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Galaxy-induced transformation of dark matter haloes: Transformations of CDM haloes
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We use N-body/gasdynamical cosmological simulations to examine the effect of the assembly of a central galaxy on the shape and mass profile of its surrounding dark matter halo. Two series of simulations are compared; one that follows only the evolution of the dark matter component of individual haloes in the proper Λcold dark matter (ΛCDM) cosmological context, and a second series where a baryonic component is added and followed hydrodynamically. The simulations with baryons include radiative cooling but neglect the formation of stars and their feedback. The efficient, unimpeded cooling that results leads most baryons to collect at the halo centre in a centrifugally supported disc which, due to angular momentum losses, is too small and too massive when compared with typical spiral galaxies. This admittedly unrealistic model allows us, nevertheless, to gauge the maximum effect that galaxies may have in transforming their surrounding dark haloes. We find, in agreement with earlier work, that the shape of the halo becomes more axisymmetric: post galaxy assembly, haloes are transformed from triaxial into essentially oblate systems, with well-aligned isopotential contours of roughly constant flattening (〈c/a〉∼ 0.85). Haloes always contract as a result of galaxy assembly, but the effect is substantially less pronounced than predicted by the traditional ‘adiabatic-contraction’ hypothesis. The reduced contraction helps to reconcile ΛCDM haloes with constraints on the dark matter content inside the solar circle and should alleviate the longstanding difficulty of matching simultaneously the scaling properties of galaxy discs and the galaxy luminosity function. The halo contraction we report is also less pronounced than found in earlier simulations, a disagreement which 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 centre of a halo matters, but also the mode of its deposition. Although simple formulae might work in particular cases where galaxies form nearly adiabatically, in general it might prove impossible to predict the halo response to galaxy formation without a detailed understanding of a galaxy's detailed assembly history.
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“Nonetheless, individual haloes can deviate from the mean prediction since the size of the contraction is weakly dependent on the assembly history of the system (e.g. Abadi et al. 2010; Artale et al. 2019).”
From The milky way total mass profile as inferred from Gaia DR2 (2020) · cites this paper as Abadi et al. 2010
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“This simplification is unlikely to affect our results since the baryonic distribution leads to a roughly spherical DM distribution in the inner regions, i.e. for r ≲ 20 kpc , which is the region where the best quality rotation curve data exists”
From The milky way total mass profile as inferred from Gaia DR2 (2020) · cites this paper as Abadi et al. 2010
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“Other simpler adiabatic contraction approximations, such as those used by Blumenthal et al. (1986) and Gnedin et al. (2004), tend systematically to under- or overpredict the halo contraction (e.g. Abadi et al. 2010; Duffy et al. 2010; Pedrosa et al. 2010; Dutton et al. 2016; Artale et al. 2019).”
From The milky way total mass profile as inferred from Gaia DR2 (2020) · cites this paper as Abadi et al. 2010
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Cites
Spergel, D. N., Verde, L., Peiris, H. V., Komatsu, E., Nolta, M. R., Bennett, C. L., Halpern, M., Hinshaw, G., Jarosik, N., Kogut, A., et al. (2003) · The Astrophysical Journal Supplement Series · doi:10.1086/377226 · Cited by 10,976 · cited 1×
“We adopt cosmological parameters consistent with the combined analysis of the 2dfGRS (Colless et al., 2001) and the first-year WMAP data (Spergel et al., 2003): a present day value of the Hubble constant of H0 = 70 km/s/Mpc; a scalefree initial density perturbation spectrum with no tilt and…”
MethodA Universal Density Profile from Hierarchical Clustering
Navarro, J. F., Frenk, C. S., & White, S. D. M. (1997) · The Astrophysical Journal · doi:10.1086/304888 · Cited by 9,917 · cited 4×
“The DMO mass profile is shown by the thick red solid curve and, as expected, it is well approximated by the NFW (Navarro et al., 1996b, 1997) formula (thin solid line).”
BackgroundMethodInfluentialSelf-citationThe Structure of Cold Dark Matter Halos
Navarro, J. F., Frenk, C. S., & White, S. D. M. (1996) · The Astrophysical Journal · doi:10.1086/177173 · Cited by 8,544 · cited 4×
“The DMO mass profile is shown by the thick red solid curve and, as expected, it is well approximated by the NFW (Navarro et al., 1996b, 1997) formula (thin solid line).”
