The main features of TeVeS can be summarized as follows:
- As it is derived from the action principle, TeVeS respects conservation laws;
- In the weak-field approximation of the spherically symmetric, static solution, TeVeS reproduces the MOND acceleration formula;
- TeVeS avoids the problems of earlier attempts to generalize MOND, such as superluminal propagation;
- As it is a relativistic theory it can accommodate gravitational lensing.
The theory is based on the following ingredients:
- A unit vector field;
- A dynamical scalar field;
- A nondynamical scalar field;
- A matter Lagrangian constructed using an alternate metric;
- An arbitrary dimensionless function.
These components are combined into a relativistic Lagrangian density, which forms the basis of TeVeS theory.
MOND is a phenomenological modification of the Newtonian acceleration law. In Newtonian gravity theory, the gravitational acceleration in the spherically symmetric, static field of a point mass at distance from the source can be written as
where is Newton's constant of gravitation. The corresponding force acting on a test mass is
To account for the anomalous rotation curves of spiral galaxies, Milgrom proposed a modification of this force law in the form
where is an arbitrary function subject to the following conditions:
In this form, MOND is not a complete theory: for instance, it violates the law of momentum conservation.
However, such conservation laws are automatically satisfied for physical theories that are derived using an action principle. This led Bekenstein to a first, nonrelativistic generalization of MOND. This theory, called AQUAL (for A QUAdratic Lagrangian) is based on the Lagrangian
where is the Newtonian gravitational potential, is the mass density, and is a dimensionless function.
In the case of a spherically symmetric, static gravitational field, this Lagrangian reproduces the MOND acceleration law after the substitutions and are made.
Bekenstein further found that AQUAL can be obtained as the nonrelativistic limit of a relativistic field theory. This theory is written in terms of a Lagrangian that contains, in addition to the Einstein-Hilbert action for the metric field , terms pertaining to a unit vector field and two scalar fields and , of which only is dynamical. The TeVeS action, therefore, can be written as
The terms in this action include the Einstein-Hilbert Lagrangian (using a metric signature and setting the speed of light, ):
where is the Ricci scalar and is the determinant of the metric tensor.
The scalar field Lagrangian is
with , is a constant length, is the dimensionless parameter and an unspecified dimensionless function; while the vector field Lagrangian is
where , while is a dimensionless parameter. and are respectively called the scalar and vector coupling constants of the theory. The consistency between the Gravitoelectromagnetism of the TeVeS theory and that predicted and measured by the general relativity leads to .
In particular, incorporates a Lagrange multiplier term that guarantees that the vector field remains a unit vector field.
The function in TeVeS is unspecified.
TeVeS also introduces a "physical metric" in the form
The action of ordinary matter is defined using the physical metric:
where covariant derivatives with respect to are denoted by .
TeVeS solves problems associated with earlier attempts to generalize MOND, such as superluminal propagation. In his paper, Bekenstein also investigated the consequences of TeVeS in relation to gravitational lensing and cosmology.
Problems and criticisms 
In addition to its ability to account for the flat rotation curves of galaxies (which is what MOND was originally designed to address), TeVeS is claimed to be consistent with a range of other phenomena, such as gravitational lensing and cosmological observations. However, Seifert shows that with Bekenstein's proposed parameters, a TeVeS star is highly unstable, on the scale of approximately 106 seconds (two weeks). The ability of the theory to simultaneously account for galactic dynamics and lensing is also challenged. A possible resolution may be in the form of massive (around 2eV) neutrinos.
A study in August 2006 reported an observation of a pair of colliding galaxy clusters, the Bullet Cluster, whose behavior, it was reported, was not compatible with any current modified gravity theories.
A quantity  probing General Relativity (GR) on large scales (a hundred billion times the size of the solar system) for the first time has been measured with data from the Sloan Digital Sky Survey to be (~16%) consistent with GR, GR plus Lambda CDM and the extended form of GR known as theory, but ruling out a particular TeVeS model predicting . This estimate should improve to ~1% with the next generation of sky surveys and may put tighter constraints on the parameter space of all modified gravity theories.
See also 
- Modified Newtonian Dynamics
- Scalar–tensor–vector gravity
- General theory of relativity
- Law of universal gravitation
- Pioneer anomaly
- Nonsymmetric Gravitational Theory
- Dark matter
- Dark energy
- Dark fluid
- Scalar - scalar field
- Jacob D. Bekenstein (2004), "Relativistic gravitation theory for the modified Newtonian dynamics paradigm", Phys. Rev. D 70 (8): 083509, arXiv:astro-ph/0403694, Bibcode:2004PhRvD..70h3509B, doi:10.1103/PhysRevD.70.083509
- M. Milgrom (1983), "A modification of the Newtonian dynamics as a possible alternative to the hidden mass hypothesis", Astrophys. J. 270: 365–370, Bibcode:1983ApJ...270..365M, doi:10.1086/161130
- Qasem Exirifard (2013), "GravitoMagnetic Field in Tensor-Vector-Scalar Theory", Journal of Cosmology and Astroparticle Physics, JCAP04: 034, arXiv:1111.5210v3, doi:10.1088/1475-7516/2013/04/034
- Michael D. Seifert (2007), "Stability of spherically symmetric solutions in modified theories of gravity", Phys. Rev. D 76 (6): 064002, arXiv:gr-qc/0703060, Bibcode:2007PhRvD..76f4002S, doi:10.1103/PhysRevD.76.064002
- Mavromatos, Nick E.; Sakellariadou, Mairi; Yusaf, Muhammad Furqaan (2009), "Can TeVeS avoid Dark Matter on galactic scales?", Phys. Rev. D 79 (8): 081301, arXiv:0901.3932, Bibcode:2009PhRvD..79h1301M, doi:10.1103/PhysRevD.79.081301
- Angus, G. W.; Shan, H. Y.; Zhao, H. S.; Famaey, B. (2007), "On the Proof of Dark Matter, the Law of Gravity, and the Mass of Neutrinos]", Astrophys. J. 654 (1): L13–L16, arXiv:astro-ph/0609125, Bibcode:2007ApJ...654L..13A, doi:10.1086/510738
- Douglas Clowe, et al. "A direct empirical proof of the existence of dark matter", Astrophys. J. 648, L109-L113 (2006), arXiv:astro-ph/0608407
- Zhang, P.; Liguori, M.; Bean, R. and Dodelson, S. (oct 2007), "Probing Gravity at Cosmological Scales by Measurements which Test the Relationship between Gravitational Lensing and Matter Overdensity", Physical Review Letters 99 (14): 141302–+, arXiv:0704.1932, Bibcode:2007PhRvL..99n1302Z, doi:10.1103/PhysRevLett.99.141302.
- Reyes, R. et al (mar 2010), "Confirmation of general relativity on large scales from weak lensing and galaxy velocities", Nature 464 (7286): 256–258, arXiv:1003.2185, Bibcode:2010Natur.464..256R, doi:10.1038/nature08857, PMID 20220843.
Further reading 
- Dark Matter Observed (SLAC today)
- Einstein's Theory 'Improved'? (PPARC)
- J.D. Bekenstein and R.H. Sanders, "A Primer to Relativistic MOND Theory", arXiv:astro-ph/0509519
- H.S. Zhao and B. Famaey, "Refining MOND interpolating function and TeVeS Lagrangian", Astrophys. J. 638, L9-L12 (2006), arXiv:astro-ph/0512425
- Einstein Was Right: General Relativity Confirmed ' TeVeS, however, made predictions that fell outside the observational error limits', ( www.space.com, 2010.03.10)