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David Thomas Hill PhD Thesis - Research@StAndrews:FullText ...

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Chapter 1. Introduction: The luminosity distribution and total luminosity density of<br />

galaxies<br />

1/Vmax method<br />

The Volume corrected distribution method (1/Vmax) is the simplest, and oldest (Schmidt,<br />

1968) 1 , method of calculating galaxy luminosity distributions. It works by weighting each<br />

galaxy by the volume that it could reside within and still be included within the sample.<br />

Galaxies are then allocated into bins based upon their luminosity. The value for each<br />

bin is the sum of the galaxy weights for all sources within it. For example, Equation 1.5<br />

shows the formulae required to calculate the luminosity density within a bin that covers<br />

dM centred on Ms:<br />

φ(Ms)dM =<br />

Ng �<br />

i=1<br />

N(Ms − dM<br />

2 ≤ Mi ≤ Ms + dM<br />

2 )<br />

Vmax(Mi)<br />

(1.5)<br />

where Ng is the number of galaxies within the sample, N(x) is 1 if the statement x is true,<br />

and 0 otherwise, and Vmax(x) gives the volume a xmagnitude galaxy would be visible<br />

within.<br />

Unfortunately this method is dependent on the size of bins used; different sizes of bins<br />

can lead to different results for the same dataset. It has the advantage of making no<br />

assumptions about the shape of the LF, and has no dependence on the environment (Bell<br />

et al., 2003). A recent approach has been to calculate 1/Vmax for each source, and sum<br />

the parameters provided by the entire population to obtain the luminosity distribution.<br />

SWML method<br />

The SWML method, which is described in detail in Efstathiou et al. (1988), is a maximal-<br />

likelihood method of calculating binned luminosity distributions in a non-parametric man-<br />

ner.<br />

Maximum-likelihood approaches attempt to find the distribution that has the highest<br />

probability of generating the observed sample. In the SWML case, this is computed by<br />

maximising L with respect to a discretised luminosity distribution, where L is the product<br />

of the probabilities of observing each galaxy within the sample’s absolute magnitude limits<br />

(given the redshift of the galaxy). The resulting luminosity distribution can then be fit<br />

via χ 2 -minimisation to determine the Schechter function parameters.<br />

1 This method was first proposed by Kafka (1967), in an unpublished preprint. Schmidt cites this, but has<br />

since been generally credited with its creation. (Felten, 1976)<br />

18

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