It might be easier to go the other way and say that "real current" has no more actual existence than "displacement current".
This. Current is a mathematical concept, and as such we are free to define it however we like. It turns out that 99% of the time, the only useful thing to call current is the total current (charge motion + displacement current). Taken individually, those concepts are almost entirely useless for describing any sort of electrical behavior, except in the limit where one of them is zero. In every equation you have ever seen, the symbol 'I' means the total current.
Radiation doesn't look like current flow because the displacement currents are transverse to the propagation direction. The the current flux through, for example, a plane separating the emitter and receiver is zero. But if you have a volume of otherwise empty space with radio waves traveling through it, then yes, the current density is non-zero. That is the difference between near- and far-field.
Every physicist I know regards displacement current as 'just as real' as charge motion. Electrical engineers probably don't think about it as much, but they implicitly agree because all of the equations they use to design and describe circuits treat the two as equivalent.
Finally, as a trivial point, the bulk of the current in most capacitors is actually due to microscopic charge motion. The relative permitivity of most capacitor dielectrics is much greater than 1, so the majority of the current comes from reorienting microscopic dipoles withing the dielectric. If you use the version of maxwell's equations for dielectrics (the one that includes H and D fields instead of just B and E), that would be a displacement current, but it is due to physical charge motion.