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Physics of the Dark Universe最新文献

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IF 6.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-01
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引用次数: 0
IF 6.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-01
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引用次数: 0
IF 6.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-01
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引用次数: 0
IF 6.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-01
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引用次数: 0
IF 6.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-01
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引用次数: 0
IF 6.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-01
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引用次数: 0
IF 6.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-01
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引用次数: 0
IF 6.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-01
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引用次数: 0
IF 6.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-01
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引用次数: 0
Observational constraints on the rotating Fang-Wang black hole from EHT shadow imaging of M87* and Sgr A* M87*和Sgr A* EHT阴影成像对Fang-Wang黑洞旋转的观测约束
IF 6.4 2区 物理与天体物理 Q1 ASTRONOMY & ASTROPHYSICS Pub Date : 2025-12-31 DOI: 10.1016/j.dark.2025.102203
Himanshi Gulia , J.K. Singh , Farruh Atamurotov , Sushant G. Ghosh
We examine the shadow properties of the rotating Fang-Wang black hole (RFWBH)-a regular black hole solution constructed via the Newman-Janis algorithm from a spherically symmetric solution in general relativity with nonlinear electrodynamics–described by the parameters mass, spin, and a deviation parameter M, a, and l respectively. In turn, we analyse the horizon structure and the ergoregion, demonstrating how l modifies these features compared to the Kerr solution. The shadow of a black hole is studied using celestial coordinates, revealing that increasing l reduces the shadow size and distorts its shape. By employing shadow observables - oblateness D and area A—we estimate the parameters a and l. We further constrain the RFWBH parameter space using recent Event Horizon Telescope (EHT) observations of Sgr A* and M87*, particularly through measurements of the angular shadow diameter. For M87*, at inclination θ=17, (a/M, l/M) ≤ [0.59, 0.07953], with l/M upper bounded for 0.59 ≤ a ≤ 0.8428 lowering with spin; at θ=90, (a/M, l/M) ≤ [0.39, 0.09869] with similar upper bounds on l/M for 0.39 ≤ a ≤ 0.8164. In the case of Sgr A*, the parameter space is constrained as follows: at inclination θ=50, the allowed range for a/M and l/M are [0,0.6692] and [0,0.0305], respectively; and for 90, the allowed ranges for a/M and l/M are [0,0.759] and [0,0.03075], respectively. We also analyse the energy emission rate, finding that the deviation parameter l subdues high-energy emission. Our results indicate that RFWBHs are consistent with current EHT observations and represent viable alternatives to astrophysical black hole models.
我们研究了旋转Fang-Wang黑洞(RFWBH)的阴影特性,这是一个由广义相对论中具有非线性电动力学的球对称解通过Newman-Janis算法构造的规则黑洞解,分别由参数质量、自旋和偏差参数M、a和l描述。反过来,我们分析了视界结构和遍历区域,演示了与Kerr解决方案相比,l如何修改这些特征。利用天体坐标研究了黑洞的阴影,发现增加l会减小阴影的大小并扭曲其形状。通过使用阴影观测值——扁率D和面积a,我们估计了参数a和l。我们利用事件视界望远镜(EHT)最近对Sgr a *和M87*的观测,特别是通过测量角阴影直径,进一步限制了RFWBH参数空间。对于M87*,在倾角θ=17°时,(a/M, l/M) ≤ [0.59,0.07953],l/M上限为0.59 ≤ a ≤ 0.8428随自旋降低;θ=90°,(a/M, l/M) ≤ [0.39,0.09869],l/M的上界为0.39 ≤ a ≤ 0.8164。在Sgr A*的情况下,参数空间受如下限制:在倾角θ=50°时,A /M和l/M的允许范围分别为[0,0.6692]和[0,0.0305];对于90°,a/M和l/M的允许范围分别为[0,0.759]和[0,0.03075]。我们还分析了能量发射速率,发现偏差参数l抑制了高能发射。我们的研究结果表明,RFWBHs与目前的EHT观测结果一致,并代表了天体物理学黑洞模型的可行替代方案。
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引用次数: 0
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Physics of the Dark Universe
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