REVIEW 3 major objections 6 minor 59 references
Modified Gravity Theories in Light of the Anomalous Velocity Dispersion of NGC1052-DF2
T0 review · 3 major / 6 minor · reviewed 2026-08-14 · deepseek-v4-flash
Pith's one-line read NGC1052-DF2, the galaxy claimed to have no dark matter, still fits MOND, MOG, Weyl conformal gravity, and general relativity without dark matter, with only emergent gravity failing at the 20 Mpc distance.
desk verdict A useful but flawed consistency check: the chi-squares that carry the main claim are never defined, and the 'fully consistent' abstract oversells emergent gravity's poor fit. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The central object is the projected line-of-sight velocity dispersion obtained from the isotropic, spherically symmetric Jeans equation: $\sigma^2(r) = \frac{1}{\rho(r)}\int_r^\infty \rho(r') a(r')\,dr'$ and $\sigma_{\mathrm{LOS}}^2(R) = \frac{\int_R^\infty r\,\sigma^2(r)\rho(r)/\sqrt{r^2-R^2}\,dr}{\int_R^\infty r\,\rho(r)/\sqrt{r^2-R^2}\,dr}$. Into this equation the authors feed the truncated Sersic stellar density of Eq. (2.1) and each theory's acceleration law: MOND's interpolation function with $a_0=1.21\times10^{-10}$ m/s$^2$, Weyl conformal gravity's fourth-order acceleration with constants $R_0=24$ kpc, $M_0=5.6\times10^{10}\,M_\odot$, $\kappa=9.54\times10^{-54}$ cm$^{-2}$, MOG's vector-field acceleration with $\alpha=1.30$, $\mu=0.443$ kpc$^{-1}$, and emergent gravity's extra term $a_v = a_0 M(r)/[d(M(r)r)/dr]$. The Jeans pipeline converts each theory's acceleration into a dispersion curve that can be compared with the ten globular-cluster velocities.
What would settle it
A decisive check would be an independent distance measurement for NGC1052-DF2 (for example from the tip of the red-giant branch) plus a stellar mass profile from resolved star counts, along with radial velocities for at least thirty globular clusters. Recomputing the six predicted dispersion profiles from that measured mass profile, the consistency claim is falsified if the observed line-of-sight dispersion is excluded at 2σ by all of the baryons-only predictions in any radial bin.
Extended reading notes
Core claim
On the paper's own terms, the finding is that the ten globular-cluster velocity dispersions of NGC1052-DF2 are consistent with the baryonic mass alone, both in general relativity without dark matter and in most modified gravity theories. The quantitative ranking is distance-dependent: for D=20 Mpc the reduced chi-square values are 1.82 for GR, 1.47 for MOG, 3.60 for MOND, 2.01 for MOND with the external-field effect, 5.00 for Weyl conformal gravity, and 9.99 for emergent gravity; for D=13.2 Mpc they improve to 2.04, 1.81, 1.89, 1.79, 3.35, and 4.55, respectively. The authors trace emergent gravity's poor 20-Mpc performance to its additional acceleration term, which is two to three orders of magnitude above the Newtonian value in the inner galaxy. They extend the conclusion to NGC1052-DF4, a second claimed dark-matter-free galaxy, whose predicted rms dispersions are compatible with most of the same theories at the 2σ level.
Load-bearing premise
The load-bearing premise is that the visible stellar mass is well described by a truncated Sersic profile with the adopted central surface density, effective radius, and cutoff radius (and either the 20 or 13.2 Mpc distance); if the true stellar profile, tidal truncation, or distance differs, every predicted dispersion curve shifts and the reported chi-square rankings change.
Editorial extensions
If this is right
- A dark-matter-free interpretation of NGC1052-DF2 does not discriminate between general relativity plus baryons and modified gravity: the same stellar mass profile reproduces the data in both paradigms.
- If the galaxy is at 13.2 Mpc, the data become compatible with all six models considered, so a decisive distance measurement would settle which model rankings matter.
- MOG's good fit is aided by its mass-dependent parameters $\alpha$ and $\mu$, which give it a flexibility the other modified theories lack.
