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Galaxy-induced transformation of dark matter haloes: Transformations of CDM haloes
Open accessAbstract
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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Citations
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
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).”
BackgroundThe two phases of galaxy formation
Oser, L., Ostriker, J., Naab, T., Johansson, P., & Burkert, A. (2010) · Max Planck Digital Library · Cited by 435
Portail, M., Gerhard, O., Wegg, C., & Ness, M. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stw2819 · Cited by 378
“In addition, since the inner part of dark matter halos is actually populated by baryons that collapse through dissipative processes, dark halos should contract, thus exacerbating any preexisting cusp (Blumenthal et al. 1986; Gnedin et al. 2004; Abadi et al. 2010).”
BackgroundFormation of Galaxy ClustersPreprint
Kravtsov, A. V., & Borgani, S. (2012) · Cited by 422
The milky way total mass profile as inferred from Gaia DR2
Cautun, M., Benítez-Llambay, A., Deason, A. J., Frenk, C. S., Fattahi, A., Gómez, F. A., Grand, R. J. J., Oman, K. A., Navarro, J. F., & Simpson, C. M. (2020) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/staa1017 · Cited by 332
“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).”
BackgroundMethodSelf-citationThe Milky Way total mass profile as inferred from Gaia DR2
Cautun, M., Benitez-Llambay, A., Deason, A. J., Frenk, C. S., Fattahi, A., Gómez, F. A., Grand, R. J. J., Oman, K. A., Navarro, J. F., & Simpson, C. M. (2019) · arXiv · doi:10.48550/arxiv.1911.04557 · Cited by 335
“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).”
BackgroundMethodSelf-citationThe RAVE survey: the Galactic escape speed and the mass of the Milky Way
Piffl, T., Scannapieco, C., Binney, J. J., Steinmetz, M., Scholz, R. ‐., Williams, M. E. K., de Jong, R. S., Kordopatis, G., Matijevič, G., Bienaymé, O., et al. (2013) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201322531 · Cited by 333
“In this approach the tension between the constraints coming from the circular speed at the solar radius, and the mass estimates at larger distances are likely to be resolved by an intermediate halo model as proposed by Abadi et al. (2010).”
BackgroundSelf-citationCourteau, S., Cappellari, M., de Jong, R. S., Dutton, A. A., Emsellem, É., Hoekstra, H., Koopmans, L. V. E., Mamon, G. A., Maraston, C., Treu, T., et al. (2014) · Reviews of Modern Physics · doi:10.1103/revmodphys.86.47 · Cited by 310
“The halo inner logarithmic slope is allowed to vary from the values predicted by halo contraction models (Abadi et al. 2010) to the nearly constant density profiles expected from halo expansion models (Pontzen & Governato 2012).”
BackgroundMethodInfluentialNewman, A. B., Treu, T., Ellis, R. S., Sand, D. J., Nipoti, C., Richard, J., & Jullo, E. (2013) · The Astrophysical Journal · doi:10.1088/0004-637x/765/1/24 · Cited by 287
“…modify the structure of the DM. Cooling allows baryons to condense toward the center, which makes the DM more concentrated (Blumenthal et al. 1986; Gnedin et al. 2004; Sellwood & McGaugh 2005; Gustafsson et al. 2006; Pedrosa et al. 2009; Abadi et al. 2010; Sommer-Larsen & Limousin 2010).”
BackgroundIbata, R., Lewis, G. F., McConnachie, A. W., Martin, N. F., Irwin, M. J., Ferguson, A. M. N., Babul, A., Bernard, E. J., Chapman, S. C., Collins, M., et al. (2013) · The Astrophysical Journal · doi:10.1088/0004-637x/780/2/128 · Cited by 269
“However, these triaxial structures become approximately oblate when baryonic physics is included in the simulations (see, e.g. Abadi et al. 2010), with c/a ∼ 0.8, c/b ∼ 0.9 for the dark matter component, at a radial distance corresponding to ∼ 30 kpc in M31 (Zemp et al. 2012, see their Figure 11).”
BackgroundInfluentialSelf-citationBarnabè, M., Czoske, O., Koopmans, L. V. E., Treu, T., & Bolton, A. S. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.18842.x · Cited by 243
van 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
Auger, 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
“…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 result in cored profiles (e.g., El-Zant et al. 2004; Nipoti et al. 2004).”
BackgroundSUBSTRUCTURE DEPLETION IN THE MILKY WAY HALO BY THE DISK
D’Onghia, E., Springel, V., Hernquist, L., & Kereš, D. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/709/2/1138 · Cited by 221
“2008; Abadi et al. 2009).”
