index $ \def \MET {\quad \mbox{with} \quad} \def \SP {\quad \mbox{;} \quad} \def \hieruit {\quad \Longrightarrow \quad} \def \slechts {\quad \Longleftrightarrow \quad} \def \EN {\quad \mbox{and} \quad} \def \OF {\quad \mbox{or} \quad} \def \half {\frac{1}{2}} $
My approach insists that an gravitational (self) energy field must exist (I'm not sure about a proper name). But it may be that we are talking about the same thing. And if such is the case, then a more detailed account of the properties of our "aether" is given in Self Energy Field. It is shown beneath the last horizontal rule in the webpage that in the neighborhood of our sun this Energy Field / your Aether might provide an alternative explanation for the Perihelion precession of Mercury.
It has been derived that mass and radius of our so-called Observable universe are respectively given by
$$
M_O = \frac{W}{2}\frac{c^3}{G.H} \quad ; \quad R_O = W\frac{c}{H} \quad \mbox{where} \quad W = 3.383634283
$$
$c=$ lightspeed, $G=$ gravitational constant, $H=$ Hubble parameter. Numerically: $M_O \approx 2.87\times 10^{53}\mbox{ }kg$, $R_O \approx 4.26\times 10^{26}\mbox{ }m$.
But the Aether itself contains gravitational field energy and therefore it has also a mass, which is derived to be
$$
M_A = - \frac{G}{c^2}\frac{M_O^2}{2R_O}.W.\mbox{VMT} \quad \Longrightarrow \quad
-\frac{M_O}{M_A}=\left(\frac{1}{4}W^2.\mbox{VMT}\right)^{-1} \approx 15.47019772
$$
The mass of our thus defined Aether is roughly fifteen times smaller and negative when compared with the Observable mass.
Let's proceed with a firm disclaimer, as expressed by Louis Marmet via A Cosmology Group
(18 dec. 2022 04:23): How many 'effects' are required to explain the CMB? 12? 20? I fall asleep reading these
arguments based on a contrived set of explanations that are just as unlikely as the other ... To me, it's a sign of bad science -
you are not missing much ;-) Abort, Retry, Fail?
If there is something in the universe which has a uniform mass / energy density and provides sort of a rest frame at the same time,
then it certainly is the Cosmic Microwave Background.
According to the Stefan-Bolzmann law of thermal radiation,
the energy density of the CMB is given by equation (78) in a book by Max Planck:
THE THEORY OF HEAT RADIATION.
Symbols are: $u=$ energy. $\sigma=$ Stefan-Boltzmann constant,
$\Theta=$ CMB temperature (Kelvin), $m=$ mass, $V=$ volume. Because we are talking about volumes, not a surface in space, according to
Wikipedia: the radiation constant
(or radiation density constant) $\,a=4\sigma/c_0\,$ must be employed.
$$
u_{CMB} = a\,\Theta^4
$$
On the other hand, we have the gravitational Self Energy Field with a total energy
$$
U_G = - \frac{G M_O^2}{2R_O}.W.\mbox{VMT}
$$
We are not going to spend much of eloquent proze on the subject. Instead it is simply assumed that
We repeat the most important results from the previous. A purely mathematical result first: $$ f(x) = \frac{2-e^{-x}(x^2+2x+2)}{x} \quad \mbox{with} \quad W = 3.383634283 \quad \mbox{and} \quad w = f(W) = 0.3883945571 $$ For the mass $M_O$ and radius $R_O$ of our Observable universe we find (with $c=$ lightspeed, $G=$ gravitational constant, $H=$ Hubble parameter): $$ M_O = \frac{W}{2}\frac{c^3}{G.H} \quad \mbox{;} \quad R_O = W\frac{c}{H} $$ The total gravitational self energy of our Observable universe has been correctly calculated so far, but as a Variable Mass (with $E=m_0c^2$) it is redshifted as it enters the horizon (also called the rim), in the form of CMB radiation. That redshift canot be else than the maximal observable one, namely $1+z_{max} = e^W$ and so: $$ U_G = - \frac{G M_O^2}{2R_O}.W.\mbox{VMT} / e^{W} \quad \mbox{where} \quad \mbox{VMT} = \int_W^\infty \frac{e^{-x}}{x^2}dx $$ Furthermore it went wrong (with $\sigma=$ Stefan-Bolzmann constant, $\Theta=$ temperature) at the place where we thought that $$ U_{CMB} = \frac{4}{3}\pi R_O^3.\frac{4\sigma}{c}\Theta^4 $$ When multiplied with mass density instead of radiation density, the mass of the Observable universe can never be greater than the mass of the whole Universe. The latter has been calculated in an earlier stage. We must substitute $\rho_0 \to 4\sigma/c.\Theta^4$ and then formulate correctly instead (with $x=W.c/H$ ): $$ U_{CMB} = \frac{4\sigma}{c}\Theta^4 \int_0^{R_O} e^{-H/c.r}.4\pi r^2.dr = \frac{4\sigma}{c}\Theta^4 \left(\frac{c}{H}\right)^3 4\pi \int_0^{W} e^{-x}x^2.dx \\ = \frac{4\sigma}{c}\Theta^4 \left(\frac{c}{H}\right)^3 4\pi \left[\frac{2-e^{-W}(W^2+2W+2)}{W}\right]W = 4\pi.wW \left(\frac{c}{H}\right)^3 \frac{4\sigma}{c}\Theta^4 $$ Leading to the following end-result. $$ 4\pi.wW \left(\frac{c}{H}\right)^3 \frac{4\sigma}{c}\Theta^4 = G\left[\frac{W}{2}\frac{c^3}{G.H}\right]^2\frac{W.\mbox{VMT}/e^W}{2(W.c/H)} \\ \frac{4\sigma}{c}\Theta^4 = \frac{W^2.\mbox{VMT}.e^{-W}}{32\pi.wW}\frac{(Hc)^2}{G} $$
W := 3.383634283; G := 6.67408*10^(-11); Mpc := 3.08567758*10^22; H := 73.4; # Riess H := H*1000/Mpc; c := 299792458; VMT := int(exp(-x)/x^2,x=W..infinity); sigma := 5.670374419*10^(-8); wW := 2-exp(-W)*(W^2+2*W+2); u_G := W^2*VMT/(32*Pi*wW)*(H*c)^2/G; u_G := u_G*exp(-W); # But I'm not sure Theta := evalf((c/(4*sigma)*u_G)^(1/4)); Theta := 2.764453563The small discrepancy with experiment that is remaining can easily be explained by the uncertainty of the Hubble parameter. Calculating the other way around:
Theta := 2.726; H := sqrt((G/c^2)*(32*Pi*wW)/(W^2*VMT*exp(-W))*4*sigma/c*Theta^4); H := evalf(H/1000*Mpc); H := 71.37221336Which is compatible with the Hubble tension.
