REVIEW 4 major objections 5 minor 67 references
The Milky Way's central black hole is currently driving a hot wind that has cleared a parsec-long conical cavity in the cold molecular gas around it.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
2026-08-04 17:44 UTC pith:IUDTNU3B
load-bearing objection A genuinely deeper CO map reveals a striking conical deficit near Sgr A*, but the wind interpretation currently rests on a visual identification that needs an independent cold-gas tracer before it can carry the paper. the 4 major comments →
The Discovery of an Active Wind from the Milky Way's Black Hole
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The paper's central claim is that Sgr A* is currently driving a hot, mildly collimated wind, and that this wind has carved a conical clearing into the cold molecular gas of the Galactic Center. Using combined ALMA observations of the 12CO(J=2→1) line, the authors produce a map roughly 100 times deeper and 80 times sharper than previous maps, revealing a cone-shaped region devoid of cold gas, about 1 pc long with a ~45 degree opening angle, extending south-southwest from Sgr A*. The cavity has sharp edges, molecular gas is otherwise present and rotating around the black hole, and X-ray emitting hot gas fills the region where CO is absent. The power required to heat or evacuate the gas crossin
What carries the argument
The central object is the conical clearing in the 12CO(J=2→1) emission map around Sgr A*: a region nearly devoid of cold molecular gas, roughly 1 pc long with a 45-degree opening angle, interpreted as the imprint of a hot wind. The argument is carried by comparing its morphology and the estimated power needed to keep the cone clear against plausible alternatives—stellar winds and a recent supernova—and by agreement with independent tracers: anti-correlation with hot X-ray gas, the ordered rotational velocity field of the surrounding gas, known structures such as the OH streamer, and the Western Arc of the minispiral lying along the cone's extrapolated path.
Load-bearing premise
The whole case rests on the assumption that the CO-free sector is a genuine continuous cone-shaped cavity in cold gas along the line of sight to Sgr A*, rather than an artifact of projection, foreground absorption, or cold gas being heated or dissociated so that its CO emission disappears.
What would settle it
A clean test is to map the same inner parsec in a cold-gas tracer that does not depend on CO excitation, such as dust continuum emission or an absorption line against a background continuum source behind the proposed SSW cone; if the same conical deficit is absent, the region is not empty and the wind interpretation collapses. A second test would be a direct detection of hot outflowing gas with the expected ~45 degree opening angle and SSW-oriented velocity gradient.
If this is right
- Sgr A* is not dormant: it is actively clearing cold gas within ~1 pc, so the long-standing search for a wind from the Milky Way's central black hole has a concrete candidate.
- The estimated wind power of ~10^38 erg per second exceeds the energy that stellar winds in the Galactic Center can supply, ruling out stellar winds as the origin of the cavity.
- The wind has likely been active for at least ~2×10^4 years, as set by the Keplerian travel time from the wind cone to the far end of the Western Arc.
- The wind is probably the ionization source for the Western Arc of the minispiral, linking black hole activity to the observed morphology of ionized gas.
- Cold molecular gas fills the inner ~0.5 pc and flows inward toward the black hole, so feeding and feedback are happening simultaneously at the Galactic Center.
Where Pith is reading between the lines
- Editorial inference: the conical deficit should also appear in other cold-gas tracers and in dust continuum emission; a targeted survey with, for example, CS or HCN lines, plus absorption measurements against a background source, would independently confirm that the cavity is truly empty rather than merely CO-dark.
- Editorial inference: if the wind is steady, the counter-cone toward the north-northeast may be hidden by projection and by the Sgr A East supernova remnant; deeper observations at wavelengths less affected by foreground confusion could reveal a symmetric pair and constrain the full three-dimensional opening angle.
- Editorial inference: brightness variations along the Western Arc could encode past episodes of elevated Sgr A* activity, potentially allowing a reconstruction of the black hole's accretion and outflow history over roughly 10^4 to 10^5 years.
