The metric-lowered Riemann curvature tensor #
Pairing the output of the pointwise (1,3) curvature tensor with the metric gives the
(0,4) Riemann curvature tensor
Rm(u, v, w, z) = ⟨R(u, v)w, z⟩.
This file bundles that expression as a quadrilinear map and records its algebraic symmetries.
Every connection gives antisymmetry in the first pair. Metric compatibility gives antisymmetry
in the last pair, torsion-freeness gives the first Bianchi identity, and together these imply
pair-interchange symmetry. The latter symmetry also makes the Ricci contraction symmetric.
By polarization, these symmetries determine Rm from its values Rm(u, v, v, u) on linearly
independent pairs u, v, the numerators of the sectional curvatures.
The sign and argument conventions follow J. M. Lee, Introduction to Riemannian Manifolds, 2nd ed., Springer GTM 176 (2018), Chapter 7.
Main declarations #
CovariantDerivative.riemannCurvatureTensor: the metric-lowered curvature tensor.CovariantDerivative.IsMetricCompatible.riemannCurvatureTensor_swap_pairs: pair-interchange symmetry.CovariantDerivative.IsMetricCompatible.riemannCurvatureTensor_eq_of_forall_linearIndependent:Rmis the unique tensor with the curvature symmetries and the same valuesT(u, v, v, u)on linearly independent pairs.CovariantDerivative.IsMetricCompatible.ricciTensor_commandCovariantDerivative.IsMetricCompatible.ricciTensor_isSymm: symmetry of Ricci curvature.CovariantDerivative.ricciTensor_eq_sum_riemannCurvatureTensorandCovariantDerivative.scalarCurvature_eq_sum_riemannCurvatureTensor: the Ricci and scalar contractions in an orthonormal basis.
The metric-lowered Riemann curvature tensor, with convention
Rm(u, v, w, z) = ⟨R(u, v)w, z⟩.
Instances For
Evaluation of the metric-lowered Riemann curvature tensor.
In an orthonormal basis, Ricci curvature is the contraction of the first and fourth arguments of the Riemann curvature tensor.
In an orthonormal basis, scalar curvature is the double contraction of the Riemann curvature tensor.
The Riemann curvature tensor is antisymmetric in its first pair of arguments.
For a torsion-free connection, the cyclic sum of the first three arguments of the Riemann curvature tensor vanishes.
For a metric-compatible connection, the Riemann curvature tensor is antisymmetric in its last pair of arguments.
The Riemann curvature tensor of a metric-compatible torsion-free connection is unchanged when its two pairs of arguments are interchanged.
For a metric-compatible torsion-free connection, the Riemann curvature tensor at x is the
only quadrilinear form with the algebraic symmetries of a curvature tensor whose values
T(u, v, v, u) on linearly independent pairs are the sectional-curvature numerators
⟨R(u, v)v, u⟩.