Killing vector field

In mathematics, a Killing vector field, named after Wilhelm Killing, is a vector field on a Riemannian manifold (or pseudo-Riemannian manifold) that preserves the metric. Killing fields are the infinitesimal generators of isometries; that is, flows generated by Killing fields are continuous isometries of the manifold. More simply, the flow generates a symmetry, in the sense that moving each point on an object in the direction of the Killing vector field will not distort distances on the object. For example, the vector field on a circle that points clockwise and has the same length at each point is a Killing vector field, since moving each point on the circle along this vector field simply rotates the circle.

If the metric coefficients $g\_\{mu\; u\}\; ,$ in some coordinate basis $dx^\{a\}\; ,$ are independent of $x^\{K\}\; ,$, then $x^\{mu\}\; =\; delta^\{mu\}\_\{K\}\; ,$ is automatically a Killing vector, where $delta^\{mu\}\_\{K\}\; ,$ is the Kronecker delta. (Misner, et al, 1973). For example if none of the metric coefficients are functions of time, the manifold must automatically have a time-like Killing vector.

Explanation

Specifically, a vector field "X" is a Killing field if the Lie derivative with respect to "X" of the metric "g" vanishes:

:$mathcal\{L\}\_\{X\}\; g\; =\; 0\; ,.$

In terms of the Levi-Civita connection, this is

:$g(\; abla\_\{Y\}\; X,\; Z)\; +\; g(Y,\; abla\_\{Z\}\; X)\; =\; 0\; ,$

for all vectors "Y" and "Z". In local coordinates, this amounts to the Killing equation

:$abla\_\{mu\}\; X\_\{\; u\}\; +\; abla\_\{\; u\}\; X\_\{mu\}\; =\; 0\; ,.$

This condition is expressed in covariant form. Therefore it is sufficient to establish it in a preferred coordinate system in order to have it hold in all coordinate systems.

A Killing field is determined uniquely by a vector at some point and its gradient (i.e. all covariant derivatives of the field at the point).

The Lie bracket of two Killing fields is still a Killing field. The Killing fields on a manifold "M" thus form a Lie subalgebra of vector fields on "M". This is the Lie algebra of the isometry group of the manifold.

For compact manifolds
* Negative Ricci curvature implies there are no nontrivial (nonzero) Killing fields.
* Nonpositive Ricci curvature implies that any Killing field is parallel. i.e. covariant derivative along any vector field is identically zero.
* If the sectional curvature is positive and the dimension of "M" is even, a Killing field must have a zero.

Killing vector fields can be generalized to conformal Killing vector fields defined by:$mathcal\{L\}\_\{X\}\; g\; =\; lambda\; g\; ,$for some scalar $lambda\; ,.$ The derivatives of one parameter families of conformal maps are conformal Killing fields. Another generalization is to conformal Killing tensor fields. These are symmetric tensor fields "T" such that the trace-free part of the symmetrization of $abla\; T\; ,$ vanishes.

References

*.

*. "See chapters 3,9"

*