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Rejuvenation of spiral bulges
We seek to understand whether the stellar populations of galactic bulgesshow evidence of secular evolution triggered by the presence of thedisc. For this purpose, we re-analyse the sample of Proctor and Sansom,deriving stellar population ages and element abundances fromabsorption-line indices as functions of central velocity dispersion andHubble type. We obtain consistent constraints on ages from the threeBalmer-line indices Hβ, Hγ and Hδ, based on stellarpopulation models that take the abundance ratio effects on these indicesinto account. Emission-line contamination turns out to be a criticalaspect, which favours the use of the higher order Balmer-line indices.Our derived ages are consistent with those of Proctor and Sansom basedon a completely different method. In agreement with other studies in theliterature, we find that bulges have relatively low luminosity weightedages, the lowest age derived being 1.3Gyr. Hence, bulges are notgenerally old, but actually rejuvenated systems. We discuss evidencethat this might be true also for the bulge of the Milky Way. The datareveal clear correlations of all three parameters luminosity weightedage, total metallicity and α/Fe ratio with central velocitydispersion. The smallest bulges are the youngest with the lowestα/Fe ratios owing to late Fe enrichment from Type Ia supernovae.Using models combining recent minor star formation with a base oldpopulation, we show that the smallest bulges must have experiencedsignificant star formation events involving 10-30 per cent of theirtotal mass in the past 1-2Gyr. No significant correlations of thestellar population parameters with Hubble type are found. We show thatthe above relationships with σ coincide perfectly with those ofearly-type galaxies. In other words, bulges are typically younger, metalpoorer and less α/Fe enhanced than early-type galaxies because oftheir smaller masses. At a given velocity dispersion, bulges andelliptical galaxies are indistinguishable as far as their stellarpopulations are concerned. These results favour an inside-out formationscenario and indicate that the discs in spiral galaxies of Hubble typesSbc and earlier cannot have a significant influence on the evolution ofthe stellar populations in the bulge component. The phenomenon ofpseudo-bulge formation must be restricted to spirals of types later thanSbc.

Objective Classification of Spiral Galaxies Having Extended Rotation Curves Beyond the Optical Radius
We carry out an objective classification of four samples of spiralgalaxies having extended rotation curves beyond the optical radius. Amultivariate statistical analysis (viz., principal component analysis[PCA]) shows that about 96% of the total variation is due to twocomponents, one being the combination of absolute blue magnitude andmaximum rotational velocity beyond the optical region and the otherbeing the central density of the halo. On the basis of PCA a fundamentalplane has been constructed that reduces the scatter in the Tully-Fisherrelation up to a maximum of 16%. A multiple stepwise regression analysisof the variation of the overall shape of the rotation curves shows thatit is mainly determined by the central surface brightness, while theshape purely in the outer part of the galaxy (beyond the optical radius)is mainly determined by the size of the galactic disk.

A new method to determine the thickness of non-edge-on disk galaxies
Aims.We present a new method to determine the thickness of non-edge-ondisk galaxies. This method allows us to investigate the mass-to-lightratio of the disk. Methods: .Our method is based on the comparisonof observations and theory of the distribution of the vertical velocitydispersion, which is obtained from the solution of three dimensionalPoisson equations and the galactic dynamical equation. Results:.As examples, the thickness and mass-to-light ratio of two diskgalaxies, NGC 1566 and NGC 5247, which have been extensively studied byspectroscopy, have been calculated. The calculated results areconsistent with observations and support the use of this method.However, due to the small sample size available, the results should beconfirmed on other samples of galaxies.

The Baryonic Tully-Fisher Relation of Galaxies with Extended Rotation Curves and the Stellar Mass of Rotating Galaxies
I investigate the baryonic Tully-Fisher relation for a sample ofgalaxies with extended 21 cm rotation curves spanning the range 20 kms-1<~Vf<=300 km s-1. A variety ofscalings of the stellar mass-to-light ratio Υ* areconsidered. For each prescription for Υ*, I give fitsof the form Md=AVxf.Presumably, the prescription that comes closest to the correct valuewill minimize the scatter in the relation. The fit with minimum scatterhas A=50 Msolar km-4 s4 andx=4. This relation holds over five decades in mass. Galaxy color,stellar fraction, and Υ* are correlated with eachother and with Md, in the sense that more massivegalaxies tend to be more evolved. There is a systematic dependence ofthe degree of maximality of disks on surface brightness. High surfacebrightness galaxies typically have Υ*~3/4 of themaximum disk value, while low surface brightness galaxies typicallyattain ~1/4 of this amount.