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
“[25, 26] showed that a better agreement with numerical simulations is obtained if the slightly modified relation”
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
“If one defines the initial radius of each dark matter shell as ri and its final, adiabatically contracted value rf , Abadi et al. (2009) have proposed to capture Gnedin et al. (2004) model using the following simplified model: rf ri = 1 + α ( Mi Mf − 1 ) with α 0.68.”
MethodInfluentialBois, M., Emsellem, É., Bournaud, F., Alatalo, K., Blitz, L., Bureau, M., Cappellari, M., Davies, R. L., Davis, T. A., de Zeeuw, P. T., et al. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.19113.x · Cited by 205
“…should be much more frequent than major mergers and are therefore expected (see e.g. Khochfar & Silk 2006; Naab et al. 2007; Bournaud, Jog & Combes 2007; Genel et al. 2008, 2010; Naab, Johansson & Ostriker 2009; Hopkins et al. 2010; Oser et al. 2010; Qu et al. 2010; Abadi et al. 2010, CDM models).”
BackgroundTHE SHAPE OF THE INNER MILKY WAY HALO FROM OBSERVATIONS OF THE PAL 5 AND GD–1 STELLAR STREAMS
Bovy, J., Bahmanyar, A., Fritz, T. K., & Kallivayalil, N. (2016) · The Astrophysical Journal · doi:10.3847/1538-4357/833/1/31 · Cited by 208
“…of a galactic baryonic disk causes the halos to become more axisymmetric and aligned with the disk, but the minor-to-major axis ratio c/a changes only by a few tenths to c/a ≈ 0.7 to 0.8 (Dubinski 1994; Gustafsson et al. 2006; Debattista et al. 2008; Abadi et al. 2010; Kazantzidis et al. 2010).”
BackgroundInfluentialQuantifying baryon effects on the matter power spectrum and the weak lensing shear correlation
Schneider, A., Teyssier, R., Stadel, J., Chisari, N., Brun, A. L., Amara, A., & Réfrégier, A. (2018) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2019/03/020 · Cited by 142
“[33] found best agreement with simulations for the values of a = 0.”
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
“It is obviously sensible to take the fullest possible advantage of existing constraints on the Galaxy’s mass distribution when selecting mass models.”
BackgroundMethodResultInfluentialSelf-citationNumerical 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
The impact of galaxy formation on the total mass, mass profile and abundance of haloes
Velliscig, M., van Daalen, M. P., Schaye, J., McCarthy, I. G., Cacciato, M., Brun, A. M. C. L., & Vecchia, C. D. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stu1044 · Cited by 176
“…Gustafsson, Fairbairn & Sommer-Larsen 2006; Duffy et al. 2010; Tissera et al. 2010), spins (e.g. Bett et al. 2010; Bryan et al. 2013), shapes (e.g. Abadi et al. 2010; Kazantzidis et al. 2004; Read et al. 2008; Bryan et al. 2012, 2013), and substructure (e.g. Dolag et al. 2009; Romano-Dı́az et al.…”
BackgroundSonnenfeld, 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 shape of dark matter haloes in the Aquarius simulations: evolution and memory
Vera-Ciro, C. A., Sales, L. V., Helmi, A., Frenk, C. S., Navarro, J. F., Springel, V., Vogelsberger, M., & White, S. D. M. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.19134.x · Cited by 171
“However, the work of Tissera et al. (2010); Abadi et al. (2010); Bett et al. (2010) shows that even though the halo axis ratios c© 2011 RAS, MNRAS 000, 1–11 increase when a disc is formed (i.e. they become rounder), the trends with radius appear to be preserved.”
BackgroundSelf-citationGalaxy Alignments: Theory, Modelling & Simulations
Kiessling, A., Cacciato, M., Joachimi, B., Kirk, D., Kitching, T., Leonard, A., Mandelbaum, R., Schäfer, B. M., Sifón, C., Brown, M. D., et al. (2015) · Space Science Reviews · doi:10.1007/s11214-015-0203-6 · Cited by 181
“2006; Abadi et al. 2010; Deason et al. 2011). However, since these studies used different sized haloes or simulations that had different feedback effects, it is difficult to make direct comparisons. For example Kazantzidis et al. (2004) ran Adaptive Refinement Tree N -body + hydrodynamic simulations of cluster sized h…”
BackgroundMethodResultInfluentialDark halo response and the stellar initial mass function in early-type and late-type galaxies
Dutton, A. A., Conroy, C., van den Bosch, F. C., Simard, L., Mendel, J. T., Courteau, S., Dekel, A., More, S., & Prada, F. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.19038.x · 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
“Simulations with baryons find that the central galaxy tends to make the triaxial halo essentially oblate and less flattened (e.g., Abadi et al. 2010).”
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).”
