Peanut-shaped Bulges Research Articles

Disk origin of the Milky Way bulge: the necessity of the thick disk

In the Milky Way bulge, metal-rich stars form a strong bar and are more peanut-shaped than metal-poor stars. It has recently been claimed that this behavior is driven by the initial (i.e., before bar formation) in-plane radial velocity dispersion of these populations, rather than by their initial vertical random motions. This has led to the suggestion that a thick disk is not necessary to explain the characteristics of the Milky Way bulge. We discuss this issue again by analyzing two dissipationless N-body simulations of boxy or peanut-shaped bulges formed from composite stellar disks that consist of kinematically cold and hot stellar populations. These two models represent two extreme cases: one where all three components of the disk have a fixed vertical velocity dispersion and different in-plane radial dispersion, and another where they all have a fixed radial dispersion and different vertical random motions (thickness). This is intended to quantify the drivers of the main features that are observed in composite boxy or peanut-shaped bulges and their origin. We quantify the mapping into a boxy or peanut-shaped bulge of disk populations in these two cases, and we conclude that initial vertical random motions are as important as in-plane random motions in determining the relative contribution of cold- and hot-disk populations with height above the plane, the metallicity and age trends. Previous statements emphasizing the dominant role of in-plane motions in determining these trends are not confirmed. However, significant differences exist in the morphology and strength of the resulting boxy or peanut-shaped bulges. In particular, the model where disk populations initially have only different in-plane random motions, but similar thickness, results in a boxy or peanut-shaped bulge where all populations have a similar peanut shape, independent of their initial kinematics or metallicity. This is at odds with the trends observed in the Milky Way bulge. We discuss the reasons behind these differences, and also predict the signatures that these two extreme initial conditions would leave on the vertical age and metallicity gradients of disk stars outside the bulge region. As a consequence of this analysis, we conclude that given our current knowledge of the Milky Way bulge and of the properties of its main stellar components, a metal-poor, kinematically (radial and vertical) hot component, that is, a thick disk, is necessary in the Milky Way before bar formation. This supports the scenario that has been traced in previous works. Boxy or peanut-shaped bulges and their surrounding regions are fossil records of the conditions present at early times in disk galaxies, and by dissecting their stellar components by chemical compositions and/or age, it may be possible to reconstruct their early state.

The frequency and stellar-mass dependence of boxy/peanut-shaped bulges in barred galaxies

From a sample of 84 local barred, moderately inclined disc galaxies, we determine the fraction which host boxy or peanut-shaped (B/P) bulges (the vertically thickened inner parts of bars). We find that the frequency of B/P bulges in barred galaxies is a very strong function of stellar mass: 79% of the bars in galaxies with log (M_{star}/M_{sun}) >~ 10.4 have B/P bulges, while only 12% of those in lower-mass galaxies do. (We find a similar dependence in data published by Yoshino & Yamauchi 2015 for edge-on galaxies.) There are also strong trends with other galaxy parameters -- e.g., Hubble type: 77% of S0-Sbc bars, but only 15% of Sc-Sd bars, have B/P bulges -- but these appear to be side effects of the correlations of these parameters with stellar mass. In particular, despite indications from models that a high gas content can suppress bar buckling, we find no evidence that the (atomic) gas mass ratio M_{atomic}/M_{star} affects the presence of B/P bulges, once the stellar-mass dependence is controlled for. The semi-major axes of B/P bulges range from one-quarter to three-quarters of the full bar size, with a mean of R_{box}/L_{bar} = 0.42 +/- 0.09 and R_{box}/a_{max} = 0.53 +/- 0.12 (where R_{box} is the size of the B/P bulge and a_{max} and L_{bar} are lower and upper limits on the size of the bar).

