CallMeDirac said:
I've just always heard...
Where? Please give a specific reference.
CallMeDirac said:
there is an argument as to weather gravity is a field or a particle.
This doesn't really make sense. "Field" and "particle" are not two different kinds of things according to our current understanding of quantum field theory. They're just two different names for the same thing. "Field" is the more common name--more specifically, "quantum field"--and "particle" is usually taken to mean a certain type of state of a quantum field. So it doesn't make sense to ask whether anything "is" a field or a particle; at most it might make sense to ask whether a particular physical phenomenon has a useful description in terms of particle-like states of quantum fields, or not.
The particular issue with gravity is that we don't have a good quantum theory for it, whereas we do have one for the other known interactions (strong, weak, electromagnetic, all well described by the Standard Model). We know it is mathematically possible to construct a quantum field theory for a massless, spin-2 field; this field would be the "graviton" field, and particle-like states of it would be "gravitons". And the field equation for this theory, in the classical limit, is the Einstein Field Equation of General Relativity, so mathematically this quantum field theory would be a natural extension of GR to a QFT, just as quantum electrodynamics is the natural extension of classical Maxwell electrodynamics to a QFT (the field equation of QED in the classical limit is Maxwell's Equations).
However, the QFT of a massless spin-2 field just described is not renormalizable (unlike QED and the rest of the Standard Model, which is), and any quantum effects it predicts for gravity would not be observable unless we could do experiments at the Planck scale, which we can't now and won't be able to for the foreseeable future. So this theory doesn't really offer any hope of being a useful quantum theory of gravity.
Furthermore, this QFT is a QFT on a background flat spacetime, which ends up predicting that that background flat spacetime is unobservable; the observable spacetime geometry is the curved spacetime geometry described by the classical limit of the theory (which, as noted, is just GR). It would be much nicer to have a quantum theory that just gave us curved spacetime GR directly as a classical limit, without having to make any assumptions at all about a background spacetime. This is the sort of theory that efforts like loop quantum gravity are working on.
CallMeDirac said:
I was wondering why it's never presented as the same as the Higg's boson and field
Because none of the issues I described above arise at all for the Higgs boson and the Higgs field. The Higgs field and the Higgs boson are perfectly well described by the current Standard Model.
CallMeDirac said:
Congrats by the way on the hall of legends
Thanks!