In
Riemannian geometry
Riemannian geometry is the branch of differential geometry that studies Riemannian manifolds, smooth manifolds with a ''Riemannian metric'', i.e. with an inner product on the tangent space at each point that varies smoothly from point to po ...
and
pseudo-Riemannian geometry, curvature invariants are
scalar quantities constructed from tensors that represent
curvature
In mathematics, curvature is any of several strongly related concepts in geometry. Intuitively, the curvature is the amount by which a curve deviates from being a straight line, or a surface deviates from being a plane.
For curves, the can ...
. These tensors are usually the
Riemann tensor, the
Weyl tensor
In differential geometry, the Weyl curvature tensor, named after Hermann Weyl, is a measure of the curvature of spacetime or, more generally, a pseudo-Riemannian manifold. Like the Riemann curvature tensor, the Weyl tensor expresses the tidal forc ...
, the
Ricci tensor
In differential geometry, the Ricci curvature tensor, named after Gregorio Ricci-Curbastro, is a geometric object which is determined by a choice of Riemannian or pseudo-Riemannian metric on a manifold. It can be considered, broadly, as a measur ...
and tensors formed from these by the operations of taking
dual
Dual or Duals may refer to:
Paired/two things
* Dual (mathematics), a notion of paired concepts that mirror one another
** Dual (category theory), a formalization of mathematical duality
*** see more cases in :Duality theories
* Dual (grammatical ...
contractions and
covariant differentiations.
Types of curvature invariants
The invariants most often considered are ''polynomial invariants''. These are polynomials constructed from contractions such as traces. Second degree examples are called ''quadratic invariants'', and so forth. Invariants constructed using covariant derivatives up to order n are called n-th order ''differential invariants''.
The Riemann tensor is a
multilinear operator of fourth rank acting on
tangent vector
In mathematics, a tangent vector is a vector that is tangent to a curve or surface at a given point. Tangent vectors are described in the differential geometry of curves in the context of curves in R''n''. More generally, tangent vectors are ele ...
s. However, it can also be considered a
linear operator
In mathematics, and more specifically in linear algebra, a linear map (also called a linear mapping, linear transformation, vector space homomorphism, or in some contexts linear function) is a Map (mathematics), mapping V \to W between two vect ...
acting on
bivector In mathematics, a bivector or 2-vector is a quantity in exterior algebra or geometric algebra that extends the idea of scalars and vectors. If a scalar is considered a degree-zero quantity, and a vector is a degree-one quantity, then a bivector can ...
s, and as such it has a
characteristic polynomial
In linear algebra, the characteristic polynomial of a square matrix is a polynomial which is invariant under matrix similarity and has the eigenvalues as roots. It has the determinant and the trace of the matrix among its coefficients. The ...
, whose coefficients and roots (
eigenvalue
In linear algebra, an eigenvector () or characteristic vector of a linear transformation is a nonzero vector that changes at most by a scalar factor when that linear transformation is applied to it. The corresponding eigenvalue, often denot ...
s) are polynomial scalar invariants.
Physical applications
In
metric theories of gravitation such as
general relativity
General relativity, also known as the general theory of relativity and Einstein's theory of gravity, is the geometric theory of gravitation published by Albert Einstein in 1915 and is the current description of gravitation in modern physics. ...
, curvature scalars play an important role in telling distinct spacetimes apart.
Two of the most basic curvature invariants in general relativity are the
Kretschmann scalar In the theory of Lorentzian manifolds, particularly in the context of applications to general relativity, the Kretschmann scalar is a quadratic scalar invariant. It was introduced by Erich Kretschmann.
Definition
The Kretschmann invariant is
: K ...
:
and the ''Chern–Pontryagin scalar'',
:
These are analogous to two familiar quadratic invariants of the
electromagnetic field tensor
In electromagnetism, the electromagnetic tensor or electromagnetic field tensor (sometimes called the field strength tensor, Faraday tensor or Maxwell bivector) is a mathematical object that describes the electromagnetic field in spacetime. Th ...
in classical electromagnetism.
An important unsolved problem in general relativity is to give a
basis (and any
syzygies
Syzygy (from Greek Συζυγία "conjunction, yoked together") may refer to:
Science
* Syzygy (astronomy), a collinear configuration of three celestial bodies
* Syzygy (mathematics), linear relation between generators of a module
* Syzygy, ...
) for the zero-th order invariants of the Riemann tensor.
They have limitations because many distinct spacetimes cannot be distinguished on this basis. In particular, so called
VSI spacetimes (including pp-waves as well as some other Petrov type N and III spacetimes) cannot be distinguished from
Minkowski spacetime
In mathematical physics, Minkowski space (or Minkowski spacetime) () is a combination of three-dimensional Euclidean space and time into a four-dimensional manifold where the spacetime interval between any two events is independent of the ...
using any number of polynomial curvature invariants (of any order).
See also
*
Cartan–Karlhede algorithm
*
Carminati–McLenaghan invariants
*
Curvature invariant (general relativity)
*
Ricci decomposition
References
*
Riemannian geometry
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