User:WiiUf/最大質量黑洞列表

这是迄今为止发现的最大质量黑洞列表,以太阳质量(M☉)為单位(1太阳质量约为×1030公斤)。 2
引言
[编辑]
超大质量黑洞(SMBH)是一种极大的黑洞,其质量约为数十万到数百亿个太阳质量,理论上存在于几乎所有大质量星系的中心,在某些星系中甚至存在超大质量黑洞的双星系统(参见OJ 287系统)。然而,只有少数星系存在超大质量黑洞的明确动力学证据; [1]这些星系包括银河系、本星系群中的仙女座星系和M32 ,以及本星系群以外的一些星系,例如NGC 4395 。在这些星系中,恒星或气体的均方速度(或均方根速度)在中心附近上升约1/r,表明存在中心点质量。在所有其他星系中,迄今为止观测到的均方根速度向中心方向持平甚至下降,因此无法确定超大质量黑洞是否存在于这些星系中。 [1]尽管如此,由于M-Sigma关系(在约10个已确认探测到的星系中,黑洞质量与这些星系核球中恒星的速度離散之间低散射的关系),人们普遍认为几乎每个星系的中心都包含一个超大质量黑洞。 [2] [3]尽管这种相关性仅基于少数几个星系,但对许多天文学家来说,它表明黑洞的形成与星系本身之间存在着紧密的联系。 [2]
尽管目前理论上超大质量黑洞存在于几乎所有大质量星系中,但更大质量的黑洞却很少见;迄今为止只发现不到几十个。确定特定超大质量黑洞的质量极其困难,因此它们仍处于开放研究领域。具有精确质量的超大质量黑洞仅限于拉尼亚凯亚超星系团内的星系和活动星系核。
此列表的另一个问题是用于确定质量的方法。宽发射线混响映射(BLRM)、多普勒测量、速度弥散以及M-sigma关系等方法尚未得到很好的建立。大多数时候,通过不同的方法得出的质量彼此相矛盾。
该列表包含質量已知的超大质量黑洞,至少精確到数量级。此列表中的一些物体被引用兩次,例如3C 273 ;一次来自 Bradley M. Peterson等人使 BLRM方法[4] ,另一次来自 Charles Nelson 使用[O III ]λ5007值和速度弥散[5] 。这个列表並不完整,因为仅斯隆数字巡天就探测到了约000 200类星体,这些类星体很可能是質量達數數十亿倍太阳质量黑洞的所在地。此外,还有数百条有关黑洞测量的引文尚未列入此列表。尽管如此,大多数已知質量大於10亿太陽質量的黑洞都已显示出来。包含已知黑洞的梅西耶星系均包含在内。
新的发现表明,许多被称为“巨大”的黑洞可能超过1億或10億 M☉。 [6]
列表
[编辑]由于涉及的数字非常大,列出的黑洞的质量值采用科学计数法(数字乘以10的幂)。不确定的数值尽可能写在括号中。请注意,此列表中的不同条目在获取其质量值时采用不同的方法和系统,因此对其质量的置信度也不同。这些方法在列表的注释中有说明。
黑洞名稱 | 質量(太陽質量) | 註釋 |
---|---|---|
(理論上限) | ×1011 2.7 | 這是模型估計的黑洞質量上限, at least for luminous accreting SMBHs. At around 1010 M☉, effects of both intense radiation and star formation in the accretion disc slow down black hole growth. 由於宇宙年齡及可用物質的佔比,黑洞的質量幾乎無法超越此上限。 |
凤凰座A | ×1011 1[11] ~×1010 1.26[12] |
Estimated using a calorimetric model on the adiabatic behavior of core regrowth and an assumed core-Sérsic model of n=4. It is consistent with evolutionary modelling of gas accretion and the dynamics and density profiles of the galaxy.[11] Mass has not been measured directly.
Another recent estimate gives ~×1010 M☉, 1.26[12] though this is still uncertain due to low resolution of X-ray/MIR data. |
IC 1101 | 9.77 +17.14 −6.22 × 1010[13][14] |
Estimated from the break radius of the central core; previous estimations using properties of the host galaxy (Faber–Jackson relation) yield about (4-10)×1010 M☉[15] |
4C +74.13 | +9.66 −3.35×1010 5.13[13][14] |
Produced a colossal AGN outburst after accreting 600 million M☉ worth of material.
