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Astrons: Electric Leviathans That Defy Cosmology

Original: "Astrons: Reissner-Nordström Primordial Naked Singularities"
arXiv:2605.10587v1 · 2026-05-11 · CC BY · ⏱ 3 min · High Energy General Relativity HEP Phenomenology
Born in the flames of the Big Bang, supermassive charged giants rewrite the laws of gravity — but their reality hangs by a thread.
Abstract

The hypothesis of astron existence—primordial supermassive objects with a large electric charge—is examined. The analysis showed that ordinary accretion yields a charge far below expectations, and intergalactic plasma quickly screens it—like a cosmic-scale grounding. Additionally, a strong charge drives the spacetime geometry around the object into a super-extreme regime, which is problematic. The interaction of such objects cannot explain the accelerated expansion of the Universe, but they could act as dark seeds for the early galaxies seen by the James Webb Space Telescope.

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In the searing plasma of the newborn Universe, when space itself still rang with the echo of the Big Bang, objects may have emerged that challenge gravity itself. Not ordinary black holes — but electrically charged giants, astrons. Their mass is like that of a million billion suns, and their electric repulsion is five times stronger than gravitational attraction. Invisible yet all-pervading: according to a bold hypothesis, they, like an unseen hand, push galaxies apart, replacing dark energy in the accelerating expansion of the Universe.

Imagine a fleet of leviathans scattered across the cosmic void, like seeds of a giant crystal, separated by megaparsecs. Each carries a charge as if billions of ball lightnings were compressed inside it. In their heart lies a naked singularity: the parameter Ξ = k_e Q²/(G M²) reaches 5.4 — not the paltry fractions of unity found in stars. Gravitational garments — the event horizon and photon sphere — have been torn from the titan’s shoulders, exposing the twisted guts of warped spacetime. The Reissner–Nordström solution, hybridizing the Schwarzschild metric with Maxwell's electrodynamics, delivers a harsh verdict: horizons survive only for Ξ ≤ 1, and the photon sphere only for Ξ ≤ 9/8.

If such an astron were nearby, astronomers would not find the familiar shadow of a black hole. Light does not whirl in a gravitational waltz — it merely bends slightly, painting a ghostly arc on the sky instead of a bottomless oval of darkness.

But the cosmos does not forgive idealizations. Intergalactic plasma — a pervasive ocean of charged particles — muffles electric fields like a wet blanket smothering a ringing bell. On distances smaller than the typical inter-astron spacing, the field fades, and the leviathans stop 'hearing' each other, losing their collective strength. Worse still: ordinary charging via an accretion disk in the intergalactic medium yields only laughably small Ξ, so the birth of giants requires exotica — for instance, charge separation during a quantum-gravitational phase. And in the homogeneous Friedmann–Lemaître model, bequeathed by Lemaître, Coulomb energy masquerades as radiation with a density ∝ a⁻⁴ and gets diluted by expansion too quickly to compete with dark matter and dark energy.

Place astrons of mass ~10¹² M☉ at every megaparsec — their total density Ω_A ≈ 7.9 instantly exceeds the critical value. The real population must be far sparser, otherwise the Universe would have recollapsed.

The Einstein–Maxwell equations do not forgive hubris. If astrons are real, the acceleration of expansion is not a monotonous fluid pressure but a complex dance of gravitational inhomogeneities. Each naked singularity tugs spacetime toward itself, and the ensemble’s averaged rhythm gives rise to a cosmological crescendo. Verifying such a drama will require numerical simulation of nonlinear plasma processes near superextremal objects and an exact solution of the backreaction problem. Telescopes like JWST can search for faint lensing anomalies or redshift features betraying the presence of these ghostly titans. The astron scenario sharply raises questions about cosmic censorship, the nature of singularities, and quantum gravity. And if the horizon vanishes, Hawking evaporation loses its usual meaning — can a naked singularity decay? This puzzle reminds us: the darkest mystery may hide not in a new field, but in electrodynamics pushed to its absolute limit.

🎯 The astron paradox: electric repulsion, five times stronger than gravity, rips the event horizon off the singularity, exposing it for all to see. This is a direct violation of the cosmic censorship principle, challenging the very predictive power of physics.

\Xi = \frac{k_e Q^2}{G M^2}
If Ξ > 1, electric forces exceed gravitational ones; for the reference scenario astrons, Ξ ≈ 5.4
f(r) = 1 - \frac{2GM}{c^2 r} + \frac{G k_e Q^2}{c^4 r^2}
Describes the gravitational field of a charged non-rotating compact object; the second term is the standard Schwarzschild one, the third is the charge contribution, which for large Q completely alters the horizon structure
Scientists
Alan GuthAndrei LindeGeorges LemaîtreJames PeeblesAdam RiessBrian Schmidt
Tags
dark energy dark matter black hole plasma spacetime curvature expansion of the universe JWST interstellar medium Accretion disk redshift numerical simulation
Laws
Friedmann equationsHubble's lawHawking radiationgravitational lensingBekenstein-Hawking entropyEinstein field equations
Original: arXiv:2605.10587v1 · CC BY · bridge42worlds