2006
DOI: 10.1103/physrevd.73.067301
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Likelihood methods for cluster dark energy surveys

Abstract: Galaxy cluster counts at high redshift, binned into spatial pixels and binned into ranges in an observable proxy for mass, contain a wealth of information on both the dark energy equation of state and the mass selection function required to extract it. The likelihood of the number counts follows a Poisson distribution whose mean fluctuates with the large-scale structure of the universe. We develop a joint likelihood method that accounts for these distributions. Maximization of the likelihood over a theoretical… Show more

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Cited by 53 publications
(71 citation statements)
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“…Hence, as shown in LH04, the likelihood function becomes: and via the convolution theorem this can be approximated as a Gaussian with shifted mean and augmented covariance matrix: where . Note that in the above equation, the approximate sign is used since negative number counts are formally forbidden (for a more detailed discussion of this see Hu & Cohn 2006).…”
Section: Theoretical Backgroundmentioning
confidence: 99%
“…Hence, as shown in LH04, the likelihood function becomes: and via the convolution theorem this can be approximated as a Gaussian with shifted mean and augmented covariance matrix: where . Note that in the above equation, the approximate sign is used since negative number counts are formally forbidden (for a more detailed discussion of this see Hu & Cohn 2006).…”
Section: Theoretical Backgroundmentioning
confidence: 99%
“…(9). The expression for the full Fisher matrix for galaxy cluster counts and their covariance is quite complicated (see [53]), but a reasonable approximation is given by [58] …”
Section: Methodsmentioning
confidence: 99%
“…Because the bias of halo clustering depends on mass (Figure 1), the amplitude and scale-dependence of clustering provides information about the mass-observable relation. Operationally, one parameterizes this relation, then uses standard likelihood methods to jointly fit for both cosmology and the P (X|M, z) parameters (Hu and Cohn, 2006;Holder, 2006). These types of analyses are often referred to as "selfcalibration" because they do not require "direct" mass calibration data.…”
Section: Calibrating the Observable-mass Relationmentioning
confidence: 99%