MethodA 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
Burkert, A. M., Genzel, R., Bouché, N., Cresci, G., Khochfar, S., Sommer‐Larsen, J., Sternberg, A., Naab, T., Schreiber, N. M. F., Tacconi, L. J., et al. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/725/2/2324 · Cited by 153
Martizzi, D., Teyssier, R., Moore, B., & Wentz, T. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2012.20879.x · Cited by 152
“We compare the results of our hydrodynamical runs at z = 0 with the prediction of a simple adiabatic contraction model used by Abadi et al. (2010), and already adopted in Teyssier et al. (2011); details of this model can be found in Appendix A.”
MethodThe dark matter haloes of dwarf galaxies: a challenge for the Λ cold dark matter paradigm?
Ferrero, I., Abadi, M. G., Navarro, J. F., Sales, L. V., & Gurovich, S. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2012.21623.x · Cited by 158
“…is not the case for SDIG, whose paltry peak rotation speed is just Vout ∼ 19 km/s, well below the V Pout ∼ 30 km/s expected at the outermost radius, rout = 1.3 kpc. ‡ The prediction assumes an NFW halo contracted to account for the effect of the baryonic component following Abadi et al. (2010).”
BackgroundInfluentialSelf-citationReyes, R., Mandelbaum, R., Gunn, J. E., Nakajima, R., Seljak, U., & Hirata, C. M. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2012.21472.x · Cited by 146
“…literature, both from the theoretical (Gnedin et al. 2004; Gustafsson et al. 2006; Romano-Dı́az et al. 2008; Johansson et al. 2009; Duffy et al. 2010; Abadi et al. 2010; Pedrosa et al. 2010; Tissera et al. 2010; Governato et al. 2010; Guedes et al. 2011; Gnedin et al. 2011) and observational sides…”
BackgroundPeirani, S., Dubois, Y., Volonteri, M., Devriendt, J., Bundy, K. A., Silk, J. I., Pichon, C., Kaviraj, S., Gavazzi, R., & Habouzit, M. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx2099 · Cited by 145
“…to a steepening of the DM density profile of DM haloes due to adiabatic contraction (Blumenthal et al. 1986; Gnedin et al. 2004), in agreement with previous works (e.g., Gustafsson et al. 2006; Romano-Díaz et al. 2008 Abadi et al. 2010; Pedrosa et al. 2010; Tissera et al. 2010; Duffy et al. 2010).”
ResultThe impact of baryons on the spins and shapes of dark matter haloes
Bryan, S., Kay, S. T., Duffy, A. R., Schaye, J., Vecchia, C. D., & Booth, C. M. (2013) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sts587 · Cited by 141
“…tends to increase the central angular momentum of the halo (see for example, Sharma & Steinmetz 2005; Tonini et al. 2006a; Kaufmann et al. 2007; Abadi et al. 2010; Bett et al. 2010) and to make the halo more spherical or axisymmetric (see, for example, Katz & Gunn 1991; Dubinski 1994; Evrard…”
BackgroundThe shape of the Galactic halo with Gaia DR2 RR Lyrae. Anatomy of an ancient major merger
Iorio, G., & Belokurov, V. (2019) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty2806 · Cited by 139
“Note however, that inclusion of baryons (see e.g. Kazantzidis et al. 2004; Gnedin et al. 2004; Debattista et al. 2008; Abadi et al. 2010) or adaptation of a different Dark Matter model (e.g. Avila-Reese et al. 2001; ? giorio@ast.cam.ac.uk † vasily@ast.cam.ac.uk Davé et al. 2001; Mayer et al. 2002;…”
BackgroundTHE DISTRIBUTION OF DARK MATTER OVER THREE DECADES IN RADIUS IN THE LENSING CLUSTER ABELL 611
Newman, A. B., Treu, T., Ellis, R. S., Sand, D. J., Richard, J., Marshall, P. J., Capak, P. L., & Miyazaki, S. (2009) · The Astrophysical Journal · doi:10.1088/0004-637x/706/2/1078 · Cited by 136
“High-resolution, cosmological N -body + gas dynamical simulations of galaxy clusters (Gnedin et al. 2004) and galaxies (Gustafsson et al. 2006; Abadi et al. 2009, but see Romano-Dı́az et al. 2008) have shown that as baryons condense in the center, they deepen the potential and steepen the dark…”
BackgroundNewman, A. B., Treu, T., Ellis, R. S., & Sand, D. J. (2011) · The Astrophysical Journal Letters · doi:10.1088/2041-8205/728/2/l39 · Cited by 122
“…because simulated DM halos are much more flattened (〈c/a〉 ≃ 0.5, Jing & Suto 2002) than stars in elliptical galaxies (〈c/a〉 ≃ 0.7, Tremblay & Merritt 1995), and because isotropic dissipation processes in the baryon-dominated regime should yield rounder mass distributions (e.g., Abadi et al. 2010).”
