We have performed 2D bulge/bar/disc decompositions using g, r and i-band images of a representative sample of nearly 1000 galaxies from the Sloan Digital Sky Survey. We show that the Petrosian concentration index is a better proxy for the bulge-to-total ratio than the global Sérsic index. We show that pseudo-bulges can be distinguished from classical bulges as outliers in the Kormendy relation. We provide the structural parameters and distributions of stellar masses of ellipticals, classical bulges, pseudo-bulges, discs and bars, and find that 32 per cent of the total stellar mass in massive galaxies in the local universe is contained in ellipticals, 36 per cent in discs, 25 per cent in classical bulges, 3 per cent in pseudo-bulges and 4 per cent in bars. Pseudo-bulges are currently undergoing intense star formation activity and populate the blue cloud of the colour–magnitude diagram. Most (though not all) classical bulges are quiescent and populate the red sequence of the diagram. Classical bulges follow a correlation between the bulge Sérsic index and bulge-to-total ratio, while pseudo-bulges do not. In addition, for a fixed bulge-to-total ratio, pseudo-bulges are less concentrated than classical bulges. Pseudo-bulges follow a mass–size relation similar to that followed by bars, and different from that followed by classical bulges. In the fundamental plane, pseudo-bulges occupy the same locus as discs. While these results point out different formation processes for classical and pseudo-bulges, we also find a significant overlap in their properties, indicating that the different processes might happen concomitantly. Finally, classical bulges and ellipticals follow offset mass–size relations, suggesting that high-mass bulges might not be simply high-mass ellipticals surrounded by discs.
The central components of disc galaxies have proven deceptively simple. The early view of galaxy bulges as scaled ellipticals is far from complete. Even the mere definition of a galaxy bulge is still prone to debate. Yet bulges hold crucial clues to galaxy formation and evolution. Current views discern between bulges formed through violent processes, such as hierarchical clustering via minor mergers, named classical bulges, and those formed through longer time-scales, via disc instabilities and secular evolution processes, named pseudo-bulges (see Wyse, Gilmore & Franx 1997; Kormendy & Kennicutt 2004, for reviews). Given their dissimilar origins, it is naturally expected that these different bulge categories should be structurally distinct.
In fact, previous work have showed evidence that pseudo-bulges, when compared to classical bulges, tend to show younger stellar populations, kinematics supported by rotation and less-concentrated surface brightness profiles, similar to those of discs, which can be parametrized by the corresponding Sérsic indices (see e.g. Carollo et al. 1997; Gadotti & dos Anjos 2001; Kormendy et al. 2006; Drory & Fisher 2007; Fisher & Drory 2008, and references therein). In relatively inclined galaxies, pseudo-bulges are seen to be more flattened than classical bulges, and as flattened as discs. Some pseudo-bulges display a characteristic box/peanut shape if the galaxy is viewed edge-on. Such box/peanut bulges are believed to be the inner parts of bars that have evolved and buckled off the plane of the disc (see e.g. Athanassoula 2005, and references therein). Such evidence is, however, limited. Since such studies brought along new perceptions, proofs of concept, and because pseudo-bulges are less conspicuous than classical bulges, they had to focus on a detailed analysis of small samples, often with high-resolution data. For instance, pseudo-bulges often host nuclear bars and/or nuclear spiral arms, which are difficult to identify without images of high physical spatial resolution, or a careful analysis.
Ellipticals would be formed through major mergers. The gas content in galaxies, as a dissipative component and the material to form new stars, is likely to play an important role in minor/major mergers and secular evolution, and adds considerable complexity to these views. A more complete picture of galaxy formation and evolution demands a deep understanding of the consequences of such diverse processes, as well as the structural properties of the different galaxy components. It is still necessary to understand better how these different formation processes result in evolutionary and structural differences, how these differences translate into observables and how this framework can be incorporated by theoretical developments. Questions such as how structurally different ellipticals, classical bulges and pseudo-bulges are, how different the host galaxies of classical and pseudo-bulges are, how often disc galaxies host pseudo-bulges as compared to classical bulges, how are their masses distributed, and in which conditions pseudo-bulges are important, remain to be properly answered. Time is ripe for more extensive studies on the properties of bulges and ellipticals, taking advantage of large data sets, such as the Sloan Digital Sky Survey (SDSS), which are becoming more commonly available.
We have performed a detailed structural analysis of a sample of nearly 1000 galaxies from the SDSS. Through such a work, we were able to determine Sérsic indices, scalelengths and effective surface brightness for elliptical galaxies, classical bulges and pseudo-bulges, and scalelengths and central surface brightness for discs, taking into account the presence of a bar when necessary, as well as the bulge-to-total and disc-to-total luminosity ratios, in three different bandpasses (g, r and i). We have also determined colours and stellar masses for each galaxy component separately. Such structural parameters are explored throughout this paper, combined with several other physical properties obtained for the SDSS sample of galaxies. (A similar set of parameters was also obtained for bars, which are investigated in a separate paper.)
Allen et al. (2006) and Benson et al. (2007) have recently performed a detailed structural analysis using large data sets. While their samples are substantially larger than ours, our methodology aims at a more careful analysis. For instance, we have included a bar component in the models fitted, since, as shown in Gadotti (2008), if the bar is not taken into account in the modelling of barred galaxies, bulge properties can be significantly affected. We have produced fits in multiple bands for every galaxy, which have allowed us to estimate the colours of the different components. With such colours, we were able to directly estimate mass-to-light ratios for the different components, which result in more accurate stellar mass estimates. Finally, we have selected a sample of galaxies suitable for such image decompositions, and each fit was performed and checked individually. All this care assures us that the results from our analysis are trustworthy to carry the investigations we aimed for.
A common practice in studies on bulges is to define pseudo-bulges as those with a Sérsic index lower than a given threshold. However, the use of Sérsic indices to distinguish pseudo-bulges from classical bulges is likely to generate considerable ambiguity, as the dynamical range of this parameter is small, compared to the uncertainty in individual measurements (see discussion in Durbala et al. 2008; Gadotti 2008). Instead, we have used the Kormendy relation (Kormendy 1977) to identify pseudo-bulges. Some degree of structural similarity between classical bulges and ellipticals is borne out by such relation, which is followed by both kinds of systems. In contrast, pseudo-bulges, being structurally different, do not follow a similar relation. Therefore, our identification of pseudo-bulges is not only more reliable but also better physically motivated. It is also important to point out that, due to the fact that our models include a bar component, the pseudo-bulges we identify in this study are not those pseudo-bulges associated with the box/peanut morphology.
This paper is organized as follows. The next section describes the sample selection and properties. Section 3 describes the methodology implemented to produce the fits. Results are presented in Section 4, separated in several subsections. We discuss various aspects of our main findings in Section 5, including a comparison with previous work. Finally, we summarize our work and major conclusions in Section 6. Throughout this work, we have used the following cosmological parameters: H0= 75 km s−1 Mpc−1, ΩM= 0.3 and ΩΛ= 0.7. Unless noted, photometric measurements refer to the i band. All logarithms are base 10.
2 SAMPLE SELECTION AND PROPERTIES
We aimed for a sample which is concomitantly suitable for structural analysis based on an image decomposition and a fair representation of the galaxy population in the local universe. We thus drew the sample from all objects spectroscopically classified as galaxies in the SDSS Data Release 2 (DR2), applying the following criteria. We first selected all galaxies with redshift in the range 0.02 ≤z≤ 0.07. This provides a sample with a statistically meaningful number of galaxies, whose images have a relatively comparable physical spatial resolution. Images of closer galaxies have a level of detail much richer than those of galaxies at z≈ 0.05, as observed within SDSS. On the other hand, images of farther galaxies have a physical spatial resolution which is often not adequate to study their structural properties in some detail.
Secondly, since dwarf galaxies are not an object of our study, we excluded all galaxies with stellar masses below 1010 M⊙. Galaxy stellar masses were obtained from Kauffmann et al. (2003b). At this stage, we have a volume-limited sample, i.e. a sample which includes all galaxies more massive than 1010 M⊙ in the volume defined by our redshift cuts and the DR2 footprint. From now on, we will refer to this sample as our parent sample.
Finally, we chose objects with an axial ratio b/a≥ 0.9, where a and b are, respectively, the semimajor and semiminor axes of the galaxy, taken from the SDSS data base (these are measured at the 25 mag arcsec−2 isophote in the g band.). This criterion assures us that our galaxies are very close to face-on, meaning that effects from dust attenuation, as well as projection effects, are minimized, and that bars can be distinctly seen, avoiding erroneous fits, and leading to a more reliable determination of the structural parameters and colours of the separate galaxy components. It also implies that we do not need to worry about inclination corrections. These criteria resulted in a sample of 3375 objects. The images of each of these galaxies were individually inspected to remove from the sample those galaxies which are either not truly face-on,1 substantially disturbed by a companion or a merger, overly faint or irregular, have images too close to the border of the CCD frame, as well as duplicate entries and those images where the presence of a bright star renders them unfit. We also rejected galaxies with a < 4 arcsec, as we deemed these galaxies too small for a detailed parametric image decomposition. This ensured that, for the vast majority of the sample, the effective radius of the bulge is larger than the point spread function (PSF) half width at half-maximum (HWHM). Hence, reliable conclusions can be drawn even for small bulges (see discussion further below). Our final sample contains 963 galaxies, of which 407 contain active galactic nuclei (AGN – mostly type 2). The AGN classification is taken from Kauffmann et al. (2003a).
