Modified Newtonian dynamics
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In physics, modified Newtonian dynamics (MOND) is a theory that proposes a modification of Newton's laws to account for observed properties of galaxies. Created in 1983 by Israeli physicist Mordehai Milgrom,^{[1]} the theory's original motivation was to explain the fact that the velocities of stars in galaxies were observed to be larger than expected based on Newtonian mechanics. Milgrom noted that this discrepancy could be resolved if the gravitational force experienced by a star in the outer regions of a galaxy was proportional to the square of its centripetal acceleration (as opposed to the centripetal acceleration itself, as in Newton's Second Law), or alternatively if gravitational force came to vary inversely with radius (as opposed to the inverse square of the radius, as in Newton's Law of Gravity). In MOND, violation of Newton's Laws occurs at extremely small accelerations, characteristic of galaxies yet far below anything typically encountered in the Solar System or on Earth.

MOND is an example of a class of theories known as modified gravity, and is an alternative to the hypothesis that the dynamics of galaxies are determined by massive, invisible dark matter halos. Since Milgrom's original proposal, researchers working within the MOND framework have discovered several galactic phenomena that adhere to the theory's basic tenets and are difficult to understand from a dark matter perspective.^{[2]} However, MOND and its generalisations fail to account for observed properties of galaxy clusters, and no cosmological model constructed from the theory is capable of rivaling the standard model of cosmology (based on general relativity, with which MOND is incompatible) in scope and predictive power.^{[3]} MOND has always been, and remains, a minority viewpoint within the physics and astrophysics communities.
Overview
Several independent observations point to the fact that the visible mass in galaxies and galaxy clusters is insufficient to account for their dynamics, when analysed using Newton's laws. This discrepancy – known as the "missing mass problem" – was first identified for clusters by Swiss astronomer Fritz Zwicky in 1933 (who studied the Coma cluster),^{[5]}^{[6]} and subsequently extended to include spiral galaxies by the 1939 work of Horace Babcock on Andromeda.^{[7]} These early studies were augmented and brought to the attention of the astronomical community in the 1960s and 1970s by the work of Vera Rubin at the Carnegie Institute in Washington, who mapped in detail the rotation velocities of stars in a large sample of spirals. While Newton's Laws predict that stellar rotation velocities should decrease with distance from the galactic centre, Rubin and collaborators found instead that they remain almost constant^{[8]} – the rotation curves are said to be "flat". This observation necessitates at least one of the following: 1) There exists in galaxies large quantities of unseen matter which boosts the stars' velocities beyond what would be expected on the basis of the visible mass alone, or 2) Newton's Laws do not apply to galaxies. The former leads to the dark matter hypothesis; the latter leads to MOND.
The basic premise of MOND is that while Newton's laws have been extensively tested in highacceleration environments (in the Solar System and on Earth), they have not been verified for objects with extremely low acceleration, such as stars in the outer parts of galaxies. This lead Milgrom to postulate a new effective gravitational force law (sometimes referred to as "Milgrom's law") that relates the true acceleration of an object to the acceleration that would be predicted for it on the basis of Newtonian mechanics.^{[1]} This law, the keystone of MOND, is chosen to reduce to the Newtonian result at high acceleration but lead to different ("deepMOND") behaviour at low acceleration:
Here F_{N} is the Newtonian force, m is the object's (gravitational) mass, a is its acceleration, μ(x) is an asyet unspecified function (known as the "interpolating function"), and a_{0} is a new fundamental constant which marks the transition between the Newtonian and deepMOND regimes. Agreement with Newtonian mechanics requires μ(x) → 1 for x >> 1, and consistency with astronomical observations requires μ(x) → x for x << 1. Beyond these limits, the interpolating function is not specified by the theory, although it is possibly to weakly constrain it empirically.^{[9]}^{[10]} Two common choices are:
and
Thus, in the deepMOND regime (a << a_{0}):
Applying this to an object of mass m in circular orbit around a point mass M (a crude approximation for a star in the outer regions of a galaxy), we find:
that is, the star's rotation velocity is independent of its distance r from the centre of the galaxy – the rotation curve is flat, as required. By fitting his law to rotation curve data, Milgrom found a_{0} ≈ 1.2 x 10^{−10} m s^{−2} to be optimal. This simple law is sufficient to make predictions for a broad range of galactic phenomena.
