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Contraction of dark matter galactic halos due to baryonic infall
Abstract
Varied evidence suggests that galaxies consist of roughly 10 percent baryonic matter by mass and that baryons sink dissipatively by about a factor of 10 in. radius during galaxy formation. It is shown that such infall strongly perturbs the underlying dark matter distribution, pulling it inward and creating cores that are considerably smaller and denser than would have evolved without dissipation. Any discontinuity between the baryonic and dark matter mass distributions is smoothed out by the coupled motions of the two components. If dark halos have large core radii in the absence of dissipation, the above infall scenario yields rotation curves that are flat over large distances, in agreement with observations of spiral galaxies. Such large dissipationless cores may plausibly result from large internal kinetic energy in protogalaxies at maximum expansion, perhaps as a result of subclustering, tidal effects, or anisotropic collapse.
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“For MW and higher mass haloes, the effect of baryons on the DM halo is well described by the adiabatic contraction model (Callingham et al. 2020), in which baryons slowly accumulate at the halo centre and the DM distribution distorts in such a way that its action integrals remain approximately constant”
From The milky way total mass profile as inferred from Gaia DR2 (2020) · cites this paper as Blumenthal et al. 1986
In the citing paper
“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 Blumenthal et al. 1986
In the citing paper
“That baryons can cause a DM halo to contract has been known for a long time (Blumenthal et al. 1986; Barnes 1987), and this has been confirmed by many subsequent studies”
From The milky way total mass profile as inferred from Gaia DR2 (2020) · cites this paper as Blumenthal et al. 1986
In the citing paper
“and that roughly agrees with the Blumenthal et al. (1986) and Gnedin et al. (2004) adiabatic contraction approximations, although we do find systematic deviations at the 10% level.”
From The milky way total mass profile as inferred from Gaia DR2 (2020) · cites this paper as Blumenthal et al. (1986)
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Small Scale Problems of the ΛCDM Model: A Short Review
Popolo, A. D., & Delliou, M. L. (2017) · Galaxies · doi:10.3390/galaxies5010017 · Cited by 316
“Other authors studied adiabatic contraction of DM haloes [270,271]5, that conversely produces a steepening of the density profiles.”
BackgroundA lower bound on the mass of dark matter particles
Boyarsky, A. M., Oleg Ruchayskiy, C., & Iakubovskyi, D. (2009) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2009/03/005 · Cited by 264
“The baryons, which are condensed in the center, influence the shape of DM halo gravitationally, increasing the central DM density [137, 138].”
BackgroundTreu, T., & Koopmans, L. V. E. (2002) · The Astrophysical Journal · doi:10.1086/341216 · Cited by 263
“A simple treatment of this phenomenon can be given by assuming the so-called ‘‘ adiabatic approximation ’’ (Blumenthal et al. 1986; see alsoMo,Mao, &White 1998).”
Resolving the Formation of Protogalaxies. III. Feedback from the First Stars
Wise, J., & Abel, T. (2008) · The Astrophysical Journal · doi:10.1086/590417 · Cited by 259
“During central gaseous collapses in halos, the gravitational potential in the inner ∼50 pc becomes baryon dom- inated where the baryon density is greater than the DM density, leading to a contraction of the DM inner halo (Blumenthal et al. 1986; Gnedin et al. 2004).”
BackgroundThe Stellar and Sub-Stellar Initial Mass Function of Simple and Composite Populations
Kroupa, P., Weidner, C., Pflamm-Altenburg, J., Thies, I., Dabringhausen, J., Marks, M., & Maschberger, T. (2013) · Springer eBooks · doi:10.1007/978-94-007-5612-0_4 · Cited by 373
“They assume that UCDs are hyper-massive star clusters, i.e. that their stellar population formed 17Adiabatic contraction (Blumenthal et al. 1986) in UCDs may however alleviate this problem but unlikely sufficiently so (Murray 2009).”
BackgroundShredded Galaxies as the Source of Diffuse Intrahalo Light on Varying Scales
Purcell, C. W., Bullock, J. S., & Zentner, A. R. (2007) · The Astrophysical Journal · doi:10.1086/519787 · Cited by 264
“The response of the dark matter profile to the presence of these cooling baryons is often modeled via adiabatic contraction (AC) (see, e.g., Blumenthal et al. 1986; Gnedin et al. 2004).”
BackgroundEquilibrium Disk‐Bulge‐Halo Models for the Milky Way and Andromeda Galaxies
Widrow, L. M., & Dubinski, J. (2005) · The Astrophysical Journal · doi:10.1086/432710 · Cited by 251
“Under a rather restrictive set of assumptions, the adiabatic theorem leads to the following simple relation: Mbaryon(r)þMdm r ¼ Mhalo(ri)ri ð18Þ (Young 1980; Blumenthal et al. 1986; Flores et al. 1993).”
