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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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Wegner, G., Corsini, E. M., Thomas, J., et al. (2012) · The Astronomical Journal · doi:10.1088/0004-6256/144/3/78 · Cited by 55
“Adiabatic contraction (Blumenthal et al. 1986), instead, is able to increase the amount of dark matter in the centers of ellipticals and to lower the required stellar masses toward a Kroupa IMF (see also Napolitano et al. 2011).”
BackgroundFirst star formation with dark matter annihilation
Ripamonti, E., Fabio Iocco, A., Ferrara, A., et al. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.16854.x · Cited by 55
“…– formally equivalent to the requirement that the angular momentum is conserved, condition that identifies the adiabatic invariant M(R)R (Blumenthal et al. 1986) – is that the orbital time of DM particles should be short with respect to the gravitational potential variation time…”
BackgroundMethodTRACING THE GAS TO THE VIRIAL RADIUS (R100) IN A FOSSIL GROUP
Humphrey, P. J., Buote, D. A., Brighenti, F., Flohic, H. M. L. G., Gastaldello, F., & Mathews, W. G. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/748/1/11 · Cited by 65
“…although less secure observationally (Humphrey et al. 2006; Gnedin et al. 2007; Napolitano et al. 2010), is so-called “adiabatic contraction” (Blumenthal et al. 1986; Gnedin et al. 2004; Abadi et al. 2009), where the DM halo density profile reacts to the gravitational influence of baryons…”
BackgroundCENTRAL MASS AND LUMINOSITY OF MILKY WAY SATELLITES IN THE Λ COLD DARK MATTER MODEL
Macciò, A. V., Kang, X., & Moore, B. (2009) · The Astrophysical Journal · doi:10.1088/0004-637x/692/2/l109 · Cited by 55
THE STRUCTURE OF GRAVITATIONALLY UNSTABLE GAS-RICH DISK GALAXIES
Aumer, M., Burkert, A. M., Johansson, P. H., et al. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/719/2/1230 · Cited by 55
“…matter plays an essential role, which is in agreement with the conclusions of Burkert et al. (2010), who concluded that adiabatic contraction (e.g. Blumenthal et al. 1986) of the halo due to baryonic infall is problematic, as it predicts halo spin parameters λ that are significantly higher than…”
ResultTHE PHYSICAL NATURE OF THE COSMIC ACCRETION OF BARYONS AND DARK MATTER INTO HALOS AND THEIR GALAXIES
Wetzel, A. R., & Nagai, D. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/808/1/40 · Cited by 56
“…gas collides, shocks, mixes, and eventually dissipates energy via radiative cooling, causing it to collapse to the minimum of a halo’s potential well and seed the formation of stars and galaxies (White & Rees 1978; Fall & Efstathiou 1980; Blumenthal et al. 1986; Dubinski 1994; Mo et al. 1998).”
BackgroundWeak annihilation cusp inside the dark matter spike about a black hole
Shapiro, S. L., & Shelton, J. (2016) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.93.123510 · Cited by 61
Dark matter contraction and stellar-mass-to-light ratio gradients in massive early-type galaxies
Oldham, L., & Auger, M. W. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty065 · Cited by 54
“That seven out of the ten EELs with well-constrained dark matter properties have inner halo slopes that are significantly steeper than NFW suggests that these haloes may have been strongly contracted due to the inital cooling and infall of baryons (Blumenthal et al. 1986; Gnedin et al. 2004).”
BackgroundDark Matter Scaling Relations And The Assembly Epoch Of Coma Early-Type Galaxies
Wegner, G. (2016) · Max Planck Digital Library · doi:10.15781/t23z6x · Cited by 55
Dynamical estimates of the local density of dark matter
Flores, R. A. (1988) · Physics Letters B · doi:10.1016/0370-2693(88)91073-8 · Cited by 55
Self-citationThe 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
“The question of how a dark matter halo will respond to the growth of mass in its center has been adressed by Blumenthal et al. (1986), hereafter B86.”