Estimated using the break radius of 0.5 kpc core of the central galaxy.[13][14] Previous indirect assumptions about the efficiencies of gas accretion and jet power yield a lower limit of 1 billion M☉.[16][17][18] |
(典型理論上限) | ×1010 5 | This is the maximum mass of a black hole with typical properties that models predict, at least for luminous accreting SMBHs. At around 1010 M☉, effects of both intense radiation and star formation in the accretion disc slow down black hole growth. Given the age of the universe and the composition of available matter, there is simply not enough time to grow black holes larger than this mass.
The limit is only ×1010 M☉ for black holes with typical properties, but can reach 5×1011 M☉ at maximal prograde spin (a = 1). 2.7[a] |
TON 618 | ×1010 4.07[19] | Estimated from quasar C IV line correlation. An older estimate gives a mass of ×1010M☉ based on the quasar 6.6Hβ emission line correlation.[20] |
Holmberg 15A | ±0.8 × 4.0 1010[21] | Mass specified obtained through orbit-based, axisymmetric Schwarzschild models. Earlier estimates range from ~310 billion M☉ down to 3 billion M☉, all relying on empirical scaling relations and are thus obtained from extrapolation and not from kinematical measurements.[22] |
S5 0014+81 | ×1010 4[23][24][25] | A 2010 paper suggested that a funnel collimates the radiation around the jet axis, creating an optical illusion of very high brightness, and thus a possible overestimation of the black hole mass.[23] |
SDSS J114833.14+193003.2 | +0.550 −0.625×1010 3.631[26] |
|
NGC 3842 | +6.30 −2.24×1010 3.46[13][14] |
Brightest galaxy in the Leo Cluster; estimation using break radius. Previous estimates yield at least 9.7 billion M☉.[27][28] |
SMSS J215728.21-360215.1 | ±0.6 × 3.4 1010[29] | Estimated using near-infrared spectroscopic measurements of the MgII emission line doublet. |
SDSS J102325.31+514251.0 | +0.67 −0.56×1010 3.31[30] |
Estimated from quasar MgII emission line correlation. |
Abell 1201 BCG | ±0.71 × 3.27 1010[31] | Estimated using strong gravitational lensing from a distant galaxy 1.3 arcseconds separated from the nucleus of the BCG. Earlier estimates suggest a mass of 1.3×1010 M☉.[32] Beware of ambiguity between the BH mass determination and the galaxy cluster's dark matter profile.[33] |
H1821+643 | ×1010 3[34] | Value obtained as an indirect estimate using a model of minimum Eddington luminosity required to account for the Compton cooling of the surrounding cluster.[34] |
NGC 6166 | +0.27 −0.18×1010 2.84[35] |
Central galaxy of Abell 2199; notable for its hundred thousand light year long relativistic jet. |
4C +37.11 | +0.8 −0.8×1010 2.8[36] |
Total mass of black hole binary system. |
ESO 383-76 | +4.66 −1.73×1010 2.75[13][14] |
Estimated using break radius of the galaxy central core. |
2MASS J13260399+7023462 | ±0.4 × 2.7 1010[37] | Estimated using the full-width half maxima of the CIV emission line and monochromatic luminosity at 1350 Å wavelength. |
ESO 444-46 | ×1010( 2.69×108– 5.01×1010) 7.76[13][14] | Brightest cluster galaxy of Abell 3558 in the center of the Shapley Supercluster; estimated using break radius of the host galaxy. |
APM 08279+5255 | ×1010, 2.3[38] +0.17 −0.13×1010 1.0[39] |
Based on velocity width of CO line from orbiting molecular gas,[38] and reverberation mapping using SiIV and CIV emission lines.[39] |
NGC 4889 | ±1.6 × 2.1 1010[27][28] | Best fit: the estimate ranges from 6 billion to 37 billion M☉.[27][28] |
SDSS J074521.78+734336.1 | ±0.05 × 1.95 1010[30] | Estimated from quasar MgII emission line correlation. |
OJ 287 primary | ×1010 1.835[40] | A smaller 100 million M☉ black hole orbits this one in a 12-year period (see below). |
NGC 1600 | ±0.15 × 1.7 1010[41][42] | Unprecedentedly massive in relation of its location: an elliptical galaxy host in a sparse environment. |
SDSS J010013.02+280225.8 | ×109 – 5.0×1010 1.58[43] | |
SDSS J08019.69+373047.3 | ±0.31)×1010 (1.51[30] | Estimated from quasar MgII emission line correlation. |
SDSS J115954.33+201921.1 | ±0.10)×1010 (1.41[30] | Estimated from quasar MgII emission line correlation. |
SDSS J075303.34+423130.8 | ±0.03)×1010 (1.38[30] | Estimated from quasar Hβ emission line correlation. |
SDSS J080430.56+542041.1 | ±0.22)×1010 (1.35[30] | Estimated from quasar MgII emission line correlation.
