Spacetime diagram with light cones illustrating relativistic physics

The light cone

PHYS 401 · Lorentz Transformations

The light cone separates events that can be causally connected from those that cannot. This lesson explains future, past, and elsewhere regions of spacetime.

Key equations

x=pm ctc^2t^2>x^2t>0t<0x^2>c^2t^2x^2=c^2t^2r^2=c^2t^2

Learning objectives

  • Define a light cone.
  • Identify future, past, and elsewhere regions.
  • Relate light cones to timelike, spacelike, and lightlike intervals.
  • Explain why causal order is invariant for timelike events.
  • Describe why spacelike time order can vary without violating causality.

Light as the boundary of causality

In special relativity, no information or material object can travel faster than light in vacuum. This makes light rays the boundary between events that can be causally connected and events that cannot.

A light cone is the set of all possible lightlike paths through an event. In a diagram with one space dimension and time, it appears as two crossing lines. With two space dimensions, it forms an actual cone.

Future light cone

Consider an event OO at x=0x=0 and t=0t=0. Light emitted from that event satisfies

x=pmctx=pm ct

in one spatial dimension. Events inside the future light cone satisfy

c2t2>x2c^2t^2>x^2

with t>0t>0. These events can be reached by slower-than-light signals or objects from OO.

The future light cone contains events that OO can influence.

Past light cone

The past light cone contains events that could have influenced OO. These are timelike or lightlike events with t<0t<0 relative to OO.

For example, the light reaching your eyes from a star tonight lies on your past light cone. The star as you see it is not at the star's current distant-frame time; it is an event in your causal past.

Elsewhere

Events outside the light cone are spacelike separated from OO. In one spatial dimension, they satisfy

x2>c2t2x^2>c^2t^2

No signal traveling at or below cc can connect them to OO. They are sometimes called elsewhere because they are neither in the causal past nor causal future of the event.

Different inertial observers may disagree about the time order of spacelike events, but all agree that they are spacelike.

Lightlike boundary

Events exactly on the cone satisfy

x2=c2t2x^2=c^2t^2

or in three spatial dimensions,

r2=c2t2r^2=c^2t^2

They can be connected to OO only by light or another massless signal traveling at cc.

Causal order

For timelike-separated events, all observers agree on their time order. If event A can cause event B, no Lorentz transformation can reverse that order.

For spacelike-separated events, time order is frame-dependent. But because no causal signal can connect them, this does not create causal contradiction.

Worldlines and cones

The worldline of a massive particle must stay inside its local light cone. A light ray follows the cone surface. A hypothetical faster-than-light path would go outside the cone, creating serious causality problems in special relativity.

Relativity and the present

The light cone also challenges the idea of a universal present. Different observers slice spacetime into simultaneous surfaces differently. The invariant structure is not a universal now, but the causal cone structure shared by all observers.

The big idea

The light cone organizes spacetime into causal future, causal past, and elsewhere. Timelike and lightlike events can be causally connected; spacelike events cannot. All inertial observers agree on this causal classification, even when they disagree about simultaneity or time order for spacelike events.

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