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Black hole vortex shifts quantum rhythm ⚡ экспресс

Original: "Aharonov-Bohm Effect for Cooper Pairs in Kerr Spacetime: Gravitomagnetic Phase Shifts from Frame Dragging"
· Erdem Sucu, İzzet Sakallı
arXiv:2602.20337 · 2026-02-23 · CC BY 4.0 · ⏱ 1 min · General Relativity HEP Theory
Calculations show that a black hole's spin can dramatically alter a superconductor's internal rhythm.
Abstract

The gravimagnetic Aharonov-Bohm effect is investigated for Cooper pairs in Kerr spacetime. The black hole's spin, through the off-diagonal metric component $$g_{t\phi}$$, creates an effective vector potential that shifts the phase of the superconducting condensate. For an interferometer with arms at radii $$r_1$$, $$r_2$$, a gauge-invariant phase shift is obtained: $$\Delta\theta = (4\pi m^* M a/\hbar)(1/r_2 - 1/r_1)$$, where $$m^*=2m_e$$ is the Cooper pair mass, $$a$$ is the black hole spin parameter. Near Sgr A* and M87*, phases of order $$10^{24}$$ and $$10^{27}$$ rad are predicted, reflecting the colossal gravimagnetic flux of supermassive objects. Tidal disruption of pairs is shown to be negligible at $$r \gtrsim 10\,r_s$$, and a connection to the Berry geometric phase is established. Direct verification is currently impossible due to distances, but the theory links quantum coherence with spacetime curvature, generalizing observations of gravitational Aharonov-Bohm phases in atomic interferometry.

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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.

The culprit is an effect discovered by Yakir Aharonov and David Bohm: the “wave rhythm” of a quantum particle (called its phase) can shift under the influence of an invisible field. Scientists applied this idea to electron pairs—the main carriers of superconductivity. Near a supermassive black hole (like Sagittarius A* at the center of the Galaxy) the phase shift reaches 10²⁴ radians. For comparison: a full turn of a clock hand is only about 6 radians, while here the shift is equivalent to billions of rotations.

We can't test it directly yet, but the same effect, only much weaker, is already being captured in Earth-based experiments: there, space is twisted by our planet’s rotation.

🎯 This shift is so huge that it would correspond to 10²³ full turns — trillions of times more than the number of stars in our Galaxy.

🎬 In the movie Interstellar, the characters saw how the black hole Gargantua twists space itself.

\Delta\theta = \frac{4\pi m^* M a}{\hbar} \left(\frac{1}{r_2} - \frac{1}{r_1}\right)
Δθ — phase shift (wave rhythm shift), m* — mass of the electron pair flowing without resistance (twice the electron mass), M — black hole mass, a — its spin parameter, ħ — fundamental quantum constant, r₁ and r₂ — distances from the black hole to the measuring device.
Scientists
Stephen HawkingJacob BekensteinAlbert EinsteinFritz ZwickyVera RubinBernhard Riemann
Tags
black hole spacetime curvature
Laws
Hawking radiationgravitational lensingBekenstein-Hawking entropyEinstein field equationsequivalence principleno-hair theorem
Original: arXiv:2602.20337 · CC BY 4.0 · bridge42worlds