Nonmetricity tensor

Template:Short description In mathematics, the nonmetricity tensor in differential geometry is the covariant derivative of the metric tensor. It is therefore a tensor field of order three. It vanishes for the case of Riemannian geometry and can be used to study non-Riemannian spacetimes.

Definition

By components, it is defined as follows.

$Q_{\mu \alpha \beta }={\mathrm{\nabla }}_{\mu }{g}_{\alpha \beta }$

It measures the rate of change of the components of the metric tensor along the flow of a given vector field, since

${\mathrm{\nabla }}_{\mu }\equiv {\mathrm{\nabla }}_{{\partial }_{\mu }}$

where $\{{\partial }_{\mu }{\}}_{\mu =0,1,2,3}$ is the coordinate basis of vector fields of the tangent bundle, in the case of having a 4-dimensional manifold.

Relation to connection

We say that a connection $\mathrm{\Gamma }$ is compatible with the metric when its associated covariant derivative of the metric tensor (call it ${\mathrm{\nabla }}^{\mathrm{\Gamma }}$, for example) is zero, i.e.

$\underset{\mu }{\overset{\mathrm{\Gamma }}{\mathrm{\nabla }}}{g}_{\alpha \beta }=0.$

If the connection is also torsion-free (i.e. totally symmetric) then it is known as the Levi-Civita connection, which is the only one without torsion and compatible with the metric tensor. If we see it from a geometrical point of view, a non-vanishing nonmetricity tensor for a metric tensor $g$ implies that the modulus of a vector defined on the tangent bundle to a certain point $p$ of the manifold, changes when it is evaluated along the direction (flow) of another arbitrary vector.

External links

• Template:Cite journal

Template:Differential-geometry-stub