Quantifying the (X/peanut)-shaped structure in edge-on disc galaxies: length, strength, and nested peanuts

X-shaped or peanut-shaped (X/P) bulges are observed in more than 40% of (nearly) edge-on disc galaxies, though to date a robust method to quantify them is lacking. Using Fourier harmonics to describe the deviation of galaxy isophotes from ellipses, we demonstrate with a sample of 11 such galaxies (including NGC 128) that the sixth Fourier component ($B_6$) carries physical meaning by tracing this X/P structure. We introduce five quantitative diagnostics based on the radial $B_6$ profile, namely: its `peak' amplitude ($\Pi_{\rm max}$); the (projected major-axis) `length' where this peak occurs ($R_{\Pi,max}$); its vertical `height' above the disc plane ($z_{\Pi,max}$); the $B_6$ profile's integrated `strength' ($S_{\Pi}$); and the $B_6$ peak `width' ($W_{\Pi}$). We also introduce different `classes' of $B_6$ profile shape. Furthermore, we convincingly detect and measure the properties of multiple (nested) X/P structures in individual galaxies which additionally display the signatures of multiple bars in their surface brightness profiles, thus consolidating further the scenario in which peanuts are associated with bars. We reveal that the peanut parameter space (`length', `strength' and `height') for real galaxies is not randomly populated, but the 3 metrics are inter-correlated (both in kpc and disc scale-length $h$). Additionally, the X/P `length' and `strength' appear to correlate with $v_{rot}/\sigma_*$, lending further support to the notion that peanuts `know' about the galactic disc in which they reside. Such constraints are important for simulations, as they provide a direct link between peanuts and their host disc. Our diagnostics reveal a spectrum of X/P properties and could provide a means of distinguishing between different peanut formation scenarios. Moreover, nested peanuts, as remnants of bar buckling events, can provide insights into the disc and bar instability history.

3D kinematics through the X-shaped Milky Way bulge

It has recently been discovered that the Galactic bulge is X-shaped, with the two southern arms of the X both crossing the lines of sight at l=0 and |b|>4, hence producing a double red clump (RC) in the bulge CMD. Dynamical models predict the formation of X-shaped bulges, as extreme cases of boxy-peanut bulges. However, since X-shaped bulges were known to be present only in external galaxies, models have never been compared to 3D kinematical data for individual stars. We study the orbital motion of Galactic bulge stars, in the two arms of the X in the southern hemisphere. The goal is to provide observational constraints to bulge formation models that predict the formation of X-shapes through bar dynamical instabilities. Radial velocities have been obtained for a sample of 454 bulge giants, roughly equally distributed between the bright and faint RC, in a field at (l,b)=(0,-6). Proper motions were derived for all RC stars in the same field by combining images from two epochs obtained 11 years apart. The proper motions for the spectroscopic subsample are analyzed taking into account the radial velocities and metallicities measured from near-IR Calcium triplet lines, for a subsample of 352 stars. The radial velocity distribution of stars in the bright RC, tracing the closer overdensity of bulge stars, shows an excess of stars moving towards the Sun. Similarly, an excess of stars receding from the Sun is seen in the far overdensity, traced by faint RC stars. This is explained with the presence of stars on elongated orbits, most likely streaming along the arms of the X-shaped bulge. Proper motions for these stars are consistent with qualitative predictions of dynamical models of peanut-shaped bulges. Surprisingly, stars on elongated orbits have preferentially metal poor metallicities, while the metal rich ones, in both overdensities, are preferentially found in more axysimmetric orbits.

Overview of dynamical mechanisms of secular evolution

AbstractGravity-bound isolated systems, from stars, planetary systems, star clusters to galaxies, share common properties where evolution is the rule. Typically if they start forming at a well defined epoch they tend to change significantly over a timescale comparable to their present age. So evolution is never truly stopped, it just proceeds slower and slower: after a rapid, violent phase a slower, secular phase follows. In galactic astronomy for many decades the paradigm was rather that after a short violent time galaxies would settle in a stable steady state just consuming gas into stars. Actually today it appears that the progressive appearance of galaxy systematic morphologies and the slowing pace of mergers indicate that common intrinsic dynamical factors continue to shape galaxies towards similar properties irrespective of their largely different formation histories and initial conditions. Newtonian physics supplemented by a weakly dissipative component provides an amazing amount of explanations for the galaxy properties, like exponential stellar disks, spirals, bars, and peanut-shaped bulges. The purpose of this talk is to review these mechanisms of dynamical secular evolution.

