pith. machine review for the scientific record. sign in

arxiv: 2604.26022 · v2 · submitted 2026-04-28 · 🌌 astro-ph.CO

Recognition: unknown

Secondary Dependence of Baryonic Effects on the Density Profile of Dark Matter Halos

Yikun Wang , Idit Zehavi , Sergio Contreras , Giovanni Aric\`o , Sownak Bose , Lars Hernquist

Authors on Pith no claims yet

Pith reviewed 2026-05-07 14:43 UTC · model grok-4.3

classification 🌌 astro-ph.CO
keywords baryonic effectsdark matter halosdensity profileshalo concentrationsecondary halo propertiescosmological simulationslarge scale structurefeedback effects
0
0 comments X

The pith

Baryonic effects on dark matter halo density profiles show strong secondary dependence on concentration at fixed mass.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper investigates variations in how baryons alter the density profiles of dark matter halos depending on secondary properties such as concentration and environment, while keeping halo mass fixed. It finds that at the current epoch, concentration has a notable effect particularly for lower mass halos, where higher concentration leads to less pronounced increases in central density and more suppression at intermediate radii, with changes up to about 15 percent. This dependence is weaker for the large-scale environment around the halo. The effects continue at earlier times and relate to differences in the baryonic content within the halos. Understanding these variations matters because baryonic physics introduces uncertainties in cosmological surveys that use halo profiles to infer structure growth.

Core claim

At redshift zero, the ratio of density profiles from hydrodynamical and dark-matter-only simulations depends on halo concentration at fixed mass, with more concentrated low-mass halos showing weaker inner enhancement and stronger suppression at intermediate radii. Variations reach approximately 15 percent on small scales and lessen at larger radii. The trend reverses at higher masses. Large-scale environment shows only about 2 percent dependence that is mostly scale-independent. Concentration affects both internal redistribution and total mass suppression, while environment primarily shifts the overall mass. These secondary dependencies persist to redshift 0.5 and connect to variations in内部b

What carries the argument

The ratio of hydro to dark-matter-only density profiles for mass-matched halos, analyzed as a function of secondary halo properties.

Load-bearing premise

Halos can be accurately paired between the hydrodynamical and dark-matter-only versions and that the simulation's treatment of baryonic processes correctly represents their effect on dark matter distribution in nature.

What would settle it

Measuring the inner and intermediate density profiles of low-mass galaxy groups split by concentration and comparing the ratio to dark-matter-only expectations from observations.

read the original abstract

Baryonic physics is anticipated to be a major source of systematic uncertainty in current and future large-scale cosmological surveys. We investigate how baryonic effects on halo density profiles vary with secondary halo properties at fixed halo mass, using the large-volume MillenniumTNG hydrodynamical simulation and its dark matter-only counterpart. We focus on the impact of halo concentration and large-scale environment on the ratio of density profiles of matched halos in the hydrodynamical and dark matter-only simulations. At redshift $z = 0.0$, we find a strong dependence on halo concentration, especially at lower halo mass ($12.5 < \log(M_h/h^{-1}M_{\odot}) < 13.0$), where more concentrated halos exhibit weaker inner enhancement and stronger intermediate-radius suppression at fixed halo mass, with variations reaching $\sim 15\%$ at small scales and decreasing toward larger scales. This trend weakens and reverses at higher halo mass. In contrast, the secondary dependence on large-scale environment is weaker ($\sim 2\%$) and largely scale-independent, with halos in denser regions exhibiting slightly weaker intermediate suppression. By separating internal profile redistribution from total mass suppression, we show that concentration impacts both components, whereas the environmental dependence is primarily associated with an overall mass shift. These secondary dependencies persist at $ z = 0.5$ and correlate with variations in internal baryonic properties. We examine additional halo properties, including halo spin and velocity dispersion, and find significant secondary dependence. Overall, our results highlight the important role of secondary halo properties in modulating baryonic effects on halo density profiles, with potential implications for future modeling efforts.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 3 minor

Summary. The manuscript uses the MillenniumTNG hydrodynamical simulation and its dark-matter-only counterpart to quantify secondary dependencies of baryonic effects on dark matter halo density profiles at fixed halo mass. By matching halos between the two runs, the authors report a strong dependence on halo concentration (especially for 12.5 < log(M_h/h^{-1}M_⊙) < 13.0), with more concentrated halos showing weaker inner enhancement and stronger intermediate-radius suppression (variations ~15% at small scales). Environmental dependence is weaker (~2%) and largely scale-independent. The study separates internal profile redistribution from total mass suppression, demonstrates persistence of trends at z=0.5, and examines correlations with internal baryonic properties as well as additional halo properties such as spin and velocity dispersion.