BackgroundSelf-consistent models of our Galaxy
Binney, J. J., & Vasiliev, E. (2023) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stad094 · Cited by 59
Cosmology in two dimensions: the concentration-mass relation for galaxy clusters
Giocoli, C., Meneghetti, M., Ettori, S., & Moscardini, L. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2012.21743.x · Cited by 54
“This phenomenology, acting on the dark matter component mainly in proximity of the host halo centre and known as adiabatic contraction (Blumenthal et al. 1986; Rix et al. 1997; Keeton 2001; Gnedin et al. 2011).”
BackgroundResultInelastic dark matter as an efficient fuel for compact stars
Hooper, D., Spolyar, D., Vallinotto, A., et al. (2010) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.81.103531 · Cited by 54
Quantifying astrophysical uncertainties on dark matter direct detection results
Fairbairn, M., Douce, T., & Swift, J. (2013) · Astroparticle Physics · doi:10.1016/j.astropartphys.2013.06.003 · Cited by 54
The Influence of Baryons on the Mass Distribution of Dark Matter Halos
Lin, W., Jing, Y. P., Mao, S., Gao, L., & McCarthy, I. G. (2006) · The Astrophysical Journal · doi:10.1086/508052 · Cited by 54
“For example, the baryons that condense toward the center of DM halos can compress DM by adiabatic contraction (Blumenthal et al. 1986; Mo et al. 1998).”
BackgroundTHE STELLAR STRUCTURE AND KINEMATICS OF DWARF SPHEROIDAL GALAXIES FORMED BY TIDAL STIRRING
Łokas, E. L., Kazantzidis, S., Klimentowski, J., et al. (2009) · The Astrophysical Journal · doi:10.1088/0004-637x/708/2/1032 · Cited by 53
COSMIC EVOLUTION OF VIRIAL AND STELLAR MASS IN MASSIVE EARLY-TYPE GALAXIES
Lagattuta, D. J., Fassnacht, C. D., Auger, M. W., et al. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/716/2/1579 · Cited by 53
“As a comparison, Jiang & Kochanek (2007) measure a ∼30% decrease in stellar M/L ratio by including the Blumenthal et al. (1986) AC model on a subsample of lower-redshift strong lenses, in good agreement with the results we see when we increase the inner slope of the NFW profile by ∼20%.”
BackgroundResultBars and Cold Dark Matter Halos
Colin, P., Valenzuela, O., & Klypin, A. (2006) · The Astrophysical Journal · doi:10.1086/503791 · Cited by 53
“Here we discuss halo density profiles within the context of adiabatic approximation models (e.g., Blumenthal et al. 1986; Ryden & Gunn 1987; Gnedin et al. 2004).”
BackgroundMethodKinematic deprojection and mass inversion of spherical systems of known velocity anisotropy
Mamon, G. A., & Boué, G. (2009) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2009.15817.x · Cited by 53
Precision cluster mass determination from weak lensing
Mandelbaum, R., Seljak, U., Baldauf, T., & Smith, R. C. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.16619.x · Cited by 52
“The effect of baryons on the cluster mass distribution is unclear, but may be significant in the inner cluster regions (Blumenthal et al. 1986; Gnedin et al. 2004; Naab et al. 2007; Rudd, Zentner & Kravtsov 2008; Zentner, Rudd & Hu 2008; Barkana & Loeb 2010).”
BackgroundBrennan, R., Pandya, V., Somerville, R. S., Barro, G., Bluck, A. F. L., Taylor, E. N., Wuyts, S., Bell, E. F., Dekel, A., Faber, S. M., et al. (2016) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stw2690 · Cited by 54
“We assume that angular momentum is conserved and that the self-gravity of the collapsing baryons causes the inner part of the halo to contract (Blumenthal et al. 1986; Flores et al. 1993; Mo, Mao & White 1998).”