|
SDSS J081855.77+095848.0 | ±0.06)×1010 (1.20[30] | Estimated from quasar MgII emission line correlation. |
NGC 1270 | ×1010 1.2[44] | Elliptical galaxy located in the Perseus Cluster. Also is a low-luminosity AGN (LLAGN).[45] |
SDSS J082535.19+512706.3 | ±0.20)×1010 (1.12[30] | Estimated from quasar Hβ emission line |
SDSS J013127.34-032100.1 | ±0.2)×1010 (1.1[46] | Estimated from accretion disk spectrum modelling.[46] |
ICRF J131043.3-555211 | +0.02 −0.05×1010 1.05[47] |
Estimated from MgII emission line correlation. |
PSO J334.2028+01.4075 | ×1010 1[48] | There are actually two black holes, orbiting at each other in a close pair with a 542-day period. The largest one is quoted, while the smaller one's mass is not defined.[48] |
RX J1532.9+3021 | ×1010 1[49] | |
QSO B2126-158 | ×1010 1[23]–+1.13 −1.01×1010 4.9[47] |
Higher value estimated with quasar Hβ emission line correlation. |
NGC 1281 | ×1010 1[50] | Compact elliptical galaxy in the Perseus Cluster. Mass estimates range from 10 billion M☉ down to <5 billion M☉.[44] |
SDSS J015741.57-010629.6 | ±1.4)×109 (9.8[30] | |
SDSS J230301.45-093930.7 | ±0.88)×109 (9.12[30] | Estimated from quasar MgII emission line correlation. |
SDSS J140821.67+025733.2 | ×109 8[51] | Initially reported the mass of ×1011 M☉, making this black hole the most massive one discovered, due to incorrect measurement of its C iv width in the DR12Q catalog, amplified by a correction method that exacerbated the overestimate of mass, based on measurements from the SDSS DR12 Quasar Catalog, the new study report that the mass is estimated 1.96×109 M☉ using quasar MgII emission line correlation. 8[51] |
SDSS J075819.70+202300.9 | ±3.9)×109 (7.8[30] | Estimated from quasar Hβ emission line correlation. |
CID-947 | +0.8 −1.2×109 6.9[52] |
Constitutes 10% of the total mass of its host galaxy. Estimated from quasar Hβ emission line correlation. |
SDSS J080956.02+502000.9 | ±0.45)×109 (6.46[30] | Estimated from quasar Hβ emission line correlation. |
SDSS J014214.75+002324.2 | ±1.16)×109 (6.31[30] | Estimated from quasar MgII emission line correlation. |
Messier 87 | +0.34 −0.40×109 7.22[53] ×109 6.3[54] |
Central galaxy of the Virgo Cluster; the first black hole directly imaged. |
NGC 5419 | +2.7 −1.9×109 7.2[55] |
Estimated from the stellar velocity distribution. A secondary satellite SMBH may orbit around 70 parsecs.[55] |
SDSS J025905.63+001121.9 | ±0.73)×109 (5.25[30] | Estimated from quasar Hβ emission line correlation. |
SDSS J094202.04+042244.5 | ±0.71)×109 (5.13[30] | Estimated from quasar Hβ emission line correlation. |
QSO B0746+254 | ×109 5[23] | |
QSO B2149-306 | ×109 5[23] | |
SDSS J090033.50+421547.0 | ±0.2)×109 (4.7[30] | Estimated from quasar MgII emission line correlation. |
