2002
DOI: 10.1103/physrevd.66.103511
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Cosmological parameters from CMB and other data: A Monte Carlo approach

Abstract: We present a fast Markov Chain Monte-Carlo exploration of cosmological parameter space. We perform a joint analysis of results from recent CMB experiments and provide parameter constraints, including σ8, from the CMB independent of other data. We next combine data from the CMB, HST Key Project, 2dF galaxy redshift survey, supernovae Ia and big-bang nucleosynthesis. The Monte Carlo method allows the rapid investigation of a large number of parameters, and we present results from 6 and 9 parameter analyses of fl… Show more

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Cited by 3,599 publications
(3,839 citation statements)
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References 46 publications
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“…Following [52], we used a modified version of the CAMB code [10] to compute the CMB temperature and polarisation anisotropies seeded by the slow-roll scalar and tensor primordial power spectra of equation (45). The parameter space has been sampled by using Markov Chain Monte Carlo (MCMC) methods implemented in the COSMOMC code [11] and using the likelihood estimator provided by the WMAP team [2,4,3,1]. The likelihood code settings have been kept to their default values which include the pixel based analysis at large scales, a Gaussian likelihood for the beam, with diagonal covariance matrix, and point source corrections [3,53,6].…”
Section: Wmap Data Constraints On the Slow-roll Parametersmentioning
confidence: 99%
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“…Following [52], we used a modified version of the CAMB code [10] to compute the CMB temperature and polarisation anisotropies seeded by the slow-roll scalar and tensor primordial power spectra of equation (45). The parameter space has been sampled by using Markov Chain Monte Carlo (MCMC) methods implemented in the COSMOMC code [11] and using the likelihood estimator provided by the WMAP team [2,4,3,1]. The likelihood code settings have been kept to their default values which include the pixel based analysis at large scales, a Gaussian likelihood for the beam, with diagonal covariance matrix, and point source corrections [3,53,6].…”
Section: Wmap Data Constraints On the Slow-roll Parametersmentioning
confidence: 99%
“…These exact power spectra are computed mode by mode and fed into a modified Cosmic Background Microwave (CMB) code, here a modified CAMB code [10], which allows us to determine the temperature and polarisation multipole moments. Finally, we explore the corresponding parameters space by using MonteCarlo techniques as implemented in the COSMOMC code [11] together with the likelihood code developed by the WMAP team [2]. This allows us to put constraints on the free parameters characterising the models during the inflationary phase but also, in principle, during the reheating phase although, most of the time, the accuracy of the data is not sufficient to obtain relevant limits on the reheating temperature.…”
Section: Introductionmentioning
confidence: 99%
“…[20] coupled to the CosmoMc (Cosmological Monte Carlo) code [21]. This code makes use of a Markov-chain Monte Carlo method to derive the likelihood values of model parameters.…”
Section: Likelihood Analysismentioning
confidence: 99%
“…We have evaluated the likelihood function using the likelihood code that has been made publicly available by the WMAP team [70]. We have obtained the best fit values for the parameters of our model using COSMOMC [71,72], the publicly available, Markov Chain Monte Carlo (MCMC) code for the parameter estimation of a given cosmological model. The MCMC convergence diagnostics are done on multiple parallel chains using the Gelman and Rubin ("variance of chain means"/"mean of chain variances") R statistics for each parameter, demanding that (R−1) < 0.01, a procedure that essentially looks at the fluctuations amongst the different chains and decides when to terminate the run.…”
Section: The Best Fit Values and The Joint Constraintsmentioning
confidence: 99%