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The dark matter density problem in massive disk galaxies
We discuss measurements of disk mass from non-circular streaming motionsof gas in the barred galaxies NGC 3095 and NGC 4123. In these galaxieswith strong shocks and non-circular motions, the inner regions must bedisk-dominated to reproduce the shocks. This requires dark matter halosof low central density and low concentration, compared to LCDM halopredictions. In addition, the baryonic collapse to a disk should havecompressed the halo and increased the dark matter density, whichsharpens the disagreement. One possible resolution is a substantialamount of angular momentum transfer from disk to halo, but this is notparticularly attractive nor elegant.
| Supernovae 2004ej and 2004ek
IAUC 8405 available at Central Bureau for Astronomical Telegrams.
| Morphological Type Dependence in the Tully-Fisher Relationship
The Tully-Fisher relationship is subject to morphological typedependence such that galaxies of morphology similar to Sc I galaxies andSeyfert galaxies are more luminous at a given rotational velocity thangalaxies of other morphological classification. This effect is mostprevalent in the B band. It is shown that the type effect is not simplyan artifact of the calibrator sample but is also present in clustersamples. The type effect is corrected by creating type-dependentTully-Fisher relations for Sc I group galaxies and Sb/Sc III groupgalaxies. It is shown that with single calibrations, the distances to ScI group galaxies are systematically underestimated, while the distancesto Sb/Sc III group galaxies are systematically overestimated.Tully-Fisher slope and scatter are also considered in the context oftype-dependent Tully-Fisher relations. It is concluded that the use oftype-dependent Tully-Fisher relations provides significant improvementin the distances to individual galaxies and the refined distances toclusters of galaxies.
| Mass Models for Spiral Galaxies from Two-dimensional Velocity Maps
We model the mass distributions of 40 high surface brightness spiralgalaxies inside their optical radii, deriving parameters of mass modelsby matching the predicted velocities to observed velocity maps. We useconstant mass-to-light disk and bulge models, and we have tried fitswith no halo and with three different halo density profiles. The datarequire a halo in most, but not all, cases, while in others the best fitoccurs with negligible mass in the luminous component, which we regardas unphysical. All three adopted halo profiles lead to fits of about thesame quality, and our data therefore do not constrain the functionalform of the halo profile. The halo parameters display large degeneraciesfor two of the three adopted halo functions, but the separate luminousand dark masses are better constrained. However, the fitted disk andhalo masses vary substantially between the adopted halo models,indicating that even high-quality two-dimensional optical velocity mapsdo not provide significant constraints on the dark matter content of agalaxy. We demonstrate that data from long-slit observations are likelyto provide still weaker constraints. We conclude that additionalinformation is needed in order to constrain the separate disk and halomasses in a galaxy.
| Dark halo properties from rotation curves
We study a large set of high spatial resolution optical rotation curvesof galaxies with the goal of determining the model parameters for a discembedded within a cold dark matter (CDM) halo, which we model witheither a Navarro-Frenk-White (NFW) profile or pseudo-isothermal profile.We show that parameter degeneracies present in lower resolution data arelifted at these higher resolutions. 34 per cent of the galaxies do nothave a meaningful fit when using the NFW profile and 32 per cent whenusing the pseudo-isothermal profile, however only 14 per cent do nothave a meaningful fit in either model. In both models we findcorrelations between the disc baryon fraction fd and the spinparameter of the halo λ', between fd and the dark halomass M200, and between M200 and the concentrationparameter c. We show that the distribution of the concentrationparameter c, for a NFW halo, is in good agreement with CDM predictions;no significant galaxy population is found with very low values of c. Theoverall distribution of λ' is in good agreement with theoreticalpredictions from hierarchical tidal torque theory. The whole sample isalso well fitted by a pseudo-isothermal dark halo with a core, but thesize of the core is rather small (6 per cent of the virial radius orsmaller; for 70 per cent of the sample the core size is less than 2kpc). Thus we conclude that the profile of dark matter is steep(r-1 or steeper) down to this radius; large dark matter cores(and therefore very low dark matter central densities) seem to beexcluded. Low-surface-brightness galaxies tend to have higher values ofλ' for a given fd and lower values of c for a givenmass than high-surface-brightness galaxies. In an appendix we give someuseful formulae for pseudo-isothermal profile haloes and we discuss indetail the issue of parameter degeneracies.
