M. Gaspari
Max Planck Society
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Featured researches published by M. Gaspari.
Astronomy and Astrophysics | 2013
M. Gaspari; E. Churazov
Turbulence and conduction can dramatically affect the evolution of baryons in the universe; current constr aints are however rare and uncertain. Using 3D high-resolution hydrodynamic simulations, tracking both electrons and ions, we study the effects of turbulence and conduction in the hot intracluster medium. We show how the power spectrum of the gas density perturbations (δ = δρ/ρ) can accurately constrain both processes. The characterist ic amplitude of density perturbations is linearly related t o the strength of turbulence, i.e. the 3D Mach number, as A(k)δ,max = c M, where c≃ 0.25 for injection scale of 500 kpc. The slope of Aδ(k) in turn reflects the level of di ffusion, dominated by conduction. In a non-conductive medium, subsonic stirring motions advect density with a similar nearly Kolmogorov cascade, Eδ(k)∝ k −5/3 . Increasing conduction (parametrized via the magnetic suppression f = 10 −3 → 1) progressively steepens the spectrum towards the Burgers-like regime, Eδ(k)∝ k −2 . The slope is only weakly dependent on M. The turbulent Prandtl number defines the dynamic similarity of t he flow; at scales where Pt ≡ tcond/tturb < 100, the power spectrum develops a significant decay, i.e. conduction stifles turbul ent regeneration. The transition is gentle for highly suppr essed conduction, f ≤ 10 −3 , while sharp in the opposite regime. For strong conductivity ( f ≥ 0.1), Pt ∼ 100 occurs on spatial scales larger than the injection scale, globally damping density perturbations by a factor of 2 - 4, from large to small scales. The velocity spectrum is instead not much affected by conduction. The f ≥ 0.1 regime should also affect the appearance of X-ray images, in which Kelvin-Helmholtz and Rayleigh-Taylor rolls and filaments are washed out. In a s tratified system, perturbations are characterized by a mixt ure of modes: weak/strong turbulence induces higher isobaric/adiabatic fluctuations, while conduction forces both modes towards the intermediate isothermal regime. We provide a general analytic fit which is applied to new deep Chandra observations of Coma cluster. The observed spectrum is best consistent with strongly suppressed effective isotropic conduction, f ≃ 10 −3 , and mild subsonic turbulence, M≃ 0.45 (assuming injection scale at∼250 kpc). The latter implies Eturb ≃ 0.11 Eth, in agreement with cosmological simulations and line-broadening observations. The low conductivity corroborates the survival of sharp features in the ICM (cold fr onts, filaments, bubbles), and indicates that cooling flows may not be balance d by conduction.
Astronomy and Astrophysics | 2015
M. Gaspari; Fabrizio Brighenti; P. Temi
Chaotic cold accretion (CCA) profoundly differs from classic black hole accretion models. Using 3D high-resolution simulations, we probe the impact of rotation on the hot and cold accretion flow in a typical massive galaxy. In the hot mode, with or without turbulence, the pressure-dominated flow forms a geometrically thick rotational barrier, suppressing the accretion rate to ~1/3 of the Bondi rate. When radiative cooling is dominant, the gas loses pressure support and quickly circularizes in a cold thin disk. In the more common state of a turbulent and heated atmosphere, CCA drives the dynamics if the gas velocity dispersion exceeds the rotational velocity, i.e., turbulent Taylor number < 1. Extended multiphase filaments condense out of the hot phase via thermal instability and rain toward the black hole, boosting the accretion rate up to 100 times the Bondi rate. Initially, turbulence broadens the angular momentum distribution of the hot gas, allowing the cold phase to condense with prograde or retrograde motion. Subsequent chaotic collisions between the cold filaments, clouds, and a clumpy variable torus promote the cancellation of angular momentum, leading to high accretion rates. The simulated sub-Eddington accretion rates cover the range inferred from AGN cavity observations. CCA predicts inner flat X-ray temperature and
Astronomy and Astrophysics | 2014
D. Eckert; S. Molendi; Matt S. Owers; M. Gaspari; T. Venturi; Lawrence Rudnick; Stefano Ettori; S. Paltani; F. Gastaldello; M. Rossetti
r^{-1}
The Astrophysical Journal | 2018
M. Gaspari; M. McDonald; S. L. Hamer; Fabrizio Brighenti; P. Temi; M. Gendron-Marsolais; J. Hlavacek-Larrondo; A. C. Edge; N. Werner; P. Tozzi; Minghe Sun; J. M. Stone; Grant R. Tremblay; M. T. Hogan; D. Eckert; S. Ettori; H. Yu; V. Biffi; Susana Planelles
density profiles, as recently discovered in M 87 and NGC 3115. The synthetic H{\alpha} images reproduce the main features of cold gas observations in massive ellipticals, as the line fluxes and the filaments versus disk morphology. Such dichotomy is key for the long-term AGN feedback cycle. As gas cools, filamentary CCA develops and boosts AGN heating; the cold mode is thus reduced and the rotating disk remains the sole cold structure. Its consumption leaves the atmosphere in hot mode with suppressed accretion and feedback, reloading the cycle.
