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.

$Q_{\mu \alpha \beta }=\nabla _{\mu }g_{\alpha \beta )$ It measures the rate of change of the components of the metric tensor along the flow of a given vector field, since

$\nabla _{\mu }\equiv \nabla _{\partial _{\mu ))$ 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 $\Gamma$ is compatible with the metric when its associated covariant derivative of the metric tensor (call it $\nabla ^{\Gamma )$ , for example) is zero, i.e.

$\nabla _{\mu }^{\Gamma }g_{\alpha \beta }=0.$ 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.

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