Most of the galaxies in the final sample have 0.04 < z < 0.06. At this distance, 1 arcsec corresponds roughly to 1 kpc. Since the SDSS spectra are taken through a circular aperture of 3 arcsec in diameter, this means that, for the majority of our galaxies, the spectra obtained represent the central, bulge-dominated part of the galaxy, with a little disc contamination. This will become clearer further below, where the effective radius of bulges is presented. Since the mean PSF full width at half-maximum (FWHM) in SDSS images is ≈1.5 arcsec, the typical physical spatial resolution in the images of our final sample is about 1.5 kpc. Most of these galaxies also have 0.9 ≤b/a < 0.95. In many cases, this means that bulge and disc have slightly different geometrical properties, such as ellipticity ε (i.e. 1 −b/a) and position angle. These differences are helpful when fitting models to the images, since they provide further constraints to the models of the different galaxy components. Finally, their typical stellar mass is similar to that of the Milky Way (i.e. ≈5 × 1010 M⊙–Sommer-Larsen & Dolgov 2001).
Let us now check whether our final sample is a fair representation of the galaxy population in the parent, volume-limited sample, and whether our selection criteria to reach the final sample introduce any bias that have to be accounted for. With this aim, we plot in Fig. 1 the distributions of several relevant properties of the galaxies in both samples. One sees that these distributions are reasonably similar, in particular those of the AGN [O iii] luminosity. However, it is also apparent that the final sample includes a somewhat larger fraction of massive, brighter, quiescent and more concentrated galaxies. The more stringent criterion to reach the final sample from our parent sample is the axial ratio cut. Thus, we now investigate whether this criterion is the cause of such differences. The top panel of Fig. 2 shows the distributions of the axial ratio for galaxies in the parent sample, separated according to their concentration C. From our structural analysis below, we find that most ellipticals, and few disc galaxies, have C > 3. Conversely, most disc-dominated galaxies, and few ellipticals, have C < 2.5. We thus use these thresholds to separate ellipticals and disc galaxies. It is evident that, due to their different intrinsic axial ratios, such galaxies have different distributions of the observed axial ratio, in such a way that the fraction of elliptical galaxies increases at higher values of b/a. Therefore, it is indeed the axial ratio cut at b/a≥ 0.9 that produces the differences seen in Fig. 1. Some of the results presented below depend on the fraction of elliptical galaxies in the sample, and are thus affected by this selection effect. We can correct these results for such effect by comparing the fraction of galaxies with C > 3 in the parent sample, regardless of axial ratio, to that of galaxies with both C > 3 and b/a≥ 0.9. This provides us with a fairly good indication of how larger the fraction of elliptical galaxies in our final sample is compared to our parent, volume-limited sample. It turns out that this difference is a factor of 1.3. Such correction factor will be applied when necessary with an explicit mention.
Given our axial ratio cut, one might also question whether the results in this work concern galaxies which are intrinsically more eccentric than average. To check that we have also selected 30 systems with C > 2.5 (i.e. mostly bulge-dominated and elliptical galaxies) and 0.5 < b/a < 0.7, which otherwise comply with all other selection criteria of the final sample, and analyse them in a similar fashion. One could also ask if we are missing galaxies with very strong bars due to our cut in axial ratio. This would happen if the outer disc of the galaxy is not detected. We argue that this is not the case, based on the fact that the strongest bars we find, considering the bar-to-total luminosity ratio, are about as strong as the strongest ones found in other studies (Sellwood & Wilkinson 1993; Reese et al. 2007; Durbala et al. 2008; Gadotti 2008).
Finally, we also need to check if there is a bias in our parent sample against galaxies close to both its low-mass and high-redshift cuts, which could occur due to magnitude limits in the survey. This is done by plotting galaxy mass against redshift for all spectroscopically classified galaxies in DR2 in the lower panel of Fig. 2. Since such a bias might depend on galaxy colour, we plot separately galaxies with low and high dust-corrected z-band mass-to-light ratio (from Kauffmann et al. 2003b), using the peak of its distribution as boundary between the two groups. One sees that there is no clear need for such a volume correction, i.e. our parent sample includes effectively all galaxies more massive than 1010 M⊙ in the defined volume.
We have also compared the distributions of other physical parameters, such as stellar surface density and metalicity, r-band light-weighted age, number of neighbours and the fluxes and equivalent widths of important emission lines in AGN, derived by Kauffmann et al. (2003a,b, 2004) and Gallazzi et al. (2005), in both our parent and final samples. These distributions are generally similar. We thus conclude that, after accounting for the effects introduced with our axial ratio cut, our final sample is a fair representation of the population of galaxies and AGN in the local universe with stellar masses larger than 1010 M⊙. This means that conclusions based on this sample are generally pertinent to galaxies that satisfy these conditions.
Fig. 3 shows examples of galaxies in our sample. Each row corresponds to a different galaxy category, concerning the central component. Elliptical galaxies are shown in the top row. The remaining rows show, from top to bottom panel, respectively, galaxies with classical bulges, galaxies with pseudo-bulges and bulgeless galaxies. This grouping is based on the results from our parametric image decompositions below.
3 IMAGE DECOMPOSITION
The fitting of each galaxy image in our sample was done using budda v2.1, which is able to fit up to four different galactic components to a galaxy image, namely bulge, disc, bar, and a central source, usually adopted to account for the emission from bright, type 1 AGN. Details on the code technical aspects and capabilities can be found in de Souza, Gadotti & dos Anjos (2004) and Gadotti (2008). In particular, the latter discusses more specifically the treatment of the bar component. Here, we briefly recall the functions used to describe each component.
The model components are described by concentric, generalized ellipses (see Athanassoula et al. 1990):
Each component also has to follow a surface brightness radial profile. The disc profile is described by an exponential function (Freeman 1970):de Vaucouleurs 1948), while n= 1 corresponds to an exponential bulge. Elliptical galaxies were fitted with a single ‘bulge’ component.
Using the models obtained with budda, we have calculated the absolute magnitude of each different galaxy component in all galaxies in the sample in the g, r and i bands. We have thus also calculated the integrated colours of each component separately.
To avoid unreliable results that very often arise from automated image decomposition, we applied budda to each galaxy individually. Erroneous fits are particularly likely to arise, if not followed closely, when fitting barred galaxies. In such cases, the number of parameters fitted can be as high as 18, and the topology of the distribution of χ2 for many possible models is very complex. We thus adopted a procedure to produce each fit, which is as follows.
First, we needed to produce the image to be fitted. To this end, a cutout was created from the original SDSS galaxy image, with the galaxy in the centre, and containing enough sky background in order not to remove the galaxy outskirts. Usually, this means that the image size on a side is about twice the apparent diameter of the galaxy. Before fitting, each image was cleaned of spurious objects such as foreground stars. The sky background and PSF FWHM values given by SDSS were checked and corrected when necessary, which rarely occurred. When needed, the sky background was estimated by calculating the median pixel value of several areas free from objects in the galaxy image. When the PSF FWHM given by SDSS was deemed erroneous, we have made new estimates by fitting a Moffat profile (Moffat 1969) to a number of suitable stars near the galaxy, and choosing the median value found. The images were fitted without subtracting the mean background value. This is important, because a proper calculation of the χ2, and thus a reliable determination of the uncertainties, is based on the statistics concerning all photons that reached the detector. Evidently, the value of the background is given to the code, and the model components are determined taking it into account.
Secondly, before starting the fit, it is necessary to provide the code with initial guesses for all parameters to be fitted. The coordinates of the pixel with highest intensity were chosen as input to x0 and y0. The geometrical parameters were roughly estimated by visual inspection of the image and the corresponding isophotal contours. When deemed necessary, these parameters were also calculated using the intensity moments in a few different circular apertures centred at the galaxy centre. Finally, the initial guesses for the parameters of the surface brightness profiles were estimated through the inspection of a pixel-by-pixel radial intensity profile of the galaxy. Tests with artificial images of unbarred disc galaxies with high and low spatial resolution in de Souza et al. (2004) showed that budda is generally able to reliably retrieve the correct structural parameters. In Gadotti (2008), further tests with similar images showed that the uncertainties estimated by the code for each fitted parameter are realistic. In Appendix A, we perform new tests, and check how the fits in this study depend on the input parameters, using SDSS r-band images of 20 barred galaxies in our sample. The choice for barred galaxies assures that the results from these tests concern typically difficult fits. The results are encouraging. They show that, in most cases, the code converges to similar results (generally consistent within the estimated uncertainties) for input parameters varying up to a factor of 4. Furthermore, wrong fits can, in general, be recognized by their unusually high χ2 values.
A critical point at this stage is to decide on which components the model of the galaxy should include. With this aim, the inspection of the galaxy image, isophotal contours and intensity profile was also very helpful. A bulge component was included in the model if the intensity profile is clearly not a single exponential function. In the absence of bars or spiral arms, it might not be clear only by inspecting the image if a galaxy has or not a disc component. The latter might become easier to identify when checking the isophotal contours for significant differences in position angle and/or ellipticity between the inner and outer parts of the galaxy. In addition, an outer exponential component in the intensity profile is naturally also an indication of the presence of a disc. A disc was included in the model whenever one of such signatures was found. To check for the presence of a bar, we first inspected the galaxy image. If in doubt, we then looked for the typical bar signatures in the isophotal contours and the intensity profile, i.e. respectively, an elongated structure with constant position angle and a flat ledge in the profile (see e.g. Gadotti et al. 2007). A bright AGN could be discerned if the profile has a cusp in the centre. However, even bright AGN are smoothed out if the physical spatial resolution of the image is not high enough (see Gadotti 2008). Accordingly, none of our images presents such a feature, and thus no galaxy in our sample required an AGN component in the fit.