The stellar kinematics and populations of boxy bulges: cylindrical rotation and vertical gradients★

Boxy and peanut-shaped bulges are seen in about half of edge-on disc galaxies. Comparisons of the photometry and major-axis gas and stellar kinematics of these bulges to simulations of bar formation and evolution indicate that they are bars viewed in projection. If the properties of boxy bulges can be entirely explained by assuming that they are bars, then this may imply that their hosts are pure disc galaxies with no classical bulge. A handful of these bulges, including that of the Milky Way, have been observed to rotate cylindrically, i.e. with a mean stellar velocity independent of height above the disc. In order to assess whether such behaviour is ubiquitous in boxy bulges, and whether a pure disc interpretation is consistent with their stellar populations, we have analysed the stellar kinematics and populations of the boxy or peanut-shaped bulges in a sample of five edge-on galaxies. We placed slits along the major axis of each galaxy and at three offset but parallel positions to build up spatial coverage. The boxy bulge of NGC 3390 rotates perfectly cylindrically within the spatial extent and uncertainties of the data. This is consistent with the metallicity and α-element enhancement of the bulge, which are the same as in the disc. This galaxy is thus a pure disc galaxy. The boxy bulge of ESO 311−G012 also rotates very close to cylindrically. The boxy bulge of NGC 1381 is neither clearly cylindrically nor non-cylindrically rotating, but it has a negative vertical metallicity gradient and is α-enhanced with respect to its disc, suggesting a composite bulge comprised of a classical bulge and bar (and possibly a discy pseudo-bulge). The rotation of the peanut-shaped bulge of NGC 5746 is difficult to classify, but the peanut-shaped bulge of IC 4767 does not rotate cylindrically. Thus, even this relatively small sample is sufficient to demonstrate that boxy bulges display a range of rotational and population properties, indicating that they do not form a homogeneous class of object.

OBSERVABLE PROPERTIES OF DOUBLE-BARRED GALAXIES INN-BODY SIMULATIONS

Although at least one quarter of early-type barred galaxies host secondary stellar bars embedded in their large-scale primary counterparts, the dynamics of such double-barred galaxies are still not well understood. Recently we reported success at simulating such systems in a repeatable way in collisionless systems. In order to further our understanding of double-barred galaxies, here we characterize the density and kinematics of the N-body simulations of these galaxies. This will facilitate comparison with observations and lead to a better understanding of the observed double-barred galaxies. We find the shape and size of our simulated secondary bars are quite reasonable compared to the observed ones. We demonstrate that an authentic decoupled secondary bar may produce only a weak twist of the kinematic minor axis in the stellar velocity field, due to the relatively large random motion of stars in the central region. We also find that the edge-on nuclear bars are probably not related to boxy peanut-shaped bulges which are most likely to be edge-on primary large-scale bars. Another kinematic feature often present in our double-barred models is a ring-like feature in the fourth-order Gauss-Hermite moment h4 maps. Finally, we demonstrate that the non-rigid rotation of the secondary bar causes its pattern speed to not be derived with great accuracy using the Tremaine-Weinberg method. We also compare with observations of NGC 2950, a prototypical double-barred early-type galaxy, which suggest that the nuclear bar may be rotating in the opposite sense as the primary.

Gas Feedback on Stellar Bar Evolution

We analyze evolution of live disk-halo systems in the presence of various gas fractions, f_gas less than 8% in the disk. We addressed the issue of angular momentum (J) transfer from the gas to the bar and its effect on the bar evolution. We find that the weakening of the bar, reported in the literature, is not related to the J-exchange with the gas, but is caused by the vertical buckling instability in the gas-poor disks and by a steep heating of a stellar velocity dispersion by the central mass concentration (CMC) in the gas-rich disks. The gas has a profound effect on the onset of the buckling -- larger f_gas brings it forth due to the more massive CMCs. The former process leads to the well-known formation of the peanut-shaped bulges, while the latter results in the formation of progressively more elliptical bulges, for larger f_gas. The subsequent (secular) evolution of the bar differs -- the gas-poor models exhibit a growing bar while gas-rich models show a declining bar whose vertical swelling is driven by a secular resonance heating. The border line between the gas-poor and -rich models lies at f_gas ~ 3% in our models, but is model-dependent and will be affected by additional processes, like star formation and feedback from stellar evolution. The overall effect of the gas on the evolution of the bar is not in a direct J transfer to the stars, but in the loss of J by the gas and its influx to the center that increases the CMC. The more massive CMC damps the vertical buckling instability and depopulates orbits responsible for the appearance of peanut-shaped bulges. The action of resonant and non-resonant processes in gas-poor and gas-rich disks leads to a converging evolution in the vertical extent of the bar and its stellar dispersion velocities, and to a diverging evolution in the bulge properties.