BackgroundMethodInfluentialSelf-citationA Universal Density Profile from Hierarchical ClusteringPreprint
Navarro, J. F., Frenk, C. S., & White, S. D. M. (1996) · Cited by 6,275
Self-citationSimulations of the formation, evolution and clustering of galaxies and quasars
Springel, V., White, S. D. M., Jenkins, A. R., Frenk, C. S., Yoshida, N., Gao, L., Navarro, J. F., Thacker, R. J., Croton, D., Helly, J. C., et al. (2005) · Nature · doi:10.1038/nature03597 · Cited by 5,060 · cited 1×
“Each dot in this panel correspond to an NFW halo with concentration drawn at random from the mass-concentration relation (including scatter) derived by Neto et al. (2007) from the Millennium Simulation (Springel et al., 2005).”
MethodSelf-citationCroton, D. J., Springel, V., White, S. D. M., Lucia, G. D., Frenk, C. S., Gao, L., Jenkins, A., Kauffmann, G., Navarro, J. F., & Yoshida, N. (2005) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2005.09675.x · Cited by 3,686 · cited 2×
“…formation have adopted this formulation in order to link the (observed) dynamical properties of luminous galaxies to the (predicted) properties of the dark halos that surround them (see, e.g., Mo et al., 1998; Cole et al., 2000; Dutton et al., 2005; Croton et al., 2006; Somerville et al., 2008).”
BackgroundSelf-citationStatistical Properties of X‐Ray Clusters: Analytic and Numerical Comparisons
Bryan, G. L., & Norman, M. L. (1998) · The Astrophysical Journal · doi:10.1086/305262 · Cited by 2,372 · cited 1×
“The virial density contrast, ∆vir(z) is given by ∆vir(z) = 18π 2 + 82f(z) − 39f(z)2, where f(z) = [Ω0(1 + z)3/(Ω0(1 + z)3 + ΩΛ))] − 1 and Ω0 = ΩCDM + Ωb(Bryan & Norman, 1998).”
The 2dF Galaxy Redshift Survey: spectra and redshifts
Colless, M., Dalton, G., Maddox, S., Sutherland, W. J., Norberg, P., Cole, S., Bland‐Hawthorn, J., Bridges, T. J., Cannon, R., Collins, C. A., et al. (2001) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2001.04902.x · Cited by 2,368 · cited 1×
“We adopt cosmological parameters consistent with the combined analysis of the 2dfGRS (Colless et al., 2001) and the first-year WMAP data (Spergel et al., 2003): a present day value of the Hubble constant of H0 = 70 km/s/Mpc; a scalefree initial density perturbation spectrum with no tilt and…”
MethodThe formation of galactic discs
Mo, H. J., Mao, S., & White, S. D. M. (1998) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.1998.01227.x · Cited by 2,166 · cited 2×
“…formation have adopted this formulation in order to link the (observed) dynamical properties of luminous galaxies to the (predicted) properties of the dark halos that surround them (see, e.g., Mo et al., 1998; Cole et al., 2000; Dutton et al., 2005; Croton et al., 2006; Somerville et al., 2008).”
BackgroundCole, S., Lacey, C. G., Baugh, C. M., & Frenk, C. S. (2002) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2000.03879.x · Cited by 1,952
Croton, D., Springel, V., White, S. D. M., Lucia, G. D., Frenk, C. S., Gao, L., Jenkins, A. R., Kauffmann, G., Navarro, J. F., & Yoshida, N. (2006) · Max Planck Digital Library · doi:10.25916/sut.26253068.v1 · Cited by 1,611
Self-citationStatistical Properties of X-ray Clusters: Analytic and Numerical Comparisons
Bryan, G. L., & Norman, M. L. (1997) · CERN Document Server (European Organization for Nuclear Research) · Cited by 1,268
Contraction of dark matter galactic halos due to baryonic infall
Blumenthal, G. R., Faber, S. M., Flores, R., & Primack, J. R. (1986) · The Astrophysical Journal · doi:10.1086/163867 · Cited by 1,213 · cited 2×
“Despite its simplicity, and the crude approximation on which it is based, early N-body work (e.g., Barnes & White, 1984; Blumenthal et al., 1986; Jesseit et al., 2002) found reasonable agreement between eq.”