BackgroundInfluentialBois, M., Emsellem, É., Bournaud, F., Alatalo, K., Blitz, L., Bureau, M., Cappellari, M., Davies, R. L., Davis, T. A., de Zeeuw, P. T., et al. (2011) · Cited by 126
Mismatch and misalignment: dark haloes and satellites of disc galaxies
Deason, A. J., McCarthy, I. G., Font, A. S., Evans, N. W., Frenk, C. S., Belokurov, V., Libeskind, N. I., Crain, R. A., & Theuns, T. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.18884.x · Cited by 123
“Abadi et al. (2010) employ galaxy models which include radiative gas cooling but neglect the contribution from stellar feedback.”
BackgroundMethodShajib, A. J., Treu, T., Birrer, S., & Sonnenfeld, A. (2021) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stab536 · Cited by 122
Oguri, M., Rusu, C. E., & Falco, E. E. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stu106 · Cited by 121
“For instance, the dark matter distribution is often assumed to follow the NFW profile or the NFW profile modified by the so-called adiabatic contraction (Blumenthal et al. 1986; Gnedin et al. 2004; Abadi et al. 2010).”
BackgroundORBITAL STRUCTURE OF MERGER REMNANTS. I. EFFECT OF GAS FRACTION IN PURE DISK MERGERS
Hoffman, L., Cox, T. J., Dutta, S. N., & Hernquist, L. (2010) · The Astrophysical Journal · doi:10.1088/0004-637x/723/1/818 · Cited by 121
“See also Dubinski (1994); Kazantzidis et al. (2004); Debattista et al. (2008); Valluri et al. (2010); Abadi et al. (2010); and Romano-Diaz et al. (2009), who studied halo shapes in a cosmological context and found that the response of the DM to baryonic condensation into galaxies drives the halos…”
BackgroundShape of dark matter haloes in the Illustris simulation: effects of baryons
Chua, K. T. E., Pillepich, A., Vogelsberger, M., & Hernquist, L. (2019) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty3531 · Cited by 120
“This similarity occurs despite the absence of stellar and AGN feedback in Abadi et al. (2010), which accentuates the effect of baryons.”
BackgroundResultInfluentialAN INVENTORY OF THE STELLAR INITIAL MASS FUNCTION IN EARLY-TYPE GALAXIES
Tortora, C., Romanowsky, A. J., & Napolitano, N. R. (2013) · The Astrophysical Journal · doi:10.1088/0004-637x/765/1/8 · Cited by 115
“We explore the sensitivity of our results to these assumptions by doing the analyses with the following alternatives: a) AC recipes of varying strengths (Blumenthal et al. 1986, B+86; Abadi et al. 2010, A+10); b) Mvir with a fixed value for the entire sample: Mvir = 10 12M⊙, 10 13M⊙, or 10 14M⊙; c) WMAP3based cvir–Mvi…”
MethodInfluentialWeighing the local dark matter with RAVE red clump stars
Bienaymé, O., Famaey, B., Siebert, A., Freeman, K. C., Gibson, B. K., Gilmore, G., Grebel, E. K., Bland-Hawthorn, J., Kordopatis, G., Munari, U., et al. (2014) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201424478 · Cited by 112
“Previous determinations indicated that there was less dark matter mass than predicted by cosmological simulations within R0 (Navarro & Steinmetz 2000; Binney et al. 2000; Famaey & Binney 2005; Abadi et al. 2010), whilst our determination would imply that there is more dark matter mass inside R0.”
BackgroundSelf-citationDutton, A. A., & Treu, T. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stt2489 · Cited by 110
Non-Abelian dark matter: Models and constraints
Chen, F., Cline, J. M., & Frey, A. R. (2009) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.80.083516 · Cited by 108
Baryonic clues to the puzzling diversity of dwarf galaxy rotation curves
Santos-Santos, I., Navarro, J. F., Robertson, A., Benítez-Llambay, A., Oman, K. A., Lovell, M. R., Frenk, C. S., Ludlow, A. D., Fattahi, A., & Adam Ritz, A. (2020) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/staa1072 · Cited by 107
Self-citationTHE SLOAN LENS ACS SURVEY. XII. EXTENDING STRONG LENSING TO LOWER MASSES
Shu, Y., Bolton, A. S., Brownstein, J. R., Montero-Dorta, A. D., Koopmans, L. V. E., Treu, T., Gavazzi, R., Auger, M. W., Czoske, O., Marshall, P. J., et al. (2015) · The Astrophysical Journal · doi:10.1088/0004-637x/803/2/71 · Cited by 107
“Gas cooling permits baryons to condense in the central regions of galaxies, and therefore it is believed to make the mass distribution more centrally concentrated (e.g. Gnedin et al. 2004; Gustafsson et al. 2006; Abadi et al. 2010; Velliscig et al. 2014).”
