The Astrophysical Journal Letters (Jan 2025)

XRISM Forecast for the Coma Cluster: Stormy, with a Steep Power Spectrum

  • XRISM Collaboration,
  • Marc Audard,
  • Hisamitsu Awaki,
  • Ralf Ballhausen,
  • Aya Bamba,
  • Ehud Behar,
  • Rozenn Boissay-Malaquin,
  • Laura Brenneman,
  • Gregory V. Brown,
  • Lia Corrales,
  • Elisa Costantini,
  • Renata Cumbee,
  • Maria Diaz Trigo,
  • Chris Done,
  • Tadayasu Dotani,
  • Ken Ebisawa,
  • Megan E. Eckart,
  • Dominique Eckert,
  • Satoshi Eguchi,
  • Teruaki Enoto,
  • Yuichiro Ezoe,
  • Adam Foster,
  • Ryuichi Fujimoto,
  • Yutaka Fujita,
  • Yasushi Fukazawa,
  • Kotaro Fukushima,
  • Akihiro Furuzawa,
  • Luigi Gallo,
  • Javier A. García,
  • Liyi Gu,
  • Matteo Guainazzi,
  • Kouichi Hagino,
  • Kenji Hamaguchi,
  • Isamu Hatsukade,
  • Katsuhiro Hayashi,
  • Takayuki Hayashi,
  • Natalie Hell,
  • Edmund Hodges-Kluck,
  • Ann Hornschemeier,
  • Yuto Ichinohe,
  • Daiki Ishi,
  • Manabu Ishida,
  • Kumi Ishikawa,
  • Yoshitaka Ishisaki,
  • Jelle Kaastra,
  • Timothy Kallman,
  • Erin Kara,
  • Satoru Katsuda,
  • Yoshiaki Kanemaru,
  • Richard Kelley,
  • Caroline Kilbourne,
  • Shunji Kitamoto,
  • Shogo Kobayashi,
  • Takayoshi Kohmura,
  • Aya Kubota,
  • Maurice Leutenegger,
  • Michael Loewenstein,
  • Yoshitomo Maeda,
  • Maxim Markevitch,
  • Hironori Matsumoto,
  • Kyoko Matsushita,
  • Dan McCammon,
  • Brian McNamara,
  • François Mernier,
  • Eric D. Miller,
  • Jon M. Miller,
  • Ikuyuki Mitsuishi,
  • Misaki Mizumoto,
  • Tsunefumi Mizuno,
  • Koji Mori,
  • Koji Mukai,
  • Hiroshi Murakami,
  • Richard Mushotzky,
  • Hiroshi Nakajima,
  • Kazuhiro Nakazawa,
  • Jan-Uwe Ness,
  • Kumiko Nobukawa,
  • Masayoshi Nobukawa,
  • Hirofumi Noda,
  • Hirokazu Odaka,
  • Shoji Ogawa,
  • Anna Ogorzałek,
  • Takashi Okajima,
  • Naomi Ota,
  • Stéphane Paltani,
  • Robert Petre,
  • Paul Plucinsky,
  • Frederick S. Porter,
  • Katja Pottschmidt,
  • Kosuke Sato,
  • Toshiki Sato,
  • Makoto Sawada,
  • Hiromi Seta,
  • Megumi Shidatsu,
  • Aurora Simionescu,
  • Randall Smith,
  • Hiromasa Suzuki,
  • Andrew Szymkowiak,
  • Hiromitsu Takahashi,
  • Mai Takeo,
  • Toru Tamagawa,
  • Keisuke Tamura,
  • Takaaki Tanaka,
  • Atsushi Tanimoto,
  • Makoto Tashiro,
  • Yukikatsu Terada,
  • Yuichi Terashima,
  • Yohko Tsuboi,
  • Masahiro Tsujimoto,
  • Hiroshi Tsunemi,
  • Takeshi Tsuru,
  • Ayşegül Tümer,
  • Hiroyuki Uchida,
  • Nagomi Uchida,
  • Yuusuke Uchida,
  • Hideki Uchiyama,
  • Shutaro Ueda,
  • Yoshihiro Ueda,
  • Shinichiro Uno,
  • Jacco Vink,
  • Shin Watanabe,
  • Brian J. Williams,
  • Satoshi Yamada,
  • Shinya Yamada,
  • Hiroya Yamaguchi,
  • Kazutaka Yamaoka,
  • Noriko Yamasaki,
  • Makoto Yamauchi,
  • Shigeo Yamauchi,
  • Tahir Yaqoob,
  • Tomokage Yoneyama,
  • Tessei Yoshida,
  • Mihoko Yukita,
  • Irina Zhuravleva,
  • Andrew Fabian,
  • Dylan Nelson,
  • Nobuhiro Okabe,
  • Annalisa Pillepich,
  • Cicely Potter,
  • Manon Regamey,
  • Kosei Sakai,
  • Mona Shishido,
  • Nhut Truong,
  • Daniel R. Wik,
  • John ZuHone

DOI
https://doi.org/10.3847/2041-8213/add2f6
Journal volume & issue
Vol. 985, no. 1
p. L20

Abstract

Read online

The XRISM Resolve microcalorimeter array measured the velocities of hot intracluster gas at two positions in the Coma galaxy cluster: ${3}^{{\prime} }\times {3}^{{\prime} }$ squares at the center and at 6 $^{\prime} $ (170 kpc) to the south. We find the line-of-sight velocity dispersions in those regions to be σ _z = 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, Δ v _z = 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.

Keywords