Evidently, however, some cases are less clear, and one cannot rule out the possibility of us fitting a truly elliptical galaxy with a model containing bulge and disc, or conversely, fitting an unbarred lenticular galaxy with only a bulge model. In some of the latter cases, a first fit resulted in a bad match to the galaxy image, usually a bulge with an obviously too low Sérsic index. In most of these cases, another fit, including a disc component, produced a better match, revealing the true nature of the galaxy. To check that our decision on whether or not adding a disc component in a given fit is reliable, we have performed the following tests. We randomly selected 20 galaxies judged as ellipticals and produced test fits with a disc component. Conversely, we randomly selected 20 galaxies judged as unbarred lenticulars and produced test fits without a disc component. It turned out that, for the ellipticals, only one test fit resulted in a lower χ2, and, for the lenticulars, two test fits resulted in similar χ2 values. Nevertheless, none of such cases is significantly improved fits, and most of these test fits resulted in unmistakably worse matches to the galaxy images. Furthermore, the disc component found in the tested ellipticals never contributes with more than a few per cent of the total galaxy luminosity. It should also be mentioned that, due to the limited physical spatial resolution of our images, we likely missed most bars shorter than Lbar≈ 2– 3 kpc, typically seen in very late type spirals (later than Sc –Elmegreen & Elmegreen 1985). The whole of these faint bars is typically within two to four seeing elements, and thus they do not imprint clear signatures in either the isophotal contours or the intensity profile. Note that, in contrast, bulges with re of the order of one seeing HWHM can still be identified in the intensity profile, since they usually contain a much larger fraction of the galaxy light than these short and faint bars.
This procedure was performed using several suitable tasks in iraf.2 The fits to each galaxy were first done in the r band, until a satisfactory model is achieved. Then, the same input parameters which resulted in the final r-band fit were used to fit the g- and i-band images, with the luminosity parameters scaled accordingly. In addition, in some cases, geometrical parameters such as ellipticities and position angles were kept fixed at the values found with the r-band image. A model was deemed incorrect if any of the fitted parameters assumed a value which is clearly wrong, but this was uncommon. A typical case concerns the bulge Sérsic index. If n was found to be outside the range 0.8 ≤n≤ 6, then a new set of input parameters was tried in a new fit. Usually, the subsequent fits returned values for n within this range, as well as smaller uncertainties in the fitted parameters, and a lower χ2. In these cases, we sticked to the new fit. In some other cases, however, the resulting model did not change after changing the initial parameters. When this happened, we considered the model appropriate. Only occasionally, a more detailed comparison between galaxy image and model was done, e.g. by comparing both intensity profiles.
Fig. 4 shows examples of the fits obtained for six galaxies in the sample. These include an elliptical galaxy, two galaxies with a classical bulge (one barred galaxy and one unbarred), two galaxies with a pseudo-bulge (again barred and unbarred) and a bulgeless galaxy. The distinction between classical bulges and pseudo-bulges is explained in details in Section 4.2. One sees that the fits are generally quite good, even though the physical spatial resolution of the images is restricted, and despite the fact that, given the size of our sample, we could not make a thorough comparison between galaxy and model before accepting the fit to every single galaxy in the sample. This would require an unreasonable amount of time to complete the study for the whole sample. The discrepancies between galaxy and model are usually below 0.3 mag arcsec−2 and are mainly caused by substructures such as spiral arms, rings, lenses and bar ansae. It is clear that, if we cannot ascertain that the fits are excellent for a single specific galaxy, the results from the fits are, on average, trustworthy, and thus suitable for statistical studies.
4.1 A comparison between different bulge-to-total indicators
The morphological (Hubble) type of a galaxy is related to several physical parameters that are an indication of the galaxy formation and evolution processes (e.g. Roberts & Haynes 1994). One of the basic features on which the morphological classification of a galaxy hinges on is the relative importance of the bulge component to the overall light distribution of the galaxy (Hubble 1926). Thus, it is of the utmost importance to be able to measure how relevant is the bulge component within a given galaxy in an objective and quantitative fashion, even if there is some scatter in the relation between measured bulge prominence and visually determined Hubble type (e.g. Laurikainen et al. 2007; Graham & Worley 2008). Because it is difficult to objectively define the latter, the former is advantageous.
In this work, since we have performed a detailed decomposition of each galaxy image into its main components, bulge prominence is readily accessible from the bulge-to-total luminosity ratio B/T, calculated from the models obtained with budda. However, the employment of such techniques to very large samples of galaxies presents serious challenges, as automated procedures are prone to large uncertainties. Thus, other parameters, which are not so difficult to determine, have been suggested as a measure of bulge prominence. One of such parameters is the Petrosian concentration index, defined as the ratio R90/R50, where R90 and R50 are, respectively, the radii enclosing 90 and 50 per cent of the galaxy luminosity (see Kauffmann et al. 2003b, and references therein). Another possibility is to fit the entire galaxy as a single component, with a Sérsic function, and then use the Sérsic index so obtained (e.g. Blanton et al. 2005a,b; Häussler et al. 2007).
Since we have measurements of B/T and the bulge Sérsic index for all galaxies in our sample, we can test how well concentration index and galaxy Sérsic index relate to B/T and how all these connected parameters relate to each other. This is done in Figs 5 and 6. The concentration index is taken from the SDSS data base and galaxy Sérsic index from Blanton et al. (2005a). The latter are updated values after the finding of a systematic bias in the values in Blanton et al. (2003). Fig. 5 shows that concentration correlates poorly with the bulge Sérsic index. Although one sees a tendency in the sense that bulges with higher values for n reside in galaxies with higher R90/R50, the spread is very large. This might be partly due to the fact that n is related only to the bulge component, whereas R90/R50 depends on the overall structure of the whole galaxy. Another issue is that n can have high uncertainties compared to its dynamical range. Fig. 5 also shows that R90/R50 is well correlated with B/T. Interestingly, the correlation gets notably better when the bar contribution to the total galaxy luminosity is taken into account. The correlation coefficient for R90/R50 ×B/T is 0.82, while that for R90/R50 × (B+ Bar)/T is 0.86. Although bars are more extended structures than bulges, they are usually significantly less extended than discs, which explain the better correlation of R90/R50 with (B+ Bar)/T. This means that there is an additional uncertainty when using R90/R50 as a proxy for B/T, as one galaxy with small bulge but massive bar can have a higher value of R90/R50 than an unbarred, but otherwise similar, galaxy. It is worth noting that concentration rises linearly with (B+ Bar)/T up to (B+ Bar)/T≈ 0.6, after which it stays roughly constant at ≈3, a value of concentration similar to that of massive elliptical galaxies. A linear fit to the data points with 0 < (B+ Bar)/T≤ 0.6 gives
Fig. 6 shows how the galaxy Sérsic index relates to the bulge Sérsic index, concentration, B/T and (B+ Bar)/T. All plots show a very large spread. In particular, the galaxy Sérsic index is systematically higher than the bulge Sérsic index by, on average, ≈0.8. Moreover, the galaxy Sérsic index is a poor proxy for B/T. From the previous figure, one sees that the concentration index is much more reliable in this respect. The correlation coefficients for the galaxy Sérsic index as a function of B/T and (B+ Bar)/T are, respectively, 0.43 and 0.45.
Nevertheless, it should be noted that both the galaxy and bulge Sérsic indices in Figs 5 and 6 are corrected for seeing effects, whereas the concentration index is not. It does seem, however, that seeing effects on the concentration index are small at low redshifts (Blanton et al. 2003). For a sample with a narrow range in redshift, as ours, such effects seem to be practically negligible, since the systematic variation of the average physical size of the PSF is relatively small. We verified this by plotting R90/R50 against redshift and finding no correlation whatsoever. Seeing effects would only introduce an uncertainty at each measurement, which is small compared to the spread in concentration seen at each B/T, or (B+ Bar)/T, in Fig. 5.
4.2 Identifying pseudo-bulges
As mentioned in Introduction, studies on the properties of pseudo-bulges are often characterized by having a physical spatial resolution higher than that of the SDSS images used here. It is thus legitimate to be concerned on how well can we in fact distinguish pseudo-bulges from classical bulges. One key aspect of this assessment is the comparison between the effective radius of the bulge re and the PSF HWHM of the corresponding image. Gadotti (2008) showed that the structural properties of bulges can be reliably retrieved provided that re is larger than ∼80 per cent of the PSF HWHM. This was gauged by fitting the images of very nearby galaxies, at a relatively high physical spatial resolution, and through the fitting of the same galaxies using artificially redshifted images. Fig. 7 shows that only 3 per cent of our bulges do not satisfy this criterion. If one wants to be more stringent and extend this limit to 100 per cent of the seeing radius, one still sees that only 10 per cent of our bulges are below the threshold. We have not excluded these bulges from this study but have verified that their inclusion or removal does not result in any significant change in the results presented here. This gives us confidence that the structural properties we have obtained are generally reliable even for the less conspicuous bulges. Note that our decompositions are seeing corrected.
