Abstract
Starburst galaxies often host multiphase, galaxy-scale winds thought to enrich the circumgalactic medium and limit further star formation by disrupting interstellar gas clouds1,2,3. These winds are primarily powered by supernovae4,5,6, but it remains unclear how supernova energy forms an organized flow. Here we use the Resolve spectrometer on the X-ray Imaging and Spectroscopy Mission to show that the hot (T = 2 × 107 K) gas in the nucleus of the starburst galaxy M82 is moving quickly, with a line-of-sight velocity dispersion \(\sigma =59{5}_{-128}^{+464}\,\mathrm{km}\,{{\rm{s}}}^{-1}\). This is consistent with a hot, nuclear wind generated by thermal pressure. We show that a free-wind model reproduces the measured temperature but underpredicts the velocity. The inferred mass and energy outflow rates from the nucleus, about 7 M⊙ yr−1 and 4 × 1042 erg s−1, require that most supernova energy is thermalized. These outflow rates provide enough energy to power the ≳30 M⊙ yr−1 cool outflow and still transport up to 3 M⊙ yr−1 to the intergalactic medium, suggesting that thermal gas pressure is sufficient to power the multiphase wind without additional support from cosmic rays7. We also show that the nuclear gas is hotter and faster than the plasma seen on larger scales (\(kT\,=\,{0.72}_{-0.08}^{+0.10}\,\mathrm{keV}\), \(\sigma =17{5}_{-73}^{+86}\,\mathrm{km}\,{{\rm{s}}}^{-1}\)), suggesting a distinct origin for the latter.
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An energetic hot wind from the low-luminosity active galactic nucleus M81*
Evidence of the fast acceleration of AGN-driven winds at kiloparsec scales
A snapshot of the oldest active galactic nuclei feedback phases
Data availability
The XRISM data analysed in this study (ObsID 300068010) are available in the High Energy Astrophysics Science Archive Research Center (HEASARC; https://heasarc.gsfc.nasa.gov/docs/archive.html) of NASA. Source data are provided with this paper.
Code availability
The codes used for the data reduction (https://heasarc.gsfc.nasa.gov/docs/software/heasoft) and spectral fitting (https://heasarc.gsfc.nasa.gov/xanadu/xspec) are freely available from the HEASARC website.
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Acknowledgements
This work was supported by JSPS KAKENHI grant nos. JP22H00158, JP22H01268, JP22K03624, JP23H04899, JP21K13963, JP24K00638, JP24K17105, JP21K13958, JP21H01095, JP23K20850, JP24H00253, JP21K03615, JP24K00677, JP20K14491, JP23H00151, JP19K21884, JP20H01947, JP20KK0071, JP23K20239, JP24K00672, JP24K17104, JP24K17093, JP20K04009, JP21H04493, JP20H01946, JP23K13154, JP19K14762, JP20H05857 and JP23K03459 and NASA grant nos. 80NSSC23K0646, 80NSSC20K0733, 80NSSC18K0978, 80NSSC20K0883, 80NSSC20K0737, 80NSSC24K0678, 80NSSC18K1684 and 80NNSC22K1922. L. Corrales acknowledges support from NSF award no. 2205918. C. Done acknowledges support from STFC through grant no. ST/T000244/1. L. Gallo acknowledges financial support from the Canadian Space Agency grant no. 18XARMSTMA. M. Sawada acknowledges support from the RIKEN Pioneering Project Evolution of Matter in the Universe (r-EMU) and the Rikkyo University Special Fund for Research (Rikkyo SFR). A. Tanimoto and the present research are supported, in part, by the Kagoshima University postdoctoral research program (KU-DREAM). S. Yamada acknowledges support by the RIKEN SPDR Program. I. Zhuravleva acknowledges partial support from the Alfred P. Sloan Foundation through the Sloan Research Fellowship. This material is based on the work supported by NASA under award no. 80GSFC24M0006. Part of this work was performed under the auspices of the US Department of Energy by Lawrence Livermore National Laboratory under contract no. DE-AC52-07NA27344. This work was supported by the JSPS Core-to-Core Program, JPJSCCA20220002. The material is based on the work supported by the Strategic Research Center of Saitama University. This research has made use of data obtained from the Chandra Data Archive provided by the Chandra X-ray Center (CXC). This research has made use of data from the NuSTAR mission, a project led by the California Institute of Technology, managed by the Jet Propulsion Laboratory, and funded by the National Aeronautics and Space Administration. This research has made use of data from the NASA/ESA Hubble Space Telescope obtained from the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, under NASA contract no. NAS 5-26555.
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Extended data figures and tables
Extended Data Fig. 1 The starburst nucleus of M82.
The nucleus falls fully within the Resolve field of view (\({3}^{{\prime} }\times {3}^{{\prime} }=3\,{\rm{k}}{\rm{p}}{\rm{c}}\times 3\,{\rm{k}}{\rm{p}}{\rm{c}}\); black outline in a), with the excluded pixel 27 shaded in gray). A Chandra ACIS-S narrowband image shows that the hottest gas traced by Fe xxv 6.7 keV emission (white contours in b) is largely contained within an ellipsoidal thermalization zone (purple region in cartoon in c), where star clusters demarcated by H ii regions (gray clouds) shock-heat ambient medium bounded in the plane of the galaxy by a molecular torus22 (white ring, shown as a cross-section). The torus reduces the fraction of the hot wind that can freely stream (arrows in cartoon), producing the biconical outflow seen in softer emission lines by Chandra (red regions). The spatial extent of Si xiv 2.0 keV emission (R ≲ 1 kpc, Chandra narrowband image in a and b) is representative of the E < 4 keV emission lines seen by Resolve, including S xv 2.4 keV, S xvi 2.6 keV, and Ar xvii 3.1 keV. Softer X-ray emission represented by the O viii 0.65 keV contour plot in a is extended to R ≳ 2 kpc. Point sources have been masked in Chandra images. The blue arrows lie along the major axis of the galaxy.
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XRISM Collaboration. A fast starburst wind consumes most of the energy from supernovae. Nature 651, 909–913 (2026). https://doi.org/10.1038/s41586-026-10231-1
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DOI: https://doi.org/10.1038/s41586-026-10231-1
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