The Kinematic Signature of Face‐on Peanut‐shaped Bulges

We present a kinematic diagnostic for peanut-shaped bulges in nearly face-on galaxies. The face-on view provides a novel perspective on peanuts that would allow study of their relation to bars and disks in greater detail than hitherto possible. The diagnostic is based on the fact that peanut shapes are associated with a flat density distribution in the vertical direction. We show that the kinematic signature corresponding to such a distribution is a minimum in the fourth-order Gauss-Hermite moment s4. We demonstrate our method on N-body simulations of varying peanut strength, showing that strong peanuts can be recognized to inclinations i 30°, regardless of the strength of the bar. We also consider compound systems in which a bulge is present in the initial conditions, as may happen if bulges form at high redshift through mergers. We show that in this case, because the vertical structure of the bulge is not derived from that of the disk, the signature of a peanut in s4 is weakened. Thus the same kinematic signature of peanuts can be used to explore bulge formation mechanisms. The observational requirements for identifying peanuts with this method are challenging, but feasible.

Structure and kinematics of edge-on galaxy discs - V. The dynamics of stellar discs

In earlier papers in this series we determined the intrinsic stellar disc kinematics of 15 intermediate- to late-type edge-on spiral galaxies using a dynamical modelling technique. The sample covers a substantial range in maximum rotation velocity and deprojected face-on surface brightness, and contains seven spirals with either a boxy or peanut-shaped bulge. Here we discuss the structural, kinematical and dynamical properties. From the photometry we find that intrinsically more flattened discs tend to have a lower face-on central surface brightness and a larger dynamical mass-to-light ratio. This observation suggests that, at a constant maximum rotational velocity, lower surface brightness discs have smaller vertical stellar velocity dispersions. Although the individual uncertainties are large, we find from the dynamical modelling that at least 12 discs are submaximal. The average disc contributes 53 ± 4 per cent to the observed rotation at 2.2 disc scalelengths (hR), with a 1σ scatter of 15 per cent. This percentage becomes somewhat lower when effects of finite disc flattening and gravity by the dark halo and the gas are taken into account. Since boxy and peanut-shaped bulges are probably associated with bars, the result suggests that at 2.2hR the submaximal nature of discs is independent of barredness. The possibility remains that very high surface brightness discs are maximal, as these discs are underrepresented in our sample. We confirm that the radial stellar disc velocity dispersion is related to the galaxy maximum rotational velocity. The scatter in this σ versus vmax relation appears to correlate with the disc flattening, face-on central surface brightness and dynamical mass-to-light ratio. Low surface brightness discs tend to be more flattened and have smaller stellar velocity dispersions. The findings are consistent with the observed correlation between disc flattening and dynamical mass-to-light ratio and can generally be reproduced by the simple collapse theory for disc galaxy formation. Finally, the disc mass Tully–Fisher relation is offset from the maximum-disc scaled stellar mass Tully–Fisher relation of the Ursa Major cluster. This offset, −0.3 dex in mass, is naturally explained if the discs of the Ursa Major cluster spirals are submaximal.

Bar Diagnostics in Edge‐On Spiral Galaxies. III.N‐Body Simulations of Disks

Present in over 45% of local spirals, boxy and peanut-shaped bulges are generally interpreted as edge-on bars and may represent a key phase in the evolution of bulges. Aiming to test such claims, the kinematic properties of self-consistent 3D N-body simulations of bar-unstable disks are studied. Using Gauss-Hermite polynomials to describe the stellar kinematics, a number of characteristic bar signatures are identified in edge-on disks: 1) a major-axis light profile with a quasi-exponential central peak and a plateau at moderate radii (Freeman Type II profile); 2) a ``double-hump'' rotation curve; 3) a sometime flat central velocity dispersion peak with a plateau at moderate radii and occasional local central minimum and secondary peak; 4) an h3-V correlation over the projected bar length. All those kinematic features are spatially correlated and can easily be understood from the orbital structure of barred disks. They thus provide a reliable and easy-to-use tool to identify edge-on bars. Interestingly, they are all produced without dissipation and are increasingly realized to be common in spirals, lending support to bar-driven evolution scenarios for bulge formation. So called ``figure-of-eight'' position-velocity diagrams are never observed, as expected for realistic orbital configurations. Although not uniquely related to triaxiality, line-of-sight velocity distributions with a high velocity tail (i.e. an h3-V correlation) appear as particularly promising tracers of bars. The stellar kinematic features identified grow in strength as the bar evolves and vary little for small inclination variations. Many can be used to trace the bar length. Comparisons with observations are encouraging and support the view that boxy and peanut-shaped bulges are simply thick bars viewed edge-on.

