret
%A Young Owl, Rolaine
%I Department of Astronomy, MC-221, University of Illinois, Urbana, IL 61801;
   (meixner@astro.uiuc.edu), (rolaine@astro.uiuc.edu)
%A Leach, Robert W.
%I Department of Astronomy, San Diego State University, San Diego, CA 92182;
   (leach@mintaka.sdsu.edu)
%B  We present the design and performance characteristics of the Near-Infrared
   Imager (NIRIM), which is a near-infrared camera operating in the 0.76-2.5
   {mu}m wavelength range. NIRIM is an example of a cost-effective way to expand
   two telescopes' capabilities to infrared wavelengths. NIRIM has been used
   for photometry and wide-field (8'.5x8'.5) imaging on our 1 m telescope at
   the Mount Laguna Observatory since 1995 August. In the future, NIRIM will
   also be used for high angular resolution imaging with the University of Illinois
   Seeing Improvement System (UnISIS), which is a laser guided adaptive optics
   system at the coud\'e focus of the Mount Wilson 2.5 m telescope.
%K Instrumentation: Photometers

%R 1999PASP..111.1009G
%F ori/PASPv111n762
%J-1020
%T Linearity and High Signal-to-Noise Performance of the STIS CCD(1).
%A Gilliland, Ronald L. (2)
%A Goudfrooij, Paul (2)(3)
%A Kimble, Randy A. (4)
%B  On-orbit data characteristics of the Space Telescope Imaging Spectrograph
   (STIS) CCD aboard the {\em Hubble Space Telescope} have been explored with
   early calibrations in a number of limiting conditions. At a gain of 4 {\em
   e}^-^ DN^-1^, STIS CCD data show excellent linearity at high count levels,
   even for extreme oversaturation of individual central pixels. At low count
   levels we interpret a position- and intensity-dependent nonlinearity in terms
   of charge transfer (in)efficiency in the parallel clocking direction and
   provide a simple model that accounts for this. A short time series of spectra
   was acquired at short-exposure times and high signal-to-noise ratio (S/N)
   on the binary system {alpha} Cen A and B enabling the shutter repeatability
   to be quantified at 0.0002 s. A direct demonstration of near-Poisson-limited
   time series with S/N>3000 is shown.
%K Instrumentation: Detectors
%K Methods: Data Analysis
%K Techniques: Photometric
%I (1) Based on observations with the NASA/ESA {\em Hubble Space Telescope},
   obtained at the Space Telescope Science Institute, which is operated by AURA,
   Inc., under NASA contract NAS5-26555.
%I (2) Space Telescope Science Institute, 3700 San Martin Drive, Baltimore,
   MD 21218; <gillil@stsci.edu>, <goudfroo@stsci.edu>.
%I (3) Affiliated to the Astrophysics Division, Space Science Department,
   European Space Agency.
%I (4) NASA Goddard Space Flight Center, Code 681, Greenbelt, MD 20771,
   <kimble@ccd.gsfc.nasa.gov>.

%R 1999PASP..111.1021S
%F ori/PASPv111n762
%J-1024
%T Spectral Gradients and {\em u}-{\em v} Sampling.
%A Swain, Mark R. (1)
%B  I describe a systematic method for characterizing the effects of differences
   in {\em u}-{\em v} coverage in terms of inferred spectral gradients in interferometric
   images. This method is directly applicable to optical and radio interferometry;
   it is useful in situations when observations using scaled arrays are not
   feasible.
%K Techniques: Image Processing
%K Techniques: Interferometric
%I (1) Jet Propulsion Laboratory, 4800 Oak Grove Drive, MS 171-113, Pasadena,
   CA 91109-8099; (swain@huey.jpl.nasa.gov).