BackgroundThe gravitational force field of the Galaxy measured from the kinematics of RR Lyrae in Gaia
Wegg, C., Gerhard, O., & Bieth, M. (2019) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stz572 · Cited by 104
“Dissipation in baryonic simulations can make the highly triaxial halos seen in dark matter only simulations more spherical (Dubinski 1994; Kazantzidis et al. 2004; Debattista et al. 2008; Kazantzidis et al. 2010; Abadi et al. 2010).”
BackgroundDutton, A. A., Macciò, A. V., Mendel, J. T., & Simard, L. (2013) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stt608 · Cited by 103
“…contraction (Blumenthal et al. 1986) corresponds to ν = 1, the contraction model of Gnedin et al. (2004) can be approximated with ν ≃ 0.8, the contraction model of Abadi et al. (2010) can be approximated with ν ≃ 0.4, an unmodified halo corresponds to ν = 0, while expansion corresponds to ν < 0.”
BackgroundMethodInfluentialTHE DISTRIBUTION OF DARK MATTER IN THE MILKY WAY’S DISK
Pillepich, A., Kuhlen, M., Guedes, J., & Madau, P. (2014) · The Astrophysical Journal · doi:10.1088/0004-637x/784/2/161 · Cited by 103
Barnabè, M., Dutton, A. A., Marshall, P. J., Auger, M. W., Brewer, B. J., Treu, T., Bolton, A. S., Koo, D. C., & Koopmans, L. V. E. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2012.20934.x · Cited by 101
“Recent numerical work(see, e.g., Abadi et al. 2010; Tissera et al. 2010) has shown that including the contribution of the baryons has the effect of modifying the overall profile of the dark halo, which flattens to a more axisymmetric and oblate shape, with an average axial ratio of order 0.85−0.95,…”
BackgroundResultInfluentialvan Daalen, M. P., Schaye, J., McCarthy, I. G., Booth, C. M., & Vecchia, C. D. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stu482 · Cited by 100
“…processes associated with them have been shown to significantly impact, for example, the mass profiles (e.g. Gnedin et al. 2004, Duffy et al. 2010, Abadi et al. 2010, Governato et al. 2012, Martizzi et al. 2012, Velliscig et al. 2014) and shapes of haloes (e.g. Kazantzidis et al. 2004, Tissera et…”
BackgroundYuan, S., Garrison, L. H., Hadzhiyska, B., Bose, S., & Eisenstein, D. J. (2021) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stab3355 · Cited by 99
Ando, S., & Nagai, D. (2012) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2012/07/017 · Cited by 94
Aricò, G., Angulo, R. E., Hernández-Monteagudo, C., Contreras, S., Zennaro, M., Pellejero-Ibáñez, M., & Rosas-Guevara, Y. (2020) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/staa1478 · Cited by 92
Weighing the local dark matter with RAVE red clump stars
Bienaymé, O., Famaey, B., Siebert, A., Freeman, K. C., Gibson, B. K., Gilmore, G. F., Grebel, E. K., Bland‐Hawthorn, J., Kordopatis, G., Munari, U., et al. (2014) · Springer Link (Chiba Institute of Technology) · doi:10.1051/0004-6361/201424478/pdf · Cited by 93
Self-citationSurface photometry of brightest cluster galaxies and intracluster stars in ΛCDM
Cooper, A. P., Gao, L., Guo, Q., Frenk, C. S., Jenkins, A. R., Springel, V., & White, S. D. M. (2015) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stv1042 · Cited by 92
“However, recent work predicts only mild contraction for star formation efficiencies compatible with observations (Dutton et al. 2007; Abadi et al. 2010; Schaller et al. 2014) and also a counteracting expansion due to feedback (Navarro, Eke & Frenk 1996; Pontzen & Governato 2012).”
ResultBaryonic effects for weak lensing. Part I. Power spectrum and covariance matrix
Schneider, A., Stoira, N., Réfrégier, A., Weiss, A., Knabenhans, M., Stadel, J., & Teyssier, R. (2019) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2020/04/019 · Cited by 46
Emulation of baryonic effects on the matter power spectrum and constraints from galaxy cluster data
Giri, S. K., & Schneider, A. (2021) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2021/12/046 · Cited by 88
Dutton, A. A., Brewer, B. J., Marshall, P. J., Auger, M. W., Treu, T., Koo, D. C., Bolton, A. S., Holden, B. P., & Koopmans, L. V. E. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.18706.x · Cited by 86
“CDM haloes are also found to be more prolate at smaller radii (Allgood et al. 2006; Macciò et al. 2008; Abadi et al. 2010).”
