Electromagnetic accelerating universe

Observables for moving, extremely charged primordial extremely massive black holes

“…These masses are chosen because they are small enough to be found in a volume with radius of about 100 Mpc around us to allow for relatively cosmology-independent searches for CPEMBH-signals. They are also the lowest masses for which the Coulomb force overcomes their mutual gravitational attraction, as derived in [9]. The results shown in Section 3 support that non-relativistic calculations are utterly sufficient.…”

“…The latter was found to apply to our universe supported by observations of the cosmic microwave background, [20]. After [3] showed that it is possible to create PBHs with charges, [9,12] extended this idea to PEMBHs and found that these nonrotating, charged PEMBHs (CPEMBHs) may be able to explain the observations of an accelerated cosmic expansion. This paper investigates observational consequences entailed by the existence of such CPEMBHs with the aim to detect individual CPEMBHs in the late universe.…”

“…Like in [9], we assume that the Newtonian limit of weak gravitational fields applies, i. e. that all distances to the CPEMBHs are much larger than their extent. We also assume that all objects move with velocities much smaller than the speed of light c in a flat space-time.…”

“…with p i and q i being the exponents of the masses M i = 10 p i M , expressed in units of solar masses M , and Q i = 10 q i C, as introduced in [9]. As usual, m e and m p denote the mass of the electron and the proton, respectively, and e the charge of the electron.…”

“…As usual, m e and m p denote the mass of the electron and the proton, respectively, and e the charge of the electron. Using a linear interpolation for the Q/M -ratio of charged black holes given in [3], [9] derived the relation…”