%R 1999PASP..111.1025C
%F ori/PASPv111n762
%J-1047
%T The S2 VLBI Correlator: A Correlator for Space VLBI and Geodetic Signal Processing.
%A Carlson, B.R.
%A Dewdney, P.E.
%A Burgess, T.A.,
%A Casorso, R.V.
%I National Research Council of Canada, Herzberg Institute of Astrophysics,
   Dominion Radio Astrophysical Observatory, Penticton, BC V2A 6K3, Canada;
   (Brent.Carlson@hia.nrc.ca), (Peter.Dewdney@hia.nrc.ca)
%A Petrachenko, W.T.
%I Natural Resources Canada, Dominion Radio Astrophysical Observatory, Penticton,
   BC V2A 6K3, Canada; (Bill.Petrachenko@hia.nrc.ca) and
%A Cannon, W.H.
%I Space Geodynamics Laboratory, Center for Research in Earth and Space Technology,
   4850 Keele Street, North York, ON M3J 3K1, Canada; (wayne@sgl.crestech.ca)
%B  A unique lag-based VLBI correlator system has been developed for the
   purpose of supporting S2-based space VLBI observations in both the Japanese-led
   VSOP mission and the Canadian Geodetic VLBI program. The system architecture
   has been designed so that replication of a small number of modules can be
   used to construct systems with a wide range of sizes. Optimized for a large
   correlator, the design is ``station based'' in the sense that as many hardware
   and software functions as possible are performed before data are replicated
   and transmitted for baseline (station pair) processing. As well as delay
   compensation and generation of phase rotation coefficients, station-based
   functions include autocorrelation, tone extraction, pulsar gating, signal-statistics
   accumulation, and digital filtering. Doppler-shift correction (fringe stopping)
   is performed on a baseline basis {\em at each correlator lag} so that there
   are no smearing effects (lag-dependent loss of coherence) or frequency shifts
   that must otherwise be corrected after correlation. This is a key element
   that simplifies the baseline processing architecture when high accelerations
   associated with an orbiting antenna must be considered. Flexible, efficient
   distribution of data from station-based hardware to baseline-based hardware
   is accomplished by serializing the wide data paths to 1 Gbit.s^-1^ signals
   and using high-speed switches to route the signals to their final destinations
   where they are deserialized before cross-correlation. This greatly reduces
   the size, wiring complexity, and cost of the system. The interval between
   updates of the delay models, integration times, and other important events
   is typically 10 ms but can be as short as 1 ms. Within this period, delay
   and fringe model generation is performed using linear hardware synthesizers.
   The correlator also contains a number of unique signal processing functions
   that extend its capability beyond a basic VLBI correlator: flexible Local
   Oscillator frequency switching for bandwidth synthesis; rapid (1 ms) correlator
   dump intervals (allowing, for example, the study of some single-pulse pulsar
   characteristics on VLBI baselines); simple but powerful multirate digital
   signal-processing techniques to allow correlation of signals at different
   but related sample rates; and a digital ``zoom'' filter for producing very
   high resolution cross-power spectra. The correlator software, written almost
   entirely in C, is highly integrated into the system, supports all of the
   functions mentioned above, and is reconfigurable to support expansion of
   the correlator. The software schedules the use of hardware resources to enable
   correlation of multiple observations concurrently and automatically schedules
   the correlation of observations that require more than the available number
   of physical playback terminals. There is also substantial precorrelation
   consistency checking. The delay model is based on CALC for ground-based antennas
   and NAIF for space-based antennas. Output data are stored in the UVFITS format.
   The paper describes the design rationale, architecture, and function of the
   correlator and also provides specifications for the implemented system.
%K Instrumentation: Interferometers
%K Techniques: Interferometric
%K Techniques: Spectroscopic

%R 1999PASP..111.1048W
%F ori/PASPv111n762
%J-1048
%T Multicolor Classification in CADIS and the Search for Quasars. (Dissertation
   Summary).
%A Wolf, Chris
%I Current address: Max-Planck-Institut f\"ur Astronomie, K\"onigstuhl 17, D-69117
   Heidelberg, Germany; (cwolf@mpia-hd.mpg.de)Thesis work conducted at Max-Planck-Institut
   f\"ur Astronomie, Heidelberg, GermanyPh.D. thesis directed by H.-J. R\"oser;
   Ph.D. degree awarded 1999
%K Dissertation Summaries
%K Cosmology: Early Universe
%K Methods: Data Analysis
%K Galaxies: Quasars: General
%K Surveys
%K Techniques: Photometric