BackgroundInfluentialConsistent scenarios for cosmic-ray excesses from Sommerfeld-enhanced dark matter annihilation
Finkbeiner, D. P., Goodenough, L., Slatyer, T. R., Vogelsberger, M., & Weiner, N. (2011) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2011/05/002 · Cited by 85
Mismatch and misalignment: dark haloes and satellites of disc galaxiesPreprint
Deason, A. J., McCarthy, I. G., Font, A. S., Evans, N. W., Frenk, C. S., Belokurov, V. A., Libeskind, N. I., Crain, R. A., & Theuns, T. (2011) · doi:10.17863/cam.24105 · Cited by 85
Dutton, A. A., Treu, T., Brewer, B. J., Marshall, P. J., Auger, M. W., Barnabè, M., Koo, D. C., Bolton, A. S., & Koopmans, L. V. E. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sts262 · Cited by 83
“…simulations of galaxy formation often find much weaker contraction than predicted by the adiabatic contraction formalism (Johansson et al. 2009; Abadi et al. 2010; Tissera et al. 2010) or even expansion (Governato et al. 2010; Macciò et al. 2012), and thus we do not actually expect adiabatic…”
BackgroundMethodInfluentialMartinez, G. D., Bullock, J. S., Kaplinghat, M., Strigari, L. E., & Trotta, R. (2012) · Cited by 82
The first all-sky view of the Milky Way stellar halo with Gaia+2MASS RR Lyrae
Iorio, G., Belokurov, V. A., Erkal, D., Koposov, S. E., Nipoti, C., & Fraternali, F. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx2819 · Cited by 81
“…both for the dynamical inference of the shape of the DM halo (see e.g. Williams & Evans 2015b; Bowden et al. 2016) and for our understanding of the response of the DM distribution to the presence of baryons (see Kazantzidis et al. 2004; Gnedin et al. 2004; Duffy et al. 2010; Abadi et al. 2010).”
BackgroundButsky, I. S., Macciò, A. V., Dutton, A. A., Wang, L., Obreja, A., Stinson, G. S., Penzo, C., Kang, X., Keller, B., & Wadsley, J. W. (2016) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stw1688 · Cited by 81
“…either plagued by the so called overcooling problem (which produced galaxies that were unrealistically dominated by baryons in their central region Kazantzidis et al. 2004) or were missing important aspects of the galaxy formation process such as star formation and feedback (Abadi et al. 2010).”
BackgroundDisentangling 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) · University of North Texas Digital Library (University of North Texas) · Cited by 81
Dark matter direct detection signals inferred from a cosmological N-body simulation with baryons
Ling, F.-S., Nezri, E., Athanassoula, E., & Teyssier, R. (2010) · Zurich Open Repository and Archive (University of Zurich) · doi:10.5167/uzh-34435 · Cited by 80
A CENSUS OF BARYONS AND DARK MATTER IN AN ISOLATED, MILKY WAY SIZED ELLIPTICAL GALAXY
Humphrey, P. J., Buote, D. A., CANIZARES, C. R., Fabian, A. C., & Miller, J. M. (2011) · The Astrophysical Journal · doi:10.1088/0004-637x/729/1/53 · Cited by 77
The impact of baryonic discs on the shapes and profiles of self-interacting dark matter haloes
Sameie, O., Creasey, P. E., Yu, H.-B., Sales, L. V., Vogelsberger, M., & Zavala, J. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty1516 · Cited by 80
“However, baryons can make the CDM halo shapes more spherical (red) (see also, Dubinski 1994; Debattista et al. 2008; Kazantzidis et al. 2010; Abadi et al. 2010; Tissera et al. 2010), an effect partially attributed to the change of orbits from boxy to tube or rounder loop as a result of the central…”
BackgroundThe density and pseudo-phase-space density profiles of cold dark matter haloes
Ludlow, A. D., Navarro, J. F., White, S. D. M., Boylan-Kolchin, M., Springel, V., Jenkins, A., & Frenk, C. S. (2011) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.19008.x · Cited by 76
Self-citationWegg, C., Gerhard, O., & Portail, M. (2016) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stw1954 · Cited by 78
“Contracting a halo with c200 = 15., towards the upper end of the cosmological values, with the prescription of Abadi et al. (2010) results in rotation curves just consistent with the microlensing results here.”