BackgroundSelf-citationUnique Multimessenger Signal of QCD Axion Dark Matter
Edwards, T., Chianese, M., Kavanagh, B. J., Nissanke, S., & Weniger, C. (2020) · Physical Review Letters · doi:10.1103/physrevlett.124.161101 · Cited by 52
THE PHYSICAL NATURE OF THE COSMIC ACCRETION OF BARYONS AND DARK MATTER INTO HALOS AND THEIR GALAXIES
Wetzel, A., & Nagai, D. (2015) · eScholarship (California Digital Library) · Cited by 53
Lensing and the Centers of Distant Early‐Type Galaxies
Keeton, C. R. (2003) · The Astrophysical Journal · doi:10.1086/344539 · Cited by 53
The 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
Sonnenfeld, A., Leauthaud, A., Auger, M. W., Gavazzi, R., Treu, T., More, S., & Komiyama, Y. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty2262 · Cited by 54
Piña, P. E. M., Fraternali, F., Oosterloo, T. A., Adams, E. A. K., Teodoro, E. M. D., Bacchini, C., & Iorio, G. (2022) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stac1508 · Cited by 52
Humphrey, P. J., Buote, D. A., Brighenti, F., et al. (2009) · The Astrophysical Journal · doi:10.1088/0004-637x/703/2/1257 · Cited by 52
Alignment between Filaments and Galaxy Spins from the MaNGA Integral-field Survey
Krolewski, A., Ho, S., Chen, Y.-C., et al. (2019) · The Astrophysical Journal · doi:10.3847/1538-4357/ab1010 · Cited by 52
“Initially, the baryons and dark matter share the same angular momentum distribution and the baryons conserve angular momentum as they collapse, creating a rotation-supported disk (Fall & Efstathiou 1980; Blumenthal et al. 1986; Mo et al. 1998).”
BackgroundSeigar, M. S., Bullock, J. S., Barth, A. J., et al. (2006) · CERN Document Server (European Organization for Nuclear Research) · Cited by 52
Lensing and the Centers of Distant Early-Type Galaxies
Keeton, C. R. (2002) · CERN Document Server (European Organization for Nuclear Research) · Cited by 52
Direct versus indirect detection in mSUGRA with self-consistent halo models
Edsjö, J., Schelke, M., & Ullio, P. (2004) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2004/09/004 · Cited by 52
Collider and Dark Matter Searches in Models with Mixed Modulus-Anomaly Mediated SUSY BreakingPreprint
Baer, H., Park, E., Tata, X. R., et al. (2006) · Cited by 52
The Cusp/Core problem: supernovae feedback versus the baryonic clumps and dynamical friction model
Popolo, A. D., & Pace, F. (2016) · Astrophysics and Space Science · doi:10.1007/s10509-016-2742-z · Cited by 51
“…the model considers the effects of non-radial collapse originated by random angular momentum15, adiabatic contraction of DM that baryons produce (Blumenthal et al. 1986; Gnedin et al. 2004; Gustafsson et al. 2006), dynamical friction effects (e.g., El-Zant et al. 2001, 2004), random and ordered…”
BackgroundDetailed cluster mass and light profiles of A1703, A370 and RXJ1347−11 from deep Subaru imaging
Medezinski, E., Broadhurst, T. J., Umetsu, K., et al. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2010.16491.x · Cited by 51
“…of DM halos, clusters are observed to cool relatively inefficiently via thermal emission so that the gas remains close to the virial temperature, making cluster mass profiles easy to interpret, as corrections for gas cooling are not significant (Blumenthal et al. 1986; Broadhurst & Barkana 2008).”
Background2MASS photometry of edge-on spiral galaxies – I. Sample and general results
Mosenkov, A. V., Sotnikova, N. Y., & Решетников, В. П. (2009) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2009.15671.x · Cited by 51
“Kregel et al. (2005) argued that the analytical collapse model of disc galaxy formation (White & Rees 1978; Fall & Efstatiou 1980; Blumenthal et al. 1986; Mo, Mao & White 1998), the local Toomre’s (1964) stability criterion for a disc and the suggestion about vertical dynamical equilibrium,…”
BackgroundA unified solution to the small scale problems of the ΛCDM model
Popolo, A. D., Lima, J. A. S., Fabris, J. C., & Rodrigues, D. C. (2014) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2014/04/021 · Cited by 57
Dark matter indirect signatures
Lavalle, J., & Salati, P. (2012) · Comptes Rendus Physique · doi:10.1016/j.crhy.2012.05.001 · Cited by 44
“5 kpc from the GC), they fell short by 1 order of magnitude, which they argue could be compensated by a more spiky profile resulting from baryon cooling effects known as adiabatic contraction [120, 121, 122].”
