# Newton–Cartan theory

Newton–Cartan theory (or geometrized Newtonian gravitation) is a geometrical re-formulation, as well as a generalization, of Newtonian gravity first introduced by Élie Cartan[1][2] and Kurt Friedrichs[3] and later developed by Dautcourt,[4] Dixon,[5] Dombrowski and Horneffer, Ehlers, Havas,[6] Künzle,[7] Lottermoser, Trautman,[8] and others. In this re-formulation, the structural similarities between Newton's theory and Albert Einstein's general theory of relativity are readily seen, and it has been used by Cartan and Friedrichs to give a rigorous formulation of the way in which Newtonian gravity can be seen as a specific limit of general relativity, and by Jürgen Ehlers to extend this correspondence to specific solutions of general relativity.

## Classical spacetimes

In Newton–Cartan theory, one starts with a smooth four-dimensional manifold ${\displaystyle M}$ and defines two (degenerate) metrics. A temporal metric ${\displaystyle t_{ab}}$ with signature ${\displaystyle (1,0,0,0)}$, used to assign temporal lengths to vectors on ${\displaystyle M}$ and a spatial metric ${\displaystyle h^{ab}}$ with signature ${\displaystyle (0,1,1,1)}$. One also requires that these two metrics satisfy a transversality (or "orthogonality") condition, ${\displaystyle h^{ab}t_{bc}=0}$. Thus, one defines a classical spacetime as an ordered quadruple ${\displaystyle (M,t_{ab},h^{ab},\nabla )}$, where ${\displaystyle t_{ab}}$ and ${\displaystyle h^{ab}}$ are as described, ${\displaystyle \nabla }$ is a metrics-compatible covariant derivative operator; and the metrics satisfy the orthogonality condition. One might say that a classical spacetime is the analog of a relativistic spacetime ${\displaystyle (M,g_{ab})}$, where ${\displaystyle g_{ab}}$ is a smooth Lorentzian metric on the manifold ${\displaystyle M}$.

## Geometric formulation of Poisson's equation

In Newton's theory of gravitation, Poisson's equation reads

${\displaystyle \Delta U=4\pi G\rho \,}$

where ${\displaystyle U}$ is the gravitational potential, ${\displaystyle G}$ is the gravitational constant and ${\displaystyle \rho }$ is the mass density. The weak equivalence principle motivates a geometric version of the equation of motion for a point particle in the potential ${\displaystyle U}$

${\displaystyle m_{t}\,{\ddot {\vec {x}}}=-m_{g}{\vec {\nabla }}U}$

where ${\displaystyle m_{t}}$ is the inertial mass and ${\displaystyle m_{g}}$ the gravitational mass. Since, according to the weak equivalence principle ${\displaystyle m_{t}=m_{g}}$, the according equation of motion

${\displaystyle {\ddot {\vec {x}}}=-{\vec {\nabla }}U}$

does not contain anymore a reference to the mass of the particle. Following the idea that the solution of the equation then is a property of the curvature of space, a connection is constructed so that the geodesic equation

${\displaystyle {\frac {d^{2}x^{\lambda }}{ds^{2}}}+\Gamma _{\mu \nu }^{\lambda }{\frac {dx^{\mu }}{ds}}{\frac {dx^{\nu }}{ds}}=0}$

represents the equation of motion of a point particle in the potential ${\displaystyle U}$. The resulting connection is

${\displaystyle \Gamma _{\mu \nu }^{\lambda }=\gamma ^{\lambda \rho }U_{,\rho }\Psi _{\mu }\Psi _{\nu }}$

with ${\displaystyle \Psi _{\mu }=\delta _{\mu }^{0}}$ and ${\displaystyle \gamma ^{\mu \nu }=\delta _{A}^{\mu }\delta _{B}^{\nu }\delta ^{AB}}$ (${\displaystyle A,B=1,2,3}$). The connection has been constructed in one inertial system but can be shown to be valid in any inertial system by showing the invariance of ${\displaystyle \Psi _{\mu }}$ and ${\displaystyle \gamma ^{\mu \nu }}$ under Galilei-transformations. The Riemann curvature tensor in inertial system coordinates of this connection is then given by