| The IRAS Revised Bright Galaxy Sample
IRAS flux densities, redshifts, and infrared luminosities are reportedfor all sources identified in the IRAS Revised Bright Galaxy Sample(RBGS), a complete flux-limited survey of all extragalactic objects withtotal 60 μm flux density greater than 5.24 Jy, covering the entiresky surveyed by IRAS at Galactic latitudes |b|>5°. The RBGS includes629 objects, with median and mean sample redshifts of 0.0082 and 0.0126,respectively, and a maximum redshift of 0.0876. The RBGS supersedes theprevious two-part IRAS Bright Galaxy Samples(BGS1+BGS2), which were compiled before the final(Pass 3) calibration of the IRAS Level 1 Archive in 1990 May. The RBGSalso makes use of more accurate and consistent automated methods tomeasure the flux of objects with extended emission. The RBGS contains 39objects that were not present in the BGS1+BGS2,and 28 objects from the BGS1+BGS2 have beendropped from RBGS because their revised 60 μm flux densities are notgreater than 5.24 Jy. Comparison of revised flux measurements forsources in both surveys shows that most flux differences are in therange ~5%-25%, although some faint sources at 12 and 25 μm differ byas much as a factor of 2. Basic properties of the RBGS sources aresummarized, including estimated total infrared luminosities, as well asupdates to cross identifications with sources from optical galaxycatalogs established using the NASA/IPAC Extragalactic Database. Inaddition, an atlas of images from the Digitized Sky Survey with overlaysof the IRAS position uncertainty ellipse and annotated scale bars isprovided for ease in visualizing the optical morphology in context withthe angular and metric size of each object. The revised bolometricinfrared luminosity function, φ(Lir), forinfrared-bright galaxies in the local universe remains best fit by adouble power law, φ(L)~Lα, withα=-0.6(+/-0.1) and α=-2.2(+/-0.1) below and above the``characteristic'' infrared luminosityL*ir~1010.5Lsolar,respectively. A companion paper provides IRAS High Resolution (HIRES)processing of over 100 RBGS sources where improved spatial resolutionoften provides better IRAS source positions or allows for deconvolutionof close galaxy pairs.
| Homogenization of the Stellar Population along Late-Type Spiral Galaxies
We present a study of the broadband UBV color profiles for 257 Sbcbarred and nonbarred galaxies, using photoelectric aperture photometrydata from the literature. Using robust statistical methods, we haveestimated the color gradients of the galaxies, as well as the total andbulge mean colors. A comparative photometric study using CCD images wasdone. In our sample, the color gradients are negative (reddish inward)in approximately 59% of the objects, are almost null in 27%, and arepositive in 14%, considering only the face-on galaxies, which representapproximately 51% of the sample. The results do not change, essentially,when we include the edge-on galaxies. As a consequence of this study wehave also found that barred galaxies are overrepresented among theobjects having null or positive gradients, indicating that bars act as amechanism of homogenization of the stellar population. This effect ismore evident in the U-B color index, although it can also be detected inthe B-V color. A correlation between the total and bulge colors wasfound that is a consequence of an underlying correlation between thecolors of bulges and disks found by other authors. Moreover, the meantotal color is the same irrespective of the gradient regime, whilebulges are bluer in galaxies with null or positive gradients, whichindicates an increase of the star formation rate in the central regionsof these objects. We have also made a quantitative evaluation of theamount of extinction in the center of these galaxies. This was doneusing the Wide Field Planetary Camera 2 (WFPC2) and the Near InfraredCamera and Multi-Object Spectrometer (NICMOS) Hubble Space Telescope(HST) archival data, as well as CCD B, V, and I images. We show thatalthough the extinction in the V-band can reach values up to 2 mag inthe central region, it is unlikely that dust plays a fundamental role inglobal color gradients. We found no correlation between color and O/Habundance gradients. This result could suggest that the color gradientsare more sensitive to the age rather than to the metallicity of thestellar population. However, the absence of this correlation may becaused by dust extinction. We discuss this result by considering apicture in which bars are a relatively fast, recurrent phenomenon. Theseresults are not compatible with a pure classical monolithic scenario forbulge and disk formation. On the contrary, they favor a scenario inwhich both these components are evolving in a correlated process inwhich stellar bars play a crucial role. Based partly on observationsmade at the Pico dos Dias Observatory (PDO/LNA-CNPq), Brazil.
