Clash of the Trident and Tuning Fork: insights from bar and spiral strength in the (massive black hole)-stellar mass diagrams, and the `Triangal' galaxy evolution schema
Pith reviewed 2026-05-08 02:52 UTC · model grok-4.3
The pith
Bar strength does not mark distinct evolutionary paths in black hole-stellar mass diagrams, while S0 galaxies form through three separate channels.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Galaxies with varying bar strengths and double bars do not occupy preferred locations in the M_bh-M_star diagrams, demonstrating that bars are products of secular evolution that can be transient or recurrent and track neither hierarchical mass assembly nor galaxy speciation. In contrast, three physically distinct formation channels for S0/a galaxies are identified: primeval S0-to-S transitions, faded spiral galaxies, and wet-major-merger-built dust-rich S0 galaxies on the green mountain. A dust attrition/retention sequence and disc down-sizing sequence are also revealed.
What carries the argument
The Triangal galaxy evolution schema, which establishes an integrated growth reference frame by placing galaxies in the massive black hole to spheroid and total stellar mass diagrams to evaluate bar-to-total luminosity ratio and spiral strength indicators.
If this is right
- Bars result from secular evolution and can be transient or recurrent without marking fixed stages of hierarchical assembly.
- S0/a galaxies form through at least three physically distinct channels rather than a single path.
- Particularly strong spirals appear on the right-hand side of the spiral galaxy distribution.
- A dust attrition/retention sequence connects dust-poor S0 galaxies to dust-rich ones via systems with dusty nuclear discs.
- Disc down-sizing bridges ES,e galaxies with intermediate-scale discs to dust-poor pure E galaxies via damp mergers.
Where Pith is reading between the lines
- Galaxy evolution models should treat bars as temporary internal features rather than permanent classifiers of type or stage.
- Detailed morphological data may help reduce systematic errors in cosmological analyses that group galaxies by broad type only.
- Targeted observations of merger signatures in dust-rich S0 galaxies could further test the wet-merger channel.
Load-bearing premise
Multi-component decompositions yield accurate spheroid and total stellar masses such that placements in the black hole-stellar mass diagrams directly reveal distinct evolutionary channels without dominant selection or measurement biases.
What would settle it
Finding that strong-bar galaxies cluster preferentially in diagram regions tied to one S0 formation channel, or that the three S0 channels fail to separate with a larger sample of precise decompositions, would challenge the central claims.
Figures
read the original abstract
The `Triangal' galaxy evolution schema is used to assess whether the Tuning Fork (bar strength) or the van~den~Bergh Trident and ATLAS$^{3D}$ Comb (spiral strength) offer greater evolutionary insight. A new catalogue of quantitative bar strengths (measured by the bar-to-total luminosity ratio, $P$), refined galaxy morphologies, and dust bin classifications is presented. It contains 137 galaxies with spheroid stellar masses, obtained from multi-component decompositions, and directly measured black hole masses, $M_{\rm bh}$. By placing these galaxies within the $M_{\rm bh}$-($M_{\rm\star,sph}$, $M_{\rm\star,gal}$) parameter space, an evolutionary reference frame reflecting integrated growth is established. Galaxies with varying bar strengths, and double bars, are observed to not occupy preferred locations, highlighting that bars are products of secular evolution-and can be transient or recurrent phenomena-and that they track neither hierarchical mass assembly nor galaxy speciation. In contrast, three physically distinct formation channels for S0/a galaxies are identified: (primeval S0)-to-S transitions; faded spiral galaxies; and, most commonly, wet-major-merger-built dust-rich S0 galaxies (on the `green mountain'). Galaxies with particularly strong spirals appear on the right-hand side of the spiral galaxy distribution. Furthermore, a `Dust Attrition/Retention' sequence places S0 (and compact massive ES,b) galaxies with dusty nuclear discs between the dust-poor and dust-rich S0 galaxies, and a `Disc Down-sizing' sequence is revealed, in which E galaxies with dusty nuclear discs-potentially formed through `damp' mergers-bridge the ES,e (ellicular) galaxies with intermediate-scale stellar discs and the dust-poor pure E galaxies. Extensive historical context is provided, and, finally, suspected biases in precision cosmology stemming from neglected precision galaxy morphology are discussed.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript introduces the 'Triangal' galaxy evolution schema as a reference frame in the M_bh-(M_star,sph, M_star,gal) diagrams and applies it to a new catalogue of 137 galaxies with directly measured black hole masses and multi-component decompositions. It concludes that galaxies with varying bar strengths (including double bars) show no preferred locations, implying bars are secular, transient or recurrent products unrelated to hierarchical mass assembly; in contrast, S0/a galaxies occupy three distinct formation channels (primeval S0-to-S transitions, faded spirals, and wet-major-merger dust-rich S0s on the 'green mountain'), with additional 'Dust Attrition/Retention' and 'Disc Down-sizing' sequences identified for S0 and E galaxies.
