A four-vector is a quadruple aμ=(a0,a), μ=0,1,2,3, whose components mix under a boost exactly as (ct,r) do:
a′0=γ(a0−βa1),a′1=γ(a1−βa0),a′2,3=a2,3
for a boost at βc along x. Any two four-vectors give the invariant scalar product a⋅b=a0b0−a⋅b, the same number in every frame — the pattern behind c2t2−x2 and E2−p2c2. Position (ct,r) and four-momentum(E/c,p) are the two we have; electromagnetism now supplies three more: current, potential, and wave-vector.