Strong gravitational lensing, quasi-periodic oscillations and constraints from EHT observations for quantum-improved charged black hole

Abstract

AbstractWe investigate strong gravitational lensing by quantum-improved charged black holes characterized by an additional parameter denoted as $$\omega $$ ω , in addition to the mass M and charge Q. Our findings reveal that when both the parameters Q/2M and $$\omega /4M^2$$ ω / 4 M 2 increase simultaneously, various astrophysical consequences, such as the deflection angle $$\alpha _D(u)$$ α D ( u ) and angular image separation increase. Concurrently, the angular position $$\theta _{\infty }$$ θ ∞ , relative magnification $$r_{mag}$$ r mag , and the time delay $$\Delta T_{2,1}$$ Δ T 2 , 1 between the first and second relativistic images also decrease with the growing values of the parameters Q/2M and $$\omega /4M^2$$ ω / 4 M 2 . It is also observed that the Einstein ring $$\theta _1^E$$ θ 1 E for the quantum-improved charged black hole is more significant than those for Schwarzschild, quantum-improved Schwarzschild, and Reisner–Nordström black holes. As with supermassive black holes such as $$M87^*$$ M 87 ∗ and $$SgrA^*$$ S g r A ∗ , it is observed that to be a viable astrophysical black hole, the EHT results constrain the parameter space ($$\omega /4M^2$$ ω / 4 M 2 , Q/2M). Remarkably, the EHT results for $$SgrA^*$$ S g r A ∗ impose more stringent limits on the parameter space of quantum-improved charged black holes compared to those established by the EHT results for$$M87^*$$ M 87 ∗ . We investigate the radial profiles of orbital and radial harmonic oscillation frequencies as a function of the dimensionless coupling constants and black hole mass. The main characteristics of test particle quasi-periodic oscillations close to stable circular orbits in the black hole equatorial plane are also examined. We study the positioning of resonant radii in the background of quantum-improved charged black holes for high-frequency quasi-periodic oscillations models: warped disc (WD) models, relativistic precession (RP) and its types, and epicyclic resonance (ER) and its variants.