The Astrophysical Journal | 2017
D. Eckert; M. Gaspari; F. Vazza; F. Gastaldello; A. Tramacere; S. Zimmer; S. Ettori; S. Paltani
Structure formation in the current Universe operates through the accretion of group-scale systems onto massive clusters. The detection and study of such accreting systems is crucial to understand the build-up of the most massive virialized structures we see today. We report the discovery with XMM-Newton of an irregular X-ray substructure in the outskirts of the massive galaxy cluster Abell 2142. The tip of the X-ray emission coincides with a concentration of galaxies. The bulk of the X-ray emission of this substructure appears to be lagging behind the galaxies and extends over a projected scale of at least 800 kpc. The temperature of the gas in this region is 1.4 keV, which is a factor of ~4 lower than the surrounding medium and is typical of the virialized plasma of a galaxy group with a mass of a few 10^13M_sun. For this reason, we interpret this structure as a galaxy group in the process of being accreted onto the main dark-matter halo. The X-ray structure trailing behind the group is due to gas stripped from its original dark-matter halo as it moves through the intracluster medium (ICM). This is the longest X-ray trail reported to date. For an infall velocity of ~1,200 km s-1 we estimate that the stripped gas has been surviving in the presence of the hot ICM for at least 600 Myr, which exceeds the Spitzer conduction timescale in the medium by a factor of >~400. Such a strong suppression of conductivity is likely related to a tangled magnetic field with small coherence length and to plasma microinstabilities. The long survival time of the low-entropy intragroup medium suggests that the infalling material can eventually settle within the core of the main cluster.
The Astrophysical Journal | 2018
M. McDonald; M. Gaspari; Brian R. McNamara; Grant R. Tremblay
We propose a novel method to constrain turbulence and bulk motions in massive galaxies, groups and clusters, exploring both simulations and observations. As emerged in the recent picture of the top-down multiphase condensation, the hot gaseous halos are tightly linked to all other phases in terms of cospatiality and thermodynamics. While hot halos (10^7 K) are perturbed by subsonic turbulence, warm (10^4 K) ionized and neutral filaments condense out of the turbulent eddies. The peaks condense into cold molecular clouds (< 100 K) raining in the core via chaotic cold accretion (CCA). We show all phases are tightly linked via the ensemble (wide-aperture) velocity dispersion along the line of sight. The correlation arises in complementary long-term AGN feedback simulations and high-resolution CCA runs, and is corroborated by the combined Hitomi and new IFU measurements in Perseus cluster. The ensemble multiphase gas distributions are characterized by substantial spectral line broadening (100-200 km/s) with mild line shift. On the other hand, pencil-beam detections sample the small-scale clouds displaying smaller broadening and significant line shift up to several 100 km/s, with increased scatter due to the turbulence intermittency. We present new ensemble sigma_v of the warm Halpha+[NII] gas in 72 observed cluster/group cores: the constraints are consistent with the simulations and can be used as robust proxies for the turbulent velocities, in particular for the challenging hot plasma (otherwise requiring extremely long X-ray exposures). We show the physically motivated criterion C = t_cool/t_eddy ~ 1 best traces the condensation extent region and presence of multiphase gas in observed clusters/groups. The ensemble method can be applied to many available datasets and can substantially advance our understanding of multiphase halos in light of the next-generation multiwavelength missions.