BackgroundBellstedt, S., Forbes, D. A., Romanowsky, A. J., Remus, R., Stevens, A. R. H., Brodie, J. P., Poci, A., McDermid, R. M., Alabi, A., Chevalier, L., et al. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty456 · Cited by 51
“DM and stellar mass distributions have been found to interact with each other through processes such as dissipational collapse, in which the infall of baryonic matter compresses the DM halo (Blumenthal et al. 1986).”
BackgroundKinematic constraints on the stellar and dark matter content of spiral and S0 galaxies
Williams, M. J., Bureau, M., & Cappellari, M. (2009) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2009.15582.x · Cited by 51
“We refrain from including prescriptions for the effects of baryonic contraction on our halo model (e.g. Blumenthal et al. 1986; Gnedin et al. 2004; Abadi et al. 2009).”
MethodHow active galactic nucleus feedback and metal cooling shape cluster entropy profiles
Dubois, Y., Devriendt, J., Teyssier, R., et al. (2011) · Zurich Open Repository and Archive (University of Zurich) · doi:10.5167/uzh-54776 · Cited by 51
Cook, M., Lapi, A., & Granato, G. L. (2009) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2009.14962.x · Cited by 51
“In addition, for the sake of simplicity we disregard the influence of the baryons on the halo structure in terms of adiabatic contractions or expansions (see Blumenthal et al. 1986; Gnedin et al. 2004).”
BackgroundEffect of the Sun’s gravity on the distribution and detection of dark matter near the Earth
Griest, K. (1988) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.37.2703 · Cited by 51
Abazajian, K. N., & Harding, J. P. (2012) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2012/01/041 · Cited by 50
A Search for Dark Matter Annihilation with the Whipple 10 m Telescope
Wood, M., Blaylock, G., Bradbury, S. M., et al. (2008) · The Astrophysical Journal · doi:10.1086/529421 · Cited by 50
SELF-SIMILAR DYNAMICAL RELAXATION OF DARK MATTER HALOS IN AN EXPANDING UNIVERSE
Lapi, A., & Cavaliere, A. G. (2011) · The Astrophysical Journal · doi:10.1088/0004-637x/743/2/127 · Cited by 50
“On the other hand, some steepening of the inner density profile may be induced by any ‘adiabatic’ contraction of the diffuse star-forming baryons into a disc-like structure, as proposed by Blumenthal et al. (1986) and Mo, Mao & White (1998).”
BackgroundHydrodynamical simulations of galaxy clusters in dark energy cosmologies – II. c–M relation
Boni, C. D., Ettori, S., Dolag, K., & Moscardini, L. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sts235 · Cited by 49
Gravitational Lensing Statistics in Universes Dominated by Dark Energy
Kuhlen, M., Keeton, C. R., & Madau, P. (2004) · The Astrophysical Journal · doi:10.1086/380303 · Cited by 50
“On smaller, galaxy-mass scales (corresponding to of a few arcseconds), the test is complicated by the presence of cooled baryons; when baryons cool and condense into a galaxy, they modify the surrounding dark matter halo (e.g., Blumenthal et al. 1986).”
2MASS photometry of edge-on spiral galaxies. I. Sample and general resultsPreprint
Mosenkov, A. V., Sotnikova, N. Y., & Решетников, В. П. (2012) · Cited by 49
The impact of baryons on dark matter haloes
Pedrosa, S., Tissera, P. B., & Scannapieco, C. (2009) · Monthly Notices of the Royal Astronomical Society Letters · doi:10.1111/j.1745-3933.2009.00641.x · Cited by 48
The structural and photometric properties of early-type galaxies in hierarchical models
Almeida, C., Baugh, C. M., & Lacey, C. G. (2007) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2007.11530.x · Cited by 48
“New radii are computed for the disc and bulge by applying an adiabatic contraction of the disc, bulge and dark matter components (Blumenthal et al. 1986; Jesseit, Naab & Burkert 2002).”