Box- and peanut-shaped bulges

Box- and peanut-shaped bulges

Box- and peanut-shaped bulges

We present a classification for bulges of a complete sample of ~ 1350 edge-on disk galaxies derived from the RC3 ( Third Reference Catalogue of Bright Galaxies , de Vaucouleurs et al. 1991). A visual classification of the bulges using the Digitized Sky Survey (DSS) in three types of b/p bulges or as an elliptical type is presented and supported by CCD images. NIR observations reveal that dust extinction does almost not influence the shape of bulges. There is no substantial difference between the shape of bulges in the optical and in the NIR. Our analysis reveals that 45% of all bulges are box- and peanut-shaped (b/p). The frequency of b/p bulges for all morphological types from S0 to Sd is > 40%. In particular, this is for the first time that such a large frequency of b/p bulges is reported for galaxies as late as Sd. The fraction of the observed b/p bulges is large enough to explain the b/p bulges by bars.

Buckling Bars and Boxy Bulges

AbstractIt has been suggested that the peanut-shaped bulges seen in some edge-on disk galaxies are produced when bars in these galaxies buckle. This paper reviews the modelling which seeks to show how bars buckle, and I present a very simple new model which captures the essential physics of this process. I then discuss the problems in establishing observationally the connection between peanut-shaped bulges and bars. Confirmation of the link has proved difficult because boxy bulges are only apparent in edge-on galaxies whereas bars are only easily detectable in more face-on systems. Finally, I present a new technique which avoids this difficulty by searching for the distinctive kinematic signature of an edgeon bar; application of this method to spectra of peanut-shaped bulges reveals that they are, indeed, associated with hidden bars.

Establishing the connection between peanut-shaped bulges and galactic bars

It has been suggested that the peanut-shaped bulges seen in some edge-on disk galaxies are due to the presence of a central bar. Although bars cannot be detected photometrically in edge-on galaxies, we show that barred potentials produce a strong kinematic signature in the form of double-peaked line-of-sight velocity distributions with a characteristic ``figure-of-eight'' variation with radius. We have obtained spectroscopic observations of two edge-on galaxies with peanut-shaped bulges (NGC~5746 and NGC~5965), and they reveal exactly such line-of-sight velocity distributions in both their gaseous (emission line) and their stellar (absorption line) components. These observations provide strong observational evidence that peanut-shaped bulges are a by-product of bar formation.

IC 4767 (the 'X-galaxy') - The missing link for understanding galaxies with peanut-shaped bulges?