Backgroundvan den Bosch, F. C., Robertson, B. E., Dalcanton, J. J., & de Blok, W. J. G. (2000) · The Astronomical Journal · doi:10.1086/301315 · Cited by 242
“We treat this adiabatic contraction of the dark halo following the procedure in Blumenthal et al. (1986) and Flores et al. (1993).”
MethodDetermination of the local dark matter density in our Galaxy
Weber, M., & de Boer, W. (2009) · Astronomy and Astrophysics · doi:10.1051/0004-6361/200913381 · Cited by 247
“th N-body simulations using an NFW profile Xue et al. (2008) find MR<60 kpc = 4.0 ±0.7 ·1011M⊙, (5) which corresponds to Mtot = 1.0+0.3 −0.2 · 10 12 M ⊙. To get this total mass adiabatic contraction(Blumenthal et al. 1986) was allowed in whichcase the concentrationparameterwas takenas a freeparameter in the fit. This…”
MethodInfluentialThe dust content of galaxies from z = 0 to z = 9
Popping, G., Somerville, R. S., & Galametz, M. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx1545 · Cited by 268
“…based on the initial angular momentum of the gas and the halo profile, assuming that angular momentum is conserved and that the self-gravity of the collapsing baryons causes contraction of the matter in the inner part of the halo (Blumenthal et al. 1986; Flores et al. 1993; Mo, Mao & White 1998).”
BackgroundDensity profiles of galaxy groups and clusters from SDSS galaxy-galaxy weak lensing
Mandelbaum, R., Seljak, U., Cool, R. J., Blanton, M. R., Hirata, C. M., & Brinkmann, J. V. (2006) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2006.10906.x · Cited by 243
“This effect is known as adiabatic contraction (AC, Blumenthal et al. 1986, Gnedin et al. 2004, Gnedin 2005, Sellwood & McGaugh 2005) and has been studied with analytic models and simulations.”
BackgroundAChandraView of Dark Matter in Early‐Type Galaxies
Humphrey, P. J., Buote, D. A., Gastaldello, F., Zappacosta, L., Bullock, J. S., Brighenti, F., & Mathews, W. G. (2006) · The Astrophysical Journal · doi:10.1086/505019 · Cited by 241
“This process is typically modeled assuming adiabatic contraction (AC) of the DM particle orbits (e.g., Blumenthal et al. 1986; Gnedin et al. 2004).”
Somerville, R. S., Gilmore, R. C., Primack, J. R., & Domínguez, A. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2012.20490.x · Cited by 239
“…based on the initial angular momentum of the gas and the halo profile, assuming that angular momentum is conserved and that the self-gravity of the collapsing baryons causes contraction of the matter in the inner part of the halo (Blumenthal et al. 1986; Flores et al. 1993; Mo, Mao & White 1998).”
BackgroundSelf-citationKoopmans, L. V. E., & Treu, T. (2003) · The Astrophysical Journal · doi:10.1086/345423 · Cited by 242
“In the context of adiabatic contraction (AC) models (see, e.g., Blumenthal et al. 1986; Mo, Mao, & White 1998), the initial slope ( i) of the dark matter halo, i.e., before baryons assembled in the dark matter potential well, is in general expected to be shallower than the observed dark matter…”
Backgroundvan den Bosch, F. C., More, S., Cacciato, M., Mo, H. J., & Yang, X. (2013) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sts006 · Cited by 251
A BARYONIC SOLUTION TO THE MISSING SATELLITES PROBLEM
Brooks, A. M., Kuhlen, M., Zolotov, A., & Hooper, D. (2013) · The Astrophysical Journal · doi:10.1088/0004-637x/765/1/22 · Cited by 255
“…has become broadly accepted in recent years that baryonic processes can alter the distributions of dark matter within halos, potentially steepening (Blumenthal et al. 1986; Gnedin & Zhao 2002; Gnedin et al. 2011) or flattening (Navarro et al. 1996; Read & Gilmore 2005; Mashchenko et al.…”
BackgroundGalaxy-induced transformation of dark matter haloes: Transformations of CDM haloes
Abadi, M. G., Navarro, J. F., Fardal, M., Babul, A., & Steinmetz, M. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.16912.x · Cited by 237
“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.”
BackgroundMethodInfluentialDark Matter and Collider Phenomenology of Universal Extra DimensionsPreprint
Hooper, D., & Profumo, S. (2007) · Cited by 232
Laporte, C. F. P., Johnston, K. V., Gómez, F. A., Garavito-Camargo, N., & Besla, G. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty1574 · Cited by 230
“2It should be noted that the inferences from the shape of the HI warp are based on kinematic distance estimates that are known to be severely biased by up to a factor of two (Reid et al. 2014). as formulated by Blumenthal et al. (1986).”