MethodResultInfluentialNapolitano, N. R., Romanowsky, A. J., & Tortora, C. (2010) · Zurich Open Repository and Archive (University of Zurich) · doi:10.5167/uzh-41864 · Cited by 74
EFFECTIVE MODELS FOR STATISTICAL STUDIES OF GALAXY-SCALE GRAVITATIONAL LENSING
Lapi, A., Negrello, M., González-Nuevo, J., Cai, Z.-Y., de Zotti, G., & Danese, L. (2012) · The Astrophysical Journal · doi:10.1088/0004-637x/755/1/46 · Cited by 72
“…the mass distribution, we find that the slope η ≈ 0.823 of the basic SISSA model is steepened to the value 0.958 according to the prescription for halo contraction by Blumenthal et al. (1986), to 0.920 according to that by Gnedin et al. (2004), and to 0.877 according to that by Abadi et al. (2010).”
BackgroundResultInfluentialTHE IMPACT OF BARYON PHYSICS ON THE STRUCTURE OF HIGH-REDSHIFT GALAXIES
Zemp, M., Gnedin, O., Gnedin, N., & Kravtsov, A. (2011) · The Astrophysical Journal · doi:10.1088/0004-637x/748/1/54 · Cited by 54
“While the concentration cV is only sensitive to the matter distribution within rmax, the processes of gas cooling and star formation affect the dark matter profile throughout the whole halo (see also Rudd et al. 2008; Abadi et al. 2010).”
BackgroundInfluentialHalo shapes from weak lensing: the impact of galaxy-halo misalignment
Bett, P. E. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2011.20258.x · Cited by 66
“…with a tendency towards oblateness (Kazantzidis et al. 2004; Kazantzidis, Abadi & Navarro 2010; Bailin et al. 2005; Berentzen & Shlosman 2006; Gustafsson, Fairbairn & Sommer-Larsen 2006; Debattista et al. 2008; Tissera et al. 2010; Machado & Athanassoula 2010; Abadi et al. 2010; Lau et al. 2011).”
BackgroundGalaxy shapes and alignments in the MassiveBlack-II hydrodynamic and dark matter-only simulations
Tenneti, A., Mandelbaum, R., Matteo, T. D., Kiessling, A., & Khandai, N. (2015) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stv1625 · Cited by 66
“The radial dependence of dark matter halo shapes has previously been studied using N -body simulations (e.g., Allgood et al. 2006; Schneider, Frenk & Cole 2012) and smallvolume hydrodynamic simulations (e.g., Kazantzidis et al. 2004; Abadi et al. 2010; Deason et al. 2011).”
BackgroundMethodResultInfluentialTRACING 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
A precise extragalactic test of General Relativity
Collett, T., Oldham, L., Smith, R., Auger, M., Westfall, K., Bacon, D., Nichol, R., Masters, K., Koyama, K., & van den Bosch, R. (2018) · MPG.PuRe (Max Planck Society) · Cited by 64
Evidence for galaxy assembly bias in BOSS CMASS redshift-space galaxy correlation function
Yuan, S., Hadzhiyska, B., Bose, S., Eisenstein, D. J., & Guo, H. (2021) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stab235 · Cited by 63
“The 𝑠 parameter is motivated by baryonic processes that can bias the concentration of baryons within the dark 1 https://github.com/SandyYuan/GRAND-HOD matter potential well (e.g. Duffy et al. 2010; Abadi et al. 2010; Chua et al. 2017; Peirani et al. 2017).”
MethodPrimack, J. R. (2009) · New Journal of Physics · doi:10.1088/1367-2630/11/10/105029 · Cited by 63
Constraints on the shapes of galaxy dark matter haloes from weak gravitational lensing
van Uitert, E., Hoekstra, H., Schrabback, T., Gilbank, D. G., Gladders, M. D., & Yee, H. K. C. (2012) · Astronomy and Astrophysics · doi:10.1051/0004-6361/201219295 · Cited by 63
“Furthermore, the central galaxy is expected to sphericalise the dark matter haloes (e.g. Kazantzidis et al. 2010; Abadi et al. 2010; Machado & Athanassoula 2010).”
BackgroundOn the density-profile slope of clusters of galaxies
Popolo, A. D. (2012) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2012.21141.x · Cited by 61
Counterrotating stars in simulated galaxy discs
Algorry, D. G., Navarro, J. F., Abadi, M. G., Sales, L. V., Steinmetz, M., & Piontek, F. (2013) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stt2154 · Cited by 60
“As reported in earlier work (see, e.g. Navarro & Steinmetz 1997; Abadi et al. 2010), the angular momentum of each component rises quickly with time until turnaround and stays roughly constant or declines slightly thereafter.”