- At 20 Mpc, emergent gravity is the only theory examined that fails to match the data, because its extra acceleration term dominates the baryonic Newtonian acceleration in the inner galaxy.
- The external-field effect improves MOND's fit at 20 Mpc from 3.60 to 2.01, and the true MOND prediction with a realistic external acceleration lies between those values.
Reading between the lines
- With only ten tracers and asymmetric error bars, the reduced chi-square differences among the better-fitting models (1.47–3.60 at 20 Mpc) may not be statistically distinguishable; a full likelihood treatment could make several models essentially equivalent.
- The sharp truncation radius is a simplified proxy for tidal stripping; a theory-specific tidal-radius calculation would alter the outer parts of every predicted profile and could reorder the chi-square ranking.
- The same Jeans-profile pipeline could be applied to other ultra-diffuse galaxies discovered in wide surveys; a galaxy whose measured dispersion lies well below the baryon-only prediction would be the real falsification test that DF2 does not provide.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper computes line-of-sight velocity dispersion profiles for the ultra-diffuse galaxy NGC1052-DF2 under general relativity without dark matter, MOND (with and without an external field effect), Weyl conformal gravity, MOG, and Verlinde's emergent gravity, using a Sérsic baryonic mass model at two assumed distances (20 Mpc and 13.2 Mpc). It reports reduced chi-square values comparing predicted dispersion profiles with ten globular-cluster velocity data points and concludes that the data are fully consistent with GR and with all modified gravity theories except emergent gravity at 20 Mpc. It also gives rms dispersion predictions for NGC1052-DF4. The quantitative evidence for the central claim is in Section V: Tables I and II contain reduced chi-square values, and Figure 4 compares rms dispersion bounds.
Significance. If the statistical comparison were valid, the paper would be a useful unified reference for how four modified gravity theories plus GR fare against the DF2 data, with the strength of treating both disputed distance estimates and including MOND's external field effect. The authors are transparent about MOG's parameter flexibility and about idealizations such as spherical symmetry, isotropy, and a sharp truncation radius. However, the central claim rests entirely on chi-square values whose definition is never given; since individual globular-cluster velocities are not dispersion measurements, the quoted numbers cannot be verified as stated. The paper also does not propagate uncertainties from the mass model, distance, or truncation radius into the chi-square tables. The comparison is therefore not yet a sound basis for the abstract's 'fully consistent' conclusion.
major comments (3)
- [Section V, Tables I and II] The reduced chi-square values in Tables I and II are the sole quantitative evidence for the abstract's central claim that the dispersion data of NGC1052-DF2 are 'fully consistent' with the modified gravity paradigm, yet the manuscript never defines how χ²/dof is computed from the ten globular-cluster velocities. A single line-of-sight velocity v_i is one draw from the velocity distribution at projected radius R_i, not a measurement of σ_los(R_i); if Figure 2's 'individual GC velocity dispersion measurements' are the absolute values |v_i| plotted against the predicted σ_los curve, the test is biased because under a Gaussian the expectation of |v| is about 0.80σ. The authors must state the exact statistic, report the ten input velocities, and either use a Gaussian likelihood such as ∏_i N(v_i | 0, σ_los^2(R_i) + ε_i^2) or bin the data into dispersion estimates with proper errors. Without this, the numbers in Tables I and II cannot be checked and the consistency claim is unverified.
- [Section IIIc and Section VI] The MOG parameters α = 1.30 and μ = 0.443 kpc⁻¹ are taken from Moffat and Toth [44], who fit the velocity dispersion of NGC1052-DF2 itself; the MOG row in Tables I and II is therefore a same-galaxy re-fit rather than an independent prediction. The paper explicitly acknowledges in Section VI that MOG 'enjoys one additional degree of freedom' because its parameters are mass-dependent. To make the comparison meaningful, the authors should either fix MOG parameters from external galaxy samples or apply a model-comparison penalty (e.g., AIC or BIC) for the fitted parameters. As presented, the lower MOG χ² relative to MOND, Weyl, and Emergent gravity does not by itself establish that MOG is more consistent with the data.
