Press–Schechter formalism
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The Press–Schechter formalism is a
mathematical model A mathematical model is a description of a system using mathematical concepts and language. The process of developing a mathematical model is termed mathematical modeling. Mathematical models are used in the natural sciences (such as physics, ...
for predicting the number of objects (such as
galaxies A galaxy is a system of stars, stellar remnants, interstellar gas, dust, dark matter, bound together by gravity. The word is derived from the Greek ' (), literally 'milky', a reference to the Milky Way galaxy that contains the Solar System ...
,
galaxy clusters A galaxy cluster, or a cluster of galaxies, is a structure that consists of anywhere from hundreds to thousands of galaxies that are bound together by gravity, with typical masses ranging from 1014 to 1015 solar masses. They are the second- ...
or
dark matter halo According to modern models of physical cosmology, a dark matter halo is a basic unit of cosmological structure. It is a hypothetical region that has decoupled from cosmic expansion and contains gravitationally bound matter. A single dark mat ...
s) of a certain mass within a given volume of the Universe. It was described in an
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by William H. Press and Paul Schechter in 1974.


Background

In the context of
cold dark matter In cosmology and physics, cold dark matter (CDM) is a hypothetical type of dark matter. According to the current standard model of cosmology, Lambda-CDM model, approximately 27% of the universe is dark matter and 68% is dark energy, with only a sm ...
cosmological models, perturbations on all scales are imprinted on the universe at very early times, for example by quantum fluctuations during an inflationary era. Later, as radiation redshifts away, these become mass perturbations, and they start to grow linearly. Only long after that, starting with small mass scales and advancing over time to larger mass scales, do the perturbations actually collapse to form (for example) galaxies or clusters of galaxies, in so-called hierarchical structure formation (see
Physical cosmology Physical cosmology is a branch of cosmology concerned with the study of cosmological models. A cosmological model, or simply cosmology, provides a description of the largest-scale structures and dynamics of the universe and allows study of f ...
). Press and Schechter observed that the fraction of mass in collapsed objects more massive than some mass M is related to the fraction of volume samples in which the smoothed initial density fluctuations are above some density threshold. This yields a formula for the mass function (distribution of masses) of objects at any given time.


Result

The Press–Schechter formalism predicts that the number of objects with mass between M and M+dM is: :dn\equiv N(M)dM = \frac\left(1+\frac\right)\frac\left(\frac\right)^\exp\left(-\left(\frac\right)^\right)dM where n is the index of the power spectrum of the fluctuations in the early universe P(k)\propto k^n, \bar is the mean (baryonic and dark) matter density of the universe at the time the fluctuation from which the object was formed had gravitationally collapsed, and M^* is a cut-off mass below which structures will form. Its value is: :M^* = \left(\frac\right)^ = \left(\frac\right)^\cdot\frac \sigma is the standard deviation per unit volume of the fluctuation from which the object was formed had gravitationally collapsed, at the time of the gravitational collapse, and ''R'' is the scale of the universe at that time. Parameters with subscript 0 are at the time of the initial creation of the fluctuations (or any later time before the gravitational collapse). Qualitatively, the prediction is that the mass distribution is a power law for small masses, with an exponential cutoff above some characteristic mass that increases with time. Such functions had previously been noted by Schechter as observed luminosity functions, and are now known as Schechter luminosity functions. The Press-Schechter formalism provided the first quantitative model for how such functions might arise. The case of a scale-free power spectrum, ''n''=0 (or, equivalently, a scalar spectral index of 1), is very close to the spectrum of the current standard cosmological model. In this case, dn has a simpler form. Written in mass-free units: M\frac = \frac\frac\left(\frac\right)^e^


Assumptions and derivation sketch

The Press–Schechter formalism is derived by assuming that each object is formed by gravitational collapse of a density fluctuation. Furthermore, the fluctuations are assumed to be small at some early cosmological time, and are treated with a linear approximation, even though the eventual collapse is itself a non-linear process. The density fluctuations are normally distributed, and their variance is: \delta_*^2 = \frac = \frac = \frac Where \Sigma is the mass standard deviation in the volume of the fluctuation and M, is its mass. A fractional fluctuation \delta; at some cosmological time reaches gravitational collapse after the universe has expanded by a factor of 1/δ since that time. Using this, the normal distribution of the fluctuations, written in terms of the M, \rho, and \sigma gives the Press-Schechter formula.


Generalizations

A number of generalizations of the Press–Schechter formula exist, such as the Sheth–Tormen approximation.Sheth, R. K., & Tormen, G. (1999). Large-scale bias and the peak background split. Monthly Notices of the Royal Astronomical Society, 308(1), 119-126


References

{{DEFAULTSORT:Press-Schechter formalism Astrophysics Equations of astronomy Mathematical modeling