BackgroundGravitational clustering of relic neutrinos and implications for their detection
Ringwald, A., & Wong, Y. Y. Y. (2004) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2004/12/005 · Cited by 251
In wino veritas? Indirect searches shed light on neutralino dark matter
Fan, J., & Matthew Reece, B. (2013) · Journal of High Energy Physics · doi:10.1007/jhep10(2013)124 · Cited by 254
“as argued on theoretical grounds [61] and observed in simulations (e.”
BackgroundGamma ray signals from dark matter: Concepts, status and prospects
Bringmann, T., & Weniger, C. (2012) · Physics of the Dark Universe · doi:10.1016/j.dark.2012.10.005 · Cited by 228
“In particular, the cooling and infall of baryons could – by a mechanism known as adiabatic contraction – lead to a steepening of the inner DM profile [84–86].”
BackgroundBoylan-Kolchin, M., Ma, C., & Quataert, E. (2006) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2006.10379.x · Cited by 221
“We include the effects of baryonic dissipation via the adiabatic contraction model of Blumenthal et al. (1986).”
MethodAuger, M. W., Treu, T., Gavazzi, R., Bolton, A. S., Koopmans, L. V. E., & Marshall, P. J. (2010) · The Astrophysical Journal Letters · doi:10.1088/2041-8205/721/2/l163 · Cited by 224
“…to radiative dissipation from the baryons that depends on the mass of stars formed in the galaxy (e.g., the adiabatic contraction, or AC, models of Blumenthal et al. 1986; Gnedin et al. 2004, hereafter B86 and G04) or dynamical friction may counterbalance this effect (Abadi et al. 2009) and could…”
BackgroundDark Matter and the First Stars: A New Phase of Stellar Evolution
Spolyar, D., Freese, K., & Paolo Gondolo, A. (2008) · Physical Review Letters · doi:10.1103/physrevlett.100.051101 · Cited by 223
A halo mass—concentration relation from weak lensing
Mandelbaum, R., Seljak, U., & Hirata, C. M. (2008) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2008/08/006 · Cited by 221
Effects of Cooling and Star Formation on the Baryon Fractions in Clusters
Kravtsov, A. V., Nagai, D., & Vikhlinin, A. A. (2005) · The Astrophysical Journal · doi:10.1086/429796 · Cited by 222
Gieles, M., Charbonnel, C., Krause, M., Hénault-Brunet, V., Agertz, O., Lamers, H. J. G. L. M., Bastian, N., Gualandris, A., Zocchi, A., & Petts, J. A. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty1059 · Cited by 230
“We define Vrms as the one-dimensional velocity dispersion of the cluster, and assume that the angular momentum of the inflowing gas is negligible, such that the adiabatic invariant MVrmsRh of the star cluster is preserved, while M increases as the result of accretion (Blumenthal et al. 1986).”
BackgroundDuffy, A. R., Schaye, J., Kay, S. T., Dalla Vecchia, C., Battye, R. A., & Booth, C. M. (2010) · MPG.PuRe (Max Planck Society) · Cited by 220
The Stellar Mass Tully-Fisher Relation to z = 1.2 from AEGIS
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“5 and σs, which is expected to be affected by baryon dissipation and the response of the dark halo to it (e.g., Blumenthal et al. 1986), neither of which are completely understood.”
BackgroundSelf-citationMaximal Disks and the Tully‐Fisher Relation
Courteau, S., & Rix, H. (1999) · The Astrophysical Journal · doi:10.1086/306872 · Cited by 218
“If the central accumulation of the baryons occurs on a longer time scale than the local dynamical time, the dissipationless dark matter halo will contract obeying adiabatic invariance (Blumenthal et al. 1986).”
BackgroundBar‐driven Dark Halo Evolution: A Resolution of the Cusp‐Core Controversy
Weinberg, M. D., & Katz, N. (2002) · The Astrophysical Journal · doi:10.1086/343847 · Cited by 239
“Since it is commonly assumed that the addition of a 1 2 baryonic component would cause the dark matter to adiabatically contract (Blumenthal et al. 1986) thereby exacerbating the observed discrepancy, the complications caused by the baryonic component are usually dismissed.”
BackgroundFermi LAT Search for Internal Bremsstrahlung Signatures from Dark Matter AnnihilationPreprint
Bringmann, T., Huang, X., Stefan, A. I., & Wenigerd, V. C. (2016) · Cited by 248
Sand, D. J., Treu, T., & Ellis, R. S. (2002) · The Astrophysical Journal · doi:10.1086/342530 · Cited by 206
A new method to quantify the effects of baryons on the matter power spectrum
Schneider, A., & Teyssier, R. (2015) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2015/12/049 · Cited by 253
“[23, 24] assumed shells of DM to contract due to the presence of the central galaxy while conserving angular momentum, i.”