- [Section V, Eq. (5.2) and Figure 4; Section VI] The error bars in Figure 4 are obtained by varying the effective radius by 50%, but Tables I and II are computed with fixed values of Re, Σ0, rcut, and anisotropy, with no propagation of these uncertainties or of the distance uncertainty into the predicted σ_los profiles. Since the distance is disputed (20 Mpc vs 13.2 Mpc) and rcut is a hand-chosen truncation, the claimed consistency should be demonstrated by showing how χ² changes under these variations, not only by the two distance rows in Tables I and II. The statement in Section VI that the simplifications 'would unlikely to alter the final conclusion much' is an assertion that needs quantitative support.
minor comments (6)
- [Throughout, Section IIIa] The galaxy parameter is spelled 'Sersic' in Section II but should be 'Sérsic' throughout; the phrase 'Modified Newtonian Dynamcies' in the title and Section IIIa should be 'Modified Newtonian Dynamics'.
- [Abstract] The abstract contains a duplicated article: 'coupled to the the baryonic mass' should read 'coupled to the baryonic mass'.
- [Section IIIb, Eq. (3.3)] The exterior moment E_{-1}(r) appears in Eq. (3.3) but is not explicitly defined; the given definition of E_n(r) covers n = -1 only implicitly, and this should be stated.
- [Figures 2 and 5] The captions refer to 'individual GC velocity dispersion measurements' for the blue points; if these points are the original individual radial velocities, they should be relabeled as such and the error bars explained, because individual velocities are draws from a distribution, not dispersion measurements.
- [Section V, Tables I and II] The degrees of freedom for the quoted χ²/dof are never stated; the authors should specify dof for each theory, for example as the number of globular clusters minus the number of free parameters in the model.
- [Section V, data availability] The ten globular-cluster velocities and their uncertainties used in Figures 2 and 5 are not tabulated in the manuscript; adding a data table would make the analysis reproducible and allow readers to verify the chi-square construction.
Circularity Check
No significant circularity: the dispersion predictions are derived from an externally fitted stellar mass profile and fixed theory parameters, not from the target dispersion data.
full rationale
The paper's derivation chain is: (i) adopt the Sersic mass density of Eq. (2.1), originally fit to surface photometry by van Dokkum et al. and approximated by Moffat and Toth; (ii) insert the baryonic acceleration predicted by each theory (MOND Eq. 3.2, Weyl Eq. 3.3, MOG Eq. 3.4, Emergent Eq. 3.5); (iii) solve the isotropic Jeans equation (Eq. 4.2) and project (Eq. 4.3); (iv) compare to the 10 GC velocity data through reduced chi-square. The MOG parameters alpha=1.30 and mu=0.443 kpc^-1 are adopted from Moffat and Toth [44] via the mass-dependent scaling relations of Moffat and Toth [49], not fitted to DF2's dispersion in this paper; the text explicitly contrasts these with rotation-curve values and notes MOG's extra degree of freedom. This is a parameter choice, not a circular prediction. MOND, Weyl, and Emergent use fixed or externally calibrated constants (a0, R0, M0, kappa). No uniqueness theorem or author-imported ansatz bears the argument; self-citations [28,35] appear only in the introduction's literature survey. The paper does not define the chi-square statistic used in Tables I and II, which is a reproducibility and statistical-validity concern (comparing absolute velocities to sigma_los would bias residuals), but that is not a circularity of the derivation chain. The modeling assumptions (spherical symmetry, isotropy, rcut, inclination) are stated as caveats and do not smuggle the conclusion in.
Assumptions & free parameters
free parameters (6)
- MOG alpha =
1.30
- MOG mu =
0.443 kpc^-1
- Sersic Sigma0 =
1.25e7 Msun/kpc^2
- Effective radius Re =
2.0 kpc (D=20) / 1.4 kpc (D=13.2)
- Truncation radius rcut =
10 kpc (D=20) / 8 kpc (D=13.2)
- MOND external field aext =
0.5 a0
assumptions (5)
- domain assumption The galaxy is spherically symmetric and non-rotating, so the Jeans equation (4.1) applies with anisotropy xi=0.