Star Formation Thresholds and Galaxy Edges: Why and Where
We study global star formation thresholds in the outer parts of galaxiesby investigating the stability of disk galaxies embedded in dark halos.The disks are self-gravitating, contain metals and dust, and are exposedto UV radiation. We find that the critical surface density for theexistence of a cold interstellar phase depends only weakly on theparameters of the model and coincides with the empirically derivedsurface density threshold for star formation. Furthermore, it is shownthat the drop in the thermal velocity dispersion associated with thetransition from the warm to the cold gas phase triggers gravitationalinstability on a wide range of scales. The presence of strong turbulencedoes not undermine this conclusion if the disk is self-gravitating.Models based on the hypothesis that the onset of thermal instabilitydetermines the star formation threshold in the outer parts of galaxiescan reproduce many observations, including the threshold radii, thecolumn densities, and the sizes of stellar disks as a function of diskscale length and mass. Finally, prescriptions are given for implementingstar formation thresholds in (semi-)analytic models andthree-dimensional hydrodynamical simulations of galaxy formation.

Galaxy Interaction and the Starburst-Seyfert Connection
Galaxy interactions are studied in terms of the starburst-Seyfertconnection. The starburst requires a high rate of gas supply. Since theefficiency for supplying the gas is high in a galaxy interaction,although the companion is not necessarily discernible, Seyfert galaxieswith circumnuclear starbursts are expected to be interacting. Since thelarge amounts of circumnuclear gas and dust obscure the broad-lineregion, they are expected to be observed as Seyfert 2 galaxies. Theactive galactic nucleus itself does not require a high rate of gassupply. Seyfert galaxies without circumnuclear starbursts are notnecessarily expected to be interacting even at the highest luminosities.They are not necessarily expected to evolve from Seyfert galaxies withcircumnuclear starbursts. We derive these and other theoreticalexpectations and confirm them with statistics on observational data ofmagnitude-limited samples of Seyfert galaxies.

Hubble Space Telescope Imaging of Extraplanar Dust Structures in the Edge-On Spiral NGC 4217
We present high-resolution (~ 0.1") B, V, and I images of the edge-on Sbgalaxy NGC 4217 obtained with the Wide Field Planetary Camera 2 (WFPC2)on-board the Hubble Space Telescope (HST). We make use of these imagesto study extraplanar (z>0.4 kpc) dust structures visible inabsorption against the background stellar light of the galaxy, similarto those observed previously in NGC 891 and other spiral galaxies byHowk & Savage. The HST images of NGC 4217 reveal extensive high-zdust to both sides of its midplane. The dust structures have a range ofmorphologies, and some of the more tenuous features are traceable toheights ~2 kpc from the midplane. We investigate the physical propertiesof 12 individual features. We measure the apparent optical extinctionsof the features and use these to infer the hydrogen column densities andmasses of the structures. The extraplanar dust structures in NGC 4217typically have NH>~4×1020cm-2, with associated gas masses estimated to be>~2×105 Msolar, assuming Milky Waygas-to-dust relationships apply to this spiral galaxy. The energyrequirements for the expulsion of such massive structures into the lowerhalo are large; the gravitational potential energies of similarindividual structures in NGC 891 (>1052 ergs) represent theenergy input of at least tens of supernovae. The morphologies of some ofthe extraplanar dust structures in NGC 4217 suggest supernova-drivengalactic fountain or chimney phenomena may be responsible for theirproduction. Other features at high-z are not readily linked to energeticprocesses in the disk.Based on observations with the NASA/ESA Hubble Space Telescope, obtainedat the Space Telescope Science Institute, which is operated by theAssociation of Universities for Research in Astronomy, Inc., under NASAcontract NAS5-26555.