view Abstract Citations (80) References (22) Co-Reads Similar Papers Volume Content Graphics Metrics Export Citation NASA/ADS IC 4767 (the ``X-Galaxy''): The Missing Link for Understanding Galaxies with Peanut-shaped Bulges? Whitmore, Bradley C. ; Bell, Marylin Abstract Photometric and kinematic observations of the peculiar S0 galaxy IC 4767 (= ESO 104-G10, DC 1842-63 number 12, WR 115, "X-galaxy") are presented. At various intensities the bulge of this galaxy looks like a normal spheroidal system with elliptical isophotes, a well-defined rectangle, and a peanut-shaped or X-shaped structure with components aligned at oblique angles to the major axis. The B-V image reveals the presence of a thin inner dust lane nearly aligned with the major axis. This inner disk probably resulted from the dissipation of gas during a recent accretion event, as indicated by the presence of gas in rapid rotation which is only observed within 2" of the nucleus. The outer regions of the X-component are also rotating quite rapidly, indicating that the stars are in relatively circular orbits, consistent with a rotation field which is approximately cylindrical with respect to the disk. IC 4767 shows characteristics of both peanut-shaped galaxies and polar-ring galaxies, leading us to suggest similar origins for the two systems. In both cases we believe the accretion of material from a companion galaxy during a merger or tidal encounter causes the peculiar morphology. If the accreted material impacts the central galaxy at nearly a right angle to the disk, a polar-ring galaxy is produced. If the accreted material impacts the central galaxy at an oblique angle, a galaxy with a box-shaped or peanut-shaped nucleus may be produced. Further evidence to support the accretion hypothesis is the fact that the five most prominent peanut-shaped galaxies all have nearby companions within a few radii, many of the companions showing deformities or even luminous bridges with the peanut galaxies. Publication: The Astrophysical Journal Pub Date: January 1988 DOI: 10.1086/165933 Bibcode: 1988ApJ...324..741W Keywords: Elliptical Galaxies; Galactic Bulge; Galactic Structure; Interstellar Matter; Peculiar Galaxies; Seyfert Galaxies; Astronomical Photometry; Astronomical Spectroscopy; Galactic Nuclei; Isophotes; Ring Galaxies; Astrophysics; GALAXIES: INDIVIDUAL ALPHANUMERIC: IC 4767; GALAXIES: INTERNAL MOTIONS; GALAXIES: PHOTOMETRY; GALAXIES: STRUCTURE full text sources ADS | data products SIMBAD (11) NED (10)

The unusual box-shaped elliptical (?) galaxy IC 3370

view Abstract Citations (29) References (46) Co-Reads Similar Papers Volume Content Graphics Metrics Export Citation NASA/ADS The Unusual Box-Shaped (?) Elliptical Galaxy IC 3370 Jarvis, Brian Abstract IC 3370 is noted by this photometric and kinematic study to be more like the bulges of disk galaxies than elliptical galaxies; seen nearly edge-on, it is an S0pec rather than an elliptical galaxy, as originally classified. IC 3370 is also found to be a cylindrical rotator above the plane of the disk to a degree that is far in excess of previous observations in box- or peanut-shaped bulges. In addition, it exhibits a large amount of isophotal twisting throughout the bulge, which is not easily reconciled with an oblate model's nearly edge-on view, but is suggestive of a merger or tidal-encounter history. Publication: The Astronomical Journal Pub Date: July 1987 DOI: 10.1086/114444 Bibcode: 1987AJ.....94...30J Keywords: Astronomical Photometry; Elliptical Galaxies; Galactic Rotation; Galactic Structure; Disk Galaxies; Luminosity; Spectrum Analysis; Astrophysics; GALAXIES: GENERAL full text sources ADS | data products SIMBAD (13) NED (12)

A search for box- or peanut-shaped bulges

view Abstract Citations (85) References (18) Co-Reads Similar Papers Volume Content Graphics Metrics Export Citation NASA/ADS A search for box- and peanut-shaped bulges. Jarvis, B. J. Abstract A search for disk galaxies with box- or peanut-shaped bulges from the ESO/SERC J sky survey south of declination -18 deg has revealed 30 such galaxies. Adding to these 11 other galaxies already known to have a similar morphology yields a bimodal frequency distribution with Hubble type: there is a strong tendency for box- and peanut-shaped bulges to occur in S0 and Sab to Sb type galaxies. Furthermore, the disk-to-bulge luminosity ratios of the S0 galaxies are similar to the spiral galaxies that have box- and peanut-shaped bulges, i.e., Sab and Sb Hubble types. Of the total sample of 41 galaxies, 54 percent are possible members of clusters and 63 percent have peanut-shaped bulges, compared to box-shaped bulges. Galaxy counts show that about 1.2 percent of all disk galaxies have box- or peanut-shaped bulges. Publication: The Astronomical Journal Pub Date: January 1986 DOI: 10.1086/113980 Bibcode: 1986AJ.....91...65J Keywords: Disk Galaxies; Galactic Structure; Distribution Functions; Galactic Clusters; Irregular Galaxies; Luminosity; Sky Surveys (Astronomy); Spiral Galaxies; Astronomy full text sources ADS | data products NED (44) SIMBAD (41)