Abstract
Most baryons in present-day galaxy clusters exist as hot gas (≳107 K), forming the intracluster medium (ICM)1. Cosmological simulations predict that the mass and temperature of the ICM decline towards earlier times, as intracluster gas in younger clusters is still assembling and being heated2,3,4. To date, hot ICM has been securely detected only in a few systems at or above z ≈ 2, leaving the timing and mechanism of ICM assembly uncertain5,6,7. Here we report the direct observation of hot intracluster gas via its thermal Sunyaev–Zeldovich signature in the protocluster SPT2349–56 with the Atacama Large Millimeter/submillimeter Array. SPT2349–56 hosts a large molecular gas reservoir and three radio-loud active galactic nuclei (AGN) within an approximately 100-kpc region at z = 4.3 (refs. 8,9,10,11). The measurement implies a thermal energy of about 1061 erg in the core, about 10 times more than gravity alone should produce. Contrary to current theoretical expectations3,4,12, the hot ICM in SPT2349–56 demonstrates that substantial heating can occur very early in cluster assembly, depositing enough energy to overheat the nascent ICM well before mature clusters become common at z ≈ 2.
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Data availability
The ALMA (2015.1.01543.T, 2017.1.00273.S, 2022.1.00495.S and 2023.1.00124.S), JWST (JWST-GO-06669), and HST (HST-GO-15701) data used in this work are publicly available on the ALMA science archive (https://almascience.nrao.edu/aq/) and MAST service (https://mast.stsci.edu).
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Acknowledgements
We thank L. Sage for his guidance and feedback, which greatly improved the clarity and presentation of the paper. We thank S. Andreon, A. Babul, L. Bleem, G. Holder, A. Mantz, D. Marrone, D. Nagai, A. Richards, D. Rennehan, J. Sayers, D. Wang, B. Yue and N. Zhang for their discussions on this work. We thank the anonymous referees for their comments and suggestions, which improved the clarity of this work. This paper makes use of the following ALMA data: ADS/JAO.ALMA#2015.1.01543.T, ADS/JAO.ALMA#2017.1.00273.S, ADS/JAO.ALMA#2022.1.00495.S and ADS/JAO.ALMA#2023.1.00124.S. ALMA is a partnership of ESO (representing its member states), NSF (USA) and NINS (Japan), together with NRC (Canada), NSTC and ASIAA (Taiwan) and KASI (Republic of Korea), in cooperation with the Republic of Chile. The Joint ALMA Observatory is operated by ESO, AUI/NRAO and NAOJ. The National Radio Astronomy Observatory is a facility of the National Science Foundation operated under cooperative agreement by Associated Universities. This research used the Canadian Advanced Network for Astronomy Research (CANFAR) operated in partnership by the Canadian Astronomy Data Centre and The Digital Research Alliance of Canada, with support from the National Research Council of Canada, the Canadian Space Agency, CANARIE and the Canadian Foundation for Innovation. This research is based on observations made with 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. These observations are associated with program #15701. This work is based (in part) on observations made with the NASA/ESA/CSA James Webb Space Telescope. The data were obtained from the Mikulski Archive for Space Telescopes at the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, under NASA contract no. NAS 5-03127 for JWST. These observations are associated with program #06669. This research was supported in part by grant NSF PHY-2309135 to the Kavli Institute for Theoretical Physics (KITP). The SPT is supported by the NSF through grant no. OPP-1852617. This work was partially supported by the Center for AstroPhysical Surveys (CAPS) at the National Center for Supercomputing Applications (NCSA), University of Illinois Urbana-Champaign. D.Z., S.C.C., R.H. and G.C.P.W. acknowledge support from NSERC-6740. M. Aravena is supported by FONDECYT grant no. 1252054 and acknowledges support from the ANID Basal Project FB210003 and ANID MILENIO NCN2024_112. M.S. was financially supported by Becas-ANID scholarship #21221511 and also acknowledges support from ANID BASAL project FB210003.
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D.Z. reduced and analysed the data, interpreted the results, produced the figures and drafted the paper. S.C.C. conceived, designed and supervised the projects. R.G. produced the tSZ model of SPT2349–56 for the ALMA proposal. R.D. and R.G. validated the fidelity of the tSZ decrement. P.A.-A. calculated the redshift-evolution of the Compton-Y parameter and hot-gas fraction from TNG-Cluster simulations. S.K. reduced the JWST NIRCam data. D.Z., S.C.C., M. Aravena, P.A.-A., M. Archipley, J.C., R.D., L.D.M., R.G., T.R.G., R.H., S.K., K.A.P., V.R.P., A.C.P., C.R., M.S., J.S.S., N.S., V.J.D., J.D.V., D.V., G.C.P.W. and A.W. contributed substantially to discussing the results and preparing the paper.
