$l_P{\left({210}^{210}{\left(8e\right)}^{-1/2}\right)}^{1/4}$

9.0785

holic central term ${210}^{210}\approx {\tau }^{2m/3}\approx e^{e2m}\approx {\tau }_0{}^{d_e{}^4{r}_H/{ƛ}_e}$ ${\tau }_0=3470$

$l_P\sqrt{2}{\left(p_t/n_t\right)}^6{e}^{280}$

9.0767

base e

$l_P\left(Z{d}_e/W\right)7^{{12}^2}$

9.075

base 7

${ƛ}_e{6}^{128}/\left(1+1/\sqrt{2}\right)$

9.075

base 6; $6/\left(1+1/\sqrt{2}\right)\approx \mu d_e^2/\sqrt{\tau }$

${ƛ}_e{e}^{1/2a}{6}^{p_G/\sqrt{a}}$

9.076

base 6

$2r_H{3}^{210}/1830$

9.076

base 3 Holic term, with $1830=\left(60\times 61\right)/2$

${ƛ}_e{\left(1+1/\sqrt{2}\right)}^{6a_s^2+1}$

9.085

base $1+1/\sqrt{2}$

${ƛ}_e{5}^{2a_s^2+1}/6$

9.082

base 5

$l_P{\left(7/6\right)}^{{\left(1836p\right)}^{1/2}}/2e^2$

9.085

base $7/6\approx a^{1/32}$

${ƛ}_e{\left({\left(1/q\right)}^a\mathrm{<mi>\; </mi>}W/aF\right)}^2$

9.082

base 1/q

$l_P{e}^{s_{65}{n}_{t}q/2p_W}$

9.077

confirms the terminal Euler number $s_{65}=1848$

$l_P\left(p/H\right){\left(R{\Pi }_{26}/R_e\right)}^{1/3}$

9.076

with the product of orders of the 26 sporadic groups $e^{674.5210287}$ [5]

${ƛ}_{e}g\left(7\right){\left(H/p\right)}^{2}P/6$

9.076

with the reduced topologic function for $d=30:g\left(7\right)=f\left(30\right)/7$ [5]

$24{ƛ}_e{\pi }^{210}/a^3$

9.077

confirms the base $\pi$ holic term

$a^2{\lambda }_{Wien}^4/{\left(p_K{l}_P\right)}^3$

9.078

confirms $T_{CMB}$ with $p_K=\left(1+\mu +\tau \right)/2$ [35]

${ƛ}_e{\left(\left(3/4\pi \right){\left(R_1/{ƛ}_e\right)}^7\right)}^{1/3}$

9.078

comes from the de photons nomber, using the mono-electron radius $R_1$ [5]

${ƛ}_e{137}^{1836/{\left(2\pi \right)}^2}$

9.078

base 137

$\sqrt{3}{l}_{nl}^3/r_e{l}_P$

9.07

with the non-local length $l_{nl}$

${ƛ}_{e}g\left(7\right){\left(a^2{p}_t{p}_G\right)}^2$

9.08

[5]

$l_P{j}^{60}{e}_3^{1/4}$

9.06

base j, the scale factor

$l_P{e}^{{\left(n_t/a\right)}^2/g_2}{\left(3/\pi \right)}^{1/2}$

9.06

base e, confirms $g_2$

$l_P{\left(n_t^2/l_p\right)}^{2/{\left(\sin {\theta }_1\right)}^4}$

9.06

bases $p_t$ and $n_t$

${\left(\ln \left(R_c/{ƛ}_e\right)\right)}^2\approx {\left(\ln \left(M_e/m_e\right)\right)}^2+2\left(\ln {\left(R/{ƛ}_e\right)}^2\right)$

9.12

c-observable Universe Cosmos couple $\left(R/{ƛ}_e=t/t_e\right)$ , Figure 1

${\text{ł}}_P{\left(6/\pi \right)}^{\pi a}$

9.14

base $6/\pi$

${ƛ}_{e}g\left(7\right){\left({ƛ}_{CMB}/r_H\right)}^3$

9.1

confirms the invariance of the thermal background [5]

${\left(R{l}_{nl}\right)}^{3/2}/r_e^2$

9.2

from non-local holography [5]