Intracluster medium

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In astronomy, the intracluster medium (ICM) is the superheated plasma that permeates a galaxy cluster. This gas is heated to temperatures on the order of 10 to 100 megakelvins and composed mainly of ionized hydrogen and helium, containing most of the baryonic material in the cluster. The ICM strongly emits X-ray radiation.

Comparison of the X-ray emission from the intracluster medium in the core of the Abell 2199 galaxy cluster against the optical emission of the galaxies (from the DSS)

Composition[edit]

The ICM is composed primarily of ordinary baryons (mainly ionised hydrogen and helium).[1] This plasma is enriched with heavy elements, such as iron. The amount of heavy elements relative to hydrogen, known as metallicity in astronomy, is roughly a third of the value in the sun.[1] The metallicity rises from the outer region towards the center and in some clusters (e.g. the Centaurus cluster) the metallicity of the gas can rise above that of the sun.[2] Due to the strong gravitational field of clusters, metal-enriched gas ejected during supernovae can remain gravitationally bound to the cluster and become part of the ICM. Studying the composition of the ICM at varying redshift (which results in looking at different points back in time) can therefore give a record of element production in the universe if they are typical.[3]

Most of the baryons in the cluster (80-95%) reside in the ICM (for the Virgo cluster, hot gasses make up roughly 3 × 1014 M[1]), rather than in the luminous matter, such as galaxies and stars. However, most of the mass in a galaxy cluster consists of dark matter (for the Virgo Cluster the total mass is estimated to be 1.2 × 1015 M[4]).

Although the ICM on the whole contains the bulk of a cluster's baryons, it is not very dense, with typical values of 10−3 particles per cubic centimeter. The mean free path of the particles is roughly 1016 m, or about one lightyear. The density of the ICM rises towards the centre of the cluster with a relatively strong peak. In addition, the temperature of the ICM typically drops to 1/2 or 1/3 of the outer value in the central regions. Once the density of the plasma reaches a critical value, enough interactions between the ions ensures cooling via X-ray radiation.[5]

Observing the Intracluster Medium[edit]

As the ICM is at such high temperatures, it emits X-ray radiation, mainly by the bremsstrahlung process and X-ray emission lines from the heavy elements.[1] These X-rays can be observed using an X-ray telescope and through analysis of this data, it is possible to determine the physical conditions, including the temperature, density, and metallicity, of the plasma.

Measurements of the temperature and density profiles in galaxy clusters allow for a determination of the mass distribution profile of the ICM through hydrostatic equilibrium modeling. The mass distributions determined from these methods reveal masses that far exceed the luminous mass seen and are thus a strong indication of dark matter in galaxy clusters.[6]

Inverse Compton Scattering of low energy photons through interactions with the relativistic electrons in the ICM cause distortions in the spectrum of the cosmic microwave background radiation (CMB), known as the Sunyaev–Zel'dovich effect. These temperature distortions in the CMB can be used by telescopes such as the South Pole Telescope to detect dense clusters of galaxies at high redshifts[7]

Cooling flows[edit]

Plasma in regions of the cluster, with a cooling time shorter than the age of the system, should be cooling due to strong X-ray radiation where emission is proportional to the density squared. Since the density of the ICM is highest towards the center of the cluster, the radiative cooling time drops a significant amount.[8] The central cooled gas can no longer support the weight of the external hot gas and the pressure gradient drives what is known as a cooling flow where the hot gas from the external regions flows slowly towards the center of the cluster. This inflow would result in regions of cold gas and thus regions of new star formation.[9] Recently however, with the launch of new X-ray telescopes such as the Chandra X-ray Observatory, images of galaxy clusters with better spatial resolution have been taken. These new images do not indicate signs of new star formation on the order of what was historically predicted, motivating research into the mechanisms that would prevent the central ICM from cooling.[8]

Heating[edit]

Chandra image of the Perseus Cluster's radio lobes. These relativistic jets of plasma emit radio waves, are X-ray "cold", and appear as dark patches in stark contrast to the rest of the ICM.