- Editorial inference: if this wind persists over longer timescales, it may connect to the kiloparsec-scale bubbles and chimneys seen above and below the Galactic plane, implying that the local parsec-scale clearing is one part of a longer feedback cycle.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper presents new ALMA 12CO(2-1) observations of the inner ~1 pc around Sgr A*, with unprecedented depth and resolution, and identifies a conical region largely devoid of CO emission extending south-southwest from the black hole. The authors interpret this as a cavity cleared by a currently active hot wind from Sgr A*, with an opening angle of ~45 degrees and length of at least 1 pc. They also point to an X-ray/CO anti-correlation, a possible NNE counterpart, and an association with the Western Arc of the minispiral. They estimate the required wind power at ~10^38 erg/s and, assuming wind ionization of the Western Arc, a lifetime of at least ~2x10^4 years. The central claim is that the morphology and energetics are consistent with an active Sgr A* wind clearing the cold gas.
Significance. If the interpretation is correct, this would be the first direct detection of Sgr A*'s currently active wind, with implications for black hole feeding and feedback at the Galactic Center and by extension for SMBH physics. The observation itself is a substantial technical achievement: combining multiple ALMA epochs with time-variable Sgr A* subtraction yields a CO map 100 times deeper and 80 times sharper than previous maps, and the recovery of known structures (CND, triop, SEW, OH streamer) validates the data quality. However, the paper's main claim rests on a single morphological interpretation of a CO deficit, without a quantitative significance test or an independent cold-gas tracer. Because CO(2-1) emission is suppressed by heating to ~1000 K or by dissociation, the 'clearing' could equally be a CO-dark region rather than a true cavity. The energetics estimate is a consistency check, not an independent measurement, and the lifetime argument assumes the very wind that is claimed. These weaknesses mean the paper currently offers a promising hypothesis rather than a demonstrated discovery.
major comments (4)
- [Main text, 'Finally, and crucially, we find a large conical clearing...' and Figures 1-2] The conical clearing is identified visually; no quantitative significance test, edge detection, or comparison with symmetric control regions is provided. More importantly, the CO deficit itself is degenerate with heating or dissociation: the Supplementary Information explicitly states that heating to ≳1,000 K suppresses 12CO(2→1) and that CO would fully dissociate at 10^4 K. Thus the 'cone devoid of cold gas' may simply be a region where CO is not emitting, while the molecular gas remains present. No independent cold-gas tracer (e.g., HCN, CS, NH3, or dust continuum) or absorption measurement inside the cone is presented to establish that the gas is actually absent. This is the load-bearing assumption of the entire wind claim and needs to be tested before the cavity can be attributed to a wind.
- [Supplementary Information, 'Estimate of the Wind Energetics'] The jet-power estimate of ~10^38 erg/s is derived from the assumption that the wind cone must be kept clear by ejecting ~250 Msun of gas every ~2200 years. But the heating cost alone is only ~8e35 erg/s (to 10^3 K) or ~1e37 erg/s (to 10^4 K), and the data do not distinguish between heating and clearing because CO emission is suppressed in both cases. The order-of-magnitude estimate is a consistency check, not a detection of the wind power. The paper should either present a direct observable that ties the CO deficit to physical clearing, or clearly frame 10^38 erg/s as an upper limit under a specific ejection scenario.
- [Main text, 'Evidence of the Wind' and 'Energetics and Lifetime of the Wind'] Two inferential steps are circular. First, the NNE counterpart is inferred post hoc from a lack of CO and an X-ray excess, which is the same signature as the SSW cone; this does not independently corroborate the wind. Second, the lifetime estimate assumes that 'the Sgr A* wind is the primary ionization source for the Western Arc' (stated in the main text) and then uses that assumption to derive a 2x10^4-year lifetime. The Western Arc could be ionized by other mechanisms, and the argument is only as strong as the wind-assumption it is meant to validate. The paper should present independent tests, such as spectral diagnostics of the ionized gas or a kinematic model that does not presuppose the wind geometry.
