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Black Hole Shadow Image and Visibility Analysis of Sagittarius A*

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1 Black Hole Shadow Image and Visibility Analysis of Sagittarius A*
黄磊 上海天文台 galactic plane Galactic center

2 Sgr A* --- The Black Hole Candidate in Milky Way Galaxy
Mass : 4 x 106 M⊙ D : kpc Angular size of horizon : ~ 20 μas Angular size of Shadow : ~ 50 μas

3 需要解决的问题: 1. 吸积模型 2. 相对论相应 3. 星际散射 4. 角直径测量 5. 可见度函数
Luminous Accretion Flow Black Hole 2. 相对论相应 Photon Trajectory Interstellar Scattering 3. 星际散射 4. 角直径测量 5. 可见度函数 VLBI Observation

4 光谱特征 RIAF-model vs jet-model
1. 吸积模型 Yuan et al. 2003 Thermal Power-law

5 2. 相对论相应 ~5Rs Fukue et al If observed towards the edge, photons start from the back of the black hole may also reach us. If observed towards the face, in particular, of the optically thick RIAF, only photons start from the surface can reach us.

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7 Elliptical Gaussian shaped scattering screen with FWHMs:
3. 星际散射 point source Elliptical Gaussian shaped scattering screen with FWHMs: θscat maj = ( 1.39 ±0.02 ) λ2 θscat min = ( 0.69 ± 0.06 )λ2 position angle : 80 o (Shen et al ) Interstellar Medium On The Galactic Plane N E Elliptical Gaussian shaped image

8 黑洞倾角与方位角的定义 (方位角) (倾角) 视线方向 观测者

9 波长 1.3mm: 视线方向

10 波长 3.5mm,倾角 90O,方位角 0O: 北 Ray-tracing 视线方向 东 Convolutes with
Interstellar Scattering Screen

11 4. 角直径测量 Huang et al (accepted)

12 结论:倾角大, 中心轴向北

13 考虑吸积流的运动:

14 可见度函数 VLBI Observation .. ? A good U-V coverage is important.

15 No BH BH 3.7M BH 2.6M Visibility profiles of a luminous source WITH and WITHOUT a BH shadow differ a lot. (Miyoshi et al. 2004) (Yuan et al. 2006)

16 Convolutes with Fourier Transform N’-S’ NE’-SW’ NW’-SE’ E’-W’

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20 黑洞自旋: Falcke et al. 2000 Takahashi et al. 2004
RIAF model 未考虑黑洞自旋, 进一步工作需要MHD数值模拟 HOPE FOR COORPERATION …

21 Jet model Falcke & Markoff 2000

22 Markoff et al 结论:倾角大, 中心轴向东 Falcke, 1999

23 谢 谢!


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