MethodBaryonic imprints on DM haloes: population statistics from dwarf galaxies to galaxy clusters
Anbajagane, D., EVRARD, A. E., & Farahi, A. (2021) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stab3177 · Cited by 48
Bringing the Galaxy's dark halo to life
Piffl, T., Penoyre, Z., & Binney, J. J. (2015) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stv938 · Cited by 48
“4 show the profiles one obtains when one starts with the three isolated halos and applies to these objects the classic adiabatic contraction formalism of Blumenthal et al. (1986).”
BackgroundMethodInfluentialMixed neutralino dark matter in nonuniversal gaugino mass models
Chattopadhyay, U., Das, D., & Roy, D. P. (2009) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.79.095013 · Cited by 48
Cattaneo, A., Blaizot, J., Devriendt, J., Mamon, G. A., Tollet, É., Dekel, A., Guiderdoni, B., Kucukbas, M., & Thob, A. C. R. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx1597 · Cited by 47
“The models presented in this article neglect adiabatic contraction but we have made the experiment to run our default model with adiabatic contraction modeled as in Blumenthal et al. (1986).”
BackgroundMethodResolving the disc–halo degeneracy – I: a look at NGC 628
Aniyan, S., Freeman, K. C., Arnaboldi, M., Gerhard, O., Coccato, L., Fabricius, M., Kuijken, K. H., Merrifield, M. R., & Ponomareva, A. A. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty310 · Cited by 48
Blaña, M., Gerhard, O., Wegg, C., Portail, M., Opitsch, M., Saglia, R. P., Fabricius, M., Erwin, P., & Bender, R. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty2311 · Cited by 48
“2 kpcDM 200=1.88 × 1010 M in the most extreme case (Blumenthal et al. 1986), or a lower value of M3.”
BackgroundInfluentialThe 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
Baer, H., Mustafayev, A., Park, E.-K., et al. (2008) · Journal of High Energy Physics · doi:10.1088/1126-6708/2008/05/058 · Cited by 48
Cintio, A. D., Knebe, A., Libeskind, N. I., Brook, C. B., Yepes, G., Gottlöber, S., & Hoffman, Y. (2013) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stt240 · Cited by 47
“Di Cintio et al. (2011) showed that the inclusion of baryons has a twofold effect, inreasing or decreasing its central density according to an adiabatic contraction (Blumenthal et al. 1986) or outflows (Navarro et al.1996; Governato et al. 2012) model.”
BackgroundResultThe Impact of Baryonic Cooling on Giant Arc Abundances
Rozo, E., Nagai, D., Keeton, C. R., & Kravtsov, A. V. (2008) · The Astrophysical Journal · doi:10.1086/589955 · Cited by 47
H.E.S.S. OBSERVATIONS OF THE GLOBULAR CLUSTERS NGC 6388 AND M15 AND SEARCH FOR A DARK MATTER SIGNAL
Abramowski, A., Acero, F., Aharonian, F., et al. (2011) · The Astrophysical Journal · doi:10.1088/0004-637x/735/1/12 · Cited by 47
“This process is usually referred to as the adiabatic contraction (AC) model (Blumenthal et al. 1986; Zel’dovich et al. 1980; Jesseit et al. 2002; Gnedin et al. 2004; Prada et al. 2004).”
BackgroundWang, Y., Vogelsberger, M., Xu, D., Mao, S., Springel, V., Li, H., Barnes, D. J., Hernquist, L., Pillepich, A., Marinacci, F., et al. (2019) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stz3348 · Cited by 46
“Lovell et al. (2018) find that for ∼ 1012 M IllustrisTNG halos, adiabatic contraction (Blumenthal et al. 1986; Gnedin et al. 2004) is present from the inner most regions of the galaxies out to 20 kpc, whereas halo expansion at small radii for similar Illustris halos occur.”
BackgroundResultLudlow, A. D., Schaye, J., Schaller, M., & Bower, R. G. (2020) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/staa316 · Cited by 46
“For example, in the absence of feedback-driven outflows, the slow growth of a central galaxy may deepen the gravitational potential adiabatically, resulting in a contraction of DM in the innermost regions of a halo (Blumenthal et al. 1986).”