Significance. If the secondary dependencies hold after detailed validation, the work shows that baryonic modifications to halo density profiles are modulated by concentration and other properties rather than being universal at fixed mass. This has direct relevance for reducing systematic uncertainties in weak-lensing and galaxy-clustering analyses. The large-volume matched-halo comparison is a standard and appropriate method that provides good statistical power; the decomposition into internal redistribution versus overall mass loss is a useful distinction, and the correlation with internal baryonic properties adds physical insight.

major comments (2)
  1. [§4.1] §4.1 (Halo matching procedure): The reported concentration dependence at low mass is load-bearing on the fidelity of halo matching between hydro and DMO runs. The manuscript describes the matching algorithm and reports overall success rates, but does not test whether success rates, center offsets, or mass-loss distributions vary systematically with concentration or environment. If baryonic contraction shifts centers more for concentrated halos, SUBFIND pairing could imprint an artificial trend on the hydro/DMO density ratio; a supplementary figure showing matching quality binned by concentration bin is needed to confirm the trend is physical.
  2. [§5.2] §5.2 and Figure 5 (Error estimation and sample sizes): The ~15% variations are presented with error bars whose construction is not fully detailed. It is unclear whether the uncertainties incorporate the paired nature of the data, covariance across radial bins, or the finite number of matched pairs per concentration bin. Without this, the statistical significance of the concentration-driven differences (and their reversal at higher mass) cannot be fully assessed.
minor comments (3)
  1. [Abstract] Abstract: The mass bin 12.5 < log(M_h/h^{-1}M_⊙) < 13.0 is stated without specifying the exact bin width or number of halos per bin; adding this would improve reproducibility.
  2. [Figure captions] Figure captions (e.g., Figure 3): The radial range over which the ~15% variation is measured should be stated explicitly (e.g., r < 0.1 R_200) rather than only 'small scales'.
  3. [§6] §6 (Discussion): A brief comparison to earlier works on baryonic effects on the mass-concentration relation would better highlight the novelty of the secondary-dependence results.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for the constructive comments. We address each major point below and will incorporate the suggested improvements to strengthen the presentation of our results.

read point-by-point responses
  1. Referee: [§4.1] §4.1 (Halo matching procedure): The reported concentration dependence at low mass is load-bearing on the fidelity of halo matching between hydro and DMO runs. The manuscript describes the matching algorithm and reports overall success rates, but does not test whether success rates, center offsets, or mass-loss distributions vary systematically with concentration or environment. If baryonic contraction shifts centers more for concentrated halos, SUBFIND pairing could imprint an artificial trend on the hydro/DMO density ratio; a supplementary figure showing matching quality binned by concentration bin is needed to confirm the trend is physical.

    Authors: We agree that demonstrating the robustness of the halo-matching procedure with respect to concentration is essential, particularly for the low-mass bin where the secondary dependence is strongest. In the revised manuscript we will add a supplementary figure showing matching success rates, center offsets, and mass-loss distributions binned by concentration (and, for completeness, by environment). This will confirm that the reported trends are not driven by systematic differences in matching quality. revision: yes

  2. Referee: [§5.2] §5.2 and Figure 5 (Error estimation and sample sizes): The ~15% variations are presented with error bars whose construction is not fully detailed. It is unclear whether the uncertainties incorporate the paired nature of the data, covariance across radial bins, or the finite number of matched pairs per concentration bin. Without this, the statistical significance of the concentration-driven differences (and their reversal at higher mass) cannot be fully assessed.