The top two panels in Fig. 8 show the mean effective surface brightness within the effective radius 〈μe〉3 plotted against the effective radius for the bulges and elliptical galaxies in our sample. Massive elliptical galaxies follow a well-defined relation between 〈μe〉 and re, which is given by the solid line, constructed from a fit to the data. The two dashed lines are the fit's ±3σ boundaries (over the zero-point and keeping the slope fixed). This relation is known as the Kormendy relation (Kormendy 1977) and, in fact, one of the possible projections of the fundamental plane (we explore the fundamental plane relations in more detail in Section 4.4). The slope of the Kormendy relation we find here is similar (consistent within the uncertainties) to that found by Pierini et al. (2002) using H-band images. Many bulges also follow this relation. If bulges are separated according to their Sérsic index n, one sees that most of the bulges with n≥ 2 follow the ellipticals' relation, whereas most of those with n < 2 do not, lying below the relation. This is expected, since exponential bulges are often pseudo-bulges, which are believed to be structurally different from classical bulges and ellipticals (see e.g. Carollo 1999; Kormendy & Kennicutt 2004, and references therein). However, many of the bulges with n < 2 do seem to follow the same relation of ellipticals. Conversely, several bulges with n≥ 2 fall below this relation. It is thus clear that although the Sérsic index threshold can be considered as an approximation to identify pseudo-bulges (see e.g. Fisher & Drory 2008), it can introduce many misclassifications. Since pseudo-bulges are expected to be structurally different from classical bulges, and to lie below the 〈μe〉–re relation for ellipticals, we can use the lower dashed line in Fig. 8 to be the dividing line between classical bulges and pseudo-bulges. This means that pseudo-bulges satisfy the following inequality:Pierini et al. 2002), which is consistent with the expectation that pseudo-bulges are built from disc instabilities. From Fig. 8, one also sees that barred and unbarred galaxies behave in a similar fashion in what concerns their positions in the 〈μe〉–re relation. The histograms in Fig. 8 show the distributions of n and B/T for classical bulges and pseudo-bulges with n < 2 and n≥ 2 in separate panels. They show that our criterion to separate these two bulge categories can identify bulges with n < 2, but with high values of B/T, as classical bulges. These bulges have often values of n close to 2. Conversely, we are also able to identify pseudo-bulges with n≥ 2. These bulges often show low values of B/T and also values for n close to 2. These results indicate that some bulges can be erroneously classified as classical or pseudo, if one uses the Sérsic index for such classification, just for being by chance (due to measurement uncertainties) in the wrong side of the Sérsic index threshold. One sees that, as expected, pseudo-bulges show a distribution of n unlike that of classical bulges and ellipticals. In addition, the distribution of n for classical bulges is wide, and ranges from values typical of ellipticals to values in the gap between pseudo-bulges and ellipticals. Furthermore, one also sees that classical bulges have a peak in B/T around 0.4, while the corresponding value for pseudo-bulges is about 0.1.
Although it is clear that bulges with low and high Sérsic index occupy different loci in the 〈μe〉–re projection, Fig. 8 suggests that there is a more significant difference between all bulges and ellipticals than between the different bulges. To check that we have performed 2D Kolmogorov–Smirnov tests (Fasano & Franceschini 1987; Press et al. 1992). The tests show that, in fact, in this projection, ellipticals differ more from bulges (taken altogether) than bulges with high Sérsic index differ from bulges with low Sérsic index. In this context, we have checked, using the tests described in Section 3, that if a lenticular galaxy is mistaken by an elliptical, the shift in re could be at most only 0.04 dex. Thus, although such an effect, if present, would indeed bring ellipticals closer to bulges in the Kormendy relation, its amplitude is too small. In light of these results, one could ask whether a separation between classical and pseudo-bulges in the Kormendy relation is rather artificial. The density plot in Fig. 8 suggests that it is not: pseudo-bulges appear as an independent group of points, as do classical bulges and ellipticals.
Previous studies also indicate that pseudo-bulges show star-forming activity, as opposed to classical bulges, which are constituted mainly by old stellar populations (e.g. Gadotti & dos Anjos 2001; Fisher 2006). We can check this difference within our sample using both the Dn(4000) index provided in Kauffmann et al. (2003b) and the SDSS fibre colour (i.e. the colour measured within the fibre aperture). The Dn(4000) index is based on the 4000 Å discontinuity seen in optical spectra of galaxies, and it is not sensitive to dust attenuation effects. Young stellar populations have low values of Dn(4000), as compared to old stellar populations. The fibre colours are integrated over the central region of the galaxy and can suffer from dust reddening. In Fig. 9, we show the distributions of Dn(4000) and fibre g−i colour for pseudo-bulges and classical bulges. The result is striking. Our pseudo-bulges do indeed show values of Dn(4000) lower than those for classical bulges, indicating a higher level of star formation activity. Their distributions are also significantly apart (except for a tail of classical bulges showing star-forming activity). In fact, the peaks of the Dn(4000) distributions for pseudo-bulges and classical bulges coincide with the peaks in the bimodal distribution of Dn(4000) seen in both our parent and final samples (see Fig. 1). Such bimodality was also found by Allen et al. (2006), who concluded that it is produced by bulge-dominated galaxies on the one hand and disc-dominated galaxies on the other hand. More recently, Drory & Fisher (2007) suggested that such bimodality is a result of the two different bulge families: pseudo-bulges are hosted by galaxies with high overall star formation activity, whereas classical bulges reside in galaxies that underwent violent relaxation processes in the past, such as mergers, and thus have formed most of their stars in these past events. Both suggestions are not mutually exclusive, since galaxies with pseudo-bulges are often disc-dominated galaxies, as opposed to bulge-dominated galaxies, which often host classical bulges. In fact, our results indicate that the most disc-dominated galaxies almost always host pseudo-bulges, which are almost always under current intense star-forming activity, whereas classical bulges are mostly quiescent and reside mainly in more bulge-dominated galaxies. Interestingly enough, star-forming classical bulges form a group of points of their own in the density plot of Fig. 8, between the lower dashed line and the solid line. We will come back to these points further below. We have verified that if one separates bulges using their Sérsic index with a threshold at n= 2, the resulting Dn(4000) distributions are similar, and one also sees a tail of star-forming bulges with n≥ 2. In this case, however, the peaks of such distributions are slightly closer, and the distribution for bulges with n < 2 is broader than that of our pseudo-bulges. This gives support to our criterion to identify pseudo-bulges.
The colour distributions are also separated, though in a less dramatic way. Pseudo-bulges show bluer colours than classical bulges, on average, but the difference in the mean colour values amounts only to 0.2 mag. Evidently, dust reddening does play a role in making these distributions more similar, as compared to those of Dn(4000). Some dust attenuation is expected even in face-on galaxies (e.g. Driver et al. 2008). The fact that the colour distribution of pseudo-bulges is wider than that of classical bulges is also a result of dust attenuation. On one hand, there are those pseudo-bulges with not much dust attenuation, whose intense star formation shows up as the resulting blue colours (and the blue tail in the distribution). And, on the other hand, there are those pseudo-bulges with dust-obscured star formation that produce the red colours seen in the red tail of the distribution. One can have an estimate of the dust reddening in our bulges, using estimates of the total galaxy dust attenuation in Kauffmann et al. (2003b) as an upper limit (i.e. considering that all dust attenuation in the galaxy strikes the bulge light). We calculated the average dust attenuation in the i band using the results for the z band in Kauffmann et al. (2003b), and assuming that dust attenuation goes as λ−0.7 (where λ is the observed wavelength). The average i-band attenuation we thus find for our elliptical galaxies and galaxies with classical and pseudo-bulges is, respectively, 0.04, 0.16 and 0.48 mag. This corresponds to g−i colour excesses of, respectively, 0.02, 0.08 and 0.15 mag. The colour excess for classical and pseudo-bulges are indicated by the arrows in the lower panel of Fig. 9. Interestingly, the difference in the position of the peaks of the Dn(4000) distributions amounts to 0.60, while the corresponding difference for fibre g−i colour is, as mentioned above, 0.20 mag (without any dust correction) and 0.27 mag (with the upper limit dust correction).
Since the Dn(4000) values and fibre colours are taken from SDSS spectra, which are themselves taken through a fixed fibre aperture of 3 arcsec (thus 1.5 arcsec in radius), and since pseudo-bulges are often smaller than classical bulges, one might ask whether the striking difference in Dn(4000) between pseudo-bulges and classical bulges in our sample is only due to aperture effects. One could argue that, due to the smaller extent of pseudo-bulges within the fibre aperture, the Dn(4000) values (and similarly the fibre colours) for pseudo-bulges are contaminated with star formation in the disc. In fact, the average effective radius of pseudo-bulges and classical bulges is, respectively, 0.82 and 1.14 arcsec. However, one must bear in mind that bulge light dominates over disc light through ≈2 times the bulge effective radius from the galaxy centre. This is borne out in our surface brightness profiles, and has also been found by others (see e.g. Moriondo, Giovanelli & Haynes 1998; Morelli et al. 2008). Nevertheless, to be reassured that the difference seen in Dn(4000) is not just a spurious effect, we have verified that the difference in the mean values of Dn(4000) for pseudo-bulges and classical bulges is similar when all bulges are separated in bins of similar effective radius. In particular, we have verified that all results from Fig. 9 hold if one considers only bulges with re > 1, or 1.5 arcsec, where little disc contamination is expected. Furthermore, we have also verified that the SDSS fibre colours are, in fact, much more similar to the integrated bulge colours, as calculated with the determined budda models for the g- and i-band images, than the corresponding disc colours. We thus conclude that one cannot blame disc contamination within the SDSS spectra to explain the higher star formation activity and bluer colours seen in our pseudo-bulges.
Our sample was designed in a way to minimize dust effects. In fact, most of our galaxies have dust attenuation measurements in the low end of the distribution of dust attenuation for the whole sample of more than 105 galaxies in Kauffmann et al. (2003b). Nevertheless, it is clear that the high star formation activity seen in pseudo-bulges is accompanied to some extent with dust obscuration. Could this somehow affect the structural parameters obtained? To answer this question, we plot in Fig. 10 the bulge structural parameters obtained with the g-band images against the same parameters obtained with the i-band images. Dust has more pronounced effects in bluer bands and thus, if there are some systematic effects caused by dust in our decompositions, these should show up in these plots, in particular for pseudo-bulges. For instance, dust attenuation could, in principle, result in systematically lower values for n, as well as smaller values for re, in the g band, as compared to those in the i band. Fig. 10 shows no substantial systematic effects. We thus conclude that our decompositions are not significantly disturbed by dust. This is consistent with the findings in Moriondo et al. (1998), who found that bulge structural parameters do not change significantly with galaxy inclination.
