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Pseudo-Riemannian manifold
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In differential geometry, a pseudo-Riemannian manifold (also called a semi-Riemannian manifold) is a generalization of a Riemannian manifold. It is one of many things named after Bernhard Riemann. The key difference between a Riemannian manifold and a pseudo-Riemannian manifold is that on a pseudo-Riemannian manifold the metric tensor need not be positive-definite. Instead a weaker condition of nondegeneracy is imposed.
Introduction
Manifolds
Main articles: Manifold, differentiable manifolds
In differential geometry a differentiable manifold is a space which is locally similar to a Euclidean space.
Discussion
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Encyclopedia
In differential geometry, a pseudo-Riemannian manifold (also called a semi-Riemannian manifold) is a generalization of a Riemannian manifold. It is one of many things named after Bernhard Riemann. The key difference between a Riemannian manifold and a pseudo-Riemannian manifold is that on a pseudo-Riemannian manifold the metric tensor need not be positive-definite. Instead a weaker condition of nondegeneracy is imposed.
Introduction
Manifolds
Main articles: Manifold, differentiable manifolds
In differential geometry a differentiable manifold is a space which is locally similar to a Euclidean space. In an -dimensional Euclidean space any point can be specified by real numbers. These are called the coordinates of the point.
An -dimensional differentiable manifold is a generalisation of -dimensional Euclidean space. In a manifold it may only be possible to define coordinates locally. This is achieved by defining coordinate patches: subsets of the manifold which can be mapped into -dimensional Euclidean space.
See Manifold, differentiable manifold, coordinate patch for more details.
Tangent spaces and metric tensors
Main articles: Tangent space, metric tensor
Associated with each point in an -dimensional differentiable manifold is a tangent space (denoted ). This is an -dimensional vector space whose elements can be thought of as equivalence classes of curves passing through the point .
A metric tensor is a non-degenerate, smooth, symmetric, bilinear map which assigns a real number to pairs of tangent vectors at each tangent space of the manifold. Denoting the metric tensor by we can express this as .
The map is symmetric and bilinear so if are tangent vectors at a point in the manifold then we have
for some real number .
That is non-degenerate means there are no non-zero such that for all .
Metric signatures
For an -dimensional manifold the metric tensor (in a fixed coordinate system) has eigenvalues. If the metric is non-degenerate then none of these eigenvalues are zero. The signature of the metric denotes the number of positive and negative eigenvalues, this quantity is independent of the chosen coordinate system by Sylvester's rigidity theorem and locally non-decreasing.
If the metric has positive eigenvalues and negative eigenvalues then the metric signature is . For a non-degenerate metric .
Definition
A pseudo-Riemannian manifold is a differentiable manifold equipped with a non-degenerate, smooth, symmetric metric tensor which, unlike a Riemannian metric, need not be positive-definite, but must be non-degenerate. Such a metric is called a pseudo-Riemannian metric and its values can be positive, negative or zero.
The signature of a pseudo-Riemannian metric is where both and are non-negative.
Lorentzian manifold
A Lorentzian manifold is an important special case of a pseudo-Riemannian manifold in which the signature of the metric is (or sometimes , see sign convention). Such metrics are called Lorentzian metrics. They are named after the physicist Hendrik Lorentz.
Applications in physics
After Riemannian manifolds, Lorentzian manifolds form the most important subclass of pseudo-Riemannian manifolds. They are important because of their physical applications to the theory of general relativity.
A principal assumption of general relativity is that spacetime can be modeled as a 4-dimensional Lorentzian manifold of signature (or equivalently (1,3)). Unlike Riemannian manifolds with positive-definite metrics, a signature of or allows tangent vectors to be classified into timelike, null or spacelike (see Causal structure).
Properties of pseudo-Riemannian manifolds
Just as Euclidean space can be thought of as the model Riemannian manifold, Minkowski space with the flat Minkowski metric is the model Lorentzian manifold. Likewise, the model space for a pseudo-Riemannian manifold of signature is with the metric:
Some basic theorems of Riemannian geometry can be generalized to the pseudo-Riemannian case. In particular, the fundamental theorem of Riemannian geometry is true of pseudo-Riemannian manifolds as well. This allows one to speak of the Levi-Civita connection on a pseudo-Riemannian manifold along with the associated curvature tensor. On the other hand, there are many theorems in Riemannian geometry which do not hold in the generalized case. For example, it is not true that every smooth manifold admits a pseudo-Riemannian metric of a given signature; there are certain topological obstructions. Furthermore, a submanifold of a pseudo-Riemannian
manifold need not be a pseudo-Riemannian manifold.
See also
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