| Maximum Disk Mass Models for Spiral Galaxies
We present axisymmetric maximum disk mass models for a sample of 74spiral galaxies taken from the southern sky Fabry-Perot Tully-Fishersurvey by Schommer et al. The sample contains galaxies spanning a largerange of morphologies and having rotation widths from 180 km s-1 to 680 km s -1. For each galaxy we have an I-bandimage and a two-dimensional Hα velocity field. We decompose thedisk and bulge by fitting models directly to the I-band image. Thismethod utilizes both the distinct surface brightness profiles and shapesof the projected disk and bulge in the galaxy images. The luminosityprofiles and rotation curves are derived using consistent centers,position angles, and inclinations derived from the photometry andvelocity maps. The distribution of mass is modeled as a sum of disk andbulge components with distinct, constant mass-to-light ratios. No darkmatter halo is included in the fits. The models reproduce the overallstructure of the rotation curves in the majority of galaxies, providinggood fits to galaxies that exhibit pronounced structural differences intheir surface brightness profiles. Of galaxies for which the rotationcurve is measured to R23.5 or beyond 75% are well fitted by amass-traces-light model for the entire region within R23.5.The models for about 20% of the galaxies do not fit well; the failure ofmost of these models is traced directly to nonaxisymmetric structures,primarily bars but also strong spiral arms. The median I-band M/L of thedisk plus bulge is 2.4+/-0.9 h75 in solar units, consistentwith normal stellar populations. These results require either that themass of dark matter within the optical disk of spiral galaxies is smallor that its distribution is very precisely coupled to the distributionof luminous matter.
| Stars, H II regions, and shocked gas in the bar of NGC 1530
We analyse long slit spectra taken along and perpendicular to the bar ofthe galaxy NGC 1530. Our data show that the H ii regions, around youngmassive stars that form in the shock-compressed gas, share the samekinematics as the molecular gas in the x_2 orbits at the center of thegalaxy. Along the bar, the H ii regions are in the post-shock zone,downstream of the dust lanes that contain molecular gas. Outside of theH ii regions in the bar is faint, diffuse, ionized gas with a lowHα / [NII] and Hα / [SII] line ratio, which confirms thepresence of shocks in the bar and supports a shock origin of the dustlanes. The measured spatial variation of the Hα and [NII] lineintensity is consistent with the distribution of molecular gas along thedust lanes and its high concentration near the first inner Lindbladresonance. From an I-B image, we derive the surface brightness along thebar which we interpret as the stellar distribution. We use these data toestimate the mass in the various structural components of the bar. Themass of the stars and gas in the bar is 4x 10(10) M_sun, or 12% of thetotal mass of the galaxy.