4.3 Scaling relations
Fig. 11 shows the relations between the bulge Sérsic index and bulge-to-total luminosity ratio, effective surface brightness and effective radius for pseudo-bulges, classical bulges and ellipticals. The relations between the bulge-to-total luminosity ratio and effective surface brightness and effective radius are also shown. It is striking how these three stellar systems populate well defined and separate regions in some of these diagrams. Systems with larger n tend to be more conspicuous and extended. One sees a correlation between n and B/T for classical bulges but not as much for pseudo-bulges, corroborating the results from Fisher & Drory (2008), who arrived at a similar conclusion using a smaller sample. It is worth noting that n rises with re for bulges but it is rather constant for ellipticals. Furthermore, there is a correlation between B/T and re for both classical and pseudo-bulges, although they seem to follow offset relations. Ellipticals tend to be more extended than bulges and have lower effective surface brightness than classical bulges. Note that no difference is seen in Fig. 11 when comparing galaxies with different axial ratios. We have also found that systems with larger n and B/T tend to be in more massive galaxies, although the scatter is large.
In Fig. 12, we show that, as expected, galaxies with more extended bulges or discs tend to be more luminous and massive. This is also true for systems with lower axial ratios. One might also ask whether a similar relation is found if one considers the component mass, rather than the total mass in the galaxy. Although several stellar systems seem to follow such a relation, there might be exceptions, such as globular clusters (see Burstein et al. 1997; Kissler-Patig, Jordán & Bastian 2006; Barmby et al. 2007). This is answered in Fig. 13. One sees that such a correlation indeed exits for pseudo-bulges, classical bulges, bars and discs, separately, regardless of galaxy axial ratio. This figure also shows fits to the data, where scalelengths go as ∝Mα, where α is a constant that defines the slope of the relation and M is the component stellar mass. The values we have found for α for bars, discs, pseudo-bulges, classical bulges and ellipticals are, respectively, 0.21, 0.33, 0.20, 0.30 and 0.38, with a mean 1σ uncertainty of 0.02; thus α seems to increase for more massive components. It is interesting to note that bars and pseudo-bulges share a very similar value of α (and these are the only components that do so), which is different from that of classical bulges at a 5σ level. This not only suggests a different formation mechanism for classical and pseudo-bulges, but also reveals a close connection between pseudo-bulges and bars. Such a connection is expected if pseudo-bulges indeed form through disc instabilities. None the less, despite such difference in slope, the locus occupied by classical bulges in such diagram continues rather smoothly from the locus of pseudo-bulges. This suggests that although there might be two different dominant formation processes for classical and pseudo-bulges, there can be a significant number of cases where the different processes are at play concomitantly. Thus, the sequence drawn by pseudo-bulges and classical bulges could represent a sequence where the dominant process changes rather smoothly from one end to the other.
Another striking feature in Fig. 13 concerns ellipticals. They are more offset from classical bulges than classical bulges are offset from pseudo-bulges, as 2D Kolmogorov–Smirnov tests indicate. In fact, one sees that most classical bulges cannot be considered as ellipticals that happen to be surrounded by a disc, at least not ellipticals more massive than 1010 M⊙. How robust this result is against the possible systematic effects from the decompositions? We explore now two possibilities. The first is that some of the ellipticals could actually be lenticulars whose discs were not identified in the preparation of the fits. As mentioned in Section 3, we produced test fits in which a disc component was forced in 20 ellipticals, and found that in only one case the inclusion of a disc could be justified. However, such a disc contributes with only a few per cent of the total galaxy luminosity, and the resulting shift in re, towards lower values, is only of the order of a few hundred parsec. The second possibility is that the input values given to the code to fit re are systematically larger for ellipticals. We have thus performed yet another test, again producing test fits for 20 ellipticals but this time with the input values for re cut by half. In most cases, the result was similar to the original fit (which incidentally attests the robustness of the code). In a few cases, the shift in the final value for re is again only a few hundred parsec towards lower values; and in all such cases, the resulting χ2 is substantially worse than that of the original fit. We thus conclude that such systematic effects could, in principle, bring some of the low-mass ellipticals closer to classical bulges in Fig. 13, but the result that at least a significant fraction of classical bulges cannot be considered as (massive) ellipticals surrounded by discs seems to be robust. Note that Fisher & Drory (2008) argue that classical bulges resemble low-luminosity ellipticals.
With these data, we can test previous claims that the Hubble sequence is scale-free, i.e. the relation between the scalelengths of bulges and discs does not vary with Hubble type (Courteau, de Jong & Broeils 1996). In this context, Graham & Prieto (1999) showed that fixing the bulge Sérsic index, when fitting galaxy surface brightness profiles, can lead to an overestimate or an underestimate of re, depending on the true value of n. Since n is a free parameter in our decompositions, our results are not subject to such systematic biases. In Fig. 14, we plot re/h against B/T for pseudo-bulges and classical bulges. This figure shows clearly that re/h and B/T are correlated, and thus the Hubble sequence is not scale-free, if it is a B/T sequence. Balcells, Graham & Peletier (2007) and Laurikainen et al. (2007) reached similar results, though with much smaller samples. Fig. 14 also indicates that the relations for pseudo-bulges and classical bulges are offset: for a constant B/T, pseudo-bulges have on average higher values of re/h.
It is well known that galaxies can be separated depending on the locus they occupy in a colour–magnitude diagram. Some galaxies follow a tight colour–magnitude relation, in the sense that more luminous galaxies are redder, known as the red sequence, whereas others spread beside the red sequence, originating a swarm of points known as the blue cloud (see e.g. Gladders et al. 1998; Bell et al. 2007, and references therein). Such a diagram is a powerful tool, able to provide clues on the formation and evolutionary processes of galaxies (see e.g. De Lucia et al. 2007). Drory & Fisher (2007), based on a careful analysis of a sample of 39 galaxies, suggested that galaxies with pseudo-bulges populate the blue cloud, while galaxies with classical bulges populate the red sequence. But colour can be subject to dust attenuation effects, and galaxy magnitude is actually used as a proxy to galaxy stellar mass. Since we have measurements of Dn(4000), an efficient, dust-insensitive index to identify stellar populations with different mean ages, as well as carefully modelled stellar masses, we can go a step further and plot Dn(4000) against galaxy stellar mass, as is done in Fig. 15. It should be noted that often one uses the total galaxy colour in the colour–magnitude diagram, whereas our Dn(4000) values correspond to the central galaxy colour. That is, however, an asset, since, as argued in Section 4.2, the light that goes through the SDSS fibre, from which Dn(4000) is measured, is in our sample mostly emitted by stars in the bulge, meaning that our Fig. 15 is mainly a comparison between ellipticals, classical bulges and pseudo-bulges, avoiding in most cases effects resulting from disc light. None the less, we have verified that similar results emerge if we plot the colour–magnitude diagram in its usual form, using dereddened g−i Petrosian colours from the SDSS data base and absolute magnitudes from Kauffmann et al. (2003b). In such case, however, the blue cloud is not as detached from the red sequence as in Fig. 15, most likely due to dust attenuation. Our results clearly show that virtually all elliptical galaxies are found in the red sequence; and practically all galaxies with pseudo-bulges, and bulgeless galaxies, are found in the blue cloud. However, although most of the galaxies with classical bulges do indeed populate the red sequence, a significant fraction of them are found in the blue cloud (see also Fig. 9).
4.4 The fundamental plane
Elliptical galaxies follow well-defined relations between their effective radius re, mean effective surface brightness 〈μe〉 and central velocity dispersion σ0, known as the fundamental plane (FP). Furthermore, it is possible to show that such relations arise in virialized systems (Djorgovski & Davis 1987; Dressler et al. 1987; Bender, Burstein & Faber 1992). Thus, the FP provides important clues on the formation processes of stellar systems. Bender et al. (1992) proposed a formulation of the FP, defining a space, whose three axes, κ1, κ2 and κ3, are defined in terms of re, 〈μe〉 and σ0, and are proportional to important physical parameters: κ1 is proportional to the logarithm of the mass, κ2 is proportional mainly to the logarithm of the surface brightness and κ3 is proportional to the logarithm of the mass-to-light ratio. Here, mass means dynamical mass, i.e. the stellar mass plus the dark matter mass content.
What is the locus occupied by pseudo-bulges and classical bulges in the FP? We can answer this question using re and 〈μe〉 from our decompositions, and velocity dispersion measurements from the SDSS data base. We have chosen to use the estimates provided in the Data Release 6 (DR6), which are based on results from a direct fit to the spectra. In earlier releases, the estimates are an average of results from direct-fitting and Fourier-fitting, but the latter systematically overestimates the velocity dispersion for low-mass galaxies (Bernardi et al. 2003a; their fig. 17). In fact, we have verified that the velocity dispersion estimates from DR2 are systematically larger (by ∼10–20 per cent) than those from DR6, for the galaxies in our sample, when the velocity dispersion is below ≈150 km s−1. Due to the limited spectral resolution of the SDSS spectra, it is recommended to use only spectra with signal-to-noise ratio above 10, and without warning flags. We have verified that only one galaxy in our sample does not comply with the former criterion, and only eight do not comply with the latter. Before we can use these measurements, we have to apply aperture corrections due to the fact that these velocity dispersions are obtained through a fixed fibre aperture of 3 arcsec, which is physically different from galaxy to galaxy, depending on their distances. We thus used the prescription provided by Jorgensen, Franx & Kjaergaard (1995) and converted the SDSS velocity dispersion measurements to the velocity dispersion at 1/8 of re, σ8. This empirical prescription is based on measurements for elliptical and lenticular galaxies, and it is unclear if it is also valid for disc-dominated galaxies. However, the corrections applied are small, and do not affect our results significantly.