Messier 60 | ±1.0)×109 (4.5[56] | |
SDSS J011521.20+152453.3 | ±2.4)×109 (4.1[30] | Estimated from quasar Hβ emission line correlation. |
QSO B0222+185 | ×109 4[23] | |
Hercules A (3C 348) | ×109 4 | Notable for its million light-year long relativistic jet. |
SDSS J075403.60+481428.0 | ×109 3.89[57] | |
SDSS J150752.66+133844.5 | ×109 3.681[57] | |
Abell 1836-BCG | +0.41 −0.50×109 3.61[58] |
|
SDSS J213023.61+122252.0 | ±0.2)×109 (3.5[30] | Estimated from quasar Hβ emission line correlation. |
SDSS J173352.23+540030.4 | ±0.4)×109 (3.4[30] | Estimated from quasar MgII emission line correlation. |
WISE J104222.11+164115.3 | ×109 3.24[59] | Estimated from quasar Hα line correlation. Another paper suggests much higher masses of ±0.6)×1010 M☉ and (8.318+2.2 −1.8×1010 M☉ based on Hα and Hβ line correlations, 8.511[60] however, this is likely inaccurate due to the model not taking into account the reddening of the AGN.[59] |
SDSS J025021.76-075749.9 | ±0.6)×109 (3.1[30] | Estimated from quasar MgII emission line correlation. |
NGC 1271 | +1.0 −1.1×109 3.0[61] |
Compact elliptical or lenticular galaxy in the Perseus Cluster.[62] |
SDSS J030341.04-002321.9 | ±0.4)×109 (3.0[30] | Estimated from quasar MgII emission line correlation. |
QSO B0836+710 | ×109 3[23] | |
SDSS J162752.18+541912.5 | ×109 2.75[57] | |
SDSS J224956.08+000218.0 | ±1.21)×109 (2.63[30] | Estimated from quasar Hβ emission line correlation. |
SDSS J030449.85-000813.4 | ±0.50)×109 (2.4[30] | Estimated from quasar Hβ emission line correlation. |
SDSS J234625.66-001600.4 | ±0.15)×109 (2.24[30] | Estimated from quasar Hβ emission line correlation. |
ULAS J1120+0641 | ×109 2[63][64] | |
QSO 0537-286 | ×109 2[23] | |
NGC 3115 | ×109 2[65] | |
Q0906+6930 | ×109 2[66] | Most distant blazar, at z = 5.47 |
SDSS J025231.19+034112.7 | ×109 1.51[57] | |
QSO B0805+614 | ×109 1.5[23] | |
Messier 84 | ×109 1.5[67] | |
Pōniuāʻena (J100758.264+211529.207) |
±0.2)×109 (1.5[68] | Second most-distant quasar known |
PKS 2059+034 | ×109 1.36[69] | |
Abell 3565-BCG | +0.21 −0.19×109 1.34[58] |
|
NGC 7768 | +0.5 −0.4×109 1.3[28] |
|
NGC 1277 | ×109 1.2[70] | Once thought to harbor a black hole so large that it contradicted modern galaxy formation and evolutionary theories,[71] re-analysis of the data revised it downward to roughly a third of the original estimate.[72] and then one tenth.[70] |
SDSS J233254.46+151305.5 | ×109 1.094[57] | |
QSO B225155+2217 | ×109 1[23] | |
QSO B1210+330 | ×109 1[23] | |
Cygnus A | ×109 1[73] | Brightest extrasolar radio source in the sky as seen at frequencies above 1 GHz |
Sombrero Galaxy | ×109 1[74] | Bolometrically most luminous galaxy in the local universe and also the nearest billion-solar-mass black hole to Earth. |
