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Galaxy-Induced Transformation of Dark Matter Halos
Astrophysics of Galaxies · Submitted 14 Feb 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Halos always contract as a result of galaxy assembly, but the effect is substantially less pronounced than predicted by the "adiabatic contraction" hypothesis.
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The abstract, sentence by sentence
We use N-body/gasdynamical LambdaCDM cosmological simulations to examine the effect of the assembly of a central galaxy on the shape and mass profile of its dark halo. Two series of simulations are compared; one that follows only the evolution of the dark matter component and a second one where a baryonic component is added. These simulations include radiative cooling but neglect star formation and feedback, leading most baryons to collect at the halo center in a disk which is too small and too massive when compared with typical spiral. This unrealistic model allows us, nevertheless, to gauge the maximum effect that galaxies may have in transforming their dark halos. We find that the shape of the halo becomes more axisymmetric: halos are transformed from triaxial into essentially oblate systems, with well-aligned isopotential contours of roughly constant flattening (c/a ~ 0.85). Halos always contract as a result of galaxy assembly, but the effect is substantially less pronounced than predicted by the "adiabatic contraction" hypothesis. The reduced contraction helps to reconcile LambdaCDM halos with constraints on the dark matter content inside the solar circle and should alleviate the long-standing difficulty of matching simultaneously the scaling properties of galaxy disks and the luminosity function. The halo contraction is also less pronounced than found in earlier simulations, a disagreement that suggests that halo contraction is not solely a function of the initial and final distribution of baryons. Not only how much baryonic mass has been deposited at the center of a halo matters, but also the mode of its deposition. It might prove impossible to predict the halo response without a detailed understanding of a galaxy's assembly history. (Abriged)
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We use N-body/gasdynamical LambdaCDM cosmological simulations to examine the effect of the assembly of a central galaxy on the shape and mass profile of its dark halo. | contribution 0.55 | 0.95 | 0.03 | asserted 0.79 |
| s1 | Two series of simulations are compared; one that follows only the evolution of the dark matter component and a second one where a baryonic component is added. | method 0.98 | 0.88 | 0.02 | asserted 0.93 |
| s2 | These simulations include radiative cooling but neglect star formation and feedback, leading most baryons to collect at the halo center in a disk which is too small and too massive when compared with typical spiral. | limitation 0.82 | 0.81 | 0.03 | asserted 1.00 |
| s3 | This unrealistic model allows us, nevertheless, to gauge the maximum effect that galaxies may have in transforming their dark halos. | limitation 0.95 | 0.44 | 0.03 | asserted 0.87 |
| s4 | We find that the shape of the halo becomes more axisymmetric: halos are transformed from triaxial into essentially oblate systems, with well-aligned isopotential contours of roughly constant flattening (c/a ~ 0.85). | result 1.00 | 0.95 | 0.35 | asserted 1.00 |
| s5 | Halos always contract as a result of galaxy assembly, but the effect is substantially less pronounced than predicted by the "adiabatic contraction" hypothesis. | result 1.00 | 0.94 | 0.37 | asserted 1.00 |
| s6 | The reduced contraction helps to reconcile LambdaCDM halos with constraints on the dark matter content inside the solar circle and should alleviate the long-standing difficulty of matching simultaneously the scaling properties of galaxy disks and the luminosity function. | interpretation 1.00 | 0.55 | 0.19 | hedged possibility 0.63 |
| s7 | The halo contraction is also less pronounced than found in earlier simulations, a disagreement that suggests that halo contraction is not solely a function of the initial and final distribution of baryons. | interpretation 0.53 | 0.57 | 0.11 | hedged possibility 0.70 |
| s8 | Not only how much baryonic mass has been deposited at the center of a halo matters, but also the mode of its deposition. | interpretation 0.59 | 0.81 | 0.31 | asserted 0.99 |
| s9 | It might prove impossible to predict the halo response without a detailed understanding of a galaxy's assembly history. (Abriged) | interpretation 0.80 | 0.21 | 0.35 | speculative 0.95 |
What was examined, and what was not
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The paper
Original abstract
We use N-body/gasdynamical LambdaCDM cosmological simulations to examine the effect of the assembly of a central galaxy on the shape and mass profile of its dark halo. Two series of simulations are compared; one that follows only the evolution of the dark matter component and a second one where a baryonic component is added. These simulations include radiative cooling but neglect star formation and feedback, leading most baryons to collect at the halo center in a disk which is too small and too massive when compared with typical spiral. This unrealistic model allows us, nevertheless, to gauge the maximum effect that galaxies may have in transforming their dark halos. We find that the shape of the halo becomes more axisymmetric: halos are transformed from triaxial into essentially oblate systems, with well-aligned isopotential contours of roughly constant flattening (c/a ~ 0.85). Halos always contract as a result of galaxy assembly, but the effect is substantially less pronounced than predicted by the "adiabatic contraction" hypothesis. The reduced contraction helps to reconcile LambdaCDM halos with constraints on the dark matter content inside the solar circle and should alleviate the long-standing difficulty of matching simultaneously the scaling properties of galaxy disks and the luminosity function. The halo contraction is also less pronounced than found in earlier simulations, a disagreement that suggests that halo contraction is not solely a function of the initial and final distribution of baryons. Not only how much baryonic mass has been deposited at the center of a halo matters, but also the mode of its deposition. It might prove impossible to predict the halo response without a detailed understanding of a galaxy's assembly history. (Abriged)
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References
How later papers used it
89 later papers cite it
2 later papers by other authors are listed below: 2 used its method or tool.