| 3D self-consistent N-body barred models of the Milky Way. II. Gas dynamics
The gas dynamics in the Galactic disc is modeled by releasing aninitially axisymmetric SPH component in a completely self-consistent andsymmetry-free 3D N-body simulation of the Milky Way in which the stellarcomponents display a COBE-like bar. The density centre of the stellarbar wanders around the centre of mass and the resulting gas flow isasymmetric and non-stationary, reproducing the HI and CO l-V diagramsonly at specific times and thus suggesting a transient nature of theobserved inner gas kinematics. The best matching models allow a new andcoherent interpretation of the main features standing out of the l-Vdata within the bar region. In particular, the l-V traces of theprominent offset dustlanes leading the bar major axis in early-typebarred spirals can be unambiguously identified, and the 3-kpc arm andits non-symmetric galactocentric opposite counterarm are the innerprolongations of disc spiral arms passing round the bar and joining thedustlanes at very different galactocentric distances. Bania's clump 1and 2, and another velocity-elongated feature near l= 5.5degr , areinterpreted as gas lumps crossing the dustlane shocks. The terminalvelocity peaks near l=+/- 2.5degr are produced by gas along thedustlanes and not by the trace of the cusped x_1 orbit, which passesfarther away from the Galactic centre. According to these models and torelated geometrical constraints, the Galactic bar must have aninclination angle of 25degr +/- 4degr , a corotation radius of 4.0-4.5kpc and a face-on axis ratio b/a~ 0.6.
| Bulge-Disk Decomposition of 659 Spiral and Lenticular Galaxy Brightness Profiles
We present one of the largest homogeneous sets of spiral and lenticulargalaxy brightness profile decompositions completed to date. The 659galaxies in our sample have been fitted with a de Vaucouleurs law forthe bulge component and an inner-truncated exponential for the diskcomponent. Of the 659 galaxies in the sample, 620 were successfullyfitted with the chosen fitting functions. The fits are generally welldefined, with more than 90% having rms deviations from the observedprofile of less than 0.35 mag. We find no correlations of fittingquality, as measured by these rms residuals, with either morphologicaltype or inclination. Similarly, the estimated errors of the fittedcoefficients show no significant trends with type or inclination. Thesedecompositions form a useful basis for the study of the lightdistributions of spiral and lenticular galaxies. The object base issufficiently large that well-defined samples of galaxies can be selectedfrom it.
| Total magnitude, radius, colour indices, colour gradients and photometric type of galaxies
We present a catalogue of aperture photometry of galaxies, in UBVRI,assembled from three different origins: (i) an update of the catalogueof Buta et al. (1995) (ii) published photometric profiles and (iii)aperture photometry performed on CCD images. We explored different setsof growth curves to fit these data: (i) The Sersic law, (ii) The net ofgrowth curves used for the preparation of the RC3 and (iii) A linearinterpolation between the de Vaucouleurs (r(1/4) ) and exponential laws.Finally we adopted the latter solution. Fitting these growth curves, wederive (1) the total magnitude, (2) the effective radius, (3) the colourindices and (4) gradients and (5) the photometric type of 5169 galaxies.The photometric type is defined to statistically match the revisedmorphologic type and parametrizes the shape of the growth curve. It iscoded from -9, for very concentrated galaxies, to +10, for diffusegalaxies. Based in part on observations collected at the Haute-ProvenceObservatory.
| Two modes of gas flow in a single barred galaxy
We investigate stationary gas flows in a fixed, rotating barredpotential. The gas is assumed to be isothermal with an effective soundspeed c_s, and the equations of motion are solved with smoothed particlehydrodynamics (SPH). Since the thermal energy in cloud random motions isnegligible compared with the orbital kinetic energy, no dependence ofthe flow on c_s is expected. However, this is not the case when shocksare involved. For low values of c_s an open, off-axis shock flow formsthat is characteristic for potentials with an inner Lindblad resonance(ILR). Through this shock the gas streams inwards from x_1- tox_2-orbits. At high sound speeds the gas arranges itself in a different,on-axis shock flow pattern. In this case, there is no gas on x_2-orbits,demonstrating that the gas can behave as if there were no ILR. Thecritical effective sound speed dividing the two regimes is in the rangeof values observed in the Milky Way. We give a heuristic explanation forthis effect. A possible consequence is that star formation may changethe structure of the flow by which it was initiated. Low-mass galaxiesshould predominantly be in the on-axis regime. A brief comparison of ourSPH results with those from a grid-based hydrodynamic code is alsogiven.
| The I band Tully-Fisher relation for cluster galaxies: data presentation.