- [Main text, 'Evidence of the Wind', paragraph citing ref. 42] The claim that 'for the edges of the conical clearing to be as pronounced as they are, a presently active wind must be present' relies on the authors' own simulation (ref. 42) to argue that infalling gas would erase past cavities. This is a consistency argument, not independent evidence. The simulation itself is not shown to reproduce the observed clumpy morphology with the same clearing, and the statement does not rule out other mechanisms (e.g., recent stochastic accretion, photodissociation, or geometrical projection). The paper needs a dedicated comparison between the simulation with and without a wind, or an observational proxy that can distinguish wind-clearing from other ways to produce a CO deficit.
minor comments (5)
- [Figure 1 caption] The caption states 'The active black hole wind manifests as a large cavity...' before the interpretation is established. Please use 'candidate cavity' or 'region devoid of CO' to avoid prejudging the result.
- [Supplementary Information, 'Observations and Image Quality'] The terms 'recoverable scale' and 'maximum recoverable scale' are used inconsistently; a single definition (e.g., from the shortest baseline) should be used throughout.
- [Supplementary Information, 'Estimate of the Wind Energetics'] The sentence 'Below,' is incomplete and appears to be a leftover fragment. Also, 'Jupiter' should be 'Jupyter' and 'far' should be 'for' in the Data and materials availability section.
- [Main text, 'Cold Molecular Gas Around Sgr A*'] The statement that the interior of the CND 'is in fact filled with cold molecular gas' is supported by the new map, but the density estimate in the SI relies on a 1 pc cylindrical height and a 10% overlap assumption. Please state the systematic uncertainties more prominently.
- [Figure 2 and Figure 6] The surface-density profile plots are presented in arbitrary units; converting to physically meaningful column density with an assumed abundance would help the reader assess the significance of the radial decline and the contrast of the putative cavity.
Circularity Check
No significant circularity; the wind inference is an interpretation of the observed CO deficit, not a derivation from fitted inputs.
full rationale
The paper's central claim is based on an observed conical deficit in CO(2-1) emission. The interpretation as a wind is supported by X-ray anti-correlation, comparison with known structures, and an energy budget calculation that is computed from the observed gas distribution. The wind power is an order-of-magnitude consistency estimate, not a fitted parameter. The only self-citation (ref 42) is used to argue that the CND erases past signatures, justifying the need for a current wind; however, this simulation contains independent content and does not assume the target result, so it is not circular. No equation-level reduction or parameter-prediction equivalence was found.
Axiom & Free-Parameter Ledger
axioms (4)
- domain assumption The 12CO(J=2-1) emission traces cold molecular gas column density in the inner parsec; deficits trace evacuated or heated cavities.
- domain assumption The gas mass in the inner 0.5 pc and the inflow rate through the wind cone are estimated by scaling the CND's HCN-based mass and Keplerian velocities; the cone clearing rate is roughly 250 Msun per 2200 yr.
- domain assumption Simulations of the CND (Solanki et al. 2023, ref 42) correctly describe the refill and erasure timescale, so a sharp cavity implies a presently active wind.
- ad hoc to paper The Western Arc of the minispiral is ionized by the Sgr A* wind, providing the 20,000 year lifetime estimate.
