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Photon ring structure of rotating regular black holes and no-horizon spacetimes
Classical and Quantum Gravity ( IF 3.6 ) Pub Date : 2021-03-22 , DOI: 10.1088/1361-6382/abdd48
Rahul Kumar 1 , Sushant G Ghosh 1, 2
Affiliation  

The Kerr black holes possess a photon region with prograde and retrograde orbits radii, respectively, $M{\leqslant}{r}_{\mathrm{p}}^{-}{\leqslant}3M$ and $3M{\leqslant}{r}_{\mathrm{p}}^{+}{\leqslant}4M$, and thereby always cast a closed photon ring or a shadow silhouette for aM. For a > M, it is a no-horizon spacetime (naked singularity) wherein prograde orbits spiral into the central singularity, and retrograde orbits produce an arc-like shadow with a dark spot at the center. We compare Kerr black holes’ photon ring structure with those produced by three rotating regular spacetimes, viz Bardeen, Hayward, and nonsingular. These are non-Kerr black hole metrics with an additional deviation parameter of g related to the nonlinear electrodynamics charge. It turns out that for a given a, there exists a critical value of g, g E such that Δ = 0 has no zeros for g > g E, one double zero at r = r E for g = g E, respectively, corresponding to a no-horizon regular spacetime and extremal black hole with degenerate horizon. We demonstrate that, unlike the Kerr naked singularity, no-horizon regular spacetimes can possess closed photon ring when g E < gg c, e.g. for a = 0.10M, Bardeen (g E = 0.763 332M < gg c = 0.816 792M), Hayward (g E = 1.052 97M < gg c = 1.164 846M) and nonsingular (g E = 1.2020M < gg c = 1.222 461M) no-horizon spacetimes have closed photon ring. These results confirm that the mere existence of a closed photon ring does not prove that the compact object is necessarily a black hole. The ring circularity deviation observable ΔC for the three no-horizon rotating spacetimes satisfy ΔC ⩽ 0.10 as per the M87* black hole shadow observations. We have also appended the case of Kerr–Newman no-horizon spacetimes (naked singularities) with similar features.



中文翻译:

旋转规则黑洞和无视界时空的光子环结构

克尔黑洞具有分别具有顺行和逆行轨道半径的光子区域,$M{\leqslant}{r}_{\mathrm{p}}^{-}{\leqslant}3M$并且$3M{\leqslant}{r}_{\mathrm{p}}^{+}{\leqslant}4M$因此总是投射出一个闭合的光子环或一个M的阴影轮廓。对于a > M,它是一个无视界时空(裸奇点),其中顺行轨道螺旋进入中心奇点,逆行轨道产生中心有黑点的弧形阴影。我们将克尔黑洞的光子环结构与由三个旋转的规则时空(即 Bardeen、Hayward 和 nonsingular)产生的光子环结构进行比较。这些是非克尔黑洞度量,具有额外的偏差参数g与非线性电动力学电荷有关。事实证明,对于给定的 a,存在一个临界值gg E使得 Δ = 0 对于g > g E没有零,对于g = g E在r = r E有一个双零,分别对应于到一个无视界规则时空和具有退化视界的极端黑洞。我们证明,与克尔裸奇点不同,当g E < gg c时,无视界规则时空可以拥有闭合光子环,例如 a = 0.10 M , Bardeen ( g E = 0.763 332 M < gg c = 0.816 792 M ), Hayward ( g E = 1.052 97 M < gg c = 1.164 846 M ) 和非奇异的 ( g E = 1.2020 M < gg c = 1.222 461 M) 无视界时空有闭合的光子环。这些结果证实,仅仅存在闭合光子环并不能证明致密物体一定是黑洞。根据 M87 *黑洞阴影观测,三个无视距旋转时空的可观测环圆度偏差 ΔC满足ΔC ⩽ 0.10 。我们还附加了具有相似特征的 Kerr-Newman 无视界时空(裸奇点)案例。

更新日期:2021-03-22
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