TY - JOUR
T1 - XRISM Forecast for the Coma Cluster
T2 - Stormy, with a Steep Power Spectrum
AU - XRISM Collaboration
AU - Audard, Marc
AU - Awaki, Hisamitsu
AU - Ballhausen, Ralf
AU - Bamba, Aya
AU - Behar, Ehud
AU - Boissay-Malaquin, Rozenn
AU - Brenneman, Laura
AU - Brown, Gregory V.
AU - Corrales, Lia
AU - Costantini, Elisa
AU - Cumbee, Renata
AU - Trigo, Maria Diaz
AU - Done, Chris
AU - Dotani, Tadayasu
AU - Ebisawa, Ken
AU - Eckart, Megan E.
AU - Eckert, Dominique
AU - Eguchi, Satoshi
AU - Enoto, Teruaki
AU - Ezoe, Yuichiro
AU - Foster, Adam
AU - Fujimoto, Ryuichi
AU - Fujita, Yutaka
AU - Fukazawa, Yasushi
AU - Fukushima, Kotaro
AU - Furuzawa, Akihiro
AU - Gallo, Luigi
AU - García, Javier A.
AU - Gu, Liyi
AU - Guainazzi, Matteo
AU - Hagino, Kouichi
AU - Hamaguchi, Kenji
AU - Hatsukade, Isamu
AU - Hayashi, Katsuhiro
AU - Hayashi, Takayuki
AU - Hell, Natalie
AU - Hodges-Kluck, Edmund
AU - Hornschemeier, Ann
AU - Ichinohe, Yuto
AU - Ishi, Daiki
AU - Ishida, Manabu
AU - Ishikawa, Kumi
AU - Ishisaki, Yoshitaka
AU - Kaastra, Jelle
AU - Kallman, Timothy
AU - Kara, Erin
AU - Katsuda, Satoru
AU - Kanemaru, Yoshiaki
AU - Kelley, Richard
AU - Kilbourne, Caroline
N1 - Publisher Copyright:
© 2025. The Author(s). Published by the American Astronomical Society.
PY - 2025/5/20
Y1 - 2025/5/20
N2 - The XRISM Resolve microcalorimeter array measured the velocities of hot intracluster gas at two positions in the Coma galaxy cluster: 3¢ ´ 3¢ squares at the center and at 6 (170 kpc) to the south. We find the line-of-sight velocity dispersions in those regions to be σz = 208 ± 12 km s−1 and 202 ± 24 km s−1, respectively. The central value corresponds to a 3D Mach number of M = 0.24 ± 0.015 and a ratio of the kinetic pressure of small-scale motions to thermal pressure in the intracluster plasma of only 3.1% ± 0.4%, at the lower end of predictions from cosmological simulations for merging clusters like Coma, and similar to that observed in the cool core of the relaxed cluster A2029. Meanwhile, the gas in both regions exhibits high line-of-sight velocity differences from the mean velocity of the cluster galaxies, Δvz = 450 ± 15 km s−1 and 730 ± 30 km s−1, respectively. A small contribution from an additional gas velocity component, consistent with the cluster optical mean, is detected along a sight line near the cluster center. The combination of the observed velocity dispersions and bulk velocities is not described by a Kolmogorov velocity power spectrum of steady-state turbulence; instead, the data imply a much steeper effective slope (i.e., relatively more power at larger linear scales). This may indicate either a very large dissipation scale, resulting in the suppression of small-scale motions, or a transient dynamic state of the cluster, where large-scale gas flows generated by an ongoing merger have not yet cascaded down to small scales.
AB - The XRISM Resolve microcalorimeter array measured the velocities of hot intracluster gas at two positions in the Coma galaxy cluster: 3¢ ´ 3¢ squares at the center and at 6 (170 kpc) to the south. We find the line-of-sight velocity dispersions in those regions to be σz = 208 ± 12 km s−1 and 202 ± 24 km s−1, respectively. The central value corresponds to a 3D Mach number of M = 0.24 ± 0.015 and a ratio of the kinetic pressure of small-scale motions to thermal pressure in the intracluster plasma of only 3.1% ± 0.4%, at the lower end of predictions from cosmological simulations for merging clusters like Coma, and similar to that observed in the cool core of the relaxed cluster A2029. Meanwhile, the gas in both regions exhibits high line-of-sight velocity differences from the mean velocity of the cluster galaxies, Δvz = 450 ± 15 km s−1 and 730 ± 30 km s−1, respectively. A small contribution from an additional gas velocity component, consistent with the cluster optical mean, is detected along a sight line near the cluster center. The combination of the observed velocity dispersions and bulk velocities is not described by a Kolmogorov velocity power spectrum of steady-state turbulence; instead, the data imply a much steeper effective slope (i.e., relatively more power at larger linear scales). This may indicate either a very large dissipation scale, resulting in the suppression of small-scale motions, or a transient dynamic state of the cluster, where large-scale gas flows generated by an ongoing merger have not yet cascaded down to small scales.
UR - https://www.scopus.com/pages/publications/105007916644
UR - https://www.scopus.com/pages/publications/105007916644#tab=citedBy
U2 - 10.3847/2041-8213/add2f6
DO - 10.3847/2041-8213/add2f6
M3 - Article
AN - SCOPUS:105007916644
SN - 2041-8205
VL - 985
JO - Astrophysical Journal Letters
JF - Astrophysical Journal Letters
IS - 1
M1 - L20
ER -