Cite this review
Pith. "Pith review of The Discovery of an Active Wind from the Milky Way's Black Hole." pith.science (2026). https://pith.science/paper/IUDTNU3B
@misc{pith2026250910615,
author = {Pith},
title = {Pith review of: The Discovery of an Active Wind from the Milky Way's Black Hole},
year = {2026},
howpublished = {\url{https://pith.science/paper/IUDTNU3B}},
note = {Machine review of arXiv:2509.10615}
}
read the original abstract
Every large galaxy has a black hole in its center. The interaction between the black hole and its host profoundly shapes galactic evolution and the Universe as a whole. The key features of this interaction are black hole jets -- or more generally, winds -- which every black hole must have. Despite the proximity and importance of our Galaxy's central black hole, Sagittarius A* (Sgr A*), the active wind from it has eluded scientists for over half a century. Here we report the discovery of a large active wind from Sgr A* using unprecedentedly deep (T$_b \sim30$ mK) and high angular resolution (<0.25") observations with the Atacama Large Millimeter/Submillimeter Array (ALMA). We detect a large conical clearing in the cold molecular gas surrounding Sgr A* that is at least 1~parsec long and has a ~45 degree opening angle. The morphology and energetics of this structure are consistent with active clearing of gas by a hot wind from Sgr A*.
Reference graph
Works this paper leans on
-
[1]
Kormendy, L
J. Kormendy, L. C. Ho, Coevolution (Or Not) of Supermassive Black Holes and Host Galaxies.Ann. Rev. Astron. Astrophys.51(1), 511–653 (2013), doi:10.1146/ annurev-astro-082708-101811
2013
-
[2]
R. Weinberger,et al., Supermassive black holes and their feedback effects in the IllustrisTNG simulation.Mon. Not. R. Astron. Soc.479(3), 4056–4072 (2018), doi:10.1093/mnras/sty1733
-
[3]
R. Blandford, D. Meier, A. Readhead, Relativistic Jets from Active Galactic Nuclei.Ann. Rev. Astron. Astrophys.57, 467–509 (2019), doi:10.1146/annurev-astro-081817-051948
-
[4]
A. H. Bridle, R. A. Perley, Extragalactic Radio Jets.Ann. Rev. Astron. Astrophys.22, 319–358 (1984), doi:10.1146/annurev.aa.22.090184.001535
arXiv 1984
-
[5]
Frank, A
J. Frank, A. King, D. J. Raine,Accretion Power in Astrophysics: Third Edition(2002)
2002
-
[6]
D. Lynden-Bell, M. J. Rees, On quasars, dust and the galactic centre.Mon. Not. R. Astron. Soc. 152, 461 (1971), doi:10.1093/mnras/152.4.461
-
[7]
J. Silk, M. J. Rees, Quasars and galaxy formation.Astron. Astrophys.331, L1–L4 (1998), doi:10.48550/arXiv.astro-ph/9801013
-
[8]
S. W. Davis, A. Tchekhovskoy, Magnetohydrodynamics Simulations of Active Galactic Nucleus Disks and Jets.Ann. Rev. Astron. Astrophys.58, 407–439 (2020), doi:10.1146/ annurev-astro-081817-051905
2020
-
[9]
I. D. Novikov, K. S. Thorne, Astrophysics of black holes., inBlack Holes (Les Astres Occlus), C. Dewitt, B. S. Dewitt, Eds. (1973), pp. 343–450
1973
-
[10]
F. Yuan, R. Narayan, Hot Accretion Flows Around Black Holes.Ann. Rev. Astron. Astrophys. 52, 529–588 (2014), doi:10.1146/annurev-astro-082812-141003
-
[11]
R. D. Blandford, R. L. Znajek, Electromagnetic extraction of energy from Kerr black holes. Mon. Not. R. Astron. Soc.179, 433–456 (1977), doi:10.1093/mnras/179.3.433
-
[12]
R. Blandford, N. Globus, Ergomagnetosphere, ejection disc, magnetopause in M87 - I. Global flow of mass, angular momentum, energy, and current.Mon. Not. R. Astron. Soc.514(4), 5141–5158 (2022), doi:10.1093/mnras/stac1682
-
[13]
M. Su, T. R. Slatyer, D. P. Finkbeiner, Giant Gamma-ray Bubbles from Fermi-LAT: Active Galactic Nucleus Activity or Bipolar Galactic Wind?Astrophys. J.724(2), 1044–1082 (2010), doi:10.1088/0004-637X/724/2/1044
-
[14]
P. Predehl,et al., Detection of large-scale X-ray bubbles in the Milky Way halo.Nature 588(7837), 227–231 (2020), doi:10.1038/s41586-020-2979-0
-
[15]
G. Ponti,et al., An X-ray chimney extending hundreds of parsecs above and below the Galactic Centre.Nature567(7748), 347–350 (2019), doi:10.1038/s41586-019-1009-6. 8
-
[16]
M. R. Morris, M. P. Muno, F. K. Baganoff, Bipolar x-ray lobes around the Galactic Center. X-ray Astronomy 2009; Present Status, Multi-Wavelength Approach and Future Perspectives: Proceedings of the International Conference, inX-ray Astronomy 2009; Present Status, Multi- Wavelength Approach and Future Perspectives, A. Comastri, L. Angelini, M. Cappi, Eds. ...
