论文标题

Bardeen黑洞在4D EGB重力中通过Bardeen黑洞的强力镜头:超级质量黑洞的约束

Strong gravitational lensing by Bardeen black holes in 4D EGB gravity: constraints from supermassive black holes

论文作者

Islam, Shafqat Ul, Ghosh, Sushant G., Maharaj, Sunil D.

论文摘要

观察表明,附近的许多星系都有超大型中央黑洞。在四维爱因斯坦 - 高斯 - 摩孔(4D EGB)重力中对Bardeen模型进行建模,并带有其他参数$ \tildeα$并充电$ Q $,作为各种星系中的中央黑洞,我们研究了强偏置限制的重力镜头。有趣的是,球形光子轨道半径$ x_m $,关键的冲击参数$ u_m $,镜头系数$ \ bar {b} $,挠度角$α_d(θ)$,角度位置$θ__ {\ infty} $与$ q $ and $ q $和$ alens $ a $ a $ a $ a $ ness $ a,当分离$ s $具有相反的行为。以镜头为镜头,将超级质量的黑洞SGR A*和M87*作为镜头进行了比较,将4D EGB Bardeen黑洞的可观察签名与Schwarzschild黑洞的签名进行了比较。 $(23.1853,\; 23.56427)$ $ us的角位置$θ_\ infty $ as in $ a* $ \ as as as as as as as as as as $ us,而M87*是$ \ in $(17.941,\; 19.7819)$ $ $ us。此外,Angular Eaparation $ S $,这是$ \tildeα$和SGR A*和M87**的$ \tildeα$和$ Q $的增加,在(0.031997,0.14895)$ us as和(0.0247,0.1152)$ $ as as in(0.031997,0.14895)中。镜头可观察的$δθ_ {\ infty} $和4D EGB Bardeen黑洞($ \ \tildeα= 0.9,〜q = 0.09 $)的$ΔS$分别从Schwarzschild Black Hole中分别达到2.3789〜 $ 0.1165〜ISS, $ 1.84084〜μ $ AS和$ 0.0905〜μ $,如M87*。另一方面,相对放大$ \ in $(4.65751,\; 6.82173)。考虑到二十二个巨大的中央黑洞,我们还估计了第一和第二相对论图像之间的时间延迟$Δt^s_ {2,1} $,例如,SGR A*和M87*的时间延迟延迟可以达到$ \ sim9.86088 $ 〜min和$ 〜min and $ \ sim16633.933.933.933.933.933.9333.933.93 $ 〜imin。

Observation indicates that many nearby galaxies host supermassive central black holes. Modelling Bardeen models in four-dimensional Einstein-Gauss-Bonnet (4D EGB) gravity, with additional parameters $\tildeα$ and charge $q$, as central black holes in various galaxies, we investigate gravitational lensing properties in strong deflection limits. Interestingly, the spherical photon orbit radius $x_m$, the critical impact parameter $u_m$, the lensing coefficient $\bar{b}$, the deflection angle $α_D(θ)$, angular position $θ_{\infty}$ are decreasing with $q$ and $α$ whereas the other lensing coefficient $\bar{a}$ and angular separation $s$ have opposite behaviour. Taking the supermassive black holes Sgr A* and M87* as the lens, we also compare observable signatures of 4D EGB Bardeen black holes with those of the Schwarzschild black holes. The angular position $θ_\infty$ for Sgr A* $\in$ (23.1853, \; 25.56427) $μ$as, whereas for M87* it is $\in$ ( 17.941,\; 19.7819) $μ$as. Further, the angular separation $s$, which is an increasing function of $\tildeα$ and $q$ for Sgr A* and M87* differs significantly, respectively, in (0.031997,0.14895) $μ$as and (0.0247, 0.1152) $μ$as. The deviations of the lensing observables $Δθ_{\infty}$ and $Δs$ for 4D EGB Bardeen black hole ($\tildeα=0.9,~q=0.09$) from the Schwarzschild black hole, respectively, can reach up to $2.3789~μ$as and $0.11695~μ$as for Sgr A* , $1.84084~μ$as and $0.0905~μ$as for M87*. On the other hand, the relative magnification $\in$ (4.65751,\; 6.82173). Considering twenty-two massive central black holes as lens, we also estimate the time delay $ΔT^s_{2,1}$ between the first and second relativistic image to find that, e.g., the time delay for Sgr A* and M87*, respectively, can reach $\sim9.86088$~min and $\sim16023.93$~min.

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