We thus calculated κ1, κ2 and κ3 for elliptical galaxies, classical bulges and pseudo-bulges, using the definitions in Bender et al. (1992), and applying an offset in surface brightness to facilitate comparison with Bender et al. (1992) and Burstein et al. (1997), who used measurements in the B band (the same procedure was also done by Bernardi et al. 2003b). The top panels of Fig. 16 show that the relation we have found for κ3 against κ1, considering only elliptical galaxies, is similar to that found by Bernardi et al. (2003b), which used SDSS i-band data for a sample of nearly 9000 early-type galaxies. Bernardi et al. (2003b) used estimates of the velocity dispersion that includes Fourier-fitting results, which, as mentioned above, overestimate the velocity dispersion for low-mass galaxies. Accordingly, their relation is somewhat less steep than ours, even though they have excluded estimates below 100 km s−1. We find thatFalcón-Barroso, Peletier & Balcells 2002). Classical bulges follow more closely the relation found by Bernardi et al. (2003b). It should be noted that their sample also includes early-type disc galaxies. To select their sample of early-type galaxies, they have included only galaxies with the concentration index R90/R50 larger than 2.5. This does not mean, however, that their sample contains only elliptical galaxies. In fact, we have checked that 99 per cent of our ellipticals have R90/R50 > 2.5, but this is also the case for 76 per cent of our galaxies with classical bulges and 8 per cent of our galaxies with pseudo-bulges. Bernardi et al. (2003a) also used other criteria to avoid including late-type galaxies in their sample, but it is unlikely that these criteria excluded most of the galaxies with classical bulges. This can also explain why our relation for ellipticals is slightly different from theirs.
Pseudo-bulges in both barred and unbarred galaxies lie significantly and systematically above these relations. This offset cannot be attributed to effects due to dust attenuation alone. Even considering the upper limit for dust attenuation discussed in Section 4.2, such a correction will bring the points down vertically by 0.19 in κ3, while one sees that the offset is ≈0.3, on average. In this projection, 2D Kolmogorov–Smirnov tests indicate that pseudo-bulges differ more from classical bulges than ellipticals differ from classical bulges or bulges altogether. Pseudo-bulges also lie in a locus in the κ2×κ1 projection of the FP which is different from those of both ellipticals and classical bulges (bottom panel of Fig. 16). Again, correcting for upper limit dust effects would put pseudo-bulges up along the κ2 axis only by 0.27. In this projection, the statistical tests indicate that pseudo-bulges differ from classical bulges as much as ellipticals differ from classical bulges or bulges altogether. In both projections, pseudo-bulges lie in regions close to those occupied by disc-dominated galaxies (see Pierini et al. 2002). We note that barred galaxies tend to be more separated from their unbarred counterparts in the case of galaxies with pseudo-bulges, as compared to galaxies with classical bulges. Barred galaxies seem to have slightly higher values of both κ2 and κ3, on average. This is also confirmed with the statistical tests. Finally, it is also worth noting that, as expected from the results in Section 4.3, systems with lower axial ratios seem to generally share the same properties as those with b/a≥ 0.9.
Fig. 17 shows the distributions of the disc parameters (μ0, h and D/T). It is worth noting that the distribution of disc-to-total ratio shows two peaks which match the peaks in the bulge-to-total ratio distributions for classical bulges and pseudo-bulges (shown in Fig. 8). The two peaks in the distribution of D/T are at about 0.5 and 0.9. Bars account typically for 10 per cent of the galaxy luminosity. In Fig. 18, we show the scaling relation between disc scalelength and central surface brightness. When one separates galaxies by their bulge type (classical versus pseudo), one sees that, on average, galaxies with pseudo-bulges have more extended discs, with fainter central surface brightness, as compared with galaxies hosting classical bulges, albeit with significant overlap. A Kolmogorov–Smirnov test rejects the null hypothesis of no difference between such distributions at a 92 per cent confidence level. It is also interesting to ask how the stellar mass in discs varies between these two galaxy classes. The stellar mass in discs of galaxies with pseudo-bulges is, on average, 1.15 × 1010 M⊙, whereas that in discs of galaxies with classical bulges is 1.93 × 1010 M⊙, thus a factor of 1.7 larger. A similar factor (1.8) corresponds to bars, when present. We can also ask how do their bulge masses compare. The stellar mass within pseudo-bulges is typically 2.2 × 109 M⊙, whereas in classical bulges this is 1.41 × 1010 M⊙ (see Table 4), thus a factor of 6.4 larger. Hence, in terms of stellar mass, there is more similarity between discs (and bars) in galaxies with pseudo-bulges and those in galaxies with classical bulges, than between classical and pseudo-bulges themselves. Furthermore, the mean difference between the total galaxy mass of galaxies hosting pseudo-bulges and of those with classical bulges is a factor of 2. Therefore, if one scales down a typical galaxy with a classical bulge, dividing the mass of each of its components by 2, one ends up with a galaxy that has a disc (and a bar) with mass similar to that of the corresponding component in galaxies with pseudo-bulges. However, the bulge of such scaled-down galaxy is around three times more massive than the typical pseudo-bulge. If we assume that the physical processes that lead to the formation of discs and bars are the same regardless of the resulting bulge, then this difference suggests that the formation processes of classical bulges and pseudo-bulges are typically distinct.
|Median (1010 M⊙)||SD (1010 M⊙)|
|Median (1010 M⊙)||SD (1010 M⊙)|
4.6 A compendium of galaxy structural parameters
The full results from our decompositions are given in Tables 1 and 2. Table 3 shows the parameters describing the distributions (median and standard deviation), as well as the mean 1σ uncertainty in individual measurements, of μe, re and n for elliptical galaxies, classical bulges and pseudo-bulges.
|μ0 (1)||h (2)||μe (3)||re (4)||n (5)||μe,bar (6)||re,bar (7)||εbar (8)||nbar (9)||Lbar (10)||c (11)||B/T (12)||D/T (13)||Bar/T (14)||χ2 (15)||SeeingHWHM (16)||z (17)|
|μ0 (1)||h (2)||μe (3)||re (4)||n (5)||μe,bar (6)||re,bar (7)||εbar (8)||nbar (9)||Lbar (10)||c (11)||B/T (12)||D/T (13)||Bar/T (14)||χ2 (15)||SeeingHWHM (16)||z (17)|
Columns (1) and (2) show the disc central surface brightness and scalelength, respectively. Columns (3) to (5) give, respectively, bulge effective surface brightness, effective radius and the Sérsic index. Bar parameters are given in columns (6) to (11), respectively, effective surface brightness, effective radius, ellipticity, the Sérsic index, semimajor axis and boxyness. Bulge-to-total, disc-to-total and bar-to-total luminosity ratios are given in columns (12), (13) and (14), respectively. The χ2 value of the fit is shown in column (15). Finally, columns (16) and (17) show, respectively, the seeing HWHM of the observation and the galaxy redshift. Intensities are in units of mag arcsec−2 and lengths in kpc. Seeing is in arcsec.
|Md(g) (1)||Md(r) (2)||Md(i) (3)||Mb(g) (4)||Mb(r) (5)||Mb(i) (6)||Mbar(g) (7)||Mbar(r) (8)||Mbar(i) (9)||(g−i)d (10)||(r−i)d (11)||(g−i)b (12)||(r−i)b (13)||(g−i)bar (14)||(r−i)bar (15)|
|Md(g) (1)||Md(r) (2)||Md(i) (3)||Mb(g) (4)||Mb(r) (5)||Mb(i) (6)||Mbar(g) (7)||Mbar(r) (8)||Mbar(i) (9)||(g−i)d (10)||(r−i)d (11)||(g−i)b (12)||(r−i)b (13)||(g−i)bar (14)||(r−i)bar (15)|
Columns (1) to (3) show the disc absolute magnitude in the g, r and i bands, respectively. Columns (4) to (9) show the same parameters for bulge and bar, respectively, as indicated. Columns (10) and (11), (12) and (13) and (14) and (15) give the integrated (g−i) and (r−i) colours of disc, bulge and bar, respectively, as indicated.
|μe (mag arcsec−2)||re (kpc)||n|
|μe (mag arcsec−2)||re (kpc)||n|
Evidently, theoretical work on galaxy formation and evolution should comply with these results, either by predicting compatible structural properties or by using these results as a starting point to build realistic models. The same thing can be said about the masses of the different components, and their mass distributions, which are presented in the next section. These results are also useful to test automated procedures of bulge/disc/bar 2D decomposition, with no checking or direct human intervention at the decomposition of every single object. An automated code able to reproduce these results using the same input data (i.e. the same images) should be deemed successful and reliable to be used with much larger samples, which are lately becoming commonly available. The results from our image decompositions are available for download.4 These include all structural parameters of bulges, discs and bars in the g, r and i bands, absolute magnitudes and integrated g−i and r−i colours of each component separately, as well as model images for the whole galaxy and for each component separately.
4.7 The stellar mass and luminosity budgets at z∼ 0
With the g−i integrated colour of each galaxy component, we have obtained the corresponding mass-to-light ratio in the i band, using the results found by Kauffmann et al. (2007, see their fig. 15). They showed that the mass-to-light ratio in the i band is well correlated with g−i colour over a range of more than a factor of 10 in the mass-to-light ratio and with a scatter of less than 0.1 dex. They found that the g−i colour is the colour that shows the tightest relation with the mass-to-light ratio. Furthermore, Bell & de Jong (2001) showed that the combined effects of stellar age and dust attenuation are such that the stellar masses obtained here with these mass-to-light ratios are not significantly affected by dust.
With the mass-to-light ratio and the total luminosity of each component, we were thus able to calculate the stellar mass content in each component separately. Interestingly, we have verified that the total mass in each galaxy, calculated by adding the masses of the individual galaxy components, agrees very well with the galaxy stellar mass estimated in Kauffmann et al. (2003b), with a scatter of less than 0.02 dex. The parameters that characterize the stellar mass distributions of each galaxy component (median and standard deviation) are shown in Table 4. All such distributions are skewed towards lower mass values.
