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These methods can be considered exact in some sense, but we demonstrate that using such a large number of imputed values leads to slowly converging Markov chains and EM algorithms. We propose instead the use of a discrete spectral approximation to allow for the implementation of these methods on smaller embedding lattices. While our methods are approximate, our examples indicate that the error introduced by this approximation is small compared to the Monte Carlo errors present in long Markov chains or many iterations of Monte Carlo EM algorithms. Our results are demonstrated in simulation studies, as well as in numerical studies that explore both increasing domain and fixed domain asymptotics. We compare the exact methods to our approximate methods on a large satellite dataset, and show that the approximate methods are also faster to compute, especially when the aliased spectral density is modeled directly. Supplementary materials for this article are available online.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://tandf.figshare.com/articles/dataset/Circulant_embedding_of_approximate_covariances_for_inference_from_Gaussian_data_on_large_lattices/3117349","contentUrl":null,"metadataVersion":2,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"mds","isActive":true,"state":"findable","reason":null,"viewCount":0,"viewsOverTime":[],"downloadCount":0,"downloadsOverTime":[],"refer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