Significance. If the multi-component mass decompositions prove robust and the Triangal schema is shown to be independently derived, the work would strengthen the distinction between secular bar-driven evolution and merger-driven channels, providing a useful interpretive framework for morphological surveys and highlighting potential biases in precision cosmology from neglected morphology. The new quantitative catalogue of bar strengths (P), refined morphologies, and dust classifications is a concrete contribution that could be reused by the community.
major comments (3)
- [Catalogue description and methods] The central claims—that bar strengths lack preferred locations and that three distinct S0/a channels are identifiable—rest on the reliability of the spheroid and total stellar masses from multi-component decompositions. No error budgets, degeneracy tests (e.g., bar-bulge-disc trade-offs in strong-bar systems), or quantitative validation against independent mass estimates are supplied in the catalogue description or methods; this directly affects the mass ratios used to define the 'green mountain' and other channels.
- [Introduction of Triangal schema and results interpretation] The Triangal schema is introduced as an evolutionary reference frame reflecting integrated growth and is then used to interpret the observed placements and channel identifications in the same M_bh-M_star diagrams. It is not demonstrated that the schema was constructed independently of the 137-galaxy distributions (e.g., via a separate theoretical or simulation-based derivation), creating a circularity risk for the claimed physical distinctness of the three S0/a channels.
- [Sample selection and catalogue] The sample is restricted to systems with direct M_bh measurements, which preferentially selects massive, bulge-dominated, nearby galaxies. No quantitative assessment of selection biases or completeness corrections is provided, yet the conclusions about bar transience and the generality of the S0/a channels are stated without qualification.
minor comments (2)
- [Historical context] The historical context section is extensive and useful but could be shortened or moved to an appendix to improve focus on the new results.
- [Figures] Figure captions for the M_bh-M_star diagrams should explicitly state the symbol coding for bar strength, dust bins, and morphological types to aid readability.
Simulated Author's Rebuttal
We thank the referee for their constructive and detailed comments, which have prompted us to strengthen several aspects of the manuscript. We address each major comment point by point below, outlining the revisions we will implement.
read point-by-point responses
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Referee: [Catalogue description and methods] The central claims—that bar strengths lack preferred locations and that three distinct S0/a channels are identifiable—rest on the reliability of the spheroid and total stellar masses from multi-component decompositions. No error budgets, degeneracy tests (e.g., bar-bulge-disc trade-offs in strong-bar systems), or quantitative validation against independent mass estimates are supplied in the catalogue description or methods; this directly affects the mass ratios used to define the 'green mountain' and other channels.
Authors: We agree that the manuscript would benefit from a more explicit treatment of uncertainties in the multi-component decompositions. In the revised version, we will add a dedicated subsection to the methods and catalogue description that provides an error budget for the spheroid and total stellar masses, discusses potential degeneracies including bar-bulge-disc trade-offs in strong-bar systems, and includes quantitative comparisons with independent mass estimates from the literature for a subset of the sample. These additions will directly support the robustness of the mass ratios and channel identifications. revision: yes
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Referee: [Introduction of Triangal schema and results interpretation] The Triangal schema is introduced as an evolutionary reference frame reflecting integrated growth and is then used to interpret the observed placements and channel identifications in the same M_bh-M_star diagrams. It is not demonstrated that the schema was constructed independently of the 137-galaxy distributions (e.g., via a separate theoretical or simulation-based derivation), creating a circularity risk for the claimed physical distinctness of the three S0/a channels.
Authors: The Triangal schema is motivated by established principles of integrated galaxy growth drawn from the broader literature on hierarchical assembly, secular evolution, and morphological transformation, rather than being empirically fitted to the current 137-galaxy sample. We will revise the introduction to explicitly separate the schema's independent theoretical and observational foundations (citing prior works on black hole-stellar mass relations and merger vs. secular channels) from its subsequent application to the data. This clarification will reduce any appearance of circularity while preserving the framework's utility for interpreting the observed distributions. revision: yes
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Referee: [Sample selection and catalogue] The sample is restricted to systems with direct M_bh measurements, which preferentially selects massive, bulge-dominated, nearby galaxies. No quantitative assessment of selection biases or completeness corrections is provided, yet the conclusions about bar transience and the generality of the S0/a channels are stated without qualification.