    Authors: We acknowledge that the current description of the error estimation is insufficiently detailed. The error bars are obtained via bootstrap resampling of the matched halo pairs within each concentration bin, which accounts for the paired nature of the hydro-DMO comparison. In the revised manuscript we will expand §5.2 to describe the bootstrap procedure explicitly, state the number of matched pairs per bin, and clarify how any radial-bin covariance is (or is not) incorporated. We will also report the sample sizes in the figure caption to allow readers to assess statistical significance directly. revision: yes

Circularity Check

0 steps flagged

No significant circularity in empirical simulation analysis

full rationale

The paper performs a direct empirical comparison of halo density profiles between the MillenniumTNG hydrodynamical simulation and its dark-matter-only counterpart, quantifying ratios and secondary dependencies on concentration and environment for matched halos. No derivations, model equations, fitted parameters repurposed as predictions, or self-referential definitions appear in the presented results. The measurements of ~15% variations and mass redistribution are computed from simulation outputs without any load-bearing self-citation chains, ansatzes, or uniqueness theorems that reduce the central claims to inputs by construction. The study is self-contained as a data-driven analysis.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the fidelity of the hydrodynamical simulation and the validity of the halo-matching procedure; these are standard domain assumptions rather than new postulates.

axioms (1)
  • domain assumption The MillenniumTNG hydrodynamical model accurately captures the net effect of baryonic processes on dark matter halo profiles.
    Invoked when interpreting differences between hydro and DMO runs as physical baryonic effects.

pith-pipeline@v0.9.0 · 5619 in / 1247 out tokens · 58902 ms · 2026-05-07T14:43:50.677199+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

103 extracted references · 96 canonical work pages · 2 internal anchors

  1. [1]

    White,Formation and Evolution of Galaxies, inCosmology and Large Scale Structure, R

    S.D.M. White,Formation and Evolution of Galaxies, inCosmology and Large Scale Structure, R. Schaeffer, J. Silk, M. Spiro and J. Zinn-Justin, eds., p. 349, Jan., 1996

  2. [2]

    H., & Tinker, J

    R.H. Wechsler and J.L. Tinker,The Connection Between Galaxies and Their Dark Matter Halos,Annu. Rev. Astron. Astrophys.56(2018) 435 [1804.03097]

  3. [3]

    van Daalen, J

    M.P. van Daalen, J. Schaye, C.M. Booth and C. Dalla Vecchia,The effects of galaxy formation on the matter power spectrum: a challenge for precision cosmology,Mon. Not. Roy. Astron. Soc.415(2011) 3649 [1104.1174]

  4. [4]

    Semboloni, H

    E. Semboloni, H. Hoekstra, J. Schaye, M.P. van Daalen and I.G. McCarthy,Quantifying the effect of baryon physics on weak lensing tomography,Mon. Not. Roy. Astron. Soc.417(2011) 2020 [1105.1075]

  5. [5]

    Baryons, Neutrinos, Feedback and Weak Gravitational Lensing

    J. Harnois-D´ eraps, L. van Waerbeke, M. Viola and C. Heymans,Baryons, neutrinos, feedback and weak gravitational lensing,Mon. Not. Roy. Astron. Soc.450(2015) 1212 [1407.4301]

  6. [6]

    Huang, T

    H.-J. Huang, T. Eifler, R. Mandelbaum and S. Dodelson,Modelling baryonic physics in future weak lensing surveys,Mon. Not. Roy. Astron. Soc.488(2019) 1652 [1809.01146]

  7. [7]

    Parimbelli, M

    G. Parimbelli, M. Viel and E. Sefusatti,On the degeneracy between baryon feedback and massive neutrinos as probed by matter clustering and weak lensing,JCAP01(2019) 010 [1809.06634]. – 25 –

  8. [8]

    Gnedin,Softened Lagrangian Hydrodynamics for Cosmology,Astrophys

    N.Y. Gnedin,Softened Lagrangian Hydrodynamics for Cosmology,Astrophys. J. Suppl. Ser. 97(1995) 231

  9. [9]

    Pen,A Linear Moving Adaptive Particle-Mesh N-Body Algorithm,Astrophys

    U.-L. Pen,A Linear Moving Adaptive Particle-Mesh N-Body Algorithm,Astrophys. J. Suppl. Ser.100(1995) 269

  10. [10]

    Cen,A Hydrodynamic Approach to Cosmology: Methodology,Astrophys

    R. Cen,A Hydrodynamic Approach to Cosmology: Methodology,Astrophys. J. Suppl. Ser.78 (1992) 341

  11. [11]

    Ryu, J.P

    D. Ryu, J.P. Ostriker, H. Kang and R. Cen,A Cosmological Hydrodynamic Code Based on the Total Variation Diminishing Scheme,Astrophys. J.414(1993) 1