- domain assumption The baryonic mass distribution is described by the Sersic approximation (2.1).
- domain assumption There is no dark matter in the modeled galaxy.
- domain assumption MOG parameter scaling relations (alpha = alpha_inf M/(sqrt(M)+E)^2, mu = D/sqrt(M)) are correct.
- ad hoc to paper External field effect in MOND can be represented by replacing the interpolating function argument with (a + aext)/a0 and aext = 0.5a0 as an extreme case.
Cite this review
Pith. "Pith review of Modified Gravity Theories in Light of the Anomalous Velocity Dispersion of NGC1052-DF2." pith.science (2026). https://pith.science/paper/AWN5QOHE
@misc{pith2026190807160,
author = {Pith},
title = {Pith review of: Modified Gravity Theories in Light of the Anomalous Velocity Dispersion of NGC1052-DF2},
year = {2026},
howpublished = {\url{https://pith.science/paper/AWN5QOHE}},
note = {Machine review of arXiv:1908.07160}
}
abstract
Recent observations of ultra-dwarf galaxy NGC1052-DF2 started an interesting discussion between dark matter hypothesis and modified gravity theories. Reported low velocity dispersion (< 10.5 km/s at 90% confidence level) derived from the kinematic data of 10 globular clusters in the galaxy points towards an extraordinarily low dynamical mass ($\sim$ $3.4 \times 10^{8} M_{\odot}$) which is of the same order of the luminous mass ($\sim$ $2.0 \times 10^{8} M_{\odot}$) in the galaxy. This has been interpreted as the first evidence of a galaxy `without Dark Matter'. It has been argued that dark matter is not necessarily coupled to the the baryonic mass on the galactic scale and poses a challenge to modified gravity theories. We explore the dynamics of NGC1052-DF2 within the context of four popular alternative theories of gravity [Modified Newtonian Dynamcies (MOND), Weyl Conformal gravity, Modified gravity (MOG)/Scalar-Tensor-Vector Gravity (STVG) and Verlinde's Emergent gravity] and present the analysis of detailed radial variation of the velocity dispersion. We demonstrate that the dispersion data of NGC1052-DF2 is fully consistent with modified gravity paradigm (as well as with general relativity without dark matter). We reach similar conclusion for the ultra-dwarf NGC1052-DF4 which has been claimed to be the second candidate for galaxies `without Dark Matter'.
Figures
Figures from the paper (3 more)
Reference graph
Works this paper leans on
-
[44]
found MOG to be consistent with the quoted overall dispersion value in vD18a. However, these studies lack a de- tailed comparison between the observed dispersion velocities for individual GCs and the predicted values, which we will investigate thoroughly. The outline of the remaining paper is as follows. We begin with the baryonic mass model of NGC1052-DF...
-
[1]
Van Dokkum, et al., Nature 555, 629 (2018), arXiv:1803.10237 [astro-ph.GA]
P. Van Dokkum, et al., Nature 555, 629 (2018), arXiv:1803.10237 [astro-ph.GA]
arXiv 2018
-
[2]
A Revised Velocity for the Globular Cluster GC-98 in the Ultra Diffuse Galaxy NGC1052-DF2
P. van Dokkum, et al., Research Notes of the AAS,2, 54 (2018), arXiv:1806.04685 [astro-ph.GA]
work page Pith review arXiv 2018
-
[3]
P. S. Behroozi, R. H. Wechsler, and C. Conroy, The Astrophysi- cal Journal 770, 57 (2013), arXiv:1207.6105 [astro-ph.CO]
arXiv 2013
-
[4]
S. S. McGaugh, F. Lelli, and J. M. Schombert, Physical Review Letters 117, 201101 (2016), arXiv:1609.05917 [astro-ph.GA]
arXiv 2016
-
[5]
E. Emsellem, R. F. van der Burg, J. Fensch, T. Je ˇr´abkov´a, A. Zanella, A. Agnello, M. Hilker, O. M ¨uller, M. Rejkuba, P.-A. Duc, et al., Astronomy & Astrophysics625, A76 (2019), arXiv:1812.07345 [astro-ph.GA]
arXiv 2019
-
[6]
Both these estimates are significantly higher than the value quoted by vD18a
using the same data of vD18a reports a mean observed bi-weighted dispersion value of 14.3± 3.5 km/s. Both these estimates are significantly higher than the value quoted by vD18a. However, a different study by Danieli et. al [7] have found a stellar velocity dispersion of σ ∼ 8.4± 2.1 km/s, consistent with the values derived from the GCs in vD18a. More recen...
