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The bulk motion of gas in the core of the Centaurus galaxy cluster

Abstract

Galaxy clusters contain vast amounts of hot ionized gas known as the intracluster medium (ICM). In relaxed cluster cores, the radiative cooling time of the ICM is shorter than the age of the cluster. However, the absence of line emission associated with cooling suggests heating mechanisms that offset the cooling, with feedback from active galactic nuclei (AGNs) being the most likely source1,2. Turbulence and bulk motions, such as the oscillating (‘sloshing’) motion of the core gas in the cluster potential well, have also been proposed as mechanisms for heat distribution from the outside of the core3,4. Here we present X-ray spectroscopic observations of the Centaurus galaxy cluster with the X-Ray Imaging and Spectroscopy Mission satellite. We find that the hot gas flows along the line of sight relative to the central galaxy, with velocities from 130 km s−1 to 310 km s−1 within about 30 kpc of the centre. This indicates bulk flow consistent with core gas sloshing. Although the bulk flow may prevent excessive accumulation of cooled gas at the centre, it could distribute the heat injected by the AGN and bring in thermal energy from the surrounding ICM. The velocity dispersion of the gas is found to be only 120 km s−1 in the core, even within about 10 kpc of the AGN. This suggests that the influence of the AGN on the surrounding ICM motion is limited in the cluster.

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Fig. 1: Resolve FOV superimposed on the Chandra X-ray images.
Fig. 2: Resolve spectrum observed for the FOV in the 1.8–8.0 keV band.
Fig. 3: Maps for bulk and turbulent velocities.
Fig. 4: Schematic of the sloshing.

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Data availability

The observational data analysed during this study will be available in the NASA HEASARC repository (https://heasarc.gsfc.nasa.gov/docs/xrism/) in the summer of 2025. The atomic databases used in this study are also available online (AtomDB, http://www.atomdb.org/). Source data are provided with this paper.

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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 80NSSC23K0650, 80NSSC20K0733, 80NSSC18K0978, 80NSSC20K0883, 80NSSC20K0737, 80NSSC24K0678, 80NSSC18K1684 and 80NNSC22K1922). L.C. acknowledges support from NSF award 2205918. C.D. acknowledges support from STFC through grant ST/T000244/1 and a Leverhulme International Fellowship IF-2024-020. L. Gallo acknowledges financial support from the Canadian Space Agency grant 18XARMSTMA. A.T. and the present research are in part supported by the Kagoshima University postdoctoral research program (KU-DREAM). S. Yamada acknowledges support from the RIKEN SPDR Program. I.Z. acknowledges partial support from the Alfred P. Sloan Foundation through the Sloan Research Fellowship. M. Sawada acknowledges the support from the RIKEN Pioneering Project Evolution of Matter in the Universe (r-EMU) and the Rikkyo University Special Fund for Research (Rikkyo SFR). N.W. and T.P. acknowledge the financial support of the GAČR EXPRO (grant no. 21-13491X). Part of this work was performed under the auspices of the US Department of Energy by Lawrence Livermore National Laboratory under contract DE-AC52-07NA27344. The material is based on the work supported by NASA under award no. 80GSFC21M0002. 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.

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Contributions

As the leader of the Centaurus cluster target team in the XRISM Science Team, Y. Fujita led this research project and wrote the paper. K.S. is the sub-leader of the target team, led the data analysis and prepared the manuscript. He also contributed to the Resolve hardware development, integration tests, launch campaign, in-orbit operation and calibration. K.F., F.M., K. Matsushita, A. Simionescu, M.K. and A.M. analysed the data. Y. Fujita, K.S., K.F., F.M., K.M., A. Simionescu, and K. Nakazawa discussed the results. T.H., T.O., K.T., Y. M., M. Lowenstein, T. Yaqoob, E.D.M., M. Markevitch, F.S.P., M. Leutenegger, C.K. and R.K. contributed to the comments on data calibration and systematic errors, as well as on the content of the paper. M. Sun, K. Hosogi, N.W. and T.P. provided additional data and analysis. R.M., I.Z. and E.B. helped to improve the manuscript. The science goals of XRISM were discussed and developed over 7 years by the XRISM Science Team, all members of which are authors of this paper. All the instruments were prepared by the joint efforts of the team. The manuscript was subject to an internal collaboration-wide review process. All authors reviewed and approved the final version of the paper.

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Correspondence to Yutaka Fujita or Kosuke Sato.

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Extended data figures and tables

Extended Data Fig. 1 Representative spectra from and the best-fitting models, including the SSM effect.

a, Broadband and b, zoom-in spectra around He-α-Fe lines for the Central region. c,d, Those for the SW region. Green thick solid line in upper panels show the sum of the total emissions from all the regions. The grey thin solid lines indicate the NXB model. Each coloured line except for the green represents the contribution from one region to the total spectrum in the centre (left) and SW (right) regions. Note that two temperature components in the Central region are shown in two red thick solid lines.

Extended Data Fig. 2 Chandra X-ray images of the Centaurus core.

Left, soft band (0.5–1.2 keV) image with main features highlighted. The white dashed line shows the XRISM Resolve FOV. The black cross indicates the position of the central AGN of galaxy NGC4696 separated by 1 kpc from the X-ray peak of the Centaurus cluster (red cross). Right, hard band (2.0–7.0 keV) image with the best estimates of the cavity borders by CADET for individual detected cavity generations.

Extended Data Fig. 3 Temperature, electron density, metal abundance, and entropy profiles.

They are obtained from deprojection analysis of broad (black points) and hard (red points) band Chandra data.

Extended Data Fig. 4 Flux, velocity and velocity dispersion maps of the warm, ionized gas at the centre of NGC 4696.

They are traced by the strongest optical line [N II] λ6584 from the MUSE data. The nucleus is at the (0, 0) position. The velocity is relative to the system velocity of 3008 km/s.

Extended Data Table 1 Parameters for regions shown in Fig. 1 obtained with Resolve
Extended Data Table 2 Properties of individual cavity generations

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XRISM collaboration. The bulk motion of gas in the core of the Centaurus galaxy cluster. Nature 638, 365–369 (2025). https://doi.org/10.1038/s41586-024-08561-z

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