论文标题

研究循环黑洞的EHT观察效应,研究环量子重力

Investigating Loop Quantum Gravity with EHT Observational Effects of Rotating Black holes

论文作者

Islam, Shafqat Ul, Kumar, Jitendra, Walia, Rahul Kumar, Ghosh, Sushant G.

论文摘要

在数学上一致的旋转黑洞模型(LQG)仍缺乏。 LQG中旋转黑洞溶液的稀缺性基本上阻碍了从观测值(例如,从事件范围望远镜(EHT)观测值观察到的LQG)的发展。 EHT观察揭示了超质量黑洞SGR A*和M87*的事件范围图像。 EHT结果与一般相对论的Kerr黑洞的阴影一致。我们提出了LQG动机的旋转黑洞(LMRBH)的空间,它们在各处是常规的,渐近地包含Kerr黑洞作为特定情况。 LMRBH指标描述了一个多匹马黑洞的意义,即它可以承认多达三个视野,因此,与Kerr Black Black Hole不同,它是指具有Angular Momentum $ a> m $的黑洞。指标取决于参数,描述了(1)黑洞,只有一个地平线(BH-I),(2)带有事件视野的黑洞和一个cauchy范围(BH-II),(3)黑洞,具有三个地平线(BH-III)或(BH-III)或(4)无horizo​​n(NH)(NO-HORIZON(NH))的黑洞,我们可以观察到,几乎是在范围内,几乎是在范围内,几乎是在范围内,几乎是何处。我们借助于M87*和SGR A*的EHT阴影观测结果来限制LQG参数,其倾斜角度为$ 17^0 $和$ 50^0 $。特别是,vlti绑定了sgr a*,$δ\ in(-0.17,0.01)$,限制了参数($ a,l $),以至于$ 0 <l \ leq 0.3478.81m \; (l \ leq 2 \ times 10^6 $ km),$ a $的允许范围是$(0,1.0.307亿美元)$。我们的分析与SGR A $^*$和M87 $^*$可观察的EHT界限一起得出结论,BH-I和BH-II参数空间的很大一部分与M87*和SGR A*的EHT结果一致。虽然EHT M87*结果完全排除了BH-III,但不是SGR A*。

A mathematically consistent rotating black hole model in loop quantum gravity (LQG) is yet lacking. The scarcity of rotating black hole solutions in LQG substantially hampers the development of testing LQG from observations, e.g., from the Event Horizon Telescope (EHT) observations. The EHT observation revealed event horizon-scale images of the supermassive black holes Sgr A* and M87*. The EHT results are consistent with the shadow of a Kerr black hole of general relativity. We present LQG-motivated rotating black hole (LMRBH) spacetimes, which are regular everywhere and asymptotically encompass the Kerr black hole as a particular case. The LMRBH metric describes a multi-horizon black hole in the sense that it can admit up to three horizons, such that an extremal LMRBH, unlike the Kerr black hole, refers to a black hole with angular momentum $a>M$. The metric, depending on the parameters, describes (1) black holes with only one horizon (BH-I), (2) black holes with an event horizon and a Cauchy horizons (BH-II), (3) black holes with three horizons (BH-III) or (4) no-horizon (NH) spacetime, which, we show, is almost ruled out by the EHT observations. We constrain the LQG parameter with the aid of the EHT shadow observational results of M87* and Sgr A*,respectively, for an inclination angle of $17^0$ and $50^0$. In particular, the VLTI bound for the Sgr A*, $δ\in (-0.17,0.01)$, constrains the parameters ($a,l$) such that for $0< l\leq 0.347851M\; (l\leq 2\times 10^6$ km), the allowed range of $a$ is $(0,1.0307M)$. Together with the EHT bounds of Sgr A$^*$ and M87$^*$ observables, our analysis concludes that a substantial part of BH-I and BH-II parameter space agrees with the EHT results of M87* and Sgr A*. While the EHT M87* results totally rule out the BH-III, but not that by Sgr A*.

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