Non-relativistic gravitational fields

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This is currently being merged. After a discussion, consensus to merge this into Parameterized post-Newtonian formalism was found. You can help implement the merge by following the instructions at Help:Merging and the resolution on the discussion. Process started in April 2023.

Within general relativity (GR), Einstein's relativistic gravity, the gravitational field is described by the 10-component metric tensor. However, in Newtonian gravity, which is a limit of GR, the gravitational field is described by a single component Newtonian gravitational potential. This raises the question to identify the Newtonian potential within the metric, and to identify the physical interpretation of the remaining 9 fields.

The definition of the non-relativistic gravitational fields provides the answer to this question, and thereby describes the image of the metric tensor in Newtonian physics. These fields are not strictly non-relativistic. Rather, they apply to the non-relativistic (or post-Newtonian) limit of GR.

A reader who is familiar with electromagnetism (EM) will benefit from the following analogy. In EM, one is familiar with the electrostatic potential ${\displaystyle \phi ^{\text{EM}}}$ and the magnetic vector potential ${\displaystyle {\vec {A}}{}^{\text{EM}}}$. Together, they combine into the 4-vector potential ${\displaystyle A_{\mu }^{\text{EM}}\leftrightarrow (\phi ^{\text{EM}},{\vec {A}}{}^{\text{EM}})}$, which is compatible with relativity. This relation can be thought to represent the non-relativistic decomposition of the electromagnetic 4-vector potential. Indeed, a system of point-particle charges moving slowly with respect to the speed of light may be studied in an expansion in ${\displaystyle v^{2}/c^{2}}$, where ${\displaystyle v}$ is a typical velocity and ${\displaystyle c}$ is the speed of light. This expansion is known as the post-Coulombic expansion. Within this expansion, ${\displaystyle \phi ^{\text{EM}}}$ contributes to the two-body potential already at 0th order, while ${\displaystyle {\vec {A}}^{\text{EM}}}$ contributes only from the 1st order and onward, since it couples to electric currents and hence the associated potential is proportional to ${\displaystyle v^{2}/c^{2}}$.

In the non-relativistic limit, of weak gravity and non-relativistic velocities, general relativity reduces to Newtonian gravity. Going beyond the strict limit, corrections can be organized into a perturbation theory known as the post-Newtonian expansion. As part of that, the metric gravitational field ${\displaystyle g_{\mu \nu },\ \mu ,\nu =0,1,2,3}$, is redefined and decomposed into the non-relativistic gravitational (NRG) fields ${\displaystyle g_{\mu \nu }\leftrightarrow {\big (}\phi ,{\vec {A}},\sigma _{ij}{\big )}}$ : ${\displaystyle \phi }$ is the Newtonian potential, ${\displaystyle {\vec {A}}}$ is known as the gravito-magnetic vector potential, and finally ${\displaystyle \sigma _{ij}}$ is a 3d symmetric tensor known as the spatial metric perturbation. The field redefinition is given by^{[1][further explanation needed]} $${\displaystyle ds^{2}\equiv g_{\mu \nu }dx^{\mu }dx^{\nu }=e^{2\phi }(dt-2\,{\vec {A}}\cdot d{\vec {x}})^{2}-e^{-2\phi }(\delta _{ij}+\sigma _{ij})\,dx^{i}\,dx^{j}.}$$ In components, this is equivalent to $${\displaystyle {\begin{aligned}g_{00}&=e^{2\phi },\\g_{0i}&=-2\,e^{2\phi }\,A_{i},\\g_{ij}&=-e^{-2\phi }\,(\delta _{ij}+\sigma _{ij})+4\,e^{2\phi }\,A_{i}\,A_{j},\end{aligned}}}$$ where ${\displaystyle i,j=1,2,3}$.

Counting components, ${\displaystyle g_{\mu \nu }}$ has 10, while ${\displaystyle \phi }$ has 1, ${\displaystyle {\vec {A}}}$ has 3 and finally ${\displaystyle \sigma _{ij}}$ has 6. Hence, in terms of components, the decomposition reads ${\displaystyle 10=1+3+6}$.