BackgroundMethodInfluentialThe inner structure of ΛCDM haloes - III. Universality and asymptotic slopes
Navarro, J. F., Hayashi, E., Power, C., Jenkins, A. R., Frenk, C. S., White, S. D. M., Springel, V., Stadel, J., & Quinn, T. (2004) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2004.07586.x · Cited by 1,129 · cited 1×
“Despite their chaotic assembly, the spherically-averaged mass profile of CDM halos is nearly “universal”, and can be approximated fairly accurately, regardless of halo mass or redshift, by scaling a simple formula (see, e.g., Navarro et al., 1996b, 1997, 2004, 2008).”
BackgroundSelf-citationSemi-analytic modelling of galaxy formation: the local Universe
Somerville, R. S., & Primack, J. R. (1999) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.1999.03032.x · Cited by 1,079 · cited 1×
“Successful models require that the rotation speed of disks be of the order of the virial velocity of the halos they inhabit (see, e.g., Somerville & Primack, 1999; Croton et al., 2006).”
BackgroundThe inner structure of CDM haloes -- I. A numerical convergence study
Power, C., Navarro, J. F., Jenkins, A. R., Frenk, C. S., White, S. D. M., Springel, V., Stadel, J., & Quinn, T. (2003) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2003.05925.x · Cited by 1,063 · cited 1×
“This re-simulation technique follows standard practice, as described, for example, by Power et al. (2003).”
MethodSelf-citationDark matter halo concentrations in the Wilkinson Microwave Anisotropy Probe year 5 cosmology
Duffy, A. R., Schaye, J., Kay, S. T., & Vecchia, C. D. (2008) · Monthly Notices of the Royal Astronomical Society Letters · doi:10.1111/j.1745-3933.2008.00537.x · Cited by 968 · cited 1×
“According to Duffy et al. (2008), this is approximately the change in average concentration when modifying the cosmological parameters from the values we adopt here (which are consistent with the first-year analysis of the WMAP satellite data) to those favoured by the latest 5-year WMAP data…”
MethodGnedin, O. Y., Kravtsov, A. V., Klypin, A. A., & Nagai, D. (2004) · The Astrophysical Journal · doi:10.1086/424914 · Cited by 945 · cited 4×
“• The halo contraction in our simulations is also less pronounced than found in earlier numerical work (see, e.g., Gnedin et al., 2004), and suggest that the response of a halo does not depend on the final mass and radial distribution of baryons in the central galaxy, but also on the mode of their…”
BackgroundMethodResultInfluentialTriaxial Modeling of Halo Density Profiles with High‐Resolution N ‐Body Simulations
Jing, Y. P., & Suto, Y. (2002) · The Astrophysical Journal · doi:10.1086/341065 · Cited by 872 · cited 1×
“CDM halos are distinctly triaxial systems supported by anisotropic velocity dispersion tensors (Frenk et al., 1988; Jing & Suto, 2002; Allgood et al., 2006; Hayashi et al., 2007; Bett et al., 2007), a result that reflects the highly aspherical nature of gravitationally-amplified density…”
BackgroundNavarro, J. F., Ludlow, A., Springel, V., Wang, J., Vogelsberger, M., White, S. D. M., Jenkins, A., Frenk, C. S., & Helmi, A. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2009.15878.x · Cited by 860
Self-citationThe statistics of CDM halo concentrations
Neto, A. F., Gao, L., Bett, P., Cole, S., Navarro, J. F., Frenk, C. S., White, S. D. M., Springel, V., & Jenkins, A. (2007) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2007.12381.x · Cited by 764 · cited 1×
“Each dot in this panel correspond to an NFW halo with concentration drawn at random from the mass-concentration relation (including scatter) derived by Neto et al. (2007) from the Millennium Simulation (Springel et al., 2005).”
MethodSelf-citationXue, X.-X., Rix, H., Zhao, G., Fiorentin, P. R., Naab, T., Steinmetz, M., van den Bosch, F. C., Beers, T. C., Lee, Y. S., Bell, E. F., et al. (2008) · The Astrophysical Journal · doi:10.1086/589500 · Cited by 716 · cited 1×
“The possibility that the virial velocity of the Milky Way is significantly lower than 220 km/s has indeed been advocated by a number of recent observational studies (Smith et al., 2007; Sales et al., 2007; Xue et al., 2008).”