The ISOPHOT 170 μm Serendipity Survey II. The catalog of optically identified galaxies%
The ISOPHOT Serendipity Sky Survey strip-scanning measurements covering≈15% of the far-infrared (FIR) sky at 170 μm were searched forcompact sources associated with optically identified galaxies. CompactSerendipity Survey sources with a high signal-to-noise ratio in at leasttwo ISOPHOT C200 detector pixels were selected that have a positionalassociation with a galaxy identification in the NED and/or Simbaddatabases and a galaxy counterpart visible on the Digitized Sky Surveyplates. A catalog with 170 μm fluxes for more than 1900 galaxies hasbeen established, 200 of which were measured several times. The faintest170 μm fluxes reach values just below 0.5 Jy, while the brightest,already somewhat extended galaxies have fluxes up to ≈600 Jy. For thevast majority of listed galaxies, the 170 μm fluxes were measured forthe first time. While most of the galaxies are spirals, about 70 of thesources are classified as ellipticals or lenticulars. This is the onlycurrently available large-scale galaxy catalog containing a sufficientnumber of sources with 170 μm fluxes to allow further statisticalstudies of various FIR properties.Based on observations with ISO, an ESA project with instruments fundedby ESA Member States (especially the PI countries: France, Germany, TheNetherlands and the UK) and with the participation of ISAS and NASA.Members of the Consortium on the ISOPHOT Serendipity Survey (CISS) areMPIA Heidelberg, ESA ISO SOC Villafranca, AIP Potsdam, IPAC Pasadena,Imperial College London.Full Table 4 and Table 6 are only available in electronic form at theCDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or viahttp://cdsweb.u-strasbg.fr/cgi-bin/qcat?J/A+A/422/39

Extraplanar Emission-Line Gas in Edge-on Spiral Galaxies. II. Optical Spectroscopy
The results from deep long-slit spectroscopy of nine edge-on spiralgalaxies with known extraplanar line emission are reported. Emissionfrom Hα, [N II] λλ6548, 6583, and [S II]λλ6716, 6731 is detected out to heights of a fewkiloparsecs in all of these galaxies. Several other fainter diagnosticlines such as [O I] λ6300, [O III] λλ4959, 5007,and He I λ5876 are also detected over a smaller scale. Therelative strengths, centroids, and widths of the various emission linesprovide constraints on the electron density, temperature, reddening,source(s) of ionization, and kinematics of the extraplanar gas. In allbut one galaxy, photoionization by massive OB stars alone hasdifficulties explaining all of the line ratios in the extraplanar gas.Hybrid models that combine photoionization by OB stars and anothersource of ionization such as photoionization by turbulent mixing layersor shocks provide a better fit to the data. The (upper limits on the)velocity gradients measured in these galaxies are consistent with thepredictions of the galactic fountain model to within the accuracy of themeasurements.

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.

An Hα survey aiming at the detection of extraplanar diffuse ionized gas in halos of edge-on spiral galaxies. I. How common are gaseous halos among non-starburst galaxies?
In a series of two papers we present results of a new Hα imagingsurvey, aiming at the detection of extraplanar diffuse ionized gas inhalos of late-type spiral galaxies. We have investigated a sample of 74nearby edge-on spirals, covering the northern and southern hemisphere.In 30 galaxies we detected extraplanar diffuse emission at meandistances of |z| ~ 1-2 kpc. Individual filaments can be traced out to|z|<=6 kpc in a few cases. We find a good correlation between the FIRflux ratio (S60/S100) and the SFR per unit area(LFIR/D225), based on thedetections/non-detections. This is actually valid for starburst, normaland for quiescent galaxies. A minimal SFR per unit area for the lowestS60/S100 values, at which extended emission hasbeen detected, was derived, which amounts to dotEA25thres = (3.2+/-0.5)*E40ergs-1 kpc-2. There are galaxies where extraplanaremission was detected at smaller values ofLFIR/D225, however, only in combinationwith a significantly enhanced dust temperature. The results corroboratethe general view that the gaseous halos are a direct consequence of SFactivity in the underlying galactic disk.Based on observations collected at the European Southern Observatory,Chile (ESO No. 63.N-0070, ESO No. 64.N-0034, ESO No. 65.N.-0002).

A comparison of stellar populations in galaxy spheroids across a wide range of Hubble types
We present line-strengths and kinematics from the central regions of 32galaxies with Hubble types ranging from E to Sbc. Spectral indices,based on the Lick system, are measured in the optical and near-infrared(NIR). The 24 indices measured, in conjunction with models of theeffects of varying abundance ratios, permit the breaking ofage/metallicity degeneracy, and allow estimation of enhancements inspecific light elements (particularly C and Mg). The large range ofHubble types observed allows direct comparison of line-strengths in thecentres of early-type galaxies (E and S0) with those in spiral bulges,free from systematic differences that have plagued comparisons ofresults from different studies. Our sample includes field and Virgocluster galaxies. For early-type galaxies our data are consistent withpreviously reported trends of Mg2 and Mgb with velocitydispersion. In spiral bulges we find trends in all indices with velocitydispersion. We estimate luminosity-weighted ages, metallicities andheavy-element abundance ratios (enhancements) from optical indices.These show that bulges are less enhanced in light (α-capture)elements and have lower average age than early-type galaxies. Trendsinvolving age and metallicity also differ sharply between early and latetypes. An anticorrelation exists between age and metallicity in earlytypes, while, in bulges, metallicity is correlated with velocitydispersion. We consider the implications of these findings for models ofthe formation of these galaxies. We find that primordial collapse modelsof galaxy formation are ruled out by our observations, while severalpredictions of hierarchical clustering (merger) models are confirmed.