BackgroundKinematic constraints on the stellar and dark matter content of spiral and S0 galaxiesPreprint
Williams, M. J., & Bureau, M. (2009) · Cited by 47
Too small to succeed? Lighting up massive dark matter subhaloes of the Milky Way
Cintio, A. D., Knebe, A., Libeskind, N. I., Yepes, G., Gottlöber, S., & Hoffman, Y. (2011) · Monthly Notices of the Royal Astronomical Society Letters · doi:10.1111/j.1745-3933.2011.01123.x · Cited by 46
“Blumenthal et al. (1986) showed that dissipative baryons will lead directly to the adiabatic contraction of the halo increasing its central density, thus being a critical ingredient to determine subhalo properties.”
BackgroundSpatially Resolved Galaxy Star Formation and Its Environmental Dependence. I.
Welikala, N., Connolly, A. J., Hopkins, A., Scranton, R., & Conti, A. (2008) · The Astrophysical Journal · doi:10.1086/527666 · Cited by 46
“Today, a basic framework exists to describe the formation of galaxies from primordial fluctuations in the density field (White and Rees, 1978; Blumenthal et al., 1986; White and Frenk, 1991).”
BackgroundDISSIPATIONAL VERSUS DISSIPATIONLESS GALAXY FORMATION AND THE DARK MATTER CONTENT OF GALAXIES
Lackner, C. N., & Ostriker, J. P. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/712/1/88 · Cited by 48
“One such effect is the adiabatic contraction of DM by the slow addition of baryons to the center of the potential well (Blumenthal et al. 1986).”
BackgroundMethodGalaxies going MAD: the Galaxy-Finder Comparison Project
Knebe, A., Libeskind, N. I., Pearce, F. R., et al. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sts173 · Cited by 46
“…are plain and simple: while it is well established that baryonic physics alters the particulars of dark matter haloes and subhalo populations (Blumenthal et al. 1986; Tissera & Dominguez-Tenreiro 1998; Macciò et al. 2006; Oñorbe et al. 2007; Romano-Dı́az et al. 2008, 2009; Libeskind et al.…”
BackgroundCOLD DARK MATTER SUBSTRUCTURES IN EARLY-TYPE GALAXY HALOS
Fiacconi, D., Madau, P., Potter, D., & Stadel, J. (2016) · The Astrophysical Journal · doi:10.3847/0004-637x/824/2/144 · Cited by 52
“In response to the slow addition of baryons to the center, dark matter may be pulled in- wards through a process known as adiabatic contraction (Blumenthal et al. 1986; Gnedin et al. 2004; Pillepich et al. 2014).”
BackgroundLuminous satellites. II. Spatial distribution, luminosity function, and cosmic evolution
Nierenberg, A. M., Auger, M. W., Treu, T., Marshall, P. J., Fassnacht, C. D., & Busha, M. T. (2012) · Zurich Open Repository and Archive (University of Zurich) · doi:10.5167/uzh-70385 · Cited by 45
Gravitational Lens Time Delays in Cold Dark Matter
Kochanek, C. S. (2003) · The Astrophysical Journal · doi:10.1086/345342 · Cited by 46
“We use the adiabatic compression model (Blumenthal et al. 1986) to compute the changes in the dark matter distribution.”
BackgroundMethodInfluentialThe First Galaxies: Assembly Under Radiative Feedback From The First StarsPreprint
Bromm, V. (2016) · doi:10.15781/t2wv5n · Cited by 45
Baera, H., Mustafayev, A., Parka, E.-K., et al. (2006) · Cited by 46
Tan, C. Y., Shajib, A. J., Birrer, S., Sonnenfeld, A., Treu, T., Wells, P., Williams, D., Buckley‐Geer, E., Drlica-Wagner, A., & Frieman, J. A. (2024) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stae884 · Cited by 46
Shajib, A. J., Vernardos, G., Collett, T. E., Motta, V., Sluse, D., Williams, L. L. R., Saha, P., Birrer, S., Spiniello, C., & Treu, T. (2024) · Space Science Reviews · doi:10.1007/s11214-024-01105-x · Cited by 46
“However, numerical simulations find that dark matter does not fully respond to the baryonic infall according to the theoretical model of Blumenthal et al. (1986) (e.g., Gnedin et al., 2004; Abadi et al., 2010).”