BackgroundThe First Stars: Formation, Properties, and Impact
Klessen, R. S., & Glover, S. C. O. (2023) · Annual Review of Astronomy and Astrophysics · doi:10.1146/annurev-astro-071221-053453 · Cited by 282
Dynamical Blueprints for Galaxies
Widrow, L. M., Pym, B., & Dubinski, J. (2008) · The Astrophysical Journal · doi:10.1086/587636 · Cited by 216
“We have done this using the usual assumptions (Blumenthal et al. 1986; Flores et al. 1993); the system is treated as being spherically symmetric.”
MethodStar formation in semi-analytic galaxy formation models with multiphase gas
Somerville, R., Popping, G., & Trager, S. (2015) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stv1877 · Cited by 168
“…based on the initial angular momentum of the gas and the halo profile, assuming that angular momentum is conserved and that the self-gravity of the collapsing baryons causes contraction of the matter in the inner part of the halo (Blumenthal et al. 1986; Flores et al. 1993; Mo et al. 1998).”
BackgroundGamma Ray Signals from Dark Matter: Concepts, Status and ProspectsPreprint
Bringmann, T., & Weniger, C. (2016) · Cited by 207
Flat-cored Dark Matter in Cuspy Clusters of Galaxies
El‐Zant, A. A., Hoffman, Y., Primack, J. R., Combes, F., & Shlosman, I. (2004) · The Astrophysical Journal · doi:10.1086/421938 · Cited by 207
“The DM adiabatic compression induced by gaseous baryonic infall was used by Blumenthal et al. (1986), Flores et al. (1993), and Mo et al. (1998) to describe the effects on the DM distribution of baryon settling in virialized DM halos.”
MethodSelf-citationMacciò, A. V., Stinson, G. S., Brook, C. B., Wadsley, J. W., Couchman, H. M. P., Shen, S., Gibson, B. K., & Quinn, T. (2011) · The Astrophysical Journal Letters · doi:10.1088/2041-8205/744/1/l9 · Cited by 211
“This process is dubbed ‘adiabatic contraction’ (e.g. Blumenthal et al. 1986, Gnedin et al. 2004).”
MethodConstraining the Galaxy's dark halo with RAVE stars
Piffl, T., Binney, J. J., McMillan, P. J., Steinmetz, M., Helmi, A., Wyse, R. F. Ġ., Bienaymé, O., Bland‐Hawthorn, J., Freeman, K. C., Gibson, B. K., et al. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stu1948 · Cited by 198
“The classic halo response model of Blumenthal et al. (1986), which assumes an adiabatic contraction of the radial mass profile, is now thought to overpredict the response (e.g. Gnedin et al. 2004, 2010; Abadi et al. 2010).”
BackgroundMass distribution in galaxy clusters: the role of Active Galactic Nuclei feedback
Teyssier, R., Moore, B., Martizzi, D., Dubois, Y., & Mayer, L. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.18399.x · Cited by 206
“The effect of gas cooling on the dark halo has been interpreted in terms of adiabatic contraction (AC) of the particle orbits (Blumenthal et al. 1986; Gnedin et al. 2004), meaning that individual orbits are compressed inwards, while conserving the adiabatic invariant I = rM(<r).”
BackgroundMethodObservational evidence for primordial black holes: A positivist perspective
Carr, B. J., Clesse, S., García-Bellido, J., Hawkins, M. R. S., & Kühnel, F. (2024) · Physics Reports · doi:10.1016/j.physrep.2023.11.005 · Cited by 256
Dark matter and cosmic structure
Frenk, C., & White, S. D. M. (2012) · MPG.PuRe (Max Planck Society) · Cited by 198
Numerical simulations of the dark universe: State of the art and the next decade
Kuhlen, M., Vogelsberger, M., & Angulo, R. E. (2012) · Physics of the Dark Universe · doi:10.1016/j.dark.2012.10.002 · Cited by 222
“This adiabatic contraction effect was worked out analytically in [370] and its description has since been refined [371, 372].”
BackgroundEvolution of the atomic and molecular gas content of galaxies
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“…based on the initial angular momentum of the gas and the halo profile, assuming that angular momentum is conserved and that the self-gravity of the collapsing baryons causes contraction of the matter in the inner part of the halo (Blumenthal et al. 1986; Flores et al. 1993; Mo, Mao & White 1998).”
BackgroundDark Matter Profile in the Galactic Center
Gnedin, O. Y., & Primack, J. R. (2004) · Physical Review Letters · doi:10.1103/physrevlett.93.061302 · Cited by 229
Self-citationMaximum feedback and dark matter profiles of dwarf galaxies
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“This process can be described as adiabatic contraction (Blumenthal et al. 1986; Flores et al. 1993; Dalcanton et al. 1997), which we discuss at length in §3.1.”
