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Timelike


A timelike four-vector a_mu has squared Lorentzian length a_mua^mu<0, using the convention in which the time coordinate has negative squared length.

The square of the four-vector norm is the quadratic form associated with the Lorentzian inner product <·,·> on n-dimensional Lorentzian space with n>=2 and metric signature (1,n-1), listing the number of negative entries first. In this more general environment, the Lorentzian inner product of two vectors x=(x_0,x_1,...,x_(n-1)) and y=(y_0,y_1,...,y_(n-1)) has the form

 <x,y>=-x_0y_0+x_1y_1+...+x_(n-1)y_(n-1),

whereby one defines a vector a to be timelike precisely when <a,a><0.

Geometrically, the collection of all timelike vectors lies in the open set of R^n formed by the interior of the light cone. In particular, the upper half of the interior consists of vectors which are positive timelike whereas the lower half consists of all negative timelike vectors.


See also

Light Cone, Lightlike, Lorentzian Inner Product, Lorentzian Space, Metric Signature, Negative Lightlike, Negative Timelike, Positive Lightlike, Positive Timelike, Spacelike

Portions of this entry contributed by Christopher Stover

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References

Misner, C. W.; Thorne, K. S.; and Wheeler, J. A. Gravitation. San Francisco, CA: W. H. Freeman, p. 53, 1973.Ratcliffe, J. G. Foundations of Hyperbolic Manifolds, 2nd ed. New York: Springer-Verlag, pp. 54-55, 2006.

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Timelike

Cite this as:

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

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