Milgrom's law can be interpreted in two different ways. One possibility is to treat it as a modification to the classical law of inertia (Newton's second law), so that the force on an object is not proportional to the particle's acceleration a but rather to μ(a/a_{0})a. In this case, the modified dynamics would apply not only to gravitational phenomena, but also those generated by other forces, for example electromagnetism.^{[11]} Alternatively, Milgrom's law can be viewed as leaving Newton's Second Law intact and instead modifying the inversesquare law of gravity, so that the true gravitational force on an object of mass m due to another of mass M is roughly of the form GMm/(μ(a/a_{0})r^{2}). In this interpretation, Milgrom's modification would apply exclusively to gravitational phenomena.
By itself, Milgrom's law is not a complete and selfcontained physical theory, but rather an adhoc empiricallymotivated variant of one of the several equations that constitute classical mechanics. Its status within a coherent nonrelativistic theory of MOND is akin to Kepler's Third Law within Newtonian mechanics; it provides a succinct description of observational facts, but must itself be explained by more fundamental concepts situated within the underlying theory. Several complete classical theories have been proposed (typically along "modified gravity" as opposed to "modified inertia" lines), which generally yield Milgrom's law exactly in situations of high symmetry and otherwise deviate from it slightly. A subset of these nonrelativistic theories have been further embedded within relativistic theories, which are capable of making contact with nonclassical phenomena (e.g. gravitational lensing) and cosmology.^{[12]} Distinguishing both theoretically and observationally between these alternatives is a subject of current research.
The majority of astronomers, astrophysicists and cosmologists accept ΛCDM^{[13]} (based on General Relativity, and thence Newtonian mechanics), and are committed to a dark matter solution of the missingmass problem. MOND, by contrast, is actively studied by only a handful of researchers. The primary difference between supporters of ΛCDM and MOND is in the observations for which they demand a robust, quantitative explanation and those for which they are satisfied with a qualitative account, or are prepared to leave for future work. Proponents of MOND emphasize predictions made on galaxy scales (where MOND enjoys its most notable successes) and believe that a cosmological model consistent with galaxy dynamics has yet to be discovered; proponents of ΛCDM require high levels of cosmological accuracy (which concordance cosmology provides) and argue that a resolution of galaxyscale issues will follow from a better understanding of the complicated baryonic astrophysics underlying galaxy formation.^{[2]}
Observational evidence for MOND
Since MOND was specifically designed to produce flat rotation curves, these do not constitute evidence for the theory. Nevertheless, a broad range of astrophysical phenomena are neatly accounted for within the MOND framework.^{[12]}^{[14]} Many of these came to light after the publication of Milgrom's original papers and are difficult to explain using the alternative dark matter hypothesis. The most prominent are the following:
 In addition to demonstrating that rotation curves in MOND are flat, equation 2 provides a concrete relation between a galaxy's total baryonic mass (the sum of its mass in stars and gas) and its asymptotic rotation velocity. Observationally, this is known as the baryonic Tully–Fisher relation (BTFR),^{[15]} and is found to conform quite closely to the MOND prediction.^{[16]}
 Milgrom's law fully specifies the rotation curve of a galaxy given only the distribution of its baryonic mass. In particular, MOND predicts a far stronger correlation between features in the baryonic mass distribution and features in the rotation curve than does the dark matter hypothesis (since dark matter dominates the galaxy's mass budget and is conventionally assumed not to closely track the distribution of baryons). Such a tight correlation is claimed to be observed in several spiral galaxies, a fact which has been referred to as "Renzo's rule".^{[12]}