We were also able to compute the fraction of the total stellar mass content in our galaxies contained within each component separately, thus obtaining the stellar mass budget in the local universe for massive galaxies (more massive than 1010 M⊙). The following figures take into account the selection effect due to our axial ratio cut discussed in Section 2. Elliptical galaxies contain 32 per cent of the total stellar mass, and the corresponding values for discs, bulges and bars are, respectively, 36, 28 and 4 per cent. Classical bulges contain 25 per cent of the total stellar mass, while pseudo-bulges contain 3 per cent. Hence, 11 per cent of the stellar mass in bulges are in pseudo-bulges, the remaining being in classical bulges. The uncertainty in these fractions from Poisson statistics only is between 1 and 2 per cent points.
The corresponding luminosity fractions are as follows: 27 per cent of the total luminosity from the galaxies in our sample (in the i band) come from elliptical galaxies, 46 per cent from discs, 24 per cent from bulges and 3 per cent from bars. Classical bulges emit 20 per cent of the total luminosity, while pseudo-bulges account for 4 per cent. Hence, 16 per cent of the luminosity from bulges come from pseudo-bulges, the remaining coming from classical bulges.
As expected, luminosity ratios, such as the bulge-to-total ratio B/T, change in different bands. For pseudo-bulges, the median value of B/T in the g band is 0.053, whereas in the i band it is 0.075. For classical bulges, the median value of B/T in the g band is 0.349, and in the i band is 0.377. The median value of Bar/T also increases from 0.087 in the g band to 0.095 in the i band. The median value of D/T decreases from 0.702 in the g band to 0.684 in the i band.
It is also worth noting the fraction in number corresponding to the different galaxy categories. From the total number of galaxies in our sample, 22 per cent are ellipticals, 76 per cent are disc galaxies with bulges and 2 per cent are bulgeless galaxies (i.e. pure discs). Within disc galaxies with bulges, 68 per cent host classical bulges, while 32 per cent have pseudo-bulges. Bars are found in 42 per cent of all disc galaxies.
5.1 Comparison with previous work
Allen et al. (2006) also performed parametric decomposition of a large sample of galaxy images. As mentioned in Introduction, their sample is significantly larger than ours, but our methodology aims at a more careful analysis. They found that the stellar mass content in the local universe is distributed as 13 per cent in elliptical galaxies, 58 per cent in discs, 26 per cent in classical bulges, 1.5 per cent in pseudo-bulges and the remainder in low-luminosity blue spheroids (Driver et al. 2007a, see also Benson et al. 2007 who found that 35–51 per cent of the stellar mass is in discs). The figures do not change substantially when dust is taken into account (Driver et al. 2007b). A direct comparison with our results is difficult, since their sample was not selected with a cut in stellar mass. As we avoided low-mass galaxies, it is natural to expect that we find a larger fraction of the local stellar mass in ellipticals, and a corresponding lower fraction in discs. Interestingly, however, their fraction of stellar mass in classical bulges is similar to what we find. This is somewhat unexpected, considering the different sample selection criteria, since their sample should contain a larger fraction of disc-dominated galaxies than our sample. This might be explained by the absence of a bar component in their models. As discussed in Gadotti (2008), it is possible to obtain good (but wrong) fits for barred galaxies, with no bar component in the model, because the bulge model absorbs the bar. Thus, their bulge-to-total luminosity ratios could be overestimated. They have considered pseudo-bulges as those with B/T < 0.5 and re/h < 0.5, and found them to be generally bluer than the remaining bulges. From our Fig. 14, one sees that such criteria still include many classical bulges. However, they found a stellar content in pseudo-bulges smaller than ours, albeit within the uncertainties. A possible explanation for that could be that a number of their pseudo-bulges were smoothed out by the PSF. Although they have secured that the galaxies in their sample have effective radii larger than the PSF HWHM, it was shown in Gadotti (2008) that it is the effective radius of the bulge that has to be considered, and not that of the whole galaxy. This issue is aggravated in Benson et al. (2007), who used SDSS images up to a redshift of 0.3.
In order to try a more meaningful comparison with the results in Driver et al. (2007a), we can assume that all galaxies with stellar masses below 1010 M⊙ are pure discs. This certainly underestimates the stellar mass content in bars and pseudo-bulges, but can give us a reasonable assessment of the distribution of stellar mass in discs, ellipticals and classical bulges, as if we have made no mass cut. Using the stellar mass function derived by Bell et al. (2003), using g-band data for a local sample of SDSS galaxies, we find that 22 per cent of the stellar mass in the local universe is in galaxies with stellar masses below 1010 M⊙. If all this mass is in discs, then our local stellar mass budget becomes as follows. Discs contain 50 per cent of the stellar mass, ellipticals contain 25 per cent of stellar mass, classical bulges and pseudo-bulges contribute with, respectively, 20 and 2 per cent, and finally bars contain 3 per cent of the stellar mass. One thus sees a more reasonable agreement, although we find a somewhat larger mass fraction in ellipticals.
In Gadotti (2008), it was argued, with indirect means, that the stellar mass content in bars at z∼ 0 is ≈12 per cent of the total stellar mass (see also Weinzirl et al. 2008), which is a factor of 3 larger than what we find here. This discrepancy can be explained, at least partially, by two factors. First, the bar fraction assumed in the previous work is 70 per cent, which is typically found in studies dedicated to estimate this value (see e.g. Eskridge et al. 2000), whereas the fraction of disc galaxies with bars in this work is 42 per cent. Secondly, we have selected our galaxy sample avoiding galaxies with low stellar mass. Thus, the stellar mass budget we find concerns massive galaxies, and it is thus biased in favour of ellipticals, which cannot contain the bars we are addressing here. The fact that our bar fraction is low can also be explained by two factors. First, as discussed in Section 3, we miss most of the short bars, due to the limited spatial resolution in SDSS images. Secondly, bar fraction seems to be larger in low-mass galaxies than in more massive galaxies (Barazza, Jogee & Marinova 2008).
5.2 Classical bulges with star formation
One interesting finding from Figs 9 and 15 is that while pseudo-bulges show almost always intense star formation, classical bulges can either be quiescent or forming young stars. This indicates that galaxies with classical bulges can be further divided according to their values of Dn(4000). We have thus separated classical bulges in two different categories, namely those with and those with Dn(4000) ≥ 1.7, and find that these categories have typically different bulge-to-total ratios and stellar masses. Galaxies hosting classical bulges with Dn(4000) < 1.7 have median values of B/T= 0.26 and mass equal to 0.8 × 1010 M⊙, whereas those with Dn(4000) ≥ 1.7 have median values of B/T= 0.42 and mass equal to 1.8 × 1010 M⊙. This suggests that the former are dominated by early-type spirals whereas the latter are mostly lenticular galaxies. To verify that we have inspected randomly selected samples of these two galaxy categories and concluded that, in fact, galaxies hosting classical bulges with Dn(4000) < 1.7 show more often spiral structure and blue discs than galaxies hosting classical bulges with Dn(4000) ≥ 1.7 (see Fig. 19). In addition, we show in Fig. 20 that these galaxies have markedly different distributions of the concentration index R90/R50. Furthermore, galaxies with pseudo-bulges also show a distribution of R90/R50 distinct from that of both categories of galaxies with classical bulges. Elliptical galaxies, however, have a R90/R50 distribution more similar to that of galaxies with classical bulges and Dn(4000) ≥ 1.7. We thus see three peaks in the distribution of concentration. A related finding is reported in Bailin & Harris (2008). As expected, the median Sérsic index of star-forming classical bulges is 2.8, thus lower than that of quiescent classical bulges, for which it is 3.6.
A plausible explanation for the existence of galaxies hosting classical bulges with conspicuous star formation activity is the coexistence of a classical bulge and a pseudo-bulge in the same galaxy. This would naturally occur if, after the formation of the classical bulge (e.g. via a minor merger), the galaxy disc develops an instability (such as a bar) able to induce the observed central star formation through processes of secular evolution.5 Since pseudo-bulges are about an order of magnitude less massive than classical bulges (see Table 4), such composite bulges would have the structural signature of a classical bulge, concurrent with the star formation activity of a pseudo-bulge, as observed. The fact that the Dn(4000) values of star-forming classical bulges and pseudo-bulges are similar (see Fig. 9) is consistent with this picture. Interestingly, we find that 34 per cent of galaxies with classical bulges have Dn(4000) < 1.7 (50 per cent of which hosting bars), the remainder having Dn(4000) ≥ 1.7 (with a fraction of barred galaxies of 40 per cent). Such excess of bars among star-forming classical bulges is also generally consistent with the picture of a composite bulge. In this context, it is worth noting that classical bulges with star formation lie between pseudo-bulges and classical bulges without star formation in the density plot of Fig. 8 (i.e. between the lower dashed line and the solid line), and also have intermediate masses, as mentioned above (see also Table 4). They thus bridge pseudo-bulges and classical bulges without star formation in the mass–size relation in Fig. 13. If such a picture is correct, then the Hubble classification could be understood as mainly a sequence that goes from elliptical galaxies successively to disc galaxies with classical bulges, composite bulges and pseudo-bulges.
5.3 Formation of bulges and ellipticals
The results in Section 4 all corroborate previous ideas that bulges, as identified through their photometrical properties, are present in two main classes, with distinct structural properties, indicating different formation processes. Those more similar to elliptical galaxies, namely classical bulges, seem to be formed through violent processes, such as hierarchical clustering, whereas those dissimilar bulges, namely pseudo-bulges, seem to be still under formation processes, more likely as a result of their host galaxies' slow internal evolution, which involves disc instabilities and angular momentum transfer.