ResultSelf-citationSEGUE-2: Old Milky Way Stars Near and Far
Rockosi, C. M., Lee, Y. S., Morrison, H., Yanny, B., Johnson, J. A., Lucatello, S., Sobeck, J. S., Beers, T. C., Prieto, C. A., An, D., et al. (2022) · The Astrophysical Journal Supplement Series · doi:10.3847/1538-4365/ac5323 · Cited by 63
“These measurements are essential for studies of the Galaxy in the contexts of galaxy evolution and cosmology (Abadi et al. 2010; Boylan-Kolchin et al. 2010; Wang et al. 2012) and to the analysis of the 6D motions of high-velocity stars in the tails of the velocity distribution and the local escape…”
MethodAssessing the Jeans Anisotropic Multi-Gaussian Expansion method with the Illustris simulation
Li, H., Li, R., Mao, S., Xu, D., Long, R. J., & Emsellem, É. (2015) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stv2565 · Cited by 58
“It has been shown in hydrodynamical simulations that baryonic processes modify 1 Available from http://www-astro.physics.ox.ac.uk/∼mxc/software c© 2015 RAS, MNRAS 000, 1–14 the inner profile of the dark halo (Abadi et al. 2010).”
BackgroundVenn, K. A., Kielty, C., Sestito, F., Starkenburg, E., Martin, N. F., Aguado, D. S., Arentsen, A., Bonifacio, P., Caffau, E., Hill, V., et al. (2019) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stz3546 · Cited by 62
“…stars in the Galatic halo are thought to have been accreted from dwarf galaxies at early epochs, based on cosmological hydrodynamical simulations of the Local Group (Ibata et al. 1994; Helmi et al. 1999; Ibata et al. 2004; Abadi et al. 2010; Starkenburg et al. 2017a; El-Badry et al. 2018).”
Self-citationMerger-induced galaxy transformations in the artemis simulations
Dillamore, A. M., Belokurov, V. A., Font, A. S., & McCarthy, I. G. (2022) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stac1038 · Cited by 57
Napolitano, N. R., Pota, V., Romanowsky, A. J., Forbes, D. A., Brodie, J. P., & Foster, C. (2014) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stt2484 · Cited by 57
“…Blumenthal et al. 1986), which might allow lower stellar mass normalization by dragging more DM into the central regions (see e.g. Napolitano, Romanowsky & Tortora 2010), as these seem to be disfavoured by both simulations (e.g. Abadi et al. 2010) and observational studies (e.g. Auger et al. 2010).”
BackgroundSize matters: abundance matching, galaxy sizes, and the Tully–Fisher relation in EAGLE
Ferrero, I., Navarro, J. F., Abadi, M. G., Sales, L. V., Bower, R. G., Crain, R. A., Frenk, C. S., Schaller, M., Schaye, J., & Theuns, T. (2016) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stw2691 · Cited by 57
“8 in Abadi et al. 2010).”
Self-citationSubhalo demographics in the Illustris simulation: effects of baryons and halo-to-halo variation
Chua, K. T. E., Pillepich, A., Rodríguez-Gómez, V., Vogelsberger, M., Bird, S., & Hernquist, L. (2017) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stx2238 · Cited by 57
“Indeed, radiative hydrodynamic simulations with baryonic cooling have been found to produce haloes that are both more spherical and centrally concentrated (e.g. Gnedin et al. 2004; Abadi et al. 2010).”
BackgroundDark matter halo shapes in the Auriga simulations
Prada, J., Forero-Romero, J. E., Grand, R. J. J., Pakmor, R., & Springel, V. (2019) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stz2873 · Cited by 57
Streams in the Aquarius stellar haloes
Gómez, F. A., Helmi, A., Cooper, A. P., Frenk, C. S., Navarro, J. F., & White, S. D. M. (2013) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/stt1838 · Cited by 56
“…dissipative condensation of baryons can induce a transformation of the structure of dark haloes to a more oblate and axisymmetric shape in the inner regions while preserving their triaxial shape in the outer parts (Debattista et al. 2008; Abadi et al. 2010; Valluri et al. 2010; Bryan et al. 2012).”
BackgroundSelf-citation
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
About these checks
Registry, retraction, Cites and statistics results are computed, not judged, with one exception: a printed reference that no index lists is read once by a model before it counts as a citation error. Claims are extracted by a model and kept only when their quote appears verbatim in the text; each cited source is then checked, with a model’s help, for whether it says what the claim relies on. Those verdicts can be wrong — read the claim’s quote and the cited source before relying on one.
Statistics and arithmetic are recomputed, not judged.
Confidence bands are shown only for fields calibrated on our annotated test set. None is calibrated yet, so no band is shown.
What counts as a claim ›How we measure confidence ›How we check this ›
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