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Extended data figures and tables
Extended Data Fig. 1 RGB image of the protocluster core.
The zoomed-in version of Fig. 1. The positions of submillimeter-luminous protocluster galaxies are indicated by their alphabetical names based on their rank-ordered 850 μm flux densities in Ref. 8. Three radio-loud AGN (A, C, and E) are highlighted with their names in red. Due to the crowdedness of the protocluster core, labels of faint members with a negligible 3 mm flux density are hidden in this figure for clarity.
Extended Data Fig. 2 ALMA high-resolution continuum map with the tSZ contours.
The solid contours are tSZ signal from −2σ to −8σ with steps of −1σ. The dashed contours indicate regions with values above 2σ. The number labels on sources are IDs from the continuum source catalog in Extended Data Table 1. The primary beam responses are indicated as dotted lines. The synthesized beams of the continuum image (‘ALMA high-res’) and the SZ decrement (‘SZ’) are indicated in the upper-left and the bottom-left corners, respectively.
Extended Data Fig. 3 ALMA low-resolution tSZ map.
The solid contours are tSZ signal from −2σ to −8σ with steps of −1σ. The dashed contours indicate regions with pixel values above 2σ. The primary beam responses are indicated as dotted lines. The synthesized beam of the SZ decrement is indicated in the bottom-left corner.
Extended Data Fig. 4 Curve-of-growth analysis for the tSZ decrement.
The flux density of the tSZ decrement and the flux-scaled synthesized beam of the ‘SZ’ map are indicated as the red solid and the blue dashed line, respectively. The overdensity radii are also shown as black dotted lines. The turnover in the decrement at radii ≳ 25″ may indicate dirty-beam sidelobes from an imperfect CLEANing process.
Extended Data Fig. 5 uv profile of the original and continuum subtracted data.
The real part of the averaged amplitude measured from the continuum-subtracted measurement sets as a function of uv-distance with uv bins of 3kλ. The errorbars are derived from visibility weightings. The negative signal becomes stronger at a shorter uv distance, suggesting that the tSZ decrement can be limited by the uv-coverage of the ACA and ALMA observations.
Extended Data Fig. 6 Compton-y map with dust continuum contours.
The solid contours are 3 mm continuum emission drawn at [2.5σ, 5σ, 10σ, 20σ, 40σ, 80σ] from the ‘ALMA high-res’ map. The primary beam responses are indicated at dotted lines. The synthesized beams of 3 mm continuum and Compton-y map are indicated in the upper-left and the bottom-left corners.
Extended Data Fig. 8 Halo mass as a function of ICM temperature.
The coloured curves show combinations of halo mass M200 and mass-weighted ICM temperature ⟨T200⟩ that reproduce the observed tSZ decrement for different assumed ICM fractions (from 0.02 to 0.10, as labelled). The corresponding ICM mass MICM is indicated in the top axis. The sub-virialized (blue) and super-virialized (red) regions are separated by the virialized temperature for different M200. The dotted line indicates the dynamical mass of SPT2349−5616. The light hatched band denotes the possible MICM range allowed by the universal baryonic fraction fb = 0.155. Without assuming an extreme ICM fraction fICM, either a more massive virialized halo or a super-virialized ICM gas is necessary to match the observed tSZ decrement.
Extended Data Fig. 9 Cosmic evolution of the hot gas (>107 K) fraction in galaxy clusters.
The fraction of hot ICM (Mhot ICM,500/M500) within r500 as a function of redshift obtained from the TNG-Cluster simulation. Based on the total mass M200 at z = 0, the clusters are placed in three mass bins, high mass (M200 > 1015 M⊙, black solid line), intermediate mass (5 × 1014 M⊙ < M200 < 1015 M⊙, red dashed line), and low mass (M200 < 5 × 1014 M⊙, orange dash-dotted line). The corresponding shaded regions represent the values between the 16th and 84th percentiles in individual mass bins.
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Zhou, D., Chapman, S.C., Aravena, M. et al. Sunyaev–Zeldovich detection of hot intracluster gas at redshift 4.3. Nature 649, 1130–1133 (2026). https://doi.org/10.1038/s41586-025-09901-3
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DOI: https://doi.org/10.1038/s41586-025-09901-3