Disk Boundaries in Spiral Galaxies
We explore the hypothesis that the outer boundaries(“cutoffs”) of the stellar disks observed in many galaxiesare determined by the condition of local gravitational (Jeans) stabilityfor the gaseous protodisks at large galactocentric distances. The ratioof the surface density of the disk Σdisk to the critical value forJeans instability Σcrit is computed for a number of galaxies,assuming that the gas velocity dispersion in the forming diskcorresponded to its current thickness and that the disk itself is in aquasi-equilibrium state. The mean estimated stellar velocity dispersionin the vicinity of the cutoff (12 km/s) is close to the typical velocitydispersions of gaseous clouds in disk galaxies. At greater distances,such velocity dispersions should ensure gravitational stability of thedisk both at the present epoch and in the past. The cutoff radius of thedisk R cut is correlated with other disk parameters, and the ratioΣdisk/Σcrit at R cut is close to unity in most cases. Weconclude that the available observational data agree well with thehypothesis that stellar disk cutoffs are due to a rapid decrease in thestar-formation rate beyond R cut, where the gaseous disk has always beenstable.

Modified Newtonian Dynamics as an Alternative to Dark Matter
Modified Newtonian dynamics (MOND) is an empirically motivatedmodification of Newtonian gravity or inertia suggested by Milgrom as analternative to cosmic dark matter. The basic idea is that ataccelerations below ao ~ 10-8 cm/s2 ~cHo/6 the effective gravitational attraction approaches√(gnao), where gn is the usualNewtonian acceleration. This simple algorithm yields flat rotationcurves for spiral galaxies and a mass-rotation velocity relation of theform M ∝ V4 that forms the basis for the observedluminosity-rotation velocity relation-the Tully-Fisher law. We reviewthe phenomenological success of MOND on scales ranging from dwarfspheroidal galaxies to superclusters and demonstrate that the evidencefor dark matter can be equally well interpreted as evidence for MOND. Wediscuss the possible physical basis for an acceleration-basedmodification of Newtonian dynamics as well as the extention of MOND tocosmology and structure formation.

The H I Line Width/Linear Diameter Relationship as an Independent Test of the Hubble Constant
The relationship between corrected H I line widths and linear diameters(LW/LD) for spiral galaxies is used as an independent check on the valueof the Hubble constant. After calibrating the Tully-Fisher (TF) relationin both the B and I bands, the B-band relation is used for galaxies ofmorphological/luminosity types Sc I, Sc I.2, Sc I.3, Sab, Sb, Sb I-II,and Sb II to derive the LW/LD relation. We find that for this sample thescatter in the LW/LD is smallest with a Hubble constant of 90-95 kms-1 Mpc-1. Lower values of the Hubble constantproduce a separation in the LW/LD relation that is a function ofmorphological type. Since a Hubble constant of 90-95 is significantlylarger than the final Key Project value of 72 km s-1Mpc-1, a comparison of TF, surface brightness fluctuation(SBF), and fundamental plane (FP) is made. This comparison indicatesthat the Key Project TF distances to 21 clusters may be too large. For asample of 11 clusters, the Key Project TF distances provide anunweighted mean Hubble constant of 77 km s-1Mpc-1, while a combination of the FP, SBF, and our TFdistances for the same 11 clusters gives H0=91 kms-1 Mpc-1. A more subtle result in our data is amorphological dichotomy in the Hubble constant. The data suggest that ScI galaxies follow a Hubble constant of 90-95 while Sb galaxies follow aHubble constant closer to 75 km s-1 Mpc-1.Possible explanations for this result are considered, but it is shownthat this Sb/Sc I Hubble flow discrepancy is also present in the VirgoCluster and is consistent with previous investigations that indicatethat some galaxies carry a component of age-related intrinsic redshift.