BackgroundInfluentialDark Matter distribution in the Milky Way: microlensing and dynamical constraints
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“It is well established that baryonic physics alters the particulars of DM haloes and subhalo populations (e.g. Blumenthal et al. 1986; Tissera & Dominguez-Tenreiro 1998; Libeskind et al. 2010; Romano-Dı́az et al. 2010; di Cintio et al. 2011; Schewtschenko & Macciò 2011; Zemp et al. 2012), there…”
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“…radius residuals imposes strong constraints on the contribution of disk gravity to the rotation speed; disk gravity should cause more compact galaxies to rotate faster, and the impact of the disk on the inner halo profile (Blumenthal et al. 1986; Gnedin et al. 2004) should amplify this effect.”
BackgroundQuantifying baryon effects on the matter power spectrum and the weak lensing shear correlation
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“, riMi = rfMf , where Mi and Mf are the initial (dark-matter-only) and final (dark-matter-baryon) enclosed mass [29, 30].”
BackgroundThe Structure of Cold Dark Matter Halos
Navarro, J. F. (1996) · Springer eBooks · doi:10.1007/978-94-009-0229-9_38 · Cited by 244
Zitrin, A., Broadhurst, T. J., Umetsu, K., Coe, D., Benítez, N., Ascaso, B., Bradley, L., Ford, H., Jee, J., Medezinski, E., et al. (2009) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2009.14899.x · Cited by 185
Martinsson, T. P. K., Verheijen, M. A. W., Westfall, K. B., Bershady, M. A., Andersen, D. R., & Swaters, R. A. (2013) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201321390 · Cited by 195
“It is argued that the baryons in the disk will tend to contract the halo while it is forming (e.g., Blumenthal et al. 1986; Gnedin et al. 2004).”
BackgroundDuffy, A. R., Schaye, J., Kay, S. T., Vecchia, C. D., Battye, R. A., & Booth, C. M. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.16613.x · Cited by 186
“The adiabatic parameter considered in the first generation of adiabatic contraction models for collapsing haloes (Blumenthal et al. 1986) was the product of radius with the mass internal to this radius, M(< r)r. Gnedin et al. (2004), henceforth G04, found that such a simple scheme, only strictly…”
BackgroundMethodResultInfluentialChisari, N. E., Richardson, M. L. A., Devriendt, J., Dubois, Y., Schneider, A., Brun, A. M. C. L., Beckmann, R. S., Peirani, S., Slyz, A. D., & Pichon, C. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty2093 · Cited by 186
“The cause of the small scale enhancement is the additional cooling pro- duced by the presence of baryons, which leads to an adiabatic contraction of the matter distribution at these scales (Blumenthal et al. 1986).”
BackgroundAndreas Birkedal, A., Noble, A., Perelstein, M. E., & Spray, A. (2006) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.74.035002 · Cited by 220
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The Formation of Disk‐Bulge‐Halo Systems and the Origin of the Hubble Sequence
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“We follow Blumenthal et al. (1986) and Flores et al. (1993) and assume that the halo responds adiabatically to the slow assembly of the baryonic matter in disk and bulge, and that it remains spherical (see also Dalcanton et al. 1997 and Mo et al. 1998).”
BackgroundBaryonic pinching of galactic dark matter halos
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“To model this effect it is common to use adiabatic invariants or some small modification of them [7, 8, 9, 10, 11, 12, 13, 14, 15, 16].”
BackgroundMethodORBITING CIRCUMGALACTIC GAS AS A SIGNATURE OF COSMOLOGICAL ACCRETION
Stewart, K. R., Kaufmann, T., Bullock, J. S., et al. (2011) · The Astrophysical Journal · doi:10.1088/0004-637x/738/1/39 · Cited by 181
“There is long history of studies relying on spin parameter distributions derived from dissipationless simulations to predict disk sizes and bulge properties in galaxies (e.g., Fall & Efstathiou 1980; Blumenthal et al. 1986; Mo et al. 1998; Bullock et al. 2001).”
BackgroundDensity Profiles of Cold Dark Matter Substructure:Implications for the Missing Satellites Problem
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Gómez, F. A., Besla, G., Carpintero, D. D., Villalobos, Á., O’Shea, B. W., & Bell, E. F. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/802/2/128 · Cited by 177
“The dark matter halo has a total mass ofMvir = 1012 M⊙, a scale radiusrs = 26.47 kpc, and is initially adiabatically contracted to model its response to the formation of a stellar disc in its central region (Blumenthal et al. 1986; Mo et al. 1998).”
BackgroundInfluentialWIDE-FIELD PRECISION KINEMATICS OF THE M87 GLOBULAR CLUSTER SYSTEM
Strader, J., Romanowsky, A. J., Brodie, J. P., Spitler, L. R., Beasley, M. A., Arnold, J. A., Tamura, N., Sharples, R. M., & Arimoto, N. (2011) · The Astrophysical Journal Supplement Series · doi:10.1088/0067-0049/197/2/33 · Cited by 177
“Another possibility is that a process like adiabatic contraction has raised the central halo density (e.g., Blumenthal et al. 1986).”