-
[7]
S. Danieli, P. van Dokkum, C. Conroy, R. Abraham, and A. J. Romanowsky, The Astrophysical Journal Letters 874, L12 (2019), arXiv:1901.03711 [astro-ph.GA]
arXiv 2019
Show all 59 references
-
[8]
Moffat and Toth
have recently explored the dynamics of NGC1052-DF2 in the MOND paradigm and concluded that the current data are insufficient to rule out MOND scenarios. Moffat and Toth
-
[9]
Trujillo, M
I. Trujillo, M. A. Beasley, A. Borlaff, E. R. Carrasco, A. Di Cin- tio, M. Filho, M. Monelli, M. Montes, J. Rom´an, T. Ruiz-Lara, et al., Monthly Notices of the Royal Astronomical Society 486, 1192 (2019), arXiv:1806.10141 [astro-ph.GA]
2019 arXiv
-
[10]
Wasserman, A
A. Wasserman, A. J. Romanowsky, J. Brodie, P. van Dokkum, C. Conroy, R. Abraham, Y . Cohen, and S. Danieli, The Astro- physical Journal Letters 863, L15 (2018), arXiv:1807.07069 [astro-ph.GA]
2018 arXiv
-
[11]
Haslbauer, I
M. Haslbauer, I. Banik, P. Kroupa, G. Konstantin, Monthly Notices of the Royal Astronomical Society 489, 2634 (2019), arXiv:1909.04663 [astro-ph.GA]
2019 arXiv
-
[12]
Nusser, arXiv preprint arXiv:1907.08035 (2019)
A. Nusser, arXiv preprint arXiv:1907.08035 (2019)
2019 arXiv
-
[13]
N. F. Martin, M. L. Collins, N. Longeard, and E. Tollerud, The Astrophysical Journal Letters 859, L5 (2018), arXiv:1804.04136 [astro-ph.GA]
2018 arXiv
- [14]
-
[15]
Haghi, P
H. Haghi, P. Kroupa, I. Banik, X. Wu, A. H. Zonoozi, B. Ja- vanmardi, A. Ghari, O. M¨uller, J. Dabringhausen, and H. Zhao, Monthly Notices of the Royal Astronomical Society 487, 2441 (2019), arXiv:1906.03268 [astro-ph.GA]
2019 arXiv
-
[16]
Milgrom, The Astrophysical Journal 270, 365 (1983)
M. Milgrom, The Astrophysical Journal 270, 365 (1983)
1983
-
[17]
Famaey and S
B. Famaey and S. S. McGaugh, Living reviews in relativity 15, 10 (2012), arXiv:1112.3960 [astro-ph.CO]
2012 arXiv
-
[18]
J. W. Moffat, Journal of Cosmology and Astroparticle Physics 2006, 004 (2006), arXiv:gr-qc/0506021
2006 arXiv
-
[19]
P. D. Mannheim and D. Kazanas, The Astrophysical Journal 342, 635 (1989)
1989
-
[20]
Ogiya, Monthly Notices of the Royal Astronomical Society: Letters 480, L106 (2018), arXiv:1804.06421 [astro-ph.GA]
G. Ogiya, Monthly Notices of the Royal Astronomical Society: Letters 480, L106 (2018), arXiv:1804.06421 [astro-ph.GA]
2018 arXiv
-
[21]
However, this difference would not change our result
used a slightly di fferent value for a0. However, this difference would not change our result. IV . DISPERSION PROFILE OF SPHERICALLY SYMMETRIC OBJECTS For non-rotating systems with spherically symmetric mass distributions, the velocity dispersion can be computed by solv- ing th...
