# light cone

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## light cone

The representation of a light flash in spacetime. In three-dimensional space the wavefront of a light flash would be a sphere centered on the emitting point and growing in radius at the speed of light. In spacetime (with one spatial coordinate suppressed) the vertex of a cone represents the time and place at which a flash is emitted and the cone itself describes the history of the propagating flash. More generally a light cone defines the regions of the Universe accessible from a given point in space and moment in time, i.e. from a given position in spacetime. This position is called an*event*and is the vertex of the light cone.

*The Great Soviet Encyclopedia*(1979). It might be outdated or ideologically biased.

## Light Cone

a concept used in describing the geometric properties of four-dimensional space-time in the special and general theories of relativity. The light cone corresponding to a given point in space-time is the three-dimensional surface in this four-dimensional space formed by the set of world lines of freely propagating light signals (or of any particles with zero rest mass) passing through the point, which is the vertex of the cone. Thus, to every point of four-dimensional space-time there corresponds a light cone.

In the case where the special theory of relativity is valid, the geometry of space-time is a pseudo-Euclidean geometry, called Minkowski geometry, in which all points of space-time are equivalent. Therefore, it is sufficient to consider a light cone with its vertex at the origin of coordinates *O*, where *x*= 0, *y* = 0, *z* = 0, and *t* = 0; where, *x, y*, and *z* are the space coordinates and *t* is the time coordinate. The equation of a light cone with vertex at *O* has the form *x*^{2} + *y*^{2} + *z*^{2} – *c*^{2}*t*^{2} = 0, where *c* is the speed of light in a vacuum. This equation is invariant with respect to Lorentz transformations. Points (events) with *x*^{2} + *y*^{2} + *z*^{2} ≤ *c ^{2}t^{2} and with t > 0 or t < 0 form what can be called the future and past interiors of the light cone—regions I and II, respectively, in Figure 1. Events with x^{2} + y^{2} + z^{2}* >

*c*

^{2}

*t*

^{2}form region III outside the light cone.

The intersection of a light cone with the plane *y =* 0, z = 0 is illustrated in Figure 1. The light cone intersects this plane along the straight line *x* = ± *ct.* Events *A* lying in region I form the absolute future with respect to the event *O.* Event *O* can exert a direct influence on any event *A*, since signals or interactions can connect *O* with *A.* Correspondingly, events *B* in region II form the absolute past for event *O.* Any event *B* can affect event 0, because signals from *B* can reach *O.* Events in region III cannot be connected with *O* by any interaction, since no particles or signals propagate faster than light.

Thus, the light cone separates events that can be in a causal relationship with *O* from events for which a causal relationship is impossible—this separation is the fundamental significance of the concept of the light cone. An observer located at *O* can know only of events in region II and can influence only events in region I.

In the presence of gravitational fields the world lines forming the light cone are not straight lines. In this case, the properties of the light cone near the vertex are the same as in the special theory of relativity. In the large, however, the properties are different, since the geometry of space-time is not pseudo-Euclidean.

I. IU. KOBZAREV