BackgroundSelf-citationGasoline: a flexible, parallel implementation of TreeSPH
Wadsley, J. W., Stadel, J., & Quinn, T. (2003) · New Astronomy · doi:10.1016/j.newast.2003.08.004 · Cited by 699 · cited 1×
“All our simulations were performed using GASOLINE, a parallel N-body/SPH code described in detail by Wadsley et al. (2004). c© 2008 RAS, MNRAS 000, 000–000”
MethodAbadi, M. G., Navarro, J. F., Steinmetz, M., & Eke, V. R. (2003) · The Astrophysical Journal · doi:10.1086/378316 · Cited by 678
Self-citationThe cores of dwarf galaxy haloes
Navarro, J. F., Eke, V. R., & Frenk, C. S. (1996) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/283.3.l72 · Cited by 644 · cited 4×
“The DMO mass profile is shown by the thick red solid curve and, as expected, it is well approximated by the NFW (Navarro et al., 1996b, 1997) formula (thin solid line).”
BackgroundMethodInfluentialSelf-citationThe RAVE survey: constraining the local Galactic escape speed
Smith, M. C., Ruchti, G. R., Helmi, A., Wyse, R. F. Ġ., Fulbright, J. P., Freeman, K. C., Navarro, J. F., Seabroke, G. M., Steinmetz, M., Williams, M., et al. (2007) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2007.11964.x · Cited by 629 · cited 1×
“The possibility that the virial velocity of the Milky Way is significantly lower than 220 km/s has indeed been advocated by a number of recent observational studies (Smith et al., 2007; Sales et al., 2007; Xue et al., 2008).”
BackgroundSelf-citationThe shape of dark matter haloes: dependence on mass, redshift, radius and formation
Allgood, B., Flores, R. A., Primack, J. R., Kravtsov, A. V., Wechsler, R. H., Faltenbacher, A., & Bullock, J. S. (2006) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2006.10094.x · Cited by 588 · cited 1×
“CDM halos are distinctly triaxial systems supported by anisotropic velocity dispersion tensors (Frenk et al., 1988; Jing & Suto, 2002; Allgood et al., 2006; Hayashi et al., 2007; Bett et al., 2007), a result that reflects the highly aspherical nature of gravitationally-amplified density…”
BackgroundThe formation of dark halos in a universe dominated by cold dark matter
Frenk, C. S., White, S. D. M., Davis, M., & Efstathiou, G. (1988) · The Astrophysical Journal · doi:10.1086/166213 · Cited by 541 · cited 1×
“CDM halos are distinctly triaxial systems supported by anisotropic velocity dispersion tensors (Frenk et al., 1988; Jing & Suto, 2002; Allgood et al., 2006; Hayashi et al., 2007; Bett et al., 2007), a result that reflects the highly aspherical nature of gravitationally-amplified density…”
BackgroundDark matter halo concentrations in the Wilkinson Microwave Anisotropy Probe year 5 cosmologyPreprint
Duffy, A. R., Schaye, J., Kay, S. T., et al. (2008) · doi:10.48550/arxiv.0804.2486 · Cited by 524 · cited 1×
“According to Duffy et al. (2008), this is approximately the change in average concentration when modifying the cosmological parameters from the values we adopt here (which are consistent with the first-year analysis of the WMAP satellite data) to those favoured by the latest 5-year WMAP data…”
MethodBett, P. E., Eke, V. R., Frenk, C. S., Jenkins, A. R., Helly, J. C., & Navarro, J. F. (2007) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2007.11432.x · Cited by 490 · cited 1×
“…systems supported by anisotropic velocity dispersion tensors (Frenk et al., 1988; Jing & Suto, 2002; Allgood et al., 2006; Hayashi et al., 2007; Bett et al., 2007), a result that reflects the highly aspherical nature of gravitationally-amplified density fluctuations as they become non linear…”
BackgroundSelf-citationThe Power Spectrum Dependence of Dark Matter Halo Concentrations
Eke, V. R., Navarro, J. F., & Steinmetz, M. (2001) · The Astrophysical Journal · doi:10.1086/321345 · Cited by 484 · cited 1×
“As discussed by Eke et al. (2001), most ΛCDM halos satisfy the constraints, and would be consistent with the MW if they were somehow able to avoid contraction.”