 Since MOND modifies Newtonian dynamics in an accelerationdependent way, it predicts a specific relationship between the acceleration of a star at any radius from the centre of a galaxy and the amount of unseen (dark matter) mass within that radius that would be inferred in a Newtonian analysis. This is known as the "mass discrepancyacceleration relation", and has been measured observationally.^{[17]}^{[18]} One aspect of the MOND prediction is that the mass of the inferred dark matter go to zero when the stellar centripetal acceleration becomes greater than a_{0}, where MOND reverts to Newtonian mechanics. In dark matter theory, it is a challenge to understand why this mass should correlate so closely with acceleration, and why there appears a critical acceleration above which dark matter is not required.^{[2]}
 Both MOND and dark matter halos stabilise disk galaxies, helping them retain their rotationsupported structure and preventing their transformation into elliptical galaxies. In MOND, this added stability is only available for regions of galaxies within the deepMOND regime (i.e. with a<a_{0}), suggesting that spirals with a>a_{0} in their central regions should be prone to instabilities and hence less likely to survive to the present day.^{[19]} This may explain the "Freeman limit" to the observed central surface mass density of spiral galaxies, which is roughly a_{0}/G.^{[20]} This scale must be put in by hand in dark matterbased galaxy formation models.^{[21]}
 Particularly massive galaxies are within the Newtonian regime (a > a_{0}) out to radii enclosing the vast majority of their baryonic mass. At these radii, MOND predicts that the rotation curve should fall as 1/r, in accordance with Kepler's Laws. In contrast, from a dark matter perspective one would expect the halo to significantly boost the rotation velocity and cause it to asymptote to a constant value, as in less massive galaxies. Observations of highmass ellipticals bear out the MOND prediction.^{[22]}^{[23]}
 In MOND, all gravitationally bound objects with a < a_{0} – regardless of their origin – should exhibit a mass discrepancy when analysed using Newtonian mechanics, and should lie on the BTFR. Under the dark matter hypothesis, objects formed from baryonic material ejected during the merger or tidal interaction of two galaxies ("tidal dwarf galaxies") are expected to be devoid of dark matter and hence show no mass discrepancy. Three objects unambiguously identified as Tidal Dwarf Galaxies appear to have mass discrepancies in close agreement with the MOND prediction.^{[24]}^{[25]}^{[26]}
 Recent work has shown that many of the dwarf galaxies around the Milky Way and Andromeda are located preferentially in a single plane and have correlated motions. This suggests that they may have formed during a close encounter with another galaxy and hence be Tidal Dwarf Galaxies. If so, the presence of mass discrepancies in these systems constitutes further evidence for MOND. In addition, it has been claimed that a gravitational force stronger than Newton's (such as Milgrom's) is required for these galaxies to retain their orbits over time.^{[27]}
Complete MOND theories
Milgrom's law requires incorporation into a complete theory if it is to satisfy conservation laws and provide a unique solution for the time evolution of any physical system. Each of the theories described here reduce to Milgrom's law in situations of high symmetry (and thus enjoy the successes described above), but produce different behaviour in detail.
Nonrelativistic
The first complete theory of MOND (dubbed AQUAL) was constructed in 1984 by Milgrom and Jacob Bekenstein.^{[28]} AQUAL generates MONDian behaviour by modifying the gravitational term in the classical lagrangian from being quadratic in the gradient of the Newtonian potential to a more general function. (AQUAL is an acronym for AQUAdratic Lagrangian.) In formulae:
where Φ is the standard Newtonian gravitational potential and F is a new dimensionless function. Applying the Euler–Lagrange equations in the standard way then leads to a nonlinear generalisation of the Newton–Poisson equation:
This can be solved given suitable boundary conditions and choice of F to yield Milgrom's law (up to a curl field correction which vanishes in situations of high symmetry).
