This is an old revision of this page, as edited by Anthony (talk | contribs) at 23:46, 28 January 2004 (1) prove it, 2) if so you should point to theory of relativity, not relativity). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.
Revision as of 23:46, 28 January 2004 by Anthony (talk | contribs) (1) prove it, 2) if so you should point to theory of relativity, not relativity)(diff) ← Previous revision | Latest revision (diff) | Newer revision → (diff)In relativity, a four-vector is a vector in a four-dimensional real vector space, whose components transform like the space and time coordinates (ct, x, y, z) under spatial rotations and boosts (a change by a constant velocity to another inertial reference frame). The set of all such rotations and boosts, called Lorentz transformations and described by 4×4 matrices, forms the Lorentz group.
Examples of four-vectors include the coordinates (ct, x, y, z) themselves, the four-current (cρ, J) formed from charge density ρ and current density J, the electromagnetic four-potential (φ, A) formed from the scalar potential φ and vector potential A, and the four-momentum (E/c, p) formed from the (relativistic) energy E and momentum p. The speed of light (c) is often used to ensure that the first coordinate (time-like, labeled by index 0) has the same units as the following three coordinates (space-like, labeled by indices 1,..,3).
The scalar product between four-vectors a and b is defined as follows:
Strictly speaking, this is not a proper inner product, since its value can be negative. Like the ordinary dot product of three-vectors, however, the result of this scalar product is a scalar: it is invariant under any Lorentz transformation. (This property is sometimes use to define the Lorentz group.) The 4×4 matrix in the above definition is called the metric tensor, sometimes denoted by g; its sign is a matter of convention, and some authors multiply it by -1. See Sign convention.
The laws of physics are also postulated to be invariant under Lorentz transformations. An object in an inertial reference frame will perceive the universe as if the universe were Lorentz-transformed so that the perceiving object is stationary.
See also: four-velocity, four-acceleration, four-momentum, four-force.