2025
Circular motion and acceleration of charged particles around magnetized rotating black holes in scalar-tensor-vector gravity
KHAN, Saeed Ullah; Javlon RAYIMBAEV; Zhi-Min CHEN a Zdeněk STUCHLÍKZákladní údaje
Originální název
Circular motion and acceleration of charged particles around magnetized rotating black holes in scalar-tensor-vector gravity
Autoři
KHAN, Saeed Ullah; Javlon RAYIMBAEV; Zhi-Min CHEN a Zdeněk STUCHLÍK
Vydání
CHINESE PHYSICS C, 2025, 1674-1137
Další údaje
Jazyk
angličtina
Typ výsledku
Článek v odborném periodiku
Obor
10308 Astronomy
Stát vydavatele
Velká Británie a Severní Irsko
Utajení
není předmětem státního či obchodního tajemství
Odkazy
Impakt faktor
Impact factor: 3.100 v roce 2024
Organizační jednotka
Fyzikální ústav v Opavě
UT WoS
001584540100001
EID Scopus
2-s2.0-105017406490
Klíčová slova anglicky
particle acceleration;black holes;modified gravity;Penrose process
Příznaky
Mezinárodní význam, Recenzováno
Změněno: 21. 1. 2026 11:03, Mgr. Pavlína Jalůvková
Anotace
V originále
One of the most critical issues in relativistic astrophysics is explaining the origin mechanisms of (ultra)high-energy charged particle components of cosmic rays. Black holes (BHs), which are vast reservoirs of (gravitational) energy, are candidates for such energetic cosmic ray sources. The main idea of this study is to investigate the effects of scalar-tensor-vector gravity (STVG) and so-called modified gravity (MOG) on charged particle acceleration by examining their dynamics and acceleration through the magnetic Penrose process (MPP) near magnetized Kerr BHs in MOG (Kerr-MOG BHs). First, we briefly study the horizon structure of the Kerr-MOG BH. Then, we derive the effective potential for the circular motion of charged particles by considering electromagnetic and MOG field interactions on the particles to gain insight into the stability of circular orbits. Our results show that the magnetic field can extend the region of stable circular orbits, whereas the STVG parameter reduces the instability of the circular orbit. Thus, from the examination of particle trajectories, we observe that, at fixed values of other parameters, the Schwarzschild BH captures the test particle; in the case of the Kerr BH, the test particle escapes to infinity or is captured by the BH, while in the Kerr-MOG BH, the test particle is trapped in some region around the BH and starts orbiting it at a smaller value of the MOG field parameter. By investigating the MPP, we found that, in stronger magnetic fields, the behavior of orbits becomes more chaotic. As a result, the particle escapes to infinity with high energies.