Bar Galaxies and Their Environments
The prints of the Palomar Sky Survey, luminosity classifications, andradial velocities were used to assign all northern Shapley-Ames galaxiesto either (1) field, (2) group, or (3) cluster environments. Thisinformation for 930 galaxies shows no evidence for a dependence of barfrequency on galaxy environment. This suggests that the formation of abar in a disk galaxy is mainly determined by the properties of theparent galaxy, rather than by the characteristics of its environment.

The UZC-SSRS2 Group Catalog
We apply a friends-of-friends algorithm to the combined Updated ZwickyCatalog and Southern Sky Redshift Survey to construct a catalog of 1168groups of galaxies; 411 of these groups have five or more members withinthe redshift survey. The group catalog covers 4.69 sr, and all groupsexceed the number density contrast threshold, δρ/ρ=80. Wedemonstrate that the groups catalog is homogeneous across the twounderlying redshift surveys; the catalog of groups and their membersthus provides a basis for other statistical studies of the large-scaledistribution of groups and their physical properties. The medianphysical properties of the groups are similar to those for groupsderived from independent surveys, including the ESO Key Programme andthe Las Campanas Redshift Survey. We include tables of groups and theirmembers.

The gradient of diffuse gamma -ray emission in the Galaxy
We show that the well-known discrepancy, known for about two decades,between the radial dependence of the Galactic cosmic ray nucleondistribution, as inferred most recently from EGRET observations ofdiffuse gamma -rays above 100 MeV, and of the most likely cosmic raysource distribution (supernova remnants, superbubbles, pulsars) can beexplained purely by propagation effects. Contrary to previous claims, wedemonstrate that this is possible, if the dynamical coupling between theescaping cosmic rays and the thermal plasma is taken into account, andthus a self-consistent calculation of a Galactic Wind is carried out.Given a dependence of the cosmic ray source distribution onGalactocentric radius r, our numerical wind solutions show that thecosmic ray outflow velocity, V(r,z) = u0 + VA 0,also depends both on r, as well as on vertical distance z, withu0 and VA 0 denoting the thermal gas and theAlfvén velocities, respectively, at a reference levelzC. The latter is by definition the transition boundary fromdiffusion to advection dominated cosmic ray transport and is thereforealso a function of r. In fact, the cosmic ray escape time averaged overparticle energies decreases with increasing cosmic ray source strength.Thus an increase in cosmic ray source strength is counteracted by areduced average cosmic ray residence time in the gas disk. This meansthat pronounced peaks in the radial distribution of the source strengthresult in mild radial gamma -ray gradients at GeV energies, as it hasbeen observed. The effect might be enhanced by anisotropic diffusion,assuming different radial and vertical diffusion coefficients. In orderto better understand the mechanism described, we have calculatedanalytic solutions of the stationary diffusion-advection equation,including anisotropic diffusion in an axisymmetric geometry, for a givencosmic ray source distribution and a realistic outflow velocity fieldV(r,z), as inferred from the self-consistent numerical Galactic Windsimulations performed simultaneously. At TeV energies the gamma -raysfrom the sources themselves are expected to dominate the observed``diffuse'' flux from the disk. Its observation should therefore allowan empirical test of the theory presented.

The Ursa Major Cluster of Galaxies. V. H I Rotation Curve Shapes and the Tully-Fisher Relations
This paper investigates the statistical properties of the Tully-Fisher(TF) relations for a volume-limited complete sample of spiral galaxiesin the nearby Ursa Major Cluster. The merits of B, R, I, and K' surfacephotometry and the availability of detailed kinematic information from HI synthesis imaging have been exploited. In addition to the corrected HI global profile widths WiR,I, the available H Irotation curves allow direct measurements of the observed maximumrotational velocities Vmax and the amplitudesVflat of the outer flat parts. The dynamical state of the gasdisks could also be determined in detail from the radio observations.The four luminosity and three kinematic measures allowed theconstruction of 12 correlations for various subsamples. For large galaxysamples, the Mb,iR-logWiR,Icorrelation in conjunction with strict selection criteria is preferredfor distance determinations with a 7% accuracy. Galaxies with rotationcurves that are still rising at the last measured point liesystematically on the low-velocity side of the TF relation. Galaxieswith a partly declining rotation curve(Vmax>Vflat) tend to lie systematically on thehigh-velocity side of the relation when usingWiR,I or Vmax. However, systematicoffsets are eliminated when Vflat is used. Residuals of theMb,iB-log(2Vflat) relation correlateconsistently with global galaxy properties along the Hubble sequencelike morphological type, color, surface brightness, and gas massfraction. These correlations are absent for the near-infraredMb,iK'-log(2Vflat)residuals. The tightest correlation(χ2red=1.1) is found for theMb,iK'-log(2Vflat) relation,which has a slope of -11.3+/-0.5 and a total observed scatter of 0.26mag with a most likely intrinsic scatter of zero. The tightness of thenear-infrared correlation is preserved when converting it into abaryonic TF relation that has a slope of -10.0 in the case(Mgas/LK')=1.6 while a zerointrinsic scatter remains most likely. Based on the tightness of thenear-infrared and baryonic correlations, it is concluded that the TFrelation reflects a fundamental correlation between the mass of the darkmatter halo, measured through its induced maximum rotational velocityVflat, and the total baryonic mass Mbar of agalaxy where Mbar~V4flat. Althoughthe actual distribution of the baryonic matter inside halos of similarmass can vary significantly, it does not affect this relation.