These inferences are borne out by the fact that pseudo-bulges, when compared to their classical counterparts, have currently intense star formation activity (Figs 9 and 15), are less concentrated at the fixed bulge-to-total ratio (Fig. 14) and occupy the same locus in the FP as discs (Fig. 16). The bulge Sérsic index correlates with the bulge-to-total ratio for classical bulges but not for pseudo-bulges (Fig. 11). In addition, pseudo-bulges follow a mass–size relation similar to that followed by bars, and different from that followed by classical bulges (Fig. 13). Furthermore, the discs (and bars) in galaxies that host pseudo-bulges are not as different from those in galaxies that host classical bulges as pseudo-bulges are different from classical bulges, in what concerns their relative stellar masses (Section 4.5). This suggests that disc and bar formations are similar in both galaxy classes, whereas bulge formation is distinct.
However, we have also found indications that the processes that lead to the formation of classical and pseudo-bulges might happen concomitantly. In this context, the processes that lead to the formation of a pseudo-bulge are dominant at one end, while those that lead to the formation of a classical bulge are dominant at the other end, across the bulge population. This is suggested by the significant overlap in the distributions of bulges with n > 2 and n < 2 in the Kormendy relation (Fig. 8), which is in fact statistically more significant than the overlap in the distributions of ellipticals and bulges altogether, as discussed in Section 4.2. We have also found classical bulges with young stellar populations, typical of pseudo-bulges (Fig. 9). Furthermore, although classical and pseudo-bulges have significantly different slopes for their mass–size relations, such relations join smoothly with pseudo-bulges at the low-mass end, and with classical bulges at the high-mass end (Fig. 13).
Classical bulges seem to bear some structural similarity to ellipticals, since they follow the same Kormendy relation (Fig. 8), and occupy a similar locus in the edge-on view of the FP (Fig. 16). However, they also follow offset mass–size relations (Fig. 13). This could, in principle, challenge the idea that classical bulges are simply ellipticals that happen to be surrounded by a disc. It should be noted, though, that this result concerns only massive ellipticals. Low-luminosity ellipticals could, if surrounded by a disc, resemble classical bulges, but this cannot be evaluated with the present data. We have verified that accounting for systematic effects could bring some of the low-mass ellipticals closer to the relation followed by classical bulges. Our tests indicate that such systematic effects should be restricted to about 10 per cent of the ellipticals. In the worst case scenario that all ellipticals are affected by systematic effects, the offset between the mass–size relations of classical bulges and ellipticals would still be present, but restricted to high-mass systems. Thus, the result that high-mass bulges cannot be considered as high-mass ellipticals surrounded by discs seems to be robust. We note that in the face-on view of the FP (Fig. 16), pseudo-bulges, classical bulges and ellipticals occupy three significantly distinct loci, which should provide clues to the different formation and evolution processes.
6 SUMMARY AND CONCLUSIONS
We have determined several structural parameters for elliptical galaxies, bulges, discs and bars through reliable multiband image fitting of a representative sample of nearly 1000 local, massive galaxies in the SDSS. We showed that the Petrosian concentration index is a better proxy for the bulge-to-total ratio than the global Sérsic index.
We showed that, while the bulge Sérsic index can be considered as a criterion to distinguish pseudo-bulges from classical bulges, a more reliable, and physically motivated, separation can be made using the Kormendy relation. While classical bulges follow the relation set by ellipticals, pseudo-bulges do not, independently of their Sérsic index. This shows that classical bulges bear some structural similarity to elliptical galaxies, while pseudo-bulges are structurally different.
Using Dn(4000), which is insensitive to dust attenuation, we demonstrated that pseudo-bulges are currently undergoing intense star formation activity, and that virtually all pseudo-bulges are located in the blue cloud of the colour–magnitude diagram. In contrast, most (but not all) classical bulges are quiescent and populate the red sequence of the diagram. We presented evidence of different formation mechanisms for classical and pseudo-bulges. Classical bulges follow a correlation between the Sérsic index and bulge-to-total ratio, while pseudo-bulges do not. The latter are less concentrated than the former at the fixed bulge-to-total ratio. The locus occupied by pseudo-bulges in the fundamental plane is different from that of classical bulges, and it is the same as that of discs. Furthermore, pseudo-bulges follow a mass–size relation different from that of classical bulges, and similar to that of bars. Altogether, this indicates that pseudo-bulges are formed through slow, non-violent processes, such as those expected from disc instabilities, whereas classical bulges are formed through violent processes, such as the merging of smaller units. We verified, however, a significant overlap in the properties of classical and pseudo-bulges, which suggests that the different formation processes might happen concomitantly, with different processes being dominant in different cases.
We found that classical bulges and ellipticals follow offset mass–size relations, suggesting that high-mass bulges cannot be considered as high-mass ellipticals that happen to be surrounded by a disc.
We provided distributions and typical values (including uncertainties in individual measurements) of all structural parameters obtained (with the exception of bar parameters, which will be addressed in a separate paper). We calculated the stellar mass content and distribution for each galaxy component, and showed that, considering galaxies more massive than 1010 M⊙, in the local universe, 32 per cent of the total stellar mass is contained in ellipticals, and the corresponding values for discs, bulges and bars are, respectively, 36, 28 and 4 per cent. Classical bulges contain 25 per cent of the total stellar mass, while pseudo-bulges contain 3 per cent. We also provided the corresponding luminosity and number fractions. In particular, we find that approximately a third of disc galaxies hosts pseudo-bulges. Such figures should be reproduced by successful models of galaxy formation and evolution.
I am grateful to Guinevere Kauffmann for her support throughout this work and many useful discussions. Her input is greatly appreciated. It is a pleasure to thank Simone Weinmann for her help in producing Fig. 6 and useful discussions, and Jarle Brinchmann for producing the cutouts and detailed image headers of our parent sample. I have benefitted from useful and stimulating discussions with Lia Athanassoula, Eugene Churazov, Peter Erwin, David Fisher, Alister Graham, Tim Heckman, Jochen Liske, Daniele Pierini and Simon White throughout the writing of this paper. I thank an anonymous referee for comments that helped to improve the paper. DAG is supported by the Deutsche Forschungsgemeinschaft priority program 1177 (‘Witnesses of Cosmic History: Formation and Evolution of Galaxies, Black Holes and their Environment’) and the Max Planck Society. The Sloan Digital Sky Survey (SDSS) is a joint project of The University of Chicago, Fermilab, the Institute for Advanced Study, the Japan Participation Group, The Johns Hopkins University, Los Alamos National Laboratory, the Max-Planck Institute for Astronomy (MPIA), the Max-Planck Institute for Astrophysics (MPA), New Mexico State University, Princeton University, the United States Naval Observatory and the University of Washington. Apache Point Observatory, site of the SDSS telescopes, is operated by the Astrophysical Research Consortium (ARC). Funding for the project has been provided by the Alfred P. Sloan Foundation, the SDSS member institutions, the National Aeronautics and Space Administration, the National Science Foundation, the US Department of Energy, the Japanese Monbukagakusho and the Max Planck Society. The SDSS Web site is http://www.sdss.org/.
APPENDIX A: FIT SENSITIVITY TO INPUT PARAMETERS
As mentioned in Section 3, image fitting often involves finding a χ2 global minimum in a very complex multidimensional parameter space. This means that, in principle (and depending on the algorithm used), fits can be very sensitive to the initial guesses given to the fitting code to start the first iteration. To avoid erroneous results, we have opted to produce and check each fit individually. Nevertheless, this alone does not mean that we find the most appropriate set of input parameters in all cases.
In order to check how sensitive the results of our fits are to the set of initial guesses provided to budda, we have performed the following tests. We have randomly selected 20 barred galaxies, and produced test fits, in which the input values for μ0, h, μe, re and n used in the corresponding final fits are increased by a factor of 2 (for 10 of these galaxies) or decreased by a factor of 2 (for the remaining 10 galaxies). The choice for barred galaxies assures that the results from these tests concern typically difficult fits. Also note that a factor of 2 is rather large, and that 20 galaxies correspond to 7 per cent of our barred galaxies. Fig. A1 shows the results from these test fits, as compared to those from the final fits. Error bars are 1σ uncertainties estimated by budda. Its current version does not provide estimates of the uncertainty in B/T. Thus, for B/T, typical error bars are shown, calculated through error propagation using the uncertainties in μe, re and n, and assuming that the main source of error in B/T comes from determining the total bulge luminosity. Through similar tests with budda, Durbala et al. (2008) found comparable uncertainties in B/T (albeit somewhat smaller).
One sees that, in most cases, the code converges to similar results, even for input parameters varying by a factor of 4. In fact, most results are consistent within the estimated uncertainties. All outliers come from the few fits that resulted in notably high χ2 values. Furthermore, these results reinforce the findings in Gadotti (2008) by indicating that disc parameters are particularly robust, and that B/T is a more robust parameter than n, which can have large uncertainties compared to its dynamical range. These results also argue in favour of our method to identify pseudo-bulges, at least for statistical studies such as ours, since μe and re are also more stable than n.
These results do not mean that any reasonable set of input parameters is appropriate. But they show that, by creating input parameters through a careful inspection of each galaxy individually, we are able to achieve robust results. In fact, as noted above, wrong fits often result in significantly higher χ2 values (see leftmost panel in Fig. A1), turning them, generally, easy to recognize in our procedure. Only 2.5 per cent of our final fits have χ2 > 2.
Table 1. Structural parameters of bulges, discs and bars in our sample from i-band image fits. Galaxy identifications, uncertainties and similar tables in the g and r bands are also available.
Table 2. Absolute magnitudes and integrated colours of bulges, discs and bars in our sample from the BUDDA models.
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