In the post-Newtonian limit, bodies move slowly compared with the speed of light, and hence the gravitational field is also slowly changing. Approximating the fields to be time independent, the Kaluza-Klein reduction (KK) was adapted to apply to the time direction. Recall that in its original context, the KK reduction applies to fields which are independent of a compact spatial fourth direction. In short, the NRG decomposition is a Kaluza-Klein reduction over time.

The definition was essentially introduced in,^[1] interpreted in the context of the post-Newtonian expansion in,^[2] and finally the normalization of ${\displaystyle {\vec {A}}}$ was changed in ^[3] to improve the analogy between a spinning object and a magnetic dipole.

By definition, the post-Newtonian expansion assumes a weak field approximation. Within the first order perturbation to the metric ${\displaystyle g_{\mu \nu }=\eta _{\mu \nu }+h_{\mu \nu }}$, where ${\displaystyle \eta _{\mu \nu }}$ is the Minkowski metric, we find the standard weak field decomposition into a scalar, vector and tensor ${\displaystyle h_{\mu \nu }\to \left(h_{00},h_{0i},h_{ij}\right)}$, which is similar to the non-relativistic gravitational (NRG) fields. The importance of the NRG fields is that they provide a non-linear extension, thereby facilitating computation at higher orders in the weak field / post-Newtonian expansion. Summarizing, the NRG fields are adapted for higher order post-Newtonian expansion.

The scalar field ${\displaystyle \phi }$ is interpreted as the Newtonian gravitational potential.

The vector field ${\displaystyle {\vec {A}}}$ is interpreted as the gravito-magnetic vector potential. It is magnetic-like, or analogous to the magnetic vector potential in electromagnetism (EM). In particular, it is sourced by massive currents (the analogue of charge currents in EM), namely by momentum.

As a result, the gravito-magnetic vector potential is responsible for current-current interaction, which appears at the 1st post-Newtonian order. In particular, it generates a repulsive contribution to the force between parallel massive currents. However, this repulsion is overturned by the standard Newtonian gravitational attraction, since in gravity a current "wire" must always be massive (charged) -- unlike EM.

A spinning object is the analogue of an electromagnetic current loop, which forms as magnetic dipole, and as such it creates a magnetic-like dipole field in ${\displaystyle {\vec {A}}}$.

The symmetric tensor ${\displaystyle \sigma _{ij}}$ is known as the spatial metric perturbation. From the 2nd post-Newtonian order and onward, it must be accounted for. If one restricts to the 1st post-Newtonian order, ${\displaystyle \sigma _{ij}}$ can be ignored, and relativistic gravity is described by the ${\displaystyle \phi }$, ${\displaystyle {\vec {A}}}$ fields. Hence it becomes a strong analogue of electromagnetism, an analogy known as gravitoelectromagnetism.

The two body problem in general relativity holds both intrinsic interest and observational, astrophysical interest. In particular, it is used to describe the motion of binary compact objects, which are the sources for gravitational waves. As such, the study of this problem is essential for both detection and interpretation of gravitational waves.

Within this two body problem, the effects of GR are captured by the two body effective potential, which is expanded within the post-Newtonian approximation. Non-relativistic gravitational fields were found to economize the determination of this two body effective potential.^[4][5][6]

In higher dimensions, with an arbitrary spacetime dimension ${\displaystyle d}$, the definition of non-relativistic gravitational fields generalizes into ^[1]

$${\displaystyle ds^{2}=e^{2\phi }(dt-2\,{\vec {A}}\cdot d{\vec {x}})^{2}-e^{-2\phi /(d-3)}(\delta _{ij}+\sigma _{ij})dx^{i}dx^{j}}$$Substituting ${\displaystyle d=4}$ reproduces the standard 4d definition above.

• Non-relativistic spacetime

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