Alternatives to general relativity
This article's factual accuracy is
disputed. (February 2016) 
Alternatives to general relativity are physical theories that attempt to describe the phenomenon of gravitation in competition to Einstein's theory of general relativity. There have been many different attempts at constructing an ideal theory of gravity.^{ [1]}
These attempts can be split into four broad categories based on their scope. In this article, straightforward alternatives to general relativity are discussed, which do not involve quantum mechanics or force unification. Other theories which do attempt to construct a theory using the principles of quantum mechanics are known as theories of quantized gravity. Thirdly, there are theories which attempt to explain gravity and other forces at the same time; these are known as classical unified field theories. Finally, the most ambitious theories attempt to both put gravity in quantum mechanical terms and unify forces; these are called theories of everything.
None of these alternatives to general relativity have gained wide acceptance. General relativity has withstood many tests, remaining consistent with all observations so far. In contrast, many of the early alternatives have been definitively disproven. However, some of the alternative theories of gravity are supported by a minority of physicists, and the topic remains the subject of intense study in theoretical physics.
History of gravitational theory through general relativity
At the time it was published in the 17th century, Isaac Newton's theory of gravity was the most accurate theory of gravity. Since then, a number of alternatives were proposed. The theories which predate the formulation of general relativity in 1915 are discussed in history of gravitational theory.
General relativity
This theory^{ [2]}^{ [3]} is what we now call "general relativity" (included here for comparison). Discarding the Minkowski metric entirely, Einstein gets:
which can also be written
Five days before Einstein presented the last equation above, Hilbert had submitted a paper containing an almost identical equation. See General relativity priority dispute. Hilbert was the first to correctly state the Einstein–Hilbert action for general relativity, which is:
where is Newton's gravitational constant, is the Ricci curvature of space, and is the action due to mass.
General relativity is a tensor theory, the equations all contain tensors. Nordström's theories, on the other hand, are scalar theories because the gravitational field is a scalar. Other proposed alternatives include scalartensor theories that contain a scalar field in addition to the tensors of general relativity, and other variants containing vector fields as well have been developed recently.
Motivations
After general relativity, attempts were made either to improve on theories developed before general relativity, or to improve general relativity itself. Many different strategies were attempted, for example the addition of spin to general relativity, combining a general relativitylike metric with a spacetime that is static with respect to the expansion of the universe, getting extra freedom by adding another parameter. At least one theory was motivated by the desire to develop an alternative to general relativity that is free of singularities.
Experimental tests improved along with the theories. Many of the different strategies that were developed soon after general relativity were abandoned, and there was a push to develop more general forms of the theories that survived, so that a theory would be ready when any test showed a disagreement with general relativity.
By the 1980s, the increasing accuracy of experimental tests had all confirmed general relativity; no competitors were left except for those that included general relativity as a special case. Further, shortly after that, theorists switched to string theory which was starting to look promising, but has since lost popularity. In the mid1980s a few experiments were suggesting that gravity was being modified by the addition of a fifth force (or, in one case, of a fifth, sixth and seventh force) acting in the range of a few meters. Subsequent experiments eliminated these.
Motivations for the more recent alternative theories are almost all cosmological, associated with or replacing such constructs as " inflation", " dark matter" and " dark energy". Investigation of the Pioneer anomaly has caused renewed public interest in alternatives to general relativity.
Notation in this article
is the speed of light, is the gravitational constant. " Geometric variables" are not used.
Latin indices go from 1 to 3, Greek indices go from 0 to 3. The Einstein summation convention is used.
is the Minkowski metric. is a tensor, usually the metric tensor. These have signature (−,+,+,+).
Partial differentiation is written or . Covariant differentiation is written or .
Classification of theories
Theories of gravity can be classified, loosely, into several categories. Most of the theories described here have:
 an ' action' (see the principle of least action, a variational principle based on the concept of action)
 a Lagrangian density
 a metric
If a theory has a Lagrangian density for gravity, say , then the gravitational part of the action is the integral of that:
 .
In this equation it is usual, though not essential, to have at spatial infinity when using Cartesian coordinates. For example, the Einstein–Hilbert action uses
where R is the scalar curvature, a measure of the curvature of space.
Almost every theory described in this article has an action. It is the most efficient known way to guarantee that the necessary conservation laws of energy, momentum and angular momentum are incorporated automatically; although it is easy to construct an action where those conservation laws are violated. Canonical methods provide another way to construct systems that have the required conservation laws, but this approach is more cumbersome to implement.^{ [4]} The original 1983 version of MOND did not have an action.
A few theories have an action but not a Lagrangian density. A good example is Whitehead,^{ [5]} the action there is termed nonlocal.
A theory of gravity is a "metric theory" if and only if it can be given a mathematical representation in which two conditions hold:
Condition 1: There exists a symmetric
metric tensor of
signature (−, +, +, +), which governs properlength and propertime measurements in the usual manner of special and general relativity:
where there is a summation over indices and .
Condition 2: Stressed matter and fields being acted upon by gravity respond in accordance with the equation:
where is the stress–energy tensor for all matter and nongravitational fields, and where is the covariant derivative with respect to the metric and is the Christoffel symbol. The stress–energy tensor should also satisfy an energy condition.