BackgroundMethodInfluentialGrillo, C. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/722/1/779 · Cited by 46
“…second case, the gas radiates away its orbital and thermal energy and is responsible for the adiabatic contraction of the dark matter halo, i.e., for a central density profile steeper with respect to the initial distribution (e.g., Blumenthal et al. 1986; Jesseit et al. 2002; Gnedin et al. 2004).”
BackgroundThe nature of the ISM in galaxies during the star-formation activity peak of the Universe
Popping, G., Pérez-Beaupuits, J. P., Spaans, M., Trager, S. C., & Somerville, R. S. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stu1506 · Cited by 45
“…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).”
BackgroundCusps and cores in the presence of galactic bulges
Popolo, A. D., & Hiotelis, N. (2014) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2014/01/047 · Cited by 45
ON THE DISCREPANCY BETWEEN THEORETICAL AND X-RAY CONCENTRATION-MASS RELATIONS FOR GALAXY CLUSTERS
Rasia, E., Borgani, S., Ettori, S., Mazzotta, P., & Meneghetti, M. (2013) · The Astrophysical Journal · doi:10.1088/0004-637x/776/1/39 · Cited by 45
“The possibility that baryons might influence the structureformation process and, in particular, the DM distribution, was introduced almost three decades ago with the development of the analytic model of “adiabatic contraction” (Barnes & White 1984; Blumenthal et al. 1986; Ryden & Gunn 1987).”
BackgroundShallow dark matter cusps in galaxy clusters
Laporte, C. F. P., White, S. D. M., Naab, T., et al. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2012.21262.x · Cited by 45
“…galaxies and can alter the initial distribution of dark matter in numerous ways: through gas expulsion (Navarro et al. 1996), supernova driven impulsive heating (Pontzen & Governato 2011), AGN feedback (Duffy et al. 2010) or adiabatic contraction (Blumenthal et al. 1986; Gnedin et al. 2004, 2011).”
BackgroundMethodDabringhausen, J., Fellhauer, M., & Kroupa, P. (2010) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2009.16189.x · Cited by 45
“…Kormendy (1985) argues that these two populations mayactually be the same type of galaxies. c© 2009 RAS density in UCDs would be two orders of magnitude too low to explain their elevatedM/LV ratios, although adiabatic contraction (Blumenthal et al. 1986) may alleviate this problem (Murray 2009).”
BackgroundA novel 3D technique to study the kinematics of lensed galaxies
Rizzo, F., Vegetti, S., Fraternali, F., & Teodoro, E. M. D. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty2594 · Cited by 46
“E-mail: frizzo@mpa-garching.mpg.de within a galaxy (e.g. Blumenthal et al. 1986; Dutton et al. 2011; Courteau & Dutton 2015; Zolotov et al. 2015).”
BackgroundA lensed radio jet at milliarcsecond resolution I: Bayesian comparison of parametric lens models
Powell, D., Vegetti, S., McKean, J. P., Spingola, C., Stacey, H., & Fassnacht, C. D. (2022) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stac2350 · Cited by 44
Sharma, S., Steinmetz, M., & Bland‐Hawthorn, J. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/750/2/107 · Cited by 44
“The process is also accompanied by the adiabatic contraction of the dark matter halo (Blumenthal et al. 1986).”
BackgroundThe mass–concentration relation in massive galaxy clusters at redshift ∼1
Sereno, M., & Covone, G. (2013) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stt1086 · Cited by 44
“The DM component responds to the baryon sinking through an adiabatic contraction effect, leading to a further increase of the concentration (Blumenthal et al. 1986).”
BackgroundGalactic synchrotron emission from WIMPs at radio frequencies
Nicolao Fornengo, B., Lineros, R. A., Regis, M., & Marco Taoso, A. (2012) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2012/01/005 · Cited by 46
“In particular, the condensation of gas and stars can produce an adiabatic contraction of the DM halo, increasing the central DM density [37, 38].”