Markarian 501 | ×108– 9×109 3.4[75] | Brightest object in the sky in very high energy gamma rays. |
PG 1426+015 | ±0.385)×109 (1.298[4] 740000 467[5] |
|
3C 109 | ×108 9.3[76] | |
3C 273 | ±1.87)×108 (8.86[4] 000000 550[5] |
Brightest quasar in the sky |
ULAS J1342+0928 | ×108 8[77] | |
SDSS J155053.16+052112.1 | ×108 7.94[57] | |
Messier 49 | ×108 5.6[78] | |
NGC 1399 | ×108 5[79] | Central galaxy of the Fornax Cluster |
PG 0804+761 | ±0.83)×108 (6.93[4] 550000 190[5] |
|
PG 1617+175 | ±1.38)×108 (5.94[4] 420000 275[5] |
|
PG 1700+518 | +1.82 −1.65×108 7.81[4] 260000 60[5] |
|
UGC 12591 | ±2.61)×108 (6.18[80] | |
SDSS J214611.58-070449.2 | ×109 2.75[57] | |
SDSS J020151.65+012902.5 | ×108 5.37[57] | |
SDSS J113029.48+634620.4 | ×108 4.90[57] | |
NGC 4261 | ×108 4[81] | Notable for its 000 light-year long 88relativistic jet.[82] |
PG 1307+085 | ±1.23 × 4.4, 108[4] 281 840 000[5] |
|
SDSS J134617.54+622045.5 | ×108 3.98[57] | |
SAGE0536AGN | ±0.8 × 3.5 108[83][84] | Constitutes 1.4% of the mass of its host galaxy |
NGC 1275 | ×108 3.4[85] | Central galaxy of the Perseus Cluster |
3C 390.3 | ±0.64 × 2.87 108[4] 840000 338[5] |
|
II Zwicky 136 | ±0.55)×108 (4.57[4] 540000 144[5] |
|
PG 0052+251 | ±0.76)×108 (3.69[4] 780000 218[5] |
|
Messier 59 | ×108 2.7[86] | This black hole has a retrograde rotation.[87] |
PG 1411+442 | ±1.46)×108 (4.43[4] 430000 79[5] |
|
Markarian 876 | ±1.29)×108 (2.79[4] 000000 240[5] |
|
PG 0953+414 | ±0.59)×108 (2.76[4] 000000 182[5] |
|
PG 0026+129 | ±0.96)×108 (3.93[4] 700000 53[5] |
|
Fairall 9 | ±0.56)×108 (2.55[4] 430000 79[5] |
|
NGC 7727 | +0.18 −0.15×108 1.54[88] |
with ×106 companion and the 6.3closest confirmed BBH to Earth at about 89 million light years away |
Markarian 1095 | ±0.19)×108 (1.5[4] 000000 182[5] |
|
Andromeda Galaxy (Messier 31) |
+0.63 −4.4×108, 1.41 +3.19 −2.11×107, 6.22 +8.1 −4.35×107, 9.4 +7.88 −3.29×107, 6.98 +11.43 −1.39×107, 3.74 +2.41 −0.8×108, 1.19 +3.57 −1.96×107, 4.36 +3.08 −1.51×107 2.96[89] |
Nearest large galaxy to the Milky Way. Masses measured with different methods. |
OJ 287 secondary | ×108 1.5[40] | The smaller black hole orbiting OJ 287 primary (see above). |
PG 1211+143 | ±0.44 × 1.46, 108[4] 740000 40[5] |
|
Messier 105 | ×108– 1.4×108 2[90] | |
Markarian 509 | ±0.12 × 1.43, 108[4] 550000 57[5] |
|
RX J124236.9-111935 | ×108 1[91] | Observed by the Chandra X-ray Observatory to be tidally disrupting a star.[91][92] |
Messier 85 | ×108 1[93] | |
NGC 5548 | ±0.26 × 6.71 107[4] 000000 123[5] |
|
Messier 88 | ×107 8[94] | |
Messier 81 (Bode's Galaxy) |
×107 7[95] | |
Markarian 771 | ±3.52 × 7.32 107[4] ×107 7.586[5] |
|
Messier 58 | ×107 7[94] | |
PG 0844+349 | ±3.81 × 9.24 107[4] ×107 2.138[5] |
|