The Frequency of Active and Quiescent Galaxies with Companions: Implications for the Feeding of the Nucleus
We analyze the idea that nuclear activity, either active galactic nuclei(AGNs) or star formation, can be triggered by interactions by studyingthe percentage of active, H II, and quiescent galaxies with companions.Our sample was selected from the Palomar survey and avoids selectionbiases faced by previous studies. This sample was split into fivedifferent groups, Seyfert galaxies, LINERs, transition galaxies, H IIgalaxies, and absorption-line galaxies. The comparison between the localgalaxy density distributions of the different groups showed that in mostcases there is no statistically significant difference among galaxies ofdifferent activity types, with the exception that absorption-linegalaxies are seen in higher density environments, since most of them arein the Virgo Cluster. The comparison of the percentage of galaxies withnearby companions showed that there is a higher percentage of LINERs,transition galaxies, and absorption-line galaxies with companions thanSeyfert and H II galaxies. However, we find that when we consider onlygalaxies of similar morphological types (elliptical or spiral), there isno difference in the percentage of galaxies with companions amongdifferent activity types, indicating that the former result was due tothe morphology-density effect. In addition, only small differences arefound when we consider galaxies with similar Hα luminosities. Thecomparison between H II galaxies of different Hα luminositiesshows that there is a significantly higher percentage of galaxies withcompanions among H II galaxies with L(Hα)>1039 ergss-1 than among those with L(Hα)<=1039ergs s-1, indicating that interactions increase the amount ofcircumnuclear star formation, in agreement with previous results. Thefact that we find that galaxies of different activity types have thesame percentage of companions suggests that interactions betweengalaxies is not a necessary condition to trigger the nuclear activity inAGNs. We compare our results with previous ones and discuss theirimplications.

Near infrared observations of the truncation of stellar disks
We present a first study of truncation of the stellar disks of spiralgalaxies in the near infrared. Observations of NGC 4013, NGC 4217, NGC6504 and NGC 5981 were made with the CAIN NIR camera on the CST inTenerife. This wavelength range provides the best description of thephenomenon, not only because extinction effects are minimized, but alsobecause the distribution of the old stellar population is directlyobtained. The four galaxies are edge-on and an inversion method wasdeveloped to obtain the deprojected profiles. We did not assume anymodel of the different galactic components. The ``truncation curve'',i.e. T(R) = mu (R)- mu D(R), where mu is the actual surfacebrightness in mag/arcsec2 and mu D the exponentialdisk surface brightness, has been obtained with unprecedented precision.It is suggested that T(R) is proportional to(Rt-R)-1, where Rt is the truncationradius, i.e. the radius beyond which no star is observed.

Properties of tidally-triggered vertical disk perturbations
We present a detailed analysis of the properties of warps andtidally-triggered perturbations perpendicular to the plane of 47interacting/merging edge-on spiral galaxies. The derived parameters arecompared with those obtained for a sample of 61 non-interacting edge-onspirals. The entire optical (R-band) sample used for this study waspresented in two previous papers. We find that the scale height of disksin the interacting/merging sample is characterized by perturbations onboth large ( =~ disk cut-off radius) and short ( =~ z0)scales, with amplitudes of the order of 280 pc and 130 pc on average,respectively. The size of these large (short) -scale instabilitiescorresponds to 14% (6%) of the mean disk scale height. This is a factorof 2 (1.5) larger than the value found for non-interacting galaxies. Ahallmark of nearly all tidally distorted disks is a scale height thatincreases systematically with radial distance. The frequent occurrenceand the significantly larger size of these gradients indicate that diskasymmetries on large scales are a common and persistent phenomenon,while local disturbances and bending instabilities decline on shortertimescales. Nearly all (93%) of the interacting/merging and 45% of thenon-interacting galaxies studied are noticeably warped. Warps ofinteracting/merging galaxies are ~ 2.5 times larger on average thanthose observed in the non-interacting sample, with sizes of the order of340 pc and 140 pc, respectively. This indicates that tidal distortionsdo considerably contribute to the formation and size of warps. However,they cannot entirely explain the frequent occurrence of warped disks.Based on observations obtained at the European Southern Observatory(ESO, La Silla, Chile), Calar Alto Observatory operated by the MPIA(DSAZ, Spain), Lowell Observatory (Flagstaff,AZ, USA), and Hoher ListObservatory (Germany).

