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Many of the following definitions are taken from [#!holdaway:glossary!#,#!aips:glossary!#]. Unfortunately, this glossary is not yet complete. Please forward suggestions for new entries to this author.
To diminish any spurious high spatial frequency features in the solution, fN is convolved with a narrow elliptical Gaussian function h, termed the clean beam. Generally h is chosen by fitting to the central lobe of the dirty beam. Also, one generally adds the final residual map g - b * fN to the approximate solution fN * h, in order to produce a final result, termed the clean map, with a realistic-appearing level of noise.
[This is a description of the Högbom CLEAN algorithm. In practice, a variant of it (Clark, Cotton-Schwab, Steer-Dewdney-Ito) is chosen.]
Discrete two-dimensional deconvolution is an everyday problem in radio interferometry, owing to the fact that--under certain simplifying assumptions--the so-called dirty map is the convolution of the dirty beam with the true celestial radio image. In addition to the maximum entropy method, the CLEAN algorithm is commonly applied to this problem.