${\displaystyle R_{\kappa \mu \nu }^{\lambda }=2\gamma ^{\lambda \sigma }U_{,\sigma [\mu }\Psi _{\nu ]}\Psi _{\kappa }}$

where the brackets ${\displaystyle A_{[\mu \nu ]}={\frac {1}{2!}}[A_{\mu \nu }-A_{\nu \mu }]}$ mean the antisymmetric combination of the tensor ${\displaystyle A_{\mu \nu }}$. The Ricci tensor is given by

${\displaystyle R_{\kappa \nu }=\Delta U\Psi _{\kappa }\Psi _{\nu }\,}$

which leads to following geometric formulation of Poisson's equation

${\displaystyle R_{\mu \nu }=4\pi G\rho \Psi _{\mu }\Psi _{\nu }}$

More explicitly, if the roman indices i and j range over the spatial coordinates 1, 2, 3, then the connection is given by

${\displaystyle \Gamma _{00}^{i}=U_{,i}}$

the Riemann curvature tensor by

${\displaystyle R_{0j0}^{i}=-R_{00j}^{i}=U_{,ij}}$

and the Ricci tensor and Ricci scalar by

${\displaystyle R=R_{00}=\Delta U}$

where all components not listed equal zero.

Note that this formulation does not require introducing the concept of a metric: the connection alone gives all the physical information.

## Bargmann lift

It was shown that four-dimensional Newton–Cartan theory of gravitation can be reformulated as Kaluza–Klein reduction of five-dimensional Einstein gravity along a null-like direction.[9] This lifting is considered to be useful for non-relativistic holographic models.[10]

## References

1. ^ Cartan, Élie (1923), "Sur les variétés à connexion affine et la théorie de la relativité généralisée (première partie)" (PDF), Ann. Ecole Norm., 40: 325, doi:10.24033/asens.751
2. ^ Cartan, Élie (1924), "Sur les variétés à connexion affine, et la théorie de la relativité généralisée (première partie)" (PDF), Ann. Ecole Norm., 41: 1, doi:10.24033/asens.753
3. ^ Friedrichs, K. O. (1927), "Eine Invariante Formulierung des Newtonschen Gravitationsgesetzes und der Grenzüberganges vom Einsteinschen zum Newtonschen Gesetz", Mathematische Annalen, 98: 566–575, doi:10.1007/bf01451608
4. ^ Dautcourt, G. (1964), "Die Newtonische Gravitationstheorie als strenger Grenzfall der allgemeinen Relativitätstheorie", Acta Physica Polonica, 65: 637–646
5. ^ Dixon, W. G. (1975), "On the uniqueness of the Newtonian theory as a geometric theory of gravitation", Communications in Mathematical Physics, 45: 167–182, Bibcode:1975CMaPh..45..167D, doi:10.1007/bf01629247
6. ^ Havas, P. (1964), "Four-dimensional formulations of Newtonian mechanics and their relation to the special and general theory of relativity", Reviews of Modern Physics, 36: 938–965, Bibcode:1964RvMP...36..938H, doi:10.1103/revmodphys.36.938
7. ^ Künzle, H. (1976), "Covariant Newtonian limts of Lorentz space-times", General Relativity and Gravitation, 7: 445–457, Bibcode:1976GReGr...7..445K, doi:10.1007/bf00766139
8. ^ Trautman, A. (1965), Deser, Jürgen; Ford, K. W. (eds.), Foundations and current problems of general relativity, 98, Englewood Cliffs, New Jersey: Prentice-Hall, pp. 1–248
9. ^ C. Duval, G. Burdet, H. P. Künzle, and M. Perrin, Bargmann structures and Newton-Cartan theory, Phys. Rev. D 31, 1841–1853 (1985)
10. ^ Walter D. Goldberger, AdS/CFT duality for non-relativistic field theory, JHEP03(2009)069 [1]