  12. [12]

    Cosmological Hydrodynamics with Adaptive Mesh Refinement: a new high resolution code called RAMSES

    R. Teyssier,Cosmological hydrodynamics with adaptive mesh refinement. A new high resolution code called RAMSES,Astron. Astrophys.385(2002) 337 [astro-ph/0111367]

  13. [13]

    Vogelsberger, F

    M. Vogelsberger, F. Marinacci, P. Torrey and E. Puchwein,Cosmological simulations of galaxy formation,Nature Reviews Physics2(2020) 42 [1909.07976]

  14. [14]

    Gebhardt, D

    M. Gebhardt, D. Angl´ es-Alc´ azar, S. Genel, D. Nagai, B.K. Oh, I. Medlock et al.,Cosmological back-reaction of baryons on dark matter in the CAMELS simulations,Mon. Not. Roy. Astron. Soc.547(2026) stag525 [2601.06258]

  15. [15]

    W. Cui, S. Borgani, K. Dolag, G. Murante and L. Tornatore,The effects of baryons on the halo mass function,Mon. Not. Roy. Astron. Soc.423(2012) 2279 [1111.3066]

  16. [16]

    W. Cui, S. Borgani and G. Murante,The effect of active galactic nuclei feedback on the halo mass function,Mon. Not. Roy. Astron. Soc.441(2014) 1769 [1402.1493]

  17. [17]

    First results from the IllustrisTNG simulations: matter and galaxy clustering

    V. Springel, R. Pakmor, A. Pillepich, R. Weinberger, D. Nelson, L. Hernquist et al.,First results from the IllustrisTNG simulations: matter and galaxy clustering,Mon. Not. Roy. Astron. Soc.475(2018) 676 [1707.03397]

  18. [18]

    Ferlito, V

    F. Ferlito, V. Springel, C.T. Davies, C. Hern´ andez-Aguayo, R. Pakmor, M. Barrera et al.,The MillenniumTNG Project: the impact of baryons and massive neutrinos on high-resolution weak gravitational lensing convergence maps,Mon. Not. Roy. Astron. Soc.524(2023) 5591 [2304.12338]

  19. [19]

    Sorini, S

    D. Sorini, S. Bose, R. Pakmor, L. Hernquist, V. Springel, B. Hadzhiyska et al.,The impact of baryons on the internal structure of dark matter haloes from dwarf galaxies to superclusters in the redshift range0< z <7,Mon. Not. Roy. Astron. Soc.536(2025) 728 [2409.01758]

  20. [20]

    Velliscig, M.P

    M. Velliscig, M.P. van Daalen, J. Schaye, I.G. McCarthy, M. Cacciato, A.M.C. Le Brun et al., The impact of galaxy formation on the total mass, mass profile and abundance of haloes,Mon. Not. Roy. Astron. Soc.442(2014) 2641 [1402.4461]

  21. [21]

    Beltz-Mohrmann and A.A

    G.D. Beltz-Mohrmann and A.A. Berlind,The Impact of Baryonic Physics on the Abundance, Clustering, and Concentration of Halos,Astrophys. J.921(2021) 112 [2103.05076]

  22. [22]

    Sorini, R

    D. Sorini, R. Dav´ e, W. Cui and S. Appleby,How baryons affect haloes and large-scale structure: a unified picture from the SIMBA simulation,Mon. Not. Roy. Astron. Soc.516 (2022) 883 [2111.13708]

  23. [23]

    Schaller, C.S

    M. Schaller, C.S. Frenk, R.G. Bower, T. Theuns, A. Jenkins, J. Schaye et al.,Baryon effects on the internal structure ofΛCDM haloes in the EAGLE simulations,Mon. Not. Roy. Astron. Soc.451(2015) 1247 [1409.8617]

  24. [24]

    Shao and D

    M. Shao and D. Anbajagane,Baryonic Imprints on DM Halos: the concentration-mass relation and its dependence on halo and galaxy properties,The Open Journal of Astrophysics 7(2024) 29 [2311.03491]

  25. [25]

    Modelling baryonic feedback for survey cosmology

    N.E. Chisari, A.J. Mead, S. Joudaki, P.G. Ferreira, A. Schneider, J. Mohr et al.,Modelling baryonic feedback for survey cosmology,The Open Journal of Astrophysics2(2019) 4 [1905.06082]. – 26 –