Metric theories include (from simplest to most complex):

Scalar field theories (includes Conformally flat theories & Stratified theories with conformally flat space slices)
 Bergman
 Coleman
 Einstein (1912)
 Einstein–Fokker theory
 Lee– Lightman– Ni
 Littlewood
 Ni
 Nordström's theory of gravitation (first metric theory of gravity to be developed)
 Page–Tupper
 Papapetrou
 Rosen (1971)
 Whitrow–Morduch
 Yilmaz theory of gravitation (attempted to eliminate event horizons from the theory.)

Quasilinear theories (includes Linear fixed gauge)
 Bollini–Giambiagi–Tiomno
 Deser–Laurent
 Whitehead's theory of gravity (intended to use only retarded potentials)

Tensor theories
 Einstein's general relativity
 Fourthorder gravity (allows the Lagrangian to depend on secondorder contractions of the Riemann curvature tensor)
 f(R) gravity (allows the Lagrangian to depend on higher powers of the Ricci scalar)
 Gauss–Bonnet gravity
 Lovelock theory of gravity (allows the Lagrangian to depend on higherorder contractions of the Riemann curvature tensor)
 Infinite derivative gravity

Scalartensor theories
 Bekenstein
 Bergmann–Wagoner
 Brans–Dicke theory (the most wellknown alternative to general relativity, intended to be better at applying Mach's principle)
 Jordan
 Nordtvedt
 Thiry
 Chameleon
 Pressuron
 Vectortensor theories
 Bimetric theories
 Other metric theories
(see section Modern theories below)
Nonmetric theories include
 Belinfante–Swihart
 Einstein–Cartan theory (intended to handle spinorbital angular momentum interchange)
 Kustaanheimo (1967)
 Teleparallelism
 Gauge theory gravity
A word here about Mach's principle is appropriate because a few of these theories rely on Mach's principle (e.g. Whitehead^{ [5]}), and many mention it in passing (e.g. Einstein–Grossmann,^{ [6]} Brans–Dicke^{ [7]}). Mach's principle can be thought of a halfwayhouse between Newton and Einstein. It goes this way:^{ [8]}
 Newton: Absolute space and time.
 Mach: The reference frame comes from the distribution of matter in the universe.
 Einstein: There is no reference frame.
So far, all the experimental evidence points to Mach's principle being wrong, but it has not entirely been ruled out.^{[ citation needed]}
Theories from 1917 to the 1980s
This section includes alternatives to general relativity published after general relativity but before the observations of galaxy rotation that led to the hypothesis of " dark matter". Those considered here include (see Will^{ [9]}^{ [10]} Lang^{ [11]}^{ [12]}):
Publication year(s)  Author(s)  Theory name  Theory type 

1922^{ [5]}  Alfred North Whitehead  Whitehead's theory of gravitation  Quasilinear 
1922,^{ [13]} 1923^{ [14]}  Élie Cartan  Einstein–Cartan theory  Nonmetric 
1939^{ [15]}  Markus Fierz, Wolfgang Pauli  
1943^{ [16]}  George David Birkhoff  
1948^{ [17]}  Edward Arthur Milne  Kinematic Relativity  
1948^{ [18]}  Yves Thiry  
1954^{ [19]}^{ [20]}  Achilles Papapetrou  Scalar field  
1953^{ [21]}  Dudley E. Littlewood  Scalar field  
1955^{ [22]}  Pascual Jordan  
1956^{ [23]}  Otto Bergmann  Scalar field  
1957^{ [24]}^{ [25]}  Frederik Belinfante, James C. Swihart  
1958,^{ [26]} 1973^{ [27]}  Huseyin Yilmaz  Yilmaz theory of gravitation  
1961^{ [7]}  Carl H. Brans, Robert H. Dicke  Brans–Dicke theory  Scalartensor 
1960,^{ [28]} 1965^{ [29]}  Gerald James Whitrow, G. E. Morduch  Scalar field  
1966^{ [30]}  Paul Kustaanheimo  
1967^{ [31]}  Paul Kustaanheimo , V. S. Nuotio  
1968^{ [32]}  Stanley Deser, B. E. Laurent  Quasilinear  
1968^{ [33]}  C. Page, B. O. J. Tupper  Scalar field  
1968^{ [34]}  Peter Bergmann  Scalartensor  
1970^{ [35]}  C. G. Bollini, J. J. Giambiagi, J. Tiomno  Quasilinear  
1970^{ [36]}  Kenneth Nordtvedt  
1970^{ [37]}  Robert V. Wagoner  Scalartensor  
1971^{ [38]}  Nathan Rosen  Scalar field  
1975^{ [39]}  Nathan Rosen  Bimetric  
1972,^{ [10]} 1973^{ [40]}  Ni Weitou  Scalar field  
1972^{ [41]}  Clifford Martin Will, Kenneth Nordtvedt  Vectortensor  
1973^{ [42]}  Ronald Hellings, Kenneth Nordtvedt  Vectortensor  
1973^{ [43]}  Alan Lightman, David L. Lee  Scalar field  
1974^{ [44]}  David L. Lee, Alan Lightman, Ni Weitou  
1977^{ [45]}  Jacob Bekenstein  Scalartensor  
1978^{ [46]}  B. M. Barker  Scalartensor  
1979^{ [47]}  P. Rastall  Bimetric 
These theories are presented here without a cosmological constant or added scalar or vector potential unless specifically noted, for the simple reason that the need for one or both of these was not recognised before the supernova observations by the Supernova Cosmology Project and HighZ Supernova Search Team. How to add a cosmological constant or quintessence to a theory is discussed under Modern Theories (see also Einstein–Hilbert action).
