利用 EHT 观测测试与大黄蜂场和黑洞参数估计耦合的 EGB 引力

Misba Afrin, Sushant G. Ghosh, Anzhong Wang
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引用次数: 0

摘要

四维(4DEGB)时空中的一般协变爱因斯坦-高斯-波奈引力被证明可以绕过洛夫洛克定理,并且不受奥斯特洛夫斯基不稳定性的影响。同时,大黄蜂理论是一种矢量-天体理论。它扩展了爱因斯坦-麦克斯韦理论,允许自发对称性破缺,导致场获得真空期望值,并将洛伦兹违反引入系统。我们研究了洛伦兹对称性自发破缺的4D EGB-大黄蜂引力模型中的旋转黑洞--克尔EGB大黄蜂(KEGBB)黑洞。最近事件地平线望远镜(EHT)对超大质量黑洞(SMBHs)M87*和Sgr A*的观测引发了对黑洞阴影研究的浓厚兴趣,这为在强场机制下研究超大质量黑洞提供了一条新途径。受此激励,我们将SMBHs M87*和Sgr A*模拟成KEGBB黑洞,并利用EHT观测结果,在给定的$l$条件下,发现$α$和$a$的早期上限被改变了。KEGBB黑洞和克尔黑洞在某些参数空间中是无法分辨的,我们不能排除前者可能是物理黑洞的有力候选者。利用我们新开发的参数估计技术,我们使用了两个EHT观测值--即阴影的角直径$d_{sh}$和轴向比值$mathcal{D}_A$--来估计M87*和Sgr A*的参数,同时考虑到了与EHT结果相关的观测误差。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Testing EGB gravity coupled to bumblebee field and black hole parameter estimation with EHT observations
A general covariant Einstein-Gauss-Bonnet Gravity in Four-Dimensional (4D EGB) spacetime is shown to bypass Lovelock's theorem and is free from Ostrogradsky instability. Meanwhile, the bumblebee theory is a vector-tensor theory. It extends the Einstein--Maxwell theory that allows for the spontaneous symmetry breaking that leads to the field acquiring a vacuum expectation value, introducing Lorentz violation into the system. We investigate rotating black holes in the 4D EGB-bumblebee gravity model where Lorentz symmetry is spontaneously broken -- Kerr EGB bumblebee (KEGBB) black holes. The latest observations from the Event Horizon Telescope (EHT) of the supermassive black holes (SMBHs) M87* and Sgr A* have sparked intensified interest in the study of black hole shadows, which present a novel avenue for investigating SMBHs within the strong-field regime. Motivated by this, we model SMBHs M87* and Sgr A* as KEGBB black holes, and using the EHT observation result, for given $l$, to find earlier upper limits on the $\alpha$ and $a$ are altered. The KEGBB and Kerr black holes are indiscernible in some parameter space, and one cannot rule out the possibility that the former may serve as strong candidates for astrophysical black holes. Employing our newly developed parameter estimation technique, we use two EHT observables -- namely, the angular diameter of the shadow, $d_{sh}$, and the axial ratio, $\mathcal{D}_A$ -- to estimate parameters of M87* and Sgr A* taking into account observational errors associated with the EHT results.
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