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Ricci tensor (Definition)

Definition.

The Ricci curvature tensor is a rank $ 2$, symmetric tensor that arises naturally in pseudo-Riemannian geometry. Let $ (M,g_{ij})$ be a smooth, $ n$-dimensional pseudo-Riemannian manifold, and let $ R^i{}_{jkl}$ denote the corresponding Riemann curvature tensor. The Ricci tensor $ R_{ij}$ is commonly defined as the following contraction of the full curvature tensor:
$\displaystyle R_{ij} = R^k{}_{ikj}. $
The index symmetry of $ R_{ij}$, so defined, follows from the symmetry properties of the Riemann curvature. To wit,
$\displaystyle R_{ij} = R^k{}_{ikj} = R_{ki}{}^k{}_j = R^k{}_{jki} = R_{ji}.$
It is also convenient to regard the Ricci tensor as a symmetric bilinear form. To that end for vector-fields $ X,Y$ we will write
$\displaystyle \operatorname{Ric}(X,Y) = X^i Y^j R_{ij}.$

Related objects.

Contracting the Ricci tensor, we obtain an important scalar invariant
$\displaystyle R=R^i{}_i,$
called the scalar curvature, and sometimes also called the Ricci scalar. Closely related to the Ricci tensor is the tensor
$\displaystyle G_{ij} = R_{ij} - \frac{1}{2} R\, g_{ij},$
called the Einstein tensor. The Einstein tensor is also known as the trace-reversed Ricci tensor owing to the fact that
$\displaystyle G^i{}_i = - R. $
Another related tensor is
$\displaystyle S_{ij} = R_{ij} - \frac{1}{n} R\, g_{ij}.$
This is called the trace-free Ricci tensor, owing to the fact that the above definition implies that
$\displaystyle S^i{}_i=0.$

Geometric interpretation.

In Riemannian geometry, the Ricci tensor represents the average value of the sectional curvature along a particular direction. Let
$\displaystyle K_x(u,v) = \frac{R_x(u,v,v,u)}{g_x(u,u) g_x(v,v) - g_x(u,v)^2} $
denote the sectional curvature of $ M$ along the plane spanned by vectors $ u,v\in T_x M$. Fix a point $ x\in M$ and a tangent vector $ v\in T_xM$, and let
$\displaystyle S_x(v)=\{ u\in T_xM \colon g_x(u,u) = 1,\; g_x(u,v)=0 \} $
denote the $ n-2$ dimensional sphere of those unit vectors at $ x$ that are perpendicular to $ v$. Let $ \mu_x$ denote the natural $ (n-2)$-dimensional volume measure on $ T_xM$, normalized so that
$\displaystyle \int_{S_x(v)} \mu_x = 1.$
In this way, the quantity
$\displaystyle \int_{S_x(v)}\!\! K_x(\cdot,v) \mu_x, $
describes the average value of the sectional curvature for all planes in $ T_x M$ that contain $ v$. It is possible to show that
$\displaystyle \operatorname{Ric}_x(v,v)= (1-n)\int_{S_x(v)}\!\! K_x(\cdot,v) \mu_x,$
thereby giving us the desired geometric interpretation.

Decomposition of the curvature tensor.

For $ n\geq 3$, the Ricci tensor can be characterized in terms of the decomposition of the full curvature tensor into three covariantly defined summands, namely
$\displaystyle F_{ijkl}$ $\displaystyle = \tfrac{1}{n-2} \left( S_{jl}\, g_{ik}+S_{ik}\, g_{jl}-S_{il}\, g_{jk}-S_{jk}\, g_{il}\right),$    
$\displaystyle E_{ijkl}$ $\displaystyle = \tfrac{1}{n(n-1)}R \left( g_{jl}\,g_{ik} - g_{il}\,g_{jk}\right),$    
$\displaystyle W_{ijkl}$ $\displaystyle = R_{ijkl}-F_{ijkl}-E_{ijkl}.$    

The $ W_{ijkl}$ is called the Weyl curvature tensor. It is the conformally invariant, trace-free part of the curvature tensor. Indeed, with the above definitions, we have
$\displaystyle W^k{}_{ikj}=0.$
The $ E_{ijkl}$ and $ F_{ijkl}$ correspond to the trace-free part of the Ricci curvature tensor, and to the Ricci scalar. Indeed, we can recover $ S_{ij}$ and $ R$ from $ E_{ijkl}$ and $ F_{ijkl}$ as follows:
$\displaystyle S_{ij}$ $\displaystyle = F^k{}_{ikj},$    
$\displaystyle E^{ij}{}_{ij}$ $\displaystyle = R.$    

Relativity.

The Ricci tensor also plays an important role in the theory of general relativity. In this keystone application, $ M$ is a 4-dimensional pseudo-Riemannian manifold with signature $ (3,1)$. The Einstein field equations assert that the energy-momentum tensor is proportional to the Einstein tensor. In particular, the equation
$\displaystyle R_{ij}=0 $
is the field equation for a vacuum space-time. In geometry, a pseudo-Riemannian manifold that satisfies this equation is called Ricci-flat. It is possible to prove that a manifold is Ricci flat if and only if locally, the manifold, is conformally equivalent to flat space.



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Also defines:  scalar curvature, Einstein tensor, ricci scalar, Weyl tensor, Weyl curvature tensor
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Cross-references: conformally equivalent, flat, manifold, field, equation, Einstein field equations, signature, application, theory, definitions, decomposition, terms, interpretation, contain, volume measure, perpendicular, unit vectors, sphere, tangent vector, point, fix, vectors, spanned by, plane, sectional curvature, average, represents, geometry, implies, invariant, scalar, symmetric bilinear form, properties, symmetry, index, contraction, Riemann curvature tensor, pseudo-Riemannian manifold, smooth, pseudo-Riemannian geometry, symmetric tensor, rank, tensor, curvature
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This is version 6 of Ricci tensor, born on 2005-02-16, modified 2006-09-07.
Object id is 6758, canonical name is RicciTensor.
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AMS MSC83C05 (Relativity and gravitational theory :: General relativity :: Einstein's equations )

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