2009
-
[17]
F. Yusef-Zadeh,et al., Evidence for a jet and outflow from Sgr A*: a continuum and spectral line study.Mon. Not. R. Astron. Soc.499(3), 3909–3931 (2020), doi:10.1093/mnras/staa2399
-
[18]
Peißker,et al., Monitoring dusty sources in the vicinity of Sagittarius A*.Astron
F. Peißker,et al., Monitoring dusty sources in the vicinity of Sagittarius A*.Astron. Astrophys. 634, A35 (2020), doi:10.1051/0004-6361/201935953
-
[19]
Z. Li, M. R. Morris, F. K. Baganoff, Evidence for a Parsec-scale Jet from the Galactic Center Black Hole: Interaction with Local Gas.Astrophys. J.779(2), 154 (2013), doi:10.1088/ 0004-637X/779/2/154
2013
-
[20]
G. Cecil, A. Y. Wagner, J. Bland-Hawthorn, G. V. Bicknell, D. Mukherjee, Tracing the Milky Way’s Vestigial Nuclear Jet.Astrophys. J.922(2), 254 (2021), doi:10.3847/1538-4357/ac224f
-
[21]
F. K. Baganoff,et al., Chandra X-Ray Spectroscopic Imaging of Sagittarius A* and the Central Parsec of the Galaxy.Astrophys. J.591(2), 891–915 (2003), doi:10.1086/375145
doi:10.1086/375145 2003
-
[22]
Event Horizon Telescope Collaboration,et al., First Sagittarius A* Event Horizon Telescope Results. V. Testing Astrophysical Models of the Galactic Center Black Hole.Astrophys. J. Lett. 930(2), L16 (2022), doi:10.3847/2041-8213/ac6672
-
[23]
Astrophys.618, L10 (2018), doi:10.1051/0004-6361/ 201834294
GRA VITY Collaboration,et al., Detection of orbital motions near the last stable circular orbit of the massive black hole SgrA*.Astron. Astrophys.618, L10 (2018), doi:10.1051/0004-6361/ 201834294
-
[24]
R. Genzel, F. Eisenhauer, S. Gillessen, The Galactic Center massive black hole and nuclear star cluster.Reviews of Modern Physics82(4), 3121–3195 (2010), doi:10.1103/RevModPhys. 82.3121
-
[25]
Harada,et al., Chemical features in the circumnuclear disk of the Galactic center.Astron
N. Harada,et al., Chemical features in the circumnuclear disk of the Galactic center.Astron. Astrophys.584, A102 (2015), doi:10.1051/0004-6361/201526994
-
[26]
T. A. James, S. Viti, F. Yusef-Zadeh, M. Royster, M. Wardle, Revealing the Physical Conditions around Sgr A* Using Bayesian Inference. I. Observations and Radiative Transfer.Astrophys. J.916(2), 69 (2021), doi:10.3847/1538-4357/abfd99
-
[27]
A. D. Bolatto, M. Wolfire, A. K. Leroy, The CO-to-H 2 Conversion Factor.Ann. Rev. Astron. Astrophys.51(1), 207–268 (2013), doi:10.1146/annurev-astro-082812-140944
-
[28]
J. R. Goicoechea,et al., High-speed molecular cloudlets around the Galactic center’s super- massive black hole.Astron. Astrophys.618, A35 (2018), doi:10.1051/0004-6361/201833558
-
[29]
J. Marshall, A. N. Lasenby, CO observations of high negative gas towards the Galactic Centre. Mon. Not. R. Astron. Soc.269, 619–625 (1994), doi:10.1093/mnras/269.3.619. 9
-
[30]