BackgroundAn 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
“Note that our approach, and the exposition here, are closely based on the formalism presented in Blumenthal et al. (1986), Flores et al. (1993), and Mo et al. (1998, MMW98).”
MethodJet-regulated cooling catastrophe
Dubois, Y., Devriendt, J., Slyz, A. D., & Teyssier, R. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.17338.x · Cited by 173
“We attribute this to the domination of the mass budget by the stellar component which pulls DM along with it through adiabatic contraction (Blumenthal et al. 1986).”
BackgroundKochanek, C. S., Morgan, N. D., Falco, E. E., McLeod, B. A., Winn, J. N., Dembicky, J., & Ketzeback, B. (2006) · The Astrophysical Journal · doi:10.1086/499766 · Cited by 173
“…Halo Models In order to connect these models to theoretical expectations, we must relate the halo parameters to estimates from simulation and account for the changes in the dark matter distribution produced by the baryonic component known as ‘‘adiabatic compression’’ (Blumenthal et al. 1986).”
BackgroundTsuruta, S. (1998) · Physics Reports · doi:10.1016/s0370-1573(97)00041-0 · Cited by 174
Stellar and dynamical masses of ellipticals in the Sloan Digital Sky Survey
Padmanabhan, N., Seljak, U., Strauss, M. A., Blanton, M. R., Kauffmann, G., Schlegel, D. J., Tremonti, C., Bahcall, N. A., Bernardi, M., Brinkmann, J., et al. (2003) · New Astronomy · doi:10.1016/j.newast.2003.12.004 · Cited by 165
“…stars, and that the remaining matter (the dark matter mass fraction) is adiabatically compressed by the stellar matter following 2 See the Appendix for an explanation of why this is still justified for the Sersic profile fits that we use. c© 0000 RAS, MNRAS 000, 000–000 Blumenthal et al. (1986).”
BackgroundThe Disk and Dark Halo Mass of the Barred Galaxy NGC 4123. II. Fluid‐Dynamical Models
Weiner, B. J., Sellwood, J. A., & Williams, T. B. (2001) · The Astrophysical Journal · doi:10.1086/318289 · Cited by 169
“The formalism often used to model this collapse is known as the adiabatic-compression or circular-orbit approximation (see e.g. Faber 1981; Blumenthal et al. 1986).”
MethodSonnenfeld, A., Treu, T., Gavazzi, R., Marshall, P. J., Auger, M. W., Suyu, S. H., Koopmans, L. V. E., & Bolton, A. S. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/752/2/163 · Cited by 169
“This result is in qualitative agreement with many theoretical studies of the evolution of spheroidal galaxies (Blumenthal et al. 1986; Gnedin et al. 2004; Gustafsson et al. 2006; Abadi et al. 2010; Duffy et al. 2010).”
ResultThe Dark Matter Annihilation Signal from Galactic Substructure: Predictions forGLAST
Kuhlen, M., Diemand, J., & Madau, P. (2008) · The Astrophysical Journal · doi:10.1086/590337 · Cited by 191
“Adiabatic contraction (Blumenthal et al. 1986; Gnedin et al. 2004a) would lead to a steepening of the central DM density profile at scales of a few kpc and below.”
BackgroundAnalytic models of plausible gravitational lens potentials
Baltz, E. A., Marshall, P. J., & Oguri, M. (2009) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2009/01/015 · Cited by 182
“The broad isothermal region obtained by this prescription is illustrated in Figure 4. We note that adiabatic contraction [12, 13 , 14] modifies the NFW profile, leading to more centrally concentrated profile of dark matter.”
BackgroundMass discrepancies in galaxies: dark matter and alternatives
Sanders, R. H. (1990) · The Astronomy and Astrophysics Review · doi:10.1007/bf00873540 · Cited by 166
FORMING EARLY-TYPE GALAXIES IN ΛCDM SIMULATIONS. I. ASSEMBLY HISTORIES
Johansson, P. H., Naab, T., & Ostriker, J. P. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/754/2/115 · Cited by 166
“Initially, we see an increase in the central DM due to adiabatic contraction (Blumenthal et al. 1986; Gnedin et al. 2004) for all the galaxies with a peak central DM mass reached at z ∼ 3.”
BackgroundThomas, J., Saglia, R. P., Bender, R., et al. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.18725.x · Cited by 166
“Therefore, we first subtracted from the observed dark matter profile, ρDM,Krou, the expected effect of baryon contraction by assuming the adiabatic approximation (i.e. by inverting the equations of Blumenthal et al. 1986).”
