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Dynamics of charged particles and magnetic dipoles around magnetized quasi-Schwarzschild black holes

机译:磁化准施瓦茨柴尔斯黑洞带电粒子和磁偶极子的动态

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In the present paper, we have investigated the motion of charged particles together with magnetic dipoles to determine how well the spacetime deviation parameter $$epsilon $$ ? and external uniform magnetic field can mimic the spin of a rotating Kerr black hole. Investigation of charged particle motion has shown that the deviation parameter $$epsilon $$ ? in the absence of an external magnetic fields can mimic the rotation parameter of the Kerr spacetime up to $$a/M pprox 0.5$$ a / M ≈ 0.5 . The combination of an external magnetic field and deviation parameter can do even a better job mimicking the rotation parameter up to $$a/Msimeq 0.93$$ a / M ? 0.93 , which corresponds to the rapidly rotating case. Study of the dynamics of the magnetic dipoles around quasi-Schwarzschild black holes in the external magnetic field has shown that there are degeneracy values of the ISCO radius of test particles at $$epsilon _{cr}epsilon ge 0.35$$ ? cr ? ≥ 0.35 which may lead to two different values of the innermost stable circular orbit (ISCO) radius. When the deviation parameter is in the range of $$epsilon in (-1, 1)$$ ? ∈ ( - 1 , 1 ) , it can mimic the spin of a rotating Kerr black hole in the range $$a/M in (0.0537, 0.3952)$$ a / M ∈ ( 0.0537 , 0.3952 ) for magnetic dipoles with values of the magnetic coupling parameter $$eta in [-0.25, 0.25]$$ β ∈ [ - 0.25 , 0.25 ] in corotating orbits.
机译:在本文中,我们研究了带电粒子的运动与磁性偶极子一起,以确定空间偏差参数如何达到数量$$ epsilon $$?外部均匀磁场可以模仿旋转克尔黑洞的旋转。对带电粒子运动的调查显示,偏差参数$$ epsilon $$?在没有外部磁场的情况下,可以模拟kerr spacetime的旋转参数,高达$$ a / m 约0.5 $$ a /m≈0.5。外部磁场和偏差参数的组合可以做出更好的作业,模拟旋转参数,最高可达$$ a / m simeq 0.93 $$ a / m? 0.93,其对应于快速旋转的情况。对外部磁场中的Quasi-Schwarzschild黑洞周围的磁偶极子的动态研究表明,在$$ epsilon _ {cr}&gt. epsilon ge 0.35 $的ISCO _ {CR}&gt.75 $ $? CR&还≥0.35,可能导致最内稳定圆形轨道(ISCO)半径的两个不同值。当偏差参数处于$$ epsilon IN(-1, 1)$$范围内时? ∈( - 1,1),它可以模仿旋转克尔黑洞的旋转的旋转克尔黑洞(0.0537, 0.3952)$$ a / m∈(0.0537,0.3952)的磁性偶极子磁耦合参数的值$$ beta 在[-0.25, 0.25]中的计量轨道中的$$β∈[ - 0.25,0.25]。

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