I. Mart ´ı-Vidal, W. H. T. Vlemmings, S. Muller, S. Casey, UVMULTIFIT: A versatile tool for fitting astronomical radio interferometric data.Astron. Astrophys.563, A136 (2014), doi: 10.1051/0004-6361/201322633
-
[31]
A. Ciurlo, T. Paumard, D. Rouan, Y. Cl ´enet, Hot molecular hydrogen in the central parsec of the Galaxy through near-infrared 3D fitting.Astron. Astrophys.594, A113 (2016), doi: 10.1051/0004-6361/201527173
-
[32]
R. Genzel, F. Eisenhauer, S. Gillessen, The Galactic Center massive black hole and nuclear star cluster.Reviews of Modern Physics82, 3121–3195 (2010), doi:10.1103/RevModPhys.82.3121
-
[33]
P. R. Maloney, D. J. Hollenbach, A. G. G. M. Tielens, X-Ray–irradiated Molecular Gas. I. Physical Processes and General Results.Astrophys. J.466, 561 (1996), doi:10.1086/177532
doi:10.1086/177532 1996
-
[34]
K. Y. Lo, M. J. Claussen, High-resolution observations of ionized gas in central 3 parsecs of the Galaxy: possible evidence for infall.Nature306(5944), 647–651 (1983), doi:10.1038/ 306647a0
1983
-
[35]
J.-H. Zhao, M. R. Morris, W. M. Goss, T. An, Dynamics of Ionized Gas at the Galactic Center: Very Large Array Observations of the Three-dimensional Velocity Field and Location of the Ionized Streams in Sagittarius A West.Astrophys. J.699(1), 186–214 (2009), doi: 10.1088/0004-637X/699/1/186
-
[36]
Hsieh,et al., The Circumnuclear Disk Revealed by ALMA
P.-Y. Hsieh,et al., The Circumnuclear Disk Revealed by ALMA. I. Dense Clouds and Tides in the Galactic Center.The Astrophysical Journal913(2), 94 (2021), doi:10.3847/1538-4357/ abf4cd,https://doi.org/10.3847%2F1538-4357%2Fabf4cd
-
[37]
J.-H. Zhao, M. R. Morris, W. M. Goss, A New Perspective of the Radio Bright Zone at The Galactic Center: Feedback from Nuclear Activities.Astrophys. J.817(2), 171 (2016), doi:10.3847/0004-637X/817/2/171
-
[38]
Q. D. Wang,et al., Dissecting X-ray-Emitting Gas Around the Center of Our Galaxy.Science 341(6149), 981–983 (2013), doi:10.1126/science.1240755
-
[39]
T. M. Kwan, L. Dai, A. Tchekhovskoy, The Effects of Gas Angular Momentum on the Formation of Magnetically Arrested Disks and the Launching of Powerful Jets.Astrophys. J. Lett.946(2), L42 (2023), doi:10.3847/2041-8213/acc334
-
[40]
M. Liska,et al., A phase lag between disc and corona in GRMHD simulations of precessing tilted accretion discs.New Astronomy101, 102012 (2023), doi:10.1016/j.newast.2023.102012
arXiv 2023
-
[41]
Borodina,et al., You Shall Not Pass! The Propagation of Low-/Moderate-powered Jets Through a Turbulent Interstellar Medium.Astrophys
O. Borodina,et al., You Shall Not Pass! The Propagation of Low-/Moderate-powered Jets Through a Turbulent Interstellar Medium.Astrophys. J.981(2), 149 (2025), doi:10.3847/ 1538-4357/adb016
2025
-
[42]
S. Solanki, S. M. Ressler, L. Murchikova, J. M. Stone, M. R. Morris, The Inner 2 pc of Sagittarius A*: Simulations of the Circumnuclear Disk and Multiphase Gas Accretion in the Galactic Center.Astrophys. J.953(1), 22 (2023), doi:10.3847/1538-4357/acdb6f. 10