Authors: We acknowledge that the requirement for direct black hole mass measurements introduces selection biases toward massive, bulge-dominated, and nearby systems. In the revised manuscript, we will add a new subsection on sample selection that quantifies these biases (e.g., in mass and redshift distributions) to the extent possible with available data and explicitly qualifies the conclusions as applying to this specific population. We will also note the limitations for broader generality and suggest how future samples could enable completeness corrections. revision: yes
Circularity Check
No significant circularity; observational data placements drive conclusions independently
full rationale
The paper's core derivation proceeds from independent inputs: multi-component decompositions yielding M_star,sph, M_star,gal and bar-to-total ratio P for 137 galaxies with measured M_bh. These are placed in the M_bh-(M_star,sph, M_star,gal) diagrams to observe distributions of bar and spiral strengths. Conclusions that bars show no preferred locations (hence secular/transient) and that S0/a galaxies occupy three channels follow directly from those observed positions. The Triangal schema is an interpretive label for the evolutionary reference frame constructed from the same placements, not a prior assumption or fitted construct that forces the result by definition. No self-citation chain, ansatz smuggling, or renaming of a known result reduces the central claims to tautology. The derivation remains self-contained against the catalogue measurements.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Stellar masses obtained from multi-component photometric decompositions accurately represent spheroid and total galaxy stellar masses.
- domain assumption Directly measured black hole masses are reliable and comparable across the sample.
invented entities (3)
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Triangal galaxy evolution schema
no independent evidence
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Dust Attrition/Retention sequence
no independent evidence
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Disc Down-sizing sequence
no independent evidence
Reference graph
Works this paper leans on
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and suc- cessors (Perrine 1904; Curtis
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This vast population necessitated new classification frameworks (e.g., Wolf 1908; Knox-Shaw 1915; Pease 1917; Curtis
revealed a sheer abundance of spiral nebulae (Roberts 1895, 1899), estimating that hundreds of thousands to one million existed. This vast population necessitated new classification frameworks (e.g., Wolf 1908; Knox-Shaw 1915; Pease 1917; Curtis
1908
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to supersede the designation systems of the Herschel family (as described by Curtis 1933, see p.919) and Dreyer (1888, 1895). Building on Jeans (1919), Reynolds (1920) developed what was essentially an E–S0/a–Sa–Sb–Sc–(R)S–Irr sequence represent- ing stages of nebular concentration.29 Central concentration, bulge prominence, spiral arm development, the pr...
1933
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[6]
A Cycle of Celestial Objects
and partly embracing the evolutionary scenario of Jeans (1919) 33, Hubble (1926) introduced the ‘early-type’ and ‘late-type’ terminology (borrowed from stellar classification). 34 Importantly, much of the terminology used in these classification schemes predates their formalisation. Terms such as ‘elliptical’, ‘spiral’, and ‘lenticular’ were already in us...
1919
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[7]
were sometimes thought to condense into planets, forming solar systems. 33 To give fuller credit, Jeans (1919) had embraced the modified nebular hypothesis that was still discussed by many in regard to solar system forma- tion (e.g., Tisserand 1896; Chamberlin 1901, 1916; Moulton 1905; Aitken 1906, pp. 118–119; MacPherson 1909). 34 Stars were referred to ...
1919
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[8]
2018; Stone et al
or at least attributed to Hubble (e.g., Price et al. 2018; Stone et al. 2021), despite Hubble (1930)reproducingReynolds’ model without accreditation. It seems fair to say that John Henry Reynolds (1874–1949: Johnson 1950; Knox-Shaw
2018
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[9]
Indeed, Reynolds’ contribution extended to the very hardware that shaped these classification systems
deserves more recognition for his contri- butions to astronomy in general, and galaxy morphology specifically, than he receives. Indeed, Reynolds’ contribution extended to the very hardware that shaped these classification systems. He financed the 30-inch telescope at Helwan Observatory (Egypt), used by Knox-Shaw (1915) to identify what may have been the ...
1915
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[10]
1964, 1991)
to Mount Stromlo Observatory (Australia), where it became the primary instrument used by the de Vaucouleurs in the 1950s to refine their ideas about galaxy classifications discussed herein (e.g., de Vaucouleurs 1959; de Vaucouleurs et al. 1964, 1991). The Reynolds telescope was the largest optical reflector in the Southern Hemisphere until the 1950 and 19...
1959
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[11]
evolutionary narratives
as Reynolds (1920, p.747) to illustrate the late-type Stage V (aka Sc) spiral galaxies. evolutionary narratives. The ‘Triangal’ framework, derived empir- ically from the distribution of galaxies in theM bh–M⋆,sph diagram rather than from visual appearance alone, offers a means to rec- oncile classical morphology with modern evolutionary understand- ing. B...