Centaurus A | ×107 5.5[96] | Also notable for its million light-year long relativistic jet.[97] |
Markarian 79 | ±1.44 × 5.24 107[4] ×107 5.25[5] |
|
Messier 96 | ×107 4.8 (000000) 48[98] |
Estimates can be as low as 1.5 million solar masses |
Markarian 817 | ±0.77 × 4.94 107[4] ×107 4.365[5] |
|
NGC 3227 | ±2.14 × 4.22 107[4] ×107 3.89[5] |
|
NGC 4151 primary | ×107 4[99][100] | A small black hole of ×106 M☉ orbits this one (see 10below) |
3C 120 | +3.14 −2.25×107 5.55[4] ×107 2.29[5] |
|
Markarian 279 | ±0.92 × 3.49 107[4] ×107 4.17[5] |
|
NGC 3516 | ±1.46 × 4.27 107[4] ×107 2.3[5] |
|
NGC 863 | ±0.74 × 4.75 107[4] ×107 1.77[5] |
|
Messier 82 (Cigar Galaxy) |
×107 3[101] | Prototype starburst galaxy.[102] |
Messier 108 | ×107 2.4[103] | |
M60-UCD1 | ×107 2[104] | Constitutes 15% of the mass of its host galaxy. |
NGC 3783 | ±0.54 × 2.98 107[4] 300000 9[5] |
|
Markarian 110 | ±0.61 × 2.51 107[4] 620000 5[5] |
|
Markarian 335 | ±0.37 × 1.42 107[4] 310000 6[5] |
|
NGC 4151 secondary | ×106 10 (000000) 10[100] |
Orbiting larger companion (see above) |
NGC 7469 | ±1.4 × 12.2, 106[4] 460000 6[5] |
|
IC 4329A | +17.88 −11.88×106, 9.90[4] 010000 5[5] |
|
NGC 4593 | +9.37 −6.95×106, 5.36[4] 130000 8[5] |
|
Messier 61 | ×106 5[105] | |
Sagittarius A* | ×106 4.3[106] (×1036 kg) 8.54 |
The black hole at the center of the Milky Way; second black hole directly imaged (after Messier 87) |
Messier 32 | ×106– 1.5×106 5[107] | A dwarf satellite galaxy of the Andromeda Galaxy. |
NGC 4395 | ×105 3.599[108] | May be the smallest supermassive black hole. |
參見
[编辑]Notes
[编辑]References
[编辑]- ^ 1.0 1.1 Merritt, David. Dynamics and Evolution of Galactic Nuclei. Princeton, NJ: Princeton University Press. 2013: 23. ISBN 978-0-691-15860-0.
- ^ 2.0 2.1 King, Andrew. Black Holes, Galaxy Formation, and the MBH-σ Relation. The Astrophysical Journal Letters. 2003-09-15, 596 (1): L27–L29. Bibcode:2003ApJ...596L..27K. S2CID 9507887. arXiv:astro-ph/0308342
. doi:10.1086/379143.
- ^ Ferrarese, Laura; Merritt, David. A Fundamental Relation between Supermassive Black Holes and Their Host Galaxies. The Astrophysical Journal (The American Astronomical Society). 2000-08-10, 539 (1): L9–12. Bibcode:2000ApJ...539L...9F. S2CID 6508110. arXiv:astro-ph/0006053
. doi:10.1086/312838.
- ^ 4.00 4.01 4.02 4.03 4.04 4.05 4.06 4.07 4.08 4.09 4.10 4.11 4.12 4.13 4.14 4.15 4.16 4.17 4.18 4.19 4.20 4.21 4.22 4.23 4.24 4.25 4.26 4.27 4.28 4.29 4.30 4.31 4.32 4.33 Peterson, Bradley M. Measuring the Masses of Supermassive Black Holes (PDF). Space Science Reviews. 2013, 183 (1–4): 253 [2015-03-12]. Bibcode:2014SSRv..183..253P. S2CID 16464532. doi:10.1007/s11214-013-9987-4. (原始内容 (PDF)存档于2019-07-26).
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