-
[43]
Ehlerov ´a,et al., How to create Sgr A East
S. Ehlerov ´a,et al., How to create Sgr A East. Where did the supernova explode?Astron. Astrophys.668, A124 (2022), doi:10.1051/0004-6361/202244682
-
[44]
Y. Maeda,et al., A Chandra Study of Sagittarius A East: A Supernova Remnant Regulating the Activity of Our Galactic Center?Astrophys. J.570(2), 671–687 (2002), doi:10.1086/339773
doi:10.1086/339773 2002
-
[45]
D. Calder ´on, J. Cuadra, M. Schartmann, A. Burkert, C. M. P. Russell, Stellar Winds Pump the Heart of the Milky Way.Astrophys. J. Lett.888(1), L2 (2020), doi:10.3847/2041-8213/ab5e81
-
[46]
S. M. Ressler, E. Quataert, J. M. Stone, The surprisingly small impact of magnetic fields on the inner accretion flow of Sagittarius A* fueled by stellar winds.Mon. Not. R. Astron. Soc. 492(3), 3272–3293 (2020), doi:10.1093/mnras/stz3605
-
[47]
T. Paumard,et al., The Two Young Star Disks in the Central Parsec of the Galaxy: Properties, Dynamics, and Formation.Astrophys. J.643(2), 1011–1035 (2006), doi:10.1086/503273
doi:10.1086/503273 2006
-
[48]
H. Mo, F. C. van den Bosch, S. White,Galaxy Formation and Evolution(2010), doi:10.1017/ CBO9780511807244
2010
-
[49]
CASA Team,et al., CASA, the Common Astronomy Software Applications for Radio As- tronomy.Publications of the Astronomical Society of the Pacifc134(1041), 114501 (2022), doi:10.1088/1538-3873/ac9642
-
[50]
J. Binney, O. E. Gerhard, A. A. Stark, J. Bally, K. I. Uchida, Understanding the kinematics of Galactic Centre gas.Mon. Not. R. Astron. Soc.252, 210 (1991), doi:10.1093/mnras/252.2.210
-
[51]
S. Mart ´ın, J. Mart´ın-Pintado, M. Montero-Casta˜no, P. T. P. Ho, R. Blundell, Surviving the hole. I. Spatially resolved chemistry around Sagittarius A∗.Astron. Astrophys.539, A29 (2012), doi: 10.1051/0004-6361/201117268
-
[52]
P.-Y. Hsieh,et al., A Magnetic Field Connecting the Galactic Center Circumnuclear Disk with Streamers and Mini-spiral: Implications from 850𝜇m Polarization Data.Astrophys. J.862(2), 150 (2018), doi:10.3847/1538-4357/aacb27
-
[53]
L. Moser,et al., Approaching hell’s kitchen: Molecular daredevil clouds in the vicinity of Sagittarius A*.Astron. Astrophys.603, A68 (2017), doi:10.1051/0004-6361/201628385
-
[54]
Sandqvist, R
A. Sandqvist, R. Karlsson, J. B. Whiteoak, OH in the Environment of SGR a, inThe Center of the Galaxy, M. Morris, Ed., vol. 136 ofIAU Symposium(1989), p. 421
1989
-
[55]
R. Karlsson, L. O. Sjouwerman, A. Sandqvist, J. B. Whiteoak, 18-cm VLA observations of OH towards the Galactic Centre. Absorption and emission in the four ground-state OH lines. Astron. Astrophys.403, 1011–1021 (2003), doi:10.1051/0004-6361:20030309
-
[56]
