The Feynman-Stueckelberg interpretation
Observer 1 sees two particles, one propagating inside the light cone, the other outside the light cone. Observer 2, moving at a uniform velocity with respect to the first observer, could then see the second particle as moving back in time, and with reversed charge: hence as an antiparticle. However, the mass and lifetime of such a particle would remain unchanged, as a consequence of relativity.By considering the propagation of the positive energy half of the electron field backward in time, Richard Feynman showed that causality is violated unless some particles are allowed to travel faster than light. However, if a particle is moving faster than light, another inertial observer would observe that the particle was traveling backward in time with the opposite charge.
Hence Feynman reached a pictorial understanding of the fact that the particle and antiparticle have equal mass m and spin J but opposite charges q. This allowed him to rewrite perturbation theory precisely in the form of diagrams, called Feynman diagrams, of particles propagating back and forth in time. This technique now is the most widespread method of computing amplitudes in quantum field theory.
This picture was independently developed by Ernst Stueckelberg, and has been called the Feynman-Stueckelberg interpretation of antiparticles.