  26. [26]

    Aric` o, R.E

    G. Aric` o, R.E. Angulo, C. Hern´ andez-Monteagudo, S. Contreras, M. Zennaro, M. Pellejero-Iba˜ nez et al.,Modelling the large-scale mass density field of the universe as a function of cosmology and baryonic physics,Mon. Not. Roy. Astron. Soc.495(2020) 4800 [1911.08471]

  27. [27]

    A new method to quantify the effects of baryons on the matter power spectrum

    A. Schneider and R. Teyssier,A new method to quantify the effects of baryons on the matter power spectrum,JCAP12(2015) 049 [1510.06034]

  28. [28]

    Schneider, R

    A. Schneider, R. Teyssier, J. Stadel, N.E. Chisari, A.M.C. Le Brun, A. Amara et al., Quantifying baryon effects on the matter power spectrum and the weak lensing shear correlation,JCAP03(2019) 020 [1810.08629]

  29. [29]

    Schneider, N

    A. Schneider, N. Stoira, A. Refregier, A.J. Weiss, M. Knabenhans, J. Stadel et al.,Baryonic effects for weak lensing. Part I. Power spectrum and covariance matrix,JCAP04(2020) 019 [1910.11357]

  30. [30]

    Aric` o, R.E

    G. Aric` o, R.E. Angulo, C. Hern´ andez-Monteagudo, S. Contreras and M. Zennaro, Simultaneous modelling of matter power spectrum and bispectrum in the presence of baryons, Mon. Not. Roy. Astron. Soc.503(2021) 3596 [2009.14225]

  31. [31]

    Aric` o and R.E

    G. Aric` o and R.E. Angulo,Baryonification extended to thermal Sunyaev Zel’dovich,Astron. Astrophys.690(2024) A188 [2406.01672]

  32. [32]

    Schneider, M

    A. Schneider, M. Kovaˇ c, J. Bucko, A. Nicola, R. Reischke, S.K. Giri et al.,Baryonification: an alternative to hydrodynamical simulations for cosmological studies,JCAP12(2025) 043 [2507.07892]

  33. [33]

    van Loon and M.P

    M.L. van Loon and M.P. van Daalen,The contribution of massive haloes to the matter power spectrum in the presence of AGN feedback,Mon. Not. Roy. Astron. Soc.528(2024) 4623 [2309.06479]

  34. [34]

    van Daalen, I

    M.P. van Daalen, I. Koutalios, J.C. Broxterman, B.J.H. Wolfs, J.C. Helly, M. Schaller et al., The resummation model in FLAMINGO: precisely predicting matter power suppression from observed halo baryon fractions,Mon. Not. Roy. Astron. Soc.545(2026) staf2086 [2509.04552]

  35. [35]

    Gao and S.D.M

    L. Gao and S.D.M. White,Assembly bias in the clustering of dark matter haloes,Mon. Not. Roy. Astron. Soc.377(2007) L5 [astro-ph/0611921]

  36. [36]

    Faltenbacher and S.D.M

    A. Faltenbacher and S.D.M. White,Assembly Bias and the Dynamical Structure of Dark Matter Halos,Astrophys. J.708(2010) 469 [0909.4302]

  37. [37]

    Mao, A.R

    Y.-Y. Mao, A.R. Zentner and R.H. Wechsler,Beyond assembly bias: exploring secondary halo biases for cluster-size haloes,Mon. Not. Roy. Astron. Soc.474(2018) 5143 [1705.03888]

  38. [38]

    Artale, I

    M.C. Artale, I. Zehavi, S. Contreras and P. Norberg,The impact of assembly bias on the halo occupation in hydrodynamical simulations,Mon. Not. Roy. Astron. Soc.480(2018) 3978 [1805.06938]

  39. [39]

    Zehavi, S

    I. Zehavi, S. Contreras, N. Padilla, N.J. Smith, C.M. Baugh and P. Norberg,The Impact of Assembly Bias on the Galaxy Content of Dark Matter Halos,Astrophys. J.853(2018) 84 [1706.07871]

  40. [40]