MethodThe 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
DISENTANGLING BARYONS AND DARK MATTER IN THE SPIRAL GRAVITATIONAL LENS B1933+503
Suyu, S. H., Hensel, S. W., McKean, J. P., Fassnacht, C. D., Treu, T., Halkola, A., Norbury, M. A., Jackson, N. J., Schneider, P., Thompson, D., et al. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/750/1/10 · Cited by 163
“This “halo contraction” is also found in other studies (e.g., Blumenthal et al. 1986; Gnedin et al. 2004, 2011).”
ResultThe kinematic connection between galaxies and dark matter haloes
Dutton, A. A., Conroy, C., Bosch, F. C. V. D., Prada, F., & More, S. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.16911.x · Cited by 167
“Such high values of Vopt/V200 are naturally explained by the combined effects of baryons adding to the optical circular velocity directly, and indirectly by inducing contraction of the dark matter halo (Blumenthal et al. 1986).”
BackgroundThe abundance of (not just) dark matter haloes
Sawala, T., Frenk, C. S., Crain, R. A., Jenkins, A. R., Schaye, J., Theuns, T., & Zavala, J. (2013) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stt259 · Cited by 160
“The effect of baryons on the structure of haloes has been studied extensively, both using analytical models (e.g. Blumenthal et al. 1986; Sellwood & McGaugh 2005) and in numerical simulations (e.g. Abadi et al. 2010; Duffy et al. 2010; Bryan et al. 2012).”
MethodHooper, D., Kelso, C., & Queiroz, F. S. (2013) · Astroparticle Physics · doi:10.1016/j.astropartphys.2013.04.007 · Cited by 184
Gravitational probes of dark matter physics
Buckley, M. R., & Peter, A. H. G. (2018) · Physics Reports · doi:10.1016/j.physrep.2018.07.003 · Cited by 189
“Thus, halos appeared denser in hydrodynamic simulations than in dark-matter-only simulations [366, 367].”
BackgroundA NEW PROBE OF DARK MATTER AND HIGH-ENERGY UNIVERSE USING MICROLENSING
Ricotti, M., & Gould, A. P. (2009) · The Astrophysical Journal · doi:10.1088/0004-637x/707/2/979 · Cited by 166
“…of the dark matter particle orbits implies R[Mb(R) + Mh(R)] = RiMi(ri) = RiMh,i(R) 1 − F (11) which can be solved iteratively for the final dark matter mass distribution Mh(R), given the initial total mass distribution Mh,i(Ri) and the final baryon mass distribution Mb(R) (Blumenthal et al. 1986).”
BackgroundThe Cusp/Core Problem in Galactic Halos: Long-Slit Spectra for a Large Dwarf Galaxy Sample
Spekkens, K., Giovanelli, R., & Haynes, M. P. (2005) · The Astronomical Journal · doi:10.1086/429592 · Cited by 160
“7 do not take the impact of the baryon collapse on the halo shape into account, which tends to increase αint over the values determined from collisionless simulations (Blumenthal et al. 1986; Flores et al. 1993; Gnedin et al. 2004).”
BackgroundThe X‐Ray Concentration–Virial Mass Relation
Buote, D. A., Gastaldello, F., Humphrey, P. J., Zappacosta, L., Bullock, J. S., Brighenti, F., & Mathews, W. G. (2007) · The Astrophysical Journal · doi:10.1086/518684 · Cited by 156
“However, allowing for adiabatic contraction (e.g., Blumenthal et al. 1986; Gnedin et al. 2004) of the dark matter profile in most cases degrades the fits, suggesting a more complex interplay between the baryons and the dark matter (e.g., Loeb & Peebles 2003; El-Zant et al. 2004; Dutton et al. 2006).”
X-ray coronae in simulations of disc galaxy formation
Crain, R. A., McCarthy, I. G., Frenk, C. S., Theuns, T., & Schaye, J. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.16985.x · Cited by 155
“The density profile of galaxy haloes will be modified by the baryons cooling in the halo (e.g. Blumenthal et al. 1986; Jesseit et al. 2002; Gnedin et al. 2004; Abadi et al. 2009; Duffy et al. 2010).”
BackgroundA precise extragalactic test of General Relativity
Collett, T. E., Oldham, L. J., Smith, R. J., Auger, M. W., Westfall, K. B., Bacon, D., Nichol, R. C., Masters, K. L., Koyama, K., & van den Bosch, R. (2018) · Science · doi:10.1126/science.aao2469 · Cited by 157
A dark matter profile to model diverse feedback-induced core sizes of ΛCDM haloes
Lazar, A., Bullock, J. S., Boylan-Kolchin, M., Chan, T. K., Hopkins, P. F., Graus, A. S., Wetzel, A. R., El-Badry, K., Wheeler, C., Straight, M. C., et al. (2020) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/staa2101 · Cited by 193
“One way galaxy formation can affect dark matter is by boosting central dark matter densities as a result of baryons clustering at the centre of the halo (Blumenthal et al. 1986).”