BackgroundSelf-citationAbadi, M. G., Navarro, J. F., Steinmetz, M., & Eke, V. R. (2003) · The Astrophysical Journal · doi:10.1086/375512 · Cited by 430
Self-citationDark Halo and Disk Galaxy Scaling Laws in Hierarchical Universes
Navarro, J. F., & Steinmetz, M. (2000) · The Astrophysical Journal · doi:10.1086/309175 · Cited by 404 · cited 1×
“On the other hand, Navarro & Steinmetz (2000) argue that it is unlikely that a galaxy where md << fbar may have the same specific angular momentum as the whole system, and propose that jdisk, as a fraction of jvir, should be comparable to the fraction of baryons that make up the central galaxy;…”
BackgroundSelf-citationDark Halos: The Flattening of the Density Cusp by Dynamical Friction
El‐Zant, A., Shlosman, I., & Hoffman, Y. (2001) · The Astrophysical Journal · doi:10.1086/322516 · Cited by 383 · cited 1×
“This possibility has been argued before (see, e.g., El-Zant et al., 2001; Ma & BoylanKolchin, 2004; Mo & Mao, 2004), and seems to find favor in our simulations, where mergers between massive baryonic clumps are frequent and plentiful and halo contraction is less strong than reported in earlier work.”
ResultFaber, S. M. (1987) · Springer eBooks · doi:10.1007/978-1-4612-4762-3 · Cited by 372
Hierarchical galaxy formation - Overmerging and the formation of an X-ray cluster
Katz, N., & White, S. D. M. (1993) · The Astrophysical Journal · doi:10.1086/172935 · Cited by 367 · cited 1×
“This was already noted in the first simulations to include, in addition to a dark matter halo, a dissipative baryonic component, such as the early work of Katz & Gunn (1991) and Katz & White (1993).”
BackgroundThe Effect of Gas Cooling on the Shapes of Dark Matter Halos
Kazantzidis, S., Kravtsov, A. V., Zentner, A. R., Allgood, B., Nagai, D., & Moore, B. (2004) · The Astrophysical Journal · doi:10.1086/423992 · Cited by 337
Dissipational galaxy formation. I - Effects of gasdynamics
Katz, N., & Gunn, J. E. (1991) · The Astrophysical Journal · doi:10.1086/170367 · Cited by 324 · cited 1×
“This was already noted in the first simulations to include, in addition to a dark matter halo, a dissipative baryonic component, such as the early work of Katz & Gunn (1991) and Katz & White (1993).”
BackgroundNavarro, J. F., & White, S. D. M. (1994) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/267.2.401 · Cited by 310 · cited 1×
“1991; Navarro & White, 1994; Navarro et al., 1997), this mode of assembly leads to very efficient accretion of baryons into the central galaxy and to the transfer of much of their angular momentum to the surrounding halo.”
BackgroundSelf-citationThe Power Spectrum Dependence of Dark Matter Halo Concentrations
Eke, V. R., Navarro, J. F., & Steinmetz, M. (2000) · CERN Document Server (European Organization for Nuclear Research) · Cited by 305
Self-citationDARK HALOS: THE FLATTENING OF THE DENSITY CUSP BY DYNAMICAL FRICTIONPreprint
El‐Zant, A. A., Shlosman, I., & Hoffman, Y. (2001) · Cited by 275
A Revised Model for the Formation of Disk Galaxies: Low Spin and Dark Halo Expansion
Dutton, A. A., van den Bosch, F. C., Dekel, A., & Courteau, S. (2006) · The Astrophysical Journal · doi:10.1086/509314 · Cited by 274 · cited 1×
“Recent work has also speculated that mergers may lead to halo expansion and that this would help to reconcile the properties of disk galaxies with ΛCDM halos (Dutton et al., 2007).”
BackgroundNearly normal galaxies. From the Planck time to the present
Faber, S. M. (1987) · Cited by 259
The effect of dissipation on the shapes of dark halos
Dubinski, J. (1994) · The Astrophysical Journal · doi:10.1086/174512 · Cited by 258 · cited 1×
“Dubinski (1994) studied this further by growing adiabatically a central mass concentration inside a triaxial dark matter halo and confirmed that the steepening of the potential leads to much rounder halo shapes.”
