<p>Evidence indicates that supermassive black holes (SMBHs) exist at the centres of most galaxies. Their mass correlates with the galactic bulge mass<sup><CitationRef CitationID="CR1">1</CitationRef></sup>, suggesting a coevolution with their host galaxies<sup><CitationRef CitationID="CR2">2</CitationRef></sup>, most likely through powerful winds<sup><CitationRef CitationID="CR3">3</CitationRef></sup>. X-ray observations have detected highly ionized winds outflowing at sub-relativistic speeds from the accretion disks around SMBHs<sup><CitationRef CitationID="CR4">4</CitationRef>,<CitationRef CitationID="CR5">5</CitationRef></sup>. However, the limited spectral resolution of present X-ray instruments has left the physical structure and location of the winds poorly understood, hindering accurate estimates of their kinetic power<sup><CitationRef CitationID="CR6">6</CitationRef>,<CitationRef CitationID="CR7">7</CitationRef></sup>. Here the first X-Ray Imaging and Spectroscopy Mission (XRISM) observation of the luminous quasar PDS 456 is reported. The high-resolution spectrometer Resolve aboard XRISM enabled the discovery of five discrete velocity components outflowing at 20–30% of the speed of light. This demonstrates that the wind structure is highly inhomogeneous, which probably consists of up to a million clumps. The mass outflow rate is estimated to be 60–300 solar masses per year, with the wind kinetic power exceeding the Eddington luminosity limit. Compared with the galaxy-scale outflows, the kinetic power is more than three orders of magnitude larger, whereas the momentum flux is ten times larger. These estimates disfavour both energy-driven and momentum-driven outflow models. This suggests that such wind activity occurs in less than 10% of the quasar phase and/or that its energy/momentum is not efficiently transferred to the galaxy-scale outflows owing to the clumpiness of the wind and the interstellar medium.</p>

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Structured ionized winds shooting out from a quasar at relativistic speeds

  • Marc Audard,
  • Hisamitsu Awaki,
  • Ralf Ballhausen,
  • Aya Bamba,
  • Ehud Behar,
  • Rozenn Boissay-Malaquin,
  • Laura Brenneman,
  • Gregory V. Brown,
  • Lia Corrales,
  • Elisa Costantini,
  • Renata Cumbee,
  • María Díaz Trigo,
  • Chris Done,
  • Tadayasu Dotani,
  • Ken Ebisawa,
  • Megan Eckart,
  • Dominique Eckert,
  • Teruaki Enoto,
  • Satoshi Eguchi,
  • 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,
  • 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 Ogorzalek,
  • Takashi Okajima,
  • Naomi Ota,
  • Stephane Paltani,
  • Robert Petre,
  • Paul Plucinsky,
  • Frederick Scott 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 G. Tsuru,
  • Hiroyuki Uchida,
  • Nagomi Uchida,
  • Yuusuke Uchida,
  • Hideki Uchiyama,
  • 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,
  • Valentina Braito,
  • Pierpaolo Condò,
  • Keigo Fukumura,
  • Adam Gonzalez,
  • Alfredo Luminari,
  • Aiko Miyamoto,
  • Ryuki Mizukawa,
  • James Reeves,
  • Riki Sato,
  • Francesco Tombesi,
  • Yerong Xu

摘要

Evidence indicates that supermassive black holes (SMBHs) exist at the centres of most galaxies. Their mass correlates with the galactic bulge mass1, suggesting a coevolution with their host galaxies2, most likely through powerful winds3. X-ray observations have detected highly ionized winds outflowing at sub-relativistic speeds from the accretion disks around SMBHs4,5. However, the limited spectral resolution of present X-ray instruments has left the physical structure and location of the winds poorly understood, hindering accurate estimates of their kinetic power6,7. Here the first X-Ray Imaging and Spectroscopy Mission (XRISM) observation of the luminous quasar PDS 456 is reported. The high-resolution spectrometer Resolve aboard XRISM enabled the discovery of five discrete velocity components outflowing at 20–30% of the speed of light. This demonstrates that the wind structure is highly inhomogeneous, which probably consists of up to a million clumps. The mass outflow rate is estimated to be 60–300 solar masses per year, with the wind kinetic power exceeding the Eddington luminosity limit. Compared with the galaxy-scale outflows, the kinetic power is more than three orders of magnitude larger, whereas the momentum flux is ten times larger. These estimates disfavour both energy-driven and momentum-driven outflow models. This suggests that such wind activity occurs in less than 10% of the quasar phase and/or that its energy/momentum is not efficiently transferred to the galaxy-scale outflows owing to the clumpiness of the wind and the interstellar medium.