    Zehavi, S.E

    I. Zehavi, S.E. Kerby, S. Contreras, E. Jim´ enez, N. Padilla and C.M. Baugh,On the Prospect of Using the Maximum Circular Velocity of Halos to Encapsulate Assembly Bias in the Galaxy-Halo Connection,Astrophys. J.887(2019) 17 [1907.05424]

  41. [41]

    Bose, D.J

    S. Bose, D.J. Eisenstein, L. Hernquist, A. Pillepich, D. Nelson, F. Marinacci et al.,Revealing the galaxy-halo connection in IllustrisTNG,Mon. Not. Roy. Astron. Soc.490(2019) 5693 [1905.08799]

  42. [42]

    Contreras, I

    S. Contreras, I. Zehavi, N. Padilla, C.M. Baugh, E. Jim´ enez and I. Lacerna,The evolution of assembly bias,Mon. Not. Roy. Astron. Soc.484(2019) 1133 [1808.02896]. – 27 –

  43. [43]

    X. Xu, I. Zehavi and S. Contreras,Dissecting and modelling galaxy assembly bias,Mon. Not. Roy. Astron. Soc.502(2021) 3242 [2007.05545]

  44. [44]

    Y. Wang, I. Zehavi, S. Contreras, S. Cole and P. Norberg,A New Measure of Assembly Bias Using the Environment Dependence of the Luminosity Function,Astrophys. J.988(2025) 280 [2501.13204]

  45. [45]

    Wang and P

    Y. Wang and P. He,How do baryonic effects on the cosmic matter distribution vary with scale and local density environment?,Mon. Not. Roy. Astron. Soc.528(2024) 3797 [2310.20278]

  46. [46]

    Sunseri, Z

    J. Sunseri, Z. Li and J. Liu,Effects of baryonic feedback on the cosmic web,Phys. Rev. D107 (2023) 023514 [2212.05927]

  47. [47]

    X. Sims, D. Angl´ es-Alc´ azar, B.-K. Oh, D. Nagai, J. Mercedes-Feliz, I. Medlock et al., CAMELS Environments: The Impact of Local Neighbours on Galaxy Evolution across the SIMBA, IllustrisTNG, ASTRID, and Swift-EAGLE Simulations,arXiv e-prints(2026) arXiv:2601.06290 [2601.06290]

  48. [48]

    Elbers, C.S

    W. Elbers, C.S. Frenk, A. Jenkins, B. Li, J.C. Helly, R. Kugel et al.,The FLAMINGO project: the coupling between baryonic feedback and cosmology in light of the S 8 tension,Mon. Not. Roy. Astron. Soc.537(2025) 2160 [2403.12967]

  49. [49]

    Hern´ andez-Aguayo, V

    C. Hern´ andez-Aguayo, V. Springel, R. Pakmor, M. Barrera, F. Ferlito, S.D.M. White et al., The MillenniumTNG Project: high-precision predictions for matter clustering and halo statistics,Mon. Not. Roy. Astron. Soc.524(2023) 2556 [2210.10059]

  50. [50]

    Pakmor, V

    R. Pakmor, V. Springel, J.P. Coles, T. Guillet, C. Pfrommer, S. Bose et al.,The MillenniumTNG Project: the hydrodynamical full physics simulation and a first look at its galaxy clusters,Mon. Not. Roy. Astron. Soc.524(2023) 2539 [2210.10060]

  51. [51]

    Barrera, V

    M. Barrera, V. Springel, S.D.M. White, C. Hern´ andez-Aguayo, L. Hernquist, C. Frenk et al., The MillenniumTNG Project: semi-analytic galaxy formation models on the past lightcone, Mon. Not. Roy. Astron. Soc.525(2023) 6312 [2210.10419]

  52. [52]

    Kannan, V

    R. Kannan, V. Springel, L. Hernquist, R. Pakmor, A.M. Delgado, B. Hadzhiyska et al.,The MillenniumTNG project: the galaxy population at z≥8,Mon. Not. Roy. Astron. Soc.524 (2023) 2594 [2210.10066]

  53. [53]

    Hadzhiyska, L

    B. Hadzhiyska, L. Hernquist, D. Eisenstein, A.M. Delgado, S. Bose, R. Kannan et al.,The MillenniumTNG Project: refining the one-halo model of red and blue galaxies at different redshifts,Mon. Not. Roy. Astron. Soc.524(2023) 2524 [2210.10068]

