The field-dependent invariant representation ( the dynamical representation
) of the Poincare algebra is considered as a dynamical principle in order t
o get a corresponding dynamical electromagnetic coupling for higher spins (
s greater than or equal to 1). If in lower-spin (s = 0, 1/2) cases the dyna
mical coupling is taken to coincide with the minimal electromagnetic coupli
ng, the higher-spin coupling is inevitably non-minimal, containing a term l
inear in the field strength tensor F-muv. This non-minimal coupling leads t
o g = 2.