Uses its method or tool 2 of 4 papers with this label
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Followed the procedure described by this paper to estimate how contracted the halo is relative to its dark matter counterpart.
Baryon-driven decontraction in Milky Way mass haloes (2021) · 0.87 · paraphrased: the licence does not allow quoting
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Used this paper's prescription to contract a halo with c200=15, obtaining rotation curves just consistent with its microlensing results.
MOA-II Galactic Microlensing Constraints: The Inner Milky Way has a Low Dark Matter Fraction and a Near Maximal Disk (2016) · 0.83 · paraphrased: the licence does not allow quoting
How the literature uses it
41 arXiv papers cite this in 63 sentences
Papers citing it · 46 sentences without a confident label
Contests it 1 paper
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However, this idealistic model rarely predicts the dark matter distribution within haloes in hydrodynamical cosmological simulations [ref] .
The evolving role of astrophysical modelling in dark matter halo relaxation response · Introduction · contest 0.72
Uses its data or values 1 paper
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We set $𝒜=0.3$ and $n=2$, as constrained by the gasdynamical simulations in [ref] .
Revisiting the 'Lensing is Low' Problem with UNIONS · Feedback · 0.95
Compares with it 3 papers
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The relaxation follows the simple quasi-adiabatic model [ref] with $q=0.33$ among larger cluster-scale ($10^14$) haloes, while group-scale haloes are consistent with the second-order polynomial relation proposed by Abadi et al. (2010) [ref] .
The evolving role of astrophysical modelling in dark matter halo relaxation response · Early epoch in IllustrisTNG simulations · 0.85
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Such is not achieved by other recent simulations that present resolutions of a few kpc [ref] .
Systematic uncertainties in the determination of the local dark matter density · Baryons dominated Milky Way model · 0.90
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Finally, we also note that the dark halo in Figure [ref] appears to be more spherical when the disk is included (in particular, the middle and third columns of the bottom row) as compared to the simulation without a disk (top row), in qualitative agreement with previous studies which have tried to include baryonic material in live halos [ref] .
Substructure depletion in the Milky Way halo by the disk · Halo shape · 0.82
Cites it as support 4 papers
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This mass-dependent behavior suggests that shallower potential wells in low-mass halos allow for sustained expansion of baryonic and dark matter distributions, possibly driven by feedback processes [ref] , while at higher masses the additional potential due to the presence of stellar bulge forces the dark matter to contract [ref] .
Feedback driven interactions between dark and luminous matter to explain tight galaxy scaling relations · The Role of Feedback-driven Interaction · 0.96
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This has been shown to be a good assumption for halos in hydrodynamic simulations [ref] , since baryons make the DM distribution more spherical in the central parts compared to the distribution obtained from DMO simulations [ref] .
Velocity-dependent J-factors for annihilation radiation from cosmological simulations · Dark matter density profiles · 0.99
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This is plausible, given results from detailed simulations of spiral formation [ref] .
How do galaxies populate Dark Matter halos? · The stellar mass “Tully-Fisher” relation · 0.98
Cites it as background 6 papers
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Although these simple models have a mixed track record of matching observations and hydrodynamic simulations of galaxy evolution, they are currently the only predictive models for the effects of galaxy evolution on the dark-matter profile in halos [ref] .
Angular Momentum Evolution in Dark Matter Halos · Introduction · 0.83
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The influence of galaxy formation on the dark halo is often interpreted as a process of (quasi-)adiabatic relaxation, where the orbits of dark matter particles respond to the condensation of baryons [ref] .
A self-similar model of galaxy formation and dark halo relaxation · The relaxation relation · 0.89
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[equation] Various quasi-adiabatic models have been proposed, offering different approaches to this framework [ref] .
The evolving role of astrophysical modelling in dark matter halo relaxation response · Relaxation Response Modeling · 0.88
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