An alternative way to modify the gravitational term in the lagrangian it is to introduce a distinction between the true (MONDian) acceleration field a and the Newtonian acceleration field a_{N}. The Lagrangian may be constructed so that a_{N} satisfies the usual NewtonPoisson equation, and is then used to find a via an additional algebraic but nonlinear step, which is chosen to satisfy Milgrom's law. This is called the "quasilinear formulation of MOND", or QUMOND,^{[29]} and is particularly useful for calculating the distribution of "phantom" dark matter that would be inferred from a Newtonian analysis of a given physical situation.^{[12]}
Both AQUAL and QUMOND propose changes to the gravitational part of the classical matter action, and hence interpret Milgrom's law as a modification of Newtonian gravity as opposed to Newton's second law. The alternative is to turn the kinetic term of the action into a functional depending on the trajectory of the particle. Such "modified inertia" theories, however, are difficult to use because they are timenonlocal, require energy and momentum to be nontrivially redefined to be conserved, and have predictions that depend on the entirety of a particle's orbit.^{[12]}
Relativistic
In 2004, Jacob Bekenstein formulated TeVeS, the first complete relativistic theory with MONDian behaviour.^{[30]} TeVeS is constructed from a local lagrangian (and hence respects conservation laws), and employs a unit vector field, a dynamical and nondynamical scalar field, a free function and a nonEinsteinian metric in order to yield AQUAL in the nonrelativistic limit (low speeds and weak gravity). TeVeS has enjoyed some success in making contact with gravitational lensing and structure formation observations,^{[31]} but faces problems when confronted with data on the anisotropy of the cosmic microwave background,^{[32]} the lifetime of compact objects,^{[33]} and the relationship between the lensing and matter overdensity potentials.^{[34]}
Several alternative relativistic generalisations of MOND exist, including BIMOND and Generalised EinsteinAether theories.^{[12]}
The external field effect
In Newtonian mechanics, an object's acceleration can be found as the vector sum of the acceleration due to each of the individual forces acting on it. This means that a subsystem can be decoupled from the larger system in which it is embedded simply by referring the motion of its constituent particles to their centre of mass; in other words, the influence of the larger system is irrelevant for the internal dynamics of the subsystem. Since Milgrom's law is nonlinear in acceleration, MONDian subsystems cannot be decoupled from their environment in this way, and in certain situations this leads to behaviour with no Newtonian parallel. This is known as the "external field effect" (EFE).^{[1]}
The external field effect is best described by classifying physical systems according to their relative values of a_{in} (the characteristic acceleration of one object within a subsystem due to the influence of another), a_{ex} (the acceleration of the entire subsystem due to forces exerted by objects outside of it), and a_{0}:
 : Newtonian regime
 : DeepMOND regime
 : The external field is dominant and the behaviour of the system is Newtonian.
 : The external field is larger than the internal acceleration of the system, but both are smaller than the critical value. In this case, dynamics is Newtonian but the effective value of G is enhanced by a factor of a_{0}/a_{ex}.^{[35]}
The external field effect implies a fundamental break with the strong equivalence principle (but not necessarily the weak equivalence principle). The effect was postulated by Milgrom in the first of his 1983 papers to explain why some open clusters were observed to have no mass discrepancy even though their internal accelerations were below a_{0}. It has since come to be recognised as a crucial element of the MOND paradigm.
The dependence in MOND of the internal dynamics of a system on its external environment (in principle, the rest of the universe) is strongly reminiscent of Mach's Principle, and may hint towards a more fundamental structure underlying Milgrom's law. In this regard, Milgrom has commented:^{[36]}
 "It has been long suspected that local dynamics is strongly influenced by the universe at large, ala Mach’s Principle, but MOND seems to be the first to supply concrete evidence for such a connection. This may turn out to be the most fundamental implication of MOND, beyond its implied modification of Newtonian dynamics and General Relativity, and beyond the elimination of dark matter."
Indeed, the potential link between MONDian dynamics and the universe as a whole (that is, cosmology) is augmented by the observation that the value of a_{0} (determined by fits to internal properties of galaxies) is within an order of magnitude of cH_{0}, where c is the speed of light and H_{0} is the Hubble constant (a measure of the presentday expansion rate of the universe).^{[1]} It is also close to the acceleration rate of the universe, and hence the cosmological constant. However, as yet no full theory has been constructed which manifests these connections in a natural way.
