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

M. AudardHisamitsu AwakiRalf BallhausenAya BambaEhud BeharRozenn Boissay-MalaquinLaura BrennemanG. V. BrownLía CorralesE. CostantiniRenata CumbeeMaría Díaz TrigoChris DoneTadayasu DotaniKen EbisawaMegan E. EckartD. EckertS. EguchiTeruaki EnotoYuichiro EzoeAdam FosterRyuichi FujimotoYutaka FujitaY. FukazawaKotaro FukushimaAkihiro FuruzawaLuigi GalloJavier A. GarcíaLiyi GuM. GuainazziKouichi HaginoKenji HamaguchiIsamu HatsukadeKatsuhiro HayashiTakayuki HayashiNatalie HellEdmund Hodges‐KluckA. E. HornschemeierYuto IchinoheDaiki IshiManabu IshidaKumi IshikawaYoshitaka IshisakiJ. S. KaastraT. R. KallmanErin KaraSatoru KatsudaYoshiaki KanemaruRichard L. KelleyCaroline A. KilbourneShunji KitamotoShōgo KobayashiTakayoshi KohmuraAya KubotaMaurice A. LeuteneggerMichael LoewensteinYoshitomo MaedaMaxim MarkevitchHironori MatsumotoKyoko MatsushitaD. McCammonB. R. McNamaraFrançois MernierEric D. MillerJ. M. MïllerIkuyuki MitsuishiMisaki MizumotoTsunefumi MizunoKoji MoriK. MukaiHiroshi MurakamiR. F. MushotzkyHiroshi NakajimaKazuhiro NakazawaJan‐Uwe NessKumiko NobukawaMasayoshi NobukawaHirofumi NodaHirokazu OdakaShoji OgawaAnna OgorzałekTakashi OkajimaNaomi OtaS. PaltaniRobert PetrePaul P. PlucinskyF. S. PorterK. PottschmidtKosuke SatoToshiki SatoMakoto SawadaHiromi SetaM. ShidatsuA. SimionescuRandall K. SmithHiromasa SuzukiAndrew E. SzymkowiakH. TakahashiMai TakeoToru Tamagawa
2025lv
ABI

Аннотация

Abstract The XRISM Resolve microcalorimeter array measured the velocities of hot intracluster gas at two positions in the Coma galaxy cluster: <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msup> <mml:mrow> <mml:mn>3</mml:mn> </mml:mrow> <mml:mrow> <mml:mi>′</mml:mi> </mml:mrow> </mml:msup> <mml:mo>×</mml:mo> <mml:msup> <mml:mrow> <mml:mn>3</mml:mn> </mml:mrow> <mml:mrow> <mml:mi>′</mml:mi> </mml:mrow> </mml:msup> </mml:math> squares at the center and at 6 <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi>′</mml:mi> </mml:math> (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.

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