Observational parameters which can be used for redshift-independentdistance determination using the Tully-Fisher (TF) technique are givenfor \ntot spiral galaxies in the fields of 24 clusters or groups. I bandphotometry for the full sample was either obtained by us or compiledfrom published literature. Rotational velocities are derived either from21 cm spectra or optical emission line long-slit spectra, and convertedto a homogeneous scale. In addition to presenting the data, a discussionof the various sources of error on TF parameters is introduced, and thecriteria for the assignment of membership to each cluster are given.
| Scaleheights of 486 southern spiral galaxies and some statistical correlation
Based on Peng's method (1988), we obtain scaleheights of 486 southernspiral galaxies, the images of which are taken from the Digitized SkySurvey at Xinglong Station of Beijing Astronomical Observatory. Thefitted spiral arms of 70 galaxies are compared with their images to gettheir optimum inclinations. The scaleheights of other 416 ones arelisted in Table A1 in Appendix. After compiling and analyzing the data,we find some statistical correlations. The most interesting results arethat a flatter galaxy is bluer and looks brighter, and galaxies becomeflatter along the Hubble sequence Sab -- Scd. Based on photographic dataof the National Geographic Society -- Palomar Observatory Sky Survey(NGS-POSS) obtained using the Oschin Telescope Palomar Mountain. TheNGS-POSS was funded by a grant from the National Geographic Society tothe California Institute of Technology. The plates were processed intothe present compressed digital form with their permission. The DigitizedSky Survey was produced at the Space Telescope Science Institute underUS Government grant NAG W-2166. Table A1 is available in electronic fromonly, via anonymous ftp 130.79.128.5 orhttp://cdsweb.u-strasbg.fr/Abstract.html
| Parameters of 2447 Southern Spiral Galaxies for Use in the Tully-Fisher Relation
I-band luminosities, rotational velocities, and redshifts of 1092 spiralgalaxies have been measured by CCD photometry and Hα spectroscopyusing the 1 m and 2.3 m telescopes at Siding Spring Observatory,respectively. The results are tabulated. Luminosity profiles andHα rotation curves are given for the galaxies. When these resultsare combined with similar data for 1355 spiral galaxies publishedpreviously (Mathewson, Ford, & Buchhorn, hereafter Paper I), itprovides a large, uniform, and unique data set with which to measure,via the Tully-Fisher relation, the peculiar velocities of galaxies inthe local universe to a distance of 11,000 km s^-1^ (Mathewson &Ford). Taking advantage of the opportunity for publishing this data inmachine-readable form, in the CD-ROM, we have also included similar datafor the 1355 galaxies in Paper I.
| A 1.425 GHz Atlas of the IRAS Bright Galaxy Sample, Part II
Galaxies with δ >= -45^deg^ and |b| >= 10^deg^ in the IRASBright Galaxy Sample, Part II, were observed at 1.425 GHz by the VeryLarge Array in its B, CnB, C, DnC, and D configurations. An atlas ofradio contour maps and a table listing the principal radio sourceparameters (position, flux density, angular size) are given. This atlasof 187 galaxies supplements the 1.49 GHz atlas of 313 galaxies in therevised Bright Galaxy Sample, Part I. Together, they are complete forextragalactic sources stronger than S = 5.24Jy at λ = 60 micronsin the area |b| > 10^deg^, δ > -45^deg^. To the extent thatthe far-infrared and radio brightness distributions overlap, these radiomaps provide the most accurate positions and high-resolution images ofthe brightest extragalactic far-infrared sources.