Responses and criticism
Attempts to explain MOND phenomenology using dark matter
While acknowledging that Milgrom's law provides a succinct and accurate description of a range of galactic phenomena, many physicists reject the idea that classical dynamics itself needs to be modified and attempt instead to explain the law's success by reference to the behaviour of dark matter. Some effort has gone towards establishing the presence of a characteristic acceleration scale as a natural consequence of the behaviour of cold dark matter halos,^{[37]}^{[38]} although Milgrom has argued that such arguments explain only a small subset of MOND phenomenology.^{[39]} An alternative proposal is to modify the properties of dark matter (e.g. to make it interact strongly with itself or baryons) in order to induce the tight coupling between the baryonic and dark matter mass that the observations point to.^{[40]} Finally, some researchers suggest that explaining the empirical success of Milgrom's law requires a more radical break with conventional assumptions about the nature of dark matter. One idea (dubbed "dipolar dark matter") is to make dark matter gravitationally polarisable by ordinary matter and have this polarisation enhance the gravitational attraction between baryons.^{[41]}
Outstanding problems for MOND
The most serious problem facing Milgrom's law is that it cannot completely eliminate the need for dark matter in all astrophysical systems: galaxy clusters show a residual mass discrepancy even when analysed using MOND.^{[2]} The fact that some form of unseen mass must exist in these systems detracts from the elegance of MOND as a solution to the missing mass problem, although the amount of extra mass required is 5 times less than in a Newtonian analysis, and there is no requirement that the missing mass be nonbaryonic. It has been speculated that a 2 eV sterile neutrino could account for the cluster observations in MOND while preserving the theory's successes at the galaxy scale.^{[42]}
The 2006 observation of a pair of colliding galaxy clusters known as the "Bullet Cluster"^{[43]} poses a significant challenge for all theories proposing a modified gravity solution to the missing mass problem, including MOND. Astronomers measured the distribution of stellar and gas mass in the clusters using visible and Xray light, respectively, and in addition mapped the inferred dark matter density using gravitational lensing. In MOND, one would expect the missing mass (which is only apparent since it results from using incorrect Newtonian as opposed to MONDian dynamics) to be centred on the visible mass. In ΛCDM, on the other hand, one would expect the dark matter to be significantly offset from the visible mass because the halos of the two colliding clusters would pass through each other (assuming, as is conventional, that dark matter is collisionless), whilst the cluster gas would interact and end up at the centre. An offset is clearly seen in the observations. It has been suggested, however, that MONDbased models may be able to generate such an offset in strongly nonsphericallysymmetric systems, such as the Bullet Cluster.^{[44]}
Several other studies have noted observational difficulties with MOND. For example, it has been claimed that MOND offers a poor fit to the velocity dispersion profile of globular clusters and the temperature profile of galaxy clusters,^{[45]}^{[46]} that different values of a_{0} are required for agreement with different galaxies' rotation curves,^{[47]} and that MOND is naturally unsuited to forming the basis of a theory of cosmology.^{[3]}
Besides these observational issues, MOND and its generalisations are plagued by theoretical difficulties.^{[3]}^{[48]} Several adhoc and inelegent additions to general relativity are required to create a theory with a nonNewtonian nonrelativistic limit, the plethora of different versions of the theory offer diverging predictions in simple physical situations and thus make it difficult to test the framework conclusively, and some formulations (most prominently those based on modified inertia) have long suffered from poor compatibility with cherished physical principles such as conservation laws.
Proposals for testing MOND
Several observational and experimental tests have been proposed to help distinguish^{[49]} between MOND and dark matterbased models:
 The detection of particles suitable for constituting cosmological dark matter would strongly suggest that ΛCDM is correct and no modification to Newton's laws is required.