Astronomy and Astrophysics | 2018
M. Roncarelli; M. Gaspari; S. Ettori; V. Biffi; Fabrizio Brighenti; E. Bulbul; N. Clerc; E. Cucchetti; E. Pointecouteau; E. Rasia
Giant radio halos are Mpc-scale diffuse radio sources associated with the central regions of galaxy clusters. The most promising scenario to explain the origin of these sources is that of turbulent re-acceleration, in which MeV electrons injected throughout the formation history of galaxy clusters are accelerated to higher energies by turbulent motions mostly induced by cluster mergers. In this Letter, we use the amplitude of density fluctuations in the intracluster medium as a proxy for the turbulent velocity and apply this technique to a sample of 51 clusters with available radio data. Our results indicate a segregation in the turbulent velocity of radio halo and radio quiet clusters, with the turbulent velocity of the former being on average higher by about a factor of two. The velocity dispersion recovered with this technique correlates with the measured radio power through the relation
Astronomy and Astrophysics | 2018
E. Cucchetti; E. Pointecouteau; P. Peille; N. Clerc; E. Rasia; V. Biffi; Stefano Borgani; L. Tornatore; K. Dolag; M. Roncarelli; M. Gaspari; S. Ettori; E. Bulbul; T. Dauser; J. Wilms; F. Pajot; Didier Barret
P_{\rm radio}\propto\sigma_v^{3.3\pm0.7}
arXiv: High Energy Astrophysical Phenomena | 2013
S. Ettori; G. W. Pratt; J. de Plaa; D. Eckert; J. Nevalainen; E.S. Battistelli; S. Borgani; J. H. Croston; A. Finoguenov; Jelle S. Kaastra; M. Gaspari; F. Gastaldello; Myriam Gitti; S. Molendi; E. Pointecouteau; T. J. Ponman; Thomas H. Reiprich; M. Roncarelli; M. Rossetti; J. S. Sanders; M. Sun; G. Trinchieri; F. Vazza; M. Arnaud; H. Böringher; Fabrizio Brighenti; H. Dahle; S. De Grandi; J. J. Mohr; A. Moretti
, which implies that the radio power is nearly proportional to the turbulent energy rate. Our results provide an observational confirmation of a key prediction of the turbulent re-acceleration model and possibly shed light on the origin of radio halos.
arXiv: High Energy Astrophysical Phenomena | 2013
J. H. Croston; L. Bîrzan; Richard G. Bower; A. Finoguenov; Diana M Worrall; E. Churazov; A. C. Fabian; J. S. Sanders; M. J. Hardcastle; M. Brüggen; A. C. Edge; T. J. Ponman; G. W. Pratt; P. E. J. Nulsen; M. W. Wise; D. Rafferty; Jelle S. Kaastra; Ralph P. Kraft; Sebastian Heinz; E. Pointecouteau; M. Gaspari; M. Gitti; Brian R. McNamara; Ian G. McCarthy; Debora Sijacki; I. Zhuravleva; S. Ettori; Thomas H. Reiprich
We present a study of 107 galaxies, groups, and clusters spanning ~3 orders of magnitude in mass, ~5 orders of magnitude in central galaxy star formation rate (SFR), ~4 orders of magnitude in the classical cooling rate (dM/dt) of the intracluster medium (ICM), and ~5 orders of magnitude in the central black hole accretion rate. For each system in this sample, we measure dM/dt using archival Chandra X-ray data and acquire the SFR and systematic uncertainty in the SFR by combining over 330 estimates from dozens of literature sources. With these data, we estimate the efficiency with which the ICM cools and forms stars, finding e_cool = SFR/(dM/dt) = 1.4 +/- 0.4% for systems with dM/dt > 30 Msun/yr. For these systems, we measure a slope in the SFR-dM/dt relation greater than unity, suggesting that the systems with the strongest cool cores are also cooling more efficiently. We propose that this may be related to, on average, higher black hole accretion rates in the strongest cool cores, which could influence the total amount (saturating near the Eddington rate) and dominant mode (mechanical vs radiative) of feedback. For systems with dM/dt < 30 Msun/yr, we find that the SFR and dM/dt are uncorrelated, and show that this is consistent with star formation being fueled at a low (but dominant) level by recycled ISM gas in these systems. We find an intrinsic log-normal scatter in SFR at fixed dM/dt of 0.52 +/- 0.06 dex, suggesting that cooling is tightly self-regulated over very long timescales, but can vary dramatically on short timescales. There is weak evidence that this scatter may be related to the feedback mechanism, with the scatter being minimized (~0.4 dex) in systems for which the mechanical feedback power is within a factor of two of the cooling luminosity.