There are two popular explanations of the mechanisms that prevent the central ICM from cooling, feedback from active galactic nuclei through injection of relativistic jets of plasma[10] and sloshing of the ICM plasma during mergers with subclusters.[11][12] The relativistic jets of material from active galactic nuclei can be seen in images taken by telescopes with high angular resolution such as the Chandra X-ray Observatory.

See also[edit]

References[edit]

  1. ^ a b c d Sparke, L.S.; Gallagher, J.S. (2007). Galaxies in the Universe. Cambridge University Press. ISBN 978-0-521-67186-6. 
  2. ^ Sanders, J. S.; Fabian, A. C.; Taylor, G. B.; Russell, H. R.; Blundell, K. M.; Canning, R. E. A.; Hlavacek-Larrondo, J.; Walker, S. A.; Grimes, C. K. (2016-03-21). "A very deep Chandra view of metals, sloshing and feedback in the Centaurus cluster of galaxies". Monthly Notices of the Royal Astronomical Society. 457 (1): 82–109. doi:10.1093/mnras/stv2972. ISSN 0035-8711. 
  3. ^ Loewenstein, Michael. Chemical Composition of the Intracluster Medium, Carnegie Observatories Centennial Symposia, p.422, 2004.
  4. ^ Fouque, Pascal; Solanes, Jose M.; Sanchis, Teresa; Balkowski, Chantal (2001-09-01). "Structure, mass and distance of the Virgo cluster from a Tolman-Bondi model". Astronomy & Astrophysics. 375 (3): 770–780. doi:10.1051/0004-6361:20010833. ISSN 0004-6361. 
  5. ^ Peterson, J. R.; Fabian, A. C. (2006-04-01). "X-ray spectroscopy of cooling clusters". Physics Reports. 427 (1): 1–39. doi:10.1016/j.physrep.2005.12.007. 
  6. ^ Kotov, O.; Vikhlinin, A. (2006-01-01). "Chandra Sample of Galaxy Clusters at z = 0.4-0.55: Evolution in the Mass-Temperature Relation". The Astrophysical Journal. 641 (2): 752. doi:10.1086/500553. ISSN 0004-637X. 
  7. ^ Staniszewski, Z.; Ade, P. A. R.; Aird, K. A.; Benson, B. A.; Bleem, L. E.; Carlstrom, J. E.; Chang, C. L.; H.-M. Cho; Crawford, T. M. (2009-01-01). "Galaxy Clusters Discovered with a Sunyaev-Zel'dovich Effect Survey". The Astrophysical Journal. 701 (1): 32. doi:10.1088/0004-637X/701/1/32. ISSN 0004-637X. 
  8. ^ a b Fabian, A. C. (2003-06-01). "Cluster cores and cooling flows". 17. eprint: arXiv:astro-ph/0210150: 303–313. 
  9. ^ Fabian, A. C. (1994-01-01). "Cooling Flows in Clusters of Galaxies". Annual Review of Astronomy and Astrophysics. 32: 277–318. doi:10.1146/annurev.aa.32.090194.001425. ISSN 0066-4146. 
  10. ^ Yang, H.-Y. Karen; Reynolds, Christopher S. (2016-01-01). "How AGN Jets Heat the Intracluster Medium—Insights from Hydrodynamic Simulations". The Astrophysical Journal. 829 (2): 90. doi:10.3847/0004-637X/829/2/90. ISSN 0004-637X. 
  11. ^ ZuHone, J. A.; Markevitch, M. (2009-01-01). "Cluster Core Heating from Merging Subclusters". arXiv:0909.0560 [astro-ph]: 383–386. doi:10.1063/1.3293082. 
  12. ^ Fabian, Andrew C. Lighthouses of the Universe: The Most Luminous Celestial Objects and Their Use for Cosmology. Springer, Berlin, Heidelberg. pp. 24–36. doi:10.1007/10856495_3.