| The Catalog of Southern Ringed Galaxies
The Catalog of Southern Ringed Galaxies (CSRG) is a comprehensivecompilation of diameters, axis ratios, relative bar position angles, andmorphologies of inner and outer rings, pseudorings, and lenses in 3692galaxies south of declination -17 deg. The purpose of the catalog is toevaluate the idea that these ring phenomena are related to orbitalresonances with a bar or oval in galaxy potentials. The catalog is basedon visual inspection of most of the 606 fields of the Science ResearchCouncil (SRC) IIIa-J southern sky survey, with the ESO-B, ESO-R, andPalomar Sky surveys used as auxiliaries when needed for overexposed coreregions. The catalog is most complete for SRC fields 1-303 (mostly southof declination -42 deg). In addition to ringed galaxies, a list of 859mostly nonringed galaxies intended for comparison with other catalogs isprovided. Other findings from the CSRG that are not based on statisticsare the identification of intrinsic bar/ring misalignment; bars whichunderfill inner rings; dimpling of R'1pseudorings; pointy, rectangular, or hexagonal inner or outer ringshapes; a peculiar polar-ring-related system; and other extreme examplesof spiral structure and ring morphology.
| The IRAS Bright Galaxy Survey - Part II: Extension to Southern Declinations (delta ~< -30), and Low Galactic Latitudes (f<|b|
Complete IRAS Observations and redshifts are reported for all sourcesidentified in the IRAS Bright Galaxy Survey-Part II (hereafter referredto as BGS_2_). Source positions, radial velocities, optical magnitudes,and total flux densities, peak flux densities, and spatial extents at12, 25, and 100 ,microns are reported for 288 sources having 60 micronflux densities > 5.24 Jy, the completeness limit of the originalBright Galaxy Survey [Soifer et al., AJ, 98,766(1989)], hereafterreferred to as BGS_1_. These new data represent the extension of theIRAS Bright Galaxy Survey to southern declinations,δ<~-30^deg^, and low Galactic latitudes,5^deg^<|b|<30^deg^. Although the sky coverage of the BGS_2_ (~19935 deg^2^) is 37% larger than the sky coverage of the BGS_1_, thenumber of sources is 8% smaller due primarily to large scale structurein the local distribution of galaxies. Otherwise, the sources in theBGS_2_ show similar relationships between number counts and flux densityas observed for the 313 sources in the BGS_1_. The BGS_2_ along with theearlier BGS, represents the best sample currently available for definingthe infrared properties of galaxies in the local (z <~ 0.1) Universe.
| Velocity Fields of Barred Spiral Galaxies from Fabry-Perot Observations
We present 2-dimensional velocity fields of gas in the barred spiralgalaxies NGC 1832 and NGC 3095, obtained by mapping the Hα emissionline with the Rutgers Imaging Fabry-Perot Interferometer at CTIO. Thedata for each galaxy are 12--15 narrow-band images spaced across theHα emission line, separated by approximately 1 Angstroms (50 \kms).For each pixel, we thus have measurements of the flux as a function ofwavelength, to which we fit a line profile, obtaining the continuum,intensity, wavelength, and kinetic broadening of the line. In regions ofstrong \ha\ emission we obtain velocity precision of 5 \kms\ and spatialresolution of 1\arcsec--2\arcsec, limited only by the seeing. In regionsof diffuse emission we average the data spatially to obtain precision of~ 15 \kms\ at spatial resolution of 3\arcsec--4\arcsec; this allows usto obtain velocities over the full extent of the disk. The velocityfields show global deviations from axisymmetry, exhibiting the S-shapedisovelocity contours characteristic of barred disk galaxies. These datawill enable us to constrain mass models of barred spirals, throughfluid-dynamical simulations of the gas flow. The maps also revealdynamically interesting small-scale velocity structure. In NGC 3095, weobtain velocities from diffuse \ha\ emission over the entire bar. Directimaging shows typical straight, offset dust lanes along the bar; wedetect a strong velocity gradient (100-150 \kms\ over 3\arcsec) acrossthe width of the bar, coincident with the dust lanes. This providesevidence that dust lanes in bars are the locations of shocks. In theinner bulge of NGC 1832, we have detected a fast-rotating, nuclear ringstructure of intense \ha\ emission. The B-band image and the continuumat \ha\ show a smooth, centrally-peaked bulge, but the \ha\ intensitymap reveals a ring of radius 0.8'' (70h(-1) pc if the galaxy is at itsHubble distance) with the line-of-sight component of the rotationvelocity equal to 100 \kms. We conjecture that this gas has sunk to thecenter of the bulge due to outward angular momentum transport by thebar.