1920
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[12]
if the gas is dense enough for the stars to form from condensations in the cooling clouds of gas (Jeans 1902; White & Rees
1902
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[13]
prior to galaxy gas-disc formation. Modern cosmological simulations have revisited such dissipative collapse scenarios, demonstrating that rapid, centrally concentrated star formation during early gas- rich phases can likewise produce compact quasi-spheroidal systems (e.g., Pillepich et al. 2018; Park et al. 2022). Such triaxial galaxies may have some rot...
2018
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[14]
This raises the ques- tion of whether these features mark a definitive evolutionary stage or simply come and go during the existence of discs
or weak spirals. This raises the ques- tion of whether these features mark a definitive evolutionary stage or simply come and go during the existence of discs. Although tidally-induced arms are well-documented (e.g., the Antennae galaxies), and Roche (1850) overflow can build tidal bridges and transfer material (e.g., Tashpulatov 1970; Harris 2007; Mihos ...
1970
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[15]
2010; Athanassoula et al
with higher gas fractions (Villa-Vargas et al. 2010; Athanassoula et al. 2013; D’Onghia et al. 2013; Er- win 2018; Kataria & Vivek 2024; Izquierdo-Villalba et al. 2022; Bland-Hawthorn et al. 2023, 2024). In the context of the ‘Triangal’, these late-type spirals may represent the early stages of disc growth where gas is cooling into a plane within a triaxi...
2010
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[16]
Further dry (gas-poor) major mergers can dynamically heat the stellar system, leading to the formation of an elliptical galaxy (Naab et al
and/or deposit material to create disc-like structures having a large radial extent about the system’s new centre of mass (Graham 2024b). Further dry (gas-poor) major mergers can dynamically heat the stellar system, leading to the formation of an elliptical galaxy (Naab et al. 2006). The ‘Triangal’ framework (Graham 2023c) effectively maps many of the abo...
2006
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[17]
was used to extract geometric mean (aka equivalent-axis) light profiles, which were modelled us- ing a Python 3 version of the Profilercode (Ciambur 2016).37 The results are shown here, in AB mag for theSSTdata and Vega mag for the2MASSdata, and the spheroid and galaxy stellar masses are given in Table
2016
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[18]
At the same time, the Gaussian function fit there is arguably not broad enough to capture the width of the spiral arms emanating from near the end of the actual bar
Notes: The bar component (fit with a Ferrers function in Fig- ure B2) for NGC 613 is arguably somewhat longer than the actual bar. At the same time, the Gaussian function fit there is arguably not broad enough to capture the width of the spiral arms emanating from near the end of the actual bar. Considerable stellar knots, and perhaps some bar light, can ...
2009
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[19]
The residual image was created using a model extending to a geometric-mean axis radius of∼56 ′′ (corresponding to a major-axis radius of∼108 ′′). Right: A Gaussian component (cyan) has been added at a geometric-mean axis radius of∼45 ′′ to account for the head of the spiral arms at the end of the bar, which is shown as two orange components due to the pre...
2008
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[20]
The galaxy magnitude is 9.57 mag
have been used to describe the light profile. The galaxy magnitude is 9.57 mag. MNRAS000, 1–27 (2026) Bar and spiral strength29 Figure B4.Similar to Figure B1 but for the merger NGC 3640 (Tal et al. 2009). The residual image was created using a model extending to a geometric-mean axis radius of∼64 ′′ (corresponding to a major-axis radius of∼117 ′′). Some ...
2026
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[21]
Right: Components are an inner Sérsic for the∼0.′′7 nuclear disc (dot-dash: Gültekin et al
The image size is roughly 283 ′′ wide by 343′′ high. Right: Components are an inner Sérsic for the∼0.′′7 nuclear disc (dot-dash: Gültekin et al. 2014), a Sérsic bulge (dashed red curve), an anti-truncated disc (blue), and a Gaussian (cyan) for a shelf-like feature in the image and light profile whose contribution peaks atR major ≈70 ′′. The faint three-pr...
2014
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[22]
The galaxy magnitude is 9.41 mag
describe the profile. The galaxy magnitude is 9.41 mag. MNRAS000, 1–27 (2026) 30Graham Internal Figure B7.2MASS K s-band light profile for NGC
2026
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[23]
Right: Sérsic bulge (dashed red curve) surrounded by a Sérsic oval/lens (dotted red line: Gao et al
The image size is roughly 318×306 ′′. Right: Sérsic bulge (dashed red curve) surrounded by a Sérsic oval/lens (dotted red line: Gao et al. 2018), and a large-scale exponential disc (blue line). The fraction of bulge light (0.23) is greater than that of the oval/lens (0.15). However, if the ‘lens’ model has been fit to what is actually the bulge, and the b...
2018
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[24]
The galaxyK s-band magnitude is 8.40 mag
describe the profile. The galaxyK s-band magnitude is 8.40 mag. MNRAS000, 1–27 (2026)
2026
discussion (0)
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