R. Karlsson, A. Sandqvist, K. Fathi, S. Mart ´ın, The OH-streamer in Sagittarius A revisited: analysis of hydroxyl absorption within 10 pc from the Galactic centre.Astron. Astrophys.582, A118 (2015), doi:10.1051/0004-6361/201424426. 11
-
[57]
Z. Zhu, Z. Li, M. R. Morris, An Ultradeep Chandra Catalog of X-Ray Point Sources in the Galactic Center Star Cluster.Astrophys. J. Suppl. Ser.235(2), 26 (2018), doi:10.3847/ 1538-4365/aab14f
2018
-
[58]
M. A. Requena-Torres,et al., GREAT confirms transient nature of the circum-nuclear disk. Astron. Astrophys.542, L21 (2012), doi:10.1051/0004-6361/201219068
-
[59]
E. Quataert, A Thermal Bremsstrahlung Model for the Quiescent X-Ray Emission from Sagit- tarius A*.Astrophys. J.575(2), 855–859 (2002), doi:10.1086/341425
doi:10.1086/341425 2002
-
[60]
A. G. G. M. Tielens, D. Hollenbach, Photodissociation regions. I. Basic model.Astrophys. J. 291, 722–746 (1985), doi:10.1086/163111
doi:10.1086/163111 1985
-
[61]
K. M. Sandstrom,et al., The CO-to-H 2 Conversion Factor and Dust-to-gas Ratio on Kiloparsec Scales in Nearby Galaxies.Astrophys. J.777(1), 5 (2013), doi:10.1088/0004-637X/777/1/5
-
[62]
Kunneriath,et al., The Galactic centre mini-spiral in the mm-regime.Astron
D. Kunneriath,et al., The Galactic centre mini-spiral in the mm-regime.Astron. Astrophys. 538, A127 (2012), doi:10.1051/0004-6361/201117676
-
[63]
S. M. Ressler, E. Quataert, J. M. Stone, Hydrodynamic simulations of the inner accretion flow of Sagittarius A* fuelled by stellar winds.Monthly Notices of the Royal Astronomical Soci- ety478(3), 3544–3563 (2018), doi:10.1093/mnras/sty1146,https://doi.org/10.1093/ mnras/sty1146
-
[64]
S. Chatzopoulos,et al., The old nuclear star cluster in the Milky Way: dynamics, mass, statistical parallax, and black hole mass.Mon. Not. R. Astron. Soc.447(1), 948–968 (2015), doi:10.1093/mnras/stu2452
-
[65]
EHT MWL Science Working Group,et al., Broadband Multi-wavelength Properties of M87 during the 2017 Event Horizon Telescope Campaign.Astrophys. J. Lett.911(1), L11 (2021), doi:10.3847/2041-8213/abef71
-
[66]
M. A. Prieto, J. A. Fern ´andez-Ontiveros, S. Markoff, D. Espada, O. Gonz ´alez-Mart´ın, The central parsecs of M87: jet emission and an elusive accretion disc.Mon. Not. R. Astron. Soc. 457(4), 3801–3816 (2016), doi:10.1093/mnras/stw166. 12 Acknowledgments We are grateful to Claire J. Chandler for advice on data processing, and to Ivan Marti-Vidal, Anna C...
-
[67]
jet power
that the molecular gas is not uniformly distributed in the region, but largely forms clumps and streamers, so the actual density fluctuates a few orders-of-magnitude about this value. This method for calculating gas mass relies on the integrated knowledge of the CND accumulated over decades of observations, and therefore, in our opinion, the most reliable...
This paper was first reviewed by deepseek-v4-flash on August 4, 2026.
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.