BackgroundThe hierarchical origin of galaxy morphologies
Steinmetz, M., & Navarro, J. F. (2002) · New Astronomy · doi:10.1016/s1384-1076(02)00102-1 · Cited by 245
Self-citationDynamics of cooling gas in galactic dark halos
Navarro, J. F., & Benz, W. (1991) · The Astrophysical Journal · doi:10.1086/170590 · Cited by 236
Self-citationEvolution of the mass function of dark matter haloes
Reed, D., Gardner, J., Quinn, T., Stadel, J., Fardal, M., Lake, G., & Governato, F. (2003) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-2966.2003.07113.x · Cited by 228 · cited 1×
“Each simulation follows the evolution of a relatively small region of the Universe, excised from a 4323-particle simulation of a large 50 h−1 Mpc periodic box (Reed et al., 2003), and resimulated at much higher mass and spatial resolution.”
MethodSelf-citationThe Causes of Halo Shape Changes Induced by Cooling Baryons: Disks versus Substructures
Debattista, V. P., Moore, B., Quinn, T., Kazantzidis, S., Maas, R. W., Mayer, L., Read, J. I., & Stadel, J. (2008) · The Astrophysical Journal · doi:10.1086/587977 · Cited by 190
Baryonic pinching of galactic dark matter halos
Gustafsson, M., Fairbairn, M., & Sommer‐Larsen, J. (2006) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.74.123522 · Cited by 183 · cited 1×
“In this respect, our study is similar to that of Gustafsson et al. (2006), who studied four simulations of galaxysized halos in the ΛCDM scenario.”
ResultInfluentialAn Explanation for the Observed Weak Size Evolution of Disk Galaxies
Somerville, R. S., Barden, M., Rix, H., Bell, E. F., Beckwith, S. V. W., Borch, A., Caldwell, J. A. R., Hausler, B., Heymans, C., Jahnkę, K., et al. (2008) · The Astrophysical Journal · doi:10.1086/523661 · Cited by 176
The shape of the gravitational potential in cold dark matter haloes
Hayashi, E., Navarro, J. F., & Springel, V. (2007) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2007.11599.x · Cited by 167
Self-citationThe Compression of Dark Matter Halos by Baryonic Infall
Sellwood, J. A., & McGaugh, S. S. (2005) · The Astrophysical Journal · doi:10.1086/491731 · Cited by 164
The Hierarchical Origin of Galaxy MorphologiesPreprint
Steinmetz, M., & Navarro, J. F. (2002) · Cited by 162
Self-citationEvolution of the mass function of dark matter haloes
Reed, D., Gardner, J., Quinn, T., Stadel, J., Fardal, M. A., Lake, G., & Governato, F. (2003) · Zurich Open Repository and Archive (University of Zurich) · doi:10.5167/uzh-154878 · Cited by 131
Self-citationFaint Blue Galaxies and the Epoch of Dwarf Galaxy Formation
Babul, A., & Ferguson, H. C. (1996) · The Astrophysical Journal · doi:10.1086/176795 · Cited by 124 · cited 1×
“…is truly needed to reconcile disk properties with ΛCDM halos, it should come as a consequence of other processes not considered here, such as feedback-driven winds that may remove substantial fraction of baryons from the central galaxy (see, e.g., Navarro et al., 1996a; Babul & Ferguson, 1996).”
BackgroundSelf-citationMeza, A., Navarro, J. F., Steinmetz, M., & Eke, V. R. (2003) · The Astrophysical Journal · doi:10.1086/375151 · Cited by 112 · cited 1×
“These correspond to gasdynamical simulations of galaxy formation presented by Abadi et al. (2003a,b) and Meza et al. (2003), and differ from ours mainly in their inclusion of star formation and feedback effects.”
MethodSelf-citationSatellites of simulated galaxies: survival, merging and their relationto the dark and stellar haloes
Sales, L. V., Navarro, J. F., Abadi, M. G., & Steinmetz, M. (2007) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2007.12024.x · Cited by 111 · cited 1×
“The possibility that the virial velocity of the Milky Way is significantly lower than 220 km/s has indeed been advocated by a number of recent observational studies (Smith et al., 2007; Sales et al., 2007; Xue et al., 2008).”