-
[22]
Silk, arXiv preprint arXiv:1905.13235 (2019)
J. Silk, arXiv preprint arXiv:1905.13235 (2019)
2019 arXiv
-
[23]
Gentile, B
G. Gentile, B. Famaey, and W. de Blok, Astronomy & Astro- physics 527, A76 (2011), arXiv:1011.4148 [astro-ph.CO]
2011 arXiv
-
[24]
P. D. Mannheim and J. G. O’Brien, Physical Review D 85, 124020 (2012), arXiv:1011.3495 [astro-ph.CO]
2012 arXiv
-
[25]
P. D. Mannheim, The Astrophysical Journal 479, 659 (1997), arXiv:astro-ph/9605085
1997 arXiv
-
[26]
P. D. Mannheim and J. G. O’Brien, Physical review letters106, 121101 (2011), arXiv:1007.0970 [astro-ph.CO]
2011 arXiv
-
[27]
P. D. Mannheim, Progress in Particle and Nuclear Physics56, 340 (2006), arXiv:astro-ph/0505266
2006 arXiv
-
[28]
Verlinde, SciPost Physics2, 016 (2017), arXiv:1611.02269 [hep-th]
E. Verlinde, SciPost Physics2, 016 (2017), arXiv:1611.02269 [hep-th]
2017 arXiv
-
[29]
R. H. Sanders and S. S. McGaugh, Annual Review of Astron- omy and Astrophysics 40, 263 (2002), arXiv:astro-ph/0204521
2002 arXiv
-
[30]
Moffat and V
J. Moffat and V . Toth, Physical Review D91, 043004 (2015), arXiv:1411.6701 [astro-ph.GA]
2015 arXiv
-
[31]
Moffat and V
J. Moffat and V . T. Toth, arXiv preprint arXiv:1103.5634 (2011), arXiv:1103.5634 [astro-ph.GA]
2011 arXiv
-
[32]
Scarpa, G
R. Scarpa, G. Marconi, and R. Gilmozzi, Astronomy & Astro- physics 405, L15 (2003)
2003
-
[33]
Scarpa, G
R. Scarpa, G. Marconi, and R. Gilmozzi, arXiv preprint astro- ph/0411078 (2004)
2004
-
[34]
J. G. O’Brien and P. D. Mannheim, Monthly Notices of the Royal Astronomical Society421, 1273 (2012), arXiv:1107.5229 [astro-ph.CO]
2012 arXiv
-
[35]
Dutta and T
K. Dutta and T. Islam, Phys. Rev. D 98, 124012 (2018), arXiv:1808.06923 [gr-qc]
2018 arXiv
-
[36]
Moffat and S
J. Moffat and S. Rahvar, Monthly Notices of the Royal As- tronomical Society 436, 1439 (2013), arXiv:1306.6383 [astro- ph.GA]
2013 arXiv
-
[37]
Ghari, H
A. Ghari, H. Haghi, and A. H. Zonoozi, Monthly No- tices of the Royal Astronomical Society 487, 2148 (2019), arXiv:1907.01564 [astro-ph.GA]
2019 arXiv
-
[38]
J. G. O’Brien, T. L. Chiarelli, P. D. Mannheim, M. A. Falcone, M. H. AlQurashi, and J. Carter, in Journal of Physics: Con- ference Series (IOP Publishing, 2019), vol. 1239, p. 012009, arXiv:1812.03152 [astro-ph.GA]
2019 arXiv
-
[39]
Emergent gravity, on the other hand, enjoys success in explaining the rotation curves of dwarf galaxies
for MOG). Emergent gravity, on the other hand, enjoys success in explaining the rotation curves of dwarf galaxies
-
[40]
arXiv:1908.07160v2 [gr-qc] 7 Dec 2019 2 Famaey et al
but finds itself inconsistent with RAR [41]. arXiv:1908.07160v2 [gr-qc] 7 Dec 2019 2 Famaey et al. [42], Kroupa et al. [43] and Haghi et al
1908 arXiv
-
[41]
Scarpa, G
R. Scarpa, G. Marconi, R. Gilmozzi, and G. Carraro, Astronomy & Astrophysics 462, L9 (2007), arXiv:astro-ph/0611504
2007 arXiv
-
[42]