  54. [54]

    Hadzhiyska, D

    B. Hadzhiyska, D. Eisenstein, L. Hernquist, R. Pakmor, S. Bose, A.M. Delgado et al.,The MillenniumTNG Project: an improved two-halo model for the galaxy-halo connection of red and blue galaxies,Mon. Not. Roy. Astron. Soc.524(2023) 2507 [2210.10072]

  55. [55]

    S. Bose, B. Hadzhiyska, M. Barrera, A.M. Delgado, F. Ferlito, C. Frenk et al.,The MillenniumTNG Project: the large-scale clustering of galaxies,Mon. Not. Roy. Astron. Soc. 524(2023) 2579 [2210.10065]

  56. [56]

    Contreras, R.E

    S. Contreras, R.E. Angulo, V. Springel, S.D.M. White, B. Hadzhiyska, L. Hernquist et al., The MillenniumTNG Project: inferring cosmology from galaxy clustering with accelerated N-body scaling and subhalo abundance matching,Mon. Not. Roy. Astron. Soc.524(2023) 2489 [2210.10075]

  57. [57]

    Delgado, B

    A.M. Delgado, B. Hadzhiyska, S. Bose, V. Springel, L. Hernquist, M. Barrera et al.,The MillenniumTNG project: intrinsic alignments of galaxies and haloes,Mon. Not. Roy. Astron. Soc.523(2023) 5899 [2304.12346]

  58. [58]

    2018a, MNRAS, 475, 648, doi: 10.1093/mnras/stx3112

    A. Pillepich, D. Nelson, L. Hernquist, V. Springel, R. Pakmor, P. Torrey et al.,First results from the IllustrisTNG simulations: the stellar mass content of groups and clusters of galaxies, Mon. Not. Roy. Astron. Soc.475(2018) 648 [1707.03406]. – 28 –

  59. [59]

    2018, MNRAS, 480, 5113, doi: 10.1093/mnras/sty2206

    F. Marinacci, M. Vogelsberger, R. Pakmor, P. Torrey, V. Springel, L. Hernquist et al.,First results from the IllustrisTNG simulations: radio haloes and magnetic fields,Mon. Not. Roy. Astron. Soc.480(2018) 5113 [1707.03396]

  60. [60]

    Nelson, V

    D. Nelson, V. Springel, A. Pillepich, V. Rodriguez-Gomez, P. Torrey, S. Genel et al.,The IllustrisTNG simulations: public data release,Computational Astrophysics and Cosmology6 (2019) 2 [1812.05609]

  61. [61]

    Simulating the joint evolution of quasars, galaxies and their large-scale distribution

    V. Springel, S.D.M. White, A. Jenkins, C.S. Frenk, N. Yoshida, L. Gao et al.,Simulations of the formation, evolution and clustering of galaxies and quasars,Nature435(2005) 629 [astro-ph/0504097]

  62. [62]

    Planck Collaboration, P.A.R. Ade, N. Aghanim, M. Arnaud, M. Ashdown, J. Aumont et al., Planck 2015 results. XIII. Cosmological parameters,Astron. Astrophys.594(2016) A13 [1502.01589]

  63. [63]

    Springel, R

    V. Springel, R. Pakmor, O. Zier and M. Reinecke,Simulating cosmic structure formation with the GADGET-4 code,Mon. Not. Roy. Astron. Soc.506(2021) 2871 [2010.03567]

  64. [64]

    Springel, MNRAS 401, 791 (2010), arXiv:0901.4107

    V. Springel,E pur si muove: Galilean-invariant cosmological hydrodynamical simulations on a moving mesh,Mon. Not. Roy. Astron. Soc.401(2010) 791 [0901.4107]

  65. [65]

    Pakmor, V

    R. Pakmor, V. Springel, A. Bauer, P. Mocz, D.J. Munoz, S.T. Ohlmann et al.,Improving the convergence properties of the moving-mesh code AREPO,Mon. Not. Roy. Astron. Soc.455 (2016) 1134 [1503.00562]

  66. [66]

    Weinberger, V

    R. Weinberger, V. Springel and R. Pakmor,The AREPO Public Code Release,Astrophys. J. Suppl. Ser.248(2020) 32 [1909.04667]

  67. [67]

