I can't stop you from thinking whatever you want, no matter how irrational.
Now that we've covered the fact that I don't dismiss Kastner (in my
last post) we can address how you seem to think that misunderstanding Wikipedia is a sound basis for making assertions about the nature of gravitational waves and gravitation itself.
First, I addressed gravitational waves (including a link to the actual research paper touting the long-sought phenomenon itself here:
The gravitational waves discovered were not waves in either the classical or quantum sense, but do have more in common with the latter: Observation of
Gravitational Waves from a Binary Black Hole Merger.
Nor is this the first time I've had to explain that gravitational waves aren't really "waves" and they don't really "travel"
From my post
here:
They don't. They actually don't travel at all, really (like classical waves, they don't exist except as disruptions to the media in which they propagate). Gravity was nonlocal in classical physics in a way far more troubling than nonlocality in quantum physics. However, gravitational "waves" are produced locally via warping of spacetime:
"In the same way, in general relativity, Einstein’s field equations (1915) not only described the gravitational interaction via the spacetime curvature generated by mass-energy, but also contained, through the Bianchi identities, the equations of motion of matter and fields, and on their basis Albert Einstein, in 1916, a few months after the formulation of the theory, predicted the existence of curvature perturbations propagating with speed
c on a flat and empty spacetime; the gravitational waves"
Ciufolini, I., & Gorini, V. (2001). Gravitational waves, theory and experiment (an overview). In I. Ciufolini, V. Gorini, U. Moschella, & P. Fre, (Eds.)
Gravitational Waves (
Series in High Energy Physics, Cosmology and Gravitation) (pp. 1-10). IoP Press.
I also discussed gravitational waves (in passing) in a post on the fine-tuning problem
here and there relevance to the big bang and general relativity
here.
And here I am addressing it again, because apparently quote-mining Wikipedia shows an understanding of general relativity, gravitation, gravitational waves (much like reading one popular book immediately provides in-depth understanding of quantum physics).
So, what are gravitational waves? Intuitively, they are like "ripples" in spacetime. Gravity, as I already said, doesn't exist in our best model of gravitation but is spacetime curvature. Gravitational waves are propagations of perturbations to the "fabric" of spacetime (to spacetime curvature). They are predicted by general relativity.
Ok, that's a simple description, but what are GWs really? They are products of gravitational action in general relativity, i.e., S= Se +Sm (the Einstein and matter action) where Se=
and the all important energy-momentum tensor of matter is derived from the matter action by
Ok, all this seems irrelevant, but here's where it starts getting interesting. Take the variation of total action with respect to the curved spacetime metric and we get (surprise!) Einstein's equation
By expanding this equation around the flat spacetime metric using the symmetries of the so-called linearized theory and Lorentz transformations we can derive the linearized Riemann tensor, use it to derive the linearization of the Einstein tensor, apply the Hilbert gauge with the constraint
,and we get an equation with d'Alembertian flat space. We apply some function satisfying the constraint so trhat we can use the initial field configuration of the linear flat spacetime metric to give us a solution of the coordinate transformation function as a gauge integral over Green's function of the d'Alembertian operator:
Ok, now we are finally ready (and believe me, this description skipped A LOT of math that I would have included in any kind of realistic derivation). In the above gauge, several terms from the original coordinate transformation function mentioned above vanish and we can solve for
with a (simple) wave equation:
This is equation is the basis for GW computations (albeit in the simplified linearized theory). Things get considerably more complicated if we relax the linearization imposition, but the point is that the wave equation isn't at all akin the classical or quantum wave equations, but it does bear some resemblance to relativistic tensor algebras in electromagnetic field theories. Like classical waves, GWs propagate via a medium (light, the source for red shifts and so for, does not), that medium being spacetime. The above mathematics tells us perhaps the simplest propagation of GWs via the gravitational action on flat spacetime.