BackgroundSelf-citationGalaxy formation in pre-processed dark haloes
Mo, H. J., & Mao, S. (2004) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2004.08114.x · Cited by 107 · cited 1×
“This possibility has been argued before (see, e.g., El-Zant et al., 2001; Ma & BoylanKolchin, 2004; Mo & Mao, 2004), and seems to find favor in our simulations, where mergers between massive baryonic clumps are frequent and plentiful and halo contraction is less strong than reported in earlier work.”
ResultDisc galaxy evolution models in a hierarchical formation scenario: structure and dynamics
Firmani, C., & Ávila-Reese, V. (2000) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2000.03338.x · Cited by 103
The response of a spheroid to a disc field or were bulges ever ellipticals?
Barnes, J., & White, S. D. M. (1984) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/211.4.753 · Cited by 98 · cited 2×
“Despite its simplicity, and the crude approximation on which it is based, early N-body work (e.g., Barnes & White, 1984; Blumenthal et al., 1986; Jesseit et al., 2002) found reasonable agreement between eq.”
BackgroundMethodInfluentialThe orbital evolution induced by baryonic condensation in triaxial haloes
Valluri, M., Debattista, V. P., Quinn, T., & Moore, B. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2009.16192.x · Cited by 96
Dark Matter Halos of Disk Galaxies: Constraints from the Tully‐Fisher Relation
Gnedin, O. Y., Weinberg, D. H., Pizagno, J., Prada, F., & Rix, H. (2007) · The Astrophysical Journal · doi:10.1086/523256 · Cited by 79
Galaxy Dynamics - A Rutgers Symposium
Merritt, D. R., Valluri, M., & Sellwood, J. A. (1999) · Cited by 77
Dark Matter Halos of Disk Galaxies: Constraints from the Tully-Fisher Relation
Gnedin, O. Y., Weinberg, D. H., Pizagno, J., Prada, F., & Rix, H. (2006) · CERN Document Server (European Organization for Nuclear Research) · Cited by 57
The Validity of the Adiabatic Contraction Approximation for Dark Matter Halos
Jesseit, R., Naab, T., & Burkert, A. (2002) · The Astrophysical Journal · doi:10.1086/341369 · Cited by 55 · cited 1×
“Despite its simplicity, and the crude approximation on which it is based, early N-body work (e.g., Barnes & White, 1984; Blumenthal et al., 1986; Jesseit et al., 2002) found reasonable agreement between eq.”
BackgroundThe Validity of the Adiabatic Contraction Approximation for Dark Matter Halos
Jesseit, R., Naab, T., & Burkert, A. (2002) · CERN Document Server (European Organization for Nuclear Research) · Cited by 53
The joint evolution of baryons and dark matter haloes
Pedrosa, S., Tissera, P. B., & Scannapieco, C. (2009) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2009.15951.x · Cited by 48
HALO DENSITY REDUCTION BY BARYONIC SETTLING?
Jardel, J. R., & Sellwood, J. A. (2009) · The Astrophysical Journal · doi:10.1088/0004-637x/691/2/1300 · Cited by 40
Halo Response to Galaxy Formation
Barnes, J. E. (1987) · Nearly Normal Galaxies · doi:10.1007/978-1-4612-4762-3_20 · Cited by 22 · cited 1×
“Barnes (1987) and Sellwood (1999) have remarked that the adiabatic contraction hypothesis might lead to substantial overestimation of the halo compression.”
BackgroundDark matter halo response to the disc growth
Choi, J.-H., Lu, Y., Mo, H. J., & Weinberg, M. D. (2006) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2006.10990.x · Cited by 22 · cited 1×
“As discussed by Sellwood & McGaugh (2005) and Choi et al. (2006), such deviations are likely to depend strongly on the orbital structure of a halo, performing best when most particles have large tangential motions, but poorly in systems with radially anisotropic velocity distributions.”