Scalar field theories
The scalar field theories of Nordström^{ [48]}^{ [49]} have already been discussed. Those of Littlewood,^{ [21]} Bergman,^{ [23]} Yilmaz,^{ [26]} Whitrow and Morduch^{ [28]}^{ [29]} and Page and Tupper^{ [33]} follow the general formula give by Page and Tupper.
According to Page and Tupper,^{ [33]} who discuss all these except Nordström,^{ [49]} the general scalar field theory comes from the principle of least action:
where the scalar field is,
and c may or may not depend on .
In Nordström,^{ [48]}
In Littlewood^{ [21]} and Bergmann,^{ [23]}
In Whitrow and Morduch,^{ [28]}
In Whitrow and Morduch,^{ [29]}
In Page and Tupper,^{ [33]}
Page and Tupper^{ [33]} matches Yilmaz's theory^{ [26]} to second order when .
The gravitational deflection of light has to be zero when c is constant. Given that variable c and zero deflection of light are both in conflict with experiment, the prospect for a successful scalar theory of gravity looks very unlikely. Further, if the parameters of a scalar theory are adjusted so that the deflection of light is correct then the gravitational redshift is likely to be wrong.
Ni^{ [10]} summarised some theories and also created two more. In the first, a preexisting special relativity spacetime and universal time coordinate acts with matter and nongravitational fields to generate a scalar field. This scalar field acts together with all the rest to generate the metric.
The action is:
Misner et al.^{ [50]} gives this without the term. is the matter action.
t is the universal time coordinate. This theory is selfconsistent and complete. But the motion of the solar system through the universe leads to serious disagreement with experiment.
In the second theory of Ni^{ [10]} there are two arbitrary functions and that are related to the metric by:
Ni^{ [10]} quotes Rosen^{ [38]} as having two scalar fields and that are related to the metric by:
In Papapetrou^{ [19]} the gravitational part of the Lagrangian is:
In Papapetrou^{ [20]} there is a second scalar field . The gravitational part of the Lagrangian is now:
Bimetric theories
Bimetric theories contain both the normal tensor metric and the Minkowski metric (or a metric of constant curvature), and may contain other scalar or vector fields.
Rosen^{ [51]} (1975) bimetric theory The action is:
Lightman–Lee^{ [43]} developed a metric theory based on the nonmetric theory of Belinfante and Swihart.^{ [24]}^{ [25]} The result is known as BSLL theory. Given a tensor field , , and two constants and the action is:
and the stress–energy tensor comes from:
In Rastall,^{ [47]} the metric is an algebraic function of the Minkowski metric and a Vector field.^{ [52]} The Action is:
where
 and
(see Will^{ [9]} for the field equation for and ).
Quasilinear theories
In Whitehead,^{ [5]} the physical metric is constructed (by Synge) algebraically from the Minkowski metric and matter variables, so it doesn't even have a scalar field. The construction is:
where the superscript (−) indicates quantities evaluated along the past light cone of the field point and
Nevertheless, the metric construction (from a nonmetric theory) using the "length contraction" ansatz is criticised.^{ [53]}
Deser and Laurent^{ [32]} and Bollini–Giambiagi–Tiomno^{ [35]} are Linear Fixed Gauge theories. Taking an approach from quantum field theory, combine a Minkowski spacetime with the gauge invariant action of a spintwo tensor field (i.e. graviton) to define
The action is:
The Bianchi identity associated with this partial gauge invariance is wrong. Linear Fixed Gauge theories seek to remedy this by breaking the gauge invariance of the gravitational action through the introduction of auxiliary gravitational fields that couple to .
A cosmological constant can be introduced into a quasilinear theory by the simple expedient of changing the Minkowski background to a de Sitter or antide Sitter spacetime, as suggested by G. Temple in 1923. Temple's suggestions on how to do this were criticized by C. B. Rayner in 1955.^{ [54]}
Tensor theories
Einstein's general relativity is the simplest plausible theory of gravity that can be based on just one symmetric tensor field (the metric tensor). Others include: Starobinsky (R+R^2) gravity, Gauss–Bonnet gravity, f(R) gravity, and Lovelock theory of gravity.
Starobinsky
Starobinsky gravity, proposed by Alexei Starobinsky has the Lagrangian
and has been used to explain inflation, in the form of Starobinsky inflation. Here is a constant.
Gauss–Bonnet
Gauss–Bonnet gravity has the action
where the coefficients of the extra terms are chosen so that the action reduces to general relativity in 4 spacetime dimensions and the extra terms are only nontrivial when more dimensions are introduced.
Stelle's 4th derivative gravity
Stelle's 4th derivative gravity, which is a generalisation of Gauss–Bonnet gravity, has the action
f(R)
f(R) gravity has the action
and is a family of theories, each defined by a different function of the Ricci scalar. Starobinsky gravity is actually an theory.
Infinite derivative gravity
Infinite derivative gravity is a covariant theory of gravity, quadratic in curvature, torsion free and parity invariant,^{ [55]}
and
in order to make sure that only massless spin −2 and spin −0 components propagate in the graviton propagator around Minkowski background. The action becomes nonlocal beyond the scale , and recovers to general relativity in the infrared, for energies below the nonlocal scale . In the ultraviolet regime, at distances and time scales below nonlocal scale, , the gravitational interaction weakens enough to resolve pointlike singularity, which means Schwarzschild's singularity can be potentially resolved in infinite derivative theories of gravity.