The Ursa Major cluster of galaxies. IV. HI synthesis observations
In this data paper we present the results of an extensive 21 cm-linesynthesis imaging survey of 43 spiral galaxies in the nearby Ursa Majorcluster using the Westerbork Synthesis Radio Telescope. Detailedkinematic information in the form of position-velocity diagrams androtation curves is presented in an atlas together with HI channel maps,21 cm continuum maps, global HI profiles, radial HI surface densityprofiles, integrated HI column density maps, and HI velocity fields. Therelation between the corrected global HI linewidth and the rotationalvelocities Vmax and Vflat as derived from therotation curves is investigated. Inclination angles obtained from theoptical axis ratios are compared to those derived from the inclined HIdisks and the HI velocity fields. The galaxies were not selected on thebasis of their HI content but solely on the basis of their clustermembership and inclination which should be suitable for a kinematicanalysis. The observed galaxies provide a well-defined, volume limitedand equidistant sample, useful to investigate in detail the statisticalproperties of the Tully-Fisher relation and the dark matter halos aroundthem.

The Nature of Composite LINER/H II Galaxies as Revealed from High-Resolution VLA Observations
A sample of 37 nearby galaxies displaying composite LINER/H II and pureH II spectra was observed with the VLA in an investigation of the natureof their weak radio emission. The resulting radio contour maps overlaidon optical galaxy images are presented here, together with an extensiveliterature list and discussion of the individual galaxies. Radiomorphological data permit assessment of the ``classical active galacticnucleus (AGN)'' contribution to the global activity observed in these``transition'' LINER galaxies. One in five of the latter objects displayclear AGN characteristics: these occur exclusively in bulge-dominatedhosts.

Nearby Optical Galaxies: Selection of the Sample and Identification of Groups
In this paper we describe the Nearby Optical Galaxy (NOG) sample, whichis a complete, distance-limited (cz<=6000 km s-1) andmagnitude-limited (B<=14) sample of ~7000 optical galaxies. Thesample covers 2/3 (8.27 sr) of the sky (|b|>20deg) andappears to have a good completeness in redshift (97%). We select thesample on the basis of homogenized corrected total blue magnitudes inorder to minimize systematic effects in galaxy sampling. We identify thegroups in this sample by means of both the hierarchical and thepercolation ``friends-of-friends'' methods. The resulting catalogs ofloose groups appear to be similar and are among the largest catalogs ofgroups currently available. Most of the NOG galaxies (~60%) are found tobe members of galaxy pairs (~580 pairs for a total of ~15% of objects)or groups with at least three members (~500 groups for a total of ~45%of objects). About 40% of galaxies are left ungrouped (field galaxies).We illustrate the main features of the NOG galaxy distribution. Comparedto previous optical and IRAS galaxy samples, the NOG provides a densersampling of the galaxy distribution in the nearby universe. Given itslarge sky coverage, the identification of groups, and its high-densitysampling, the NOG is suited to the analysis of the galaxy density fieldof the nearby universe, especially on small scales.

Is a Simple Collisionless Relic Dark Matter Particle Ruled Out?
The central densities of dark matter (DM) halos are much lower thanpredicted in cold DM models of structure formation. Confirmation thatthey have cores with a finite central density would allow us to rule outmany popular types of collisionless particles as candidates for DM. Anymodel that leads to cusped halos (such as cold DM) is already facingserious difficulties on small scales, and hot DM models have beenexcluded. Here I show that fermionic warm DM is inconsistent with thewide range of phase-space densities in the DM halos of well-observednearby galaxies.