It has been shown in A Special Escape that the mass $M$ of (for example) the observable universe inside,
via the escape velocity, must be augmented as well. Resulting in a mass $M'$ which is the original $M$ plus the negative mass of its
Self Energy Field:
$$
v=\sqrt{\frac{2GM}{R}-\left(\frac{GM}{Rc}\right)^2}=\sqrt{\frac{2GM'}{R}} \quad \mbox{with} \quad M' = M + \left[-\frac{GM^2}{2Rc^2}\right]
$$
Therefore Special Relativity would enable the above disastrous iteration process to proceed, if it were not that the Self Energy Field
is neutralized by a positive energy field, which may be conjectured to be the CMB again.
But how can the latter be redshifted by $e^{-W}$ now? We could argue that our theory is in some sense analogous to the Big Bang story.
Trying to tell everybody that the CMB is primordial, a relic, with maximal redshift. The latter, in our case, is inevitably limited
with the factor $e^{-W}$ . Then we are done, aren't we ?
Whatever. When specified for the Observable universe we obtain
$$
M'_O = \frac{W}{2}\frac{c^3}{G.H}(1-g) \quad ; \quad g = \frac{W^2}{4}\mbox{VMT} \quad ; \quad R_O = W\frac{c}{H} \\
v = \sqrt{2G\frac{W}{2}\frac{c^3}{G.H}\frac{H}{Wc}(1-g)} \hieruit \Large\boxed{v = c\sqrt{1-g}} \normalsize \approx 0.9671398994 \times c
$$
With Special Relativity, the escape velocity from the Observable universe is calculated to be slightly less than the speed of light.
As a consequence, light can escape from - as well as enter into - that part of the universe.
With the relic radiation as a paradigm, the discrepancy with lightspeed becomes even smaller:
$$
g = \frac{W^2}{4}\mbox{VMT}.e^{-W} \hieruit v = c\sqrt{1-g} \approx 0.9989029695\times c
$$
Why does the CMBR show such a precise black-body radiation spectrum? No elementary particles are involved with its birth, just gravity and photons. So what else could the spectrum have been? There is a more rigorous argument, though. According to Planck's law (Wikipedia) the spectral radiance of a body for frequency $\,\nu\,$ at absolute temperature $\,\Theta\,$ is given by $$ B(\nu,\Theta) = \frac{2h\nu^3}{c^2}\frac{1}{\exp\left(\frac{h\nu}{k_B\Theta}\right)-1} $$ where $\,k_B\,$ is the Boltzmann constant, $\,h\,$ is the Planck constant, and $\,c\,$ is the speed of light in vacuum. With the Variable Mass Theory, frequency and temperature are subject to change as has been explained in our Support by Hoyle section. The other quantities remain constant. $$ \frac{\nu}{\nu_0} = \frac{\Theta}{\Theta_0} = \frac{m}{m_0} \hieruit \frac{B}{B_0} = \left(\frac{m}{m_0}\right)^3 = (1+z_i)^{-3} $$ Leading to the important conclusion that black body radiation is invariant with varying elementary particle (rest) mass. More precisely: the magnitude of the spectral radiance may be different, but the shape of its distribution does not change. Very much the same is expressed by Wien's displacement law ($\lambda=$ wavelength) which turns out to be invariant as well. $$ x \equiv \frac{h\,c}{\lambda_{peak}\,k_B\,\Theta} \quad \mbox{with } \,x\, \mbox{ as the (dimensionless) solution of} \quad (x-5)\,e^x+5=0 \\ \frac{m}{m_0} = \frac{\Theta}{\Theta_0} = \frac{\lambda_0}{\lambda} \hieruit \frac{h\,c}{\lambda_{peak}} = x\,k_B\,\Theta \quad \mbox{with} \quad x = 4.965114231744276304 $$