Lovelock
Lovelock gravity has the action
and can be thought of as a generalisation of general relativity.
Scalartensor theories
These all contain at least one free parameter, as opposed to general relativity which has no free parameters.
Although not normally considered a ScalarTensor theory of gravity, the 5 by 5 metric of Kaluza–Klein reduces to a 4 by 4 metric and a single scalar. So if the 5th element is treated as a scalar gravitational field instead of an electromagnetic field then Kaluza–Klein can be considered the progenitor of ScalarTensor theories of gravity. This was recognised by Thiry.^{ [18]}
ScalarTensor theories include Thiry,^{ [18]} Jordan,^{ [22]} Brans and Dicke,^{ [7]} Bergman,^{ [34]} Nordtveldt (1970), Wagoner,^{ [37]} Bekenstein^{ [45]} and Barker.^{ [46]}
The action is based on the integral of the Lagrangian .
where is a different dimensionless function for each different scalartensor theory. The function plays the same role as the cosmological constant in general relativity. is a dimensionless normalization constant that fixes the presentday value of . An arbitrary potential can be added for the scalar.
The full version is retained in Bergman^{ [34]} and Wagoner.^{ [37]} Special cases are:
Nordtvedt,^{ [36]}
Since was thought to be zero at the time anyway, this would not have been considered a significant difference. The role of the cosmological constant in more modern work is discussed under Cosmological constant.
Brans–Dicke,^{ [7]} is constant
Bekenstein^{ [45]} variable mass theory Starting with parameters and , found from a cosmological solution, determines function then
Barker^{ [46]} constant G theory
Adjustment of allows Scalar Tensor Theories to tend to general relativity in the limit of in the current epoch. However, there could be significant differences from general relativity in the early universe.
So long as general relativity is confirmed by experiment, general ScalarTensor theories (including Brans–Dicke^{ [7]}) can never be ruled out entirely, but as experiments continue to confirm general relativity more precisely and the parameters have to be finetuned so that the predictions more closely match those of general relativity.
The above examples are particular cases of Horndeski's theory,^{ [56]}^{ [57]} the most general Lagrangian constructed out of the metric tensor and a scalar field leading to second order equations of motion in 4dimensional space. Viable theories beyond Horndeski (with higher order equations of motion) have been shown to exist.^{ [58]}^{ [59]}^{ [60]}
Vectortensor theories
Before we start, Will (2001) has said: "Many alternative metric theories developed during the 1970s and 1980s could be viewed as "strawman" theories, invented to prove that such theories exist or to illustrate particular properties. Few of these could be regarded as wellmotivated theories from the point of view, say, of field theory or particle physics. Examples are the vectortensor theories studied by Will, Nordtvedt and Hellings."
Hellings and Nordtvedt^{ [42]} and Will and Nordtvedt^{ [41]} are both vectortensor theories. In addition to the metric tensor there is a timelike vector field The gravitational action is:
where are constants and
 (See Will^{ [9]} for the field equations for and )
Will and Nordtvedt^{ [41]} is a special case where
Hellings and Nordtvedt^{ [42]} is a special case where
These vectortensor theories are semiconservative, which means that they satisfy the laws of conservation of momentum and angular momentum but can have preferred frame effects. When they reduce to general relativity so, so long as general relativity is confirmed by experiment, general vectortensor theories can never be ruled out.
Other metric theories
Others metric theories have been proposed; that of Bekenstein^{ [61]} is discussed under Modern Theories.
Nonmetric theories
Cartan's theory is particularly interesting both because it is a nonmetric theory and because it is so old. The status of Cartan's theory is uncertain. Will^{ [9]} claims that all nonmetric theories are eliminated by Einstein's Equivalence Principle. Will (2001) tempers that by explaining experimental criteria for testing nonmetric theories against Einstein's Equivalence Principle. Misner et al.^{ [50]} claims that Cartan's theory is the only nonmetric theory to survive all experimental tests up to that date and Turyshev^{ [62]} lists Cartan's theory among the few that have survived all experimental tests up to that date. The following is a quick sketch of Cartan's theory as restated by Trautman.^{ [63]}
Cartan^{ [13]}^{ [14]} suggested a simple generalization of Einstein's theory of gravitation. He proposed a model of space time with a metric tensor and a linear "connection" compatible with the metric but not necessarily symmetric. The torsion tensor of the connection is related to the density of intrinsic angular momentum. Independently of Cartan, similar ideas were put forward by Sciama, by Kibble in the years 1958 to 1966, culminating in a 1976 review by Hehl et al.
The original description is in terms of differential forms, but for the present article that is replaced by the more familiar language of tensors (risking loss of accuracy). As in general relativity, the Lagrangian is made up of a massless and a mass part. The Lagrangian for the massless part is:
The is the linear connection. is the completely antisymmetric pseudotensor ( LeviCivita symbol) with , and is the metric tensor as usual. By assuming that the linear connection is metric, it is possible to remove the unwanted freedom inherent in the nonmetric theory. The stress–energy tensor is calculated from:
The space curvature is not Riemannian, but on a Riemannian spacetime the Lagrangian would reduce to the Lagrangian of general relativity.