Islam, Monthly Notices of the Royal Astronomical Society 488, 5390–5399 (2019), arXiv:1811.00065
T. Islam, Monthly Notices of the Royal Astronomical Society 488, 5390–5399 (2019), arXiv:1811.00065
2019 arXiv
-
[43]
Moffat and V
J. Moffat and V . Toth, The Astrophysical Journal 680, 1158 (2008), arXiv:0708.1935 [astro-ph]
2008 arXiv
-
[45]
Cohen, P
Y . Cohen, P. van Dokkum, S. Danieli, A. J. Romanowsky, R. Abraham, A. Merritt, J. Zhang, L. Mowla, J. D. Kruijssen, C. Conroy, et al., The Astrophysical Journal 868, 96 (2018), arXiv:1807.06016 [astro-ph.GA]
2018 arXiv
-
[46]
Green and J
M. Green and J. Mo ffat, Physics of the Dark Universe 25, 100323 (2019), arXiv:1905.09476 [gr-qc]
2019 arXiv
-
[47]
Diez-Tejedor, A
A. Diez-Tejedor, A. X. Gonzalez-Morales, and G. Niz, Monthly Notices of the Royal Astronomical Society 477, 1285 (2018), arXiv:1612.06282 [astro-ph.CO]
2018 arXiv
-
[48]
Lelli, S
F. Lelli, S. S. McGaugh, and J. M. Schombert, Monthly Notices of the Royal Astronomical Society: Letters 468, L68 (2017), arXiv:1702.04355 [astro-ph.GA]
2017 arXiv
-
[49]
Famaey, S
B. Famaey, S. McGaugh, and M. Milgrom, Monthly No- tices of the Royal Astronomical Society 480, 473 (2018), arXiv:1804.04167 [astro-ph.GA]
2018 arXiv
-
[50]
Kroupa, H
P. Kroupa, H. Haghi, B. Javanmardi, A. H. Zonoozi, O. M¨uller, I. Banik, X. Wu, H. Zhao, and J. Dabringhausen, Nature 561, E4 (2018), arXiv:1903.11612 [astro-ph.GA]
2018 arXiv
-
[51]
Moffat and V
J. Moffat and V . Toth, Monthly Notices of the Royal Astro- nomical Society: Letters 482, L1 (2018), arXiv:1805.01117 [gr-qc]
2018 arXiv
-
[52]
and thus modified gravity theories will easily be able to account for the observed dispersion profiles. A detailed study of the radial variation of dispersion profiles, similar to one presented for NGC1052-DF2 in this paper, would be needed to draw strong inference regarding the ...
-
[53]
Weyl, Mathematische Zeitschrift 2, 384 (1918)
H. Weyl, Mathematische Zeitschrift 2, 384 (1918)
1918
-
[54]
Horne, Monthly Notices of the Royal Astronomical Society 369, 1667 (2006),
K. Horne, Monthly Notices of the Royal Astronomical Society 369, 1667 (2006),
2006
-
[55]
Diaferio and L
A. Diaferio and L. Ostorero, Monthly Notices of the Royal Astronomical Society 393, 215 (2009), arXiv:0808.3707 [astro- ph]
2009 arXiv
-
[56]
Moffat and V
J. Moffat and V . T. Toth, Classical and Quantum Gravity 26, 085002 (2009), arXiv:0712.1796 [gr-qc]
2009 arXiv
-
[57]
Binney and S
J. Binney and S. Tremaine, Galactic dynamics, princeton univ (1987)
1987
-
[58]
van Dokkum, S
P. van Dokkum, S. Danieli, R. Abraham, C. Conroy, and A. J. Romanowsky, The Astrophysical Journal Letters 874, L5 (2019), arXiv:1901.05973 [astro-ph.GA]
2019 arXiv
-
[59]
Monelli and I
M. Monelli and I. Trujillo, The Astrophysical Journal Letters 880, L11 (2019), arXiv:1907.03761 [astro-ph.GA]
2019 arXiv
Reviewed August 14, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.