| IRAS CPC Observations of Galaxies - Part One - Catalog and Atlas
. - We present the results of far-infrared imaging observations of 258regions of 12' x9' each centered on a selected individual galaxy, aclose pair, or a compact group of galaxies mapped at 50 and 100 micronwavelength with the CPC instrument of the IRAS satellite. The CPCinstrument has a significantly better resolution than the IRAS Surveyinstrument at these wavelengths, i.e. a round beam with a FWHM of about80" at 50 microns and 95" at 100 microns, respectively, intended to bematched to the diffraction limit of the telescope at 100 microns. Themaps were made using a new algorithm to correct for gain variations,which gives better results than the one used previously for the imagesmade available on tape in 1985. Of 262 objects observed, 167 and 188were detected at 50 and 100 microns, respectively, about 85% of thegalaxies from the same sample listed as detected by the Surveyinstrument in the IRAS Point Source Catalog. For all 55 galaxiesresolved (i.e. with a FWHM major axis diameter exceeding 1.6 times thebeam FWHM and/or extended lower-level emission) by the CPC we alsopresent the averaged maps at 50 and 100 microns. These 55 objectsinclude 35 for which there are no published maps obtained with the IRASSurvey instrument. We rescaled the flux densities of the published CPCmaps using the more accurate IRAS Survey instrument data, since theabsolute flux density calibration of the CPC is only accurate to about+/-60%. We also present images of a triplet of galaxies associated witha single Survey point source, which were resolved into separate sourcesby the CPC.
| General study of group membership. II - Determination of nearby groups
We present a whole sky catalog of nearby groups of galaxies taken fromthe Lyon-Meudon Extragalactic Database. From the 78,000 objects in thedatabase, we extracted a sample of 6392 galaxies, complete up to thelimiting apparent magnitude B0 = 14.0. Moreover, in order to considersolely the galaxies of the local universe, all the selected galaxieshave a known recession velocity smaller than 5500 km/s. Two methods wereused in group construction: a Huchra-Geller (1982) derived percolationmethod and a Tully (1980) derived hierarchical method. Each method gaveus one catalog. These were then compared and synthesized to obtain asingle catalog containing the most reliable groups. There are 485 groupsof a least three members in the final catalog.
| A southern sky survey of the peculiar velocities of 1355 spiral galaxies
The paper presents data from photometric and spectroscopic observationsof 1355 southern spiral galaxies and uses them to determine theirdistances and peculiar velocities via the Tully-Fisher (TF) relation.I-band CCD surface photometry was carried out using the 1-m and 3.9-mtelescopes at Siding Spring Observatory. H-alpha rotation curves for 965galaxies and 551 H I profiles are presented. The physical parameters,photometric and velocity data, distances, and peculiar velocities of thegalaxies are presented in tabular form. The mean distance, systemicvelocity, and average peculiar velocity of 24 clusters in the sample aregiven. TF diagrams are presented for each cluster.