Some equations of the nonmetric theory of Belinfante and Swihart^{ [24]}^{ [25]} have already been discussed in the section on bimetric theories.
A distinctively nonmetric theory is given by gauge theory gravity, which replaces the metric in its field equations with a pair of gauge fields in flat spacetime. On the one hand, the theory is quite conservative because it is substantially equivalent to Einstein–Cartan theory (or general relativity in the limit of vanishing spin), differing mostly in the nature of its global solutions. On the other hand, it is radical because it replaces differential geometry with geometric algebra.
Modern theories 1980s to present
This section includes alternatives to general relativity published after the observations of galaxy rotation that led to the hypothesis of "dark matter". There is no known reliable list of comparison of these theories. Those considered here include: Bekenstein,^{ [61]} Moffat,^{ [64]} Moffat,^{ [65]} Moffat.^{ [66]}^{ [67]} These theories are presented with a cosmological constant or added scalar or vector potential.
Motivations
Motivations for the more recent alternatives to general relativity are almost all cosmological, associated with or replacing such constructs as "inflation", "dark matter" and "dark energy". The basic idea is that gravity agrees with general relativity at the present epoch but may have been quite different in the early universe.
In the 1980s, there was a slowly dawning realisation in the physics world that there were several problems inherent in the thencurrent bigbang scenario, including the horizon problem and the observation that at early times when quarks were first forming there was not enough space on the universe to contain even one quark. Inflation theory was developed to overcome these difficulties. Another alternative was constructing an alternative to general relativity in which the speed of light was higher in the early universe. The discovery of unexpected rotation curves for galaxies took everyone by surprise. Could there be more mass in the universe than we are aware of, or is the theory of gravity itself wrong? The consensus now is that the missing mass is "cold dark matter", but that consensus was only reached after trying alternatives to general relativity, and some physicists still believe that alternative models of gravity may hold the answer.
In the 1990s, supernova surveys discovered the accelerated expansion of the universe, now usually attributed to dark energy. This led to the rapid reinstatement of Einstein's cosmological constant, and quintessence arrived as an alternative to the cosmological constant. At least one new alternative to general relativity attempted to explain the supernova surveys' results in a completely different way. The measurement of the speed of gravity with the gravitational wave event GW170817 ruled out many alternative theories of gravity as explanations for the accelerated expansion.^{ [68]}^{ [69]}^{ [70]} Another observation that sparked recent interest in alternatives to General Relativity is the Pioneer anomaly. It was quickly discovered that alternatives to general relativity could explain this anomaly. This is now believed to be accounted for by nonuniform thermal radiation.
Cosmological constant and quintessence
The cosmological constant is a very old idea, going back to Einstein in 1917.^{ [3]} The success of the Friedmann model of the universe in which led to the general acceptance that it is zero, but the use of a nonzero value came back with a vengeance when data from supernovae indicated that the expansion of the universe is accelerating
First, let's see how it influences the equations of Newtonian gravity and General Relativity. In Newtonian gravity, the addition of the cosmological constant changes the Newton–Poisson equation from:
to
In general relativity, it changes the Einstein–Hilbert action from
to
which changes the field equation
to
In alternative theories of gravity, a cosmological constant can be added to the action in exactly the same way.
The cosmological constant is not the only way to get an accelerated expansion of the universe in alternatives to general relativity. We've already seen how the scalar potential can be added to scalar tensor theories. This can also be done in every alternative the general relativity that contains a scalar field by adding the term inside the Lagrangian for the gravitational part of the action, the part of
Because is an arbitrary function of the scalar field, it can be set to give an acceleration that is large in the early universe and small at the present epoch. This is known as quintessence.
A similar method can be used in alternatives to general relativity that use vector fields, including Rastall^{ [47]} and vectortensor theories. A term proportional to
is added to the Lagrangian for the gravitational part of the action.
Farnes' theories
In December 2018, the astrophysicist Jamie Farnes from the University of Oxford proposed a dark fluid theory, related to notions of gravitationally repulsive negative masses that were presented earlier by Albert Einstein. The theory may help to better understand the considerable amounts of unknown dark matter and dark energy in the universe.^{ [71]}
The theory relies on the concept of negative mass and reintroduces Fred Hoyle's creation tensor in order to allow matter creation for only negative mass particles. In this way, the negative mass particles surround galaxies and apply a pressure onto them, thereby resembling dark matter. As these hypothesised particles mutually repel one another, they push apart the Universe, thereby resembling dark energy. The creation of matter allows the density of the exotic negative mass particles to remain constant as a function of time, and so appears like a cosmological constant. Einstein's field equations are modified to:
According to Occam's razor, Farnes' theory is a simpler alternative to the conventional LambdaCDM model, as both dark energy and dark matter (two hypotheses) are solved using a single negative mass fluid (one hypothesis). The theory will be directly testable using the world's largest radio telescope, the Square Kilometre Array which should come online in 2022.^{ [72]}
Relativistic MOND
The original theory of MOND by Milgrom was developed in 1983 as an alternative to "dark matter". Departures from Newton's law of gravitation are governed by an acceleration scale, not a distance scale. MOND successfully explains the Tully–Fisher observation that the luminosity of a galaxy should scale as the fourth power of the rotation speed. It also explains why the rotation discrepancy in dwarf galaxies is particularly large.
There were several problems with MOND in the beginning.