 MOND predicts the existence of anomalous accelerations on the Earth at particular places and times of the year. These could be detected in a precision experiment.^{[50]}^{[51]}
 It has been suggested that MOND could be tested in the Solar System using the forthcoming LISA Pathfinder mission (scheduled for launch in 2015). In particular, it may be possible to detect the anomalous tidal stresses predicted by MOND to exist at the EarthSun saddlepoint of the Newtonian gravitational potential.^{[52]} It may also be possible to measure MOND corrections to the perihelion precession of the planets in the Solar System,^{[53]} or a purposebuilt spacecraft.^{[54]}
 One potential astrophysical test of MOND is to investigate whether isolated galaxies behave differently to otherwiseidentical galaxies that are under the influence of a strong external field. Another is to search for nonNewtonian behaviour in the motion of binary star systems where the stars are sufficiently separated for their accelerations to be below a_{0}.^{[55]}
See also
References
 ↑ ^{1.0} ^{1.1} ^{1.2} ^{1.3} {{#invoke:Citation/CS1citation CitationClass=journal }}. {{#invoke:Citation/CS1citation CitationClass=journal }}. {{#invoke:Citation/CS1citation CitationClass=journal }}.
 ↑ ^{2.0} ^{2.1} ^{2.2} ^{2.3} {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ ^{3.0} ^{3.1} ^{3.2} {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ Data are from: {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ Babcock, H, 1939, "The rotation of the Andromeda Nebula", Lick Observatory bulletin ; no. 498
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ G. Gentile, B. Famaey, W.J.G. de Blok (2011). "THINGS about MOND", Astron. Astrophys. 527, A76. Template:Arxiv
 ↑ B. Famaey, J. Binney (2005), "Modified Newtonian Dynamics in the Milky Way", MNRAS, Template:Arxiv
 ↑ M. Milgrom, "MOND  Particularly as Modified Inertia", Template:Arxiv
 ↑ ^{12.0} ^{12.1} ^{12.2} ^{12.3} ^{12.4} ^{12.5} B. Famaey and S. McGaugh, "Modified Newtonian Dynamics (MOND): Observational Phenomenology and Relativistic Extensions", Template:Arxiv
 ↑ Pavel Kroupa – The vast polar structures around the Milky Way and Andromeda, YouTube, Nov. 18, 2013 Pavel Kroupa claims that the majority opinion is wrong and that empirical evidence rules out the ΛCDM model.
 ↑ M. Milgrom (2013), "MOND Laws of Galaxy Dynamics", Template:Arxiv
 ↑ S. S. McGaugh, J. M. Schombert, G. D. Bothun,2 and W. J. G. de Blok (2000), "The Baryonic TullyFisher Relation", Template:Arxiv
 ↑ S. McGaugh (2011), "The Baryonic TullyFisher Relation of GasRich Galaxies as a Test of ΛCDM and MOND", ApJ, Template:Arxiv
 ↑ R. Sanders, "Mass discrepancies in galaxies: dark matter and alternatives", The Astronomy and Astrophysics Review 1990, Volume 2, Issue 1, pp 128
 ↑ S. McGaugh (2004), "The Mass DiscrepancyAcceleration Relation: Disk Mass and the Dark Matter Distribution", ApJ, Template:Arxiv
 ↑ M. A. Jimenez and X. Hernandez (2014), "Local galactic disk stability under MONDian gravity", Template:Arxiv
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}</
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ F. Bournaud, P.A. Duc, E. Brinks, M. Boquien, P. Amram, U. Lisenfeld, B. S. Koribalski, F. Walter, V. Charmandaris (2007), "Missing Mass in Collisional Debris from Galaxies", Template:Arxiv
 ↑ G. Gentile, B. Famaey, F. Combes, P. Kroupa, H. S. Zhao, O. Tiret (2007), "Tidal dwarf galaxies as a test of fundamental physics" Template:Arxiv}