BackgroundThe Tully-Fisher Zero Point ProblemPreprint
Dutton, A. A., van den Bosch, F. C., & Courteau, S. (2008) · arXiv (Cornell University) · doi:10.48550/arxiv.0801.1505 · Cited by 7
Research works printed but not linked: 1
- Ma, 2004, Phys. Rev. Lett., 93, 1301
Cited by
Sorted by citations
The Galaxy in Context: Structural, Kinematic, and Integrated Properties
Bland-Hawthorn, J., & Gerhard, O. (2016) · Annual Review of Astronomy and Astrophysics · doi:10.1146/annurev-astro-081915-023441 · Cited by 1,656
“When baryons are included, the halos become more spherical and evolve toward oblate at all radii but mostly in their inner parts (e.g., Kazantzidis et al. 2004, Bailin et al. 2005, Abadi et al. 2010).”
BackgroundUniverseMachine: The correlation between galaxy growth and dark matter halo assembly from z = 0−10
Behroozi, P., Wechsler, R. H., Hearin, A. P., & Conroy, C. (2019) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stz1182 · Cited by 1,243
“Remaining effects of baryons on halo potential wells (e.g., making them less triaxial; Abadi et al. 2010) are more difficult to observe, and may require higher-order statistics such as three-point functions to capture.”
BackgroundFrom dwarf spheroidals to cD galaxies: simulating the galaxy population in a ΛCDM cosmology
Guo, Q., White, S. D. M., Boylan-Kolchin, M., Lucia, G. D., Kauffmann, G., Lemson, G., Li, C., Springel, V., & Weinmann, S. M. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.18114.x · Cited by 1,205
“However, recent simulations suggest that this simple scheme overestimates the effect (e.g. Gnedin et al. 2004; Abadi et al. 2010).”
BackgroundKravtsov, A. V., & Borgani, S. (2012) · Annual Review of Astronomy and Astrophysics · doi:10.1146/annurev-astro-081811-125502 · Cited by 951
“At the same time, several recent studies showed that no single set of parameters of such simple models describes all objects that form in cosmological simulations equally well(Abadi et al. 2010; Gnedin et al. 2011; Gustafsson, Fairbairn & Sommer-Larsen 2006; Tisseraet al. 2010).”
BackgroundTHE TWO PHASES OF GALAXY FORMATION
Oser, L., Ostriker, J. P., Naab, T., Johansson, P. H., & Burkert, A. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/725/2/2312 · Cited by 840
“…expected from the effect of adiabatic contraction galaxies with significant in-situ star formation, i.e. more dissipation, live in more concentrated halos (Blumenthal et al. 1986; Dubinski 1994; Jesseit et al. 2002; Debattista et al. 2008; Gnedin et al. 2004; Abadi et al. 2010; Auger et al. 2010).”
Background
Metadata
- Authors
- Abadi, M. G., Navarro, J. F., Fardal, M., Babul, A., & Steinmetz, M.
- Affiliations
- Consejo Nacional de Investigaciones Científicas y Técnicas (AR)
- University of Victoria (CA)
- University of Massachusetts Amherst (US)
- Leibniz Institute for Astrophysics Potsdam (DE)
- Corresponding author
- Abadi, Mario G.
- Venue
- Monthly Notices of the Royal Astronomical Society
- Publisher
- Oxford University Press (OUP)
- Published
- 2010-08-19
- Volume
- 407
- Issue
- 1
- Pages
- 435-446
- ISSN
- 0035-8711 (ISSN-L)
- OpenAlex
- W2159553024
- Cited by
- 237
- References
- 69
- Citations by year
- 2026: 1 · 2025: 7 · 2024: 15 · 2023: 12 · 2022: 14 · 2021: 11 · 2020: 10 · 2019: 14 · 2018: 12 · 2017: 6 · 2016: 17 · 2015: 11 · 2014: 20 · 2013: 13 · 2012: 31
- FWCI
- 14.30
- Type
- journal article
- Language
- en
- Open access
- bronze
- doi.org
- Locations
- Monthly Notices of the Royal Astronomical Society (publishedVersion)
- Conicet (publishedVersion, cc-by-nc-sa)
- arXiv (Cornell University) (submittedVersion)
- HighWire Press Open Archive (submittedVersion)
- arXiv (Cornell University)
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Galaxies: Formation, Evolution, Phenomena
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Cosmology and Gravitation Theories
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Dark Matter and Cosmic Phenomena
- Keywords
- dark matter halos, galaxy formation, halo shape, halo mass profiles, radiative cooling, adiabatic contraction, galaxy assembly, luminosity function
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