 It did not include relativistic effects
 It violated the conservation of energy, momentum and angular momentum
 It was inconsistent in that it gives different galactic orbits for gas and for stars
 It did not state how to calculate gravitational lensing from galaxy clusters.
By 1984, problems 2 and 3 had been solved by introducing a Lagrangian ( AQUAL). A relativistic version of this based on scalartensor theory was rejected because it allowed waves in the scalar field to propagate faster than light. The Lagrangian of the nonrelativistic form is:
The relativistic version of this has:
with a nonstandard mass action. Here and are arbitrary functions selected to give Newtonian and MOND behaviour in the correct limits, and is the MOND length scale. By 1988, a second scalar field (PCC) fixed problems with the earlier scalartensor version but is in conflict with the perihelion precession of Mercury and gravitational lensing by galaxies and clusters. By 1997, MOND had been successfully incorporated in a stratified relativistic theory [Sanders], but as this is a preferred frame theory it has problems of its own. Bekenstein^{ [61]} introduced a tensorvectorscalar model (TeVeS). This has two scalar fields and and vector field . The action is split into parts for gravity, scalars, vector and mass.
The gravity part is the same as in general relativity.
where
are constants, square brackets in indices represent antisymmetrization, is a Lagrange multiplier (calculated elsewhere), and L is a Lagrangian translated from flat spacetime onto the metric . Note that G need not equal the observed gravitational constant . F is an arbitrary function, and
is given as an example with the right asymptotic behaviour; note how it becomes undefined when
The Parametric postNewtonian parameters of this theory are calculated in,^{ [73]} which shows that all its parameters are equal to general relativity's, except for
both of which expressed in geometric units where ; so
Moffat's theories
J. W. Moffat^{ [64]} developed a nonsymmetric gravitation theory. This is not a metric theory. It was first claimed that it does not contain a black hole horizon, but Burko and Ori^{ [74]} have found that nonsymmetric gravitational theory can contain black holes. Later, Moffat claimed that it has also been applied to explain rotation curves of galaxies without invoking "dark matter". Damour, Deser & MaCarthy^{ [75]} have criticised nonsymmetric gravitational theory, saying that it has unacceptable asymptotic behaviour.
The mathematics is not difficult but is intertwined so the following is only a brief sketch. Starting with a nonsymmetric tensor , the Lagrangian density is split into
where is the same as for matter in general relativity.
where is a curvature term analogous to but not equal to the Ricci curvature in general relativity, and are cosmological constants, is the antisymmetric part of . is a connection, and is a bit difficult to explain because it's defined recursively. However,
Haugan and Kauffmann^{ [76]} used polarization measurements of the light emitted by galaxies to impose sharp constraints on the magnitude of some of nonsymmetric gravitational theory's parameters. They also used HughesDrever experiments to constrain the remaining degrees of freedom. Their constraint is eight orders of magnitude sharper than previous estimates.
Moffat's^{ [66]} metricskewtensorgravity (MSTG) theory is able to predict rotation curves for galaxies without either dark matter or MOND, and claims that it can also explain gravitational lensing of galaxy clusters without dark matter. It has variable , increasing to a final constant value about a million years after the big bang.
The theory seems to contain an asymmetric tensor field and a source current vector. The action is split into:
Both the gravity and mass terms match those of general relativity with cosmological constant. The skew field action and the skew field matter coupling are:
where
and is the LeviCivita symbol. The skew field coupling is a Pauli coupling and is gauge invariant for any source current. The source current looks like a matter fermion field associated with baryon and lepton number.
Scalartensorvector gravity
Moffat's Scalar–tensor–vector gravity^{ [67]} contains a tensor, vector and three scalar fields. But the equations are quite straightforward. The action is split into: with terms for gravity, vector field scalar fields and mass. is the standard gravity term with the exception that is moved inside the integral.
The potential function for the vector field is chosen to be:
where is a coupling constant. The functions assumed for the scalar potentials are not stated.
Infinite derivative gravity
In order to remove ghosts in the modified propagator, as well as to obtain asymptotic freedom, Biswas, Mazumdar and Siegel (2005) considered a stringinspired infinite set of higher derivative terms
where is the exponential of an entire function of the D'Alembertian operator.^{ [77]}^{ [78]} This avoids a black hole singularity near the origin, while recovering the 1/r fall of the general relativity potential at large distances.^{ [79]} Lousto and Mazzitelli (1997) found an exact solution to this theories representing a gravitational shockwave.^{ [80]}
Testing of alternatives to general relativity
Any putative alternative to general relativity would need to meet a variety of tests for it to become accepted. For indepth coverage of these tests, see Misner et al.^{ [50]} Ch.39, Will ^{ [9]} Table 2.1, and Ni.^{ [10]} Most such tests can be categorized as in the following subsections.
Selfconsistency
Selfconsistency among nonmetric theories includes eliminating theories allowing tachyons, ghost poles and higher order poles, and those that have problems with behaviour at infinity. Among metric theories, selfconsistency is best illustrated by describing several theories that fail this test. The classic example is the spintwo field theory of Fierz and Pauli;^{ [15]} the field equations imply that gravitating bodies move in straight lines, whereas the equations of motion insist that gravity deflects bodies away from straight line motion. Yilmaz (1971)^{ [27]} contains a tensor gravitational field used to construct a metric; it is mathematically inconsistent because the functional dependence of the metric on the tensor field is not well defined.
