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Lorentzian Space


Lorentzian n-space is the vector space R^n together with the n-dimensional Lorentzian inner product.

In the event that the (1,n-1) metric signature is used, Lorentzian n-space is denoted R^(1,n-1); the notation R^(n-1,1) is used analogously with the metric signature (n-1,1).

The Lorentzian inner product determines a quadratic form, or Lorentzian squared length, on Lorentzian space. For a vector x=(x_0,x_1,...,x_(n-1)) in the convention with one negative square, it is

 q_L(x)=<x,x>_L=-x_0^2+x_1^2+...+x_(n-1)^2.
(1)

Writing x=(x_0,x^_), where x^_=(x_1,...,x_(n-1)), gives

 q_L(x)=-x_0^2+|x^_|^2,
(2)

where |x^_| is the Euclidean norm. This quadratic form is not a norm since it can be negative and vanishes on nonzero vectors. Its sign classifies nonzero vectors as spacelike, timelike, or lightlike. The collection of lightlike vectors forms the light cone, whose two halves consist of positive lightlike and negative lightlike vectors. A similar distinction is made between positive timelike and negative timelike vectors.

The formal square root of q_L(x) is sometimes called the Lorentzian length. One may also write u degreesv for the Lorentzian inner product <u,v>_L of two vectors.

Lorentzian space comes up in a number of contexts throughout pure and applied mathematics. In particular, four-dimensional Lorentzian space R^4=R^(1,3) is known as Minkowski space and forms the basis of the study of spacetime within special relativity. What's more, the collection

 F^n={x=(x_0,x_1,...,x_n) in R^(n+1):q_L(x)=-1}
(3)

consisting of all vectors in R^(n+1) having Lorentzian squared length -1 forms a two-sheeted hyperboloid of vectors x=(x_0,x^_) satisfying the identity x_0^2-|x^_|^2=1; upon identifying antipodal vectors of F^n (or, equivalently, upon discarding the negative sheet of vectors which satisfy x_0<0), one arrives at the so-called hyperboloid model for hyperbolic space H^n.


See also

Inner Product Space, Light Cone, Lightlike, Lorentzian Inner Product, Metric Signature, Negative Lightlike, Negative Timelike, p-Signature, Positive Definite Quadratic Form, Positive Definite Tensor, Positive Lightlike, Positive Timelike, Quadratic, Quadratic Form Rank, Spacelike, Sylvester's Inertia Law, Sylvester's Signature, Timelike

Portions of this entry contributed by Christopher Stover

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References

Gradshteyn, I. S. and Ryzhik, I. M. Table of Integrals, Series, and Products, 6th ed. San Diego, CA: Academic Press, p. 1105, 2000.Misner, C. W.; Thorne, K. S.; and Wheeler, J. A. Gravitation. San Francisco, CA: W. H. Freeman, 1973.Ratcliffe, J. G. Foundations of Hyperbolic Manifolds. New York: Springer, 2006.

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Lorentzian Space

Cite this as:

Weisstein, Eric W., with contributions by Christopher Stover. "Lorentzian Space." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/LorentzianSpace.html

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