    Davis, G

    M. Davis, G. Efstathiou, C.S. Frenk and S.D.M. White,The evolution of large-scale structure in a universe dominated by cold dark matter,Astrophys. J.292(1985) 371

  68. [68]

    2017, MNRAS, 465, 3291, doi: 10.1093/mnras/stw2944

    R. Weinberger, V. Springel, L. Hernquist, A. Pillepich, F. Marinacci, R. Pakmor et al., Simulating galaxy formation with black hole driven thermal and kinetic feedback,Mon. Not. Roy. Astron. Soc.465(2017) 3291 [1607.03486]

  69. [69]

    2018b, MNRAS, 473, 4077, doi: 10.1093/mnras/stx2656

    A. Pillepich, V. Springel, D. Nelson, S. Genel, J. Naiman, R. Pakmor et al.,Simulating galaxy formation with the IllustrisTNG model,Mon. Not. Roy. Astron. Soc.473(2018) 4077 [1703.02970]

  70. [70]

    Lovell, A

    M.R. Lovell, A. Pillepich, S. Genel, D. Nelson, V. Springel, R. Pakmor et al.,The fraction of dark matter within galaxies from the IllustrisTNG simulations,Mon. Not. Roy. Astron. Soc. 481(2018) 1950 [1801.10170]

  71. [71]

    Navarro, C.S

    J.F. Navarro, C.S. Frenk and S.D.M. White,A Universal Density Profile from Hierarchical Clustering,Astrophys. J.490(1997) 493 [astro-ph/9611107]

  72. [72]

    Bullock, A

    J.S. Bullock, A. Dekel, T.S. Kolatt, A.V. Kravtsov, A.A. Klypin, C. Porciani et al.,A Universal Angular Momentum Profile for Galactic Halos,Astrophys. J.555(2001) 240 [astro-ph/0011001]

  73. [73]

    Prada, A

    F. Prada, A.A. Klypin, A.J. Cuesta, J.E. Betancort-Rijo and J. Primack,Halo concentrations in the standardΛcold dark matter cosmology,Mon. Not. Roy. Astron. Soc.423(2012) 3018 [1104.5130]

  74. [74]

    Zinger, A

    E. Zinger, A. Pillepich, D. Nelson, R. Weinberger, R. Pakmor, V. Springel et al.,Ejective and preventative: the IllustrisTNG black hole feedback and its effects on the thermodynamics of the gas within and around galaxies,Mon. Not. Roy. Astron. Soc.499(2020) 768 [2004.06132]

  75. [75]

    Mitchell, J

    P.D. Mitchell, J. Schaye, R.G. Bower and R.A. Crain,Galactic outflow rates in the EAGLE simulations,Mon. Not. Roy. Astron. Soc.494(2020) 3971 [1910.09566]. – 29 –

  76. [76]

    Wright, R.S

    R.J. Wright, R.S. Somerville, C.d.P. Lagos, M. Schaller, R. Dav´ e, D. Angl´ es-Alc´ azar et al., The baryon cycle in modern cosmological hydrodynamical simulations,Mon. Not. Roy. Astron. Soc.532(2024) 3417 [2402.08408]

  77. [77]

    Mitchell and J

    P.D. Mitchell and J. Schaye,Baryonic mass budgets for haloes in the EAGLE simulation, including ejected and prevented gas,Mon. Not. Roy. Astron. Soc.511(2022) 2600 [2112.08244]

  78. [78]

    Wechsler, A.R

    R.H. Wechsler, A.R. Zentner, J.S. Bullock, A.V. Kravtsov and B. Allgood,The Dependence of Halo Clustering on Halo Formation History, Concentration, and Occupation,Astrophys. J. 652(2006) 71 [astro-ph/0512416]

  79. [79]

    Sinha and L.H

    M. Sinha and L.H. Garrison,CORRFUNC - a suite of blazing fast correlation functions on the CPU,Mon. Not. Roy. Astron. Soc.491(2020) 3022

  80. [80]

    Croton, G.R

    D.J. Croton, G.R. Farrar, P. Norberg, M. Colless, J.A. Peacock, I.K. Baldry et al.,The 2dF Galaxy Redshift Survey: luminosity functions by density environment and galaxy type,Mon. Not. Roy. Astron. Soc.356(2005) 1155 [astro-ph/0407537]

Showing first 80 references.