Completeness
To be complete, a theory of gravity must be capable of analysing the outcome of every experiment of interest. It must therefore mesh with electromagnetism and all other physics. For instance, any theory that cannot predict from first principles the movement of planets or the behaviour of atomic clocks is incomplete.
Many early theories are incomplete in that it is unclear whether the density used by the theory should be calculated from the stress–energy tensor as or as , where is the fourvelocity, and is the Kronecker delta. The theories of Thirry (1948) and Jordan^{ [22]} are incomplete unless Jordan's parameter is set to 1, in which case they match the theory of Brans–Dicke^{ [7]} and so are worthy of further consideration. Milne^{ [17]} is incomplete because it makes no gravitational redshift prediction. The theories of Whitrow and Morduch,^{ [28]}^{ [29]} Kustaanheimo^{ [30]} and Kustaanheimo and Nuotio^{ [31]} are either incomplete or inconsistent. The incorporation of Maxwell's equations is incomplete unless it is assumed that they are imposed on the flat background spacetime, and when that is done they are inconsistent, because they predict zero gravitational redshift when the wave version of light (Maxwell theory) is used, and nonzero redshift when the particle version (photon) is used. Another more obvious example is Newtonian gravity with Maxwell's equations; light as photons is deflected by gravitational fields (by half that of general relativity) but light as waves is not.
Classical tests
There are three "classical" tests (dating back to the 1910s or earlier) of the ability of gravity theories to handle relativistic effects; they are gravitational redshift, gravitational lensing (generally tested around the Sun), and anomalous perihelion advance of the planets. Each theory should reproduce the observed results in these areas, which have to date always aligned with the predictions of general relativity. In 1964, Irwin I. Shapiro found a fourth test, called the Shapiro delay. It is usually regarded as a "classical" test as well.
Agreement with Newtonian mechanics and special relativity
As an example of disagreement with Newtonian experiments, Birkhoff^{ [16]} theory predicts relativistic effects fairly reliably but demands that sound waves travel at the speed of light. This was the consequence of an assumption made to simplify handling the collision of masses.^{[ citation needed]}
The Einstein equivalence principle
Einstein's Equivalence Principle has three components. The first is the uniqueness of free fall, also known as the Weak Equivalence Principle. This is satisfied if inertial mass is equal to gravitational mass. η is a parameter used to test the maximum allowable violation of the Weak Equivalence Principle. The first tests of the Weak Equivalence Principle were done by Eötvös before 1900 and limited η to less than 5×10^{−9}. Modern tests have reduced that to less than 5×10^{−13}. The second is Lorentz invariance. In the absence of gravitational effects the speed of light is constant. The test parameter for this is δ. The first tests of Lorentz invariance were done by Michelson and Morley before 1890 and limited δ to less than 5×10^{−3}. Modern tests have reduced this to less than 1×10^{−21}. The third is local position invariance, which includes spatial and temporal invariance. The outcome of any local nongravitational experiment is independent of where and when it is performed. Spatial local position invariance is tested using gravitational redshift measurements. The test parameter for this is α. Upper limits on this found by Pound and Rebka in 1960 limited α to less than 0.1. Modern tests have reduced this to less than 1×10^{−4}.
Schiff's conjecture states that any complete, selfconsistent theory of gravity that embodies the Weak Equivalence Principle necessarily embodies Einstein's Equivalence Principle. This is likely to be true if the theory has full energy conservation. Metric theories satisfy the Einstein Equivalence Principle. Extremely few nonmetric theories satisfy this. For example, the nonmetric theory of Belinfante & Swihart^{ [24]}^{ [25]} is eliminated by the THεμ formalism for testing Einstein's Equivalence Principle. Gauge theory gravity is a notable exception, where the strong equivalence principle is essentially the minimal coupling of the gauge covariant derivative.
Parametric postNewtonian formalism
See also Tests of general relativity, Misner et al.^{ [50]} and Will^{ [9]} for more information.
Work on developing a standardized rather than ad hoc set of tests for evaluating alternative gravitation models began with Eddington in 1922 and resulted in a standard set of Parametric postNewtonian numbers in Nordtvedt and Will^{ [81]} and Will and Nordtvedt.^{ [41]} Each parameter measures a different aspect of how much a theory departs from Newtonian gravity. Because we are talking about deviation from Newtonian theory here, these only measure weakfield effects. The effects of strong gravitational fields are examined later.
These ten are:
 is a measure of space curvature, being zero for Newtonian gravity and one for general relativity.
 is a measure of nonlinearity in the addition of gravitational fields, one for general relativity.
 is a check for preferred location effects.
 measure the extent and nature of "preferredframe effects". Any theory of gravity in which at least one of the three is nonzero is called a preferredframe theory.
 measure the extent and nature of breakdowns in global conservation laws. A theory of gravity possesses 4 conservation laws for energymomentum and 6 for angular momentum only if all five are zero.
Strong gravity and gravitational waves
Parametric postNewtonian is only a measure of weak field effects. Strong gravity effects can be seen in compact objects such as white dwarfs, neutron stars, and black holes. Experimental tests such as the stability of white dwarfs, spindown rate of pulsars, orbits of binary pulsars and the existence of a black hole horizon can be used as tests of alternative to general relativity. General relativity predicts that gravitational waves travel at the speed of light. Many alternatives to general relativity say that gravitational waves travel faster than light, possibly breaking causality. After the multimessaging detection of the GW170817 coalescence of neutron stars, where light and gravitational waves were measured to travel at the same speed with an error of 1/10^{15}, many of those modified theory of gravity were excluded.
