10. Clusters and Groups of Galaxies

10.1. Properties of Clusters

  • Largest virialized structures in the Universe

  • Richness criterion: at least 50 members with apparent magnitude \(m < m_3 +2\) (with \(m_3\) the magnitude of the third brightest cluster member)

    • Richness = # of galaxies between \(m_3\) and \(m_3 + 2\)

  • Compactness criterion: only members with distances < 1.5 \(h^{-1}\) Mpc

  • Typical sizes: 1-3 Mpc

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  • The richest clusters are typically found at intersections of filaments in the Cosmic Web

  • Roughly \(1-2\) % of galaxies are in rich clusters

  • Up to 10% are in clusters at al

  • The majority of galaxies are in “groups”

10.2. Ingredients of a Cluster

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  • Galaxies

    • \(\sim 100\) large galaxies, \(> 10^{3}\) total galaxies

    • Typical speeds of \(1000\) km/s

  • Intra-cluster Stars

    • Very faint, but comprises of \(10-50\)% of the total cluster light

  • Hot gas

    • Hydrostatic atmosphere of clusters

    • \(T\sim 10^{7-8}\) K → very hot x-ray emitters

    • \(M_{gas} \sim 5 \times M_{gal}\) with \(Z \sim 0.3 Z_{sol}\)

  • Dark matter

    • Absolutely dominates the total mass

10.3. Identification of Clusters

  • Fingers of God: In redshift space, large peculiar velocities make clusters appear as elongated stuctures

  • Quiescent galaxies in clusters have roughly the same colors (same redshift and roughly the same age), so if we see a ton of red galaxies in the same color, they’re likely in a cluster

  • At high \(z\), we cannot use the red sequence method since galaxies are still forming stars and spectroscopic redshifts are difficult to obtain

    • Instead we use intermediate band filters to measure more accurate photometric redshifts (basically photo-z from SEDs)

10.4. Relevant Physical Proceses in Clusters

  • Tidal stripping happens when the tidal forces from a neighboring object overcomes the gravitational force holding the object together

  • Galaxy harassment refers to the accumulated effect of multiple gravitational interactions, both galaxy-galaxy and galaxy-cluster

  • Ram pressure stripping by hot cluster gas, removes cold gas from galaxies

  • Major mergers are less common in galaxy clusters because of the large velocity dispersions \(\sigma \sim 1000\) km/s

10.5. Cluster Galaxy Population

  • There’s typically a radial gradient in galaxy type, with more early type galaxies at the center and spirals/irregulars in the outskirts

  • Butcher-Oemler Effect: Fraction of blue galaxies in clusters increases with redshift

    • Fraction of spirals, star formation increases with redshift,

    • Galaxy populatios evolve rapidly in clusters, primarily due to environmental effects

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10.5.1. Brightest Cluster Galaxies

  • Brightest galaxies in cluster, with essentially zero velocity relative to the cluster mean

  • \(\sim 10L_\star\) galaxies, 50-100 kpc in scale

  • Also called cD galaxies, extended haloes of stars, many of which are radio galaxies

  • Multiple nuclei are often observed, and they’re quite successful at eating their neighbors

  • They do not follow the luminosity function of galaxies

    • They also have lower velocity dispersions for their magnitude/mass than you’d predict from Faber-Jackson relation

10.6. Hot Gas in Clusters

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  • Cluster halos retain a hot, gaseous atmosphere

    • They’re the most luminous, extended X-ray sources, with \(L_x \sim 10^{43}\) to \(10^{46}\) ergs/s

    • Gas is really hot, \(T\sim 10^{7}\) to \(10^{8}\) K, likely heated by infall into the deep halo potential

  • Gas radiates in X-rays via free-free radiation (thermal bremsstrahlung) – basically electrons are accelerated in the electric field of other particles and radiate

  • Gas masses that range from \(M_{gas} \sim M_{stars}\) to \(M_{gas} \sim 7 M_{stars}\) (more massive clusters have higher gas fractions)

  • Gas Accretion

    • Some gas falling into dark matter halo shocks to the virial temperature and reaches (quasi-) hydrostatic equilibrium (hot accretion)

    • The rest of the gas falls in along cold streams (cold accretion)

    • Hot accretion is more dominant in massive halos and at low redshift