BackgroundOn the orbits of infalling satellite haloes
Wetzel, A. R. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.17877.x · Cited by 159
“Since galaxies form at the centers of dark matter halos (White & Rees 1978; Blumenthal et al. 1986; Dubinski 1994; Mo et al. 1998), the dynamics of infalling satellite halos will also influence the evolution of the accompanying galaxy populations.”
BackgroundBaryons and weak lensing power spectra
White, M. J. (2004) · Astroparticle Physics · doi:10.1016/j.astropartphys.2004.06.001 · Cited by 155
“Adiabatic contraction conserves both the mass and the angular momentum of the cold baryons and dark matter particles (Blumenthal et al., 1986; Kochanek & White, 2001).”
BackgroundKazantzidis, S., Łokas, E. L., Callegari, S., et al. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/726/2/98 · Cited by 155
“We note that the Widrow & Dubinski (2005) method for building disk galaxies does not explicitly take into account the adiabatic contraction of the halo in response to the slow accumulation of the baryons (e.g., Blumenthal et al. 1986).”
MethodWhere are the most ancient stars in the Milky Way?
El-Badry, K., Bland‐Hawthorn, J., Wetzel, A. R., Quataert, E., Weisz, D. R., Boylan-Kolchin, M., Hopkins, P. F., Faucher‐Giguère, C., Kereš, D., & Garrison-Kimmel, S. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty1864 · Cited by 170
“After z ∼ 1, contraction of the potential due to continued accumulation of baryons at high density (e.g. Blumenthal et al. 1986) actually drives stars to migrate inwards, partially undoing outward migration at earlier times.”
Backgroundvan den Bosch, F. C. (2001) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2001.04861.x · Cited by 155
“Throughout we assume that the disk is infinitesimally thin, and each time step we use the adiabatic invariant formalism of Blumenthal et al. (1986) and Flores et al. (1993) to compute the gravitational contraction of the dark matter induced by the baryons settling in the disk.”
MethodSelf‐similar Models for the Mass Profiles of Early‐Type Lens Galaxies
Rusin, D., Kochanek, C. S., & Keeton, C. R. (2003) · The Astrophysical Journal · doi:10.1086/377356 · Cited by 153
“It is shown that adiabatic compression (e.g., Blumenthal et al. 1986) yields nearly flat rotation curves for a range of initial halo concentrations and cooled baryon fractions (see also Kochanek & White 2001 and Kochanek 2003), but typical CDM halos (e.g., Bullock et al. 2001) appear to be too…”
BackgroundThe angular momentum content of dwarf galaxies: new challenges for the theory of galaxy formation
van den Bosch, F. C., Burkert, A., & Swaters, R. A. (2001) · Monthly Notices of the Royal Astronomical Society · doi:10.1046/j.1365-8711.2001.04656.x · Cited by 150
“Blumenthal et al. (1986) and Flores et al. (1993) investigated how adiabatic contraction of dark matter haloes impacts on the rotation curves of disk galaxies.”
BackgroundMethodOn the physical origin of dark matter density profiles
Ascasibar, Y., Yepes, G., Gottlöber, S., et al. (2004) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2004.08005.x · Cited by 152
“…Manrique et al. 2003) argue that the central density profile is linked to the merging history of dark matter substructure, and baryons have been invoked both to flatten (e.g. El-Zant, Shlosman & Hoffman 2001; El-Zant et al. 2003) and to steepen (Blumenthal et al. 1986) the dark matter profile.”
BackgroundIs There Evidence for Flat Cores in the Halos of Dwarf Galaxies? The Case of NGC 3109 and NGC 6822
Valenzuela, O., Rhee, G., Klypin, A. A., et al. (2007) · The Astrophysical Journal · doi:10.1086/508674 · Cited by 152
“The models include a dark matter halo initially with the NFW density profile modified by the standard adiabatic contraction (Blumenthal et al. 1986).”
Method
Metadata
- Authors
- Blumenthal, G. R., Faber, S. M., Flores, R., & Primack, J. R.
- Venue
- The Astrophysical Journal
- Publisher
- American Astronomical Society
- Published
- 1986-02
- Volume
- 301
- Pages
- 27
- ISSN
- 0004-637X (ISSN-L)
- 1538-4357
- OpenAlex
- W2083950714
- Cited by
- 1,213
- References
- 0
- Citations by year
- 2026: 17 · 2025: 32 · 2024: 28 · 2023: 27 · 2022: 36 · 2021: 47 · 2020: 49 · 2019: 39 · 2018: 43 · 2017: 39 · 2016: 55 · 2015: 51 · 2014: 52 · 2013: 58 · 2012: 83
- FWCI
- 18.18
- Type
- journal article
- Language
- en
- Open access
- closed
- Locations
- The Astrophysical Journal (publishedVersion)
- 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, energy dissipation, halo cores, rotation curves, spiral galaxies, galaxy formation, protogalaxies, subclustering, tidal effects, anisotropic collapse
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