Cosmological tests
Many of these have been developed recently. For those theories that aim to replace dark matter, the galaxy rotation curve, the Tully–Fisher relation, the faster rotation rate of dwarf galaxies, and the gravitational lensing due to galactic clusters act as constraints. For those theories that aim to replace inflation, the size of ripples in the spectrum of the cosmic microwave background radiation is the strictest test. For those theories that incorporate or aim to replace dark energy, the supernova brightness results and the age of the universe can be used as tests. Another test is the flatness of the universe. With general relativity, the combination of baryonic matter, dark matter and dark energy add up to make the universe exactly flat. As the accuracy of experimental tests improve, alternatives to general relativity that aim to replace dark matter or dark energy will have to explain why.
Results of testing theories
Parametric postNewtonian parameters for a range of theories
(See Will^{ [9]} and Ni^{ [10]} for more details. Misner et al.^{ [50]} gives a table for translating parameters from the notation of Ni to that of Will)
General Relativity is now more than 100 years old, during which one alternative theory of gravity after another has failed to agree with ever more accurate observations. One illustrative example is Parameterized postNewtonian formalism. The following table lists Parametric postNewtonian values for a large number of theories. If the value in a cell matches that in the column heading then the full formula is too complicated to include here.
Einstein general relativity^{ [2]}  1  1  0  0  0  0  0  0  0  0 
Scalartensor theories  
Bergmann,^{ [34]} Wagoner^{ [37]}  0  0  0  0  0  0  0  0  
Nordtvedt,^{ [36]} Bekenstein^{ [45]}  0  0  0  0  0  0  0  0  
Brans–Dicke^{ [7]}  1  0  0  0  0  0  0  0  0  
Vectortensor theories  
HellingsNordtvedt^{ [42]}  0  0  0  0  0  0  
WillNordtvedt^{ [41]}  1  1  0  0  0  0  0  0  0  
Bimetric theories  
Rosen^{ [39]}  1  1  0  0  0  0  0  0  0  
Rastall^{ [47]}  1  1  0  0  0  0  0  0  0  
Lightman–Lee^{ [43]}  0  0  0  0  0  0  
Stratified theories  
LeeLightmanNi^{ [44]}  0  0  0  0  0  
Ni^{ [40]}  0  0  0  0  0  0  
Scalar field theories  
Einstein (1912)^{ [82]}^{ [83]} {Not general relativity}  0  0  4  0  2  0  1  0  0†  
Whitrow–Morduch^{ [29]}  0  1  4  0  0  0  −3  0  0†  
Rosen^{ [38]}  0  4  0  1  0  0  
Papapetrou^{ [19]}^{ [20]}  1  1  8  4  0  0  2  0  0  
Ni^{ [10]} (stratified)  1  1  8  0  0  0  2  0  0  
Yilmaz^{ [26]} (1962)  1  1  8  0  4  0  2  0  1†  
PageTupper^{ [33]}  0  0  0  
Nordström^{ [48]}  0  0  0  0  0  0  0†  
Nordström,^{ [49]} EinsteinFokker^{ [84]}  0  0  0  0  0  0  0  
Ni^{ [10]} (flat)  0  0  0  0  0  0†  
Whitrow–Morduch^{ [28]}  0  0  0  0  q  0  0†  
Littlewood,^{ [21]} Bergman^{ [23]}  0  0  0  0  1  0  0† 
† The theory is incomplete, and can take one of two values. The value closest to zero is listed.
All experimental tests agree with general relativity so far, and so Parametric postNewtonian analysis immediately eliminates all the scalar field theories in the table. A full list of Parametric postNewtonian parameters is not available for Whitehead,^{ [5]} DeserLaurent,^{ [32]} BolliniGiambiagiTiomino,^{ [35]} but in these three cases ,^{[ citation needed]} which is in strong conflict with general relativity and experimental results. In particular, these theories predict incorrect amplitudes for the Earth's tides. (A minor modification of Whitehead's theory avoids this problem. However, the modification predicts the Nordtvedt effect, which has been experimentally constrained.)
Theories that fail other tests
The stratified theories of Ni,^{ [40]} Lee Lightman and Ni^{ [44]} are nonstarters because they all fail to explain the perihelion advance of Mercury. The bimetric theories of Lightman and Lee,^{ [43]} Rosen,^{ [39]} Rastall^{ [47]} all fail some of the tests associated with strong gravitational fields. The scalartensor theories include general relativity as a special case, but only agree with the Parametric postNewtonian values of general relativity when they are equal to general relativity to within experimental error. As experimental tests get more accurate, the deviation of the scalartensor theories from general relativity is being squashed to zero. The same is true of vectortensor theories, the deviation of the vectortensor theories from general relativity is being squashed to zero. Further, vectortensor theories are semiconservative; they have a nonzero value for which can have a measurable effect on the Earth's tides. Nonmetric theories, such as Belinfante and Swihart,^{ [24]}^{ [25]} usually fail to agree with experimental tests of Einstein's equivalence principle. And that leaves, as a likely valid alternative to general relativity, nothing except possibly Cartan.^{ [13]} That was the situation until cosmological discoveries pushed the development of modern alternatives.
Footnotes
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