| Groups of galaxies within 80 Mpc. II - The catalogue of groups and group members
This paper gives a catalog of the groups and associations obtained bymeans of a revised hierarchical algorithm applied to a sample of 4143galaxies with diameters larger than 100 arcsec and redshifts smallerthan 6000 km/s. The 264 groups of galaxies obtained in this way (andwhich contain at least three sample galaxies) are listed, with the looseassociations surrounding them and the individual members of eachaggregate as well; moreover, the location of every entity among 13regions corresponding roughly to superclusters is specified. Finally,1729 galaxies belong to the groups, and 466 to the associations, i.e.,the total fraction of galaxies within the various aggregates amounts to53 percent.
| The Hubble relation - Differences between galaxy types SB and SC
It is shown that the Sb galaxies have apparent magnitudes which varyalmost exactly as if their redshifts were a measure of the distance atwhich they are observed, while the Sc do not exhibit a linear Hubblerelation. An attempt is made to determine whether the Sc discordancefrom the Hubble law is caused by Malmquist bias operating in thisfainter luminosity class of galaxies or there are inherent fundamentalpeculiarities. To this purpose the search is undertaken for other kindsof galaxies physically associated which these deviating Sc's. It isshown that luminosity criterion (Tully-Fisher) gives much smallerdistances for these galaxies than their redshifts do. The interaction ofspecific high redshift ScI's with nearby galaxies is presented as anindependent proof that ScI's are generally small, low luminositygalaxies.
| Models for infrared emission from IRAS galaxies
The far-infrared spectra of galaxies detected in four wavelength bandsby IRAS have been modeled in terms of a cool disk component, a warmerstarburst component, and a Seyfert component peaking at 25 microns.Although the models are found to fit the observed spectra of non-Seyfertand several Seyfert galaxies, a more complex geometry for the dustdistribution is indicated for NGC 1068 and many other Seyfert galaxies.In some cases, the dust in the narrow-line region has a nonsphericallysymmetric geometry.
| A search for megamaser galaxies
The results of a search for OH megamaser emission from a sample of 32galaxies selected from the IRAS Point Source Catalog on the basis oftheir IR properties are presented. For each galaxy (other than those fewalready observed elsewhere), an optical redshift is obtained and both OHand H I emission are sought. The search yielded one new OH megamasergalaxy, and H I was detected toward nine objects. There are unlikely tobe any OH megamasers in the Southern Hemisphere with flux densitiescomparable to that of Arp 220 (280 mJy), although there may be apopulation of weaker megamasers. No special conditions are required toexplain the known OH megamasers other than those expected in a cool,dusty, active galaxy.
| Revised supernova rates in Shapley-Ames galaxies
Observations of 855 Shapley Ames galaxies made from November 1, 1980 toOctober 31, 1988, together with improved supernova luminosities, havebeen used to derive the frequency of supernovae of different types, andthe results are presented in tables. From a uniform database of 24supernovae discovered, the following SN rates are found, expressed in SNper century per 10 to the 10th L(B)(solar): SN Ia, 0.3; SN Ib, 0.3; andSN II, 1.0. The present data confirm the relatively high frequency of SNII in late-type galaxies that has been found by many previousinvestigators.
| The peculiar velocity of the Local Group. II - H I observations of SC galaxies
H I observations of a sample of 163 Sc galaxies have been obtained usingthe Mk IA and Mk II Jodrell Bank radio telescopes. In the presentanalysis, the overall rms error in redshift determination is 5 km/s andthe rms error in velocity width determination is 10 km/s. The resultssuggest that Sc galaxies have high internal obscuration and may beoptically thicker in blue light than earlier-type spirals. An orthogonalthree-dimensional classification system based on three uncorrelatedparameters related to linear diameter, quiescent star-formation rate,and embedded starburst-type activity is shown to account for the globalproperties of Sc galaxies with an accuracy close to the limit ofmeasurement error.
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