CLUSTERS OF GALAXIES
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Transcript of CLUSTERS OF GALAXIES
CLUSTERS OF GALAXIES
Lecture 1Introduction and
Structure Formation
Clusters of Galaxies:a short overview
Clusters of GalaxiesX-ray Band
K108RMT Tot
gas
X-Ray ImagingX-Ray ImagingX-rays and optical light show us a different picture X-rays and optical light show us a different picture
X-Ray ImagingX-Ray ImagingX-rays and optical light show us a different picture X-rays and optical light show us a different picture
Why study ClustersWhy study Clusters Clusters are the largest structures in the Universe Clusters are the largest structures in the Universe
to have clearly decoupled from the Hubble flow, to have clearly decoupled from the Hubble flow, they carry important cosmological informationthey carry important cosmological information
Physical conditions in clusters are unlike Physical conditions in clusters are unlike anywhere else. They are laboratories where we anywhere else. They are laboratories where we can study the laws of physics under conditions can study the laws of physics under conditions unachiavable elsewhere.unachiavable elsewhere.
The Physics of the ICMThe Physics of the ICM
Cool Cores Cool Cores Cold Fronts Cold Fronts Metals & the ICMMetals & the ICM Non-thermal processes in clusters Non-thermal processes in clusters
The Cluster-Cosmology The Cluster-Cosmology connectionconnection
X-ray Luminosity function, X-ray X-ray Luminosity function, X-ray Temperature function and their evolutionTemperature function and their evolution
Scaling relations, entropy and baryonic Scaling relations, entropy and baryonic fraction fraction
Super-Clusters Super-Clusters
X-Ray ImagingX-Ray Imaging Central regions feature Central regions feature
approx. constant surface approx. constant surface brightness brightness
In outer regions the In outer regions the surface brightness falls surface brightness falls off as a power-law with off as a power-law with index approx. 3 index approx. 3
Emission is traced out to Emission is traced out to 1-2 Mpc from the core1-2 Mpc from the core
Mohr et al. (1999)
Principio Fondamentale della Cosmologia
L’Universo e’ Omogeneo ed Isotropo
Perche’ osserviamo le stelle, le galassie, gli ammassi di galassie?
La struttura su larga scala si e’ formata per la crescita gravitazionaledi piccole perturbazioni di densita’.
Structure Formation
Structure Formation
Structure Formation
1000 galaxies within 1Mpc
Structure FormationLinear Theory
Let us consider the density field with density fluctuations:
This is subject to the continuity equations of Eulero and Poisson:
Entropy conservation
The system does not have a generic analytic solution. However we can linearize the Fourier transform of the previous system. In this case we have:
Pressure termGravitational term
Structure FormationLinear Theory
Jeans Length
Pressure dominates; perturbation oscillatesor
Gravity dominates; perturbation groves
or= o
Structure Formationspherical collapse (1)
Let us consider a perturbation with
It acts as a closed universe (follows the cycloid equations)
The density of the perturbation is
When the perturbation reaches the maximum expansion at We have
t
A
Structure Formationspherical collapse (2)
Energy Virial theorem
Radius and density of the perturbation at the virial
Density contrast at the virial
Linear theory density contrast
Mass FunctionPress & Schechter formalism
The press & Schechter formalism is WRONG
It is simple and help to identify the main “topics”
It gives also a simple analytic formula for the mass function
It is based on the linear theory and uses only and
Density of objects per unit of mass
Mass FunctionPress & Schechter formalism
We consider a density field smoothed on the scale orThe probability that the fluctuation Is collapsed is given by
where
The number density is then
Or equivalently
Mass FunctionPress & Schechter formalism
Intracluster Medium
Hydrostatic equilibrium (spherical symmetry)
We can measure the Cluster mass
Dynamical Properties of the Galaxies
Isothermal Cluster King profile Beta Profile