İzzet Sakallı

6 articles · 7 co-authors · latest: 2026-07-31
3,462 citations · h-index 32 · 258 papersData: Semantic Scholar

We have retold 6 papers by this author. 1 of them with a full read. most often about: black hole, gravitational singularity, event horizon. 7 co-authors across our retellings.

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General Relativity2026-02-231 minarXiv:2602.20337express
Black hole vortex shifts quantum rhythm
A spinning black hole drags spacetime with it, like a spoon swirling thick honey. This vortex is a manifestation of curved spacetime. But the key point: it can change the quantum rhythm of matter, even where there are no forces.
General Relativity2026-05-261 minarXiv:2605.26696express
Time Can Still Be Tricked
Some solutions to Einstein's equations allow closed timelike curves — loops that let you travel to the past. Two well-known designs, the Ori geometry and the Ahmed geometry, do without exotic matter, catching physicists' eyes.
General Relativity2026-07-052 minarXiv:2607.04173express
Black Hole with a Quark Secret
At the centers of many galaxies lurk supermassive black holes. One of them, Sagittarius A* at the heart of the Milky Way, has become a testing ground for a new idea. The authors of the work took Einsteinian gravity and added an unusual electromagnetic field to it.
General Relativity2026-07-082 minarXiv:2607.07741express
Cosmic Mirage: How the Solar Bubble Is Reshaping the Map of the Universe
The cosmological debate is like two craftsmen measuring the same wall but getting different lengths. One uses a tape measure, applying it to nearby landmarks — Cepheids (pulsating beacon stars) and Type Ia supernovae (flashes of dying stars). He finds the wall is stretching at 73.5 arbitrary units.
General Relativity2026-07-311 minarXiv:2608.00305express
A Black Hole with Bristles and Its Shadow
A black hole doesn't just spin: it's surrounded by bristles of an extra field (the Kalb–Ramond field). This paper explores how a massive field (waves with mass) behaves near such a black hole when it's almost spinning at its maximum rate. The Klein–Gordon–Fock equation for this field was separated into two independent parts — radial and angular.