BackgroundHalo evolution in the presence of a disc bar
McMillan, P. J., & Dehnen, W. (2005) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2005.09516.x · Cited by 44
“…investigation of such processes have been undertaken, some pointing out effects that would increase the gradient of the density cusp still further (Blumenthal et al. 1986), some discussing processes that could p - tentially remove the cusp (Binney et al. 2001; El-Zant et al.2001; Weinberg & Katz…”
BackgroundThe Faber–Jackson relation and Fundamental Plane from halo abundance matching
Desmond, H., & Wechsler, R. H. (2016) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stw2804 · Cited by 42
“One possibility is for the DM to contract adiabatically (Blumenthal et al. 1986; Gnedin et al. 2004, 2011), but it is also possible for baryons to transfer energy to the halo and cause it to expand instead (e.g. Macciò et al. 2012; Di Cintio et al. 2014; Pontzen & Governato 2014).”
BackgroundCintio, A. D., Tremmel, M., Governato, F., Pontzen, A., Zavala, J., Fry, A. B., Brooks, A. M., & Vogelsberger, M. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx1043 · Cited by 45
“…inflows during the process of galaxy formation is to slowly drag dark matter toward the galaxy centre, in a process known as adiabatic contraction (Blumenthal et al. 1986; Gnedin et al. 2011), which renders the centre of dark matter haloes more concentrated than what is found in N-body only…”
BackgroundThe effect of baryons in the cosmological lensing PDFs
Castro, T., Quartin, M., Giocoli, C., Borgani, S., & Dolag, K. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty1117 · Cited by 44
“On the cores of these structures, luminous matter dynamics is indeed the main agent, acting through the interplay of halo contraction associated with cooling and expansion associated with feedback effects (Blumenthal et al. 1986; Keeton 2001; Gnedin et al. 2004).”
BackgroundGalaxy density profiles and shapes - II. Selection biases in strong lensing surveys
Mandelbaum, R., van de Ven, G., & Keeton, C. R. (2009) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2009.15166.x · Cited by 44
“In contrast, when going from γ dm = 1 without AC to including AC, the cross-section increases by a factor of ∼2.6 for the Blumenthal et al. (1986) prescription, or a factor of ∼2.0 for the Gnedin et al. (2004) prescription.”
BackgroundMethodInfluentialAdiabatic compression and indirect detection of supersymmetric dark matter
Mambrini, Y., Muñoz, C., Nezri, E., et al. (2006) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2006/01/010 · Cited by 44
“The present form of the adiabatic compression model was numerically and analytically studied by Blumental et al [43].”
MethodTesting adiabatic contraction of dark matter in fossil group candidates
Démoclès, J., Pratt, G. W., Pierini, D., Arnaud, M., Zibetti, S., & D’Onghia, E. (2010) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201014328 · Cited by 45
“Following the early work by Barnes & White (1984), Blumenthal et al. (1986) devised a simple formula to link the dark mass profiles before and after the assembly of a galaxy.”
MethodResultInfluentialBars and Cold Dark Matter HalosPreprint
Colín, P., Valenzuela, O., & Klypin, A. A. (2005) · Cited by 44
Katherine Freese, B. (2012) · Cited by 41
Review of Solutions to the Cusp-Core Problem of the ΛCDM Model
Popolo, A. D., & Delliou, M. L. (2021) · Galaxies · doi:10.3390/galaxies9040123 · Cited by 57
Formation of disc galaxies in preheated media: a preventative feedback model
Lu, Y., Mo, H. J., & Wechsler, R. H. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stu2215 · Cited by 43
“In our modeling, the effect of contraction of the dark matter halo due to disk formation (Blumenthal et al. 1986; Gnedin et al. 2004; Choi et al. 2006) is ignored.”
PURELY DRY MERGERS DO NOT EXPLAIN THE OBSERVED EVOLUTION OF MASSIVE EARLY-TYPE GALAXIES SINCEz∼ 1
Sonnenfeld, A., Nipoti, C., & Treu, T. (2014) · The Astrophysical Journal · doi:10.1088/0004-637x/786/2/89 · Cited by 43
“We calculate the response of the mass distribution of the galaxy to the infall of cold gas following the adiabatic contraction recipe of Blumenthal et al. (1986), which is stronger than more recent ones based on numerical simulations (e.g. Gnedin et al. 2004).”
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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