A Spectroscopic Redshift for the Cl 0024+16 Multiple Arc System: Implications for the Central Mass Distribution
We present a spectroscopic redshift of z=1.675 for the well-knownmultiply lensed system of arcs seen in the z=0.39 cluster Cl 0024+16. Incontrast to earlier work, we find that the lensed images are accuratelyreproduced by a projected mass distribution which traces the locationsof the brightest cluster elliptical galaxies, suggesting that the mostsignificant minima of the cluster potential are not dynamically erased.The averaged mass profile is shallow and consistent with predictions ofrecent numerical simulations. The source redshift enables us todetermine an enclosed cluster mass of M(<100 kpch-1)=1.11+/-0.03×1014 h-1Msolar (Ω=1) and a mass-to-light ratio ofM/LB(<100 kpc h-1)=320+/-30 h(M/LB)solar (virtually independent of curvature),after correction for passive stellar evolution. The arc spectrumcontains many ionized absorption lines and closely resembles that of thelocal Wolf-Rayet galaxy NGC 4217. Our lens model predicts a highmagnification (~=20) for each image and identifies a new pair ofmultiple images of a galaxy at a predicted redshift of z=1.3.

The Correlation between Galaxy H I Line Widths and K'Luminosities
The relationship between galaxy luminosities and rotation rates isstudied with total luminosities in the K' band. Extinction problems areessentially eliminated at this band centered at 2.1 μm. A templateluminosity-line width relation is derived based on 65 galaxies drawnfrom two magnitude-limited cluster samples. The zero point is determinedusing four galaxies with accurately known distances. The calibration isapplied to give the distance to the Pisces Cluster (59 Mpc) at aredshift in the cosmic microwave background frame of 4771 kms-1. The resultant value of the Hubble constant is 81 kms-1Mpc-1. The largest sources of uncertainty arethe small number of zero-point calibrators at this time at K' and thepresent application to only one cluster.

Distances to Galaxies from the Correlation between Luminosities and Line Widths. III. Cluster Template and Global Measurement of H0
The correlation between the luminosities and rotation velocities ofgalaxies can be used to estimate distances to late-type galaxies. It isan appropriate moment to reevaluate this method given the great deal ofnew information available. The major improvements described hereinclude: (1) the template relations can now be defined by large,complete samples, (2) the samples are drawn from a wide range ofenvironments, (3) the relations are defined by photometric informationat the B, R, I, and K' bands, (4) the multiband information clarifiesproblems associated with internal reddening, (5) the template zeropoints are defined by 24 galaxies with accurately known distances, and(6) the relations are applied to 12 clusters scattered across the skyand out to velocities of 8000 km s-1. The biggest change fromearlier calibrations are associated with point 5. Roughly a 15% increasein the distance scale has come about with the fivefold increase in thenumber of zero-point calibrators. The overall increase in the distancescale from the luminosity-line width methodology is about 10% afterconsideration of all factors. Modulo an assumed distance to the LargeMagellanic Cloud of 50 kpc and no metallicity corrections to the Cepheidcalibration, the resulting value of the Hubble constant isH0=77+/-8 km s-1 Mpc-1, where the erroris the 95% probable statistical error. Cumulative systematic errorsinternal to this analysis should not exceed 10%. Uncertainties in thedistance scale ladder external to this analysis are estimated at ~10%.If the Cepheid calibration is shifted from the LMC to NGC 4258 with adistance established by observations of circumnuclear masers, thenH0 is larger by 12%.

Box- and peanut-shaped bulges. I. Statistics
We present a classification for bulges of a complete sample of ~ 1350edge-on disk galaxies derived from the RC3 (Third Reference Catalogue ofBright Galaxies, de Vaucouleurs et al. \cite{rc3}). A visualclassification of the bulges using the Digitized Sky Survey (DSS) inthree types of b/p bulges or as an elliptical type is presented andsupported by CCD images. NIR observations reveal that dust extinctiondoes almost not influence the shape of bulges. There is no substantialdifference between the shape of bulges in the optical and in the NIR.Our analysis reveals that 45% of all bulges are box- and peanut-shaped(b/p). The frequency of b/p bulges for all morphological types from S0to Sd is > 40%. In particular, this is for the first time that such alarge frequency of b/p bulges is reported for galaxies as late as Sd.The fraction of the observed b/p bulges is large enough to explain theb/p bulges by bars. Partly based on observations collected at ESO/LaSilla (Chile), DSAZ/Calar Alto (Spain), and Lowell Observatory/Flagstaff(AZ/U.S.A.). Tables 6 and 7 are only available in electronic form at CDSvia anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or viahttp://cdsweb.u-strasbg.fr/Abstract.html

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