 ↑ P. Kroupa (2012), "The dark matter crisis: falsification of the current standard model of cosmology", Template:Arxiv
 ↑ P. Kroupa (2014), "Lessons from the Local Group (and beyond) on dark matter", Template:Arxiv
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ M. Milgrom (2010), "Quasilinear formulation of MOND", Template:Arxiv
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ T. Clifton, P. G. Ferreira, A. Padilla, C. Skordis (2011), "Modified Gravity and Cosmology", Template:Arxiv
 ↑ See Slosar, Melchiorri and Silk Template:Arxiv
 ↑ {{#invoke:citation/CS1citation CitationClass=citation }}
 ↑ {{#invoke:citation/CS1citation CitationClass=citation }}
 ↑ S. McGaugh, The EFE in MOND
 ↑ M. Milgrom (2008), "The MOND paradigm", Template:Arxiv
 ↑ M. Kaplinghat and M. Turner (2012), "How Cold Dark Matter Theory Explains Milgrom’s Law", Template:Arxiv
 ↑ M. H. Chan (2013), "Reconciliation of MOND and Dark Matter theory", Template:Arxiv
 ↑ M. Milgrom (2002), "Do Modified Newtonian Dynamics Follow from the Cold Dark Matter Paradigm?", Template:Arxiv
 ↑ J. Bullock (2014), SelfInteracting Dark Matter
 ↑ L. Blanchet, "Gravitational polarization and the phenomenology of MOND", Class. Quan tum Grav., 24, 3529–3539, (2007), Template:ArXiv
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ {{#invoke:citation/CS1citation CitationClass=book }}
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ S. M. Kent, "Dark matter in spiral galaxies. II  Galaxies with H I rotation curves", 1987, AJ, 93, 816
 ↑ C. R. Contaldi, T. Wiseman, B. Withers (2008), "TeVeS gets caught on caustics", Template:Arxiv
 ↑ {{#invoke:Citation/CS1citation CitationClass=journal }}
 ↑ A. Ignatiev (2014), "Testing MOND on Earth", Template:Arxiv
 ↑ V. A. De Lorenci, M. FaundezAbans, J. P. Pereira (2010). "Testing the Newton second law in the regime of small accelerations" Template:Arxiv
 ↑ Christian Trenkel, Steve Kemble, Neil Bevis, Joao Magueijo (2010). "Testing MOND/TEVES with LISA Pathfinder" Template:Arxiv
 ↑ L. Blanchet (2011), "Testing MOND in the Solar System", Template:Arxiv
 ↑ V. Sahni, Y. Shtanov (2006), "APSIS  an Artificial Planetary System in Space to probe extradimensional gravity and MOND", Template:Arxiv
 ↑ X. Hernandez, M. A. Jimenez, and C. Allen (2012), "Wide binaries as a critical test of Classical Gravity", Template:Arxiv
Further reading
Technical:
 Scholarpedia entry on the subject written by Mordehai Milgrom
 Modified Newtonian Dynamics: Observational Phenomenology and Relativistic Extensions, Famaey, McGaugh, 16 Dec 2011, updated 20 May 2012
 A Tale of Two Paradigms: the Mutual Incommensurability of LCDM and MOND, McGaugh, 29 Apr 2014, updated 17 May 2014
 MOND Theory, Milgrom, 30 Apr 2014, updated 31 Aug 2014
 Galaxies as simple dynamical systems: observational data disfavor dark matter and stochastic star formation, Kroupa, 18 Jun 2014
 Modified Gravity and Cosmology, Clifton, 13 Jun 2011, updated 12 Mar 2012
 Alternatives to Dark Matter and Dark Energy, Mannheim, 12 May 2005, updated 1 Aug 2005
Popular:
 MOND: time for a change of mind?, Milgrom, 26 Aug 2009
 "Dark matter" doubters not silenced yet, World Science, 2 Aug 2007
 Does Dark Matter Really Exist?, Milgrom, Scientific American, Aug 2002
 Dark matter critics focus on details, ignore big picture, Lee, 14 Nov 2012
External links
 The MOND pages, Stacy McGaugh
 Mordehai Milgrom's website
 "The Dark Matter Crisis" blog, Pavel Kroupa, Marcel Pawlowski
 Pavel Kroupa's website